-------
Table B-6. (Continued)
Hiylura
Class
Subclass
Order
Family Replicate/ fOroanisms/m2) Mean Abundance
Genus gRayteg 1 2 3 4 5 f Organ
Decapoda
Alpheidae
AlPheus fl
-------
Table B-7. Macroinfauna collected at Station M-6, Miami Harbor Interim
CCHD6 Study Area.
Fhylura
Class
Subclass
Order
Family Replicate/ fOraanisns/Tn2! Mean Abundance
Genus Species 1 2 3 4 5 f Organisms/m2)
Cnidaria
Anthozoa
Artiiuaria sp-
19
4
Hydrozoa
19
19
19
11
Rhynchocoela
38
8
Aschelminthes
Nematoda
38
229
287
249
210
203
Mollusca
Aplacophora
19
4
Cephalopoda
Sepiolidae
19
4
Gastropoda
Coluntoellidae
38
19
11
Haminoeidae
19
4
Retxisidae
Rissoidae
19
19
8
Pelecypoda
19
Cuspidariidae
19
76
Lucinidae
38
8
Nuculidae
134
287
57
96
Nuculanidae
76
15
Semelidae
19
4
Tellinidae
Thyasiridae
19
57
229
38
306
130
Scaphopoda
Dentaliidae
38
19
11
S iphcnodental iidae
19
38
11
Annelida
Oligochaeta
19
19
8
Polychaeta
19
Aqpharetidae
38
57
Tsolda oulchella
19
440
92
Isolda sp.
134
134
54
Capitalliffaw
38
38
76
57
42
Chaedtqpteridae
19
4
Cirratulidae
191
803
153
268
153
314
Darvillf iftw
19
19
8
Glyoeridae
76
19
15
GcniadLidae
19
19
38
19
-------
Table B-7. (OortiruBd)
Fhylura
Class
Subclass
Order
Family Reel icate/ (Organisms/m2) Mean Abundance
Genus Species 1 2 3 4 5 fOroanisrns/ro2)
Lumbrineridae
57
76
27
Lumbrineris sd.
210
96
57
73
Magelcnidae
Maaelona sp.
19
4
Maldanidae
19
4
Nephtyidae
19
38
38
19
sp.
57
96
31
Opheliidae
19
4
Ctohelina sd.
76
15
Orbiniidae
96
115
306
229
287
207
Paraemdae
Aricid*# sp.
57
19
76
38
19
42
Pisicsiidae
19
4
Folytnoidae
19
4
Sabellidae
19
4
Spicnidae
19
4
Pricoosoio so.
134
19
287
306
96
168
Sipuncula
19
4
Arthropoda
Crustaoea
C£phalocarida
Hutrfiinscniel 1 idae
Hutrhinsoniella maeraca
19
4
Malacostraca
OmaoRa
Nannastacidae
19
4
Caircvlasois so. B
19
19
8
Diastylidae
DiasWliS sp.
19
19
38
15
Euderella sp-
57
19
19
57
30
Isopoda
QTatbi idae
Gnathla sp.
19
19
19
19
15
Cirolanidae
Ccnilera cylirifrawa
19
38
19
15
Anphipoda
Aaginellidae
Maverella sd.
19
4
-------
Table B-7. (Qcntiruad)
Fhylun
Class
Subclass
Order
Famil>r Replicate/fOrganisms/m2^ Mean Abundance
Anjpeliscidae
Airoelisca aaassizi
2027
3920
402
1270
Airoelisca sd.
19
4
Aoridae
Urciola so.
19
4
Eusiridae
Eusirus sp.
38
8
Lysianassidae
19
4
Hinocnedon sc.
19
19
8
Oediaercrtidae
19
38
38
19
Unidentified sp. A
19
19
19
19
15
Paramphithoidae
Epiperi? sp.
19
4
Paradaliscidae
19
4
RvDxooephalidae
Paff9PhWJS sp.
19
4
Synopiidae
19
4
SYUtYX sp.
19
76
38
27
Decapoda
Pasiphaeidae
Leotochela Dacwlata
19
38
11
Process idae
Processa sd.
19
4
Tanaidacea
Paratarwidae
19
38
11
Ostraooda
Podoocpida
Paracyprididae
19
4
Echinodernata
C^hiuroidea
Ophiuridae
76
19
57
38
38
Totals
3285
2672
1927
6097
2367
3278
Nfumber of Species
25
33
28
29
30
69
Shcvnnon-Weaver Diversity
2.50 3.81 3.90 2.37,'4.13
3.85
-------
Table B-8. Macro irifauna Collected at Station M-7, Miami Harbor Interim
OCMDS Study Area.
Riylura
Class
Subclass
Order
Family Replicate/fOrganians/m2) Mean Abundance
Germs Species 1 2 3 4 5 fOroanisms/m2)
Cnidaria
Hydrozoa
19
19
8
Rhynchocoela
19
19
19
11
Asc±ielmirtthes
Nematoda
497
363
746
134
363
421
Mollusca
Gastropoda
Oolumbellidae
19
19
38
15
E^itoniidae
Haminoeidae
19
19
19
11
Marginellidae
Granulina ovuliformis
Retusidae
Turridae
19
19
8
Pelecypoda
Cuspidariidae
19
19
76
38
76
46
Lucinidae
38
8
Nuculidae
172
249
268
287
249
245
Nuculanidae
19
19
8
Solemyacidae
Thyasiridae
Volrulella Dersimilis
96
76
210
172
111
Scaphqpoda
Dentaliidae
19
38
11
S iphonodental iidae
19
4
Annelida
Oligochaeta
38
3S
57
57
38
Polychaeta
Aqpharetidae
191
19
76
19
57
72
Tsolda pilchella
115
38
31
Isolda sp.
19
325
69
Capital 1 JiiM
19
76
115
172
76
drzatulidae
96
325
191
134
803
310
_DccrvillftidBe
38
8
Flabelligeridae
19
4
Ganiadidae
19
4
Glyoeridae
38
8
Hesicriiftftp
19
4
Luntorineridae
38
19
11
sp.
19
19
57
38
27
-------
Table &-8. (Oantinued)
Fhylun
Class
Subclass
Order
Family Reel icate/ (Organisms/m2) Mean Abundance
Genus Species 1 2 3 4 5 (Oraanisns/nt2)
Magelonidae
19
4
Maldanidae
76
38
19
19
30
Nephtyidae
Nechtvs sp.
19
96
23
Nereidae
19
4
Orruphidae
38
19
57
19
27
Opheliidae
38
19
11
Orbiniidae
134
134
382
96
115
172
Paraonidae
Aricide? sp-
115
115
153
191
19
119
Polynoidae
19
4
Sabellidae
19
4
Spicrddae
19
4
Pri
-------
Table B-8. (Continued)
Fhylum
Class
Subclass
Order
Family
Genus Species
Replicate/ (OrganisnE/m2) Mean Abundance
1 2 3 4 5 (Oroanisms/m2^
Rvoooooephalidae (dam.)
Haroinia sp. A
Haminia spp.
Paraphoxus sp.
Stegooehalidae
steoooeohaloides sp.
Syncpiidae
Svrrhoe sp.
CXmaoea
Bodotriidae
Cvclaspis sp. A
Diastylidae
PiflgtYliS sp.
Unidentified genus A
Leuccnidae
Eudorella sp.
Leuoon sp.
Nannastacidae
Canpvlaspis sp. B
Isopoda
Anthuridae
Cirolanidae
Ctnilera cvlindraoea
DesnoGcnidae
Desnoscroa sp.
Giiathiidae
Cftattlia sp-
Mysidiaaaa
Taraidaoea
Apseudidae
toseudes sp.
Paratanaidae
Spbyrapiilae
atiynpg sp-
Ostracoda
Pycnogcnida
Nyi^iicriidae
EYlTtaO sp.
38
19
19
19
19
38
57
19
19
38
38
38
38
19
38
57
76
57
38
19
57
38
19
19
19
38
19
19
19
19
38
96
19
19
76 134
19 19
38
19
96
19
38
19
19
4
8
11
4
8
15
4
4
69
8
38
4
15
15
54
4
11
30
15
4
19
-------
Table B-8. (Continued)
Hiylum
Class
Subclass
Order
Family Replicate/fOrganisms/m2) Mean Abundance
SSIUS-SES^K— 1 2 2 4 5 fOroanisns/m2)
EcJunodernata
Ophiuroidea 57 11
Air^hiuridae 19 57 19 19 23
Ophiuridae 76 57 57 38
Totals 4698 5234 7050 5388 6936 5867
Number of Species 39 34 32 41 41 79
Shannon-Weaver Diversity
3.41 3.22 2.69 3.45 3.07
3.42
-------
Table B-9. Macro infauna Oollectod at Station M-8, Miami Harbor Interim
0CMD6 Study Area.
Fftylura
Class
Subclass
Order
Family Replicate/ (Ortaanisms/rc2) Mean Abundance
Cnidaria
? .
(un-ieuu-sj;
Hydrozoa
19
4
Porifera
Unidentified sp. A
96
38
115
50
Rhynchoooela
19
4
Aschelminthes
Nematoda
76
172
344
134
860
317
Mollusca
Cephalopoda
Sepiolidae
Gastropoda
Columbellidae
19
19
38
115
38
Glycymeridae
19
4
Haminoeidae
19
19
8
Marginellidae
Granulina cvuliformis
Retusidae
19
4
Rissoidae
19
38
11
Pelecypoda
Cuspidariidae
19 .
4
Muculidae
38
96
344
.631
134
249
Nuculanidae
38
38
15
T.imaninidae
Limacina inflata
19
19
8
Lucinidae
210
42
Scsnelidae
Tftyasiridae
38
172
191
96
99
Volrulella rarsimilis
172
34
Veneridae
57
11
Scaphopoda
Dental iidae
19
153
34
Siphfncxlental i idafi
38
38
38
57
34
Annelida
Polychaeta
57
11
Arpharetidae
76
57
27
Isolds pulchella
19
172
497
138
IsQld^ sp.
153
31
Capital 1idrte
57
134
38
46
Cirratulidae
287
96
96
172
325
195
Glyceridae
38
19
11
-------
Table &-9- (Continued)
Fftylum
Class
Subclass
Order
Family
Genus Species
¦Reelicate/(Oroanisms/m2 ^
-1 2 3 4 5
Mean Abundance
forganisms/m2)
Goniadidae
19
4
Lumbrineridae
Luntorineris sd.
19
134
19
38
42
Magelcnidae
Maaelona so.
19
4
Maldanidae
19
4
Nephtyidae
19
76
19
NephtY5 sp.
38
76
19
27
Cnuphidae
19
4
Opheliidae
19
4
Ppheiina sp.
57
19
15
Orbiniidae
76
57
631
631
76
294
Paracnidae
Aricidea sd.
19
38
57
38
134
57
Spionidae
19
4
Prianosoio so.
38
134
287
229
38
145
Syllidae
38
8
Sipuncula
Golfinqiidae
19
4
Arthropoda
Crustaoea
Malaoostraca
Acphipoda
Aeginellidae
sp-
Anpeliscidae
Airoelisca
Haplocro sp. B
Aoridae
Unciol* SSX2
GamoaridBB
HyperiidM
Tpata-imn
Lysianassidae
Hi|i»iwtn sp.
Oedicerrtidhe
Unidentified sp. A
Paradaliacditae
Harpinia sp. B
H^iirinitf **>•
38
306 3499 4379
38
19
19
38
19
19
19
19
19
38
19
19
19
38
19
38
19
57
1652
8
4
4
15
8
4
4
30
4
-------
Table B-9. (Qontlmed)
Hiylum
Class
Subclass
Order
Family Replicate/ (Orqanisns/nt2^ Mean Aburriance
GfflU? Spegjes 1 2 3 4 5 fOmanisns/m2^
Synopiidae
Svrrtioe sp. 57 19 15
Cumaaea
Leucxnidae
Euriorella sp. 76 76 19 34
Nannastacidae
CgFPYlaSPiS sp. A 19 4
Cairovlasois sp. B 19 19 8
amella 6p. B 19 4
Presarrylflspjg sp. 19 19 38 15
Isopcda
Cirolanidae
Conllera cvlindraoea 38 8
Gnathiidae
Gnathla sp. 57 57 IS 27
Tanaidaoea
Leptognathiidae
Laptoanathia sp. 19 4
Paratariaidae 19 38 11
Sphyrapidae
Sahvracus sp. 19 4
Ostracoda
Myodooopida
Asteropidae 38 8
HiUcraedidae
Hart>arwp rerreictelfltu? 115 23
Padooopida
Cytherellidae 19 19 8
Paracyprididae 19 19 8
Ophiuroidea
Ariphiuri*e 19 4
OphiuridBB 57 38 38 38 34
Pycnoqcnida
Anootheiik*
tiStfiEBCOQilifl sp. 19 4
-------
Table B-9. (Oontimad)
Fhylum
Class
Subclass
Order
Family
Repl icate/ (Ornanisms/m2) Mean Abundance
Chordata
Ascidiacea
Unidentified juvenile
19
4
Totals
914 1852
6439
7528
3456
4044
Number of Species
19 26
34
37
35
74
Shanncn-Weaver Diversity
3.64 4.19 2.83 2.69 4.05
3.80
-------
Table &-10. Macroinfauna Collected at Staticn M-9, Hiami Hartoor Interim
0CMD6 Study Area.
Fhylum
Class
Subclass
Order
Family
Genus Species
Replicate/(Organisms/m2!
1 2 3 4 5
Mean Abundance
fOrctaiusng/TTi^
Cnidaria
Arrthozoa
Actiriiaria
Pliynchocoela
Aschelmirrthes
19
19
Nematoda
841
401
19
96
860
443
Mollusca
Aplacophora
19
19
19
11
Cephalopoda
Sepiolidae
Gastropoda
Atlarttidae
19
4
Colunbellidae
76
57
38
34
Glycymeridae
19
4
Haminoeidae
38
19
11
Retusidae
Rissoidae
38
19
11
Pelecypoda
Cuspidariidae
134
38
38
42
Nuculidae
38
96
27
Limacinickke
Limacina inflate
19
4
Lucinidae
38
8
Anodantia alist
19
4
Thyasiridne
363
765
38
19
268
291
Verier idae
38
8
Vitr inellidae
38
19
19
15
Scaphopoda
Dental iidae
19
38
19
57
27
Siphcnodentaliidaft
38
19
11
Annelida
Oligochaeta
57
11
Polychaeta
Aqpharetidae
19
4
capitellidtoc
37
11
drratajl idae
1128
669
38
57
937
566
Glyaeridae
19
4
Gcniadidae
19
19
8
IxmbrxnexiAse
38
8
Iirifcrinaris so.
57
96
19
34
-------
Table B-10. (Continued)
Riylum
Class
Subclass
Order
Family Replicate/(Organisms/m2) Mean Abundance
Genus Species 1 2 3 4 5 (Oroanisms/m2)
Maldanidae 19 19 8
Opheliidae
Oohelina sp. 19 38 11
Orbiniidae 115 57 19 96 19 61
Paraonidae
Aricidea sp. 96 19 19 325 92
Fhyllodocidae
Rwllodooe sp. 19 4
Pilargiidae 19 4
Spicriidae 19 4
PrionoGPio sp. 134 96 76 115 84
Sipuncula 38 8
Golfingiidae
Arthropoda
Crustaoea
Malaoo6traca
Anphipoda
Anpeliscidae
Ancelisca aoassizi 76 38 57 34
Hyperiidae
19 4
TffjtnqpT"" scftizwenra is 4
Lysianassidae
Hinxjnedcn sp. 19 4
Oedicerotidae 38 76 23
Unidentified sp. A 38 38 15
Unidentified sp. B 19 19 19 11
unidentified sp. C 19 4
Partial isddae 57 38 19
RKBtDoepbalidae
ap. B 19 38 19 19 19
Rirosinicte
Primp icfcmcnl 19 4
ScinidM
f^Hnia rnp. 19 4
19 4
Syncpiida®
Svrrftoe 9p.
Cunaaea
DiastyliAw
sp. 19 38 11
-------
Table B-10. (Continued)
Fhylura
Class
Subclass
Order
Family
Reolicate/ fOmanisms/m2'
Mean Abundance
Genus Species
1
2
3 4
5
(Oroanisne/m2)
Leuconidae
Eudorella so.
38
19
57
23
Nannastacidae
CaircvlasDis so. B
19
19
8
Decapoda
Dorippidae
Clvthocerus so.
19
4
Isopoda
Gnathiidae
Gnathia so.
19
4
Tanaidacea
Paratanaidae
19
19
19
11
Ostracoda
Myodocopida
Halocyprididae
Unidentified genus A
19
4
Unidentified genus C
19
4
Fhilaredidae
19
4
Harbartsus paucichelatus
19
4
Sarsiellidae
Sarsiella so.
19
4
Rriooopida
Paracyprididae
19
4
Echinoderrnata
Ophiuroidea
57
19
19
19
Ophiuridae
19
4
Totals
3820
3570
553 1144 3573
2536
Number of Species
29
33
14 23
34
66
Shannon-Weaver Diversity
3.38
3.78
3.44 3.97 3
.51
4.08
-------
APPENDIX B
EVALUATION OF THE DISPERSION CHARACTERISTICS OF THE MIAMI
AND FORT PIERCE DREDGED MATERIAL SITES
PREFACE
This Appendix contains the report by Scheffner and Swain of the Coastal Engineering Research Center
and a supplementary letter by Scheffiier presenting results for a sediment distribution representative of
sediment from Miami Harbor The report contains results for a sediment distribution representative of
the Miami Channel.
Since the completion of the both the report and supplementary letter, it was discovered that incorrect
units for the suspended sediment concentrations were presented. Concentrations were given in mg/1
whereas the concentrations were actually volummetric void ratios. To convert the volummetric void
ratios to concentrations, the values must be multiplied by the particle density (2 65g/cc) The values in
Figures 2 6 and 2 10 and Tables 2 4 and 2.5 of the report and the table in the supplementary letter need
to be multiplied by 2 65x10s to represent concentrations in mg/1 Table 2.4 and the table in the
supplementary letter are reproduced with modified values below
Table 2.4 (modified)
Summary of Computed Suspended Sill, and Clav Concentration
^Concentration in mg/1 above ambient)
Elapsed Time (sec) I Approximate Distance from Dredge (Miles)
Depth
1500
3000
4500
6000
(ft)
0.8
1 6
2.3
3.2
200
0.000000318
1 7755
4 505
2.65
250
0 018815
11.395
6.625
2.438
300
14.575
23.055
5 83
1.749
350
151.05
15 37
2.915
1.007
400
39 75
6 36
1.8285
0.689
Summary of Computed Maximum Suspended Silt and Clav Conce Oration
(Concentration in mg/1 above ambient)
Elapsed Time (sec) / Approximate Distance from C'redge (Miles)
Depth
1500
3000
4500
6000
(ft)
0 8
1 6
2 3
3 2
200
0 0000053
9 01
20 405
10 865
250
0 17755
53
29 15
10 335
300
87 45
103 35
24 91
7,42
350
715 5
68 9
13 515
4 24
400
193 45
26 5
7 95
2915
-------
EVALUATION OF THE DISPERSION CHARACTERISTICS
OF THE MIAMI AND FORT PIERCE
DREDGED MATERIAL DISPOSAL SITES
by
Norman U. Scheffner
and
Abhiaanyu Swain
Coastal Engineering Research Center
April 1989
Final Report.
Prepared for
US Army Engineer District, Jacksonville
Jacksonville, Florida 32232-0019
-------
PREFACE
This report describes a comprehensive approach for evaluating the
environmental suitability of proposed open water disposal sites for dredged
material. Two proposed Florida disposal sites are evaluated in this investi-
gation, one off the coast of Miami and one off the coast of Fort Pierce. The
purpose of the evaluation is to determine whether either site poses a contami-
nation threat to sensitive nearshore coral reefs. Two criteria are necessary
of a site if it is to be approved as environmentally acceptable. The first is
concerned with the immediate effects of the disposal operation, material from
the descending plume of sediments can not contaminate areas outside the
designated disposal site. This short-term phase analysis represents several
minutes to several hours following the initial release of material from the
dredge. The second phase of investigation determines whether material
deposited within the disposal site can be eroded and subsequently transported
out of the site by either local current fields or by storm conditions. This
long-term phase examines mound stability for periods of time up to one year
following the disposal operation.
A two-phase numerical modeling methodology was selected for this
investigation. The approach utilizes the Disposal From an Instantaneous Dump
(DIFID) model for calculating the short-term fate and a coupled hydrodynamic/
sediment transport model for computing the long-term fate of the disposed
material. The project was authorized and funded by the US Army Engineer
District, Jacksonville (SAJ), under the project management of Mr. Ronald Tapp
and Ms. Elizabeth Rhodes and under the general direction of Mr. A. J. Salem.
Much of the prototype data required for numerical model input were
provided by or extracted from research publications of Dr. T. N. Lee, School
of Marine and Atmospheric Science, Division of Meteorology and Physical
Oceanography, University of Miami, Florida. Supplementary velocity
measurement data were also obtained from other sources. The study was
conducted at the US Army Engineer Waterways Experiment Station's (WES) Coastal
Engineering Research Center (CERC). The numerical investigation was
completed, and this report prepared by Drs. Norman U. Scheffner and A. Swain.
Providing general supervision were Dr. James R. Houston and Mr. Charles C.
Calhoun, Jr., Chief and Assistant Chief, respectively, CERC; direct supervisior
1
-------
the proiect was provided bv Mr u i a
y "r » L. Butler, chief of the Research Division
and Mr Bruce A. Eb.r.oU, Chief of the Coastal Processes Branch of th.
Research Division. Commander and Director of WES during the course of this
study and che preparation and Dublleatinn nf »-u«
UQ puoiicacion ot this report was COL Dwayne G.
Lee, CE. Technical Director was I)jr. Robert. V. Whalin
2
-------
CONTENTS
Page
PREFACE ]
INTRODUCTION 6
Background and Objective 6
Scope of Report 1C
PART I: LITERATURE REVIEW 12
The Gulf Stream 12
Gulf Stream Meanders 1£
Spin-off Eddies 2C
Prototype Velocity Data 2]
Depth Averaged Velocity 22
Velocity Field Input Data 36
Upwelling and Dovmwelling 37
PART II: THE SHORT-TERM SIMULATION OF DISPOSAL OPERATIONS 3S
Input Data Requirement 4C
Method and Procedure for Short-Term Model Simulations 4^
Miami Disposal Site 4S
Fort Pierce Disposal Site 52
PART III: THE SIMULATION OF LONG-TERM DISPOSAL FATE 56
Sediment Transport 57
Velocity Field Distribution 6£
Sediment Transport Due to Non-Storm Velocity Fields 62
Fort Pierce 63
Miami 69
PART IV: CONCLUSION 74
REFERENCES 75
3
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LIST OF TABLES
No . Pap.e
1.1 Disposal Sice Characteristics for Miami and Fort Pierce 11
1.2 Basic Dimensions of the Gulf Stream Meanders 20
1.5 Current Meter Locations and Depth Averaged Velocities 28
1.6 Velocity Distribution Offshore of Miami 34
1.7 Velocity Distribution Offshore of Fort Pierce 34
1.8 Summary of Upwelling Related Velocity Calculations
(Osgpod et al. 1987) 38
2.1 Instantaneous Dredge Capacities and Dimensions 42
2.2 Characterization of Dredged Material for Miami and Fort Pierce . . 43
2.3 Input Data Related to Disposal Operation for the Miami and Fort
Pierce ODMDS 44
2.4 Summary of Computed Maximum Suspended Silt and Clay Concentration
(Concentration in rag/1 above ambient) 51
2.5 Summary of Computed Maximum Suspended Sediment Concentration
(Concentration in rag/1 above ambient) 53
LIST OF FIGURES
NcL_ Pa&e
1.1 Location of ODMDS, bathymetry map, and coral reefs for the Miami.
site . : 7
1.2 Location of ODMDS, bathymetry map, and coral reefsfor the Fort
Pierce site 8
1.3. A schematic diagram of the origin of the Gulf Stream Gurrent
(after Sverdrup, JOhnson, Flemming, and Stommel 1965) 13
1.4. Satellite-derived path of the Gulf Stream (NOAA 1983) 15
1.5. Mean position and meander deviation of the Gulf Stream surface
(Bane and Brooks 1979) 18
1.6. Example of the propagation of Gulf Stream meanders at
quarter - period snapshots (Bane 1983) 19
1.7. Current meter locations for Miami (Lee, Brooks, and Duing 1977) . . 24
1.8. Current meter locations for Fort Pierce (Lee, Brooks, and Duing
1977) ' 25
1.9. Measured velocity profiles offshore of Miami 26
1.10 Measured velocity profiles offshore of Fort Pierce 27
1.11. Depth-averaged current vectors from Miami to Fort Pierce 32
1.12. Depth-averaged current vectors north of Fort Pierce 33
1.13. Velocity vector distribution offshore of Miami 35
1.14 Velocity vector distribution offshore of Fort Pierce 35
2.1. Computational phases of the DIFID model (from Brandsma and Divorky,
1976) 41
2.2 Suspended sediment cloud at 200 ft deep at 1500 sec after dump . . 47
2.3 Suspended sediment cloud at 200 ft deep at 3000 sec after dump 47
2.4 Suspended sediment cloud at 200 ft deep at 4500 sec after dump . . 48
2.5 Suspended sediment cloud at 200 ft deep at 6000 sec after dump ... 48
4
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No Pa g
2 6 Time - concentration for Miami at 200, 250, 300, 350, and 400 ft. , . 5
2 7 Deposition pattern for the Miami site 5
2.8 Three-dimensional view of the Miami site disposal mound 5
2.9 Contour plot of the deposition pattern for the Miami site 5
2.10 Time-concentration for Fort Pierce at 10, 20, 30, 40, and 50 ft . . 5
2.11 Deposition pattern for the Fort Pierce site 5
2.12 Three-dimensional view of the Fort Pierce site disposal mound ... 5
2.12 Contour plot of the deposition pattern for the Fort Pierce site . . 5
3.1 Sediment transport vs velocity - Miami disposaL site 5
3.2 Sediment transport vs velocity - Fort Pierce disposal site .... 5
3.3 WIS station 163 wave characteristic summary for the Miami site . . 5
3.4 WIS station 153 wave characteristic summary for the Fort Pierce
site .
3.5 Velocity vectors around an idealized disposal mound 6
3.6 Gradation curve of Fort Pierce sediment 6
3.7 Initial mound configuration for Fort Pierce £
3.8 Fort Pierce mound configuration at 6 months 6
3.9 Final Fort Pierce mound configuration at 12 months 6
3.10 Time history of long-term erosion of the Fort Pierce mound 6
3.11 Final (24 hr) Fort Pierce storm mound configuration 6
3.12 Time history of storm erosion of Fort Pierce mound 6
3.13 Initial mound configuration for Miami "6
3.14 Final Miami mound configuration at 3 months 7
3.15 Time history of long-term erosion of the Miami mound 7
3.16 Final (24 hr) Fort Pierce storm mound configuration 7
3.17 Time history of storm erosion of Miami raound 7
5
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evaluation OF THE DISPFRSTQN characteristics
OF THE MIAMI AND FORT PIERCE
DREDGED MATERIAL DISPOSAL SITES
INTRODUCTION
Background and Objective
1. Dredging of estuaries, bays, harbors, and coastal inlets in the
United States is often required in order to maintain minimum navigation
depths. The selection of an environmentally acceptable disposal site for this
dredged material requires some means of predicting the effects of the disposal
operation on the coastal and inland water environment. One means of predic-
tion is the utilization of numerical models capable of simulating the short-
and long-term diffusion and transport of dredged material from the disposal
site.
2. The Corps of Engineers have become increasingly active in the area
of maintenance dredging of harbor channels and coastal inlets. The
designation of acceptable disposal sites for this material-is, however,
becoming increasingly difficult. Open water disposal sites are often selected
as a means of minimizing any adverse effects resulting from the disposal of
material in the vicinity of the dredging operation. This approach is accept-
able if the designated site is far enough removed from any environmentally
sensitive area that material at the site will remain at the site and not
represent a possible source of contamination.
3. The Planning Division, US Army Engineer District, Jacksonville
(SAJ), is preparing an Environmental Impact Statement (EIS) for submission to
the US Environmental Protection Agency (EPA). The purpose of the EIS is to
evaluate the environmental impact of dredged material disposed at the proposed
Ocean Dredged Material Disposal Sites (ODMDS) offshore of Miami and Fort Pierce,
Florida. The location and bathymetries of these .sites are shown in Figures 1.1
and 1.2.
6
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Government Cut
OOMOS
Coral R*«f«
STATUTE MILES
NAUTICAL WILES 8|
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GENERAL LOCATION WAP
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25"45'00
2 S 44-45
25 44 30"
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NAUTICAL Mll£S
BATHYMETRIC MAP
Oceon Dredged Moteriol Disposal Site Miorni,Florida.
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¦ The EPA has expressed a concern regarding the fate of the disposed
materials at both proposed ODMDS. It is feared that discharged sediments frc
either disposal site may be carried by the Gulf Stream and its spin-off eddie
onto sensitive shore-parallel coral reefs located approximately 1 mile off-
shore of the barrier islands. In addition to sediment transported by eddies
and ambient currents, the possibility of resuspension and subsequent transpor
of material from the disposal site during storm events is also an expressed
concern.
5. The SAJ requested the US Army Engineer Waterways Experiment
Station's (WES) Coastal Engineering Research Center (CERC) to perform a
technical study of the Gulf Stream, the spin-off eddies, and other relevant
environmental forces, with respect to the potentials for reef contamination b
dredged material originating from either proposed ODMDS. The CERC was first
requested to study the acceptability of the proposed sites offshore of Miami
and Fort Pierce. If these sites are not found to be environmentally
acceptable, the first acceptable offshore location which does not pose a
contamination threat to the reefs should be identified.
6. A preliminary technical review was performtid by the CERC (MFR,
9 February 1988) of the available literature provided by SAJ (Memorandum,
4 December 1987). The review concluded that a detailed disposal site evalua-
tion should be performed in order to determine whether velocities in the Gulf
Stream and its spin-off eddies are sufficient in magnitude to transport
disposed material from the proposed ODMDS onto the coral reefs.
7. The study reported here uses a numerical modeling approach for
estimating both short-term and long-term fate of dredged material disposed at
a proposed ODMDS. The modeling of the short-term diuaving operation is
performed by the Disposal From an Instantaneous Dump [DIFID) model (Johnson
et al. 1988). Long-term simulations, using a newly teveloped coupled
hydrodynamic/sediment transport model (Scheffner 1981) , use depth averaged
velocity fields to determine whether non-storm related currents are capable o]
transporting sediments outside of the designated 0DMD3 over long periods of
time following the initial deposition. The effects o! storm erosion are
separately examined with the model by simulating the passage of a storm surge
over the site.
9
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Scope of Report
8. The purpose of this study is to evaluate the dispersion character-
istics of the proposed disposal sites offshore of Miami arid Fort Pierce.
These two sites were selected as representative of the two primary
environments found off the east coast of Florida. The first is typified by
the proposed Miami site at which the bathymetry is complex, the water is deep
(greater than 500 ft), and the site is directly influenced by the Gulf Stream
and its spin-off eddies. Due to the close prqximity of the Gulf Stream to the
disposal site, it is feared that disposed sediments may be carried onto the
coral reefs by spin-off eddies shed by the Gulf Stream.
9. In contrast to the Miami site, the Fort Pierce disposal site is
removed from the direct effects of the Gulf Stream, is situated on a broad,
gently sloping shelf, and is located in shallow water (less than 75 ft). This
ODMDS has a small cross-sectional area of flow compared to that of the Miami
site. A comparison of the site characteristics of both the Miami and
Fort Pierce ODMDS is given in Table 1.1.
10. This investigation will classify each of the proposed disposal sites
as either dispersive of non-dispersive according to whether the local current
fields are capable of transporting material fron the disposal site onto the
reef area. This approach requires documenting the local velocities, at each
site in order to identify a reef-directed component which may be attributed to
the Gulf Stream. This component will be used to compute a sediment transport
rate and direction for use in evaluating the possibility of disposal site
related reef contamination. The following section represents the result of an
extensive literature review which begins with a description of the Gulf Stream
and its major characteristics. This portion of the review is included to
verify that shoreward directed spinoff eddies do exist and should be inves-
tigated as a possible source of sediment transport. This background d>cumen-
tation will be followed by a quantification of velocity magnitudes and
directions which are shown to be representative of each site. These
velocities will then be used as model input for the short- and long-teirm
stability analyses of Parts II and III.
10
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Table 1.1
Disposal Site Characteriseics for Miami and Fort Pierce
Characteristics
Miami
Fort Pierce
Vater depth
Greater than 500 ft
Less than 75 ft
Bottom slope
Steep (0.02-0.05)
Mild (0.001-0.002)
Topography
Complex (nonlinear)
Simple (linear)
Terrace
Miami Terrace confined
to a 2 mile offshore zone
No terrace zone
Flow cross-
section of
ODHDS
About 3,168,000 sq ft
About 294,000 sq ft
Continental
Margin
Wide
Narrow
Continental
Contains inner, mid, and
and outer shelf with sharp
shelf break.
Contains inner shelf
only
Direction of
Velocity
Westerly and northerly
Northerly
Magnitude of
velocities:
westerly
northerly
0.15-1.5 ft/sec
0.7-3.5ft/sec
0.05-0.5ft/sec
0.20-1.5ft/sec
Average axis of
Gulf Stream
15 miles offshore
80 miles offshore
Coastal currents
are primarily
driven by
Gulf Stream
Wind and tidal forcing
Gulf Stream
Effects
Present
Free
Dredged
materials
90% sand (fine
to medium)
90% sand (fine
to medium)
10% clay
10% clay
11
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part i: literature review
The Gulf Stream
11. The objective of the literature review is to identify the primary
characteristics of the Gulf Stream and quantify Its basic structure,
magnitude, and limits of influence along the south and southeast coast of the
United States. A brief summary of the origin and dynamics of the Gulf Stream
is presented in this section as a preliminary background for the present ODMDS
selection study as well as for future site selection studies. The terms Gulf
Stream or stream are used throughout this section of the report to refer to
the entire current system off the south and east coast of the United States,
including the Florida Current.
12. Figure 1.3 presents a schematic diagram of the dominant currents
and current induced secondary circulation patterns off the east coast of the
United States. The origin of the Gulf Stream begins as the Atlantic and North
Equatorial Current systems combine with the South Equatorial and Guyana
Current systems. This combined flow discharges through the Caribbean Sea
and Yucatan Channel into the southeastern portion of the Gulf of Mexico.
Because the waters are colder than the surrounding Gulf of Mexico, a density
differential is created which results in a deflection of the current from the
Gulf of Mexico toward the Straights of Florida. This density driven flow is
most pronounced during winter months. During this time, the current is often
sharply deflected from the Yucatan Channel through the Straights of Florida
as shown in Figure 1.3. However, the loop current can extend well into the
Gulf of Mexico during the summer months (Leipper 1967). Regardless of the
specific path, the current enters the Straights of Florida in nearly the' same
temperature, salinity, and density as when it entered the Caribbean Sea
(Lee, et al. 1977).
13. The dynamics of the Gulf Stream are driven by the large tides of
the Caribbean Sea which dominate the smaller tides of the Gulf of Mexico.
These large tides force water through the long channel between the Florida
Peninsula and the islands of Cuba and the Bahamas, developing a water level
differential of about 2/3 ft (Stommel 1965) between the Gulf of Mexico and
12
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-------
the Atlantic Ocean. As the current flows through the Straights of Florida
toward Miami, the axis of flow makes an abrupt 90 degree turn to the north and
enters the continental shelf channel. The approximate point of deflection is
indicated as position A in Figure 1.3. The cross-sectional area occupied by
the stream undergoes a change from approximately 90 miles wide and 1 mile deep
at Key West to approximately 50 miles wide and 0.5 miles deep in the vicinity
of Miami. This reduction in flow area causes an increase in stream velocity
with an accompanying decrease in free surface water level between Key West and
Miami.
14. The Gulf Stream continues along the south and southeast coast of
the United States as shown in Figure 1.3. It is seen that the stream hugs the
continental shelf from the deep water region offshore of Miami, north to
shallow water depths of less than 100 m at Cape Canaveral. Beyond Cape
Canaveral, the stream is diverted into deeper water in the vicinity of the
Charleston bump (Brooks and Bane, 1978; Legeckis 1979), a topography anomaly
in the continental shelf slope between the 200 and 600 m isobaths. North of
the bump, the stream moves back onshore into waters of about 300 a. This
onshore shift o£ the current is primarily due to a steady Increase in bottom
slope north of Charleston. This increasing slopq, coupled with ridge and
trough bottom features, prevalent strong northwest winds, and barocllnic
instabilities cause the stream to subsequently deflect off the continental
shelf and become confined to a path between the 300 m and 400 m isobaths.
Position B in Figure 1.3 Indicates the approximate location of the offshore
point of deflection.
15. The lateral extent of the width of the stream about its average
axis is shown in Figure 1.4. This figure, obtained from the National Oceanic
and Atmospheric Administration's (NOAA) field station at Miami and reproduced
in the Journal of Geophysical Research (1983) represents satellite imagery of
the Sea Surface Temperature (SST) structure of the Gulf Stream. The figure
demonstrates the variability in width of influence of the Gulf Stream about
its mean axis. The following section will investigate the spatial and
temporal characteristics of the Gulf Stream.
14
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jr
Figure 1 U Satellite-derived path of tho Gulf Stream (NOAA 1983)
15
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Culf Stream Meanders
16. The Gulf Stream is a high velocity thermal current which flows
along the outer continental shelf. The time-dependent structure of the stream
is a function of a combination of forces including the current distribution,
bottfom topography, wind stress, entrainment of fluid from below the free
surface, and rotational forces developed due to the rotation of the earth.
The constantly changing spatial and temporal structure of the streaa has been
widely studied and documented in the literature. Although an attempt to
quantify these dynamics are beyond the scope o£ this report, many of the
references used in this literature review to document the characteristics of
the Gulf Stream have been included in the list of references. Since this
report is intended to determine whether the Gulf Stream can adversely affect
either of the two proposed disposal sites, this section begins with a
description of commonly observed features which may directly impact either
ODMDS.
17. The high velocity main body of the Gulf Streaa propagates in wave
like patterns referred to as meanders. The dynaaic features are'a result of
forces such as shearing Instabilities of the stream, geostrophic imbalances,
the transfer of kinetic energy to the mean flow, the passage of cold fronts,
the random passage of wind events, etc. Although the mean axis of the stream
propagates to the north, these forcings can produce localized undulations
about the mean axis which can locally flow either upstream (southerly),
downstream (northerly), onshore or offshore.
18. Many documenting measurements quantifying the spatial variation of
meanders have been reported. Duing (1975) obtained 2 weeks of current profile
measurements off the coast of Miami and identified a current meander with a
^*-6 day period which was propagating to the north at approximately 45 cm/sec
with a wave length of nearly 200 km. Duing's data showed that when the lxis
of the Gulf Stream was displaced offshore, southerly flows occurred over
portions of the Miami terrace. Conversely, when the axis of the stream vas
displaced onshore, flows over the terrace were directed to the north. Thermal
gradients can be used to measure the primary features of meanders as they grow
in size or become skewed. Lee and Moore (1977), for example, have correlated
the distribution of meanders with the propagation of SST derived isotherms.
16
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19. Meanders of the scream are commonly observed between Jupiter Inlet
and Cape Hatteras where the stream enters the wide continental shelf region
after passing through the topographic constriction formed by the Florida coast
and the Little Bahama bank. This discharge of water from a confined to an
unconfined area results in meanders in the stream axis which are no longer
primarily controlled by the continental shelf bathymetry (Lee et al 1981) but
are strongly influenced by weather patterns, long waves from the deep sea,
tidal forcing, and local wind fields Northeast of Cape Hatteras, the Gulf
Stream moves beyond our area ,of interest into deep water where they are no
longer controlled by continental shelf bathymetry.
20. The meandering process is well illustrated in an example presented
by Bane and Brooks (1979) and Bane (1983), shown in Figures 1.5 and 1 6. In
Figure 1.5, a 64-week period of SST data are used to show the shoreward and
seaward envelope of occupation of the Gulf Stream in relation to the location
of the time - averaged mean axis shown by the dashed line. Figures 1.6 uses
quarter-period (16-week) incremental plots of the axis to illustrates how two
typical meanders (labeled A and B) occupy the shaded limits of the stream as
they propagate northward. Table 1.2 lists the basic dimensions of meanders
typical of those documented along the south and southeast coasts of Florida.
17
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200
200 km
Figure 1.5. Mean position and meander deviation of the Gulf Stream surface
(Bane and Brooks 1979)
18
-------
700
V
200
TOO rn
WOO
700
200 m
700
Figure 1.6. Example of the propagation of Gulf Stream meanders at
quarter-period snapshots (Bane 1983)
19
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Table 1.2
Basic Dimensions of the Gulf Stream Meanders
Wave length (longitudinal)
Lateral displacement (east-west)
Average velocity of propagation
Maximum downstream current speed recorded
Features
Dimensions
90 - 260 km
1 - 100 km
47 cm/sec
134 cm/sec
Results of this investigation have shown that much of the Continental Shelf
area south of Cape Hatteras is subject to the direct influence of the Gulf
Stream. Nearshore areas can also be affected by the Gulf Stream even though
the area in question may not be directly impacted by the envelope of meanders.
The following section will address Gulf Stream eddies in order quantify their
potential impact on the proposed Miami and Fort Pierce disposal sites.
21. The movement of the Gulf Stream through the continental shelf often
creates rotational patterns which propagate away from the main body of the
Stream, These patterns generally represent unstable meanders which have
become detached from the main body of the stream. This can occur if the
meander becomes too pronounced or deviates too far from the main axis of flow,
in which case , detachment into the low velocity ambient current can be caused
by topography anomalies, wind fields, or barotropic Instabilities. These
detached secondary currents are referred to as spin-off eddies and are
commonly observed in the shallow slope and terrace waters (40-80 a) off the
coast of Florida. The following sections describe some of their basic
characteristics.
22. Richardson (1985) identifies three distinct zones of the Gulf
Stream. These are the clockwise rotating onshore eddy, the axis or main body
of the Stream, and the counterclockwise rotating offshore eddy. The high
velocity axis of the Gulf Stream acts as a barrier separating the onshore and
offshore regions. Depending on the environmental conditions, detached onshore
eddies can propagate to the north, shoreward, or to the south with short-lived
Spin-off Eddies
20
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periods ranging from 2 days Co 2 weeks. Eddy diameters range from 10 to 30 k
and can extend from the surface to a depth of approximately 200 m (Lee and
Mayer 1977). Detached eddies have been observed to propagate with surface
velocities ranging from 20 to 100 co/sec
23. The above sections of this report have documented the dynamic
properties of the Gulf Stream and its spin-off eddies. The data presented
indicate that, at times, the Gulf Stream does generate, or contribute to,
shoreward directed velocity fields which may affect either or both of the
proposed disposal sites. Thfe effects can be compounded when coupled with
shoreward-directed flood tide conditions. The magnitude of this total
shoreward directed velocity field will be determined from the available data
such that a boundary condition velocity field for each ODMDS can be defined a«
input to the short- and long-term sediment transport calculations. The
following sections describe the selection of a maximum shoreward-directed
velocity for each of the designated sites based on available prototype data.
Prototype Velocity Data
2U. The site designation approach utilizes sediment transport theory
and numerical modeling techniques to determine possible magnitudes of erosion
and/or transport of sediment from a specified disposal site. The computation:
are based on a specific depth and background velocity field for each site
which will be documented to be representative of the location. The site
evaluation approach is inherently conservative in that a constant, maximum-
valued, reef-directed velocity is selected as a boundary condition for
sediment transport calculations. In reality, the velocity field is continu-
ously fluctuating as a function of tides, wind fields, waves, the Gulf Stream,
etc.; therefore, no single representative value is truly descriptive of any
-location. Also, two measuring periods would yield two different values;
however, when the length of data is sufficiently long, the two computations
should not vary significantly in magnitude. Data which cover sufficiently
long periods of time to satisfy these criteria will be used in determining
appropriate boundary conditions.
25. Since maximum values are to be selected, the degree of accuracy
achieved by this approach is considered adequate as a basis for reliable
21
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predictions of the dispersion characteristics of a disposal site. If it can
be shown, for example, that the prototype velocity in 500 ft of water never
exceeds 30 cm/sec (or 40, or 50) and that a velocity magnitude of 100 cm/sec
is necessary for initiating and transporting sediment transport at that depth,
then the data are adequate to show that the site under investigation is non-
dispersive and will not represent a source of contamination. Severe storm
conditions are not included in this analysis since it is assumed that disposal
operations would be discontinued during storm events.
26. A large data base of published current meter data was identified
i
which was acceptable for quantifying the velocity patterns off the eastern
coast of Florida. Data included measurements at multiple depths in the water
column for various mooring string sites extending from south of Miami to north
of Fort Pierce and from less than 1 km to more than 100 km offshore. Although
the spatial distribution of data is sparse in its coverage of the disposal
site locations, the data base is adequate for determining a velocity field
which is representative of each survey area and can be used to evaluate the
transport potential of each disposal site. In the present context, adequacy
refers to data which covers a sufficient length of time and number of vertical
locations within the water column, that a reliable depth-averaged velocity can
be computed.
27. Multiple sources of acceptable velocity data were located*for
application in the present Miami and Fort Pierce disposal site study. The
following sections will use this data, in addition to other available data, to
develop a spatially consistent data base of depth averaged velocity vectors.
The intent of this multiple station analysis and inter-comparlson is to
develop velocity vectors which are consistent with surrounding data and are,
therefore, truly representative of the area.
Depth Averaged Velocity
28. The site designation approach computes short-term and long-term
potentials for sediment transport as a function of a site-specific, depth-
averaged velocity field. The depth averaged condition was selected for two
reasons. First, due to the limited time available for this study, a represen-
tative velocity field had to be defined from existing data. Available data
22
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was sufficient for determining a maximum shore-directed, depth-averaged
current but was not adequate in either duration or distribution to define any
meaningful vertical velocity distribution trend. Secondly, an "average"
vertical distribution probably does not exist, since the vertical velocity
structure shows a continuously changing current gradient due to variations in
the wave fields, salinity gradients, thermoclines, and Gulf Stream meanders.
Also, attempting to compute site-specific sediment movement as a function of a
three-dimensional velocity distribution is not feasible. For these reasons, a
depth-averaged current was selected for input to both the DIFID and long-terra
sediment models. The computation of the selected velocity field is described
in the following sections.
29. Two examples data sources are used here to demonstrate the
computation of a shoreward-directed depth-averaged velocity field. Both
sources of data are reported by Lee, Brooks, and Duing (1977). The Miami data
was collected as a portion of the SYNOPS 71 (Synoptic Observations of Profiles
in the Straights) project. The research vessels Calanus (C), Humble (H),
Pillsbury (P), and Gerda (G) simultaneously collected 16 days of vertical
profiles of horizontal velocities. These measurements were taken every*3
hours at the four locations between Miami and Bimini shown in Figure 1.7.
Ship - deployed measurement stations for the Fort Pierce area are shown in
Figure 1.8. These reported data are based on the analysis of multiple data
sets, collected at each of the data collection stations over a period-of
approximately 5.5 years.
30. Velocity measurements for the Miami transects are based on
Profiling Current Meter data (PCM). The data were reduced to u (+• to the
east) and v (+ to the north) velocity components and then averaged over 5 m
depth intervals. Details of the deployment can be found in Lee, Brooks, and
Dulng 1977, Duing and Johnson 1972 and Duing 1973. Figure 1.9 displays three
types of velocity profiles which were constructed from the velocity time
series data records for mooring sites C, H, P, arid G. These represent the
measured maximum, minimum, and mean velocity. The depth averaged value is
also indicated in the figure. The minimum u velocity (negative referring to
westward) and corresponding v component were used to compute the shore-
directed depth-averaged velocity vector indicated by the dotted line.
23
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CMAMJS
KJMBUC
wasauffr
GtHOA
ttscdrmf
Current meter locations for Miami (Lee, Brooks, and Duing 1977)
-------
Current Meter
Locotionj
FORT PIERCE
80' 79'W
Figure 1 8. Current neter locations for Fort Pierce
(Lee, Brooks, and Duing 1977)
25
-------
STATION C
U-COuPONENT CM/SEC V-COMPONEfn CM/SEC
- too
too 200
200
400
MINIMUM
600
800
100 200
-100
200
U MAXIMUM
J 400
600
800
STATION- H
200
£ 400
c.
U-COUPONENT CM/SEC
-too 0 100 200
MAXIMUM
U,
600
MINIMUM
800 L
V-COMPONEMT cm/scc
-100 0 100
MAXIMUM
LEGEND
800 l-
CURRENT PROHlfS
uean
vuiu:i
DEPTH AVERACED
VUIMIMUM / V MAXIMUM
Figure 1 9
Measured velocity profiles offshore of Miami
26
-------
STATION. P
U-COWPONENT cm/sec
¦100 0 100 200
200 -
J 400
Q.
600
BOO
U MAXIMUM
MINIMUM
V-COUPONENT CM/SEC
-100 0 100 200
t 400
MAXIMUM
MINIMUM
U-COUPONENT CU/SEC
-100 0 100 200
200
£ 400
Q.
O
600
S00
V 1 1
\
V
i
(
i
(
- K
i
^ MAXIMUM
\_U MINIMUM
STATION. C
200
£ <00
a
600
V-COUPONEXT CU/SEC
-100 0 100 200
rrv-
800 L-
f / (
/ / A* MAXIMUM
MINIMUM
LEGEND
Current profiles
MEAN
VUIMIMUU / v MAXIMUM
depth Avtraced
Figure 1 9
27
(Continued)
-------
31. The Dropsonde data collection method was used to measure the
velocity distribution for the Fort Pierce transects shown in Figure 1,8. This
technique Involves the deployment of multiple Dropsonde Instruments which
record the vertical distribution of the horizontal velocity field as the
instrument descends through the water column. A cubic spline function Is then
used to compute a vertically averaged velocity vector at 50-o Increments
throughout the water column. The data set for Fort Pierce is based on 18 days
of Dropsonde deployment (Lee, Brooks, and Dulng 1977). Details of the
measurement technique are reported in Richardson and Schmitz 1965. The
minimum (westerly) u , corresponding v , ancl computed depth averaged values
for each of the Fort Pierce stations are shown in Figure 1.10.
STATION 40
u-ccuponcwt cu/src
-200 -100 0 100 200
200
~00
too
000
T
T
I
1
STATION 60
l'-CCvD0Nf>T cu/stc
-700 -100 0 '00 JOO
200
X ,00
600
800 L-
T~
T
T
~1
STATION 70
U-COKPONtMT CW/StC
-100 0 1 00 200
:oo
£. «CO
600
BOO
I
I
T
n
V-C0UP0NC*T CM/SCC
-200 -100 0 100 200
~i r
200
400
600
#00 >-
I
~T7 1
r
v-C0UP0«.C-l Cu/StC
200 -100 0 100 200
"1 1 1 1—r-|
y
JOO
J
I «00
a
w
o
600
/
BOO L-
v-COmpONCmT cw/SCC
-200 -100 0 100 200
"i 1 r 1—7—•
/
JOO
}
* 400
&
w
o
600
600
/
ircc.o
VUbN UUU
OCPTH AVtHACCO
Figures 1 .10. Measured velocity profiles offshore of Fort Pierce
28
-------
STATION 100
U-COmPOnEnT cm/sec
-100 o 100 200
T—TT
200
£ *00
a
600
800 L-
T
n
\
/
(
\
\
200
£ 400
Si
o
600
eoo L
STaTiON no
U-COUPONENT CM/SEC
-100 0 100 200
1 fl 1 1
)
(
)
\
\
station 120
U-COMPONCNT CM/SEC
-100 0 100 200
200
£ *00
a.
600
800 L
1
/
\
200
£ *oo
a
600
800 L-
V-COUPONENT CM/SEC
100 0 100 200
H 1—JT 1
I
\
200
£ *oo
a.
600
'800 —
V —COMPONENT CM/SEC
-100 0 100 200
T 1 I
/
/
V-COUPONENT CM/SEC
-100 0 100 200
200
£ +00
a.
600
800
T
\
LEGEND
VUINIUUM
depth avcracc:
Figure 1.10 (Continued)
29
-------
32. Available current meter data for all additional locations between
Miami and Fort Pierce were similarly analyzed. The purpose was to demonstrate
a spatial consistency in depth averaged velocities in order to show that the
velocities assigned to each proposed site are representative of their
respective locations. Table 1.5 identifies the current meter stations,
coordinates, and depth-averaged u and v velocity components for all gage
locations identified in the literature review.
Table 1.5
I
Current Meter locations and Depth Averaged Velocities
Current Eastward Northward Direction
Meter Latitude Longitude Velocity Velocity Vector (from north)
Stations (North) (West) cm/sec cm/sec cm/sec degs
Lee,
Brooks, and
Duing 1977
Miami(Spring)
10
25
32.0
80
3.0
17.5
55.5
58.2
342
20
25
31.0
80
0.0
12.2
45.3
46.9
345
30
25
32.0
79
57.1
7.1
66.8
67.;:
354
40
25
32.0
79
54.1
8.2
59.7
60.*
352
50
25
32.0
79
51.1
22.6
26.9
35.2
320
60
25
32.0
79
48.1
21.2
50.8
55.C
337
70
25
32.0
79
42.1
12.5
54.9
56.3
347
80
25
32.0
79
36.2
21.3
43.5
48.4
334
90
25
32.0
79
30. 2
19.1
34.2
39.2
330
100
25
32.2
79
24.2
20.4
23.4
31.1
319
110
25
32.2
79
21.2
22.7
26.3
34.8
319
120
25
32.2
79
19.5
24.5
20.9
32.2
310
130
25
32.2
79
17.1
35.3
20.4
40.8
300
Lee,
Brooks, and
Duing 1977
Miami
C
25
45.0
79
59.0
25.6
20.4
49.3
343
H
25
45.0
79
52.5
29.3
44.7
53.4
327
P
25
45.0
79
47.0
21.2
50.8
55.0
337
G
25
45.0
79
36.0
24.0
58.8
63.5
328
10
25
44. 5
80
3.0
14.5
47.0
49. 3
343
20
25
44.5
80
0.0
25.6
20.4
32.8
309
30
25
44.5
79
57.0
29.0
5.3
29.4
280
40
25
44.5
79
54.0
31.4
14.0
34.4
294
50
35
44. 5
79
51.1
29.3
44.7
53.4
327
60
25
44.5
79
48.1
25.2
12.4
28.1
296
70
25
44.5
79
42.1
26.3
57.1
63.0
335
80
25
44. 5
79
36.1
24.0
58.8
63.5
338
90
25
44. 5
79
30.1
23.4
35.8
CD
CM
327
100
25
44. 5
79
19.4
13.5
26.8
30.0
333
100
25
44. 5
79
27.1
15.2
38.9
41.8
339
30
-------
110 25 44.5 79 24.1 12.1 43.3 45.0 344
120 25 44.5 79 21.2 16.2 43.5 46.4 340
130 25 44.5 79 19.4 13.5 26.8 30.0 333
Lee, Brooks, and Duing 1977 Miami Bal Harbor
10 25 51.0 80 5.7 21.0 46.0 50.6 335
20 25 51.0 80 4.5 18.0 46.0 76.2 346
30 25 51.0 80 1.6 21.5 28.8 35.9 323
40 25 51.0 79 58.6 32.6 3.8 32.8 276
50 25 51.0 79 56.1 30.5 1.8 30.6 275
60 25 51.0 79 53.6 37.8 43.0 57.3 319
70 25 51.0 79 51.1 36.2 64.0 73.5 330
80 25 51.0 79 47.4 29.4 24.1 38.0 309
90 25 51.0 79 41.0 21.1 44.8 49.5 335
100 25 34.6 79 34.6 19.6 UU.Q 48.2 336
110 25 51.0 79 28.3 10.1 33.0 34.5 343
120 25 51.0 79 21.2 12.1 14.0 14.8 305
130 25 51.0 79 17.8 12.3 6.0 13.7 296
Lee, Brooks, and Duing 1977 Near Miami
R 25 50.7 80 05.0 31.0 72.4 78.9 337
R2 25 50.9 80 4.3 34.8 79.0 86.3 334
R3 25 51.0 80 3.3 29.1 10.5 30.9 290
R5 25 51.1 79 57.3 41.2 20.4 45.0 296
R6 25 51.1 79 51.1 52.4 17.5 55.3 289
N1 25 51.2 79 47.4 25.1 55.0 60.5 336
N2 25 50.9 79 22.0 5.0 5.0 7.1 315
R7 25 34.5 80 04.0 26.2 57.4 63.1 336
R9 26 8.9 80 3.7 18.2 55.5 58.4 342
R10 26 23.0 80 1.8 28.7 55.4 62.4 333
Lee, Brooks and Duing 1977 Fort Pierce
40 27 26.0 79 53.7 21.3 78.0 80.8 345
50 27 26.0 79 50.7 12.6 31.0 33.5 338
60 27 26.0 79 47.6 32.5 69.8 77.0 335
70 27 26.0 79 44.6 17.6 86.4 88.2 349
80 27 26.0 79 38.5 7.7 100.0 100.2 356
90 27 26.0 79 32.5 10.4 74.5 75.2 352
100 27 26.0 79 26.4 28.5 48.8 56.5 330
110 27 26.0 79 20.3 29.0 49.5 57.4 330
Leaman and Vertes 1982 Near Jupiter Inler
1 27 01 79 52 11.8 91.2 92.0 353
2 27 01 79 48 7.9 103.6 103.9 355
3 27 01 79 42 2.9 106.8 106.9 359
4 27 01 79 38 27.9 96.2 100.4 344
5 27 01 79 31 2.3 79.8 78.9 358
6 27 01 79 25 11.8 65.0 66.0 350
7 27 01 79 18 11.1 70.0 70.9 351
8 27 01 79 12 10.5 45 4 46.7 347
31
-------
Richardson, Schmitz,
and Niiler 1969 Cape Kennedy
Sec 5
28
20
80
06
16.2
33.5
37.2
334
28
20
79
58.5
19.0
51.8
55.2
339
28
20
79
52.5
16.3
75.0
77.0
348
28
20
79
33
18.0
80.7
82.0
347
28
20
79
07
31.7
33.5
46.1
317
Lee et
al
1986
Ponce
De Leon
Inlet
1
26
58.0
79
56.8
17.2
58.2
60.6
344
2
27
29.9
79
59.1
19.9
75.1
77.7
345
3
28
00.2
79
59.8
19.2
22.1
29.0
345
4
28
58.2
80
39.2
5.7
44.8
45.0
353
5
29
00. 7
80
21.7
15.1
44.6
47.0
341
6
29
00.0
80
08.2
25.5
52.9'
58.7
334
7
29
00.2
80
02.2
23.5
35.4
42.5
327
8
29
03 . 9
79
50. 9
11.7
39.3
41.0
344
9
29
00.2
79
00. 2
27.1
11.1
29.3
293
10
29
00. 1
79
07. 5
16.8
20.4
26.1
320
11
30
00. 6
80
16. 3
20. 7
53.4
57.3
339
Lee and Atkinson
1983 Near St
. Augustine
Inlet
4
29
10.0
80
10.0
20.0
6.0
20.9
287
5
29
30.0
80
30.0
14.0
14.0
19.8
315
6
29
30.0
80
20.0
12.0
75.0
76.0
351
9
30
00.0
80
30.0
30.0
28.1
41.1
313
10
30
00.0
80
20.0
35.0
75.0
82.8
345
12
30
40.0
80
15.0
18.0
10.0
20.6
300
15
30
50.0
80
10.0
10.0
8.0
12.8
307
25
32
30.0
78
30.0
30.0
15.1
33.5
297
Lee and Waddel
1983
A
30
00.0
80
15.0
20.2
31.4
37.3
327
B
30
00.0
79
40.0
32.2
1.2
32.3
270
C
30
00.0
79
20.0
19.6
5.4
20.4
286
D
30
00.0
78
10.0
20.4
26.6
33.5
323
E
30
00.0
77
00.0
26.0
34.4
43.6
323
Williams and Lee
1987
Al
28
35.8
80
31.2
5.2
60.3
60.5
355
A2
28
37.9
80
21.2
14.3
46.3
48.5
343
B1
29
53.6
81
14.9
2.8
12.0
12.3
347
B2
29
57.8
81
1.2
4.2
34.0
34.3
353
CI
31
1.1
81
16.6
5.6
15.0
20.0
340
C 2
30
57.2
80
56.1
4.9
31.5
31.9
351
32
-------
33. The velocity data presented in Table 1.5 are shown in vector form
in Figure 1.11 for the lower east coast (Miami to Fort Pierce) and Figure 1.1
for the upper east coast. At Miami the mainstream vectors are directed towar'
the shore due to the combined effects of a complex bathymetry and the approxi
mate 90 degree northerly deflection of the Gulf Stream at Miami. Flow is
generally directed to the north at Jupiter Inlet and Fort Pierce, as demon-
strated by the vectors at these two locations. This uniform orientation is
partially due to the fact that the offshore topography at Jupiter Inlet and
Fort Pierce is smooth and mild in gradient across the entire continental shelf
(Lee and Atkinson 1983). In addition to the mild bathymetry and shallow water
depth, the area is relatively free from the direct influence of the Gulf
Stream.
34. The velocity data presented in Table 1.5 and shown in Figures 1.11
and 1.12 were analyzed to produce summary velocity vectors at 2 mile intervals
across transects offshore of Miami and Fort Pierce. The proposed disposal
site locations are each located approximately U miles offshore. Tables 1.6
and 1.7 present these vector data along with the corresponding distance
offshore, water depth, and bottom slope. The results presented in Tables 6
and 7 are shown in vector form in Figures 1.13 and 1.14.
33
-------
FT. \
PIERCE
JUPITER 'NLET
ATLANTIC
OCEAN
WEST
PALM BEACH
SCALE
100 CM/SEC
FORT •
LAUDERDALE
\ \ \ VV
\ \
MIAMI •;
79rW
Figure 1.11. Depth-averaged current vectors from Miami to Fort Pierce
34
-------
CHARLESTON
HARBOR
Savannah
32'
ATLANTIC
SCALE
ponce; de
llon inlett
29'
CAPE
CANAVERAL
2
8Cr
79'W
Figure 1.12. Depth•averaged
current
35
vectors north of Fort Pierce
-------
Table 1.6
Velocity Distribution Offshore of Miami
Dlatano* D«pth
allea ft
0 V Hafiiiuid* Dlr«otlon
c«/»*C c"/»ec _cm />ee D««r»» '!!! P*—r|t
2
21
0.0222
34 .4
71.9
79.7
335.
U
258
0.0222
11.1
17.0
19-3
313.
6
B31
0.0515
25.6
20.1
32.B
309.
B
960
0.0119
27.3
12.9
30.2
295.
10
1092
0.0125
30.2
9.7
31.7
288.
12
1152
0.0057
31.«
1<4 0
31.1
291.
1800
0.0670
29.3
Ml.7
53.1
327.
16
2H00
0.0568
25.2
12.1
28.1
296.
18
2562
0.0)53
26.3
31.8
13.6
323.
20
2568
0.0006
26.2
57.1
63.0
335.
Too ahillou to dump
Table 1.7
Velocity Distribution Offshore of Fort l'lerce
Distance Depth U V Magnitude Direction
ml les ft Slope cm/sec cnusec ca/sec Degrees frenr.ark
2
32
0.0021
5.6
15.0
16.0
340.
«3
0.0010
10.0
8.0
12.8
308.
b
50
0.0009
20.0
6.0
20.9
287.
8
60
0 0009
25.5
52.9
58.7
331.
10
63
0.0003
23.5
35.1
12.5
326.
12
77
0.0013
28.7
55.1
62.1
333.
14
102
0.0021
25.0
66.7
71.2
339-
16
155
0.0050
21.3
78.0
80.85
315.
18
255
0.0095
12.6
31.0
33.5
338.
20
376
0.0115
32.5
69.8
77.0
335.
Too shallow to dump
36
-------
MIAMI
100
U. • DtriH AVERAG! D f AST £ Rl Y VELOCITY
--C
Vg • Of PTH AVERAGE NOPTHf fllY VClOClTV
70
I
U
it
>•
4
0
14
0TTAJ»C4 f ACM ImOU MilU
Figures 1.13. Velocity vector distribution offshore of Miami
fOATPKUCt
<~
too
TOO
U •DirtM AVERAGED tAJURlY VELOCITY
v# • 0{ rrn av( ftAcco no at hi h y vf ioc»t y
xo
0
1
I
I
14
>1
Olf T ' HQm ImO" I Willi
Figures 1.1^ Velocity vector distribution offshore of Fort Pierce
37
-------
Velocity Field Input nam
35. The short-term D1FID model and the long-term sediment transport
model require a velocity field boundary condition for each site in order to
calculate sediment transport. The velocity fields for driving the long-term
simulations were based on an approximate average of the 2, 4, 6, and 8 mile
offshore values for the Miami and Fort Pierce data shown In Tables 1.6
and 1.7. Values of 50 cm/sec (1.64 ft/sec) for Miami and 30 cm/sec (0.98
ft/sec) for Fort Pierce were used. In order to account for short-term
velocity fluctuations about the selected long-term values, the approximate
maximum of the inner 8-mile values shown in Tables 1.6 and 1.7 were selected
for the short-term simulations. Values of 85 cm/sec (2.79 ft/sec) and 60
cm/sec (1.97 ft/sec) were adopted for the Miami and Fort Pierce sites. The
corresponding angles of orientation (measured clockwise from true north) for
the velocity vectors are approximately 320 and 317 degrees for Miami and Fort
Pierce.
36. The depth averaged non-storm related velocity field approach for
analyzing the stability of each proposed ODMDS was used to analyze sediment
dispersion during dumping and to investigate long-term erosion resulting from
normal meteorological conditions. However, storm-induced erosion of an
existing mound may initiate sediment transport which may adversely impact the
reefs when normal long-term conditions would not. For this reason, a storm-
related velocity field was selected for simulation with the long-term model.
37. Peak velocities for a storm event were based on prototype obser-
vations during hurricane David. Smith (1982) Investigated the influence of
this hurricane on the continental shelf waters off south Florida north of Fort
Pierce Inlet. On 3 September 1979 hurricane David passed over an inner and
middle shelf prototype data collection area near Fort Pierce, producing a
record water level at the Fort Pierce inlet. Bottom pressure fluctuations
recorded on the inner shelf indicated a storm surge of approximately 3 ft
above the normal high water mark with a corresponding current of over
2.7 ft/sec. Based on these prototype velocity data, a numerical model input
velocity of 6 ft/sec for Miami and 4 ft/sec for Fort Pierce were used in the
Mng-term sediment transport model to simulate storm effects at the respective
l rps
38
-------
Upvelllnp and Downwelling
38. All prototype velocity data obtained in the literature review
represent horizontal velocities and all numerical modeling efforts are depth
averaged; therefore, vertical transport of sediments are not addressed in the
present approach. This section of the report briefly investigates the
occurrences of upwelling and downwelling in the vicinity of the Gulf Stream as
a possible source of transport of dredged material from the disposal site onto
the reefs. During upwelling, the deep waters are brought into the euphotic
zone (water depth less than 50 m) along the outer continental shelf (Lee et al
1981). The intent of this section is to determine whether these vertical
currents are adequate to erode and transport sediment.
39. The precise origin of upwelling and downwelling appears unclear;
however, it is suspected that they are a response to the movement of the Gulf
Stream (Smith 1983). Upwelling and downwelling events have been observed in
the vicinity of meander crests (Brooks and Bane, 1983) and have been corre-
lated with wind stress forcings which contribute to the formation of meanders.
Green (1944) documented an upwelling event off Daytona Beach which was
associated with southerly winds during July and August. Brooks and Mooers
(1977) investigated the relationship between wind fields and upwelling and
downwelling offshore of Miami. They concluded that southerly winds cause
upwelling while northerly winds produce downwelling on both side of the Stream
axis. The purpose of this section is to review the available literature and
document the magnitude of the vertical velocity w associated with an
upwelling event in order to assess its potential for transporting sediment.
40. Lee and Atkinson (1983) documented upwelling velocities associated
with a frontal eddy to be on the order of 0.01 cm/sec based on the measured
movement of an isotherm associated with an upwelling event. They also
estimated w by using vortlcity conservation principles and calculated a
value of 0.014 cm/sec. Osgood et al. (1987) used surface floats and current
meter data to compute a value of 0.048 cm/sec for a time series of data from a
documented event. A summary of reported upwelling velocity magnitudes
reported by Osgood et al. (1987), is shown in Table 1.8.
39
-------
Table 1.8
Summary of Upwelling Related Velocity Calculations
(Osgood et al. 1987^
Researchers
Lee and Atkinson
(1983)
Lee and Atkinson
(1983)
Chew et al
(1985)
Chew et al
(1985)
Rossby et al.
(1985)
Levine et al.
(1986)
Osgood et al.
(1987)
Method of
Calculation
tracking an Isotherm
vorticity conservation
tracking an isotherm
thermal wind balance
Rafos floats
Swallow float
Heat equation
Depth of w
Calculation (m) cm/sec
50
50
28-45
200
500
400
219
0.010
0.014
0.010
0.100
0.100
0.080
0.048
41. The results of this brief examination indicate that vertical
velocities during an upwelling event are on the order of 0.1 co/sec. As a
sediment transporting mechanism, velocities of this magnitude are not
considered significant with respect to horizontal velocities on the order of
30 to 40 cm/sec. Any possible transport by these vertical velocities would be
insignificant in comparison to sediment transported by the horizontal velocity
field. The following sections will, therefore, address sediment transp6rt as
a function of only the horizontal velocity fields previously described.
40
-------
PART II: THE SHORT-TERM SIMULATION OF DISPOSAL OPERATIONS
42. Section II of this report Investigates the short-term fate (less
than a day) of dredged material at the proposed Miami and Fort Pierce disposal
sites. The analysis approach will determine whether the combined effects of
the local topography at the site and the depth-averaged velocity field
developed in Section I, impact the effectiveness of the dredged material
disposal operation. Can the dredged material be physically placed within the
designated ODMDS limits as the material descends through the water column to
the ocean floor or are the local currents of sufficient magnitude to transport
material from the disposal vessel onto sensitive coral reefs? If the dredged
material can not be confined within the designated ODMDS limits, then an
alternate site further offshore should be evaluated for site designation.
A3. The short-term site evaluation phase is made by numerically
modeling the disposal operation using the DIFID numerical model. Theory and
background of the model are reported in Johnson and Holliday (1978), Johnson
(1987), and Johnson, Trawle, and Adamec (1988). The model computes the time
history of a single disposal operation from the time the dredged material Is
released from the barge until it reaches equilibrium on the ocean floor. The
DIFID model separates the dumping operation into three distinct phases. In
the first phase, material released from the bin Is assumed Co form a
hemispherically shaped cloud which descends through the water column under the
influence of gravity. This phase is called the convective descent phase. In
shallow water, such as the Fort Pierce site, this can be completed within a
few seconds of the initial dump. In deep water, such as the Miami site, this
time can be greater than 3 minutes. The increased descent time is due to both
the greater depth and to a corresponding loss of momentum of the released
material as it travels through the water column.
44. The cloud of material continues to descend through the water column
until it either impacts the bottom or has reached a stable point of neutral
buoyancy. In either case, the horizontal spreading of material marks the end
of the descent phase and beginning of the dynamic collapse phase. If the
disposal load is primarily composed of non-cohesive material, this phase nay
simply represent a settling and consolidation of the sediment into a mound;
however, if the load contains cohesive sediment, a comb ination of buoyancy ar.
41
-------
suspension may occur in which the cloud of suspended sediment may be
transported a considerable distance from the point of disposal.
45. When the rate of horizontal spreading in the dynamic collapse phase
becomes lfess than the spreading rate due to turbulent diffusion, the material
begins the final transport-diffusion phase. The termination of this phase
marks the end of the short-term investigation. The resulting post-disposal
sediment mound represents the initial boundary condition for the long-term
transport computations to be described in Section III. An idealization of
all three phases of the short-term disposal are shown in Figure 2.1
Input Data Requirement
46. The DIFID model requires site-specific input data in order to
quantitatively predict the short-term fate of sediment released during a
disposal operation. Input data include the characteristics of the dredge, a
description of the local environment to include the local depth and velocity
field, and a knowledge of the characteristics of the dredged material. In
addition, certain modeling parameters and coefficients must be specified. A
brief description of these input parameters is presented here.
47. The primary goal of the short-term modeling effort Is to determine
whether disposed material could be transported from the disposal site onto the
reefs. Since the potential for reef contamination increases with increasing
volumes of material in the water column, a conservative approach was adopted
in which a large capacity dredge was specified for model simulation. The
selected dimensions shown in Table 2.1 are representative of the largest
instantaneous dumping type dredge anticipated by SAJ (Tapp, 1988) to be
involved with the Miami and Fort Pierce dredging operation. A dredge of these
dimensions was, therefore, used for both the Miami and Fort Pierce
s emulations.
a2
-------
BARGE
'//////
CONVECTIVE
DESCENT
DYNAMIC COLLAPSE ON
BOTTOM
LONG-TERM PASSIVE
DIFFUSION
BOTTOM
ENCOUNTER
DIFFUSIVE SPREADING
¦ ¦GREATER THAN
DYNAMIC SPREADING
NOTE. Typical durations of descent and collapse
phases in 400-ft-deep water.
Convective descent - 1 /2 mm.
Dynomic collapse - 10 min.
Figure 2.1. Computational phases of the DIFID model
(from Brandsma and DIvorky, 1976)
-------
Table 2.1
Instantaneous Dredge Capacities and Dimensions
Overall length 236 ft
Beam length 53 ft
Depth of container 21 ft
Opening width of bin 12 ft
Unloaded draft of vessel 3.9 ft
Loaded draft of vessel 19.7 ft
Volume 4000 cu yds
Capacity 5400 tons
The location maps shown in Figures 1.1 and 1.2 show the disposal site
environment for Miami and Fort Pierce.
48. The Miami site is located in deep water with bathymetry contours
between approximately 400 and 750 ft. A depth of 400 feet, corresponding to
the shoreward limit of the designated site, with a bottom slope of 0.0658 was
specified for the simulations. An examination of bathymetry at the Fort
Pierce site indicates that the water depth varies between approximately 40 and
54 ft.
49. The DIFID model computes the convectlve descent of a cloud of
sediment from the bottom of the loaded dredge through the water column. In
order to properly model the descent phase, the total water depth must be
greater than the loaded draft of the dredge plus the computed radius of the
released sediment cloud. The specified dredge dimensions used for both site
simulations required a minimum of 60 ft of depth. The shallower depth at Fort
Pierce produced unstable results because the sediment cloud corresponding to
the 4000 cu yd load did not have a chance to complete the convective descent
stage. The choice of utilizing the 60 ft depth for the Fort Pierce simula-
tions was selected over the option of specifying a smaller capacity dredge.
This is not a severe assumption considering that depths of almost
55 fr. are representative of that site. A bottom slope of 0.0 was specified.
30 Depth-averaged velocities of 2 79 ft/sec (85 cm/sec) for the Miami site
and 1 97 it/sec (60 cm/sec) for the Fort Pierce site were selected as input to
44
-------
the DIFID modal- The angles of orientation of the velocity vectors for the
Miami and Fort Pierce sites is 320 and 317 degrees, measured clockwise from
magnetic north. The simulations performed in this section are relative to
this axis.
51. Additional input required for the D1F1D model include specifying
the composition of the material in the dredge. Normally, the dredged materi
is composed of a solid fraction (rock, sand, clay, etc.) and a fluid
component. Each component must be defined according to its respective
density, concentration by volume (component percentage of total load volume)
fall velocity, and voids ratio (volume of water to volume of solids ratio).
In addition, the in-barge percent distribution of solids must be specified.
The selection of material densities, fall velocities, and void ratios for bo
the Miami and Fort Pierce sices was based on information obtained from SAJ
(Tapp 1988), from a recent DIFID application in Mobile Bay (Reese 1988), and
from numerous DIFID applications reported by Johnson and Holliday (1978). T1
selected composition of the disposal load used for both sites is shown in
Table 2.2
Table 2.2
Characterization of Dredged Material for Miami and Fort Pierce
Density
Volumetric
Fall Velocity
Cohesive
DescriDtion
e/cc
ratio
ft/sec
Voids Ratio
(1 or 0)
SAND
2.650
0.6300
0.04660
0.00
0
SIL-CLAY
2.650
0.0700
0.00256
1.00
1
WATER
1.023
0.3000
0.00
52. The concentration percentages of the total load are based on an
assumed solids content of 70 percent by volume of the material in the barge.
Sieve analyses received from SAJ (Tapp 1988) showed medium well graded sand
(non-cohesive) was representative of at least 90 percent of the solids in the
load (90* of 70% - 63*). Cohesive silts and clays were specified for the
remaining 10 percent of solids A bulk density of 2.16 gm/cc and an aggregat
^5
-------
void ratio of 1.4 was specified for both sites to compute the final thickness
of the composite mound.
53. There are numerous model parameters in addition to the internal
model coefficients required as input to the DIFID model. Grid resolution and
time step parameters were selected to best represent each disposal site. The
internal model coefficients recommended by Johnson and Holliday (1978) and
used by Reese (1988) were used for both site simulations. The parameters and
coefficients used are shown in Table 2.3.
Table 2.3
Input Data Related to Disposal Operation for
the Miami and Fort Pierce ODMDS
Variables Miami Fort Pierce
Grid sire (ft) 200 200
Number of cells:
cross-shore direction 105 105
Alongshore direction 28 28
Time step (sec) 100 100
Duration of simulation (sec) 6000* 10800
Ambient velocity (ft/sec) 2.79 1.97
Ambient density (gm/cc) 1.023 1.023
DINCR1 1.0 1.0
DINCR2 1.0 1.0
Entrainment coefficient A1APH0 0.200* 0.235
BETA 0.0 0.0
CM 1.0 1.0
Drag coefficient for sphere, CD 0.5 0.5
GAMA 0.25 0.25
Drag coefficient for elliptic
cylinder, CDRAG 10 10
US
-------
CFRIC 0.01
CD3 0.10
CDA 1.00
Entrainment due to cloud collapse,
ALPHAC 0.0010
Bottom friction, FRICTN 0.0100
A1AMDA. 0.005
Vertical diffusion coefficient,
AXYO 0.0100
0.01
0.10
1.00
0.0010
0.0100
0.005
0.0100
* Adjustments in value from those of Fort Pierce were required for the deepei
depths of the Miami site.
Method and Procedure for Short-Term Model Simulations
54. The objective of the short-term simulations was to determine
whether dredged material could be effectively placed within the limits of the
designated disposal sites under the action of a realistic localized velocity
field. Of particular interest was whether the settling material (primarily
sand) or the suspended sediment cloud (silts and clays) could be transported
from the dredge onto the reef area. Data received from SAJ (Tapp, 1988) and
shown in Figures 1.1 and 1.2 indicated that the reef areas are located a
minimum of approximately 1.5 miles due west of the shoreward edge or 2.0 miles
from the center of either ODMDS. If the average release point is considered
to be at the center of the designated site, an effective distance between the
disposal site and the nearest reef of approximately 3.0 miles is computed from
Che angle of orientation of the velocity vector. In order to investigate
these far field effects, the model grid dimensions were specified to be 105
cells in the flow direction by 28 cells in the transverse direction. The grid
spacing of 200 ft produces an effective modeling area of 1 mile by U miles
The disposal release point was selected at approximately 0 U miles (grid cell
10) from the upstream boundary
U]
-------
55. The approach taken Co investigate the possibility of reef contamina-
tion was to determine both the depth and extent of deposition and the sediment
plume concentration impact produced by a single disposal load under the
maximum, reef-directed, non-storm condition likely to be encountered during a
dumping operation. Two parameters were of interest. First, the total
deposition pattern was computed to indicate the maximum distance from the
dredge at which measurable (above 0.01 ft) deposition could be expected. This
maximum excursion distance provides an indication of the spatial extent of
direct deposition of material on the bottom.
56. The second measure of impact, and the primary parameter of interest
to this study, quantifies the movement and concentration of the moving cloud
of suspended sediments. As the cloud is transported from the dredge by the
ambient currents, it grows larger (diffuses) and, correspondingly, less
concentrated. The second phase of Investigation looks at the change in time
of the location and concentration of this cloud of sediment as it is diffused
and transported toward the reef area. An example of transport and diffusion
of the cloud is shown in Figures 2.2, 2.3, 2.4, and 2.5 in which the horizon-
tal distribution of the suspended sediment concentration of the silt-clay
cloud is shown at the 200 ft level (below the surface) for the Miami simula-
tion. With the release point assumemed to be at the center of the disposal
site (specified as cell 10, the nearest reef is located at approximately grid
cell number 89. The 1500, 3000, 4500, and 6000 sec snapshots shows the
increase in size and corresponding decrease in concentration of the settling
cloud as it is transported toward the reef area.
57. Results of the concentration computation are used to produce a
concentration (in ppt or mg/1 above ambient conditions) versus distance
relationship along the axis of the grid at five discrete depths for four
specified time periods (i.e., along the axis of symmetry at grid N - 14 of
Figures 2.2-2.5). Quarter-point times were selected to show results at the
1/4, 1/2, 3/4 and final point of any specified time period following the
initial release of material from the barge. The following sections present
the results of these simulations for the Miami' and Fort Pierce sites.
8
-------
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U 9
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Figure 2 5 Suspended sediment cloud at 200 ft deep at 6000 sec after dump
50
-------
Miami Disposal Site
58. Results of the sediment concentration computation for Miami are
shown in Figure 2.6. The disposal release point is located at approximately
mile 0.4 and the reef at approximately mile 3.5. Note that these figures
represent distance-concentration plots at the quarter-point times along the
reef-directed cloud axis. The uppermost graph of Figure 2.6, for example,
summarizes the data presented in Figures 2.2 through 2.5. The depths of 200,
250, 300, 350, and 400 ft were used in order to present an overall representa-
tion of the numerical results. For example, at 1500 sec after the initial
dump, simulations of the disposal operation shows concentrations of suspended
silt and clay at the 200 ft depth to be 10 ppm. Results demonstrate that
the descent phase of the hemispherically shaped cloud passes through the water
rapidly leaving little sediment in the upper water column. The examples
presented in Figure 2.6 indicate that a point of maximum concentration is
reached at a depth of approximately 350 ft and that a concentration decrease
Is seen both above and below this point. This relationship of maximum
concentration is maintained for each quarter point as the cloud disperses.
All results indicate a decreasing concentration in both time after disposal
and distance from the release point as shown In the summary Table 2.A.
51
-------
3000
see
x~
4300
see
1
3000
1
see
200 FEET
0 0 0 3 to 15 2 0 2.3 3 0 3.3 4 0
250 FEET
00 05 10 15 2 0 23 '3 0 3 3 40
O
3
§ o
f= °
300 FEET
0 0 0 5 1.0 1.3 2 0 2.5 2 0 3.9 4.0
U
Z
o
o
6000
350 hEl
3D 05 '0 15 ?0 25 JO 3 5 <0
A
)
\
400 FEET
CO 05 10 15 10 2 5 30 3 5 <0
D'Stance: in uiles
Figure 2 6 i ime - concent r,it l on for Miami at 200, 250. 300, 330, and 400 ft
5 2
-------
Table 2.4
Summary of Computed Maximum Suspended Silt and Clay Concentration
(Concentration In mg/1 above ambient)
Elapsed Time (sec)/Approxlmate Distance from
Dredge (Miles)
6000
3.2
Depth
1500
0.8
3000
1.6
4500
i_
liti
200
250
300
1. 2x10"13
7.1x10"9
5.5x10"6
5.7x10"^
1.5xlO"5
6.7x10"7
4.3xl0"6
8.7xl0"6
5.8x10"^
2.4x10"6
1.7xlO"6
2.5xl0"6
2.2xl0"6
l.lxlO"6
6.9x10"7
l.OxlO"6
9.2x10"7
6.6x10"7
3.8x10"7
2.6x10"7
350
400
59. A plot of the total sediment deposition versus distance along the
axis of the disposal grid is shown in Figure 2.7. A three-dimensional view of
the resulting disposal pattern is shown in Figure 2.8 with the corresponding
contour plot shown in Figure 2.9. The stable material mound is composed
primarily of the sand portion of the disposal load and will be the subject of
the long-term disposal simulations described in Section III.
53
-------
10IPL DCPOSITION
r
in
m
i
I:
£
om%a i" «iici
Figure 2.7. Deposition pattern for the Miami site
Figure 2 8 Three-dimensional view of the Miami site disposal mound
^ ~
fe§i=
I:
2.79rr/S£C
¦200 FT
0 0
XGKD * 18.0
200 rr
"Lg'jre 2 9 Contour plot of the deposition pattern for the Miami site
56
-------
Fort Pierce Disposal Site
60. Results of the sediment concentration computation for the Fort
Pierce site are shown In Figure 2.10. Depths of 10, 20, 30, 40, and 50 ft
were specified In the simulation. Note that because of the shallow depth,
sediment remains in suspension throughout the water column. Also, the figures
show the depth of maximum concentration to be located at approximately the
30 ft depth. A trend, similar to that shown in the Miami simulations, of
decreasing concentration with increasing distance and time is seen. This
trend can be seen in the concentration summary Table 2.5.
61. A plot of the total deposition in ft versus distance along the axis
of the disposal grid is shown in Figure 2.11. Three-dimensional results of
the disposal mound are shown in Figure 2.12 with the corresponding contour
plot shown in Figure 2.13. Due to the shallow water depths and relatively low
velocities, the stable mound can be seen to be conical in shape.
Table 2.5
Summary of Computed Maximum Suspended Sediment Concentration
(Concentration In rim/l above amblentl
Time (sec)/Approximate Distance from Dredge (Miles)
Depth
2700
5400
8100
10800
(ft)
1.0
2.0
3.0
4.0
10
1.2x10-5
2.4x10-6
7.8x10-7
*
20
2.3x10-5
4.4x10-6
1.4x10-6
*
30
2.8x10-5
5.5x10-6
1.7x10-6
*
40
2.3x10-5
4.4x10-6
1.4x10-6
*
50
1.2x10-5
2.4x10-6
7.8x10-7
*
+ Results at the 10800 sec were below the computationa . threshold of the
model, hence, no values are reported.
53
-------
o
n
2700
S£C
o
r4
200 FEET
5400
StC
6100
STC
o
o
o
2 0
0 1
0 0
2 5
3.0
3 5
o
250 FEET
o
o
o
0 0
2.0
0
2 5
3 0
0 5
5
4.0
o
SEC
2700
o
see
8100
StC
300 FEET
o
o
o
0.0 0.5
2 0
3.3 JO
J.5 4.0
5
o
o
ru
350 FEET
o
o
o
00
0 5
2.3
2 0
3 5
3.0
A
A
400 FEET
00 05 10 15 20 2.5 30 35 40
distance; in wiles
Figure 2 10 Time-concentration for Fore Pierce ac 10. 20, 30, AO, and 50 ft
56
-------
IOTP*, dcpositjon
M li II It )• II » • 1 *
DISTWCt JN MU5
Figure 2.11. Deposition pattern for the Fort Pierce site
Figure 2.12 Three-dimensional view of the Fort" Pierce site disposal mound
i o
-
-
-
--
-
-
! __
¦
_j
_j
j
-
1 A..
1 1_
—
"1
n
-
-
—
- i
-
-
-
-
-
- -
---
n ,
A
_ _
, ^
i
tj
li!.:
1 ! 1 1 i
-
i
t
S
y r
~ n
T
.j
i ; i i i . i
—
| i ' | i I !
r
-
-
-
-
. .
- ¦
J
_1
0.0 * CRD 180
Figure 2.13. Contour plot of the deposition pattern for the Fort Pierce site
57
-------
PART III: THE SIMULATION OF LONG-TERM DISPOSAL FATE
62. The final task of the evaluation study investigates the long-term
fate of disposed material in open water. This analysis will concentrate on
classifying the disposal sites as either dispersive or non-dispersive based on
whether the local velocity field is adequate to erode and transport material
from the mound onto the coral reefs. Transport simulations will be made for
periods of time ranging from a day to a year. This phase of the project
differs from Phase II in that the short-term investigation determined whether
the material could be effectively placed within a designated site during the
dumping process when material descends through the water column and collapses
on the ocean bottom. The long-term analysis assumes that the material has
been successfully deposited on the bottom and has assumed a stable mound
configuration. Whether the mound is dispersive or non-dispersive now depends
on whether the local current field is capable of resuspending and transporting
material such that the mound deformes and is moved from its initial position.
Changes in the computed sediment transport patterns are used to compute these
changes in location and configuration. For example, as material is eroded
from the higher velocity regions near the top of the mound and deposited in
areas of lower velocity in the lee of the mound, the shape, orientation, and
center of mass of the mound change.
63. The long-term analysis will consist of two approaches. The first
will utilize the long-term velocity field developed in Section I of this
report to determine whether these velocities are sufficient in magnitude to
suspend and transport bottom sediments from an existing disposal mound of a
specified initial configuration. The second phase will simulate the passage
of a storm surge over the mound. Both approaches will use a sediment
transport model to compute non-cohesive sediment transport and the associated
bathymetric change as a result of a time varying velocity field around the
mound. A brief description of the modeling approach follows.
58
-------
Sedlmpnc Transport
64. Empirical relationships for computing sediment transport as a
primary function of ambient water velocity, depth, and sediment grain size
were reported by Ackers and White (1973). These relationships were subse-
quently modified by Swart (1976) to reflect an increase in sediment transport
when a wave field is superimposed on the ambient current field. This addi-
tional transport reflects the fact that additional sediments are suspended by
wave induced bottom orbital velocities. These additional sediments in the
water column are available for transport by the localized velocity field.
Details of an application of the combined Ackers-White and Swart modification
methodology were reported by Vemulakonda et al. (1987) in which computed
erosion and deposition volumes were shown to adequately reproduce measured
bathymetric changes computed from periodic maintenance dredging surveys in the
entrance channel of St Marys Inlet, Florida.
65. Prior to computing long-term simulations, a sensitivity test of the
transport predictions was performed for the local conditions at the proposed
Miami and Fort Pierce disposal locations. The goal of this testing was to
determine threshold velocities needed to initiate sediment movement at each
site under the localized environmental conditions of depth and wave field.
Sediment transport curves were prepared for each site for a velocity range of
0.0 to 4.0 ft/sec and for a sediment diameter size of 0.1 mm to 0.2 mln in
increments of .02 mm. These curves are shown in Figures 3.1 and 3.2.
66. Approximations for wave height and period used in the generation of
Figures 3.1 and 3.2 were determined from the Wave Information Study (WIS)
20-yr hindcast data base (Jensen, 1983). Figures 3.3 and 3.4 represent a
reproduction of the wave summary statistics for WIS Stations 163 (for the
Miami site) and 153 (for the Fort Pierce site). Note that the wave heights
and periods selected are representative of larger than average wave
conditions; hence the transport rates used in this analysis will be
conservative. Average depths of 600 ft for Miami and 50 ft for Fort Pierce
were selected from Figures 1.2 and 1.3 to represent depths at the center of
Che designated sites.
59
-------
H - 6.53 FT, T - 6 SEC, D - 600 FT
.20
.12
r
WOmm
50
125.0 JSI-0 ro.O SCO.O OS.O rSD.O 875.0
smirorr transport ¦ ioooo icu ft/sec/fti
Figure 3.1. Sediment transport v« velocity • Miaai disposal alt*
H - 8.17 FT, T - 0 SEC, D - 50 FT
Q
.14
.12
OflOmm
vt.o sae.o oro ro.o
SaiPtWT TRUSTOR! » 10000 (CU FT/SEC/fT)
Figure 3.2. Sediment transport vs velocity - Fort Pierce disposal site
60
-------
SHOBfLIHe
^IfiEtHroCCURRtNdEfxioin OF HEIG
FOP ALL DIRECTIONS
AZIMUTH
height! nrraes)
HEIGHT AND PERIOO FOR ALL DIRECTIONS
PERIOD!SECONDS)
<:i
*•!
5.i
i]
n
5 S:» * ?:. 'WiWfc.
"" 1?il iJf|' |R '« !U "t " "! n
: 'It ijj | ,j j
- 4.J9
ota^" ™ laAi 26l9 tjiv l^iz sSs 4J9 1A4 49 lii
AVE MSiri) ¦ O.SJ LARGEST HS!M) « *.91 TOTAL CASES « 5M40
4e
TOTAL
??S
Figure 3.3. WIS station 163 wave characteristic summary for the Miami site
FOP ALL DIRECTIONS
AZIrtUTH
HEIGHT!METRES)
>0 •
0 -
H
! |i|
& - GftEAUR
TOTAL
HEIGHT AND PERIOD FOR ALL DIRECTIONS
PERIOD!SECONDS)
0.0- 30- 4.0- 5.0- 6.0- 7.0- 8.0- 9.0- 10.0- 11.0-
2.9 5.9 <..9 S.9 {.9 7.9 6.9 ?.9 io.9 LONGER
644
™ 'is f|| \\i n $ si !i
s? m
AVE HS!MI * 0.78 LARGEST HSIMI e 3.61 TOTAL CAGES *
*8
25*
6^4 I4j9 16lS 10>7 7i 7 1JJ4 942 737 469 9^4
5M<>0
TOTAL
Figure 3 U UI5 station 1S3 wave cha r nc t c r i s t i c summary for che
Fore Pierce ^ i t c
61
-------
67. Depth-averaged non-storm velocity fields were shown in Section I of
this report to be approximately 1.64 ft/sec (50 cm/sec) for the Miami site and
0.98 ft/sec (30 cm/sec) for the Fort Pierce site. Results shown in Figures
3.1 and 3.2 indicate that these velocities are marginally adequate to trans-
port sediment; however, locally elevated velocity vectors in the vicinity of
the mound crest may be adequate to transport sediment from the mound. The
following section will address the velocity field distribution as the ambient
current field flows over the mound.
Velocity Field Distribution
68. The sediment transport modeling approach is based on an accurate
velocity distribution around the mound. A steady state numerical model was
developed specifically for this purpose. The model, based on the simplified
equations of motion and the continuity equation, computes a velocity
distribution around a mound of specified dimensions as a result of a constant
imposed "upstream" velocity field boundary condition. A sample computation is
shown in Figure 3.5 in which the depth averaged velocity vectors can be seen
to increase in magnitude and change orientation as the velocity field is
influenced by the presence of the disposal mound.
69. A sediment transport rate corresponding to each vector is computed
for the entire numerical grid in order to yield a spatial transport
distribution. This distribution is input to a non-cohesive sediment con-
tinuity model which computes bathymetric changes as a result of transport
gradients. When more sediment enters a computational cell than exits the
cell, deposition will occur. Conversely, when more leave than enter, erosion
will be shown. No net change occurs for a uniform flow field in which equal
amounts of sediment enter and leave a cell. When the velocity field is below
the local transport threshold value (such as those shown in Figures 3.1 and
3.2), no transport occurs and no net erosion or deposition results.
62
-------
i r t M
mil
Mill
I t II I
Mill
ihii
11 ii i
ii m i
11111
11 i i
m 11
MOUN
Figure 3.5. Velocity vectors around an idealized disposal mound
70. Velocity field simulation computations are updated at a 3-hr time
step to reflect the changing shape of the mound. As the transport patterns
adjust in response to the time-varying velocity field, material is transported
from regions of high velocity and deposited in regions of low velocity. This
process will continue until either the velocities fall below the threshold
value required to transport sediment or the mound reaches an equilibrium
condition in which equal amounts of sediment enter and leave a computational
cell. In the latter scenario, the mound has dispersed to the point that the
Identity of the mound has been lost and it no longer effects the current
regime.
71. Erosion and deposition patterns associated with the changing shape
of the disposal mound are also computed at every 3-hr time step. These
computations indicate the time variation in depth of sediment deposition
versus distance from the mound. The distance at which zero depth changes
occur will indicate the first location from the mound at which no mound
material has been deposited; hence, the maximum radius of mound influence on
the environment If material from the mound is deposited beyond a designated
63
-------
point, i.e., on the reefs, then the disposal site can be considered
dispersive. For the present study, the critical distance of excursion is the
distance from the disposal mound to the reefs.
72. Two simulations will be used to determine whether the presence of
the mound poses a potential threat to the coral reef area. The first is a
long-term simulation in which the mean non-storm velocity field and wave
condition for each site is continually subjected to the mound. Simulations
are performed to determine either an excursion rate of the mound in feet per
day or to demonstrate that a point of equilibrium has been reached and the
mound ceases to move. The second is to simulate a storm related event and
compute the total excursion associated with that storm. This simulation will
utilize a sustained storm driven velocity surge for a duration of 24 hours, a
time scale typical of a hurricane event. If either the long-term average
velocities or the high intensity storm induced velocities can be shown to be
of sufficient magnitude to transport material from the mound onto the reef
areas, it can be concluded that the site is potentially dispersive with
respect to long-term events, and that alternate disposal areas further
offshore should be investigated.
Sediment Transport Due to Non-Storm Velocity Fields
73. The results shown in Figures 3.1 and 3.2 indicate that sediment
transport is initiated at velocity threshold values of approximately 1.0
ft/sec and 2.0 ft/sec for the Fort Pierce and Miami sites respectively.
Although the observed ambient velocities at both sites are below these
critical values (0.98 and 1.64 ft/sec), the effect of the mound on the
velocity distribution may result in elevated velocities on the mound which are
sufficient in magnitude to erode and transport material. In addition to the
velocity magnitude, model input includes the specification of a single
sediment size.
74. Although Figures 3.1 and 3.2 show that the mean sediment diameter
is not a critical parameter when the velocity magnitude is near the sediment
transport threshold, a sediment size of 0.2 mm was selected for all
simulations. The specification of a fine-grained non-cohesive sediment for
both sites provides a threshold evaluation of the onset of mound erosion since
64
-------
fine grained materials are eroded before coarse grained materials are.
Results obtained from SAJ (Tapp, 1988) indicate average specific gravLties of
materials which will be disposed of at the Miami and Fort Pierce sites to be
2.78 and 2.70 respectively, indicative of quartz sand. A typical grain size
analysis of a sample obtained from the Fort Pierce harbor is shown in Figure
3.6. The report classifies the material as "poorly graded sand (SP)." In
view of this classification, a fine sand specification will provide an
estimate of maximum erosion potential. The analysis further indicates a D50
diameter of approximately 3 mm; therefore, the use of a 0.2 mm material in the
I
transport computations serves two functions. It provides a threshold
indication of fine material transport, and it provides an indication of fine
grain mound transport; as such, it yields a "worst case" prediction of
sediment erosion from the mound.
75. A test mound measuring 250 ft square and 10 ft high was used as the
design mound configuration for both simulations. A mound of this dimension
would contain a volume of approximately 20,000 cubic yards. Although
idealized, this configuration will provide an indication of mound stability.
The following sections will address the long-term and storm event analysis.
Fort Pierce
76. The proposed disposal site offshore of Fort.Pierce (Figure 1.1) is
located in shallow water, with ^n average depth of only approximately 50 ft.
A wave with a height of 8.17 ft (2.49 m) and period of 8 seconds was used to
indicate a rough, but non-storm, sea state. Results of Section I indicate
this area to be outside of the direct influence of the (lulf Stream; therefore,
depth averaged velocities are relatively low, on the or
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GRADATION CURVES
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-------
77. A 1-year simulation of the idealized mound at the Fort Pierce site
was made. Results indicate that material from the mound migrated a total
distance of 600 ft in 6 months of sustained maximum current. At this point,
the outer edge of the mound reached the computational boundary. The
approximate center of mass of the mound migrated approximately 700 ft during
the 1 year simulation. During this tine, the shape of the mound became
elongated, and a scour hole developed in front of the mound. Figures 3.7,
3.8, and 3.9 show the initial configuration, the mid-simulation shape, and the
configuration at the end of the simulation. Figure 3.10 presents the monthly
change of shape through a central cross-section of the mound. The rate of
excursion of the leading edge of the mound is approximately 3 ft per day.
Center of mass migration is less than 2.0 ft per day. At either rate, a
migration onto the reef area would require in excess of 10 years. During this
time, the mound would realistically erode and disperse in many directions,
resulting in a lower, less dispersive profile.
78. In order to Investigate the erosion producing capability of a storm
event, a hypothetical hurricane was constructed with a sustained 24-hour
depth-averaged surge velocity of 4 ft/sec. The initial mound configuration is
identical to that shown in Figure '3.7. The final mound shape at the end of
the storm event is shown in Figure 3.11. Cross - sectional profiles at 6-hr
intervals are shown in Figure 3.12. Results indicate that the maximum radius
of transport resulting in deposition of more than 0.1 ft to be approximately
500 ft The corresponding mound crest migration is 350 ft.
6 7
-------
TOTAL ELAPSED TIME - 0.00 HOURS
Figure 3.7. Initial mound configuration for Fort Pierce
TOTAL ELAPSED TIME - 4320.00 HOURS
Q
Figure 3
Fort Pierce mound configuration at h months
68
-------
TOTAL ELAPSED TIME - 8640.00 HOURS
i
7 /
o
*0
Figure 3.9. Final Fort Pierce mound configuration at 12 months
O
O
UJ o
O d
O o
107 5 0 0 93> S
DISTRNCC in rcCT
F:rure 3 10 Tirr.e history of long-term erosion of the Fort Pierce mound
69
-------
n
I
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TOTAL ELAPSEO TIME
24.00 HOURS
Figure 3.11. Final (24 hr) Fort Pierce storm mound configuration
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Figure 3 12
Time hiscorv of scorn erosion of Fort: Pierce mound
70
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Miami
79. The proposed disposal site for Miami Is located at a depth of
approximately 600 ft with a corresponding maximum velocity field of approxi-
mately 1,64 ft/sec (50 cm/sec). A 3-month simulation of the idealized mound,
using a wave height of 6.53 ft (1.99 m) and period of 6 sees, was performed.
The initial and final mound configuration and the evolution of the mound with
time, shown on Figures 3.13, 3.14, and 3.15, indicate no transport or erosion.
The result that the velocity field is not adequate to either suspend or
I
transport material at a depth of 600 ft is not surprising in view of the
threshold values shown in Figure 3.1.
80. A storm event for the Miami site was assumed to have a sustained
velocity of 6.0 ft.sec for 24 hours. The post-storm mound configuration is
shown in Figure 3.16. The corresponding time changes of the cross - section at
6-hr intervals is shown in Figure 3.17. As can be seen in the figures, a
mound located in 600 ft of water is little effected by velocities of a
magnitude realistically representative of the disposal site offshore of Miami.
TOTAL ELAPSED TIME - 0.00 HOURS
-------
TOTAL ELAPSED TIME - 2160.00 HOURS
FLgure 3 14. Final Miami mound configuration at 3 months
52
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DISTANCE IN ret7
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Figure 3 IS Time hisrory of long-terra erosion of the Miami mound
-------
TOTAL ELAPSED Time - 24 00 HOURS
Figure 3.16. Final (24 hr) Fort Pierce storm mound configuration
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Figure 3 1/
Tirr.c hi.-:cory ot iiorra erosion <> f Mi..mi rno'ind
n
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PART IV: CONCLUSION
81. The purpose of this investigation is to determine whether sediment
from the proposed Miami and Fort Pierce disposal sites could be transported
onto the sensitive near-shore coral reefs. Numerical modeling techniques were
utilized to answer these questions. The approach taken was first to review
the available literature and document the magnitude of velocities which are
representative of each site. The question of reef contamination was then
addressed in a two-phase modeling approach. In the short-term analysis, the
actual disposal operation was modeled to determine whether material from the
descending sediment plume could be carried In suspension by the ambient
velocity field onto the reefs before settling into the disposal site. The
long-term investigation computes sediment transport and the associated erosion
and deposition of the disposal mound as a function of the local velocity
field. Results of the study indicate that neither the Miami nor the Fort
Pierce site pose an environmental threat to the reef areas. These results are
briefly summarized below.
82. The first level of investigation requires the defining of a non-
storra velocity field for both proposed disposal sites. Existing velocity
records were extensively examined to quantify a depth-averaged velocity field
which would represent the most severe reef-directed currents. The approach is
based on the assumption that shore parallel or offshore directed velocities
present no environmental threat to the reefs but that a worst case condition
of maximum shoreward directed velocities could possibly effect the reef areas.
The review of data showed that a maximum depth-averaged, velocity of 0.97
ft/sec (30 cm/sec) and 1.64 ft/sec (50 cm/sec) was representative of the
Fore Pierce and Miami sites. In order to simulate a more extreme condition,
larger values of 2.79 ft/sec (85 cm/sec) for Miaibi and 1.97 ft/sec (60 cm/sec)
for Fort Pierce were selected for the short-term simulation phase.
83. The short-term modeling of the disposal operation shows that most
of the material from the disposal load settles into a mound within several
hours after the initial release of sediment from the dredge. Model results
indicate the maximum distance from the barge showing deposition in excess of
0 01 ft was 1600 ft for Miami and ^00 ft for Fort Pierce The silt and clay
portion of the disposal load creates a suspension cloud or turbidity plume
1U
-------
which is transported toward the reefs by the specified ambient currents. This
cloud increases in size and decreases in concentration with distance from the
point of disposal. The concentration of the suspended sediment cloud was
computed at five specified depths for each site simulation. Results at the
conclusion of the simulation indicate maximum concentrations above background
levels at the reef (taken to be approximately 3 miles from the disposal area)
to be 0.00000089 mg/1 at a depth of 200 feet for the Miami site. This value
corresponds to an elapsed time of 1.66 hours after the initial sediment
release. At 2.25 hours after disposal, a maximum concentration of 0.0000017
I
mg/1 at a depth of 30 ft was computed for the Fort Pierce site. As shown,
both values are less than one part per million. The short-term modeling
efforts, therefore, indicate that the local ambient velocity fields are not
adequate in magnitude to transport any significant amount of material from the
dumping operation onto the reef area.
84. The long-term modeling effort was conducted to determine whether a
disposal mound is stable over long periods of time. Two types of simulations
were conducted. A long duration simulation of a specified mound configuration
was conducted for each site using a reef directed non-storm depth-averaged
velocity field of 0.97 ft/sec (30 cm/sec) and 1.64 ft/sec (50 cm/sec) for the
Fort Pierce and Miami sites. Results of these simulations show that the local
velocity field at Miami is below the threshold value required for eroding and
transporting material, i.e., a 3-month simulation showed no erosion of a mound
located in 600 ft of water. The mound at Fort Pierce was shown to erode,
deform, and migrate at a rate of approximately 2-3 ft/day. These results were
based on a 1-year simulation in which the centroid of the mound moved approx-
imately 700 ft. Additional shorter duration simulations were made for each
site in order to investigate storm related transport of material from the
mound onto the reefs. A 24-hour sustained storm surge velocity of 4.0 ft/sec
for Fort Pierce and 6.0 ft/sec for Miami was input to the long-term sediment
transport model. . Results for the Fort Pierce simulation show that material
was moved a maximum distance of approximately 550 ft in 24 hours. The Miami
simulation showed that essentially no material was transported as a result of
the surge Conclusions of the long-term simulation indicate that sediment
will be transported from the Fort Pierce site during both ambient and storm
conditions, but that the race of movement should not effect the reef system.
75
-------
For the proposed Miami site, simulations show that local velocity fields are
simply not adequate to move material in 600 ft of water.
85. The simulation approach taken in this study involves the specifica-
tion of a local velocity field directed to maximize the transport of material
from the disposal site onto the sensitive reef area. Numerical simulations
are used to evaluate whether this velocity field is adequate to contaminate
the coral reef with dredged material. The disposal operation and the disposal
mound are modeled as a potential source of contamination. Both the short-term
disposal and long-term erosion simulations of sediment transport as a function
of local velocity fields indicate little pqssibility of reef contamination as
a direct result of either proposed Miami or Fort Pierce disposal sites.
76
-------
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Analysis," Journal of the Hydraulics Division. American Society of Civil
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Bane, J. M., and Brooks, D. A. 1979. "Gulf Stream Meanders Along the
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Bane, J. M. , and Dewar, W. K. 1988. "Gulf Stream Bimodality and Variability
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Brandsma, M. G., and Divoky, D. J. 1986. "Development of Model for
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Brooks, L. H. 1979. "Fluctuations in Transport of the Florida Current at
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Brooks, D. A., and Bane, J. M. 1983. "Gulf Stream Meanders off North
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Brooks, D. A., and Bane, J. M. 1978. "Gulf Stream Deflection by a Bottom
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Duing, W. 1975. "Synoptic Studies of Transients In the Florida Current,"
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Duing, W., Moores, N. K., and Lee, T. N. 1977. "Low-Frequency Variability
in the Florida Current and Relation to Atmospheric Forcing from 1972 to 1974,"
Journal of Marine Research. Vol 35, pp 129-161.
Hall, H. M. 1986. "Horizontal and Vertical Structure of the Gulf Stream
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Hood, P. L. 1985. "Surface Energetics of the Gulf Stream Cyclonic Frontal
Zone off Onslow Bay, North Carolina," Journal of Geophysical Research. Vol 88,
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Jensen, R. E. 1983 (Jan). "Atlantic Coast Hindcast, Shallow-Water
Significant Wave Information," WIS Report 9, US Army Engineer Waterways
Experiment Station, Vicksburg MS.
77
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Johnson, B. H. 1987 (Jul). "Users Guide for Models of Dredged Material
Disposal in Open Water," Draft Technical Report, US Army Engineer Waterways
Experiment Station, Vicksburg, MS.
Johnson, B. H. , and Holliday, B. W. 1978. "Evaluation and Calibration of the
TETRA TECH Dredged Material Disposal Model Based on Field Data," Technical
Report, D-78-47, US Array Engineer Waterways Experiment Station, Vicksburg, MS.
Johnson, B. J., Trawle, M. J., andAdamec, S. A. 1988. " Dredged Material
Disposal Modeling in Puget Sound," Journal of the Waterway. Port. Coastal and
Ocean Division. American Society of Civil Engineers, Vol 114, No. 6,
pp 700-713.
Learaan, K. D. , and Vertes, P. S. 1982. "The Subtropical Atlantic Climate
Study (STACS), Summary of RSMAS Pegasus Observations in the Florida Straits,"
Technical Report, UM RSMAS No. 83012, University of Miami, Rosenstiel School
of Marine and Atmospheric Science, Miami, Florida.
Lee, T. N. 1975. "Florida Current Spin-Off Eddies," Deep Sea Research,
Vol 22, pp 753-765.
Lee, T. N. 1972. "Florida Current Spin-Off Eddies," Ph.D Dissertation,
Florida State University, Tallahassee, Florida.
Lee, T. N., and Atkinson, L. P. 1983. "Low Frequency Current and
Temperature, Variability from Gulf Stream Frontal Eddies and Atmospheric
Forcing along the Southeast U.S Outer Continental Shelf," Journal of Geophysi-
cal Research. Vol 88, No. C8, pp 4541-4567.
Lee, T. N., Atkinson, L. P., and Legeckis, R. 1981. "Observation of a Gulf
Stream Frontal Eddy on the Georgia Continental Shelf, April 1977," Deep sea
Research, Vol 29, pp 347-378.
Lee, T. N., Brooks, I., and Duing, W. 1977. "The Florida Current: Its
Structure and Variability," Technical Report UM-RSMAS, No. 77003,
The University of Miami, Rosenstiel School of Marine and Atmospheric Science,
Miami, FL.
Lee, T. N., Ho, J. W. , Kourafalou, V., and Wang, J. D. 1984. "Circulation on
the Continental Shelf of the Southeastern United States. Part I: Subtidal
Response to Wind and Gulf Stream Forcing During Winter," Journal of Physical
Oceanography. Vol 14, No. 6, pp 1001-1012.
Lee, T. N., and Mayer, D. A. 1977. "Low Frequency Current Variability and
Spin-Off Eddies along the Shelf off Southeast Florida," Journal of Marine
Research. Vol 35, No. 1, pp 193-220.
Lee, T. N. , and Mooers, N. K. 1977. "Near Bottom Temperature and Current
Variability over the Miami Slope and Terrace," Bulletin of Marine Science,
Vol 27, No. 4, pp 758-775.
Lee, T. N., and Waddel, E. 1983. "On Gulf Stream Variability and Meanders
Over Black Plateau at 30 N," Journal of Geophysical Research. Vol 88, No. C8,
pp 4617-4631.
Legeckis, R. 1979. "Satellite Observations of the Influence of Bottom
Topography on the Seaward Deflection of the Gulf Stream off Charleston, South
Carolina," Journal of Physical Oceanography. Vol 9, pp 483-^97.
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Legeckis, R., and Bane, J. M. 1983. "Comparison of the TRISO-N Satellite and
Air Craft Measurements of Gulf Stream Surface Temperatures , " Journal of
Geophysical Research. Vol 88, No. C8, pp 4611-4616.
Leipper, D. F. 1967. "A Sequence of Current Patterns in the Gulf of Mexico,B
Report 67-9T, Texas A&M University, College Station, Texas.
Levine, E. R. , Connors, P. C. , Cornillon, P. C., and Rossby, H. T. 1986.
Gulf Stream Kinematics along an Isopycnal Float Trajectory," Journal of
Physical Oceanography. Vol 16, pp 1317-1328.
Osgood, E. K. , Bane, J. M. , and Devar, K. U. 1987. "Vertical Velocities and
Dynamical Balances in Gulf Stream Meanders," Journal of Geophysical Research.
Vol 92, No. C12, pp 13029-13040.
Reese, S. I. 1988. "Personal dommunication on Short-Term Simulation of
Disposal Operations in Mobile Harbor," Al.
Richardson, P. L. 1985. "Average Velocity and Transport of the Gulf Stream
Near 55 W," Journal of Marine Research. Vol 43, pp 83-111.
Richardson, U. S., Schmitz, W. J. , and Niller, P. P. 1978. "The Velocity
Structure of the Florida Current from the Straights of Florida to Cape Fear,"
Deep Sea Research, Vol 16, pp 225-234.
Richardson, W. S., and Schmitz, U. J. 1965. "A Technique for the Direct
Measurement of Transport with Application to the Straits of Florida," Journal
of Marine Research. Vol 23, No. 2, pp 172-185.
Rinkel, M., Vargo, S., Lee, T. N. , Schott, F., Zantopp, R. , Leaman, K., Smith,
K., Maul, G., and Proni, J. 1986. "Physical Oceanography Study of Florida's
Atlantic Coast Transport Study," Florida Institute of Technology,
St. Petersburg, FL.
Rossby, T. A., Bower, S., and Shaw, P. T. 1985. "Particle Pathways in the
Culf Stream," Bulletin, American Meteorological'Society, Vol 66, No. 9,
pp 1106-1110.
Scheffner, N. U. (in preparation). "Dredged Material Disposal Numerical
Modeling for Site Selection in New York Bight," Technical Report, Coastal
Engineering Research Center, US Army Engineer Waterways Experiment Station,
Vicksburg, MS.
Schott, F. A., Lee, T. N., and Zantopp, R. 1988. "Variability of Structure
and Transport of the Florida Current in the Period Range of Days to Season,"
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Currents on the South Carolina Continental Shelf," Journal of Geophysical
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Smith, N. P 1983. "Temporal and Spatial Characteristics of Summer Upwelling
along Florida's Atlantic Shelf," Journal of Physical Oceanography. Vol 13, pp
1709-1715.
Smith, N. P. 1982 "Response of Florida Atlantic Shelf U'acers to Hurricane
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Stommel, H 1965 "The Culf Stream' A Physical and Dynamic Description,"
79
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University Press, Berkeley, California, and Cambridge University Press,
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Swain, A. 1988. "Open Water Dredged Material Disposal Site for Port
Everglades, Florida," Memorandum for Records, Coastal Engineering Research
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Swart, D. H. 1976. "Predictive Equations Regarding Coastal Transports,"
Proceedings of the 15th Coastal Engineering Conference. Honolulu, Hawaii.
Tapp, R. L. 1988. "Personnel Communication on Dredges and Dredged Material
Characteristics associated with the Proposed Miami and Fort Pierce Disposal
Sites".
Vemulakonda, S. R., Scheffner, N. W., Earickson, J. A., and Chou, L. V.
1988. "Kings Bay Coastal Processes Numerical Model," Technical Report
CERC-88-3, US Army Engineer waterways Experiment Station, Vicksburg, MS.
Webster, F. A.. 1961. " A Description of Gulf Stream Meanders off Onslow
Bay," Deep Sea Research, Vol 8, pp 130-143.
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Meanders: A Closed Look in June-July 1984," Journal of Physical Oceanography.
Vol 17, No 5.
SO
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APPENDIX C
MIAMI ODMDS
SITE MANAGEMENT AND MONITORING PLAN
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MIAMI ODMDS
Site Management and Mnnirorina Plan
Introduction. It is the responsibility of EPA under the Marine
Protection, Research, and Sanctuaries Act (MPRSA) of 1972 to
manage and monitor each of the Ocean Dredged Material Disposal
Sites (ODMDSs) designated by the EPA pursuant to Section 102 of
MPRSA. As part of this responsibility, a management and
monitoring plan has been developed to specifically address the
deposition of dredged material into the Miami ODMDS.
Site Management and Monitoring Team. An interagency Site
Management and Monitoring team, consisting of representatives of
EPA, COE, State of Florida, NOAA-AOML, University of Miami, and
the Port of Miami has been established to review and comment on
all Miami ODMDS management and monitoring activities. Other
agencies will be asked to participate where appropriate. This
SMMP team will evaluate existing monitoring data, the type of
proposed disposal (i.e., O&M vs. construction), the type of
material (i.e., sand vs. mud), location of placement within the
ODMDS and quantity of proposed material. This team will make
recommendations to the responsible agency on appropriate
monitoring techniques, level of monitoring, significance of
results and potential management options.
SITE MANAGEMENT
Section 228.3 of the Ocean Dumping Regulations (40 CFR 228.3)
defines ODMDS site management as "..regulating times, rates, and
methods of disposal and quantities and types of materials
disposed of; developing and maintaining effective ambient
monitoring programs for the site; conducting disposal site
evaluation studies; and recommending modifications in site use
and/or designation." The plan may be modified if it is
determined that such changes are warranted as a result of
information obtained during the monitoring process.
Management Objectives. There are three primary objectives m the
management of each ODMDS. These are:
o Protection of the marine environment;
o Beneficial use of dredged material whenever practical; and
o Documentation of disposal activities at the ODMDS.
The following sections provide the framework for meeting these
objectives to the extent possible.
-------
Miami ODMDS Site Management and Monitoring Plan Angust 1995
Material volumes. The Miami ODMDS was first used in April, 1990
for disposal of maintenance material. Because routine
maintenance dredging is sporadic, the next expected disposal at
the proposed ODMDS should be the newly authorized deepening of
the Federal Miami Harbor Project. Approximately five million
cubic yards is expected to be disposed within the ODMDS from this
project. Subsequent maintenance dredging should not occur until
2000.
TABLE: Volumes Disposed and Estimated Volumes of Material to be
Disposed at Miami Site
Completion Type of Volume Composition
Date Action (cubic yards)
1990
1995
1995
1996
Maintenance 225,000
U.S. Coast Guard 3,000
Basin
NOAA Restoration 300
Deepening Proj. 5,000,000
silt/clay
sand/gravel
limerock rubble
sand/silt/
clay/rabble
2000
Maintenance
250,000
silt/clay
Because the site is located in deep water (427 to 785 ft.), no .
restrictions are presently placed on disposal volumes. Disposal
of unrestricted volumes is dependent upon results from future
monitoring surveys.
Material suitability. Two basic sources of material are expected
to be placed at the site, i.e. construction or new wDrk dredged
material and maintenance dredged material. These sediments will
consist of mixtures of silt, clay and sand, in varyi ig
percentages.
The disposition of any significant quantities of bea':h compatible
sand from future projects will be determined during permitting
activities for any such projects. It is expected that the State
of Florida will exercise its authority and responsibility,
regarding beach nourishment, to the full extent during any future
permitting activities. Utilization of any significant quantities
of beach compatible dredged material for beach nourishment is
strongly encouraged and supported by EPA where environmentally
acceptable. Disposal of coarser material should be planned to
allow the material to be placed so that it will be within or
accessible to the sand-sharing system, to the maximum extent
practical, and following the provisions of tine Clean Water Act.
In addition, the suitability of dredged material for ocean
2
EI* \ Return 4
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Miami QDMOS Site Management and Monitoring Plan
August 1995
disposal must be verified by the COE and agreed to by EPA prior to
disposal. Verification will be valid for three years from the
time last verified with the option of a two year extension.
Verification will involve: 1) a case-specific evaluation against
the exclusion criteria (40 CFR 227.13(b)), 2) a determination of
the necessity for bioassay (toxicity and bioaccumulation) testing
for non-excluded material based on the potential for contamination
of the sediment since last tested, and 3) carrying out the testing
and determining that the non-excluded, tested material is suitable
for ocean disposal.
Documentation of verification will be completed prior to use of
the site. Documentation for material suitability for dredging
events proposed for ocean disposal more than 5 years since last
verified wili be a new 103 evaluation and public notice.
Documentation for material suitability for dredging events
proposed for ocean disposal less than 5 years but more than 3
years since last verified will be an exchange of letters between
the COE and EPA.
Should EPA conclude that reasonable potential exists for
contamination to have occurred, acceptable testing will be
completed prior to use of the site. Testing procedures to be used
will be those delineated in the 1991 EPA/COE Dredged Material
Testing Manual and 1992 Regional Implementation Manual. This
includes how dredging operations will be subdivided into project
segments for sampling and analysis. Only material determined to
be suitable through the verification process by the COE and EPA
will be placed at the designated ocean disposal site.
Time of disposal. At present no restrictions have been determined
to be necessary for disposal related to seasonal variations in
ocean current or biotic activity. If new information indicates
that endangered or threatened species are being adversely
impacted, seasonal restrictions may be incurred.
The disposal of dredged material with a median grain size of less
than 0.125 mm and material with a composition consisting of
greater than 10% fine grained material (grain size of less than
0.074mm) by weight will be halted at the Miami ODMDS during
periods of onshore current eventst An approved real-time current
monitoring program must be implemented by the user prior to
disposal to ensure that fine grained sediments disposed at the
Miami ODMDS are not transported to area reefs and hardbottoms.
Disposal Technique. No specific disposal technique Ls required
for this site. Dredged material will be placed within a 500 foot
radius of the center of site to additionally ensure protection of
live bottom communities outside of the site and to contain the
majority of the disposal mound and plume within the ODMDS
boundaries during periods of strong currents.
3
EI* \ Region 4
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Miami ODMDS Site Management and Monitoring Plnn
August 1995
SITE MONITORING
The MPRSA establishes the need for including a monitoring program
as part of the Site Management Plan. Site monitoring is conducted
to ensure the environmental integrity of a disposal site and the
areas surrounding the site and to verify compliance with the site
designation criteria, any special management conditions, and with
permit requirements. Monitoring programs should be flexible, cost
effective, and based on scientifically sound procedures and
methods to meet site-specific monitoring needs. A monitoring
program should have the ability to detect environmental change and
assist in determining regulatory and permit compliance. The
intent of the program is to provide the following:
(1) Information indicating whether the disposal activities
are occurring in compliance with the permit and site
restrictions; and/or
(2) Information concerning the short-term and long-term
environmental impacts of the disposal; and/or
(3) Information indicating the short-term and long-term fate
of materials disposed of in the marine environment.
The main purpose of a disposal site monitoring program is to
determine whether dredged material site management practices,
including disposal operations, at the site need to be changed to
avoid significant adverse impacts.
Baseline Monitoring. The results of investigations presented in
the designation EIS will serve as a general pre-disposal
characterization of the ODMDS and nearby vicinity (see EIS
Appendix A). Site specific investigations included: 1985
Environmental Survey in the Vicinity of An Ocean Dredged Material
Disposal Site, Miami Harbor, Florida; and 1986 Miami Harbor
Interim Ocean Dredged Material Disposal Site Video Survey.
A bathymetric survey will be conducted by the COE or site user not
more than 60 days prior to the dredging cycle or project disposal.
The surveys will be taken along lines spaced at 500 foot intervals
or less and be of sufficient length to adequately cover the
disposal area. Accuracy of the surveys will be +. 0.5 feet. These
surveys will be referenced to the appropriate datum and corrected
for tide conditions at the time of survey.
Disposal Monitoring. For all disposal activities, the dredging
contractor will be required to prepare and operate under an
approved electronic verification plan for all disposal operations.
As part of this plan, the contractor will provide an automated
system that will track (1 to 5 minute intervals) the horizontal
location and draft condition (vertical) of the disposal vessel
from the point of dredging to the disposal area, and return to the
point of dredging. Required digital data for each load are as
fol1ows:
/¦./'I 4
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Miami ODMDS Site Management and Monitoring Finn August 1995
(a) Date;
(b) Time;
(c) Vessel Name;
(d) Dump Number;
(e) Map Number on which dump is plotted (if appropriate);
(f) Beginning and ending coordinates of the dredging area
for each load;
(g) Actual location at points of initiation and completion
of.disposal event and the compass heading at the
beginning of each dump;
(h) Description of material disposed, e.g., rock, sand,
silt, or clay;
(i) Volume of material disposed; and
(j) Disposal technique used.
As a precaution to protect marine mammals as well as sea turtles
during disposal operations, a bow observer will be stationed on
vessels participating in disposal activities.
As a follow-up to the baseline bathymetric survey, the COE or
other site user will conduct a bathymetric survey within 30 days
after disposal. The number of transects required will be the same
as in the baseline survey. The user will be required to prepare
daily reports of operations and submit to the COE a monthly report
of operations for each month or partial month's work. The user is
also required to notify the COE and EPA within 24 hours of
becoming aware of a violation of the permit and/or contract
conditions during disposal operations.
Material Tracking. Based on the type and volume of material
disposed, various monitoring surveys may be used to determine if
and where the disposed material is moving.
The primary concern regarding use of the Miami ODMDS is the
potential for adverse impact on nearshore reefs due to short and
long-term transport of dredged material from the ODMDS and
subsequent sedimentation and/or light attenuation. The management
requirements discussed previously have been adopted to minimize
this potential. To further quantify the potential of impact, the
Site Management and Monitoring Team has decided to focus
monitoring efforts on analysis of the transport mechanisms at the
ODMDS.
The Site Management and Monitoring Team has identified two major
monitoring objectives: 1) Assess intensity and frequency of
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Miami ODMDS Site Managemtnl and Monitoring Plan
August 1995
disposal plumes reaching nearshore reefs, 2) Assess the potential
for long-term transport of dredged material towards critical
habitats. Additional objectives may be added as new information
is obtained from the current monitoring system and from the
studies described below.
Objective 1
Field studies will be conducted during the current Miami-Harbor
Deepening Project to quantify disposal plume concentrations during
onshore current events due to Florida Current Spinoff Eddies.
Data collected from these field studies will be used to calibrate
computer models for at least two separate current regimes (eddy
present and eddy absent) for assessing the intensity and frequency
of disposal plumes reaching nearshore reefs. Results from the
computer modelling will be examined with respect to potential
impact on the reef communities. Based on the expected impact, the
real-time current monitoring management requirement can be
modified or discontinued. The monitoring plan for this objective
is currently under development.
Objective 2
Field studies will be conducted to quantify bottom currents and
dredged material resuspension at the Miami ODMDS. Data collected
from these field studies will be used m calibrating computer
models for assessing the potential for long-term transport of
dredged material towards critical habitats. Should the modelling
indicate that significant quantities of dredged material will
reach critical habitats, management techniques will be examined or
the ODMDS will be relocated. The monitoring plan for this
objective is currently under development.
Reporting and Data Formatting. Disposal summary reports should be
provided by the COE to EPA within 45 days after project
completion. These should consist of dates of disposal, volume of
disposal, approximate location of disposal and pre- and post-
disposal bathymetric survey results in both hard copy and
electronic formats. Other disposal data should be available upon
request. In addition, EPA should be notified of ODMDS use 15 days
prior to dredging cycle or project disposal.
A brief report on the real-time monitoring results should be
provided to SMMP team members by the permittee within 45 days
after project completion. This report should include: number of
times disposal was delayed due to restricted current conditions;
the date, time and duration of each delay; any operational or
logistical inconsistencies or complications in conducting this
program; and any conclusions or recommendations.
Material tracking, disposal effects monitoring and any other data
collected should be provided to SMMP team members and federal and
state agencies as appropriate. Data will be provided to other
interested parties requesting such data to the extent possible.
Data will be provided for all surveys in a report generated by the
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Miami ODMDS Site Management and Monitoring Plan
August 1995
action agency. The report should indicate how the survey relates
to the SMMP and previous surveys at the Miami ODMDS and should
provide data interpretations, conclusions, and recommendations,
and should project the next phase of the SMMP.
Modification of ODMDS SMMP. The SMMP will be modified on an as
needed basis. Should the results of the monitoring surveys
indicate that continuing use of the ODMDS would lead to
unacceptable impacts, then either the ODMDS Management Plan will
be modified to alleviate the impacts, or the location of the ODMDS
would be modified. In addition, should the results of the
monitoring surveys indicate that specific management practices are
not needed, then the SMMP would be modified. The SMMP will be
reviewed and revised if appropriate at a minimum of every ten
years.
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APPENDIX D
MIAMI OCEAN DREDGED MATERIAL DISPOSAL SITE DESIGNATION
FLORIDA COASTAL ZONE MANAGEMENT PROGRAM
CONSISTENCY EVALUATION
Submitted by:
U.S. Environmental Protection Agency
Region IV
August 1995
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Florida Coastal /.one Management Program Consistency Evaluation
August 1995
I. INTRODUCTION
The U.S. Environmental Protection Agency (EPA), in cooperation with the
U.S. Army Corps of Engineers (COE), has prepared an Environmental Impact
statement (EIS) titled "Environmental Impact Statement For Designation of a
Miami, Florida Ocean Dredged Material Disposal Site." This EIS evaluates the
environmental conditions relevant to the designation of an ocean disposal site
offshore Miami, Florida. Additionally, the EIS evaluates the proposed Miami
site according to the eleven environmental criteria required for site
designations under 40 CFR 228.6 (Ocean Dumping Regulations).
The site proposed for final designation is the Miami site that received
an EPA interim designation (40 CFR 228.12) and was used for dredged material
disposal for the first time in April 1990. The total area of the proposed
site is 1 square nautical mile (nmi). The western boundary of this site is
located 3.6 ami east of Virginia Key, Florida in the Atlantic Ocean. Since
April 1990, approximately 300,000 cubic yards of dredged material have been
disposed at the interim site.
The site designation is needed in this area to provide an ocean disposal
option for dredging projects in the area. Potential sources of the dredged
material are Government Cut, the Port of Miami channels and turning basins,
and the Miami Harbor Deepening Project. It should be emphasized that final
designation of the interim Miami site does not by itself authorize any
dredging or on-site disposal of dredged material. EPA and the COE must
conduct an environmental review of each proposed ocean disposal project. That
review ensures that there is a demonstrated need for ocean disposal and that
the material proposed for disposal meets the requirements for dredged material
given in the Ocean Dumping Regulations.
II. THE FLORIDA COASTAL ZONE MANAGF.MF.NT PROGRAM (CZMP)
There are eight Florida statutes relating to ocean disposal site
designations. This assessment discusses how the referenced EIS for thg Miami
site designation will meet the CZMP objectives to protect coastal resources
while allowing multiple use of coastal areas. Consult the EIS for further
data and information.
Although the EIS serves a dual role of NEPA documentation for site
designation and COE permitting under Section 103 of the Marine Protection,
Research, and Sanctuaries Act (MPRSA) of 1972, as amended (see Section 2.01 of
EIS), this CZMP consistency evaluation is only relevant for si :e designation.
Therefore, COE permitting actions will need a separate CZMP co i:ustency
evaluation.
A. Chapter 161: Beach and Shore Preservation
The intent of Chapter 161 is the protection of thousands of miles of
Florida's coastline by regulating construction activities near and within
these areas. The Miami site designation will, by itself, require no new
construction and therefore no related support activities will t e; subject to
the construction regulations in this chapter
The western boundary of the Miami ODMDS is located 3.6 nxr l from Virginia
Key, the nearest beach and shore-related amenity. Sediment transport an the
vicinity of the site is driven mainly by the Florida Current. However, eddy
currents associated with the Florida Current have been shown to occur within
this area. Modelling, which has been compared to field studies, has indicated
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that these frontal eddies should not result in significant transport of
dredged material toward the shore. In addition, provisions have been
established in the Site Management and Monitoring Plan to ensure that
transport does not occur toward the shore. In the event that significant
accumulation of the dredged material towards any amenity is evident, use of
the site can be modified or terminated by EPA.
B. Chanter 253: State Land?
This chapter addresses the responsibilities of the State Board of
Trustees in managing the State sovereign lands by issuing leases, easements,
rights of way, or other forms of consent for those wishing to use State lands,
including State submerged lands.
Since the Miami site is not within State waters, Chapter 253 is not
re 1evant.
C. Chapter 258: State Parks and Preserves
Figure 5 in the EIS locates the Parks and Preserves in the vicinity of
the proposed Miami site. As similarly discussed in Section A above, the
distance from these areas to the proposed site should prevent any impacts to
these areas from use of the site.
D. Chapter 267: Historic Preservation
There are no known features of historical importance in the vicinity of
the proposed site, and therefore it is unlikely that the proposed site
designation will result in any impact to these areas. The bottom video survey
of the ODMDS did not reveal any new such areas.
E. Chapter 288: Commercial Development and Capital Improvements:
Industrial Siting Act
The final designation of the Miami site provides an environmentally
acceptable ocean location for the disposal of dredged material that meets the
Ocean Dumping Criteria. If ocean disposal is selected as the most feasible
option for a dredged material disposal project, this site designation ensures
that an ocean disposal option is available in the area. Therefore, the
designation removes one barrier to free and advantageous flow of commerce in
the area in that dredging projects and their associated navigational benefits
cannot be halted due to the lack of an acceptable ocean disposal site.
The Industrial Siting Act is not applicable to this proposed site
designation.
F. Chapter 370: Saltwater Fisheries
Chapter 370 ensures the preservation, management and protection of
saltwater fisheries and other marine life. Most commercial and recreational
fishing activity in the Miami vicinity is concentrated in inshore and
nearshore waters. No natural hardbottom areas are known to occur in proximity
to the proposed site. The nearest fisheries area is located about 1.3 nmi
from the site. In short, the Miami site does not represent a unique habitat
for any of the important commercial or recreational fisheries. Use of the
site will smother the non-motile or slow moving benthic organisms at the site.
However, the ability of these organisms to recolonize in similar sediments
render 3 this impact short-term and insignificant. Should the disposed
material differ m grain-size, other benthic organisms would likely colonize
the area. The EIS served as the Biological Assessment from which the National
Marine Fisheries Service (IIMFS) determined that populations of
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August 1993
endangered/threatened species under their purview would not be adversely
affected by the designation and use of the ODMDS (See FEIS section 7.03).
G. Chapter 37 6: Pollutant Discharge Prevention and Removal
Possible effects associated with the use of this site are local
mounding, temporary increases in turbidity and the smothering of benthic
organisms. The effect on the benthos should be minor as discussed in Section
F above. The great depths at the site will ensure that any mounding does not
become a hazard to navigation. Turbidities resulting from use of the site
will be temporary. Any suspended sediments remaining in the water column will
be diluted and dispersed so that the long term effect would not be greater
than ambient suspended solids concentrations. This is supported by the results
of dispersion modelling, which has been compared to field studies and has
indicated that these frontal eddies should not result in significant transport
of dredged material toward the shore. In addition, provisions have been
established in the Site Management and Monitoring Plan to ensure that
transport does not occur toward the shore.
Any material proposed for ocean disposal must meet the criteria given in
40 CFR Part 227 (Ocean Dumping Criteria) . EPA and the COE will continue to
monitor the site as long as it is used to detect movement of the material and
any associated impacts. The Site Management and Monitoring Plan (SMMP) for
the Miami ODMDS is included in the EIS (see Appendix C).
H. Chapter 403: Environmental Control
The principle concerns raised in this chapter are similar to those
addressed in many of the chapters discussed above: pollution control, waste
disposal and dredging.
The COE and EPA will evaluate all federal dredged material disposal
projects in accordance with the EPA criteria given m the Ocean Dumping
Regulations (40 CFR Sections 220-229), the COE regulations (33 CFR 209.120 and
209.145), and any state requirements. The COE will also issue permits to
private dredged material disposal projects after review under the same
regulations. EPA has the right to disapprove any ocean' disposal project if,
in its judgement, all provisions of the MPRSA and associated implementing
regulations have not been met.
III. CONCLUSIONS
Based on the information presented in the EIS and the above summary, EPA
concludes that the proposed designation of the Miami ODMDS is consistent with
the Florida CZMP to the extent feasible.
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APPENDIX E
EVALUATION OF THE
MIAMI OCEAN DREDGED MATERIAL DISPOSAL SITE (ODMDS)
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CEWF.S-CR-P
21 March 1995
Evaluation of the Miami Ocean Dredged Material Disposal Site (ODMDS)
Introduction
1. Limited capacity in existing disposal sites for dredged material in the Miami, Florida area
combined with the planned deepening of the Miami Harbor creates a need to designate an
environmentally acceptable, adequately sized, and economically feasible offshore Qcean Dredged
Material Disposal Site (ODMDS). In December 1987, the US Army Engineer District,
Jacksonville (SAJ) requested assistance from the US Army Engineer Waterways Experiment
Station's Coastal Engineering Research Center (CERC) to perform a site designation investigation
of the proposed ODMDS offshore of Miami, see Figure la. Figure lb shows the bathymetry at
the proposed ODMDS. The purpose of the study was to determine the acceptability of the site
with respect to the potential effects of the dredging operation on live coral reef areas located
shoreward of the ODMDS. Specifically, the question was whether material from the ODMDS
could be transported from the disposal site and deposited onto coral reefs located along the
adjacent coast.
2. Conclusions of the study were reported by Scheffner and Swain (1989) and indicated that the
proposed disposal site did not pose a threat to the live reef areas. These conclusions were based
on numerical model simulations of: 1) the short-term (Johnson et al. 1988) fate and transport of
material in the water column from the disposal site to the reef and 2) a long-term (Scheffner
1989) simulation of the erosion and transport from a non-cohesive disposal mound located in the
ODMDS. Because data were not available for validation of the short-term modeling results, no
quantitative verification of the results were presented in the initial report. Additionally, the long-
term transport was limited to non-cohesive material of a single, uniform grain size.
3. Although the numerical approach adopted for the study represented the state-of-the-art in
disposal site analysis, the lack of model verification to prototype measurements has resulted in a
reluctance to accept the conclusion that the disposal site will not adversely impact the coral reefs.
As a result of these concerns, the proposed ODMDS designation request may not be approved by
the Florida State Department of Environmental Resources (DER). Although these concerns are
valid, the amount of data necessary for such a verification has never been available and such data
collection effort was not planned as a component 6f the original study. However, an acceptable
and cost effective ODMDS must be located and approved in the near future; otherwise, SAJ
dredging activities in the Miami area will have to be terminated.
4. At the time that the numerical model tests were run, the technology was not available to
monitor the spatial and temporal variations that occur during the disposal of dredged material.
However, during a field data collection activity in Mobile, Alabama (Kraus 1991), it was shown
that such measurements could be accurately taken acoustically. This acoustic technology along
with conventional sampling techniques were used to monitor the proposed Miami ODMDS (Proni
et al. 1991 and Tsai et al. 1992) in a joint field data collection project performed by the Atlantic
Oceanographic and Meteorological Laboratory (AOML) of the National Oceanic and Atmospheric
Administration, SAJ, and CERC.
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5. In response to a recent request by SAJ, a cooperative effort between Rosenstiel School of
Marine and Atmospheric Science (RSMAS) of the University of Miami, AOML, and CERC has
been undertaken. RSMAS provided data describing the environmental conditions at the study
site. AOML analyzed field data, and CERC utilized predictive numerical models to characterize
movement of suspended material and bottom sediments at the ODMDS. This memorandum
describes the use of theory and field measurements to address all reservations concerning the
conclusions reached by the original numerical modeling investigation and provides predictions
based on the most recent model versions. The following three sections summarize findings with
respect to: 1) analyzing water samples and developing a theoretically based and field calibrated
acoustic backscatter versus sediment concentration curve, 2) running of the Short Term FATE
(STFATE) model with hydrodynamic data specified according to the field conditions which
occurred during monitoring and are representative of the site, and 3) performing an analysis of
the potential resuspension and transport of bottom sediment at the site.
Field Measurements
6. The primary concern of the DER is founded on the lack of verification of the numerical
model predictions of suspended sediment concentrations at the reef area. The 1990-91 field data
collection project at Miami produced the data capable of providing quantitative verification of the
numerical model predictions. The field monitoring was comprised of three phases. During the
first field monitoring project, which was conducted from 24 to 26 April 1990, conductivity,
temperature, current, and total suspended solids (TSS) concentration measurements were
obtained. Water samples were gathered with a water sampling arrangement utilizing a towed
body in which the entrance port of a pumping system was mounted at a depth between 3 and 8
meters below the ocean surface. This is the only portion of the water column from which water
samples were obtained. On 28 August 1990, a second field collection exercise was conducted, in
which Rhodamine dye was introduced into the hopper of the dredge while enroute to the disposal
site. After disposal, the residual plume was monitored using NOAA's Acoustic Concentration
Profiler. Water samples were drawn from the residual plume and analyzed for the presence of
dye with a Turner Fluorometer. No dredged material discharges occurred during the third
monitoring period, 26-28 June 1991, due to dredging contractors scheduling. This effort was
undertaken to gather background water samples only.
7. It is desirable to compare acoustical measures of TSS with conventional water samples in
order to obtain an empirical calibration of the relationship between acoustic backscatter intensity
and suspended material for each particular dredged material and disposal site. However, the
20kHz system, used in phase one of the field exerfcise, has a certain zone (several meters adjacent
to the transducer face), over which the data becomes saturated from immediate return. Because
of the method of the pumped sampling and limitations of the acoustical data at locations where
water samples were collected, a calibration of the acoustical data to field measurements is
difficult.
Sample Analysis
8. Despite the inability to perform an acoustic calibration to field data, it was determined that
analyzing the existing samples would provide valuable information regarding the residual plume
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left after dredged material discharge. Tsai et al. (1992) determined that, although the bulk of
the discharged material descends as a viscous mass, a small portion, perhaps in the form of
individual fines, remains within the water column.
9. TSS concentrations were determined by AOML from pumped samples (Proni et al. 1993)
taken from residual plumes as they moved along a nearly straight path to the North-Northeast.
Values for all samples of dredged material discharges plotted against time are shown in Figure 2.
Data from three of the discharges have been selected and included in Figure 3 to obtain a
smoother estimate of dilution with time (or distance) from the discharge. A curve can be fit to
the data to give an estimate of the normalized dilution with time or distance for discharges
occurring within the designated site. From Figure 3, a dilution factor of 0.1 occurs 20 minutes
after discharge. For example, an initial concentration of 80 mgIt (no bottle samples exceeded a
concentration of 80 mg It) would diminish to 8 mg/f after 20 minutes or at a distance of 600 m
from the point of discharge (current speed assumed to be 50 cm/s). The dilution factor decreases
to approximately 0.05 at 45 minutes. The concentration in the example becomes 4 mg/f at a
distance of 1350 m. The maximum background concentration measured in June 1991 was 3.1
mg/f. Therefore, the TSS concentration of dredged material will not impact the coral reefs a
distance of about 3 miles ( = 5000 m) from the ODMDS with concentrations in excess of
background levels.
Acoustic Calibration
10. Because it was not possible to perform an acoustic calibration to TSS samples taken in the
field, an alternate method had to be devised to produce concentration data which would be used
to determine if the Short Term FATE (STFATE) model was producing concentration values
within an order of magnitude of those obtained in the field. It was determined that.the
environmental conditions (i.e. grain size, cohesiveness, salinity) at the disposal site could be
adequately represented in the conversion from acoustic backscatter to concentration by acoustical
theory calibrated to field data. The acoustical theory used in the conversion has been elucidated
by Thevenot and Kraus (1993). The concentration ratio between a scattering volume and a
volume of known concentration is given by
C = 10{K ' °5'] W
where a = 0.1 according to theory, and K is a site specific constant.
11. The coefficients a and K are typically determihed empirically through fitting to field data.
Because field data corresponding to acoustic backscatter measurements are not available, the
theoretical value 0.1 is used for a. Bottom grab samples taken at the Miami dredging operations
were found to be similar to the material disposed during the Mobile, Alabama field data
collection project. Therefore, it was determine that the same value for K (6.78) would be used in
this study. Figure 4 (from Ogushwitz 1992) shows a comparison of data taken from two acoustic
instruments at Mobile, Alabama, the best fit to the data greater than 10 mg/f, and the theoretical
backscatter versus concentration relationship. This figure shows that the best fit line deviates
only slightly from the theoretical line for concentration values greater than 10 mg/f. Converting
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die Miami acoustical measurements using the above theory will provide estimated concentration
within an order of magnitude for concentrations ranging from 10 to 1000 mgIt (Ogushwitz
1992).
Short Term Fate Analysis
12. In order to run STFATE, four types of input data are required. The first two types of input
data pertain to the ambient conditions at the disposal site. Specifically, a density profile of the
water column is required as well as an indication of the current velocities at the site. Because
Scheffner and Swain (1989) were criticized for using depth averaged velocities, the velocity
profile option of STFATE was selected. Input is also required regarding the material to be
disposed and the dimensions and velocity of the disposal vessel.
Verification to Prototype Data
13. The primary concern expressed by the DER regarding the Scheffner and Swain (1989) study
was that the STFATE model was not verified to prototype data. Therefore, an initial set of
STFATE runs were made with the input parameters which coincided with a dredged material
discharge operation monitored on 26 April 1990 (Proni et al 1991). Although several disposal
operations were monitored, the disposal associated with the highest quality acoustic data was
selected for verification of the STFATE model due to limited time to complete the study.
Density stratification information that occurred at the time of the disposal was derived from
measurements of conductivity, temperature, and depth taken during the monitoring project. An
Acoustic Doppler Current Profiler obtained current profiles, and these data were used as input to
STFATE. Grain size information was obtained from a bottom grab sample taken from the
channel being dredged. The final input required are the dimensions of the vessel and its speed
during disposal. Estimates of the dimensions of a typical disposal vessel were the same, as used
in Scheffner and Swain (1989). The speed of the vessel at disposal was estimated based on
observations of the disposal operations.
14. After all of the required input information was obtained, vertical contours of TSS
concentration were developed for the STFATE simulations and compared to concentration
measured with acoustic techniques. The acoustic backscatter was converted to concentration
using the relationship discussed above. The residual plume was followed during the acoustic
monitoring by visual observation of the surface plume, thus the vertical concentration profiles
from the STFATE model were taken at the highest concentration for the least depth of calculation
and were consistent throughout the water column.' Six passes were made through the discharge
plume, covering the period between disposal and 25 minutes after disposal. Because each pass
through the plume took over 150 sec, the spatial distribution shown in the acoustic transects may
vary from the snapshot of the water column developed to represent the STFATE model output.
However, this difference was considered to be well less than an order of magnitude. Because
data was previously unavailable to verify the spatial and temporal distribution of concentration
results of such models, this data represents the first comprehensive data set which is spatially
adequate for verifying the STFATE model.
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15. Figure 5 shows acoustical measurements of the water column taken over a period of 0 to 150
sec after the disposal of dredged material. Contour intervals representing one half order of
magnitude illustrate the TSS in the water column, ranging from .1 to 1000 mg/£. The period
shown in Figure 5 includes the convective descent phase, 0 to 42 sec after discharge according to
model results, and dynamic collapse phase, 42 to 177 sec after discharge, of the material's
descent in the water column. During these two phases of the discharge, the model results
illustrate a single cloud of material falling through the water column with decreasing density,
similar to the field data (Figure 5).
16. Figure 6 shows acoustic measurements of TSS concentration taken 150 to 300 sec after the
discharge of dredged material. Two distinct clouds of material can be seen, one in the upper
water column and one in the lower water column, both with maximum concentrations exceeding
1000 mg/£. During this phase of material descent model results were converted to vertical
profiles of TSS concentration to facilitate comparison to prototype data. Scales on figures
showing model results are arbitrary (i.e., 0 does not represent the point of discharge). The
figure is centered around the maximum concentration of the plume, and the scale is based on the
plume extent. Figure 7 illustrates model results at 240 sec after discharge at which time the
center of the plume is approximately 90 m north (to the right on Fig 7) of the discharge location.
Contour lines represent the TSS concentration of dredged material in the water column and are
given in orders of magnitude, i.e., .1, 1, 10, 100, 1000 mgIt. Similar to the prototype data
shown in Figure 6, Figure 7 shows two clouds of material with maximum concentration
exceeding 1000 mgII, one at approximately 30 meter depth and another near the ocean floor.
17. Figures 8 and 9 show the TSS concentration measurements taken in the field and the TSS
concentration from model simulation, respectively. The field data was collected during the
period from 570 to 720 sec after disposal of dredged material. The simulated data shown in
Figure 9 represents a snapshot of the water column 600 sec after discharge. Disposal occurred
360 m east (to the right in Fig 9) and 450 m south (out of the page) of the center of the plume,
about 575 m total distance from the location of discharge to the center of the plume. In both
plots, a cloud of material with concentrations exceeding 100 mg/I can be seen suspended in the
water column. Except for minor differences, e.g. the numerical simulation predicts that the
cloud of material to be deeper in the water column than observed in the field data, the simulated
concentrations seem to be an accurate account of the fate of the disposed dredged material.
18. Figure 10, the TSS concentration measured in the field from 930 to 1080 sec after disposal,
shows a cloud of material comparable to that seen in Figure 8, with maximum concentrations in
Figure 10 lower (100 mg/£) than those found in Rgure 8 (1000 mg/O- Similarly, Figure 11, the
TSS concentration in the water column from model simulations at 1000 sec after disposal (about
985 m from the discharge point), shows a cloud of material comparable to Figure 9, with lower
maximum concentrations (10 mgU as compared to 100 mg/f). When the field data (Figure 10)
are compared to simulated data (Figure 11) 1000 sec after disposal, each illustrate a cloud of
suspended material with concentrations greater than 10 mgH. A significant portion of the cloud
exceeds 100 mg/£ in the field data; however, concentrations do not exceed 35 mg It in the
simulated data.
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19. In Figures 9 and 11, the simulated plume descends deeper in the water column than shown in
the field data, Figures 8 and 10. The simulated plume is effected by the density gradient which
occurs at an approximate 105 m depth causing the plume to remain in suspension above this
depth. Another density gradient was measured at 43 m, and the field data indicate that material
is trapped at this depth. The difference in the plume depth in the model results and field data
during 570 to 1080 sec after disposal are due to the lack of sensitivity of the STFATE model to a
change in density occurring at a depth of 43 m. The material shown in the field data to be
trapped at the surface has been effected by a similar density stratification occurring at a depth of
23 m. The density profile described has been documented by Proni et al (1991). Stripping of
the material from the barge, which has been added to subsequent versions of STFATE, may also
attribute to this difference in field data and simulated results.
20. Figure 12 illustrates the TSS concentration in the water column from the field measurements
taken 1350 to 150O sec after dredged material discharge. Figure 13 shows the TSS concentration
calculated 1400 sec after disposal for the simulation. These data were taken between two plumes
of higher concentration about 550 m from the location of discharge. This appears to coincide
with monitoring procedures. Both figures show similar distributions of TSS concentration below
60 m with maximum concentrations exceeding 1 mgII. The simulation computed concentrations
in the center of the plume are in excess of 10 mg/f but the field data indicate lower
concentrations.
21. Figures 5 through 13 illustrate that the STFATE model provides reasonably accurate
predictions of the fate of dredged material from the time of disposal to 25 minutes after the
discharge in that the simulated spatial distributions of material are similar to the actual spatial
distribution with concentrations within an order of magnitude. The spatial distributions of
material from field and simulated data cannot be compared at precisely equivalent times because
the acoustic technology used to obtain the field measurements required 150 sec to pass through
the dredged material residual plume. The simulated data are reported as a snapshot of the water
column at a single time providing a more intuitive insight into the material dispersion. Other
differences regarding the comparison of field and simulated data include assumptions made
regarding the disposal vessel and discharged material. Samples of dredged material were taken
and are being analyzed but the bulk density could not be included as input in the short time frame
allowed for this study. The results show that the simulation is predicting the convection and
advection of material up to 25 minutes after disposal to the degree required for the present study
(within an order of magnitude for concentration measurements taken in mg/£).
Prediction of Plume Movement
22. For the purpose of predicting the long term diffusion of dredged material and to determine if
material will reach the coral reefs, environmental conditions pertaining to velocity and density
stratification of the water column at the study site were provided by RSMAS. Information which
was not provided by RSMAS included parameters related to dredged material and vessel
dimensions, therefore, this input remained the same as that used for the verification of the
STFATE model. The depth, which must remain constant if a velocity profile is used, was
selected to be 750 ft. If the slope were included, it is reasoned that material would settle to the
bottom more quickly than simulated, decreasing the amount of material remaining in suspension.
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This represents the maximum depth of the disposal site, and it was reasoned that the deeper the
dredged material had to fail the more likely it was to be trapped in suspension. The velocity
distribution used as input into STFATE for the purpose of predicting dredged material movement
originated from Lee et al (1977). The mean velocities, which included northerly velocities of
175 cm/sec at the surface and 43 cm/sec mid-depth in the water column and westerly currents of
5.4 cm/sec at the surface and 1.9 cm/sec near the bottom, were used. These data were obtained
in June 1971 and are representative of the summer conditions when most material is discharged.
23. Measurements of temperature and salinity were taken from Roemmich and Wunsch (1985)
and were converted to density with the equation
= p
P a +0.698F
where
p = density (g/cc)
P = 5890 + 38T- 0.3757*2 +35
a - 1779.5 + 11.257-0.0745r2 - (3.8 + 0.017)5
T — temperature (°C)
S — salinity (ppt).
These data were collected in September, 1981 and do not represent the density during the
summer months. Summer temperatures presented by RSMAS were not adequate (not sufficiently
deep) to describe the density profile. The data described were input into STFATE and represent
average conditions encountered at the site.
24. Results of the sediment concentration computation for Miami are shown in Figure 14. The
disposal release point is located at the origin, and the distance is the absolute distance from the
disposal site to the residual plume. The depths of 27.4 m (90 ft), 54.9 m (180 ft), 82.3 m (270
ft), 109.7 m (360 ft), and 135.6 m (445 ft) were used in order to present an overall
representation of the numerical results. For example, at 3000 sec after the initial dump,
simulations of the disposal operation shows concentrations of suspended silt and clay at the 27.4
m (90 ft) depth to be 5.5 mg/l. Results illustrate a decreasing amount of material suspended in
the water with time. The simulated TSS concentration simulated falls below the maximum
background concentration measured in June 1991 p.l mg/f) after 9000 sec at all depths.
25. It may seem unacceptable to incur concentrations twice the background level for periods of
almost 2 hours in an area of coral reefs (i.e., 6.5 mg/f, at time 6000 sec, at depth 54.9 m).
However, the plume can be shown to move almost due north for over 2.5 hours, not reaching the
reefs with concentration levels below background levels. The path of the simulated TSS
concentrations is illustrated in Figure 15, with squares representing points along its path. The
"X" is the location of the disposal, assumed to be in the center of the disposal site.
26. In the August 1990 field study, acoustical methods were combined with adding a tracer to the
material to follow the residual plume. The plume was monitored for 1.5 hours using this method
7
-------
and was found to move due north. After the tracer could no longer be detected, the reef areas
were monitored, and no tracer was detected. The circles, shown in Figure 15, represent the
results of the dye study conducted by SAJ and AOML in August 1990. Filled circles indicate
dye was detected and open circles indicate no dye detected. The simulated path of the dredged
material is almost identical to the actual path of dredged material in August, 1990.
27. The question can then be asked if the coral reefs are effected at times of maximum westerly
currents. The same conditions as above were run with the maximum westerly currents reported
by Lee et al (1977) (57 cm/sec at the surface and 16 cm/sec near the bottom), and the residual
plume reached the coral reefs at approximately 1.7 hr (see asterisk in Figure 15). The maximum
concentration predicted near the coral reefs at this time was computed to be 0.02 mg/t. During
the verification runs, a maximum westerly current speed of 66.8 cm/sec was input at the mid
depth of the profile, which exceeds the velocity reported by Lee et al (1977) (57 cm/sec). The
resulting location of the residual plume after approximately 17 minutes is shown as a triangle in
Figure 15. The maximum TSS concentration was found to be greater than 10 mg/t by both
simulation and prototype data. However, the maximum concentration decreases to below 1 mg/£
in about 23 minutes. The material is not anticipated to reach the coral reefs before 40 minutes.
Long Term Fate Analysis
28. The final task of the study investigates the long-term fate of disposed material. Scheffner and
Swain (1989) determined the Miami ODMDS to be non-dispersive, i.e. the velocities at the site
were not sufficient to move significant amounts of the dredged material on the bottom. Empirical
relationships for computing sediment transport as a primary function of ambient water velocity,
depth, and sediment grain size were reported by Ackers and White (1973). These relationships
were subsequently modified (Swart 1976) to reflect an increase in sediment transport when a
wave field is superimposed on the ambient current field. The Long Term FATE (LTFATE)
model uses the Swart (1976) modification to compute sediment transport at the dredged material
disposal site. The model has been verified to prototype data by Scheffner (1991) and was shown
to be a viable approach to providing quantitative predictions of disposal site stability. The
program was modified to output the shear stress based on the equation taken from Ackers and
White (1973).
29. The present investigation involves determining the potential for moving material other than
uniformly graded, non-cohesive sediments. This question is addressed by calculating shear stress
values on the mound and in the surrounding area that can be used to determine the effect on any
dredged material. The difference between shear stress values on the mound and the surrounding
area provides an indication of the normal movement and the increase caused by the disposal
mound.
Non-Storm Conditions
30. In order to run LTFATE to determine long term mound evolution, two types of input data
are required, wave data characteristics at the site and time series of tidal elevations and
velocities. The wave height, period and direction data were taken from the 20-year Wave
Information Study (WIS) Revised Atlantic Coast Hindcast (Hubertz, et al 1993) database This
8
-------
database was processed through a wave simulation procedure, developed by Borgman and
Scheffner (1991), that generates waves statistically similar to those known to occur at the site,
i.e., preserving seasonality, directionality, distribution, sequencing, etc. The advantage of the
procedure is that the simulated data reflect the trends of the entire 20-year database, not merely
one specific event. The tidal database is composed of tidal harmonic constituents which can be
used to simulate a tidal time series at the disposal site. The constituents are based on a 6-month
simulated tidal time series computed by a long-wave hydrodynamic finite element model (Luettich
et al. 1992). A residual current velocity of 50 cm/sec to the west was used because this was
determined to be an approximate threshold value for the initiation of sediment movement by
Scheffner and Swain (1989).
31. As in the Scheffner and Swain (1989) study, the Miami ODMDS was found to be non-
dispersive. The shear stress values were determined as an indication of the potential of material
resuspension. For non-storm conditions, the shear stress ranged from 2.54 to 3.64 dynes/cm2,
throughout the simulated domain. As shown in Figure 16, the critical shear stress for cohesive
dredged material for field data illustrated by Teeter and Pankow (1989) was found to be 2.5
dynes/cm2. This value is conservative because the typical critical shear stress value is given to
be 5.0 dynes/cm2 (Teeter and Pankow 1989). A difference of 0.14 dynes/cm2 (3.64-3.50) is
shown to be the difference between the shear stress on the disposal mound and that of the
surrounding area. This variability in shear stress represents the maximum difference between the
values on the dredged material mound and the surrounding area. The minimum difference was
shown to be 0.10 dynes/cm2 when the surrounding shear stress was 2.54 dynes/cm2. If the
critical value for shear stress is taken from Figure 16, the entire simulated domain is in the
significant erosion range. If the typical value of 0.5 dynes/cm2 is used, the entire simulated
domain is below the significant erosion range. In either case, the mound has little consequence
to the amount of sediment moved.
Storm Conditions
32. A storm event for the Miami site was assumed to have a sustained velocity of 6.0 ft/sec for
24 hours. The findings of this study agree with those of Scheffner and Swain (1989), in which
the mound located in 600 ft of water is little effected by the velocities of a magnitude realistically
representative of the disposal site offshore of Miami. The shear stress increased by an order of
magnitude over non-storm conditions, ranging from 38.9 to 45.9 dynes/cm2. The maximum
difference in shear stress between the dredged material mound and the surrounding area is
1.8 dynes/cm2. The increase in shear stress to due the presence of the dredged material mound is
only 5% of the shear stress of the surrounding area. This increased in shear stress is anticipated
to have little impact on the sediment movement in the area.
Summary and Conclusions
33. Background conditions and dredged material plumes were monitored offshore of Miami,
Florida as a cooperative effort between SAJ, AOML, and CERC on three occasions, and the data
were subsequently analyzed to determine the validity of numerical simulation methods used in
9
-------
predicting the fate of dredged material. The objective was to determine if dredged material
would reach coral reefs located shoreward of the Miami ODMDS.
34. Field samples taken in April 1990 and June 1991 were analyzed for TSS concentration by
AOML. The dredged material plume was found to decrease in concentration to the level of
background measurements in approximately 45 minutes. During that time, the plume may move
about 1500 m but not nearly the 5000 m necessary for the material to reach the sensitive coral
reefs.
35. Acoustic backscatter measurements were used to verify the residual plume concentrations
predicted by the STFATE model. Acoustic theory was used to convert backscatter intensity to
TSS concentrations. The simulated concentrations accurately predicted the acoustic field
measurements to within an order of magnitude. After being verified, the STFATE model was
run with input provided by RSMAS. The results indicate that the disposal site is dominated by
northerly flows produced by the Gulf Stream Current. Thus, the material generally moves in a
northerly direction as verified by field data collect in August 1990. The dispersion of the
material will reduce concentrations to within background levels before moving sufficiently
westerly to reach the coral reefs. Even in the maximum westerly flow, the coral reefs are not
anticipated to be effected.
36. Under normal environmental conditions, shear stress values at the ODMDS are low, and little
movement is anticipated for either cohesive or non-cohesive material. During storm events, the
shear stress values increase by an order of magnitude. However, the shear stress on the dredged
material disposal mound increases by less than 2 dynes/cm2 above the shear stress of the
surrounding area. When subjected to storms, material is anticipated to move from the mound for
short periods of time but large dispersion of the mound is not predicted, therefore the material is
not expected to effect the coral reefs.
37. Amongst the data collected during three field monitoring studies and two numerical model
prediction studies, no evidence has been found to indicate that dredged material will migrate on
to coral reefs. The predominant current velocities are toward the north-northeast, away from the
sensitive areas. Even in the maximum anticipated westerly currents, the dredged material is
shown in field data to disperse to well within the limits of background concentrations
in approximately half the time it would take to reach the reefs. The model predictions have not
been fully verified to prototype data in the upper few meters of the water column (results are
illustrated beginning at 30 meters), however, field data collected and analyzed by AOML indicate
that concentrations in the upper 3 to 8 m of the water column decrease to just above background
levels in the minimum time required to reach the reefs. Therefore, the discharge of dredged
material at the placement site is not predicted to cause an increase in naturally occurring
concentration of TSS on the coral reefs located shoreward of the Miami ODMDS.
REFERENCES
Ackers, P. and White, R.W. 1973. "Sediment Transport: New Approach and Analysis,
Journal of the Hydraulics Division, Vol 99, No HY11, pp 2041-2060.
10
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Bergman, L.E. and Scheffner, N.W. 1991. "The Simulation of Time Sequences of Wave
Height, Period, and Direction," Technical Report DRP-91-2, Coastal Engineering Research
Center, US Army Engineer Waterways Experiment Station, Vicksburg, MS.
Johnson, B.J., Trawle, M.J., and Adamec, S.A. 1988. "Dredged Material Disposal Modeling in
Puget Sound," Journal of the Waterway, Port, Coastal, and Ocean Division, Vol 114, No. 6, pp
700-713.
Hubertz, J.M., Brooks, R.M., Brandon, W.A., and Tracy, B.A. 1993. "Hindcast Wave
Information for the US Atlantic Coast," WIS Report 30, Coastal Engineering Research Center,
US Army Engineer Waterways Experiment Station, Vicksburg, MS.
Kraus, N.C. (ed.) 1991. "Mobile, Alabama, Field Data Collection Project, 18 August - 2
September, 1989, Report 1: Dredged Material Plume Survey Data Report," Technical Report
DRP-91-3, Coastal Engineering Research Center, US Army Engineer Waterways Experiment
Station, Vicksburg, MS.
Lee, T.N., Brooks, I., and Diiing, W. 1977. "The Florida Current; its Structure iand
Variability," Technical Report UM_RSMAS 77003, Rosenstiel School of Marine and
Atmospheric Sciences, University of Miami, Miami, FL.
Luettich, R.A., Westerink, J.J., and Scheffner, N.W. 1992. "ADCIRC: An Advanced Three-
Dimensional Circulation Model for Shelves, Coasts, and Estuaries - Report 1: Theory and
Methodology of ADCIRC-2DDI and ADCIRC-3DL," Technical Report DRP-92-6, Coastal
Engineering Research Center, US Army Engineer Waterways Experiment Station, Vicksburg,
MS.
Ogushwitz, P.R. 1992. "Analysis of Measure Sound Scattering from Suspended Sediment
Plumes," Coastal Engineering Research Center, US Army Engineer Waterways Experiment
Station, Vicksburg, MS.
Proni, J.R., Tsai, J.J., and Dammann, W.P. 1991. "Miami Harbor Dredged Material Disposal
Project," Coastal Engineering Research Center, US Army Engineer Waterways Experiment
Station, Vicksburg, MS.
Proni, J.R., Craynock, J.F., and Tsai, J.J. 1993. "Miami Harbor Dredged Material Disposal
Project: Total Suspended Solids Measurements," 'Coastal Engineering Research Center, US
Army Engineer Waterways Experiment Station, Vicksburg, MS.
Roemmich, D. and Wunsch C. 1985. "Two Transatlantic Sections: Meridional Circulation and
Heat Flux in the Subtropical North Atlantic Ocean," Deep Sea Research, Vol 32, No 6, pp 619-
664.
Scheffner, N.W. and Swain, A. 1989. "Evaluation of the Dispersion Characteristics of the
Miami and Fort Pierce Dredged Material Disposal Sites," Coastal Engineering Research Center,
US Army Engineer Waterways Experiment Station, Vicksburg, MS.
11
-------
Scheffner, N.W. 1989. "Disposal Site Evaluation for the New York Bight," Coastal Engineering
Research Center, US Army Engineer Waterways Experiment Station, Vicksburg, MS.
Scheffner, N.W. 1991. "A Systematic Analysis of Disposal Site Stability," Proceedings of
Coastal Sediments '91, ASCE, pp 2012-2026.
Swart, D.H. 1976. "Predictive Equations Regarding Coastal Transports," Proceedings of the 15A
Coastal Engineering Conference, ASCE, pp 1113-1132.
Teeter, A.M. and Pankow, W. 1989. "Schematic Numerical Modeling of Harbor Deepening
Affects on Sedimentation, Charleston, SC," Miscellaneous Paper HL-89-7, Hydraulics
Laboratory, US Army Engineer Waterways Experiment Station, Vicksburg, MS.
Thevenot, M.M. and Kraus, N.C. 1993. "Comparison of Acoustical and Optical Measurements
of Suspended Material in the Chesapeake Estuary," Journal of Marine Environmental
Engineering, Vol 1, pp 65-79.
Tsai, J.J., Proni, J.R., Dammann, W.P., and Kraus, N.C. 1992. "Dredged Material Disposal at
the Edge of the Florida Current," Chemistry and Ecology, Vol 6, pp 169-187.
Michelle M. Thevenot, PE
Research Division
Coastal Engineering Research Center
12
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Covornmeni Cut
ODMDS
STATUTE MILES
NAUTICAL MILES
GENERAL LOCATION MAP
Ocean Dredged Molenal Disposal Site Miami, Florida
25* 4 7' OD
25* 46' JO'
25* <6 00
25* *5 30
25' 15 '
25* 45 00
25* 4* 45
?b' 44 JO
25' 4 4 CO'
25' 43" 00
ODMDS
I
NAUTICAL miles
0A7HYME TRlC MAP
Oceon Oreaged Material Disposal S"le Miomi, Florida
-------
103
Miami Harbor Project
All Discharges
o°
1 0
-2
I | I I I I [ 1 I I I | I I I I | F I I I (
I f I I 1 I I I I I I I I I I I I I 1 I I 1 I F I I I I I I I I I
0
5 10 15 20 25 30 35 40 45 50 55
Time (min)
• ¦ i •11 ¦ i
60 65
-------
Normalized Concentration
Discharges Nos. 1, 3 & 4
10° —
o.i
nm-J
20 25 30 35 40
Time (min)
-------
-20
-30J
-40-
best fit to data
-50-
o«
- 60 H
theory
-80-
00
-90-
O - 100-
LlJ
-110
10 100
Concentra on (m
1000
-------
SCATTERING STRENGTH ABOVE BACKGROUND
MHDP 04-26-90 14:16:00—14:18:30 Background time = 14:16:00
Vertical avg. = 3.0 meters. Repeated 5 times.
Horizontal avg. = 2.50 seconds. Threshold = 15.0 millivolts.
D.C. Offset = 0.0 millivolts. Absorption coefficient = -.00500 dB/m.
0 20 40 60 80 100 120 140 160 180 200 220
Distance (M)
0
Time (sec)
150
-------
SCATTERING STRENGTH ABOVE BACKGROUND
MHDP 04-26-90 14:18:30-14:21:00 Background time = 14:16:00
Vertical avg. = 3.0 meters. Repeated 5 times.
Horizontal avg. = 2.50 seconds. Threshold = 15.0 millivolts.
D.C. Offset = 0.0 millivolts. Absorption coefficient = .00500 dB/m.
o 80
1 20 -
m
0 20
150
80 100 120 140
Distance (M)
Time (sec)
160 180 200 220
Concentration
(mg/l)
>1000
500
100
50
10
5
1
.5
.1
<. I
300
-------
T-240
30
2 60
90
120
137
450
900
600
300
750
150
Distonce (M)
-------
SCATTERING STRENGTH ABOVE BACKGROUND
MHDP 04-26-90 14:25:30-14:28:00 Background time = 14:16:00
Vertical avg. = .3.0 meters. Repeated 5 times.
Horizontal avg. = 2.50 seconds. Threshold = 15.0 millivolts.
D.C. Offset = 0.0 millivolts. Absorption coefficient = .'00500 dB/m.
0)
a 80-
1 00 -
1 20 -
0 20
570
80 100 120 140
Distance (M)
Time (sec)
160 180 200 220
720
eeo
EZ]
Concentration
(mg/l)
>1000
500
100
50
10
5
1
5
.1
<.1
-------
T-600
30
60
90
120
137
150
300
450
Distance (M)
-------
SCATTERING STRENGTH ABOVE BACKGROUND
MHDP 04-26-90 14:31:30-14:34:00 Background time = 14:16:00
Vertical avg. = 3.0 meters. Repeated 5 times.
Horizontal avg. = 2.50 seconds. Threshold = 15.0 millivolts.
D.C. Offset = 0.0 millivolts. Absorption coefficient = .00500 dB/m.
Concentration
(mg/l)
J , , , , ¦ . 1 I I '¦* a
0 20 40 50 80 100 120 140 160 180 200 220
Distance (M)
Time (sec)
930
v
1080
-------
Distance (W)
-------
SCATTERING STRENGTH ABOVE BACKGROUND
MHDP 04-26-90 14:38:30-14:41:00 Background time = 14:16:00
Vertical avg. = 3.0 meters. Repeated 5 times.
Horizontal avg. = 2.50 seconds. Threshold = 15.0 millivolts.
D.C. Offset = 0.0 millivolts. Absorption coefficient = .00500 dB/m.
0 20 40
I ' I i ¦ I i 1 1 r
80 100 120 140 160 180 200 220
Distance (M)
Time (sec)
Concentration
(mg/l)
>1000
500
100
50
10
5
1
.5
.1
<.1
1350
1500
-------
T-1400
30
_c
a
a>
O
90
100
137
0
900
600
300
Distance (M)
-------
12 0
10 0
8 0
6 0
4- 0
2 0
0
CP
E
c
o
c
270 FT
0ACKCROUND
^ 3 1 mg/l
4500 SEC
6000 SEC
disposal site
(109 7m)
360 FT
BACKCROUND
3 1 mg/l
9000 SEC
bOOu SIC
DISPOSAL SITE
_L
1135 6M)
445 FT
BACKCROUND
3 1 mg/l
9000 SEC
I I
3 < 5 6
Distance (Miles)
1 , /''/
-------
Coral R< efs
1 7hr •
2 5hr
50mm
Government Cut
min
17 min
ODMDS
STATUTE MILE
nautical miles
path or residual plumc
Ocean Dredged Material Disposal Site Miami, Florida
FT, f£T
^ ¦
-------
significant
erosion „
particle erosion
b dynes/cm
-------
APPENDIX F
MIAMI HARBOR DREDGED MATERIAL DISPOSAL PROJECT
-------
MIAMI HARBOR DREDGED MATERIAL DISPOSAL PROJECT
John R. Proni, Ph.D.
Director, NQAA/ERL/AOML Ocean Acoustics Division
John J. Tsai, Ph.D.
Research Physicist, NQAA/ERL/AOML Ocean Acoustics Division
Paul Dammann, P.E.
Research Oceanographer, NQAA/ERL/AOML Ocean Acoustics Division
National Oceanic and Atmospheric Administration
Atlantic Oceanographic and Meteorological Laboratory
4301 Rickenbacker Causeway
Miami, Florida 33149
June 1991
-------
TABLE OF CONTENTS
Page
I. INTRODUCTION 1
II. FIELD OPERATION 5
III. DATA ANALYSIS 9
Water Depths 9
Temperature Profiles 15
Density Stratification 19
Salinity Measurements 20
Current Velocity 21
Dredged Materials 23
Acoustic Profiles 26
IV. DISCUSSION 28
V. RESULTS 41
VI. CONCLUSIONS AND COMMENTARY 43
VII. ACKNOWLEDGMENTS 45
VIII. REFERENCES 45
IX. APPENDICES 47
Appendix A A-l
Appendix Bl Bl-1
Appendix B2 B2-1
Appendix Cl Cl-1
Appendix C2 C2-1
Appendix C3 C3-1
Appendix C4 C4-1
Appendix D D-l
Appendix El El-1
Appendix E2 E2-1
Appendix E3 E3-1
Appendix E4 E4-1
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FIGURE CAPTIONS
Figure Page
1. Location map of Miami ODMDS. Insert at the upper right
corner indicates the location of the map in Florida.
Circles and squares represent active artificial reefs,
except dotted squares are proposed artificial reefs 2
2. Signal flow chart of acoustic concentration profiler
system 7
3. Bathymetric map in the vicinity of the Miami ODMDS;
water depth in feet 14
4. Temperature profiles from six CTD stations of Phase 1 16
5. Density profiles from six CTD stations of Phase 1 17
6. Salinity profiles from six CTD stations of Phase 1 18
7. Location map of the Miami Harbor. The turning basin
is indicated as a * at the end of the Miami Ship
Channel. The insert at the lower left corner shows
the three sediment stations 24
8. Gradation curves of particle-size distribution for
the three sediment stations in the Miami Harbor
Turning Basin 25
9. Acoustic iso-concentration contours of one dump on
April 26, 1990, corresponding to four transects at
different times. The gap in concentration indicated
in (a) at 90 to 100 m distance is attributed to
acoustic absorption at the frequency of 20 kHz by a
cloud of bubbles in the water near the surface 30
10. Acoustic iso-concentration contours of the first
transect of Fig. 9, showing the method to calculate
the entrainment coefficients. The backscattering
strength levels shown in Figs. 9 and 10 are in
decibels and represent particulate concentrations
of suspended materials in the water column 32
11. Temperature, salinity and density profiles at
15:59:00 on April 25, 1990 during Phase 1 35
12. Comparison between acoustic scattering strength
from ACP and echo amplitude from ADCP at 30 m and
50 m. Top: from ACP; bottom: from ADCP 36
13. Comparison between acoustic scattering strength
from ACP and echo amplitude from ADCP at 70 m and
90 m. Top: from ACP; bottom: from ADCP 37
-------
FIGURE CAPTIONS (continued)
Figure Pag
14. Peak concentration as function of time at six fixed
depths for April 26, 1990 during Phase 1 38
15. Time series of echo amplitudes at seven fixed depths
from 10 ra (top) to 130 m (bottom) for April 26, 1990
during Phase 1 40
16. Current profiles for the five transects of second
dump on April 26, 1990 during Phase 1 42
-------
I. INTRODUCTION
There are only limited upland disposal sites of dredged material in
the Miami, Florida area and the recently planned deepening of the Miami
Harbor creates a need to designate by the U.S. Environmental Protection
Agency (EPA) an environmentally acceptable, adequately sized and
economically feasible offshore Ocean Dredged Material Disposal Site
(ODMDS) for the greater Miami, Florida area (EPA, 1990). Two independent
studies were carried out to comply with the Marine Protection, Research,
and Sanctuaries Act (MPRSA) of 1972. Physical, chemical and biological
characteristics and their interactive effects were measured (Conservation
Consultants, Inc., 1985) and the probable dispersion fate of dredged
materials that might be dumped at the site was modeled (Scheffner and
Swain, 1989). The Draft Environmental Impact Statement of EPA (EPA, 1990)
concluded that the interim-designated site, about five nautical miles
offshore from Government Cut at Port of Miami and shown in Fig. 1, is
suitable for designation for disposal of dredged material.
Both natural and artificial reefs are found in the proposed Miami
ODMDS vicinity. The seaward extent of the natural reef zone in the area
lies approximately 2.4 km inshore of the west side of the interim
disposal site (Fig. 1). Two concentrations of artificial reef sites are
also located in the area, one group about 6 km north and slightly inshore
and the other about 3 km south and inshore of the proposed disposal site
(Fig. 1). There are concerns about the potential contamination of these
reef areas due to the proposed disposal of up to 6 million cubic yards of
material from the Miami Harbor deepening project. One of the major
reasons is that the proposed ODMDS is situated on the continental slope
where the ocean circulation is strongly influenced by the nearby Florida
Current. The Florida Current is that portion of the Gulf Stream system
that connects the Loop Current in the Gulf of Mexico to the Gulf Stream
1
-------
Miami Ocean Dredged Material Disposal Site
23° 30*
Os
ARTIFICIAL REEF I
Port of Miami G
Virginia Key
ODMDS
STATUTE MILES
NAUTICAL MILES
Cape Florida
JO
Fig. 1. Location map of Miami OOKDS. Insert at the upper right
corner indicates the location of the map in Florida.
Circles and squares represent active artificial reefs,
except dotted squares are proposed artificial reefs.
-------
as the flow proceeds through the Straits of Florida and into the open
Atlantic Ocean (Lee et al., 1977). When the western edge of the Florida
Current is over the continental shelf, the current draws the coastal
waters north with it. When the western edge is seaward of the shelf,
cyclonic spin-off eddies are formed. Following their formation, spin-off
eddies travel northward along the continental margin at speeds ranging
from 20 to 50 aVsec. Eddies occur on the average of once per week and
can be recognized as disruptions of prevailing temperature and salinity
fields and of local current patterns (Lee and Mayer, 1977). These
cyclonic eddies play an important role in coastal exchange processes,
removing coastal water and replacing it with water from the Florida
Current.
Because the designated Miami ODMDS lies near the western edge of the
Florida Current and the mean current can be greater than 100 ao/sec in
the spring and summer, transport, dispersion and mixing of dredged
material dumped in this area could be affected greatly by physical
processes associated with the Florida Current. Therefore, a monitoring
study of dredged materials from the turning basin area, Port of Miami,
that were dumped in the designated Miami ODMDS was undertaken during the
period of April 24 to April 26, 1990. A second phase of study took place
between June 26 and June 28, 1990. One major objective of the study is
to identify and monitor environmentally significant physical processes at
the ODMDS site, which would change the fate of dredged materials dumped
at: the site. One of those significant quantities is the maximum
reef-directed shoreward current that would transport dumped material to
the coral reef area. Another objective is to. compare the in-situ
measurements and observations with results of a numerical modeling study
(Scheffner and Swain, 1990).
3
-------
The Ocean Acoustic Division (QAD) of the Atlantic Oceanographic and
Meteorological Laboratory (AOML), a component of NQAA (National Oceanic
and Atmospheric Administration), has been at the forefront of the
analysis and technology required for understanding coastal ocean
processes and their influence on the dispersion of material discharged
into the open ocean. During the last 15 years, OAD has applied this
acoustic remote sensing technique to study ocean disposal of different
materials at various environments and locations. Among these studies were
sewage sludge in New York Bight (Proni et al., 1976), river bottom
dredged material in Lake Ontario (Proni et al., 1977), pharmaceutical
wastes off Puerto Rico, drilling muds from an oil rig in the Gulf of
Mexico (Trefey arid Proni, 1983), dredged material in New York Bight
(Tsai, 1984; Tsai and Proni, 1985), and more recently dredged material in
Mobile Bay. Results from these studies have provided good evidence that
acoustic remote sensing can be very useful for studying waste disposal in
the ocean.
• The Miami Harbor Dredging Material Dumping Study is a joint project
of the U.S. Army Engineer District, Jacksonville and the Coastal
Engineering Research Center (CERC) of the U.S. Army Engineer Waterways
Experiment Station (WES), Vicksburg, Mississippi, and was conducted by
QAD/AQML of NQAA, Miami. Hie plume concentration of discharged material
and current velocity were monitored continuously to depths as great as
160 m and are believed to provide the first reliable measurements of
sediment plume dynamics over such depths in the open ocean. The data and
observations for all dredged material placement operations during this
project indicate that the waste plume moved toward the north to north-
east, that is northward and away from sensitive coral reef areas of
concern. The results also support predictions from previous numerical
modeling and certain conclusions reached in the EPA Draft EIS. The
4
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procedures followed and results obtained are expected to provide
information on other ODMDS's managed by the Jacksonville District.
II. FIELD OPERATION
The entire operation took place in two phases, Phase I from April 24
to 26, 1990 and Phase II from June 26 to 28, 1990. During Phase I, eight
dumps of dredged material from the Miami Harbor turning basin area were
carried out, and the waste plumes were monitored continuously with an
Acoustic .Concentration Profiler (ACP) of QAD/AOML and an Acoustic Doppler
Current Profiler (ADCP) of RDI (RD Instruments, Inc.). Hie ADCP was not
used during the Phase II because it was not available during that time.
There were no dumps monitored during Phase II because the contracted
dredging operation was unexpectedly finished early. During both phases,
CTD (Conductivity-Temperature-Depth) stations were taken using a Seabird
CTD profiler, and water/sediment samples were collected continuously from
a towed pump sampler when the ship was underway. Sediment samples were
collected from the dredging vessel with a sediment grab sampler during
Phase I.
The ADCP was mounted at the port side of the monitoring vessel (Sea
Explorer), opposite to the towed transducer of the ACP. The ADCP
transmits short acoustic pulses along narrow beams at a known, fixed
frequency (150 MHz). It listens to and processes the echoes from
successive volumes (depth cells or'bins) along the beams to determine how
much the frequency has changed. The difference in frequency between
transmitted and reflected sound is proportional to the relative velocity
between the ADCP and the particles in the water that do the reflecting
(backscattering). This frequency shift results from the Doppler effect.
The ADCP uses an autocovariance method to compute the mean value or first
moment of the Doppler frequency, and from this computed first moment of
5
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frequency, velocity of the scatterers is determined. However, the current
at each depth cell is assumed to be the same for all beams (the
homogeneous velocity assumption). The ADCP also provides echo amplitude
as a byproduct of the AGC (Automatic Gain Control) circuits. This echo
amplitude estimates backscatter intensity and is comparable with the
acoustic intensity measurement from ACP. Backscattering cross sections
derived from both the ADCP echo amplitude and the ACP acoustic intensity
can be used to estimate the particulate concentrations of suspended
wastes in the water column and to compare with particle concentrations
derived from bottle samples.
The ACP has five major components as a system (Fig. 2). (1) It has
transducers mounted in a streamlined towbody, aiming vertically downward
and towed on the starboard side of the ship at a nearly constant depth of
about 1 m below the water surface. The two transducers have acoustic
frequencies of 20 kHz and 200 kHz. (2) The ACP uses a Datasonic model
DFT-210 dual channel acoustic transceiver with several features not found
in standard acoustic transceivers. It provides digital control of
transmitter output pulse and receiver gain characteristics to allow
accurate measurement of target echo levels. A precision low noise
preamplifier is incorporated within the receiver to extend the system
dynamic range and to allow measurement of very low backscattering levels.
The DFT-210 also offers multiple receiver outputs and interfaces for
simultaneous recording and display. (3) Two Raytheon TDU-850 digital
chart recorders were used to record echographs from the DFT-210, one for
20 kHz signals and the other for 200 kHz. The TDU-850 is a thermal
display unit which generates hard copy of true gray shades at high speed
and with high resolution, producing near photographic quality. It
features a universal interface that transfers data rapidly and relies on
synchronization of clock and data signals to transfer the image in a
6
-------
•ZBM ComDuter
"with A/D Converter
Raytheon TDU-850
Thermal Paper Recorder
°t t 3
Sharp SX-DJ 00
DAT Recorder
3bH 83 .59 54
* ©_® e
Systron Dormer Model 8720
Time Code Generator
= 1 1
G
• g.~,n.- i.i • i - I-1 i i.i.i i +
i ni
Sharp SX-DJ 00
DAT Recorder
aoaa
o a
Sony PCM-F1
Audio Digital Processor
r
5E39G
5c=-==-*3
5S~S£[q
I
Datasanic DFT-210
Transceiver
20 KHz and 200 KHz
Transducers
Video Cassette Recorder
Video Cassette Recorder
Fig. 2. Signal flow chart of acoustic concentration profiler system.
7
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raster scan format. (4) Both receiver outputs from the 20 kHz and
200 kHz transducers were also recorded respectively onto two Sharp
SX-D100 digital audio tape (DAT) recorders with IRIG-B tine code gene-
rated from a Systron Donner Model 8720 time code generator. The recorded
outputs were processed later to obtain the acoustic back-scattering
strength from which the waste concentration is derived. (5) The receiver
outputs were recorded separately on two standard VHS video cassette
tapes using a Sony PCM-Fl Audio Digital Processor. These VHS tapes serve
as backup and have the same data as those on the DAT.
There were eight dumps in total for the entire operation. Before
each dump and between successive dumps, the Sea Explorer monitored the
water column to obtain background concentrations of suspended materials
and ambient currents in the area using the ACP and ADCP on board the
vessel. Ambient density and salinity were measured by taking CTD
stations at the previous dumping spots that were determined from the ship
track records. There were six CTD stations in Phase I and 50 stations in
Phase II. CTD stations taken during Phase II were not based on the
actual dumping location because no dumping took place in Phase n.
Sediment samples were collected directly from the dredging vessel
Atchafalaya for each dump. The dumping would occur for most of the dumps
when Atchafalaya had just made the turn to head shoreward. Both the ADCP
and ACP were set r^ady to operate upon the approach of Atchafalaya and
the Sea Explorer proceeded to make the transects immediately after the
dumping commenced. The Sea Explorer would track the waste plume for
several transects until the ACP could not detect the plume any more. It
usually took about 40 minutes since the release. During each transect,
water samples were taken by a towed V-fin with a pump that pumps water
continuously through a hose to the deck of the moving ship. The water
sampling took place at approximately constant depth by maintaining
8
-------
constant ship speed, and collecting samples only during the time when
transects were in the plume. During the first two-day operation, ship
positions were automatically logged with a computer and displayed in real
time to assist monitoring. A drift buoy was to be deployed to mark the
spot of each dump but was never used. However, the surface features of
the waste plume were visible up to 30 minutes and were helpful in
tracking the plume. All ship tracks are presented in Appendix A for
reference.
III. DATA ANALYSIS
The primary data obtained from the Phase I were the ACP data
recorded on the DAT and VHS tapes and the ADCP data stored on computer
diskettes. In addition, water samples and sediment samples were
collected during Phase I. However, no detailed analysis has been done
with the water samples and the sediment samples. Grain size distribu-
tions are available from analysis of samples taken in 1988. CTD data
were obtained in Phases I and II and made up the major portion of data
collected in Phase II. CTD stations are summarized in Table 1 for Phase
I and in Tables 2-1, 2-2 and 2-3 for Phase II. Station locations are
presented on page Bl-2 of Appendix Bl and page B2-2 of Appendix B2. For
Phase II, station locations are separated into three sections for the
three days and listed on pages B2-4, 19, and 38. All temperature,
salinity, and density profiles fdr both phases were plotted for each
station as shown in Appendices Bl and B2. All observational data and
results of analysis are described below.
Water Depths
The Miami ODMDS is situated on the continental slope with depths
ranging from 425 to 785 feet, or 130 to 240 m (Fig. 3). The depth at the
9
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Table 1
CTD stations and temperature, density and salinity gradients
for Phase I
CTD
No.
Date
Time
Temperature
Gradients
(deg C/ta)
Density
Gradients
(gn^cc/m)
Salinity
Gradient
(ppt/m)
Overall
Middle
Overall
Middle
Overall
1
04/24/90
10:49:30
-0.107
-0.055
-0.275
0.023
0.014
0.064
0.011
2
13:16:30
-0.108
-0.107
0.025
0.019
0.017
3
18:17:00
-0.109
-0.068
0.023
0.019
0.018
4
04/25/90
11:12:00
-0.127
-0.081
0.030
0.019
0.029
5
15:59:00
-0.124
-0.130
0.030
0.027
0.018
6
04/26/90
09:29:00
-0.138
-0.100
0.028
0.027
0.017
10
-------
Table 2-1
CTD stations and temperature, density and salinity gradients
for June 26, 1990 of Phase II
CTD Date
No.
Time
Temperature
Gradients
(deg C/hi)
Density
Gradients
(gta/cc/m)
Salinity
Gradient
(ppt/ta)
Overall
Middle
Overall
Middle
Overall
1 06/26/90
10:12:00
-0.135
-0.195
0.038
0.058
0.002
3
12:34:20
-0.106
-0.155
0.027
0.036
0.006
4
13:25:13
-0.112
-0.155
0.032
0.044
0.008
5
14:21:50
-0.103
-0.147
0.025
0.043
0.008
6
15:18:30
-0.103
-0.162
0.026
0.039
0.005
7
16:04:44
-0.104
-0.201
0.024
0.056
0.009
8
16:59:23
-0.098
-0.227
0.022
0.071
0.012
9
18:18:00
-0.105
-0.332
0.026
0.126
0.014
11
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Table 2-2
CID stations and temperature, density and salinity gradients
for June 27, 1990 of Phase II
CTD
Date
Time
Temperature
Density
Salinity
NO.
Gradients
Gradients
Gradient
(deg C/to)
(gtVcc/ln)
(ppt/m)
Overall
Middle
Overall
Middle
Overall
17
06/27/90
00:47:14
-0.113
-0.320
0.028
0.096
0.012
18
01:50:43
-0.109
-0.285
0.024
0.085
0.010
19
03:39:23
-0.088
-0.098
0.018
0.026
0.010
20
10:50:57
-0.137
-0.365
0.035
0.115
0.010
21
11:25:13
-0.124
-0.133
0.030
0.039
0.008
22
12:39:16
-0.101
-0.140
0.023
0.033
0.010
23
14:10:02
-0.105
-0.222
0.025
0.066
0.007
24
14:50:13
-0.132
-0.660
0.038
0.210
0.002
28
16:36:39
-0.113
-0.214
0.026
0.062
0.008
29
17:46:03
-0.118
-0.199
0.028
0.059
0.007
30
19:31:08
-0.119
-0.216
0.027
0.062
0.008
31
20:25:12
-0.332
0.098
32
22:14:20
-0.111
-0.288
0.025
0.092
0.015
12
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Table 2-3
CTD stations and temperature, density and salinity gradients
for June 28, 1990 of Phase II
CID Date
No.
Time
Temperature
Gradients
(deg C/m)
Density
Gradients
(gm/cc/m)
Salinity
Gradient
(ppt/in)
Overall
Middle
Overall
Middle
Overall
33 06/28/90
00:04:15
-0.119
-0.314
0.029
0.088
0.006
34
01:03:26
-0.112
-0.157
0.026
0.042
0.006
35
02:49:02
-0.132
-0.185
0.031
0.055
0.006
37
05:02:39
-0.093
-0.143
0.018
0.033
0.010
38
06:52:58
-0.119
-0.268
0.027
0.070
0.006
39
07:43:14
-0.413
0.133
42
15:05:34
-0.354
0.099
13
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Miami Ocean Dredged Material Disposal Site
23*47'oo"
25° 45 30
2SC44'30"
25* 4 j'OO"
ODMDS
I
NORTH
NAuTlCA. UlLl
Fig. 3. Bathymetric map in the vicinity of the Miami ODMDS;
water depth in feet.
14
-------
center of the site is approximately 625 feet (191 m). The average
declivity of the slope at the ODMDS is approximately 325 feet (100 m) per
nautical mile (1.85 km). The eight dumps during Phase I took place at
locations with depths varying from 120 m to 170 m.
Temperature Profiles
The temperature profiles indicate a well mixed surface layer of 25°C
temperature for the three-day period of Phase I (Fig. 4). There are
strong gradients below 50 m depth and extend possibly all the way to the
ocean bottom. The surface temperature varies only about 0.5 degree a
day. Temperature gradients differ significantly from time to time and
day to day, however. This temperature difference creates important
variations in density stratification (Fig. 5) because the salinities do
not change significantly (Fig. 6). One temperature profile at the time
10:49:30 on April 24, 1990 shows a distinguishable second gradient at the
intermediate water of small depth region between 35 and 65 m. There also
exists a slight gradient instead of constant temperature in the surface
layer for April 25, 1990 at 11:12:00. On April 24 at 10:49:30, the
temperature profile indicates a four layer structure with different
gradients.
Temperatures in June show stronger gradients, but in general there
is a shallower mixed layer near the surface. In fact, six profiles on
June 26, three on June 27 and one oh June 28 show no mixed layer near the
surface. In contrast, two mixed layers were observed at 06:52:58 on June
28. Daily differences seem to be small when temperature profiles were
grouped together and plotted in the same graphs for similar depths. All
individual temperatures for each station with their salinity and density
profiles are included in Appendix Bl for Phase I and Appendix B-2 for
Phase II.
15
-------
0.0
04/24/90 10:49:30
04/24/90 13:16:30
.... 04/24/90 18:17:00
04/25/90 1 1:12:00
04/25/90 15:59:00
04/26/90 09:29:00
22.0-
44.0-
66.0-
88.0-
22.0
20.0
24.0
1 6.0
18.0
26.
Temperature (deg C)
Fig. 4. Temperature profiles from six CID stations of Phase I.
-------
0.0
_ 04/24/90 10:49:30
.. 04/24/90 13:16:30
.. 04/24/90 18:17:00
. 04/25/90 1 1:12:00
.. 04/25/90 15:59:00
.. 04/26/90 09:29:00
22.0-
£ 44.0-
x:
66.0-
88.0-
1 10.0
23.8
24.6
23.0
25.4
26.2
27.0
Sigma —t
Fig. 5. Density profiles from six CID stations of Phase I.
-------
0.0
_ 04/24/90 10:49:30
.... 04/24/90 13:16:30
... 04/24/90 18:17:00
... 04/25/90 1 1:12:00
... 04/25/90 15:59:00
... 04/26/90 09:29:00
22.0-
£ 44.0-
si
£ 66.0-
88.0-
34.0
34.8
36.4
35.6
37.2
38.0
Salinity (ppt)
Fig. 6. Salinity profiles from six CTD stations of Phase I.
-------
The observed temperature gradients are listed in Table 1 for Phase I
and in Tables 2-1, 2-2, and 2-3 for Phase II. The maximum overall
gradient is about -0.138°C per meter depth for Phase I (April 26 at
09:29:00, page Bl-7) and -0.137°C for Phase II (June 27 at 10:50:57, page
B2-24). However, the temperature profile observed on April 24 shows
double gradients at 10:49:30 (page Bl-3). In fact, there exist more than
two gradients at different depths for this station. The middle water
temperature gradient is always greater than that of deeper water. Most
of the June profiles also show these double gradients. Three profiles on
June 27 (12:39:16, 14:10:02 and 14:50:13 on pages B2-26, 27, and 28
respectively) and four on June 28 (05:02:39, 06:52:58, 07:43:14 and
15:05:34 on pages B2-43, 44, 45 and 46 respectively) have more than two
gradients.
Maximum temperatures always occur at the surface and range from 25°C
in April to about 29°C in June. These observations are in the ranges of
annual mean reported by Lee and Mooers (1977) and EPA (1990).
Density Stratification
Density profiles also show gradients at all times and days and are
strongly associated with the temperature variation. Whenever there is a
constant temperature layer near the surface, there is a constant density
layer in the same depth range. Whenever there are temperature gradients,
there are density gradients withifi the same depth range. The multiple
layer structure at 10:49:30 on April 24 also appears in the density
profile. The double mixed layer in temperature at 06:52:58 on June 28
also appears in density. Clearly the density variations largely follow
the temperature variations.
Observed density ranges from 1.024 gm/cc to 1.027 gm/cc in April.
In June, the surface density was about 1.023 gm/cc or smaller, and
19
-------
densities near the bottom can be larger than 1.027 gm/cc because of the
deeper water at some of the stations. These values agrees fairly with
the report by EPA (1990). Density gradients are shown in Tables 1 and
2-1, 2-2, 2-3 for overall depths and the middle water column. Itie middle
water column gradients in general are greater than those in deeper water
near the bottom just as in the case of temperature. The maximum overall
density gradient is 0.038 gnv/cc/m at 10:12:00 on June 26 (page B2-5).
Salinity Measurements
Salinity at the dump site was fairly constant through all depths
except at the deep water below 100 m for Phase I (Fig. 6). Salinity
fluctuates vigorously in deep water with apparent local variations at
different times and locations. The salinity profile generally increases
slightly with depth from the surface and begins to decrease at about the
thermocline depth. The surface salinity is about 36.3 ppt, and maximum
salinity can be as much as 36.6. The lower salinity near-bottom water
can reach as low as 35.6 in April (Phase I). One profile on April 24 at
10:49:30 (page Bl-3) shows a rapid increase and decrease within 10 m
depth, and indicates a salt finger.
In June, the salinity generally remains constant to some depth,
increases very slightly to a certain maximum, and then decreases rapidly
to the bottom with strong gradient. It reached 35.0 ppt at 240 m depth
(June 27, at 03:39:23, page B2-23'). In some cases, salinity near the
surface and the bottom appear to be constant at differert times, but it
varies significantly in the middle water column (June 27 j'rom 01:50:43 to
22:14:20 and June 28 from 02:49:02 to 15:05:34). One profile from June
28 at 06:52:58 (page B2-44) shows distinguishing features from the
others. It indicates a rapid increase in salinity and then decreases
20
-------
with a strong gradient. The maximum salinity gradient occurred at
11:12:00 on April 25 with value of 0.029 ppt/m (page Bl-6).
Current Velocity
The current profiles from the ADCP provide very good information on
the current structure at the Miami ODMDS. However, ADCP data were
available only for Phase I, and there are no current measurements during
Phase II.
An i-nitial sample interval of two minutes was selected for the first
day of Phase I. The primary objective of the current measurements was to
determine the. water column ambient current profile and, in particular,
the vertical shear, i.e., the change of horizontal current with depth at
the time of discharge and during the subsequent tracking period. Since
the tracking ship crosses a plume in about 15-30 sec, it was not antici-
pated that the ADCP should provide data on plume-related currents.
Furthermore, since the key assumption of spatial homogeneity of currents
in different beam "look" directions for the JANUS geometry is clearly
violated for dredged material discharge plumes, it is unrealistic to
expect reliable horizontal current data for plume traverses. However,
once the initial transient currents generated by the falling plume
material have been reduced or eliminated and the "quasi-equilibrium"
plume condition has been reached, then reliable current data may be
gathered during (residual) plume traverses.
Nevertheless, it was decided to reduce the ADCP sample intervals to
30 seconds to evaluate ADCP plume-related current data. The sample
intervals were reduced to 30 seconds for the second and third days. The
processed current profiles are presented in Appendices CI, C2 and C3.
Appendix Cl presents horizontal (north and east) and vertical
current components with AGC (Automatic Gain Control) amplitude at fixed
21
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depths for all transects of each dump. When the ship was inside the
plume judging from the acoustic profiles, the current components are
represented by different symbols. Those current measurements outside the
tracked plume are represented by a star (*) symbol. Whenever a question
mark (?) appears, it indicates the current data at that depth were
invalid and are placed there for continuity of the time series. For each
transect at a fixed depth, two plots were presented to indicate the
current direction and its speed.
Appendix C2 presents current measurements as a function of depth at
different times either from the center position of each transect or from
all positions within one transect for each dump. The time indicated in
the plots is the guide to tell whether it is a collection of all center
positions of the transects or a collection of all measurements within the
plume. In most of the cases, the north component keeps constant to the
thermocline depth and then decreases with depth, and sometimes reverses
direction in deep water. The maximum north component can be as high as
150 cm/sec. The east component mostly fluctuates between +20 cnv^sec to
-20 cnv/sec, with the maximum value sometimes reaching 60 cnv/sec. The
vertical component fluctuates as the east component does, but with a
smaller maximum value.
Appendix C3 presents five current measurements at fixed depths for
each transect of all dumps. Based on the ship track, the plots were
rearranged such that the directions of transects are the same from west
to east when several transects were plotted together. No consistent
pattern was observed. Four consecutive current measurements for each
transect of all dumps are also plotted and shown to indicate the change
of current within the plume.
Hie ADCP also provides an echo amplitude signal that represents the
concentration of suspended material in the water column. Appendix C4
22
-------
shows time series of echo amplitudes that were observed at fixed depths
and corrected for spherical spreading during Phase I. The depth
intervals are between 10 m and 130 m with a 20 m increment for the eight
depths in each plot. Generally, the top curve is for a 10 m depth and
the bottom curve is for 130 m depth.
The ADCP current profiles were processed with programs developed in
NQAA/AOML that are similar to programs provided by R&D Instruments. The
transmit pulse and bin length is 4 m for 150 kHz frequency. The data
were averaged over 30 seconds which consists of 9 individual pings. The
standard deviations of north and east current are 19.7 cm/sec and
18.5 cn\/sec respectively (Atle Lohrmann, personal communication). They
include the variance introduced by ship motion (pitch and roll) and the
variation in the current field over the survey area as well as the
instrument noise. The standard deviation of the vertical current
measurements is 9.5 aVsec which includes the instrument noise and the
variation introduced by the ship motion. Variances of both east current
component and vertical component are almost as large as the magnitudes
themselves.
Dredged Materials
The disposed material was dredged from the turning basin of Miami
Harbor shown as a star in Fig. 7. Sediment samples and field data were
collected from this basin area on' December 12, 1988 and again on April
19, 1989. The 1988 sample stations were labeled MHTB-1 to MHTB-3 and
shown as * in the lower left corner insert of Fig. 7. The gradation
curves for 1988 data are shown in Fig. 8 for all' three stations. An
individual curve of each station is presented in Appendix D along with
corresponding suspended sediment-time curves for test specimens of
23
-------
CORPS OF £NG'N£gR5
MIAMI
t CUOC COVMT?
M^er rtiiMrpiAu
^^•(A«AH0O«|(Q
«crto
t
W fl«6Uft fT
MHTB-1 *
MHTB-2 *
MHTB-3
Sediment Stations
Miami Harbor Turning Basin
MIAMI HARBOR. FLA.
ICALC W 'CCT
DCPARTMEKT of TMt AMfT
VACKSOffYllLC OlSTlllCT, C0*P9 Of (WUtltM
jACJCiOffvriLC, njJ/GSA
Fig. 7. Location map of the Miami Harbor. The turning basin is
indicated as a * at the end of the Miami Ship Channel.
Ttie insert at the lower left corner shows the three
sediment stations.
?Cl
-------
Gradation Curves
M
Class
IT
ifioation
Sand
Co4r^
Medium
Fine
Silt
Cojric
F.r*
CJay
Co*rw
Medium
Fine
j-.
• MHTB-J
X MHTB-2
a MHTB-3
10
1.0
01 0.01
Grain Size (mm)
0.001
ooooi
Fig. 8. Gradation curves of particle-size distribution for
the three sediment stations in the Miami Harbor
Turning Basin.
?c;
-------
50 gras/liter and 100 gms/liter. The most common materials are coarse
silt and fine to medium sand.
Acoustic Profiles
There were two types of acoustic data recording. CXie type was
recorded on Raytheon thermal paper recorder, which was also displayed in
real time during the field study. Portions of these acoustic echograms
are shown in Appendix El, which correspond to transects of the eight
dumps during a three-day period. The vertical coordinates are depth in
meters and have different depth scales for different dumps. The
horizontal coordinates show hour and minute. Except the first dump on
April 24, 1991 (page El—2), all time scales shown represent a 21 minute
time period, and have a horizontal distance of 1890 m when the ship speed
was taken to be constant at 3 knots for all transects.
The other type of acoustic data was recorded on DAT tapes. These
data represent the same data as the first type, but can provide more
detailed plume structure when processed numerically to extract the
acoustic backscattering intensity from the data. The acoustic intensity
is considered to be proportional to the particulate concentration (Tsai,
1984), and contour plots of equal intensity levels will provide the
detected sediment plume field for each transect. These contour plots are
shown in Appendix E2. The concentration levels are shown in db and
equivalent to backscattering strength which is proportional to the
logarithm of acoustic intensity. The actual processing is summarized in
the following.
The recorded acoustic signal on DAT represents the root mean square
voltage V in integer format at the output of the receiver. This 10-kHz
double side band signal was filtered to remove 60-cycle noise and to
provide anti-aliasing protection for analog demodulation. Output from
26
-------
the demodulator was further filtered and amplified for input to a 12-bit
analog to digital (A/D) converter interfaced to an IBM compatible
personal computer (PC). The voltage at the input of the A/D converter is
proportional to the root mean square plane wave sound pressure P at a
reference location 1 m from the face of the acoustic transducer, that is,
20Log(V) = RR + RL + G
where FR is the receiving response of the transducer given in decibels
referenced to 1 volt per micropascal (db/lV/luPa), G is the overall
system gain in db, and RL is the reverberation level given by
RL = 20Log(P).
For a cloud of particulate scatterers such as a sediment plume, the
reverberation level is given by
RL = SL - 20Log(r) - 2ar + S + 10Log(ctb/2),
where SL is the source level (db/uPa/V), r is range in meters, a is
absorption coefficient in db/to, S is the volume scattering strength in
db, c is speed of sound in the water and is taken to be 1500 iVsec, t is
transmitted pulse duration in sec, and b is equivalent solid angle of a
uniform beam containing the same integrated power as the actual trans-
mitted beam and is given in steradians. Therefore, the volume scattering
strength is
S - 20Log(V) - RR - G - SL +20Log(r) + 2ar - 10Log( ctb/2).
These scattering strengths represent the waste concentrations observed in
the water column, and are plotted in constant levels as contours shown in
Appendix E2.
27
-------
The horizontal axis of those contour plots is distance in meters
which is calculated from time of transect by the ship velocity of 3
knots. One of the important observations is the waste materials near the
ocean bottom at the first few transects. It is proved that the material
does reach the bottom and acoustic imaging is useful to provide
information for tracking wastes even in strong current and deep water.
During the first or two transects of each dump, it appears to indicate
that acoustic signals were blocked by the bubbles generated during the
dumping process. It occurred in the Mobile Bay Project too.
Appendix E3 shows time series of acoustic backscattering strength at
fixed depth for Phase I. Each plot represents waste concentration at one
fixed depth for one particular dump. Each peak of the time series is the
observed plume and its peak value provides the maximum waste
concentration during that particular transect. Hie distance obtained by
multiplying time by tracking ship speed gives the plume width at that
time.
Appendix E4 is an illusion of detailed plume structure at fi'xed
depth for a particular transect. The plume width increases with depth to
some point and stays unchanged or even decreases thereafter in most
cases. The plume width also increases with time as indicated by
transects at later times. However, the peak value or maximum
concentration decreases both with depth and time in general.
IV. DISCUSSION
A central question in the present study is whether the discharged
material remained within the designed site boundaries. The present study
encompassed a grand total of six days, April 24 through 26, 1990, and
June 26 through 28, 1990. Discharge events occurred in the period of
April 24 through April 26, 1990, so that observations on discharged
28
-------
material remaining within the site are restricted to this 72-hour period.
Generally speaking, there are two time frames regarding escape of
material from the designed site: a short term time frame, e.g., a few
hours or so and a larger term time frame extending over days and beyond.
Model results have indicated that the vast bulk of the discharged
material should fall directly to the bottom and that a gradually
diminishing quantity of material should remain within the water column.
The material that remains within the water column for some period of time
is expected to be "fine" material, i.e., of small size, and of low
concentration. In the early stage of a dredging operation, the material
dredged may contain much "fines" whereas as the operation continues a
lesser quantity of fines may result.
Consider the sequence of plume transects presented in Fig. 9. The
first transect, shown in Fig. 9(a), was taken less than one minute after
initiation of discharge. Acoustic returns are obtained from throughout
the water column to the bottom. Thus a portion, most likely the largest
portion, of discharge material falls rapidly to the bottom. A portion of
the material remains within the water column as a wispy cloud. This
portion was tracked not only for the discharge shown in Fig. 9(b) to (d),
but for each discharge in the entire study.
It may be readily discerned from these data that the width of the
discharged plume increases with depth. This increase in width with depth
is due to the entrainment process. ' An entrainment coefficient, a, may be
estimated directly from the acoustical data. To see this, Brandsma and
Divoky (1976) that the entrainment, E, may be expressed as
E » Aa (v - v )
X *
29
-------
04-26-90 14:16.00-14:18:30 04-26-90 14:18:30-14:21:00
0 20 40 60 BO 100 120 MO 160 160 200 220 0 20 40 60 80 100 120 140 160 180 200 220
i^->
o
04-26-90 14:25:30-14:28:00
a. 80 -
0 20 40 60 80 100 120 140 160 180 200 220
Distance (M)
04-26-90 14:31:30-14:34:00
100 -
20 -
100 120 140 160 160 200 220
Distance (M)
rig. 9. Acoustic iso-concentration contours of one dump on April 26, 1990,
corresponding to four transect at different times. TTie qap in
concentration indicated in (a) at 90 to 100 m distance is attributed
to acoustic absorption at the frequency of 20 kHz by a cloud of
bubbles in the water near the surface.
-------
where A «= area of hemispherical dump volume,
a » entrainment coefficient,
v « vector velocity of discharged material,
v^ - vector velocity of ambient water.
For v >> va
clV/dt = aA(dz/dt)
where V * volume of hemispheric discharge. Then,
a - (1/A) (dV/dz),
and for a hemispheric radius, r,
V = (2/3) Jir3 ,
A - 2jir2
so that
a - dr/dz.
Thus, by measuring the coordinates, i.e., depth and distance, of an
iso-backscatter contour at two different depths, the value of a may be
estimated. For example, from Fig. 10, for the iso-concentration line
marking the outer boundary of the • plume, i.e., scattering strength above
background equals -70 decibels, at 20 m depth, a horizontal coordinate of
118 m is indicated while at 50 m depth, a horizontal coordinate of 138 m
is indicated. Thus,
a - dr/dz « (138-118)/(50-20) = 0.67.
31
-------
SCATTERING STRENGTH ABOVE BACKGROUND
MHDP 04-26-90 14:16:00—14:18:30 Background time = 14:16:00
Vertical avg. = 3.0 meters. Repeated 5 times.
Horizontal avg. = 2.50 seconds. Threshold = 15.0 millivolts.
D.C. Offset = 0.0 millivolts. Absorption coefficient = .00500 dB/m.
Q_ 80
80 100 120 140 160 180 200 220
Distance (M)
m
ein
L~3
ABOVE
-40
-45
-50
-55
-60
-65
-70
-75
BELOW
-35
-35
-40
-45
-50
-55
-60
-65
-70
-75
Fig. 10. Acoustic iso-concentration contours of the first transect
of Fig. 9, showing thfe method to calculate the entrainment
coefficients. The backscattering strength levels shown in
Figs. 9 and 10 are in decibels and represent particulate
concentrations of suspended mat lis in the water column.
-------
for a given discharge plume, two estimates for a may be made: a plume
ingress estimate and a plume egress estimate. Depending on the circum-
stances of the discharge and time of transect, both or neither estimates
may be made. For Fig. 10, the egress estimate appears superior to the
ingress estimate. Nevertheless, in the 25 m to 50 m depth interval, an
ingress estimate for a of 0.57 was obtained.
Estimates of a have been made for various discharges in the present
rtudy; these estimates are summarized in Table 3. In selecting the depth
interval for estimation of a, some care with regard to the water column
vertical density structures and current structure must be given. From
the density profile shown in Fig. 11, it may be seen that the upper 50 m
c r so of the water column are well mixed with little structure in the
censity profile. At about 55 m depth, a density step occurs and struc-
ture appears within the water column. A change in the slope of the
iso-backscattering contour line occurs there, thus leading to a different
estimate for a in that depth region.
The wispy clouds of material which remain within the water column
cradually diminish in density or concentration as time goes by; within
the first 20 minutes the concentration of material within the water
column and below the 50 m depth horizon diminishes by about four orders
cf magnitude. Note that this concentration reduction is measured rela-
tive to the concentration which existed within the water column about two
minutes after discharge. The reduction of water column concentration
with time is illustrated in Figs. 12 and 13 for a discharge on April 26,
1990 and in Fig. 14.
Various processes affect the cloud of discharged material remaining
within the water column. One of these processes is the advection of the
material by ambient water currents. Our concern is principally with the
horizontal advection of the material; ambient vertical currents were in
33""
-------
Table 3
Entrainment Coefficients calculated frcm acoustic profiles.
lhe ingress and egress depths are water depths used to
calculate the the Entrainment Coefficients.
Dump Date Time Interval Ingress Egress
Estimate Depth Estimate Depth
2
04/24/90
16:13:30-16:15:30
0.74
50
m
0.80
80
m
5
04/25/90
14:37:00-14:39:30
0.78
50
ra
0.50
30
m
7
04/26/90
11:29:30-11:31:30
0.53
60
m
0.83
40
m
8
04/26/90
14:16:30-14:18:00
0.57
50
m
0.67
60
m
Average
Standard Deviation
0.66
0.11
0.70
0.13
-------
Temperature (deg C)
16.0 18.0 20.0 22.0 24.0 26.0
i i i i i i
Salinity (ppt)
35.0 35.4 35.8 36.2 36.6 37.0
0.C
MHDP-I 04/25/90 15:59:00
24.0-
i—D
E 48.0-
—S
jC
J" 72.0-
96.0-
120.0
24.6
25.2
24.0
25.8
26.4
27.0
Sigma-t
Fig. 11. Temperature, salinity and density profiles at 15:59:00
on April 25, 1990 during Phase I.
-------
MH0PU60 14 16.00- 14 36 00 20KHj Background lima* M: 16:00
Depth - JO 0 meters
-20-i
-120
220-
| 190-
Q.
^ 160-
130
8 10 12 14 16 18 20
Time (minutes)
MHDPI 160 14 16 00- 1 4 J 6:00 20KH2 Dock ground time k | 4 16 00
Depth - 50 0 meters
-70-,
-40 -
cn
C
-60
-»0
- 100
•120
190 -1
160-
° 130
o
100
1 ' 1 I 1
8 10 12 14
Time (minutes)
16
> 1 ¦
18
• 1
20
Fig. 12. Comparison between acoustic scattering strength from ACP
and echo amplitude from ADCP at 30 m and 50 m. Top: from
ACP; bottom: from ADCP.
-------
LO
WH0P116D 14:16:00-106 00 20KH* Oockground lima* 1 4:1 6.00
Ocplh - 70 0 meters
-20-1
-40-
(/)
cr
c
190 -i
T3
D
160-
Q.
£
O
r
1 JO-
u
LJ
100
¦ i ¦' t ' * i
2 4
• I ' ¦ ' I ¦ ¦ ' I '
8 10 12
Time (minutes)
• i '
14
16
¦—i—1—«—¦—i
18 20
MHDP116B 14-16 00- 14 3600 20KHi Background lime* 1 4.1 6 00
Deplh ¦» 90 0 meters
-20-,
-100
190-
° 160-
6 8 10 12 M 16 18 20
Timo (minutes)
Fig. 13. Comparison between acoustic scattering strength from ACP
and echo amplitude from ADCP at 70 m and 90 m. Top: from
ACP; bottom: from ADCP.
-------
MHDP 04/26/90
for 40 m, 50 m, 60 m, 70 m, 80 m, 90 m, 100 m
Fig. 14. Peak concentration as function of time at six fixed depths
for April'26, 1990 during Phase I.
-------
general quite small during the exercise. A key question is the existence
of vertical shear within the water column and its effect in displacing
the upper portion of water column material vs. the deeper portion of
water column material. There are two different components of data which
bear on this issue; the first is the acoustic Doppler measurements of the
north and east directed components of the ambient current as a function
of depth, and the second is the relative displacement of the centroid of
cloud concentration as a function of depth as determined from acoustic
backscattered measurements.
An estimate of the difference in the horizontal current vL at two
h
different depths in the water column zx and z2 can be made directly from
the backscatter amplitude information. The AGC amplitude will be used to
compare with Doppler estimates. For depths zx and z2, one can write
[vh (z2)-vh (zx ) ]t - c(z2 )-r(z1 ,
where t equals the time from initial discharge to the time of plume
observation, and r(z) is the range from coordinate origin (cyclindr'ical
coordinates) at the time of plume observation.
From Fig. 15, we see that the maximum time difference between peak
concentrations encounters at amy two depths in the water column is
approximately 30 seconds. Thus, for a ship speed of 1.5 in/sec,
r(z,)-r(z,) < 45 m = 4500 cm.
2 1 i
Then
vh(z2 )-vh(z1 ) < 4500/t
Now t « 18 minutes = 1080 seconds, so
v. (z, ) -v. (z, ) < 4.3 cm/sec.
n 2 11
39
-------
MHDP-I ADCP 04/26/90
Begin at 14:15:51
2501
200-
UJ
100-
50
14
Time (minutes)
Fig. 15. Time series of echo amplitudes at seven fixed depth; from 10 m
(top) to 130 m (bottom) for'April 26, 1990 during Hiase I.
-------
How does the Doppler estimate compare with the proceeding result?
From Fig. 16, we note that there is much variability in the estimate of
horizontal (north) velocity from the ADCP. If the first two plume
transects are disregarded, the remaining transects indicate very little
vertical shear to be present with an uncertainty greater than the
AGC-derived limit.
In each of the discharge events, a portion of the discharged
material was observed to remain in the upper portion of the water column.
iMs material remaining in the upper part of the water column exists as a
wispy cloud having undergone a reduction in concentration in excess of
three orders of magnitude from the original concentration which existed
immediately after discharge. The material below 50 m depth in the water
column has undergone em even greater reduction in concentration.
A series of plume crossings was carried out for approximately
one-half hour after discharge. The locations and time of these plume
crossings for each of the discharges is shown on pages A2 to A6 of
Appendix A. We see that for each discharge the motion of the material
remaining in the upper portion of the water column is generally in'a
north-northeast direction. The discharges occurred over a three-day
period and available ship tracks resulting from an approximately 48 hour
period consistently indicated a generally north-northest movement of the
residual plume material. The discharge site is sufficiently far at sea
that tidal current influences are expected to be minimal.
V. RESULTS
(1) Acoustical detection and mapping of dredged material discharge plume
within the entire water column and impacting the ocean bottom, have
been made for the interim Miami ODMDS located at the western edge of
the Florida Current (Gulf Stream). These detections and complete
41
-------
ADCP 04/26/90
ADCP 04/26/90
-fc»
(\5
E
u
u
>
E
V
o
z
1 00.0 T
60 OH
20.0-
-20.0H
-60.0 H
I 4.1 7:51
I 4:20:2 J
14-26:21
14:32:21
14-39:52
-ioo.o-
00
20 0
40.0
60.0
80.0
o
u
>
'€
£
150.0-1
90.0-
30.0 H
-30.0-
-90.0-
100.0
14:17:51
I 4:20:23
14:28:21
14:32:21
I 4:39:52
-150.0-
0 0 20 0 40 0 60.0
O^plh- (m)
80.0
100.0
E
U
8
2
E
CJ
ft
o
UJ
150 O-i
90.0
30.0
-30.0
-90.0
-150.0
0.0
250.0-)
j
210.0-
a 170.0
20.0
40.0
60.0
80.0
^ 130.0
90.0
50.0
T
0.0 20.0 40 0 60.0
Depth (m)
80 0
4 17 51
4-20 23
4 28 21
4 32 2 1
4 39 5)2
100 0
4-17-51
4:20-23
4 26 21
4-32 21
4 39 52
100 0
Fig. 16. Current profiles for the five transects of the second
dump on April 26, 1990 during Phase I.
-------
mappings have been achieved at the deepest dredged material site
(typically 140 m depth) studied to date.
(2) A high concentration central portion of the discharge descended
quickly and directly to the bottom. This central portion descended
with a speed of 2 m per second or greater.
(3) The deep water discharge plumes observed in this study displayed the
major generic features observed in shallow water discharge plumes,
namely lateral growth through entrainraent, rapid descend of a
central core, impact with the bottom and formation of an expanding
bottom surge and rapid decrease of water column concentration
residual with time.
(4) Of the residual material left in the water column, that material
below about 50 m depth underwent approximately a four order of
magnitude reduction in concentration in one-half hour while that
remaining in the upper portion of water column underwent approxi-
mately a three order of magnitude reduction in concentration.
(5) Over the time period during which the residual material remaining
within the water column from various discharges was detected and
tracked, about 48 hours, the general movement was towards the
north-northeast. Vertical current shear did not separate the top
and bottom portions of the plume in most cases of the observations.
VI. CONCLUSIONS AND COMMENTARY
The key conclusion is that the material discharged , except for a
low concentration residual remaining within the water column, reached
bottom within the designated site boundaries. A total of eight discharge
plumes were detected and tracked for a period of about one-half hour on
average; for the three day time period during which the discharge
43
-------
occurred, the resulting plumes were observed to be transported in a north
to northeast direction.
A very interesting point regarding the knowledge gained on
discharged plume behavior during the course of the present three day
study is this: while it is a valid criticism that only a very limited
sample of ambient current conditions were obtained during the course of
the study, and that the ambient current field may undergo significant
changes in both magnitude and direction over the course of a year thereby
significantly affecting the transport of any residual plume material left
within the water column, the same may not be said of the ambient density
profile. That is to say, so long as the physical structure and constitu-
tion of the dredged material being discharged remains essentially the
same, it may be expected that the changes which occur over the course of
a year in the ambient water column density structure will not signifi-
cantly alter the main discharge features, as listed in section V, item 3,
observed in the present study.
The principal basis for this conjpcture is that a very rapid
convective descent of a central core plume discharge portion is oberved
to occur. The discharge material descends at a much higher rate than
would be expected on the basis of individual particulate settling
velocities, thereby indicating a cohesive body structure in the central
plume. This descent is so rapid that any variations which may be
expected to occur in the water column density profile over the course of
a year will not significantly affect the descent.
The effects of water column density structure are, however, of
significance in affecting both the formation and longer-term fate of the
water column residual plume. It is this residual plume which is most
strongly affected by both ambient current and density water column
profiles.
44
-------
Not addressed in the present study is the issue of resuspension of
material deposited on the ocean's bottom. To address this question,
near-bottom current data is required and observation of resuspension
events, if any.
VII. ACKNCWLEDGMENTS
The help and assistance in planning and execution of the present
study of Mr. Mark Skarbek of the Jacksonville District and of Dr. Nick
Krause of the Waterways Experiment Station are hereby gratefully
acknowledged. The expert electronic assistance of Charles A. Lauter is
appreciated.
VIII. REFERENCES
Brandsma, M. G., and D. J. Divoky, 1.976. Development of models for
prediction of short-term fate of dredged material discharged in the
estuarine environment. Report D-76-5, U.S. Army Engineering
Waterways Experiment Station, Vicksburg, Miss.
Conservation Consultants, Inc., 1985. Environmental survey in the
vicinity of an ocean dredged material disposal site, Miami Harbor,
Florida. Final Report to EPA.
EPA, 1990. Draft environmental impact statement for iesignation of a
dredged material disposal site located offshore Miami, Florida.
Wetlands and Coastal Programs Section, U.S. Environmental Protection
Agency, Region V, Atlanta, Georgia.
Lee, T. N., I. Brooks, and W. Duing, 1977. The Florida Current: Its
structure and variability. Technical Report No. 77033, University
of Miami, Rosenstiel School of Marine and Atmospheric Sciences.
45
-------
Lee, T. N., and D. A. Mayer, 1977. Low-frequency current variability and
spin-off eddies along the continental shelf off southeast Florida.
J. Mar. Res., 35 (1), 193-220.
Lee, T. N., and C. N. K. Mooers, 1977. Near-bottom temperature and
current variability over the Miami slope and terrace. Bull. Mar.
Sci., 27 (4), 758-775.
Proni, J. R., F. C. Newman, E. R. Meyer, H. B. Stewart, D. J. Walter, R.
L. Sellers, and C. A. Lauter, 1977. On the use of acoustics in
applied, oceanographic and coastal engineering problems with emphasis
on the oceanic transport of particulate material. Thalassia
Juqoslavica, 13, 389-393.
Proni, J. R., F. C. Newman, R. L. Sellers, and C. Parker, 1976. Acoustic
tracking of of ocean-dumped sewage sludge. Science, 193, 1005-1007.
Scheffner, N. W., and A. Swain, 1989. Evaluation of thu dispersion
characteristics of the Miami and Fort Pierce dredged material
disposal sites. Coastal Engineering Research Center, Final Report
to U.S. Army Engineer District, Jacksonville.
Trefry, J. H., and J. R. Proni, 1983. Drilling fluid discharge near the
Texas Flower'Gardens, northwest Gulf of Mexico. In: Energy Wastes
in the Ocean, I. W. Duedall (ed.), Wiley-Interscience, New York.
Tsai, J. J., 1984. Acoustic remote sensing of waste disposal. NQAA
Tech. Memo. ERL AOML-59, 100 pp.
Tsai, J. J., and J. R. Proni, 1985. 'Acoustic study of dredged-material
dumping in the New York Bight. _In: Wastes in the C:ean, Vol. 6,
Near-Shore Waste Disposal, B. Ketchum et al. (eds.),
Wiley-Interscience, New York.
46
-------
APPENDIX G
MIAMI HARBOR DREDGED MATERIAL DISPOSAL PROJECT.
TOTAL SUSPENDED SOLIDS MEASUREMENTS
-------
MIAMI HARBOR DREDGE MATERIAL
DISPOSAL PROJECT:
Total Suspended,Solids Measurements
John R. Proni, Jules F. Craynock, John J. Tsai
A Report to the
U.S. Army Corps of Engineers
National Oceanic & Atmospheric Administration
Atlantic Oceanographic and Meteorological Laboratory
4301 Rickenbacker Causeway
Miami, Florida 33145
April 16, 1993
-------
Mention of a caimercial establishment, company or product does not
constitute any endorsement by the fO^/Environmental Research
laboratories or the U.S. Government. Use, for publicity or
advertisement, of information fran this publication concerning
proprietary products or their testing is not authorized. This report
has been prepared by personnel of the Ocean Acoustics Division and
represents their best scientific judgement. This report does not
represent any official position by the National Oceanic and Atmospheric
AAninistration.
-------
TABLE OF CONTENTS
I. Introduction pg 1
i
II. Procedure 1
III. Data Presentation & Analysis 2
A. Presentation 2
Discharge One 2
Discharge Two 3
Discharge Three 3
Discharge Four 4
Discharge Five 4
Discharge Six 4
Discharge Seven 4
Background Samples 5
B. Analysis 5
Summary 9
Acknowledgements 9
References 10
List of Figures 11
Appendix
-------
I. INTRODUCTION
In April 1990, a field data collection project was undertaken to investigate the short-
term fate of dredged material discharged in the designated Miami Ocean Dredged
Material Disposal Site (ODMDS) before dredging of the Miami River and the Miami
Harbor Turning Basin begins. A discussion of this project is presented in reference one
and two. As part of the study, series of water column samples of total suspended
material was obtained. Later, in June 1991, a second project was carried out in order to
obtain an expanded series of background water column suspended material values.
II. PROCEDURE
Sediment plumes resulting from eight placement operations, occurring in the period
April 24 to April 26, 1990, of dredged material were sampled and monitored acoustically.
A test discharge, for logistics evaluation, was conducted in the morning of April 24th.
Water column sediment sampling was guided by acoustical systems employed, in
particular by the Acoustic Concentration Profiler or ACP, and by visual surface detections
of subsequent-to-discharge plumes. Before each discharge, and between successive
discharges, the surveying vessel Seaward Explorer monitored the water column to obtain
background concentrations of suspended material and ambient currents :n the area using
the ACP and ADCP on board the surveying vessel. Ambient density ;ind salinity
were measured by taking CTD casts at locations of previous discharge that were
determined from ship track records. Sediment samples were collected directly from the
dredging vessel Atchafalaya for each discharge. Discharge occurred when the
1
-------
Atchafalaya began to turn to return shoreward. The ACP was set ready to operate upon
the approach of Atchafalaya, and the Seaward Explorer proceeded to make the transects
immediately after the dumping commenced. The Seaward Explorer tracked the sediment
plume for several transects until the concentration of suspended material could no longer
be detected by the ACP. This reduction in concentration usually took about 60 minutes
after the release. During each transect, water samples were collected by a towed V-Fin
with a pump that discharged water continuously via a hose to the deck of the Seaward
Explorer. The water sampling took place at approximately constant depth by maintaining
constant ship speed, and only during the periods when transects crossed the plume.
Ship position was determined using LORAN and GPS and was automatically logged with
a computer and displayed in real time to assist monitoring. Surface features of the
sediment plume were visible up to 60 minutes after discharge and were helpful in tracking
the plume.
III. DATA PRESENTATION AND ANALYSIS
(A) Presentation
Three data sets for each discharge are presented: (i) acoustical data including the
first several transects for each discharge (ii) track data for each discharge and (iii) water
bottle sample data for each discharge.
Discharge One
The first discharge of the study occurred at about 16:14 on April 24, 1990. In
Figure 1 the acoustical data are shown from the first five passes over the discharge
2
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plume. The Seaward Explorer first encountered the discharge plume between 16:14 and
16:15. Other encounters shown in Figure 1 occurred at about 16:17, 16:19,16:21 and
16:26. In Figure 2 the ship track for this discharge event is shown. Plume encounters
were made at various times subsequent to the first few minutes following the discharge
event shown in Figure 1. These encounters are marked by various symbols on the ship's
track. For example, the encounter at 16:40 is marked by a hexagon, the encounter at
16:45 with a triangle and so on. The small stars are time marks. In Table I, the
concentrations of particulate matter, measured in mg/liter, for the sample stations shown
in Figure 2 are given. The sample concentration values are plotted against time after
discharge in Figure 3.
Discharge Two
The second discharge occurred at about 09:37 on April 25, 1990. In Figure 4 the
acoustical data from the first five passes over the discharge are shown. The track data
for discharge two are shown in Figure 5. The suspended particulate values measured
are given in Table II and plotted in Figure 6.
Discharge Three
Discharge three occurred at 12:04 on April 25, 1990. The acoustical data for the
first six passes over this discharge are shown in Figures 7 and 8. Extensive absorption
by bubbles is seen in the first pass over this discharge. Some residual bubble absorption
is seen in the second pass over the discharge and no discernable absorption is seen in
^ny of the subsequent plume encounters The track data for discharge three are shown
3
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in Figure 9. The suspended particulate values measured during discharge three are
shown in Figure 10.
Discharge Four
Discharge four occurred at about 14:37:30 on April 25, 1990. The acoustical data
for the various transects over this discharge are presented in Figure 11. The
corresponding ships track is presented in Figure 12. The corresponding total suspended
material data is presented in Figure 13.
Discharge Five
Discharge five occurred at about 17:49 on April 25, 1990. The acoustical data for
the various transects over the discharge are presented in Figure 14. The corresponding
ship track and total suspended solids (TSS) data are presented in Figures 15 and 16,.
respectively.
Discharge Six
Discharge six occurred at about 11:30 on April 26, 1990. No track data was
available for this discharge. The acoustical data for the various transects over the
discharge are presented in Figure 17. The corresponding TSS data is presented in
Figure 18.
Discharge Seven
Discharge seven occurred at about 14:16 on April 26, 1990. No track data was
available for this discharge. The acoustical data for the various transects over the
discharge are presented in Figure 19 The corresponding TSS data is presented in
Figure 20.
4
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June 1991 Background Samples
Additional Background TSS Measurements were obtained by NOAA/OAD and US
Army Corps of Engineers personnel aboard the S/V Sable on June 27 and 28, 1991.
These data are presented in the appendix. Sampling transects were conducted through
Government Cut and north and south atong the predominant offshore reef line. Water
samples for TSS analysis were collected using a small V-Fin pump sampler deployed
from the side of the S/V Sable. Simultaneous CTD casts were conducted utilizing a
Seabird CTD system. Pumped samples were analyzed for turbidity with a HACH portable
turbidimeter. Offshore fixes were determined via LORAN-C, samples sites A, B, C within
Government Cut were determined by shore sightings. Table A-1 and Table A-2
summarize the TSS/turbidity measurements. Charts 1, 2, and 3 indicate sampling
positions as well as a detailed depiction of the Government Cut positions. CTD cast data
are included for each of the stations completed within the two days. On both days of
operations sample stations were conducted during an outgoing tide. Ship traffic during
the sampling period through Government Cut was relatively light and seas we're calm.
(B) Analysis
As discussed in reference one, during the disposal operation a quantity of the
dredged material discharged remains suspended for some period of time within the water
column. Although the bulk of the discharged material is thought to descend as a
cohesive mass, a small portion ot the, perhaps in the form of individual fines, are thought
5
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to remain within the water column. Entrapment processes, which are known to occur
within such discharges, could play a key role in the formation of the residual cloud of
material within the water column. Once the residual cloud is formed, the cloud then drifts
with the ambient current with continued settling and dispersion of the cloud material.
In the present study, samples of the residual cloud material were gathered using
a pumping system to fill water bottles aboard ship. The nozzle of the hose used in the
pumping system is attached to a V-Fin device which was towed about 1 meter below the
ocean's surface. It took about 30 seconds to fill a bottle, so with a ship's speed typically
being one to two knots, or 0.5 m/sec to 1.0 m/sec, water is included in the sample
gathered over a 15 to 30 meter distance. This has the effect of smoothing peak
concentration values in cloud volumes of size less than about 30 meters. This smoothing
effect is more pronounced in the earlier portion of residual water column material tracking
than in later portions, say three or so minutes after discharge, as the material has
dispersed or spread out in space and has become more homogeneous through mixing.
Consider the TSS data displayed in Figure 10 for discharge number three. This
data displays a series of peaks of diminishing order in time, i.e. 61 mg/l, 10.2 mg/l, 5.8
mg/l, 1.9 mg/l and 2.0 mg/l, separated by a set of relatively low concentration sample
values. This data is interpreted in the following way: the sampling device more accurately
passed through higher concentration regions of the cloud (at the towing depth of the V-
fin) to obtain the afore-listed concentration peaks and in between those peaks did not so
accurately target or pass through high concentration regions of the cloud. Inasmuch as
it is always a question in sampling of material discharged in the ocean as to whether the
6
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sampling device was indeed within the volume of material to be sampled, it is noted that
the basic confirmation for proper space-time sampling was achieved using acoustical
devices. In addition to acoustical detection of residual water column material a visible
ocean surface signature (a milk-like coloring) was available. The acoustical systems
show the subsurface distribution of material corresponding to a particular surface
detection
TSS values for all discharges plotted against time are shown in Figure 21. A
background concentration estimate may be obtained from the lowest of the TSS values
shown in Table I, as such values presumably are obtained from complete or partial
"misses' in sampling of the residual plume. A second background concentration estimate
may be made from the data gathered on June 27 and 28, 1991 and displayed in Table
II assuming, of course, that data gathered on those dates are also applicable for April
1990. Using the data from Table II gathered at those points proximate to the designated
discharge area (stations 1,2,3,5,6 and 7 for Jun 27, 1991 and station 6 for June 28, 1991
a background value of about 0.5 mg/l is obtained. Using in-between-peak low values
from discharge 2 for example, a background value of about 0.2 mg/l is obtained. As
discussed earlier, many of the values are judged to be gathered at locations somewhat
separated from cloud regions of highest concentration. Data from three of the discharges
have been selected and included in Figure 22 to obtain a smoother estimate of dilution
with time (or distance) from the discharge. Figure 22 has been constructed by
normalizing the data for three discharges, i.e discharges one, three and four, by the
largest (i.e. initial) value recorded for each discharge respectively. From among these
7
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three discharges local maximum values, i.e. values higher than at least one preceding
value were selected and plotted. An estimated fit curve has been drawn to give a crude
estimate of the normalized dilution with time or distance for discharges occurring within
the designated site. Thus, for example, an initial concentration of 80 mg/l would diminish
to 8 mg/l after one-half hour or at a distance of 900 meters from the point of discharge
(current speed assumed is 100 cm/sec).
In reference one, a very crude estimate was made of the quantity of material
residing within the residual water column cloud about 20 minutes after discharge. The
main drawbacks of that were the delineation of the geometric dimensions of the plume
of material within the water column and the lack of TSS measurements for a calibration
of the acoustical system. The geometric delineation issue is still not resolved so that the
assumption made in reference one, namely that the geometric delineation is provided by
the plume delineation beginning one to two meters below the ocean's surface, is still
required. The TSS measurements discussed in this document were obtained in the upper
few meters of the water column. The assumption made in reference one is that an
average TSS of about 10 mg/l is present in the residual cloud. If it is assumed that the
near-surface TSS data values are typical of the subsurface cloud as a whole, the 10 mg/l
assumed in reference one appears to be reasonable perhaps even conservative.
Retaining the 10 mg/l estimate a very crude estimate that about 0.6% of the total solid
material discharged remains within the water column about 20 minutes after discharge.
8
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SUMMARY
Total suspended material (TSS) samples were obtained for a number of dredged
material discharges at the Miami Ocean Dredged Material discharge site. Initial TSS
values gathered in the upper few meters of the water column, approximately one minute
after discharged, ranged from about 34 mg/l to 77 mg/l. A residual plume of dredged
material remained within the water column. The plume was tracked for about forty-five
minutes to one-hour and TSS samples obtained. About one-half hour after discharge
plume concentration was observed to have a value of about a few mg/l. The general
direction of movement of the residual plume cloud was North-Northeast.
ACKNOWLEDGEMENTS
The assistance and support of Dr. Nick Kraus and Michelle Thevenot, of the U.S.
Army Corps of Engineers Waterways Experiment Station, is greatly appreciated. The
support and field participation of Mr. Mark Skarbek of the Jacksonville District U.S. Army
Corps of Engineers is also greatly appreciated.
9
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REFERENCE
1. Tsai, J.J., Proni, J.R., Dammann, W.P., and Kraus, N.C., (1992), Dredged Material
Disposal at the Edge of the Florida Current, Chemistry and Ecology 6, pp. 169-187.
2. Proni, J.R., Tsai, J.J., and Dammann,. W.P., (1991), Miami Harbor Dredged Material
Disposal Project, A report to the U.S. Army Corps of Engineers.
10
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LIST OF FIGURES
Table 1 Total Water Column Suspended Material
Figure 1 Acoustic Record 04/24/90,16:11-16:31
Figure 2 Navigational Track 04/24/90,16:17-17:19
Figure 3 TSS Plot Discharge One
Figure 4 Acoustic Record 04/25/90, 09:35-09:55
Figure 5 Navigational Track 04/25/90,09:30-10:39
Figure 6 TSS Plot Discharge Two
Figure 7 Acoustic Record 04/25/90,12:03-12:23
Figure 8 Acoustic Record 04/25/90,12:17-12:37
Figure 9 Navigational Track 04/25/90, 12:05-12:59
Figure 10 TSS Plot Discharge Three
Figure 11 Acoustic Record 04/25/90,
Figure 12 Navigational Track 04/25/90,
Figure 13 TSS Plot Discharge Four
Figure 14 Acoustic Record 04/25/90,
Figure 15 Navigational Track 04/25/90,
Figure 16 TSS Plot Discharge Five
Figure 17 Acoustic Record . 04/26/90,
Figure 18 TSS Plot Discharge Six
Figure 19 Acoustic Record 04/26/90,
Figure 20 TSS Plot Discharge Seven
Figure 21 TSS Plot All Discharges
Figure 22 Normalized Concentration
Discharge One, Three and Four
Figure 23 Acoustic Record 04/24/90,
Test Discharge
14:36-14:56
14:30-15:09
17:40-18:00
16:30-17:59
11:29-11:49
14:15-14:35
11
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TABLE I
Total Water Column Suspended Material
Discharge TSS Time
# (mg/l) Since
Discharge
Discharge TSS Time
# (mg/l) Since
Discharge
Discharge TSS Time
# (mg/l) Since
Discharge
TEST
| 13:57
77.4
01:00
No. 2
09:37
0.0
00:00
No. 3
12:04
61.0
02:00
0.6
03:00
0.6
04:00
I No. 1
33.6
01:00
2.7
12:00
0.2
06:00
;
7.0
03:00
0.2
13:00
2.0
07:00
0.1
06:00
1.6
17:00
1.7
10:00
0.5
08:00
0.3
20:00
10.2
12:00
3.1
11:00
0.5
23:00
1.0
16:00
0.1
30:00
1.4
19:00
*0.4
34:00
5.8
20:00
I
0.0
38:00
1.1
24:00
0.2
42:00
0.2
29:00
0.5
46:00
1.9
35:00
0.2
55:00
0.8
39:00
0.2
56:00
2.0
49:00
-------
TABLE I continued
Total Water Column Suspended Material
Discharge TSS Time
# (mg/l) Since
Discharge
Discharge TSS Time
# (mg/l) Since
Discharge
Discharge TSS Time
# (mg/l) Since
Discharge
No. 4
29.5
00:30
No. 5
3.0
02:00
No. 6
0.1
00:00
0.6
08:30
2.0
04:00
0.1
02:00
3.4
11:30
3.3
05:00
0.5
05:00
|
1.1
16:30
5.1
06:00
4.5
08:00
0.3
19:30
0.6
07:00
1.2
14:00
1.7
22:30
0.1
17:00
1
'
0.8
20:00
0.9
26:00
0.6
31:00
1.2
38:00
0.4
45:00
TSS is measured in milligrams per liter
Time is measured in minutes and seconds
-------
TABLE I continued
Total Water Column Suspended Material
Discharge TSS Time
# (mg/l) Since
Discharge
No. 7
6.1
04:00
2.8
10:00
1.4
15:00
0.8
17:00
1.5
21:00
3.4
23:00
0.1
25:00
0.6
35:00
0.1
44:00
0.1
54:00
1.0
58:00
0.4
64:00
TSS is measured in milligrams
Time is measured in minutes and seconds
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0 5 10 15 20 25 30 35 40 45 50 55 60
Time (min)
Figure 16
-------
30-
60-
90-
120-
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Miami Harbor Project
Discharge No. 6
10 15 20 25 30 35 40
0
5
50 55 60
45
Time (min)
Figure 18
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102 I-
Miami Harbor Project
All Discharges
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0 5 10 15 20 25 30 35 40 45
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-------
Normalized Concentration
Discharges Nos. 1 , 3 & 4
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Time (min)
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1406
1412 1418
Time
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