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4-38
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4-39
-------
The analysis of the data indicates that there is a distinct ozone elevational gradient at Whiteface
Mt., and that the MCCP sites in the South experience higher cumulative ozone exposures than sites in
the North. Figure 4-61 (Appendix E) also indicates increased mean ozone concentration with elevation
for 19 ozone monitoring stations in the eastern U.S.( see Table 4-17 for station codes). The length of
time that the MCCP has monitored ozone is too short for investigating the existence of any temporal
trend. However, the Whiteface Mountain summit has an uninterrupted monitoring record since 1973.
As shown in Figure 4-62 (Appendix E), no trend in annual mean ozone concentration is discernable for
this 15 year time period.
Site Name
Rowland Forest (HF)
Moosilauke (MS)
Whiteface 1 (WF1)
Whiteface 3 (WF2)
Whiteface 4 (WF3)
Huntington Co., NY (HU)
Hampshire Co., MA (HA)
Beaver Co., PA (BE)
Shenandoah 1 (SHI)
Shenandoah 2 (SH2)
Shenandoah 3 (SH3)
Big Meadows, VA (BM)
Dickey Ridge, VA (DI)
Sawmill Run, VA (SM)
Whitetop Mtn, VA (WT)
Marion County, VA (MA)
Giles Co., TN (GI)
Mt. Mitchell 1 (MM1)
Mt. Mitchell 2 (MM2)
TABLE 4-17
Ozone Exposure
Sum of Season Dose
(for daylight hours 7AM - 6PM)
Sum of Season Dose (ppm * hr)
.> 0.07 ppm
1986 1987
N.D.
N.D.
2.29
N.D.
N.D.
5.09
9.14
N.D.
N.D.
N.D.
N.D.
5.56
3.21
11.39
N.D.
4.11
16.38
8.34
N.D.
0.82
7.81
9.68
9.41
3.47
5.74
9.26
13.06
9.49
9.01
6.07
28.50
31.07
26.80
38.54
9.27
16.73
5.14
6.68
1988
4.16
12.51
20.51
16.50
N.D.
11.36
34.93
31.70
23.27
39.44
20.88
31.89
40.25
30.16
37.68
26.92
28.91
45.17
19.49
4-40
-------
Sulfur Dioxide
Sulfur dioxide concentrations are very low throughout the network as indicated in Table 4-18.
Table 4-18
Sulfur Dioxide Measurements Summary for Selected MCCP Sites
Max Mean # hourly averages
Rowland HF 12 ppb 1.07 ppb 1371
Whiteface WF1 20 ppb 1.42 ppb 1990
Whiteface WF3 16 ppb 0.86 ppb 2962
Whitetop WT 47 ppb 2.08 ppb 4310
Mt. Mitchell MM1 12 ppb 1.41 ppb 996
Figures 4-63 through 4-66 (Appendix E) show the frequency distributions derived from
continuous SC>2 measurements. Stations operating on a weekly schedule (filterpack) reported similarly
low values for the warm season May 1 through October 31, 1987. The northern sites exhibited a strong
directional variability on the basis of 36-hour back trajectories. Air masses from the south and west had
significantly higher SO2 concentrations than air masses from any other sector. The southern stations
exhibited a more even pattern of SC>2 concentration as function of air mass trajectories. Because SC>2 is
the precursor gas to cloud water sulfate, it is not surprising to find similar directional variabilities for
both sulfur compounds.
Because of the very low concentration levels of sulfur dioxide during the warm season, it is very
difficult to reliably measure an altitudinal gradient. It is equally difficult to discern a geographic gradient
from the data set.
Hydrogen Peroxide
Hydrogen peroxide (P^C^) plays a key role in the formation of sulfuric acid in the atmosphere
(Calvert et al., 1985; Seigneur and Saxena, 1988). The aqueous phase oxidation of dissolved SC>2 by
H22 was applied to Norway spruce. Joslin et al. (1988)
showed that H2C>2 was effectively removed from cloud water upon contact with red spruce foliage.
Cloud water H2C>2 measurements from the MCCP network can help to quantify the role of this
compound as an oxidant and as a possible agent of forest damage.
Olszyna et al. (1988) reported cloud water HjC^ measurements for the MCCP site at Whitetop
Mountain, VA. The highest concentration measured (246.6 /trnol/1) was more than twice any previously
reported cloud concentration. Daum et al. (1984) used an aircraft to sample stratiform clouds in the
eastern USA and reported H2O2 concentrations varying from 0 to 75/tmol/l. Romer et al. (1985) used
an aircraft to collect cloud samples at various European locations and found that H2O2 concentrations
varied from 0.05 to 88 jtmol/1. Lazrus et al. (1985) reported that in 284 cloud samples at Whiteface
Mountain, NY, ^O^ concentrations varied from 0 to H2nmol/\. Kelly et al. (1985) reported total
peroxide (assumed to be H2O2) levels for an additional 190 cloud samples collected at Whiteface
Mountain and found similar H2C>2 levels (0 to 100 jtmol/1).
4-41
-------
Cloud water H2O2 levels for four MCCP sites from 1986-1988 are presented in Table 4-19. Not
all cloud water samples were analyzed for H£>2- Mean concentrations were similar for all sites except
Shenandoah, VA The low mean concentration reported for this site may be an artifact of the small
sample size. The highest H2O2 levels were recorded at each site during summer. Spring and fall levels
were typically less than half of the summer values. Kadlecek et al. (1985) reported H2O2 concentrations
in winter clouds at Whiteface Mountain to be always much lower than 1 /tmol/1. This seasonal trend is
no doubt due to the photochemical production rate of H2O2 in the gas phase, which would be expected
to exhibit a strong annual trend with maximum production in summer and minimum during winter.
The distribution of H2O2 concentrations in cloud water collected at the Whiteface and Whitetop
sites is shown in Figure 4-67 (Appendix E). A higher frequency of very high H2O2 concentrations was
observed at Whitetop Mountain, VA
TABLE 4-19
Cloud Water H2O2 Measurements at MCCP Summit Sites for 1986-88
All concentrations are in jonol/L
Site Minimum Maximum Mean # Samples
Whiteface, 1.6 136.4 37.7 54
Shenandoah, VA 0.3 49.0 12.3 22
Whitetop, VA 0.8 246.6 44.1 141
Mitchell, NC 0.3 196.0 41.9 236
THROUGHFALL
The chemistry of throughfall water is a composite of rain, cloud, and dry deposition, tree
emissions and absorptions, evaporation from the canopy, and biological activity on the canopy and in the
collected sample. Also, physical features (terrain slope and aspect, canopy structure and individual
canopy element geometry, and wind velocity) affect where canopy collection of rain and cloud occurs and
how the directed flow develops within the canopy. It is difficult to properly attribute the sources and
sinks to the correct mechanisms since they are difficult to measure separately and have considerable
variations across the canopy and within and between events.
For a rain event, there is an initial period during which the canopy is wetted until the storage
capacity is satisfied. The excess accumulation over evaporation drips through the canopy as throughfall
or flows down the tree trunk as stemflow. The common method for determining canopy storage capacity
involves linearly relating the unperturbed rain amounts (which can be subject to collection problems in
high wind environments) to the corresponding average throughfall from many events. The offset from
the origin provides the storage capacity, assuming that evaporation is much less than the water held by
the canopy.
For a cloud event, the storage capacity may be satisfied only after prolonged exposure to clouds.
While the cloud water may be relatively inconsequential to forest hydrology in most areas, it has the
potential to contribute to foliar/needle damage (because of the higher concentrations of dissolved species
in the cloud water as compared with rain, and the extended period of evaporation that further con-
centrates the less volatile chemicals). However, measurements of evaporation of intercepted water are
rare, further complicating efforts to quantify this process. Most events at high elevation are a mixture of
4-42
-------
rain and cloud, but the canopy storage cannot be obtained directly because the cloud water enhances
throughfall, without being collected as precipitation. In many cloud events, the throughfall amount
slightly exceeds what was measured as rain, providing an estimate of cloud water deposition, if estimates
of canopy storage for the appropriate canopy composition can be made.
Seasonal data from the summit of Whitetop Mountain (May 1987 - May 1988) have shown,
however, that differences between throughfall volumes and precipitation volumes are generally poor
indicators of the volume of cloud deposition due to substantial and unknown evaporation losses,
especially during the summer. At this site during the wanner months, monthly deposition volumes under
canopies are less than or about equal to those in the open. This pattern occurred despite the fact that
other information (computed cloud water flux and total sulfate deposition in throughfall) indicated that
cloud deposition occurred during the warmer months as well.
One reason for this summer pattern is the higher frequency of orographic clouds with low liquid
water contents and high ion concentrations. These events rarely result in much water reaching the forest
floor, while still accounting for a considerable deposition of ions to the canopy. In contrast, during
periods when evaporation is less important due to lower temperatures and solar radiation levels, the
accumulation of additional water from clouds can be observed. MCCP research is now in progress in
which the cloud, precipitation, and throughfall chemistries are monitored. If the dry deposition of SO^
and Cl are relatively small, their enrichments in the throughfall can be used to further refine the cloud
water deposition. The biologically and/or chemically more active species H+, NO/, and NH^+ cannot
be used for this purpose since considerable loss of these species is possible.
Within the last two decades, interest in throughfall has broadened from a hydrological focus to
include nutrient cycling, particularly fertilization and leaching (Parker, 1983). Data are now being taken
with sufficient time resolution to monitor the changing chemical environments on the canopy surfaces.
These results will aid simulation studies designed to provide a better understanding of the beneficial and
harmful effects from extended periods of canopy wetting.
Initial analysis of Whiteface data indicated that ion depositions have a larger variability than
does the deposition of water. The data collected apply only to the site from which they were taken and
to sites where the wind regimes and canopy composition and structure are similar. Event-based com-
parisons of throughfall and rain chemistry were made at the same two sites on Whiteface Mountain, NY.
The lower site was affected by rain only, and the upper site had additional cloud water deposition.
Throughfall from both sites included whatever dry deposition had occurred since the last wetting, residue
after evaporation of the last rain/cloud, and emissions from the tree itself and biology living on the tree
surfaces. Table 4-20 summarizes enrichment ratios integrated over the summer season in species
deposition, where the uncertainty was obtained using standard error propagation calculations. No
estimates of bias were possible.
4-43
-------
TABLE 4-20
Deposition Enrichment Ratios (Throughfall/Bulk Precipitation) at Whiteface Mountain, NY
Water (cm)
H+
NK/+
N0i
so/-
K+
cr
Under Canopy
Upper Site
8.51 ± 0.48
0.95 ± 20%
< 0.35
0.86 ± 23%
1.45 ± 19%
9.4 ±44%
2.51 + 27%
Open Rain
Lower Site
8.31 ± 0.08
0.71 ± 13%
1.11 ± 22%
1.65 ± 19%
1.16 ± 14%
> 13
> 2.0 + 25%
Of particular interest is the loss of the first three species at the upper (balsam fir) site, either on
the canopy or in the collected sample. Given that this site also had a substantial input of these species
from cloud water (current estimates suggest deposition on the same order as from rain), this suggests
that about half the H+ and the NO/ and at least 75% of the NH^+ that should have been deposited
were not present at the time of analysis. Samples were refrigerated immediately after the event and the
analysis was completed within a few days. Sulfate and chloride have reasonable enrichments given
contributions from dry and from cloud at the upper site. Foliar leaching is responsible for the ten-fold
increase in K+ deposition.
This section does not provide a comprehensive review of throughfall with an investigation of the
role of cloud water deposition; rather, it is a characterization of the gross features of the throughfall
compared with the precipitation obtained during the same time. For each weekly pair of samples, the
ratio of deposition in throughfall to open precipitation was calculated. The median values are presented
in Table 4-21.
TABLE 4-21
Median Value of Site Enrichment Ratios (Throughfall/Bulk Precipitation).
Site SO^2- NO/ NHf+ H+
Shenandoah, VA - upper 1.3
Shenandoah, VA - middle 1.3
Shenandoah, VA - lower 1.1
Moosilauke, NH 1.3
1.8
1.7
1.2
1.0
0.9
1.0
1.0
0.8
0.5
0.2
0.1
0.9
Not all sites have the same enrichment behavior because the relative input strengths differ, the
fraction of total deposition due to cloud water affects the ratios, and the canopy type helps create its
own chemical and biological environment. While dry deposition of various ionic species can be es-
timated and is in some cases relatively small, foliar exchange can be either a major source or sink. The
degree of interaction between the acidic deposition and the canopy is reflected primarily in the loss of
H+ and NH^+, and an increase in base cations in the throughfall samples.
Similar weekly integrated throughfall measurements made during 1987 and 1988 at two sites in
spruce-fir forests of the Black Mountains showed that while the yearly H+ average was 24% to 34% of
4-44
-------
the total ions in rain, it was only 16% to 23% in throughfall (Robarge, 1989). Similarly, NH4+ was 8%
to 10% in rain, but only 3% to 5% in throughfall. Similar trends for these ions have been reported in
other canopies (Bredemeier, 1988; Joslin et al., 1988; Waldman and Hoffmann, 1988; Olson et al., 1981;
Rodenkirchen, 1986) and in controlled experiments (Kaupenjohann et al., 1988; Kelly and Strickland,
1986; Evens 1982; Scherbatskoy and Klein, 1983). Recent data (May 1987 - May 1988) from Whitetop
Mountain give further evidence of the importance of the foliar exchange (see Table 4-22).
TABI£4-22
Actual (keq/ha/yr) and Percent Ion Contribution to Total Deposition at Whitetop, VA
Percentages for cations and anions are treated separately (Joslin et al., 1988).
H+ NH,+ Ca2+ Mg2^ Na+ K+ NO/ SO^ Or
Throughfall & 1.27 0.21 1.26 0.27 0.16 0.35 0.72 2.50 0.37
Stemflow 36% 6% 36% 8% 5% 10% 20% 70% 10%
Precipitation 0.50 0.14 0.07 0.02 0.03 0.01 0.20 0.52 0.04
66% 18% 9% 3% 4% 1% 26% 69% 5%
Cloud 63% 26% 5% 2% 3% 1% 32% 64% 4%
Precipitation and cloud water had similar proportional contributions to total deposition;
throughfall was different from both. Because of the large, unquantifiable amount of foliar exchange,
cation deposition in throughfall (with the possible exception of Na"1") was of little use in estimating
cloud water or dry deposition. Of the major anions, nitrate appeared slightly depleted (see also
Lindberg et al., 1987) and chloride was somewhat enriched (both foliar absorption and leaching of
chloride has been observed; Leonardi and Flueckiger, 1987). Sulfate appeared the least affected by foliar
exchange. In addition, the concentrations and total quantities of sulfur deposited and passing through
these forest canopies was large relative to the size of total foliar pool. The time period for which
throughfall sulfate is used to represent total sulfate deposition should be sufficiently long so that
differences in canopy residue sulfate are small relative to the amount passing through. The reproducibil-
ity and completeness of wash-off, the importance of dry deposition of aerosol sulfate and sulfur dioxide,
and the sequence of meteorological systems affecting the site affect the utility of this approach.
DEPOSITION
Cloud Water Droplet Deposition
Estimates of cloud water and chemical deposition to high-elevation forests are now reviewed.
Because cloud water is usually collected over hour-to-event time intervals during intensive sampling
campaigns, few full measurements exist for seasonal or annual cloud water deposition. Annual cloud
deposition estimates that have been published are usually extrapolated from short-duration, growing
season (generally April-October) cloud water chemical composition and model or throughfall-based cloud
water interception rates. Extrapolation of cloud water or chemical fluxes to annual values is highly
uncertain because winter chemical concentrations are generally not known (see section on winter data
from Whiteface Mountain, NY) and because cloud water interception rates in winter depend on
unknown rime ice collection efficiencies.
4-45
-------
Historical Perspective —
Table 4-23 summarizes past estimates of chemical and water'deposition due to the interception
of wind-driven cloud droplets. The MCCP has been evaluating the cloud deposition model (CDM) and
revising the technique used to estimate cloud deposition at its high elevation sites. These estimates are
presented later in this section. This historical perspective is presented to give background for the later
discussion of deposition at MCCP sites. Cloud water chemical deposition values presented in Table 4-
23 have been converted to a consistent set of units (kg/ha/mo) for ease of intercomparison among
estimates. Cloud water deposition is reported as an annual estimate (cmtyr, extrapolated from shorter
time periods) to facilitate comparison with annual precipitation totals. All deposition estimates
presented here are based either on canopy throughfall data or model-derived cloud water fluxes.
Lovett et al. (1982) reported estimates of sulfate and nitrate deposition from clouds on Mt.
Moosilauke, NH, using cloud water fluxes computed from a model (Lovett, 1984). He estimated that
cloud water deposition contributed about 70% of the total (cloud and precipitation) chemical fluxes for
SO^2' and NO/.
Mueller and Weatherford (1988) computed cloud deposition on Whitetop Mountain, VA, for a
26-day period in the spring of 1986. Using Lovett's model (Lovett, 1984), they computed cloud deposi-
tion for every hour during the study period, although some meteorological parameters and ion con-
centrations had to be estimated to fill in missing data. The cloud water SO^ flux was between 5.3 and
9.1 kg/ha/mo, while NOj flux was between 2.8 and 5.4 kg/ha/mo. The ranges reflect projected variation
in unmeasured model input data.
4-46
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TABLE 4-23
A Review of Chemical Ion and Cloud Water Deposition Via Droplet
Interception, Various Locations, Investigators, and Years.
Sitefl
MS.NH
MS.NH
MS.NH
MS.NH
UF1.NY
UF.NY
UF3.NY
WF3.NY
UF.NY
UF.NY
UT.VA
UT.VA
WT.VA
UT.VA
MM.NC
MM.NC
CL.NC
MM.NC
MM.NC
MM.NC
MM.NC
MM.NC
SH.VA
SH.VA
SH.VA
SM.NC
SM.NC
SM.NC
RT.QUE
HN.CA
GDF.GB
I,
Ref.°
Lovett7
Lovett
Lobett7
Mohnen2
Mohnen2
Mohnen2
Lindberg
Lindberg5
Mohnen2
Mohnen2
Mueller7
Mohnen2
2
Mohnen
Mohnen2
Saxena
Stogner
Dasch
Lin5
Lin5
Lin5
Mohnen
Mohnen2
Krovetz7
Sigmon
Mohnen2
Lindberg7
Lindberg
Lindberg5
Schemenauer
Ualdmen7
DoUarcr
Cloud Droplet Deposition Frequency H2° Flux site Coll.
H+ H»4+ MO/ SO/" H20 Cloud Method" Elev Per.'
[kg/ha/K>]
.20
.
.
.04
.18
.05
.04
-
.
.
.
.22
.20
.
.17
.12
(.03)
.09
.18
.11
.09
.13
.01
.02
.04
.14
.05
.
.11
.01
.01
1.
.
.
0.
2.
0.
0.
-
.
.
.
2.
11.
.
1.
0.
(0.
0.
1.
0.
0.
1.
0.
0.
0.
1.
0.
.
.
0.
-
4
24
3
8
5C
6
8
2
8
3)
6
3
7
1
1
13
21
26
0
5**
03
8.5
.
_
0.8
4.8
3.0
1C
1.2
.
_
4.3
7.7
10.4
_
3.2
3.2
(0.9)
1.9
4.0
2.8
2.6
2.2
0.5
0.8
1.3
2.2
1**
1.1
.
0.5
0.5
11.5
.
.
1.7
11.2
7.0
2
1.3
_
_
8.1
13.8
13.1
_
9.8
7.3
(2.2)
5.2
8.0
5.6
5.5
8.9
0.6
1.2
1.3
7.2
4
4
.
0.3
0.7
lcm/yr} Dflir] (•)
68
34-98
153
(18)
(127)
13
5-31
112
1
.
_
.
25-56
35-77
-
18
32
75
57
.
.
9
5
.
.
37
9-70
77
2
-
40
40
40
23
42
27
-
5-13
30
10
.
31
31
27-41
25-52
-
62
28
41
30
27
27
7
7
7
25
.
10-35
44
.
7
model
th.fall
model
model
model
th.fall
model
model
model
model
model
model
th.fall
model
model
model
th.fall
model
model
model
model
th.fall
model
th.fall
model
model
model
model
assumed
assumed
msmt.
1220
1220
1220
1000
1483
1200
1225
1225
1200
900
1686
1686
1686
1686
2020
2020
1987
2020
2020
2020
2020
2000
1014
1014
1014
1740
1740
1740
970
780
850
80-81
87
87
87
86-88
86-87
86
86
86
87
87
86
86
86
86
86
87
88
87
87
86-87
86-87
87
86
86-88
86-87
85
82-83
82
a MS = Moosilauke, NH; UF = Whit'eface Mtn, NY; WT = Whitetop, VA; MM = Mt. Mitchell, NC;
CL = Clingmans Dome, NC; SH = Shenandoah, VA; SM = Great Smoky Mtns. NC; RT = Roundtop, Quebec
, HN = Henmnger Flats, CA; GDF = Great Dunn Fell, Great Britain
1 = Peer-reviewed journal article or book chapter; 2 = Technical report subject to EPRI or US EPA
review; 3 = Unpublished data summary or submitted manuscript
C NO/ and NH^ were estimated from total N cloud deposition and the overall NH^/NOj ratios given by Lovett
, (in Lindberg & Johnson, 1989)
Annual cloud water flux was determined by: (1) a version of the Lovett model (1984); (2) collecting
throughfall under the canopy and correcting for precipitation and evaporation; or (3) direct
micrometeorological measurements.
e Collection period refers to the years when data were collected. Most data are from short-term, intensive
sampling performed during the growing season (April-October). None represent rime ice conditions.
note: Data in parentheses were calculated from information provided in the paper; Mohnen's Whiteface Mt.
estimates are based on data from sites at 1483 and 1245m.
4-47
-------
Lindberg et al. (1988) used Integrated Forest Study (IPS) data to estimate cloud, precipitation,
and dry deposition at a high-elevation site in the Great Smoky Mountains. Cloud water SO4 and NOj
deposition were estimated to be 7.2 and 2.2 kg/ha/mo, respectively, both two to five times greater than
estimates from a nearby low-elevation site for the period January-April 1986.
More recent deposition estimates from the IPS appear in discussions by Lovett, Knoerr and
Conklin, and Ragsdale in a draft summary of the IPS (edited by Lindberg and Johnson 1989). Cloud
water H+ deposition at these two sites was estimated to be 30% to 40% of total H+ deposition. The
IPS scientists concluded that the primary sources of uncertainty in cloud water deposition were
immersion time, cloud water amount, and ion concentrations. These IPS results were only presented as
a graphical summary with no presentation of methodology, chemical concentrations, or quantitative
uncertainties.
Following Lovett's work, Saxena and co-workers estimated cloud water and chemical deposition
on Mt. Gibbs (Mt. Mitchell State Park, NC), while assuming canopy structure and collection efficiency
for cloud droplets (Saxena et al., 1989a; Lin and Saxena, 1989; Stogner and Saxena, 1988; Saxena et al.,
1989b). Table 4-23 illustrates some of the cloud deposition estimates for Mt. Mitchell. There is a wide
range of cloud water deposition values from two research institutions (2 to 20 kg of SO4/ha/mo).
Although variation in cloudiness and pollutant concentrations are primary causes of differences between
years, the variety of results for one year suggests that the early Mt. Mitchell cloud deposition modeling
results are uncertain.
One of the Mt. Mitchell area estimates (Dasch, 1988) from nearby Clingmans Dome has been
compared with coincident data collected by Saxena et al. (1989b). The representativeness of the two
results remains unknown because of the lack of direct measurements of cloud water deposition. A
comparison of cloud frequency versus cloud water flux from all investigators indicates that Dasch's cloud
water deposition was anomalously low compared to cloud frequency in other published results (see Table
4-23).
Status of the Cloud Deposition Model -
The cloud deposition model (COM) used by the MCCP is an improved version of the model
originally developed by Lovett (1984). Modifications to Lovett's model are briefly described by Mohnen
(1988a). Work related to the CDM has concentrated on examining the following:
* the difference in model performance caused by using a site-specific vertical profile of forest
canopy surface area versus the model default profile based on data from Lovett's Mt. Moosilauke
forest (Lovett, 1984)
* the difference in model performance caused by using site-specific vertical profiles of wind
speed versus the default profile based on Lovett's site
* the difference in model performance caused by changing from the original Lovett droplet
collection efficiency scheme, based on individual tree components (twigs and branches), to an
experimental scheme designed to consider (crudely) the effect of tree morphology ("bulk
collector" versus individual branches and twigs); several experimental schemes were tried, each
used a slightly different technique for merging bulk collection efficiency (applicable to the most
dense portion of a tree crown) with Lovett's tree component collection efficiencies (Thorne et.
al., 1982)
4-48
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* the importance of using site-specific meteorological data (for model input) versus data from a
nearby site
* overall model performance relative to canopy throughfall measurements
Data have been collected from two spruce stands near the summit of Whitetop. These include
canopy-top wind speed and related profiles of speed, spatial variation in cloud liquid water, vertical
airspeed at canopy top, and canopy throughfall (TF) rates. One TF plot (A) was located about 75 m
northeast of the Whitetop summit, while the second (B) was located about 125 m east-northeast of A.
A larger TF database exists for plot B because of the construction and operation of an automated TF
volume measurement system. Plot A is considered a near-summit site (local slope less than 5%) and its
architecture is fairly open (leaf area index=4.8; maximum canopy height=15 m), whereas plot B is a
north-facing slope site (local slope almost 20%) that is closed with very little tree mortality (leaf area
index=11.0; maximum canopy height=17.5 m). The leaf area index values provided here represent the
ratio of the total (full-sided) leaf area to the associated ground area.
Preliminary findings of the CDM evaluation are now summarized:
* model performance was little affected by the surface area (SAI) profile used; this is consistent
with expectations from a previous analysis (Mueller 1990) of model sensitivity to this feature
(computed cloud water flux is not sensitive to modest uncertainty in the height of the SAI
profile maximum)
* model performance was greatly affected by wind speed profile changes-the default profile of
Lovett produced lower cloud deposition estimates than actual profiles- the difference was on
the order of a factor of 4 at plot B and a factor of 1.5 at plot A
* several modified (to test different methods for incorporating bulk collection efficiency into the
Lovett model framework) droplet collection efficiency schemes were tested-much data are still
needed to better understand the relationship between collection efficiency and tree morphology;
the scheme used to make subsequent cloud deposition estimates for this report (Mueller, 1990)
produced 60-70% lower deposition estimates than Lovett's (1984) original scheme
* site-specific meteorological data (measured canopy-top wind speed and spatially-adjusted liquid
water content) were found to result in much better model performance at plot B than data
collected at the mountain summit
* overall, the CDM performed better in simulating cloud flux to the closed stand (plot B) as
opposed to the open stand (plot A), but the difference was likely due to a greater uncertainty in
model input wind data for plot A. Using the most updated version of the model and "best"
inputs, flux was overestimated at plot A by 20-50%, depending on which version of the modified
collection efficiency scheme was used, with computed flux bias ranging from -20-30% for plot B.
Current Modelling Results -
The version of the CDM used for the spruce-fir sites in this analysis of cloud deposition was
configured with the modified version of the droplet collection efficiency scheme that produced the least
bias for the Whitetop evaluation. This modified scheme used measured bulk droplet collection efficiency
(Joslin et. al., 1990) in place of Lovett's individual tree component efficiencies for those portions of the
tree crowns having the highest leaf-to-total surface area ratios (ie. ratios > 0.85). This represents a
4-49
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major change from the 1988 analysis (Mohnen, 1988a). The uncertainty in deposition calculations
caused by using this particular parameterization is unknown. Default SAI profiles (similar to those
used in the 1988 analysis) were used for all sites except WT where site-specific profiles were known.
Another major change from the 1988 analysis was the use of a = 0.20 in place of a = 0.27 for the wind
speed extinction coefficient. The default (Lovett) value of a = 0.27 and the value that appeared to be
most representative of conditions at Whitetop a = 0.10 yield considerably different results. The best
value for each of the other MCCP sites was not known. A compromise was to use a = 0.20, due to a
lack of evidence favoring any specific value over another. Site-specific wind speed profiles were used in
all WT CDM runs.
The methodology followed for this analysis was very similar to that used in the 1988 MCCP
report (Mohnen, 1988a). Cloud impaction events at each MCCP site were classified according to the
synoptic meteorological conditions. A detailed analysis of cloud chemistry and meteorological variables
(wind speed and liquid water content) was conducted by Vong et al. (1989). In addition to synoptic
typing, Vong et al. found that specific air trajectory directions computed within a given event type can
further characterize event conditions. For example, ion concentrations measured during events classified
as Varm sector" (with respect to a cyclonic weather system) were sometimes different when segregated
according to whether associated backward air trajectories crossed the heavily industrialized Ohio River
Valley. This technique was able to explain half of the variance in the chemistry and meteorological
variables, and can be used to estimate non-monitored, multiple-hour means for the different synoptic
types. Deposition estimates for MCCP sites can now be made for periods when data are incomplete as
long as cloud frequency and event type can be determined.
In this analysis, cloud event synoptic type was determined for each hour of each growing season
at each site for the 1986-88 period. The results of the synoptic/trajectory (subclass) analysis performed
by Vong et al. (1989) were used to develop subclass means of aqueous ion concentrations for non-
precipitating clouds, wind speed and liquid water content. These parameters form the basis for
estimating cloud deposition to high elevation forests. This approach, by reducing the chemistry and
meteorological variance within each subclass, enables subclass means to be used in place of hourly data
for computing deposition flux in a manner that removes the bias associated with non-random, part-time
cloud sampling. The frequencies of the various synoptic meteorological classes for each site used in this
analysis are summarized in Table 4-24. Detailed definitions of these classes are found in the 1988
MCCP deposition report (Mohnen, 1988a). In summary, these classes are:
class 1: pre-warm front
class 2: NW sector of cyclone
class 3: post-cold front
class 4: warm sector of cyclone
class 5: stationary front
class 6: marine flow (off Atlantic)
classes 7&8: cutoff low in upper atmosphere
class 9: cap cloud
4-50
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Table 4-24
Frequency of Occurrence of Various Synoptic Meteorological Classes
by Site and Year for Growing Season
Site
MS
WF
MM
WT
Growing
Season
May 15 -
Oct 15
Jun 1 -
Sep30
May 1 -
Oct 15
May 1 -
Oct 15
Year
1986
1987
1988
1986
1987
1988
1986
1987
1988
1986
1987
1988
a
Percent Frequency by Class
1
26
27
31
16
27
9
0
0
0
0
0
0
2
3
18
7
3
10
1
3
3
1
1
5
2
3
15
8
9
33
26
36
15
13
18
12
20
16
4
36
26
51
32
20
39
43
43
39
57
41
40
5
0
0
0
0
0
1
3
3
1
1
2
2
6
11
19
2
6
5
0
35
21
27
28
21
21
7&8
9
2
1
8
0
7
0
5
3
0
4
13
9
0
0
0
2
12
6
1
11
11
2
6
6
b
Overall
Cloud
27
22
7
44
40
23
32
29
22
38
30
26
a. Frequencies include only those cloud hours that could be
classified. Frequencies may not sum to 100 due to roundoff.
b. Growing season cloud frequency (%).
Some of the synoptic meteorological classes contained only a few hours per site. Hence, a
complete event characterization was not possible for all classes/subclasses at all sites. The subclasses
that proved to be of most importance were those involving trajectories crossing or avoiding the Ohio
Valley within synoptic class 4, north versus other trajectories in synoptic class 3, and east versus other
trajectories in synoptic class 6. Examples of some of the more extreme differences found between
subclasses are provided in Table 4-25. All data in the table are for precipitation-free hours only (this
avoids the likely contamination of cloud water samples by precipitation).
4-51
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Table 4-25
Examples of Differences Between Synoptic/Trajectory Subclasses for Selected Sites
Site
MS
WF
MM
WT
Synoptic Subclass
Class
6 East traj.
Other traj.
3 N traj.
Other traj.
4 Ohio traj.
Other traj.
6 East traj.
Other traj.
Speed
(m/s)
3.9
3.6
11.3
10.5
11.0
9.0
5.9
5.7
Mean
LWC
(gfr*5)
0.18
0.16
0.42
0.46
0.16
0.24
0.24
0.23
a
Conditions
[H]
Oeq/L)
135
275
30
80
756
383
113
400
[S04]
Oeq/L)
101
66
27
116
947
317
130
586
a. Average of given parameter over all hourly measurements in
subclass. LWC=liquid water content; [H]=cloud hydrogen ion;
cloud sulfate ion.
Cloud deposition estimates for each site were made by computing, for each subclass, the mean
water deposition flux using the COM and subclass-mean wind speed and liquid water content. Best
estimates of canopy structure (Mohnen, 1988a) and growing season averages of other, less important
CDM inputs (i.e., temperature and pressure) were used to estimate the gross (pre-evaporation) cloud
water flux to specific forest canopies at each site. However, these deposition estimates are known to be
sensitive to canopy structure and the local influences of topography and forest inhomogeneity on
meteorology. Thus, the "potential" cloud deposition was also examined to determine site-to-site
deposition-related variability not dependent on model performance.
Potential deposition (K,) for ion X was defined as
Fp =uW[X]
where u is canopy top wind speed, W is liquid water content and [X] is the cloud water concentration
of X. The deposition of cloud water and, consequently, X, to a forest canopy is known to be highly
correlated with the product u W (Mueller and Imhoff, 1989). The mean potential deposition was
computed, when possible, for each subclass as
Fp = [{u W [X]ct }/(u W)] u W-* l^j , (1)
where [X]ct was the cube-root transformed cloud water concentration of X and the triple product of
uW[X]c, was averaged over all hours in a subclass. The subclass mean solute concentrations [X] used
to estimate Fp as in (1) are calculated as water content and wind speed weighted mean values, where the
solute concentration is in cube root-transformed units. The concentration is back-transformed to
4-52
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after the weighted mean is determined. Use of the cube-root transform, avoids errors associated with
skewed data distributions. Weighting [X] by W and u minimizes the influence of any inter-variable
correlations on the calculated triple products (uW[XJ) for each synoptic class. The factor f^y in (1) is
a unique adjustment applied to the computed Fp for each site to correct for placement of the wind
speed sensor (canopy top wind speed is most relevant to deposition flux), and the spatial differences, at
some sites, between the location where W and [X] were measured and the canopy of interest. The basis
for most of these adjustments were previously described in Mohnen (1988a). For Mt. Moosilauke, f^y
= 1 because no adjustments were needed. For Whiteface Mt., f^y = 0.33, the product of the
adjustment factor (0.33) for converting the summit u to canopy-top u, the adjustment factor (0.357) for
converting the summit W to canopy-top W, and the adjustment factor (2.8) for converting the summit
[X] to canopy-top [X] assuming that the elevational difference in [X] was due only to dilution (note that
the water content and [X] adjustments cancel out). For Mt. Mitchell, the f^* of 0.62 converted u from
that measured at 16.5 m above ground to that at canopy-top (about 9 m). For Whitetop Mt. f^/y was
computed to vary with wind direction (a direction frequency-weighted adjustment was computed for each
subclass - values ranged from 1.14 to 3.41), and the u measured at 7.4 m at the summit was converted
to a u value for the nearby canopy top (about 15m).
The results of the F., analysis are summarized in Table 4-26. Synoptic classes 2, 7 and 8 are
rare and, therefore appear together under "other classes" in the table.
Table 4-26
Mean Potential Deposition by Subclass0 and Site
(a) Sulfate ion
Class/Subclass* Mean Potential Deposition
MS MM WF WT
I/none 0.40 - 0.48
3/Ntraj. - 0.39 - 0.20
3/non-N traj. - 0.97 0.17 0.10
4/OH traj. 0.23 0.44 0.67 1.69
4/non-OH traj. - 0.54 0.28 0.39
6/Etraj. 0.05 0.33 - 0.29
6/non-E traj. - - - 1.63
9/none - - - 0.55
other classes - 1.20 0.002 0.78
4-53
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Table 4-26 (continued)
Mean Potential Deposition by Subclass0 and Site
(b) Nitrate ion
Class/Subclass* Mean Potential Deposition
MS MM WF WT
I/none
3/N traj.
3/non-N traj.
4/OH traj.
4/non-OH traj.
6/E traj.
6/non-E traj.
9/none
other classes
0.23
-
-
0.14
-
0.02
-
-
-
_
0.12
0.31
0.20
0.18
0.16
-
-
0.51
0.14
-
0.05
0.24
0.19
-
-
-
0.002
_
0.03
0.10
0.50
0.11
0.20
0.69
0.23
0.33
a. Results shown only for those subclasses having a minimum of 10 hr of
observations. At Whitetop (WT), Fp is for plot A (summit).
b. "None" indicates no trajectory subclass considered.
In simple terms, R, is the canopy-top horizontal cloud flux of ion X. Thus, high values of R, are
associated with windy conditions, dense clouds, and/or high cloud water ion content. Mean values of Fp
vary greatly from one subclass to another and from one site to another. If all other conditions
affecting cloud deposition were identical at all the sites (this means, among other things, that site-to-site
variations in cloud droplet size distribution and canopy structure would be insignificant), then the mean
hourly cloud deposition flux would vary according to R, alone. Values of Fp>l /*eq m~2 s'1 were found
for only two sites. Class-weighted mean values of R, for each site (Table 4-27) show that the greatest
overall cloud deposition potential (using the subclasses shown in Table 4-26 and weighting subclass-
mean Fp values by the relative frequencies of observed wind speed for each subclass) for sulfate and
nitrate is at Whitetop. This conclusion is valid only for those specific forest canopies considered here.
For any given mountain, different forest canopies exposed to different meteorological conditions could
have considerably lower or higher deposition potentials.
4-54
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Table 4-27
Class-weighted Deposition Potential by Site for 1986-88
Site0 Class-weighted Deposition Potential (jceq/m2s)
Sulfate Nitrate
MS
WF
MM
WT
0.27
0.35
0.54
0.64
0.16
0.12
0.19
0.24
a. The stand on MS is on a ridge, but not at the highest point on the
mountain. The stand on MM is near the mountain summit. The stand on
WF is several hundred meters below the summit (no trees are on the WF
summit). The WT stand is near the summit.
Another measure of deposition potential-the growing season potential exposure (Pe)--takes into
account the frequency of cloud impaction. As defined here, Pe represents the total cloud ion mass
passing horizontally at canopy top through a unit area during a growing season. Thus, Pe=t
where t is the growing season cloud exposure time and is the weighted mean value of Fp listed
in Table 4-27. Combining the data in Tables 4-24 and 4-27, one finds that the potential growing season
exposure to sulfate and nitrate cloud deposition was also a maximum at the Whitetop site for every
year of the analysis. If the average cloud collection efficiency was known for a given stand (this is what
the COM is designed to compute) and the total collecting surface area of the stand per unit of ground
area (SAI) was known, then the values in Table 4-28 could be used to estimate the growing season
cloud deposition total.
4-55
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Table 4-28
Growing Season Cloud Deposition Potential Exposure' (Pe) by Site and Year
Site Year Growing Season Potential Exposure to Cloud Deposition0
Sulfate (eq/m2) Nitrate (eq/m2)
MS
WF
MM
WT
1986
1987
1988
1986-88
1986
1987
1988
1986-88
1986
1987
1988
1986-88
1986
1987
1988
1986-88
1.0
0.8
0.3
0.7
1.6
1.5
0.9
1.3
2.5
2.3
1.7
2.2
3.5
2.8
2.4
2.9
0.6
0.5
0.2
0.4
0.6
0.5
0.3
0.5
0.9
0.8
0.6
0.8
1.3
1.0
0.9
1.1
a The Pe units used here are not to be interpreted as depositable [H]™ equivalents per unit of
ground area, but equal instead to the growing season horizontal flux ofjH]^ equivalents
through a vertical plane at canopy top.
Hourly cloud water, sulfate and nitrate deposition estimates computed for each site using the
CDM and class-mean meteorological and chemical variables are listed in Table 4-30 by class/subclass.
Deposition was computed for both CDM evaluation stands on Whitetop (plots A and B mentioned
earlier in this section) to illustrate the expected differences in deposition at two sites in relatively close
proximity on the same mountain. WT Plot A was the open stand of low density and plot B was closed
and dense.
4-56
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Table 4-29
1986-88 Computed Mean Hourly Cloud Deposition by Site0 and Subclass
(a) Cloud water
Class/subclass Mean Computed Flux (mm/hr)
MS MM WF WT(A) WT(B)
I/none
3/N traj.
3/other traj.
4/OH traj.
4/non-OH traj.
6/E traj.
6/non-E traj.
9/none
other classes
0.11
0.15
0.11
0.36
0.31.
0.21
0.25
0.26
0.09
0.15
0.11
0.10
0.09
0.09
0.06
0.04
0.29
0.19
0.49
0.22
0.46
0.60
0.27
0.29
0.68
0.21
1.29
0.18
0.26
1.25
0.55
0.63
Class/subclass
ClassAsubclass
(b) Sulfate ion
Mean Computed Flux (eq/ha/hr)
MS MM WF WT(A) WT(B)
I/none
3/N traj.
3/other traj.
4/OH traj.
4/non-OH traj.
6/E traj.
6/non-E traj.
9/none
other classes
0.43
1.15
1.81
0.54 1.96
0.79
0.11 0.50
-
0.90
1.07
0.13
-
0.12
0.30
0.26
-
-
0.32
0.01
„
0.59
0.30
2.40
0.56
0.60
3.53
2.83
0.87
.
1.30
0.33
4.94
0.48
0.39
6.79
5.41
1.65
(c) Nitrate ion
Mean Computed Flux (eq/ha/hr)
MS MM WF WT(A) WT(B)
I/none
3/N traj.
3/other traj.
4/OH traj.
4/non-OH traj.
6/E traj.
6/non-E traj.
9/none
other classes
0.24 - 0.06
0.38 - 0.22 0.49
0.59 0.03 0.16 0.18
0.32 0.94 0.04 0.71 1.46
0.28 0.10 0.22 0.19
0.05 0.21 - 0.29 0.19
1.67 3.22
0.39 0.17 . 0.96 1.83
0.41 0.003 0.43 0.81
a. Values shown only if hours of data exist for a subclass
4-57
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The large variations between subclasses in computed water and ion flux was expected because of
the large variations in meteorology and chemistry. Uncertainty in these flux estimates is unknown, but is
expected to be larger for MS, MM and WF because of the greater uncertainty in the inputs to the
model for these sites, It is also expected to be larger for those subclasses for which relatively few hours
of data were collected (a mininum of 10 hours was used as a selection criterion). The WT flux
estimates may be 20% - 30% higher for both plots, based on results of the CDM testing at these sites.
However, some assumptions were necessary (e.g., previously analyzed relationships between summit
wind speed at 7 m and canopy top wind speeds at both plots was assumed to hold for the entire 3-year
period) to run the CDM for both plots A and B because site-specific wind speed and liquid water
content data, representative of canopy top, were not always part of the subclass analysis done by Vong
et al. (1989).
One interesting feature of note is the difference in computed cloud deposition between WT plots
A and B. Deposition is sometimes greater at one and sometimes greater at the other, depending on
subclass. This occurs because of the variation in prevailing wind direction among subclass type.
Subclasses with a prevailing direction from southeast through west produce lower water deposition
because of the sheltering effect of the mountain-plot B is in the lee of the mountain under these
conditions, near the location of the lee eddy that has been observed frequently in videotaped images of
the mountain. However, wind speeds are very similar for other directions, and the greater surface area
at plot B causes deposition estimates to be much higher during these conditions.
Yearly growing season estimates of cloud deposition were computed using the synoptic class
frequency data and the mean hourly flux estimates shown in Table 4-29. For each site, the
subclass-mean flux estimates include subclasses that account for more than 75% of the total cloud
impaction hours. The mean hourly flux during the unrepresented periods was assumed to equal the
computed mean averaged over the represented periods. This was not expected to introduce much bias
into the estimated deposition fluxes. However, int the future, other estimation techniques should also be
tested. Table 4-30 summarizes the computed growing season deposition totals for each site.
4-58
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Table 4-30
Computed Growing Season Total Cloud Deposition Flux by Site
Site Year
Cloud Water
Flux (on) [H]
Cation Deposition (eq/ha)/(kg/ha)
[NH4] [K + Mg + Ca + Na]
MS 1986
1987
1988
86-88
WF 1986
1987
1988
86-88
MM 1986
1987
1988
86-88
WT(A) 1986
1987
1988
86-88
WT(B) 1986
1987
1988
86-88
12.9
10.1
3.5
8.8
11.6
10.5
6.0
9.4
33.5
27.5
21.8
27.6
53.1
39.4
34.3
42.3
77.3
61.2
54.3
64.3
486/0.5
349/0.3
141/0.1
325/0.3
144/0.1
156/0.2
81/0.1
127/0.1
1205/1.2
1114/1.1
855/0.9
1058/1.2
1514/1.5
1189/1.2
1047/1.0
1250/1.2
2454/2.5
1983/2.0
1764/1.8
2067/2.1
189/ 3.4
135/ 2.4
55/ 1.0
126/ 2.3
107/ 1.9
96/1.7
64/1.2
89/ 1.6
377/ 6.9
377/ 6.9
278/ 5.0
344/ 6.3
780/14.0
602/10.8
525/ 9.5
636/11.4
1229/22.1
985/17.7
866/15.6
1027/18.5
23/-
17/-
11-
161-
161-
111-
10/-
14/-
100/-
113/-
83/-
99/-
149/-
110/-
93/-
117/-
221/-
170/-
144/-
178/-
4-59
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Table 4-30 (continued)
Site Year Afflon Deposition (eq/ha)/(kg/ha)
[SO4] [NO3] [a]
MS
1986
1987
1988
86-88
435/21
313/15
127/6
292/14
250/16
178/11
73/5
167/11
18/0.6
13/0.5
5/0.2
12/0.4
WF 1986 220/11 54/3 6/0.2
1987 202/10 67/4 5/0.2
1988 128/6 31/2 3/0.1
86-88 183/9 51/3 6/0.5
MM 1986 1091/52 406/25 68/2.4
1987 1052/51 396/25 64/2.3
1988 791/76 296/18 48/1.7
86-88 978/60 366/23 60/2.1
WT(A) 1986 1737/83 667/41 87/3.1
1987 1337/64 522/32 62/2.2
1988 1173/56 463/29 54/1.9
86-88 1416/68 551/34 68/2.4
WT(B) 1986 2817/135 1053/65 105/3.7
1987 2244/108 858/53 82/2.9
1988 1981/95 769/48 74/2.6
86-88 2347/113 893/55 87/3.1
First note that uncertainties in canopy structure, and hence wind speed profile and droplet
collection efficiency could easily make these values biased by a factor of two for all sites but WT. These
values indicate changes relative to previous MCCP estimates of cloud deposition. For example,
compared to the 1988 estimates for the 1987 growing season, the current 1987 sulfate deposition totals
are higher for MS (+81%), lower for WF (-78%), higher for MM (+70%) and lower for WT(A)
(-16%). To some extent these differences reflect changes in the COM, but are mostly due to the more
detailed characterization of the forest canopy which became available to MCCP through the efforts of
the USDA Forest Service. In addition, improvements in characterizing the meteorology and chemistry
associated with the various cloud event synoptic classes also necessitated a recalculation of the 1987
interception values. At WF the differences are also due to different assumptions concerning the wind
speed profile, canopy structure and spatial variability of cloud water ion concentrations.
Another interesting finding is the large deposition flux estimated for WT(B) compared to
WT(A). This is in spite of the fact that plot B at WT is occasionally sheltered in the lee of the
mountain and intercepts less cloud water during such periods. The primary reason that WT(B) estimates
are larger than those for WT(A) is the much greater canopy density of the former. COM performance
for WT(B) has been tested (Mueller et al., 1990) and found to be good (within 20% of throughfall
rates). At WT, unlike the other sites, different wind directions were considered when computing
deposition for the synoptic classes. This was done to maximimze the accuracy of the wind speed
4-60
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adjustments needed to convert from 7 m speed at the summit to canopy top speed. There is a
possibility that the partitioning of wind directions for the synoptic classes (which was done using only
1988 data) was not representative of all years of the analysis. The data indicate that west-northwest is
the most prevalent wind direction for most synoptic classes, with south- southeast often being the
second most prevalent. Overall, W and WNW winds-which do not place the WT(B) site in the
mountain lee-appear to be twice as frequent as SE and SSE winds. Thus, on a long-term basis, the
sheltering effect may not be as important as previously believed in its influence on deposition at this
site.
The greatest computed growing season cloud deposition fluxes were found for WT and MM
which also had the longest growing seasons. The differences between MS and WF may be greater than
they appear here because of the uncertainty in model input data for these two sites. The mean
monthly computed cloud deposition flux is provided in Table 4-31 to facilitate comparison of deposition
rates independent of growing season length. Despite an almost 2:1 advantage in cloud frequency, WF
mean monthly deposition estimates were generally lower than those for MS. The primary reason for
the difference is the lower canopy surface area at the modeled WF site. Differences between the
northern (MS and WF) and southern (MM and WT) sites are so great that they are likely to be real
despite uncertainties in the model, and they exist independent of the longer growing season in the south.
Table 4-31
Mean Monthly Computed Cloud Deposition Flux
Site Year Computed Water Computed Ion Flux (kg/ha/month)
Flux (mm/month) [H] [NH4] [SO4] [NO3] [Cl]
MS
1986
1987
1988
86-88
25
20
7
17
0.10
0.07
0.03
0.06
0.67
0.47
0.19
0.44
4.1
2.9
1.2
2.7
3.0
2.2
0.9
2.0
0.12
0.09
0.04
0.08
WF 1986 29 0.04 0.48 2.6 0.8 0.05
1987 26 0.04 0.42 2.4 1.0 0.05
1988 15 0.02 0.28 1.5 0.5 0.03
86-88 23 0.03 0.39 2.2 0.8 0.04
MM 1986 60 0.22 1.21 9.4 4.5 0.43
1987 49 0.20 1.21 9.0 4.4 0.40
1988 39 0.15 0.89 6.9 3.3 0.30
86-88 49 0.19 1.11 8.4 4.0 0.38
WT(A) 1986 95 0.27 2.51 14.9 7.4 0.55
1987 70 0.21 1.94 11.5 5.8 0.39
1988 61 0.19 1.69 10.0 5.1 0.35
86-88 75 0.22 2.04 12.1 6.1 0.43
WT(B) 1986 138 0.44 3.95 24.1 11.7 0.67
1987 109 0.35 3.17 19.2 9.5 0.52
1988 97 0.32 2.78 17.0 8.5 0.47
86-88 115 0.37 3.30 20.1 9.9 0.55
4-61
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The cloud deposition information contained in this report has been produced using
state-of-the-science computational methods. The state of the science is such that considerable
uncertainty remains in the deposition estimates despite recent advances in our knowledge concerning
cloud deposition to forest canopies. However, the deposition potential-as defined previously--and the
computed deposition fluxes both indicate trends toward higher cloud deposition at the southern sites.
Differences between northern and southern sites are due to site specific parameters and not latitude.
The southern sites have a significantly different canopy structure than the Whiteface Mtn. site. The
southern sites are also exposed to a different mix of cloud event types (as defined by synoptic
meteorology and computed air trajectories) when compared to the northern sites, and different event
types have been shown to be characterized by differences in conditions affecting cloud deposition. More
work needs to be done to better define conditions at each site before more accurate deposition estimates
can be obtained.
Dry Deposition
Model Data Requirements --
The Atmospheric Turbulence Diffusion Laboratory (ATDL) model used by the MCCP,
DRYDEP, calculates the dry deposition velocities of sulfur dioxide, ozone, nitric acid vapor, sulfate, and
nitrate from meteorological and site-specific biological information. Site information includes: major and
minor plant species type, leaf area index for plant species, and site location. Stomatal resistance
parameters include plant species, light response coefficients, minimum stomatal resistance, and optimum,
maximum, and minimum temperatures for stomatal function. All available meteorological data such as
wind speed, standard deviation of direction, global radiation, air temperature, relative humidity, canopy
wetness, and rainfall are also used.
Model Application --
The current big-leaf model does not directly account for nonuniform terrain. Only Rowland met
the model requirements. Therefore, to estimate dry deposition at the other sites, the model was run
with the aerodynamic resistance set to zero in an attempt to estimate the maximum effect of an uneven
surface. Table 4-32 shows the warm period and the species for which deposition flux density was
inferred at each site.
TABLE 4-32
Chemical Species for Which Deposition was Inferred
Site Period Species
Rowland, ME 4/7 - 10/12 O3 SO2 HNO3 SO4 NO/
Whiteface, NY 6/1 - 10/6 O3 SO2 SO^
Moosilauke, NH 5/15 - 10/21 O3
Shenandoah, VA 4/1 - 11/16 O3 SO2 HNO3 SO4 NOj
Mitchell, NC 5/1 - 10/21 O3 SO2 NO,.
Whitetop, VA 4/26 - 10/18 O3 SO2
4-62
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Model Sensitivity Testing --
The effect of estimating deposition velocities when setting aerodynamic resistance to zero varies
by chemical species. For example, the effect for ozone, which has considerable canopy resistance, would
be less than the effect for HNOj, for which canopy resistance is assumed to be zero. Ozone deposition
velocities for 1987 Rowland data showed a 14% increase when calculated with zero resistance. HNOj
deposition velocities calculated with and without aerodynamic resistance for Shenandoah showed an
offset of 0.36 cm/sec, and an increase of 59% when calculated with zero resistance.
. Some uncertainty was included in leaf area index (LAI) values used for most sites; only the
values for Mitchell were obtained by direct measurement. Therefore, the sensitivity of deposition velocity
to changes in LAI was evaluated using ozone at Rowland. The primary and secondary tree species have
LAIs of 5.5 and 0.2, respectively. Deposition velocity (Vd) was calculated with primary LAI values from
2.5 to 11.0, with the secondary LAI held constant. For each of seven values of LAI, the resulting Vd
values were averaged for the period of record. Paired values of normalized LAI and Vd were deter-
mined using the accepted values as the base. The results showed that if estimated LAI values were in
error by as much as 25%, Vd would either be overestimated by 12% or underestimated by 15%. This is
probably within the uncertainty of the model estimates. The current model also tended to overestimate
deposition velocities for chemical species for which canopy resistance is important, such as ozone and
SO2, (Matt and Womack, 1988; Matt et al., 1987).
Model Results ~
The warm season total deposition flux density (kg/ha/mo) is a function of deposition velocity,
concentration, and season length. Table 4-33 displays the available dry deposition values for 1987 and
1988. The values were derived by multiplying weekly deposition velocities derived from the model by the
appropriate weekly concentrations for the warm period at each site. Estimates based on the mean were
substituted for missing data. Estimates for 3 to 6 missing weeks yielded reasonable results. However, as
in the case of SC>2 and SO^ for Shenandoah-1, substituting estimates for more than 50% of the warm
period led to anomalous results.
During 1987 ozone values for Whiteface seem low due to moderate deposition velocities and the
short season. For that year, Moosilauke and Whiteface, if scaled to the Rowland warm season, would
have ozone deposition values of approximately 6.81 and 9.75 kg/ha/mo, respectively. On the other hand,
if Shenandoah was similarly scaled down, ozone deposition would still be the largest with 9.29 kg/ha/mo.
Although ozone exposure was considerably greater in 1988 than in 1987, deposition flux density
was approximately the same for both years for three northern sites due to a marked decrease in
deposition velocities during 1988. Deposition velocities also decreased somewhat at the southern sites,
but this was offset by very much higher average ozone concentrations.
Sulfur dioxide concentrations were also higher during 1988 at all reporting sites. However, SO2
deposition velocities were uniformly lower, producing only modest increases in deposition flux density at
Rowland and Whiteface. Only Mt. Mitchell recorded a substantially higher SO2 flux density during
1988.
In general, for chemical species with sufficient available data, northern sites received less dry
deposition than southern sites. However, within each region there was marked variability in seasonal
ozone and SO2 deposition. Also, seasonal deposition totals did not adequately reflect weekly site-specific
variability.
4-63
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TABLE 4-33
MCCP Wann Season Diy Deposition
Site Elev.(m) Diy deposition flux density
(kg/ha/mo)
O3 SO2 SQ4 HN05 NOj NO2
Rowland, ME (1987) 65 5.48 0.22 0.11 0.29 0.002
(1988) 5.39 0.28 0.15 0.37 0.03
Moosilauke, NH (1987) 1000 5.%
(1988) 6.57 0.31 1.61 0.01
Whiteface, NY (1987) 1483 6.46 0.30 0.36
(1988) 6.09 0.51 0.28
Shenandoahl, VA (1987) 1015 14.06 3.06 0.80 0.007
(1988) 14.83
Shenandoah3, VA (1987) 524 13.36 1.32 0.19 1.03 0.005
(1988) 15.11
Mt. Mitchelll, NC (1987) 1950 7.70 0.39 0.20
(1988) 12.7 1.48 1.64 0.21
Mt. Mitchell2, NC (1987) 1775 7.81
(1988) 10.56
Whitetop Mt, VA (1988) 1689 11.95 0.75
Precipitation Deposition
In this section, wet deposition for the 1987 and 1988 warm seasons at the MCCP sites is
estimated using standard NADP/NTN or MAP3S measurements of precipitation amount and chemistry.
These estimates were obtained from NADP and MAP3S reports for the network stations closest to the
MCCP sites or, in one case, for an NADP-type collector operated at the Shenandoah MCCP site.
To represent wet deposition via precipitation at the Rowland, ME, site, Mohnen (1988a) used
data from the NADP/NTN site at Greenville, ME, located approximately 100 km west of Rowland.
Other MCCP sites had NADP/NTN type samplers no more than 25 km distant. Details for these
stations are shown in Table 4-34.
.For comparison with MCCP cloud water deposition, wet deposition only for the warm season
are reported as monthly deposition. The growing season is longest at the Shenandoah and Rowland
sites, extending from early April at both locations to mid-November and early October, respectively. Mt.
Mitchell and Whitetop Mountain have the next longest growing seasons, followed by Mt. Moosilauke and
Whiteface with the shortest (June to early October). For consistency the concurrent growing season
4-64
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(June to October) was used for 1987 data and all available data (until August 23) were used for the
same period during 1988.
TABLE 4-34
Sites Used to Estimate Wet Deposition via Precipitation for MCCP Sites.
MCCP Site Wet Deposition Site LaL Long. Elevation
Howland Forest, MA NTN Greenville ME09 45°9' 69°9' 322 m
Whiteface Mtn, NY NTN Whiteface NY98 44°3' 73°!' 622 m
MAP3S Whiteface (co-located)
Moosilauke, NH NTN Hubbard Brook NO2 43°6' 71°2' 250 m
Shenandoah, VA NTN Big Meadows VA28 38°!' 78°6' 1074 m
Whitetop, VA NTN Whitetop VA29 36°8' 81°6' 1689 m
Mt Mitchell, NC NTN Clingmans Peak NC45 35°44' 82° 17' 1987 m
MCCP pollutant deposition and climatological data tend to form two distinctly different groups.
Because of physical proximity, and similar influences from synoptic systems, the Howland, MA, Whiteface
Mountain, NY, and Mt. Moosilauke, NH, sites are considered together as northern sites and the
Shenandoah, VA, Whitetop, VA, and Mt. Mitchell, NC, sites are grouped together as southern sites.
The wet deposition data for the two groups of sites are shown in Table 4-35 [kg/ha/mo] for
SCXf2", NOy, NH/+, and H+ ions in precipitation (not cloud) collected at the NADP/NTN sites. At
Whiteface Mountain, NY, both NADP/NTN and MAP3S collected precipitation, but during 1987 the
NADP/NTN site was hit by lightning, so only the MAP3S data were used. Rain gauge data were used to
calculate precipitation amount. About 98% of the precipitation was analyzed for chemical composition
during 1987. Missing samples were replaced by actual precipitation amount for that week and the
volume-weighted mean concentrations of growing season data for that site and year. A further discus-
sion of the calculation procedures is presented by Mohnen (1988a).
The data indicate that the most westerly sites in the north, Whiteface, NY, and Moosilauke, NH,
received greater wet deposition via precipitation than did the more northeasterly location in Maine. Big
Meadows, VA, and nearby Shenandoah had the most NH/+ deposition from rain.
These data suggest that the highest elevation site, Mt. Mitchell, NC, had the largest wet flux for
SO/2" and NO/. Hubbard Brook, NH, (a low elevation site in the north), Shenandoah, VA (a medium-
-elevation site in the south), and Whitetop Mountain, VA, (the second highest site) had similar wet
deposition for 1987. The lowest site, Greenville, ME has the least wet deposition via precipitation.
For comparison, available data for the 1988 growing season are presented in Table IV-18 for
several MCCP sites. Data for all of the same sites as for 1987 are not currently available.
The 1988 precipitation chemistry data indicate that the southern sites exceeded the northern
sites in SO/2' and NOf deposition, with the differences being greater for SO/=. Shenandoah had the
most NH/"1" deposition. These values for wet deposition via precipitation are about 20% to 50% of the
deposition via cloud water interception during 1987.
4-65
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TABLE 4-35
Concurrent Warm Season Wet Deposition via Precipitation in the Eastern USA
from NADP/NTN or MAP3S Sites Near MCCP Monitoring Locations
(for the period 26 May to 6 October, 1987, or 31 May to 23 August, 1988.)
[kg-ion/ha/mo].
Data are (invalidated and subject to change.
Location H+ NH,+ SO^~ NO/ Year
Greenville, ME * 0.11 1.28 0.65 1987
Whiteface, NY * 0.33 2.27 ,0.95 1987
.032 1.11 1.18 0.93 1988
Hubbard Brook, NH * 0.28 2.84 1.46 1987
.041 0.11 2.16 1.10 1988
Whitetop, VA * 0.31 3.20 1.32 1987
.053 0.14 2.84 1.17 1988
Mt. Mitchell, NC * 0.46 5.15 2.26 1987
.051 0.12 2.69 1.19 1988
Big Meadows, VA * 0.48 2.32 1.43 1987
.016 0.92 2.90 1.34 1988
Shenandoah, VA * 0.35 3.11 1.25 1987
.045 1.76 2.80 1.19 1988
Not reported
Wet. Cloud and Dry Deposition
Cloudwater deposition is the factor which differentiates mountains from lowlands and the
relative importance of cloud and rain deposition is discussed here. It is hypothesised that the principal
deleterious effects on forests which might be associated with such deposition are direct effects of acids
on foliage, mobilization of aluminum because of ions deposited to soils, or excess nitrogen fertilization
influence on winter damage. Since most of these effects are more significant for warm season deposi-
tion, the analysis intervals were selected for each site to correspond roughly with the periods between
local forest bud break and fall dormancy. These periods differed to some extent for the MCCP sites.
However, cloudwater deposition calculated for Whitetop Mountain seems to stand out above the
rest. Since this peak is substantially lower than Mount Mitchell which is only about 90 miles southwest
of Whitetop, the difference is difficult to explain.
4-66
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It is apparent from Tables 4-31, 4-33 and 4-35 that cloud deposition based on current models
estimate, is comparable to deposition of rain at all summit locations. Dry deposition of sulfur-bearing
compounds is reported as sulfur rather than as SC«2 or sulfate anion (Table 4-33).
If the geographic gradients suggested by the data in Table 4-33 continue in future estimates, then
some interesting conclusions could be drawn. First, the Shenandoah site seems to experience the
greatest dry deposition. In the case of both sulfur and nitrogen budgets, dry deposition is significant in
the three Northern sites. This gradient reflects the wet deposition gradient reported in both the
National Academy of Sciences findings on acid rain and in the 1989 NAPAP interim assessment. The
more easterly sites, Moosilauke and Howland are very much lower in pollutant burden than are the
Whiteface and southern sites. With the exception of Moosilauke and Howland, the MCCP site warm
season sulfur deposition is 20-40 kg/ha-year. This level is about that reported for annual deposition at
the more contaminated low elevation sites in rain.
It is not yet clear whether cold season sulfur deposition should really be factored in to the
mountain estimates. There is some evidence of SC>2 loss from snowpack and the excess ions in snow-
pack melt are of much greater consequence in the acidification of lakes than they might be in determin-
ing ion concentrations in frozen soils. In any case, it is clear that mountaintop sulfur deposition is quite
significant, approximating or exceeding that of near-source low elevation sites.
For all of the data reported so far, dry deposition sulfate ion in fine particles is very small
relative to wet deposition and in many cases relative to that of SC>2 dry deposition as well. Dry
deposition of nitrogen is more uncertain because of the lack of dependable data for nitric acid.
However, ammonium ion dry deposition accounts for a substantial amount of the total nitrogen
deposited; this material appears to be mainly in the form of ammonium sulfate. The season-long values
for Shenandoah for nitric acid try deposition may be biased somewhat low of the actual values, because
most of the determinations were performed relatively late in the study period. In any case, the nitric
acid dry deposition appears to be quite significant for that site, and probably for the other southern sites
as well.
Overall growing season fertilization rates are 10-20 kg N/ha-season for the southern sites and
lower for the northern ones. This application of nitrogen is driven mainly by wet deposition and the
estimates could go up or down as model predictions are improved.
Table 4-36 summarizes the average monthly sulfur and acidic nitrogen (excludes ammonium ion)
deposition fluxes determined to-date for the MCCP sites for the 1987-88 growing seasons. At the cloud-
free Howland site, dry deposition appears to account for less than one-third of the total acidic sulfate
and nitrate ion deposited. The Shenandoah site has a very low cloud impaction frequency due to its low
elevation, and dry deposition is probably of greater relative importance there (it could exceed 50% of the
total deposition flux) than at any of the other high elevation sites. Estimates for Whiteface suggest that
dry sulfur deposition accounts for less than 30% of the total sulfur deposition flux.
The greatest amount of information is available for comparing estimated cloud and wet
deposition at the four high-elevation spruce-fir sites (Moosilauke, Whiteface, Whitetop and Mitchell).
Cloud-to-wet deposition ratios (Table 4-37) vary from near unity at Moosilauke and Whiteface to near 4
at Whitetop. In terms of acid deposition, clouds seem to be of greater relative importance at the two
southern sites (WT and MM) than at the two northern sites.
4-67
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Site
Year
TABLE 4-36
(a)
Estimated 1987-88 Sulfur Deposition Budgets at MCCP Sites'1
Growing Season Mean S Deposition (kg S/ha-mo)b
Wet (Measured) Qoud (Computed) Dry (Computed)0
Howland, MEd 87
88
87-88
0.43
0.15
0.19
0.17
Moosilauke, NH* 87
88
87-88
Whiteface, NY 87
88
87-88
Shenandoah, VA 87
88
87-88
Whitetop, VAf 87
88
87-88
Mitchell, NC 87
88
87-88
a. Not all data were
b. Average fluxes for
0.95
0.72
0.84
0.76
0.39
0.58
1.04
0.93
0.99
1.07
0.95
1.01
1.72
0.90
1.31
available in time for inclusion in
combined 1987-88 period were c
0.97
0.40
0.69
0.80 0.27
0.50 0.35
0.65 0.31
1.80
3.83
3.33
3.58
3.00
2.30
2.65
this report.
omputed by averaging values given separately
for the two years.
c. Sulfuf (S) flux computed as the sum of individual computed SO2 gas and SOj aerosol fluxes
(approximate maximum rates due to assumption that aerodynamic resistance within forest canopy
was zero).
d. Greenville, ME NADP data used for wet deposition fluxes.
e. Hubbard Brook, NH NADP data used for wet deposition fluxes.
f. Near-summit (plot A) site.
g. Nitrogen in ammonium ion not considered.
h. Nitrogen (N) flux computed as the sum of individual computed HNOj gas and NOj aerosol
fluxes (approximate maximum rates due to assumption that aerodynamic resistance within forest
canopy was zero).
4-68
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TABLE 4-36 (continued)
Site
Estimated 1987-88 Acidic Nitrogen Deposition Budgets at MCCP Sites'^
Growing Season Mean N Deposition (kg S/na-mo)6
Wet (Measured) Cloud (Computed) Dry (Computed)*
Year
Rowland, MEd 87
88
87-88
0.15
0.07
0.09
0.08
Moosilauke, NHe 87
88
87-88
Whiteface, NY 87
88
87-88
Shenandoah, VA 87
88
87-88
Whitetop, VAf 87
88
87-88
Mitchell, NC 87
88
87-88
a. Not all data were
b. Average fluxes for
0.33
0.25
0.29
0.21
0.21
0.21
0.28
0.27
0.28
0.30
0.26
0.28
0.51
0.27
0.39
available in time for inclusion in
combined 1987-88 period were c
0.50
0.20
0.35
0.23
0.11
0.17
0.23
1.31
1.15
1.23
0.99
0.75
0.87
this report.
omputed by averaging values given separately
for the two years.
c. Sulfuf (S) flux computed as the sum of individual computed SC«2 gas and SO^ aerosol fluxes
(approximate maximum rates due to assumption that aerodynamic resistance within forest canopy
was zero).
d. Greenville, ME NADP data used for wet deposition fluxes.
e. Hubbard Brook, NH NADP data used for wet deposition fluxes.
f. Near-summit (plot A) site.
g. Nitrogen in ammonium ion not considered.
h. Nitrogen (N) flux computed as the sum of individual computed HNOj gas and NOj aerosol
fluxes (approximate maximum rates due to assumption that aerodynamic resistance within forest
canopy was zero).
4-69
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Table 4-37
Estimated Cloud-to-Wet Deposition Flux Ratios
Site Year Sulfate Nitrate
MS
WF
WT°
MM
1987
1988
87-88
1987
1988
87-88
1987
1988
87-88
1987
1988
87-88
1.0
0.6
0.8
1.1
1.3
1.1
3.6
3.5
3.5
1.7
2.6
2.0
1.5
0.8
1.2
1.1
0.5
0.8
4.4
4.4
4.4
1.9
2.8
2.2
a. Near-summit plot.
In summarizing the deposition results, MCCP and IPS researchers have estimated that
cloudwater deposition provides a substantial fraction of the total chemical deposition to high-elevation
eastern USA forests. Lindberg and Johnson (1989) estimated that cloudwater contributes approximately
25% to 50% of total SO^, N, and H+ deposition at two high-elevation sites on Whiteface Mountain,
NY and in the Great Smoky Mountains National park, NC. MCCP results indicate that cloudwater
SO^2', H+, NO/, and NH^+ deposition exceeded wet deposition via precipitation for three sites located
above 1400 m, while two lower elevation sites received cloudwater chemical inputs that were at least
one-half of precipitation chemical deposition. Preliminary estimates for dry deposition are considerably
smaller than either cloud or precipitation deposition at all MCCP sites except one site located in a
deciduous forest at Shenandoah, VA (Mohnen, 1988a; Krovetz et al., 1989). While the current large and
undefined uncertainties that are associated with cloud water and dry deposition models make firm
estimates for complex terrain impossible, there is a general consensus in the literature that cloud water
deposition represents a substantial increment over precipitation and dry inputs to high-elevation forests
in the eastern USA
4-70
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SECTION 5
METEOROLOGICAL ASSESSMENT OF AIR QUALITY
CASE STUDY ON THE IMPACT OF AIR MASS ORIGIN ON AIR QUALITY
A simple case study was performed at a northern MCCP site to investigate the relationship
between synoptic weather patterns and cloudwater ion and gas phase pollutant concentrations. If
meaningful results could be obtained, then there would be a basis to extend this type of analysis to other
sites and to other synoptic categories.
In this case, ion concentrations during warm sector synoptic conditions were investigated for the
1986-88 field seasons at Whiteface Mountain. Warm sector conditions are defined as the southeast
sector of the classical cyclone model or the west side of a high pressure system. Stagnant conditions
sometimes occur with semi-permanent "Bermuda High" type situations which often lead to air pollution
episodes. Therefore, warm sector conditions were classified as "non-stagnant" and "stagnant", the latter
requiring that warm sector, high pressure conditions at or to the south of the site were persisting for at
least 72 hours.
Table 5-1 shows the concentrations of selected ions for cloudwater and pollutant concentrations
for gases and sulfate aerosol for three categories: non-warm sector (category 0); non-stagnant warm
sector (category 1) and stagnant warm sector (category 2) conditions based on hourly samples. For all
ions, gases and sulfate aerosol, both warm sector concentrations are greater than other sector concentra-
tions by a factor of 2 to 3, indicative of the relatively warm and humid conditions, together with
favorable south to southwesterly trajectories, which favor high pollutant levels. Stagnant conditions
exhibited the maximum sample concentrations for all ions, gases and sulfate aerosol.
METEOROLOGICAL INFLUENCES ON CLOUDWATER CHEMISTRY
Air mass back-trajectories during all hours at all MCCP sites originated most frequently from
the western quadrant, and least frequently from the southeast. For cloudy periods, back trajectories
favored the southwestern quadrant, with a secondary frequency peak in the eastern quadrant, especially
for southern sites.
Synoptic scale mechanisms responsible for cloud formation differed for northern and southern
portions of the Appalachians. Nearly two-thirds of cloud events at Whiteface Mountain, NY, were
associated with pre-warm frontal synoptic conditions. However, at Whitetop Mountain, VA, over
two-thirds of all cloud events were associated with warm-sector and marine flow conditions.
The amount of acidic deposition to a mountain site depends on factors such as cloud frequency,
windspeed, liquid water content, and the history of the air mass in which the clouds are formed. To
relate cloudwater composition with large-scale circulation features, cloud events collected during the
1986-88 field seasons were classified according to nine synoptic features responsible for cloud production.
This scheme classifies cloud events according to a mountain's location relative to surface weather map
features for hours when cloud was observed at the sites.
5-1
-------
TABLE 5-1
CLOUD WATER ION STATISTICS
CATEGORIZED BY SYNOPTIC CONDITIONS
FOR WHITEFACE MT. SUMMIT: 1986-88
HYDROGEN ION (hourly measurements: /rniol/1)
Synoptic Cat. Frequency Percent Mean
Maximum
Synoptic Categories:
0 - not in warm sector
1 - warm sector, non-stagnant conditions
2 - warm sector, stagnant conditions
Minimum
0
1
2
1&2
All
382
139
68
207
589
SULFATE ION (hourly
Synoptic Cat.
0
1
2
1&2
All
Frequency
384
139
68
207
591
NITRATE ION (hourly
Synoptic Cat.
0
1
2
1&2
All
Frequency
384
139
68
207
591
64.9
23.6
11.5
35.1
100
measurements:
Percent
65.0
24.5
11.5
35.0
100
measurements:
Percent
65.0
23.5
11.5
35.0
100
134
335
320
330
203
MttlOl/l)
Mean
78
203
214
206
123
jimol/1)
Mean
61
130
191
150
92
1288
1412
1778
1778
1778
Maximum
547
668
1112
1112
1112
Maximum
752
632
1344
1344
1344
0.3
0.3
50.1
0.3
0.3
Minimum
0.4
0.3
40.8
0.3
0.3
Minimum
0.7
0.3
18.4
0.3
0.3
AMMONIUM ION (hourly measurements: ianol/l)
Synoptic Cat.
0
1
2
1&2
All
Frequency
384
139
68
207
591
Percent
65.0
23.5
11.5
35.0
100
Mean
80
181
227
196
121
Maximum
770
652
920
920
920
Minimum
0.7
0.5
43.0
0.5
0.3
5-2
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TABLE 5-1 (Continued)
GAS CONCENTRATION STATISTICS
CATEGORIZED BY SYNOPTIC CONDITIONS
FOR WHTTEFACE MT. SUMMIT: 1986-88
OZONE (hourly measurements: ppbv)
Synoptic Cat. Frequency Percent Mean
Maximum
Synoptic Categories:
0 - not in warm, sector
1 - warm sector, non-stagnant conditions
2 - warm sector, stagnant conditions
Minimum
0
1
2
1&2
All
6590
1292
565
1857
8447
SULFUR DIOXIDE
Synoptic Cat.
0
1
2
1&2
All
Frequency
4581
1025
456
1481
6062
78.0
15.3
6.7
22.0
100
41.9
57.3
69.7
61.1
46.1
127.1
132.6
135.3
135.3
135.3
11.0
23.0
32.0
23.0
11.0
(hourly measurements: ppbv)
Percent
75.6
16.9
7.5
24.4
100
HYDROGEN PEROXIDE (hourly
Synoptic Cat.
0
1
2
1&2
All
Frequency
594
90
188
278
872
Percent
68.1
10.3
21.6
31.9
100
Mean
0.8
2.4
2.3
2.3
1.2
measurements:
Mean
0.6
0.8
1.5
1.3
0.8
Maximum
13.7
17.7
20.0
20.0
20.0
ppbv)
Maximum
6.0
2.8
3.8
3.8
6.1
Minimum
0
0
0
0
0
Minimum
0.0
0.1
0.0
0.0
0.0
5-3
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Four of the nine synoptic types are associated primarily with the main sectors of a cyclone. The
nine synoptic types are: a) pre-warm-frontal clouds, b) northwest-sector of cyclone clouds, c) post-cold-
frontal clouds, d) warm-sector synoptic types including the southeast sector of the cyclone and stagnant
conditions, e) stationary-front cloudiness, f) easterly flow that advects moisture inland from the Atlantic,
g) and h) cutoff-low-aloft types (these two categories were created based on the location of the cutoff
relative to the site), and i) cap cloud which involves no important synoptic scale features within several
hundred km of the site and high cloud bases at nearby airports.
A site-cloud climatology was developed for Whiteface Mountain, NY, Mt. Moosilauke, NH,
Whitetop Mountain, VA, Shenandoah, VA, and Mt. Mitchell, NC. As Table 5-2 shows, at the northern
sites (NY and NH), the post-cold-frontal type (c) and warm-sector synoptic types (d) comprised most of
total cloud hours. At the southern sites (VA and NC), the warm-sector type (d) was most frequent
while the second most frequent cloud synoptic type (f) was a result of easterly flow.
Table 5-2
Percentage of Cloud Hours by Synoptic Type for Five MCCP Mountain Sites
(1986 - 88 Field Seasons)
Synoptic
Type Whiteface Moosilauke Shenandoah Whitetop Mitchell
a. pre-warm front 16.5 25.5 6.5 0.1
b. northwest of cyclone 5.8 11.5 4.5 4.2 2.5
c. post cold front 32.4 11.0 23.9 16.0 15.2
d. warm sector 30.7 31.8 11.3 45.4 41.9
e. stationary front 0.3 0.1 3.2 1.5 2.5
f. easterly marine flow 4.0 15.9 43.7 23.1 26.8
g. low aloft (W-flow) 3.4 2.0 1.8 5.0 2.9
h. low aloft (SE-flow) 1.4 2.2 5.1 0.1
i. cap cloud 5.5 - - 4.6 8.2
Two types of statistical models were applied to the data for 1986-88. The first model, partial
least-squares regression on latent variables (PLS), was used to identify combinations of meteorological
parameters that predicted linear combinations of chemical concentrations (Vong et al., 1988a; Geladi and
Kowalski, 1985). The linear combinations were formed from correlated variables.
The original data consisted of hourly cloud water samples and corresponding hourly meteoro-
logical parameters of trajectory, synoptic type, cloud type, and local winds. Trajectories were obtained
from a mixed-layer model that uses rawinsonde measurements to define the transport field (Kahl and
Samson, 1988). The chemical data were square-root transformed before analysis to keep extreme
samples from dominating the results. Hourly samples from continuous cloud events were aggregated
into sub-events with consistent trajectories.
A six-component PLS model identified significant covariance structure in the meteorological
variables that was related to the chemical data. The correlations that were revealed among synoptic
types and mixed layer trajectories were physically realistic. For example, the "marine" synoptic type
occurred with easterly trajectories and high cloudwater chloride concentrations, the warm-sector synoptic
type (d) occurred frequently with SW trajectories and high SO^2" concentrations, and the post-cold-
5-4
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frontal synoptic type (c) occurred with NW trajectories and low SOj2' concentrations. This agreement
added confidence to the use of the two types of meteorological variables (synoptic type and mixed-layer
trajectory). PLS identified significant covariance in the chemical data also. H+, NH4+, SOj2-, and H+
were correlated.
Based on the PLS modeling, the following synoptic-trajectory classes were posed as the most
important influences on cloudwater chemistry at the four sites for further analysis:
Synoptic type (d) = warm-sector, SW trajectory
Synoptic type (d) = warm-sector, all other trajectories
Synoptic type (i) = cap-cloud, SW trajectory
Synoptic type (i) = cap-cloud, all other trajectories
Synoptic type (c) = post-cold frontal, NW trajectory
Synoptic type (c) = post-cold-frontal, all other trajectories
Synoptic type (f) = marine-flow, SE to NE trajectory
Synoptic type (f) = marine-flow, all other trajectories
All other synoptic type (a, b, e, g, h) and trajectory combinations
The second model, analysis of variance (ANOVA), was used to test the hypothesis that this
smaller number of meteorological variables would describe variability in cloudwater chemistry. Classes 3
and 4 were combined with 1 and 2 because both represented stable atmospheric conditions, and there
were few observations of cap cloud compared to synoptic types c, d, and f. The ANOVA model (Box et
al., 1978; Vong et al., 1988b) tested for differences in cloudwater chemistry for the seven remaining
synoptic/trajectory classes.
This model was highly significant (p < 0.001). The three main effects were significant; there
were differences between sites, cloud-only (non-precipitating) and mixed rain/cloud (precipitating) types,
and synoptic-trajectory classes. Table 5-3 gives mean ion concentrations for all MCCP sites for selected
synoptic-trajectory classes and cloud types.
TABLE 5-3
Analysis of Variance Results for Four Ion Concentrations:
Mean Values for all MCCP Sites (1986-88) in *eq/L for Selected Synoptic-Trajectory Classes, All Clouds
Ion
Synoptic-Trajectory Class SO^2' H+ NH4+ NO/
Warm sector - Ohio Valley Trajectory 361 304 161 133
Warm sector - Other trajectories 246 190 117 88
Post cold front - NW trajectories 131 90 59 43
Marine flow - E trajectory 134 138 47 61
Mean of all 9 classes (all cloud) 199 170 86 78
Mean: non-precipitating cloud 262 220 116 104
Mean: precipitating cloud 113 101 47 43
The site-class interaction terms confirmed different warm-sector synoptic type dependencies of
SO/2' on trajectory. The highest SO^2', H+, NH^+, and NO/ concentrations occurred with the
5-5
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warm-sector synoptic type (d) when the trajectories pointed toward the Ohio Valley. This is consistent
with the notion of transport from that high emission area.
Remaining variation within each synoptic-trajectory class is expected to be related to variation in
gas- and aqueous-phase chemical processes, scavenging, and meteorology that could not be described in
the synoptic-trajectory classification scheme. For example, the height of the monitoring site above cloud
base should affect the amount of available liquid water and, therefore, aqueous phase concentrations, but
testing that effect for all sites was not possible because cloud base data were not always available. For
one site (Whiteface Mountain, NY) there were consistent differences between two collection sites located
at different elevations when 106 hours of simultaneous data were compared; the lower site had higher
concentrations. The modeling approach described here was able to characterize several factors that
influence the composition of mountain cloudwater composition in the eastern USA
GAS CONCENTRATION VS. AIR MASS TRAJECTORIES
Ozone
Mean ozone concentration is not strongly a function of 36-hour air mass trajectory sector, as
shown in Figures 5-1 through 5-6 (Appendix E) for the 1986-88 period. Northern sites have somewhat
higher mean values for southeasterly to southwesterly trajectories while southern sites exhibit a fairly
uniform distribution. A clearer pattern emerges from high ozone concentrations. Figures 5-7 through
5-17 (Appendix E) focus on trajectory dependency for ozone values greater than 70 ppb and 100 ppb.
Rowland, Moosilauke and Whiteface favor west-southwesterly trajectories during ozone episodes whereas
the southern sites exhibit a broader and more northerly distribution of trajectories. This pattern is
consistent with the weaker, more stagnant airflow conditions found over the southeastern states in
summer and their proximity to the center of semi-permanent high pressure systems. In the Northeast,
ozone episodes are usually associated with backside flow around a stagnant high pressure system (e.g.
Bermuda High).
Hydrogen Peroxide
Gas phase measurements for H^ at Whiteface and Whitetop are shown in Figures 5-18 and 5-19,
(Appendix E) respectively. Despite the overall lack of variability in concentrations, mean values at
Whiteface are highest for southwesterly trajectories, which is consistent with the pattern found for ozone.
Hydrogen peroxide is a secondary product resulting from complex photochemical reactions initiated by
ozone. The directional dependence at Whitetop is less clear, but peak H^ values there are associated
with westerly trajectories.
Sulfur Dioxide
In summer, mean S02 concentrations are low, averaging under 3 ppb at all sites. As with the
other gases, S02 values (Figures 5-20 to 5-23 - Appendix E) are higher with west to southwesterly
trajectories for sites in the north. Southern sites exhibit higher concentrations for north to northwesterly
flow. The differing dependence of gas concentrations on trajectory between northern and southern sites
suggests a common air mass source region for relatively high concentrations-the Ohio Valley.
5-6
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SECTION 6
METHODS AND PROTOCOLS
This section discusses field collection and laboratory analysis methods for cloud water chemistry,
liquid water content, and supporting measurements such as meteorology, throughfall, and precipitation.
Uncertainties are discussed with each method.
The MCCP collects cloud water only during the growing season, the onset of which varies
depending on site location. At most sites, sampling is conducted for intensive campaigns of ap-
proximately three to six weeks, during which every cloudy period is sampled. At least three intensive
sampling periods have been conducted during the growing seasons (approximately April-October) of 1986
through 1988 except for two sites that started during 1987.
Cloud water collection is begun as soon as possible after the start of a cloud event, which is
defined by both visibility and volume. When a stationary object approximately 1 km from the collection
site is consistently obscured from view for more than 15 minutes, a cloud event is defined to have
started. Collection is discontinued when either the stationary object is no longer obscured from view, or
less than 10 ml of sample has been collected over a 20 minute period. Liquid water content and
aqueous phase chemistry are monitored during these cloud events. Gases, meteorology, precipitation
chemistry, and throughfall chemistry are measured during cloudy and non-cloudy periods throughout each
intensive sampling campaign.
CLOUD WATER COLLECTION
Mohnen and Kadlecek (1989) discussed the processes governing cloud collector efficiency and
design. Passive cloud water collectors, such as the MCCP designated ASRC design (Falconer and
Falconer, 1980), depend on ambient wind speed to impact droplets onto 0.4 mm wires strung between
two circular disks. Active cloud water collectors have a blower or fan to provide the velocity difference
between the droplet and the collecting string that is necessary for impaction. Factors that govern the
overall efficiency for collector accumulation of liquid water include: impaction on the inertial collector
surface (based on Langmuir stopping distance); accumulation/coalescence of individual droplets into a
film or larger droplet; transport of the water from the collector surface to the storage container via
gravitational, centrifugal, or pressure forces; evaporation of deposited cloud water from the collector
surface; and resuspension (blow off) of water due to high wind speed at the collector surface. Various
collector designs attempt to maximize efficiency for droplets above 2 to 5 nm diameter (a smaller cut-off
size would allow collection of unactivated aerosol). However, the reduced collection efficiency below 5
itm diameter allows small droplets to escape collection.
During winter, supercooled cloud water freezes on impact with the collector strings. Collection
efficiency is reduced due to the increased surface area of the strings covered by rime, so the accumulated
rime is collected manually as often as possible to minimize this effect (Kadlecek et al., 1988). MCCP
does not perform winter sampling.
Two types of cloud water collectors are used at MCCP sites, the ASRC passive collector and the
Cal-Tech active string collector. Both have been found to collect water with equivalent chemistries over
wind speeds ranging from about 3 to 30 m/s (Mohnen and Kadlecek, 1989). At most sites, the collectors
are placed on the top platform of towers above the surrounding canopy. The only exceptions to this are
Whiteface Mountain, where the collector is on the roof of the summit research lab, and Whitetop
Mountain, where it is on a platform built over the research trailer.
6-1
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Once a cloud event has begun, clean tubing and a collection bottle are attached to a collector and
it is deployed. Collection bottles are changed hourly, and a portion of each hourly sample is analyzed in
the field for pH. Five to 10 ml is preserved for hydrogen peroxide analysis. Each bottle is refrigerated
until it is sent to a laboratory for chemical analysis. At the end of each event, the cloud collectors are
detached and rinsed with deionized water until the conductivity of the rinse water is within % 10
^Siemens. Collectors are covered until the next cloud event. When more than 125 ml is collected at the
end of one hour, the sample is split into two aliquots; one split is sent to the Central Analytical Lab
(CAL) and the other to the site-associated analytical lab. Further details are provided in the MCCP
Standard Operating Procedures Manual (1989); Quality Assurance procedures and results are described.
FREQUENCY OF CLOUD
For forest exposure and cloud water deposition estimates, it is necessary to understand when and
where liquid water is present, at what mass concentration, and how the water is distributed among
different droplet sizes. These data are referred to collectively as describing the presence of liquid water
in the atmosphere.
The emphasis of the cloud frequency analyses conducted by the Mountain Cloud Chemistry Project
(MCCP) is to estimate cloud impaction at mountain summits and the overall cloud distribution in the
Appalachian Mountains. Because routine observations are scarce on mountains, other data sources were
necessary to estimate long-term horizontal and vertical cloud distribution. This section describes the
methodologies and associated uncertainties in determining regional and site-specific cloud frequency
estimates. The data sources considered are National Weather Service (NWS) surface airport observa-
tions, US Air Force Real-Time Nephanalysis archives, and site-specific mountain cloud measurements
conducted by the MCCP.
Regional Estimates
Airport observations have been analyzed to obtain cloud climatologies for the eastern USA
(Warren et al., 1986). Surface airport observations consist of hourly measurements of cloud base height,
coverage, and type. Cloud base heights have been measured since the mid 1920s using either a fixed- or
rotating-beam ceilometer. This technique has an estimated accuracy of,+ 30 up to 1000 m in elevation,
and of +. 10% above 1000 m (WMO, 1976). Data are archived by the National Climatic Data Center
for all reporting airport stations.
A limitation to airport observations is that few stations are located within mountainous areas.
Airport-mountain comparisons have been investigated by Bailey and Markus (1987) and Imhoff and Malo
(1989). A common finding is that airports are good indicators of mountain cloudiness for large-scale
cloud systems but are poor indicators of small-scale cloud systems typically associated with orographic
effects (e.g., cap cloud).
Bailey et al. (1989) have examined the temporal and spatial variations of low-level clouds (below
2000 m) in the eastern USA using the Real-Time Nephanalysis (RTNEPH), the global cloud archives
produced by the US Air Force. An earlier version, called 3-Dimensional Nephanalysis (3DNEPH) was
begun in 1971 (Fye, 1978) and replaced in 1984 by the improved RTNEPH version. Both versions use
all conventional surface and rawinsonde data, pilot reports and satellite data to produce three-
dimensional cloud information. RTNEPH data are organized according to a horizontal grid system
superimposed upon a polar stereographic projection. Grid point spacing is 47.7 km at 60° latitude
where projection is true. Each grid point contains the following data for every 3-hour period: type of
low, middle and high clouds, present weather, maximum cloud top, minimum cloud base, total percent
6-2
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sky coverage, and percent coverage for 15 fixed layers. Gordon et al. (1984) have used 3DNEPH analysis
of observed monthly mean cloud amounts to calculate radiative fluxes with a cloud model. Hughes and
Henderson-Sellers (1985; 1986) have compiled a global cloud climatology for 1979. Schulz and Samson
(1988) used 3DNEPH data to determine non-precipitating low cloud frequencies for central North
America for 1982.
The uncertainties in the RTNEPH data archives consist of the limitations in each data source that
was included. Limitations to the surface airport readings have been discussed previously. The satellite
visual data processor cannot distinguish between clouds and bright areas of snow or ice. Therefore,
unless accurate snow or ice data were available, the analyses may be in error. In addition, small cloud
elements over high variability backgrounds (coastlines and mountainous areas) may not have been
detected. The 47.7 km grid spacing precludes resolution at smaller space scales, and thus the RTNEPH
analyses are best used for regional analysis. Low-level clouds, particularly for multi-layer cloud condi-
tions, are best detected by surface and rawinsonde observations and least by satellites. In areas where
airport station density is low, low-cloud information may not be well represented.
Site-specific Methods
Three different techniques for estimating the frequency of cloud impaction have been used by the
MCCP since the 1986 field season. From the project's onset, relative humidity has been used at most
sites to estimate periods of cloud presence in lieu of an affordable direct measurement technique. The
Whitetop site has always used a reflectometer to determine the presence of cloud, but its cost (in excess
of $10,000) precluded its use throughout the MCCP network. Beginning with the 1988 field season, the
new Mallant optical cloud detector was installed at most sites. This section describes the three
techniques while the next section inter-compares the techniques. A fourth technique (Krovetz et al.,
1988) has also been used on an experimental basis, particularly at the Shenandoah site. This technique
will not be discussed here because it was not used to derive official presence of cloud estimates.
Relative humidity (RH) is sensed by a Rotronics MP-100 combination temperature/RH probe
housed in a naturally aspirated radiation shield. Cloud presence is determined subjectively by analyzing
the time series trace during saturation and near-saturation conditions. The tendency for the sensor's
response in these conditions to drift upward with time has precluded the use of a wholly objective RH
cloud threshold (such as a minimum RH value) to define cloud events. Average RH values are recorded
hourly based on 5-second samples. As verified by field observations, the onset of cloud is typically
marked by a sharp rise in RH to near 100% followed by a leveling off, and cloud dissipation is marked
by an abrupt drop of several percentage points.
The uncertainties inherent in the RH technique are several: the element of subjective interpreta-
tion, the sensor's 5% accuracy specification, the use of hourly averaged values, and its slow response
time relative to the two optical techniques. Overall, it is suspected that this technique may somewhat
overestimate the frequency of cloud due to the fact that near-saturation conditions can occur in the
absence of clouds such as during heavy or prolonged rain events.
A backscatter reflectometer (visibility sensor Weathertronics Model 8340) has been used by TVA
since 1986 as a cloud detector. According to Valente et al. (1989), "observations at Whitetop have shown
that by using a signal of 0.15 (5% of the output range) as the definition of presence of cloud, haze and
liquid precipitation are not mistaken for cloud impaction." The instrument has a visibility range of
1000+m to 10 m, corresponding to a signal output of 0 to 100% of scale, respectively. The detection
threshold of 5% of scale corresponds to a visibility of about 260 m according to the manufacturer's
literature. This instrument has not been used at MCCP sites other than Whitetop.
6-3
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The uncertainties with the reflectometer are not well defined. However, the method used to obtain
hourly signal values will tend to overemphasize the presence of cloud within an hour in which cloud was
present less than half the time. This occurs because the signal's scale is logarithmic whereas hourly
averages are derived arithmetically (private communication, TVA). Hourly average reflectometer values'
are based on 5-minute intermediate average values derived from 20-second samples. Given that the first
5% of scale (cloud absent) corresponds to a visibility range of about 740 m while the remaining 95% of
scale (cloud present) corresponds to about a 250 m visibility range, arithmetic averaging of percent of
scale values within an hour will give greater weight to "cloud present" signals. This can be a source of
discrepancy when comparing different measurement techniques during variably cloudy hours.
The Whitetop site has also used a time-lapse video recording system to estimate cloud base
elevation. The system is located about 4.5 km northwest of the mountain at an elevation about 760m
less than the site elevation of 1689 m. The location provides a clear view of the mountaintop from one
direction and is limited to daytime observations. Cloud base heights are derived hourly through manual
interpretation of the video record.
The Mallant Optical Cloud Detector is a forward-scattering optical device originally developed by
the Energy Research Foundation in The Netherlands (Mallant and Kos, 1989). Following successful
laboratory and field tests (Valente et al., 1989), a modified design was built by Associated Weather
Services and deployed at all summit sites in 1988. It has an adjustable detection threshold corresponding
to liquid water content at an assumed mass median droplet diameter. Hourly recordings indicate the
percentage of time with cloud present based on 5-second samples. Each sample produces a binary signal
corresponding to cloud presence (=1) and absence (=0).
The Mallant instrument's detection threshold is set at an equivalent LWC value of approximately
0.04 g/m3 for a droplet mass median diameter of about 11 microns. This is roughly equivalent to a
visibility of 350 m (Atlas and Bartnoff, 1953). The uncertainty in this threshold is on the order of ±0.02
g/m3 due to the uncertainties in the FSSP-based laboratory calibrations and on the imprecision of the
adjustment potentiometers. Under ambient field conditions, the actual detection threshold will also be a
function of the cloud's drop size distribution. Therefore, this instrument's response to cloud, especially
"thin" clouds, is variable. It has also been observed that this instrument can be susceptible to droplet
accumulation on the optical lenses which results in a reduction in the sensitivity to the presence of
cloud. The detector does not contain heaters and therefore is suitable only for above-freezing cloud
conditions.
Comparison of Methods
This section presents results of several intercomparison tests between the three primary techniques
used to estimate presence of cloud.
Mallant vs. Reflectometer-
Several intercomparisons of the Mallant cloud detector and the TVA reflectometer have taken
place, beginning with the 1987 liquid water content instrument "shoot-out" at Whitetop Mountain
(Valente et al., 1989). This first intercomparison used an original Mallant prototype whereas all later
intercomparisons used the modified design. In all intercomparisons the TVA reflectometer was desig-
nated an arbitrary "standard" to define periods when cloud was present or absent. The first intercom-
parison, covering a two-week period in 1987, found that the Mallant prototype had 98% agreement with
the reflectometer during cloud events and 93% agreement during non-cloud events.
Four other intercomparisons were conducted during 1988 and 1989 using four different Mallant
instruments. These tests comprised over 5700 field hours. The Mallant design agreed with 96% to 99%
6-4
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of the cloud/no cloud observations taken by the reflectometer. When clouds were indicated by the
reflectometer, the Mallants agreed 92% to 95% of the time for three of the instruments, and 80% for
the other. The lower agreement of this one instrument was the result of it not responding to cloud for
a 24-hour period within one extended cloud event. It is suspected that water droplets accumulated on
its lenses, reducing the instrument's sensitivity. When the reflectometer indicated that clouds were absent,
agreement with all four Mallants ranged from 98% to 100%.
Relative Humidity vs. Mallant-
Concurrent estimates of hourly cloud presence using the RH and Mallant techniques were made
throughout the 1988 field season at four MCCP summit sites: Mitchell, Moosilauke, Shenandoah and
Whiteface. A minimum of 2300 hours of simultaneous values were taken at each site. Based on its
favorable intercomparison results with the TV A reflectometer, the Mallant detector was designated the
standard in the intercomparisons with RH. An hour with cloud as defined by the Mallant required the
instrument to be detecting cloud for at least 50% of the hour. Overall agreement between techniques on
an hourly basis ranged from 87% to 96%. During cloud conditions as defined by the Mallant, agreement
ranged from 81% to 94%. During no-cloud conditions, they were in agreement 88% to 96% of the time.
RH vs. Mallant and Reflectometer-
The early 1989 field season was the first opportunity for the standard MCCP RH sensor to operate
together with the Mallant and reflectometer instruments at Whitetop Mountain. Based on over 1100
hours of operation, RH agreed with the reflectometer 91% of the time, and 90% with the Mallant.
During cloudy conditions the agreement was 86% and 85%, respectively. During non-cloudy conditions,
the agreement was 94% and 91%, respectively.
LIQUID WATER CONTENT
The MCCP initiated network-wide measurements of cloud liquid water content (LWC) in 1987
using the TVA-Valente filter collection method. This section presents the results of a review of LWC
and drop size measurement methods and a field comparison of several LWC instruments. Most LWC
measurement instruments have been designed for aircraft operation where the speed of the aircraft is an
aid to operation. Ground-based instruments are typically modified versions of aircraft systems, and can
be classified according to their operating principle as thermal, optical, or inertial impaction methods.
The Johnson-Williams liquid water instrument consists of a heated wire that is cooled by the
evaporation of liquid water droplets. An instrument time constant of approximately 1-2 sec may cause
underestimation of water contents (Spyer-Duran, 1968). A further limitation is a limited response to
droplets larger than 30 ion. The instrument must be calibrated in a cloud tunnel to achieve the expected
accuracy.
The NHRL Nimbiometer and the CSIRO (King) Probe are heated-wire instruments. Improve-
ments were made by Merceret and Shricker (1975) by operating the instrument at a constant tempera-
ture below 100°C where the power dissipated is proportional to the square of the liquid water content.
King et al. (1978) improved the instrument by increasing the cooling by liquid water relative to cooling
by dry air. Measurements agree with other instruments to about 5% at LWC of 2 g/m3. The advantage
of this design is that wet calibration is not required. However, at low air speeds typical of ground-based
systems, the errors are proportional to \-^2 (King et al., 1978), making it necessary to vary the aspira-
tion speed with wind speed. Particle Measuring Systems, Inc., has developed a King Probe prototype to
6-5
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measure LWC of up to 1 g/nv3. The probe is oriented using a wind vane. A field test at Whitetop
Mountain, VA, indicated that further development and testing are needed because of short circuits
during wet, cloudy periods, sensitivity to radio frequency interference, and rain droplet contamination of
the inlet (at wind speeds > 3 m/s).
Chylek (1978) investigated an optical technique that uses the extinction of radiation of a wave-
length of 11 ^m and found that infrared extinction should be directly proportional to liquid water
content. Several attempts to use this technique in cloud and fog have been encouraging (Gertler and
Steele, 1980; Jiusto and Lala, 1982), but practical problems have limited its full use. Comparison of a
laser transmissometer (Jiusto and Lala, 1982) with a droplet spectrometer (FSSP-100) revealed good
agreement up to water contents of about 1 g/m3. The presence of many large droplets (> 28 ^m)
degrades Chylek's (1978) approximation and contributes to forward scatter errors. At LWC less than 0.5
g/m5, the transmissometer system was within 10% of filter measurements and 35% of FSSP-100 values.
This promising technique is still in the development stage.
Another instrument estimates LWC by measuring scattered intensity in the near forward direction
(0.25 to 5°). BIyth et al. (1984) designed an instrument with a 26 cm path with discrete detectors at five
different angles from the scattering axis. Based on theoretical calculations, the signals are weighted to
provide a signal proportional to LWC. Comparison with drop spectrometers and infrared transmis-
someters show excellent agreement. This instrument still requires development to construct a field unit
suitable for routine observations.
Gerber (1984) proposed a similar instrument based on the principle that light scattered by the
droplets in the near-forward direction is strongly correlated with infrared extinction, and is thus also
proportional to LWC according to the Chylek (1978) relationship. Gerber Scientific offers the Particle
Volume Monitor (PVM), capable of measuring in situ, and in real time, the integrated volume of
particulates suspended in the atmosphere with a stated precision of 0.002 g/nv'. A narrow beam from a
780 nm laser diode irradiates the droplets in the open air along a 40 cm path. Calibration results
indicate % 10% agreement with an infrared transmissometer in controlled fogs (Gerber, 1988).
A prototype instrument developed by Scott McLaren of ASRC SUNY-Albany, NY, uses a chilled
mirror dewpoint sensor to measure the dewpoint of two differently treated streams of sampled air, and
switches streams at five minute intervals. The first stream contains air that has been heated to evaporate
the cloud droplets into the air stream, and the second stream is filtered to remove the droplets. By
measuring the small difference in dewpoint between these air streams, the LWC can be calculated from
psychrometric principles, provided that significant changes in LWC do not occur between the two
adjacent averaging periods.
Filters and impactors are the oldest method of measuring liquid water content. Examples are
reported by Houghton and Radford (1938) and Wattle et al. (1984). The operating principle is simply
to draw a large volume of cloudy air through a filter and then weigh the accumulated water. Using large
air flows and large collection areas minimizes the size selection collection problems. With light wind
and droplets below precipitation size, this technique comes close to providing an absolute measurement
of LWC. One limitation is that during periods with less than 100% relative humidity, evaporation may
result in an underestimate of LWC. The method requires constant attention and averages over the
one-hour sample period.
Impaction techniques are similar to filtering, but they emphasize droplet sizing instead of mass
concentration. A glass slide with a gelatin coating (Jiusto, 1965) or another material sensitive to water
drops is used for collection. With gelatin, droplets leave impressions that are twice the diameter of the
impinging droplets. The slides are analyzed with an optical microscope to determine drop size distribu-
tion and water content. This technique may discriminate against either the large or small end of the
6-6
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spectrum, depending on the collection method. Baumgardner (1983) estimated a 32% error in measure-
ment.
Optical particle spectrometers measure the size distribution of particles by light scattering. Size is
determined by a calibration of the light pulse amplitude from particles of known size. LWC is calcu-
lated by integrating the droplet volumes from the measured droplet spectrum and dividing the total mass
of liquid water by the sampled air volume. Different optical configurations compensate for the size
dependence of the scattering efficiency. Virtually all designs exhibit some uncertainty at sizes of the
order of the wavelength of the light source. Perhaps the greatest obstacle to using these instruments in
cloud is that the aerosol configuration discriminates against large particles such as cloud droplets
(Davies, 1968).
Particle Measuring Systems, Inc., developed the Forward Scatter Spectrometer Probe (FSSP-100)
with a unique sample inlet configuration. The laser light source is focused to a 100 nm diameter;
scattered light is split to separate the light scattered by particles in the center of the beam from the
signal, making it possible to avoid the aerodynamic focusing used in other systems. The signals from
particles that pass through edges of the sample volume are eliminated by measuring the time it takes for
a particle to cross the beam and comparing this with a running average. This design alleviates inlet
problems, but the use of forward scattering with small collection angles has resulted in a scattering
response with several multi-valued regions (Pinnick et al., 1981), especially between 0.5 and 2 nm and
near 8 urn diameter. FSSP measurement uncertainty under the best conditions is about 34%, and an
uncorrected system could have errors from 54% to 105% (Dye and Baumgardner, 1984; Baumgardner,
1983). FSSP-100 sampling efficiency remains open; in low wind conditions the sample should be
representative. The probe should be aligned into the wind and, in gusty conditions, correction to the
sampling rate may be necessary. To compensate for variable winds, modifications that continuously
adjust the fan speed are available.
The TVA-Valente instrument (Valente, 1988) used by the MCCP collects droplets by filtration
from a metered air volume in an Ertalyte plastic cartridge filled with eight layers of a high collection
efficiency polypropylene mesh. Inlet velocity is matched to the mean wind velocity to minimize non-
isokinetic sampling errors. A rain shield minimizes collection of precipitation-size droplets; however,
significant precipitation-induced errors are likely at wind speeds above 10 m/s.
Liquid water content (LWC) measurement in the MCCP follows the same collection schedule as
that described for cloud water. The LWC collector is deployed near the cloud water collector at the
start of an event. The collector cartridge is weighed at the beginning and end of an hour and the hourly
LWC is calculated by dividing the weight gain by the sampled air volume. The inlet velocity is adjusted
to match the mean wind velocity to minimize anisokinetic sampling errors. A rain shield is used to
minimize collection of precipitation-sized droplets. The sampler must also be pointed onto wind and an
inlet size is selected depending on wind speed. Detailed operational procedures can be found in the
MCCP Standard Operation Procedures (1989).
During 1988, MCCP used optical cloud detectors to record the hours with patchy clouds. The
collection mesh and range of inlet velocities were designed to collect cloud droplets from 3 to 200 ^m in
diameter with greater than 95% efficiency. A rain shield excludes rain (droplet radius > 500 urn) and
drizzle (200-500 /»m radius) falling at an angle of greater than 15° from horizontal. However, during
high winds combined with precipitation and cloud, some precipitation will be sampled. LWC measure-
ments of clouds by the MCCP therefore differentiate between precipitating and non-precipitating events
because the technique may overestimate LWC during precipitating events.
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Droplet Size Distribution from LWC
Cloud droplet size distributions (or size spectra) are measured using impactors or a forward
scattering spectrometer probe (FSSP) that measures the degree of scattering of a narrow laser beam as
particles pass through the beam (Knollenberg, 1981). The amount of scattering depends on particle size.
The instrument can detect droplet diameters from < 1 itm to 100 iaa.
Because median droplet size is important for cloud droplet interception processes but is not
routinely monitored by MCCP, it is sometimes estimated from measured liquid water content (LWC).
MCCP scientists have, investigated the relationship between the median droplet volume diameter (dn)
and LWC for stratus and stratocumulus clouds. The parameter dn is defined as the droplet diameter
that divides the total cloud liquid water into equal parts by volume (Best, 1951). Stratus and stratocum-
ulus clouds were examined because of their similarity to clouds observed from mountaintop forests.
Seventeen data pairs, representing 96 measured droplet size distributions, were used to determine the
correlation between dn and LWC. One-half of the variance in dn was explained by variance in LWC,
suggesting that LWC and droplet size distribution are related for mountaintop clouds but that con-
siderable size spectra variability is associated with other factors.
LWC from Cloud Sampler Collection rate
An additional size spectra feature having implications for cloud deposition modeling is the large
variation in the size spectrum for a given value of LWC. Large fluctuations in droplet number con-
centration and diameter imply that, despite a general tendency for the size spectrum to vary with LWC,
a large amount of noise exists in the data. If droplet-leaf capture efficiency is non-linearly dependent on
droplet size, then the large variability in the size spectrum will result in a biasing of cloud deposition
estimates.
A data analysis technique for estimating LWC has been examined at several MCCP sites. The
collection of cloud water (at a volume collection rate Rc) by a passive ASRC string collector such as
used by Falconer and Falconer (1980) is known to depend on the dimensions of the strings, cloud
droplet diameter, wind speed (M), and LWC. A given droplet size distribution has a characteristic
diameter that is presumed to be representative of the droplet size spectra. This diameter is not known.
Assuming a constant linear relationship, several investigators have used- regression to determine an
empirical relationship between LWC and RC/M (e.g., Saxena et al., 1989).
At Shenandoah, Krovetz et al. (1989) compared LWC (gravimetric measurement) from the ratio
, where V is the measured collector cloud water volume and S is the Stokes number (Fuchs,
1964). S was computed using the known string diameter, measured wind speed, and a constant droplet
diameter. They reported a correlation (r2 = 0.77) between 11 pairs of measured and estimated LWC
values.
These regressions assumed that the effect of droplet size on droplet collection efficiency is
constant. However, measured droplet spectra have been found to be highly variable over short time
intervals, even when liquid water content was relatively constant (Mueller and Imhof, 1989). Therefore,
estimated median droplet size from LWC data or LWC from a passive sampler collection rate are
considered to be a crude approximation of the distribution or concentration of liquid water in the
atmosphere.
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GASES
Gaseous measurements in MCCP are made using a combination of standardized and research
techniques. The ultraviolet (UV) photometric method for ozone and the UV fluorescence method for
sulfur dioxide are the most well-defined gas measurements, with traceable quality assurance standards.
Measurement methods for nitric acid, sulfur dioxide, and hydrogen peroxide lack traceable quality
assurance standards, but have been involved in inter-comparison, laboratory, and field studies. Table 6-
indicates the measurements that are made at each MCCP site.
Ozone
Ozone measurements at MCCP sites are made with the UV photometric technique described by
Bowman and Horak (1972), which is equivalent to the US EPA's reference method (Federal Register,
1980). The TECO Model 49 used in the MCCP has a minimum detectable limit and precision of 2 ppb.
Ambient ozone values are 40 to 50 ppb at MCCP sites.
TABLE 6-1
Gas Measurements at MCCP Sites
Site Gas Measurement
Rowland, ME Ozone, sulfur dioxide, nitrogen oxides
Mitchell, NC Ozone, sulfur dioxide, nitrogen oxides
Moosilauke, NH Ozone
Shenandoah, VA Ozone, sulfur dioxide, nitrogen oxides
Whiteface, NY Ozone, sulfur dioxide, nitrogen oxides, hydrogen peroxide
Whitetop, VA Ozone, sulfur dioxide, nitrogen oxides, hydrogen peroxide
Sulfur Dioxide
Sulfur dioxide (802) is measured using continuous and integrated methods. Continuous detection
of the characteristic fluorescence by SO2 when irradiated by ultraviolet light was described by Okabe
(1973). These monitors have been designated as equivalent to the US EPA's reference method (Federal
Register, 1979). The TECO model 43 used for SO2 has a minimum detectable limit of 2 ppb with a
precision of 5 ppb. The maximum SO2 concentrations at MCCP sites are in the 20 ppb range with a
mean of approximately 2 ppb. This instrumentation thus provides a good estimate of the upper limits of
SO2 at MCCP sites, while lower SO2 limits are not well defined.
Integrated measurements of SO2 are made using the filter pack or the annular denuder system.
The filterpack system has been characterized by Anlauf (1986) and Sickles (1987). In the filterpack unit,
SO2 is collected on a Whatman 41 filter impregnated with sodium carbonate in glycerol (Huygen, 1963).
The minimum detectable limit for SO2 using the filterpack system is estimated to be 0.5 ppb. Factors
influencing the sensitivity of the method include sampling time, analytical sensitivity, and sampling
environment. A comparison of the filterpack method and a TECO SO2 monitor indicated agreement
over a range of ambient concentrations (Anlauf, 1986).
The annular denuder system described by Possanzini (1983) is a multi-constituent sampler than can
be used to measure a number of atmospheric gases: SO^ HNOj, NHj, and HONO. Diffusion denude-
rs have been used by several investigators to separate gases and aerosols, to collect gases for analysis, or
6-9
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as preseparators (Forrest, 1984; Shaw, 1982; Perm, 1972). The overall sensitivity of the technique is
comparable to the filterpack method for 803.
Nitric Acid
Nitric acid measurements in MCCP are made using either the fllterpack or the annular denuder
system (ADS). Because of possible biases in HNOj' and NOj" sampling with the filterpack, a total
inorganic nitrate value is obtained from ion chromatographic analysis of the Teflon and nylon filters.
Using total inorganic nitrate as a measure of nitric acid could result in overestimation of nitric acid.
Nitric acid and nitrous acid are collected on a sodium carbonate coated annular denuder in the ADS
system. For long sampling times (greater than 48 hrs), the nitrous acid can be oxidized to nitrate on
denuder surface; this gives an overestimation of the nitric acid due to the potential biases listed above.
Hydrogen Peroxide
Gaseous hydrogen peroxide is measured with an automated monitor described by Lazrus (1986).
This technique reacts peroxide with p-hydroxyphenylacetic acid in the presence of peroxidase. The
minimum detectable limit is estimated to be 0.05 ppb with a precision of 0.01 ppb. Hydrogen peroxide
levels range from 0.1 to 3.0 ppb at the MCCP sites. When the monitor was compared with laboratory-
generated standards, the two agreed within 10% across a concentration range of 0.06 to 128 ppb
(Kleindienst, 1988).
METEOROLOGICAL MEASUREMENTS
The MCCP meteorological measurement program was designed to complement the cloud water
collection and analysis as well as to define the climate of high-elevation Appalachian Mountain forests.
Each MCCP site measures wind speed, wind direction, temperature, relative humidity, solar radiation,
barometric pressure, and precipitation. Beginning with the 1988 field season, cloud presence was
measured with an optical cloud detector. All MCCP sites except Whitetop use the same package of
sensors and follow the protocols of measurement established by the MCCP Quality Assurance (QA) Plan
(1988) and detailed in the MCCP's Standard Operating Procedures (1989) and the Meteorological Site
Technician's Handbook. The Whitetop site follows a measurement protocol that is similar but not
identical to the MCCP QA Plan.
Wind speed and wind direction are measured with the R.M. Young Wind Monitor (Model
# 05103). Wind speed is sensed by a helicoid propeller that rotates a six-pole magnet that in turn
generates an AC sine wave with a frequency proportional to wind speed. Wind direction is sensed by a
thermoformed plastic vane that transmits its angular position via a coupling to a 10 K ohm poten-
tiometer. The sensor is calibrated at the start and end of each field season, and is subjected to at least
one Quality Control (QC) check during the season. Most sites perform the QC check monthly. Wind
speed is checked via an 1800 rpm motor and a torque disk for starting threshold, and wind direction is
checked versus reference directions.
Temperature and relative humidity are measured with the Rotronic Instrument Model MP-100
combination sensor. A capacitive element senses relative humidity and a resistive device (RTD) senses
temperature. Both transducers are housed inside a Gortex cap and wired to a PC board that outputs
voltages corresponding to the ambient conditions. The sensor probe is housed in a naturally-aspirated
radiation shield. The sensor is calibrated at the start and end of each field season versus a collocated
reference. During the field season, weekly QC checks are performed using a psychron.
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Solar radiation is measured with a Li-Cor pyranometer (Model # L1200S). The sensor uses a
silicon photodiode to measure solar radiation on a horizontal surface. The sensor is calibrated at the
start and end of each field season versus a collocated reference.
Barometric pressure is measured with a Met One, Inc. barometer (Model # 090-B). A piezoresis-
tive diaphragm senses the pressure, and its signal is converted by PC circuitry to a voltage. The sensor
is calibrated at the start and end of each field season against a collocated reference.
A Weathertronics tipping bucket gauge (Model # 6021-B) is used to measure precipitation. Each
0.1 mm of precipitation results in a tip of the bucket. At the start and end of each field season the
sensor is calibrated by applying a known volume of water at a standard rate to the sensor. During the
field season, monthly QC checks are performed in the same manner. This parameter has not been
measured at the Whiteface Mountain peak since the 1988 field season due to high winds.
Meteorological sensors were installed to best represent weather conditions in the vicinity of the
cloud water collector without interfering with the collection process. Most sites locate their cloud water
collector on towers or roofs above the local forest canopy top. Thus, most meteorological sensors are
similarly exposed adjacent to the cloud water collectors. Precipitation and barometric pressure, however,
are measured near the surface. Table 6-2 lists each site's sensor mounting location and height above the
local canopy.
The purpose of the meteorological measurement program is to define the weather conditions at
each site's cloud water collector station. Therefore, these measurements are site-specific and are not
necessarily representative of weather conditions elsewhere. This is especially true for wind measure-
ments, which are strongly influenced by local topography and surface roughness. In addition, the
meteorological monitoring program is designed for growing season (April-October) only.
TABLE 6-2
MCCP Site Sensor Mounting Locations and Height Above Canopy
Height Above Canopy (m)
Site
Howland*
Moosilauke
Whiteface*
Shenandoah-1
Shenandoah-2
Shenandoah-3
Whitetop
Mitchell-1
Mitchell-2
Mitchell-3
Mount
Type**
R
T
R
T
T
T
R
T
T
T
Wind
Speed/Dir.
9.1
9.0
17.0
5.5
8.2
8.2
2.0
11.9
9.0
9.4
Temp/RH
9.1
6.0
16.0
3.6
3.7
3.7
0.0
7.3
6.0
4.9
Pressure
2.0
-10.0
9.0
-10.0
-16.5
-21.9
-4.5
- 7.3
-18.0
-13.2
Precip.
2.0
- 8.0
-11.0
-16.5
-21.9
-3.0
-5.9
-18.0
-15.2
Cloud
Freq.
N/A
4.1
15.0
1.7
N/A
N/A
0.0
5.4
N/A
N/A
a T - from tower
R - above roof platform
b heights are relative to ground level
c not measured since 1988
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THROUGHFALL
Weekly integrated collections of throughfall and bulk or wet-only precipitation were made
during the summer of 1988 at some MCCP sites to compare throughfall inputs to the soil with what
would have been deposited had only rain occurred. Ten 16 cm diameter funnels were deployed randomly
along the cardinal directions from the center of a 0.1 hectare circular plot. Each collector was mounted
approximately 1.5 m above ground level. A nylon wool plug inserted in the neck of the funnels and
replaced weekly prevented large material from falling into the collection bottle attached to the funnel.
Weekly throughfall data were obtained from a proportional composite of at least 10 collectors, and the
precipitation data were from a single collector, either wet-only or bulk. To minimize chemical changes
between collection and analysis, about 1 ml of chloroform was added to each bottle at the beginning of
the week (occasionally preservative evaporation occurs).
A bulk precipitation (BP) collector identical to a throughfall collector is deployed in an open
area. The collection schedule is identical to that of throughfall. The BP is weighed in the field and a
250 ml aliquot is reserved for lab analysis. The wet-only precipitation collector is located adjacent to the
BP collector. An Aerochem Metrics collector is used for wet-only (WO) collection and standard NADP
procedures for buckets are followed. Collection frequency and sample handling are identical to that for
throughfall and bulk precipitation. Laboratory analysis methods and procedures for TF, BP, and WO
are identical to those for cloud water analysis.
The measurement of throughfall has involved a variety of collectors, usually insufficient in
number given the spatial variability in deposition. Buckets, funnels, rain gauges, and troughs of various
sizes have been used (Reigner, 1964; Hamilton and Rowe, 1949; Goodell, 1952). The uniformity of
terrain and canopy dictate the effective collection area needed to adequately estimate throughfall to a
canopy location. The intention is typically to sample randomly, collecting from, canopy features accord-
ing to their relative densities. For example, Helvey and Patric (1965) determined the number of gauges
necessary to sample throughfall to a 5% error depending on rain amount (see Table 6-3).
TABLE 6-3
Mean Number of Throughfall Gauges and Collection Area Needed for 5% Error
Under a Uniform Canopy (from Helvey and Patric, 1965).
Throughfall Total Collection
(cm) # of Gauges Area in m2
< 0.5 46 0.25
0.5-1.0 18 0.06
1/0-1.5 14 0.04
> 1.5 13 0.04
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In a more complex and higher elevation canopy typical of the conditions on Whiteface Moun-
tain, the throughfall variability is larger, requiring more collection area to obtain a 90% confidence level
for a 10% coefficient of variation (Kadlecek, 1989), as shown in Table 6-4. At the upper site, 17
buckets (28 cm diameter) were used, and at the lower site 15 buckets were used. The ratio of highest to
lowest collected volume during a single event ranged from about 2 to 8, with the higher factor applying
primarily to low-volume events. Collectors with larger surface areas, such as troughs, give data with a
smaller range, and those with smaller collection areas produce a larger range. The principles are the
same for any canopy; the actual values depend on the canopy properties.
TABLE 6-4
Throughfall Bucket Collection Area Required for 10% Relative Standard Deviation
in a Complex Canopy on Whiteface Mountain, NY (from Kadlecek, 1989).
Collection Area in m2
Precipitation 1200 m elevation 600 m elevation
(cm) balsam fir beech, birch, maple
< 0.25 2.9 8.8
0.25-0.76 2.4 3.3
0.76-1.52 3.0 0.8
> 1.52 1.3 0.6
Note: These averages were obtained from 8 events at the upper site and 13 events at the lower site.
Similar data from the 1000 m elevation (spruce, fir, beech) based on a regular 25-bucket grid
(bucket diameter of 28 cm, bucket spacing of 5 m) showed that had only three collectors been used,
there was a 90% probability that the three-bucket average would have differed from the 25-bucket
average by more than 30%. This is not to say that 25 collectors were enough, only that too few
collectors can give biased results because the canopy directs the flow unevenly and, in the case of cloud
water, exposed features are the preferred deposition sites. Longer sampling times tend to average out
some of these differences because, as the wind vector changes during events, several segments of the
canopy are sampled. Sampling at the sub-event level is expected to require more collectors for the same
uncertainty discussed here.
Reynolds and Leyton (1963) recommend 20 rectangular troughs with a total collection area of
about 10 m2 to obtain a standard error of 5% to 10%. Eidmann (1959) used trough collectors with an
opening of about 1 m2. One method of calculating how many collectors are necessary is to first deter-
mine by experiment the variation in collection over the study area; then, the number of collectors would
be equal to the squared ratio of the standard deviations to the desired standard error of the mean
(Kittredge, 1948; Helvey and Patric, 1965).
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CLOUD INTERCEPTION
Particles greater than a few urn in diameter (including cloud droplets) are deposited onto
surface by impaction and sedimentation. Impaction is primarily due to the inability of particles in the
airstream to follow rapid changes in air flow; their inertia carries them into surfaces protruding into the
airflow. Sedimentation is the result of the acceleration of particles downward under the influence of
gravity. After a short time, aerodynamic drag balances gravity for small particles, and the particles fall at
a constant velocity. A detailed description of the deposition process is beyond the scope of this section:
the interested reader is directed to Fuchs (1964), Chamberlain (1975), Bache (1979a), and Waldman and
Hoffmann (1987) for further information.
The deposition process for cloudwater is a function of the free stream velocity of the droplets,
the concentration of droplets (liquid water content of the cloud), the droplet size distribution, and the
size, shape and distribution of elements protruding into the flow. While there are several empirical
descriptions of particle deposition to vegetative canopies (e.g., Bache, 1979b; Thorne et al., 1982; Grant,
1983), the actual deposition process is not well understood. One attempt at relating impaction efficiency
(deposition) to these basic physical parameters is (Bache, 1979a):
E.I. = St2/(St + 0.6)2 (1)
where:
E.I. = efficiency of impaction
St = Stokes number, defined as:
St = (Dp - Da)-u-c-dp2/9vdc (2)
where:
Dp = density of the particles
Da = density of air
u = velocity
c = Cunningham slip correction factor
dp = diameter of the particles
v = dynamic viscosity
dc = characteristic length scale of the collecting surface
Stokes calculations have previously been applied to deposition processes by Davidson and Friedlander
(1978). Unfortunately, there are few field data with which to evaluate these relationships. Turbulent
transport over and among non-homogeneous surfaces, the driving mechanism for cloudwater deposition,
requires more research before the process will be fully understood and viable relationships identified.
Shuttleworth (1977) described a simple, steady-state computational model of fog/cloudwater
deposition to, and evaporation from, a uniform vegetation canopy. The model is based on the analogy
of electrical resistance in a direct-current circuit similar to the "big leaf" concept first defined by
Monteith (1965) and subsequently applied to deposition by Wesely and Hicks (1977), Unsworth (1981),
and Hicks et al. (1987), among others.
Lovett (1984) adapted the Shuttleworth model to a balsam fir forest canopy on Mt. Moosilauke,
NH. Lovett included the effects of vertical variation in canopy structure through the construction of a
multiple-layer model in which the vertical turbulent transport of droplets is controlled by the
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aerodynamic resistances between model layers and between the top layer and the air above the canopy.
The droplet size distribution in the model is based on a distribution function described by Best (1951),
with all droplet diameters occurring in the range of 0 to 30 m. While research carried out in forests
has raised questions about the applicability of aerodynamic theory for fluxes over forests (e.g., Stewart
and Thorn, 1973; Thorn et al., 1975; Knoerr and Mowry, 1977), the model has been applied to estimate
the flux of both water and ions in cloudwater to forests (Lovett and Reiners, 1986).
The Lovett model forms the basis of two cloud deposition models used to estimate the con-
tribution of cloudwater deposition to the total deposition budget at the MCCP sites (Mueller 1989;
Krovetz et al., 1989). Modifications to the model have been made for the Whitetop Mountain site and
the Shenandoah site, and manuscripts describing this work are currently in review. The modeling work
at Whitetop has been directed towards spruce forests, while the work at Shenandoah has been directed
towards deciduous forests.
The canopy structure portion of the model had to be generalized to enable computations at
locations other than the original Mt. Moosilauke study site. The spruce version of the model (CDM-S)
allows the input of projected (silhouette) leaf area index which is used to calculate the full-sided leaf
area index. Unless other input data are provided, the spruce model uses the vertical profile of total
surface area index (sum of leaf area index and total non-leaf surface area index) and the distribution of
surface area by canopy component type determined by Lovett for his balsam fir canopy. Canopies
shorter than the Moosilauke canopy studied by Lovett (10.6 m) are assumed to have the full crown of
the Moosilauke canopy with shortened boles. Conversely, the boles are lengthened for canopies of more
than 10.6 m in height, producing a smaller crown-to-total height ratio (a modification consistent with
Whittaker et al., 1974).
The spruce model also allows modifications to both the wind speed profiles and the eddy
diffusivity profiles within the canopy. These modifications are not based on experimental data, but they
can be used for computational comparisons of model output. The spruce model also allows the user to
select the cloud droplet size distribution relevant to the cloud type being modeled if the original
distribution (Best, 1951), is considered inappropriate, and to input a measured cloud liquid water content
if available.
The deciduous version of this model (CDM-D), developed at the Shenandoah site, is a hybrid of
the original Lovett (1984) model, the model described by Bache (1979b), and recent research on
deciduous forest canopies. The distribution of both leaf and twig/branch surface area are determined
using the grid technique of Aber (1979). The deciduous model uses the Best (1951) droplet size
distribution with additional droplet size categories and a mean droplet diameter of 20 m. Liquid water
content can either be entered directly or calculated from an empirical formula relating capture efficiency
of the cloud water collector to liquid water content. Droplet capture efficiency was changed to cor-
respond to the morphology of deciduous leaves; it is computed for planar objects having characteristic
sizes determined from field sampling of fallen leaves (see Bache, 1979a). Wind speed profiles above and
through the canopy are based on work in a deciduous forests by Sigmon et al. (1984), in complex terrain
by Mowry (1980), and basic micrometeorological theory. Exponential decay of wind speed is used above
the canopy, while linear decay is used within the canopy.
The differences in structure between the spruce and deciduous versions of the model result in
different outputs for identical meteorological conditions. While differences in deposition between the
two types of canopies would be expected from theories concerning the capture efficiency of leaves versus
needles (as well as the morphology of coniferous vs. deciduous canopies), separating actual differences in
deposition from model errors is difficult. No comparison of the models has yet been performed, and
very few validation data are available. A priority for future work is to validate and compare the models
to identify differences in deposition between the canopy types.
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Cloud Deposition Model Application
Lovett tested his original model against a limited amount of data collected on Mt. Moosilauke,
NH. The CDM-S has undergone limited testing at Whitetop Mountain, VA; for six cloud events during
1987, mean water flux (0.33 mm/hr) appeared to agree with the mean measured throughfall rate but only
36 percent of the variance was described. Another model test in a new spruce stand resulted in
model-predicted water flux of 0.4 mm/hr compared to a measured throughfall rate of 0.3 mm/hr.
Cloudwater collection rate explained 84 percent of the variance in throughfall rate. These results are
not conclusive because of uncertainties in the inputs (such as forest stand characteristics, liquid water
content, and windspeed) (Mueller and Imhoff, 1989). Due to limited testing, the uncertainties in cloud
droplet interception modeling are unknown at this time.
The response of the original Lovett cloudwater deposition model to varying meteorological and
canopy structure inputs was summarized by Lovett (1984) and Lovett and Reiners (1986). Some key
results and sensitivities are:
Computed cloudwater flux showed a near-linear dependence on input wind speed.
Cloudwater deposition was proportional to liquid water content (LWC); this
proportionality defined a deposition velocity generally in the range of 10 to 70 cm/sec
for windspeeds of 2 to 20
Cloudwater flux, as simulated by the model, was a complex function of the distribution
of surface area among various canopy component types (e.g., the relative amounts of
needle and twig sizes).
The modeled contribution of droplet sedimentation compared to impaction decreased
rapidly as wind speed increased above 2 m/sec.
Computed cloudwater deposition was sensitive to droplet size distribution.
Cloudwater flux increased locally downwind of a forest edge or gap; edge effects could
raise droplet deposition velocities from about 40 to 200 cm/sec.
Cloudwater flux was insensitive to the vertical droplet eddy diffusivity profile.
The sensitivity of the CDM-S model (used by MCCP) to changes in model parameters has been
examined by Mueller (1989) (see Table II-5). He calculated that the cloudwater flux parameter was most
sensitive to lack of canopy uniformity as represented by a simulated forest edge. Cloudwater deposition
at the edge was computed to be four to five times greater than in a closed forest.
The second most important model parameters, in terms of output sensitivity, were cloud liquid
water content (LWC) and drop size distribution. As with Lovett's original model, the CDM-S and
CDM-D produced computed fluxes that vary linearly with LWC. When the droplet size spectrum is
assumed to co-vary with LWC, model response became non-linear; different forms of the drop size and
LWC relationship result in computed flux differences by a factor of two. The model is sensitive to the
concentration of larger droplets because of collection efficiency and fall speed dependencies on droplet
size.
Droplet capture efficiency (computed from the Stokes equation 2, above) was the third most
sensitive parameter in the CDM-S version of the cloudwater deposition model (it was second in the
CDM-D). Mueller (1989) tested the CDM-S model sensitivity to capture efficiency by varying it across
the range of possible values derived from the uncertainty in the experimental data (Thorne et al., 1986)
and found that deposition varied by 100 percent. Differences between CDM-S and CDM-D result from
different capture efficiency related to morphological differences between conifer needles and deciduous
leaves.
6-16
-------
Other parameters had less influence on cloudwater flux calculations. Evaporation was important
for computed net cloudwater flux when testing model simulations against canopy throughfall data. The
effect of net radiation data on model performance is not known because net radiation was not measured
by MCCP (Mueller, 1989).
The relative insensitivity of the CDM-S to vertical in-canopy profiles of surface area, wind
speed, and eddy diffusivity is fortunate because these parameters are poorly characterized for the MCCP
sites and nearby forests. Of these three parameters, the surface area profile appears most important
because it determines the computed wind speed profile in the CDM-S and it affects estimates of the
vertical turbulent transport rate. Unlike deciduous canopies that tend to have surface area more evenly
distributed in the vertical, spruce-fir canopies tend to have the surface area concentrated in a shallow
crown space. Differences of 10 to 20 percent in the vertical location of the canopy surface area
maximum are relatively unimportant for predicting cloud water deposition with CDM-S. Lovett (1988)
calculated that simultaneously increasing three key model input parameters (cloud liquid water content,
cloud frequency, and wind speed) by 25 percent resulted in an increase from 154 cmfyr to 300 cmfyr
cloud water deposition using the Lovett (1984) cloud droplet interception model. Decreasing these three
parameters by 25 percent reduced the predicted cloud water flux from 154 to 65 cm/yr. Therefore, the
cloudwater deposition model errors for Lovett's sensitivity analysis were linearly related to the product of
the windspeed, liquid water content, and cloud frequency errors. (Uncertainty in these three measure-
ments and in cloudwater chemical composition are discussed in SosyT chapter 6). Lovett concluded that
uncertainty in the input data in addition to extreme variability in time and space make cloudwater
deposition modeling impractical for the estimation of cloud water deposition over hectare spatial scales
or seasonal temporal scales.
DRY DEPOSITION
Dry deposition is more difficult to measure directly than wet deposition, and the corresponding
data set is therefore meager. Methods to measure dry deposition include the use of surrogate surfaces,
mass balances, and micrometeorological techniques.
The use of surrogate surfaces has been reviewed by Stevens (1985). Uncertainties in this method
result from unknown collection efficiencies, unknown relationships of surrogate to natural surfaces, and
exposure of the surrogate surfaces to wet forms of deposition. Mass balance approaches have been used
by Eaton et al. (1978) and Galloway and Whelpdale (1980), among others. In this approach, dry
deposition results as the residual in a mass balance calculation. Therefore, at best, dry deposition
estimates can be as good as the combined variability of the measured parameters. Micrometeorological
techniques include at least five methods (Hicks et al., 1980): (1) the eddy correlation method (the only
direct method for determining mass flux density); (2) the variance method; (3) the eddy accumulation
method; (4) the gradient method; and (5) the modified Bowen ratio method. Micrometeorological
techniques produce more reliable results than surrogate surfaces or mass balance methods, but routine
implementation is difficult and expensive. In the MCCP, models requiring readily available data sets
have been used to estimate dry deposition.
The Inferential Model - Development and Description
Models used to estimate dry deposition take two general forms, both using the concept of
electrical resistance. The more complex form, which considers the vertical distribution of canopy
structure and air transport structure, has been used in models by Murphy et al. (1977), Shreffler (1978),
Bache (1979a & b, 1984), Slinn (1982), and Davidson et al. (1982). The simpler form has often been
referred to as the "big-leaf concept, first introduced by Monteith (1965).
6-17
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The MCCP uses the best available simple modeling tool to convert dry species concentrations to
dry deposition flux densities in adopting the inferential big-leaf model under development by the
ATDD/NOAA. This model conceptualizes the system as an Ohm's law analogy of mass flowing to and
from a surface through a sequence of series and parallel resistances. These include an aerodynamic
resistance that is a function of the turbulent exchange properties of the atmosphere, a quasi-laminar
boundary layer resistance that accounts for the role molecular diffusivity plays adjacent to leaf surfaces,
and a surface canopy resistance that accounts for leaf transfer processes involving stomatal, cuticular, and
mesophyll resistances as well as soil resistances. Simplified models of this type, which simulate canopy
transfer processes as if the canopy was a single or "big leaf, show exchanges driven by the concentration
gradient of the species in question (ozone, sulfur dioxide, particles, etc.) limited by the appropriate set of
resistances in the diffusion pathway. Measured data or submodels must provide estimates of the
resistances and the source or sink strengths. Errors may occur for environments having complex terrain
or patchy surfaces.
When using big-leaf models for water vapor and sensible heat exchange (e.g., Stewart and Thorn,
1973; Jams et al., 1976), internal leaf resistance is negligible. For other gases, such as carbon dioxide
and air pollutants, leaf sinks or sources are taken into account by defining a virtual resistance to a zero
sink or by using a relationship between the environment and the source or sink strength. Such methods
have been used to predict carbon dioxide exchange (Waggoner, 1969; Sinclair et al., 1976). For most
atmospheric pollutants, the zero-sink case is appropriate, and a deposition velocity is defined as the
inverse of the sum of the resistances (Hicks et al., 1987). Such models have been used to predict
pollutant flux (Matt et al., 1987; Hosker and Lindberg, 1982; Unsworth, 1980; Wesely and Hicks, 1977).
Currently, estimations of resistance come from climatological and physiological data. Hicks et
al. (1985) propose estimating aerodynamic resistance from the standard deviation of the horizontal wind
direction and mean horizontal wind speed. Based on work by Brutsaert (1975) and Garratt and Hicks
(1973), they also propose the quasi-laminar boundary layer resistance as a function of the Schmidt and
Prandl numbers. Canopy surface resistance is the most difficult to estimate where the primary transfer
resistance is through the stomata but may also include cuticular and mesophyll resistances. An addition-
al complication arises when resistances vary through the canopy depth and a weighted average value for
the big leaf must be derived. In some experimental work, the canopy surface resistance is evaluated as a
residual by measuring the flux, the total resistance, the aerodynamic resistance, and the quasi-laminar
boundary layer resistance (Baldacchi, 1987). In the model, gross stomatal resistance is combined in
series with gross mesophyll resistance, while cuticular resistance is combined in parallel with these, and
the gross canopy resistance is determined by weighing with the leaf area index (Hicks, 1985). A review
of stomatal resistance concepts is presented by Jarvis (1971). Gross stomatal resistance can be modeled
as a function of PAR (Baldacchi et al., 1987; Burroughs and Milthorpe, 1976) as mediated by the effects
of water stress, humidity, and temperature (Rodriguez and Davies, 1982; Fisher et al., 1981; Jarvis, 1976).
Mesophyll and cuticular resistances, although measured experimentally, have yet to be adequately
modeled.
6-18
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SECTION 7
DESCRIPTION OF DATA BASE AND QUALITY ASSURANCE PLAN
DESCRIPTION OF DATA BASE
The Data Management Center (DMC) of the Fleming Group in Albany, NY, is the central
collection, processing, analysis, and distribution point for data collected at MCCP sites and laboratories.
DMC activities include data acquisition and entry, storage and documentation of data files, data valida-
tion, reduction, and certification, report generation and distribution, data archiving and analysis, and
model testing and evaluation. Types of data handled are:
physical measurements (e.g., presence of cloud, precipitation, cloud LWC)
meteorological measurements (e.g., temperature, wind speed and direction)
aqueous phase measurements (e.g., cloud, precipitation, and throughfall chemistry)
gas phase measurements (e.g., ozone, sulfur dioxide, hydrogen peroxide)
ancillary data (e.g., site latitude, longitude, and elevation).
These data are stored in an ORACLE relational database. The computer hardware is a DEC
VAX 11/750 with the VMS version 4.1 operating system. The database is implemented using ORACLE
version 5.0.20. All programming applications are written in C using the Digital version 2.1 compiler.
MCCP data are available from the Data Management Center by written request to The Fleming
Group, 55 Colvin Ave., Albany, NY 12206. Timeseries data sets have been developed for the analysis of
multiple parameters in time sequences. The MCCP data are organized into hourly records containing all
measurements available for that hour, including meteorological, gas, physical, and chemical data. The
data are further organized by site, month, and year, and are available on floppy disk or magnetic tape.
These data sets are available for 1986 to 1988 data.
INTERNAL QUALITY ASSURANCE
Internal quality assurance/quality control (QA/QC) for the MCCP is coordinated and managed
by the Fleming Group, in Albany, NY. QA consists of:
development of standard operating procedures (SOPs) and quality assurance plans;
preparation of training sessions and site technician certification;
writing annual QA/QC summaries;
conducting system audits; and
• data validation and certification.
Standard quality control practices for the field (i.e., methods of tracking performance) include
training (by on-site personnel), station checks, station logs, zero/span checks, precision measurements,
and calibrations. All station checks, routine measurements, and record keeping follow the MCCP SOP
and QA plan. Table III-l summarizes the data quality objectives for the MCCP.
Additional quality control is provided by a site QA coordinator who verifies that monitoring
procedures are followed, checks all instrument calibration records, and confirms any effect of problems
on the final data. The network QA officer informs the project manager of problems at each site.
7-1
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The QA office also monitors laboratory quality control procedures for both the on-site laborato-
ries and a central analytical laboratory (CAL), the Illinois State Water Survey (ISWS), that analyzes
samples from all the sites. The latter is the same laboratory that analyzes the NADP/NTN rain samples.
The CAL established the QA/QC protocols for the laboratories and prepares QC check solutions.
Performance of site labs with respect to CAL are evaluated by split sample comparisons. A
split is a sample that has been divided into two aliquots in the field. The results from the analyses of
these split samples are used to determine the precision between the two labs. Table III-2 summarizes
the splits analysis results for 1986, 1987, and 1988.
An internal systems audit for each site is performed annually by the QA Office. Inspection
includes evaluation of all aspects relevant to the goals of the program and adherence to the Project QA
Plan. Upon completion, a report is written to describe the results of the audit and recommending
actions for improvement.
Quality Assurance reports to management have been prepared on an annual basis. Copies of
these reports may be obtained from The Fleming Group or the EPA
7-2
-------
APPENDIX A
EUROPEAN MONITORING
We present this review European cloud water chemistry to provide a context for viewing USA
and Canadian data. Few true "networks" exist; site specific data for Sweden and Italy are included for
comparison with FRG and North American data.
GERMANY
Since 1916, several researchers in the Federal Republic of Germany have collected fog/cloud
water using string collectors (Linke, 1916; Rubner, 1931; 1935; Grunow, 1953; 1957; 1958; Baumgartner,
1958a; 1958b). The interest in fog/cloud chemistry has grown in recent years primarily in response to an
increase in forest damage. It has been hypothesized that chemical species in fog/cloud water intercepted
by forest canopies contribute to that damage. Hence, several institutions developed a variety of fog/clo-
ud collectors. To ensure data compatibility and quality, in 1986 the Federal Ministry for Research and
Technology (BMWFT) funded a comparison of collectors at the Center for Environmental Research,
University of Frankfurt (Enderle and Jaeschke, 1988).
Although there is currently no cloud monitoring network in Germany, several groups have
initiated limited field experiments. Of special interest are cloud chemistry data obtained over an
extended period of time, such as reported by the University of Frankfurt group (Schmitt, 1989), the
German Weather Service in Hamburg (Kroll and Winkler, 1989), and the University of Bayreuth
(Trautner, 1988).
The Frankfurt group obtained cloud samples from Little Feldberg Mountain, a region close to
urban centers and heavily industrialized complexes, including chemical factories. These results are shown
in Table Al-1. The Weather Service group operated five mountain sampling sites during an 18-month
period from October 1986 through May 1988: Hohenpeissenberg (HP), Kahler Asten (KA), Wasserkuppe
(WK), Grosser Arber (GA), and Schauinsland (SL). Each fog event contributed one sample for
chemical analysis. These values, presented in Table Al-2, were standardized to a uniform liquid water
content (LWC) of 0.2 g/m3 to avoid additional variability due to different LWCs.
TABLE Al-1
Arithmetic mean, maximum, and minimum concentrations in 410 cloud/fogwater samples
for the Calls of 1983 - 1986 in Kleiner Feldberg/Taunus, 15 km north of Frankfurt
Values are in
Mean Maximum Minimum
831 5620 87.4
NO/ 778 7067 28.6
Cl- 243 2257 17
NH^+ 1197 5210 55.4
H+ 158 5011 0.0126
A-l
-------
TABLE Al-2
German Weather Service Mountain Sites (Active impactor-type collector)
All values are normalized to LWC of 0.1
Station
Ion Species
Oteq/L)
H+
NO/
NO/
# of events
LWC (g/m5)
HP
151
110
102
172
381
0.025
KA
200
219
229
321
126
0.057
WK SL
43
108
82
139
85
73
47
133
20 22
0.055 0.042
GA
148
260
223
310
195
0.127
The Bayreuth group (Trautner, 1988) collected a total of 25 weekly samples at a mountain site
in the Bavarian Fichtelgebirge (Wuelfersreuth). Each fog event yielded one sample, and no attempt was
made to differentiate precipitating and non-precipitating events. The mean ion concentrations are listed
in Table Al-3.
TABLE Al-3
Weekly Fog/Cloud Water Samples Obtained with Passive String Collector
at Wuelfersreuth (Fichtelgebirge)
September 1984 - March 1986 (Fall/Spring only).
LWC (g/m5
Ion Species (/teq/L)
so/2-
NO/
Mean
3.9
336
334
253
Standard
Deviation
4.0
191
192
149
Maximum
3.4
0.137
892
936
569
Minimum
6.5
0.003
65
68
44
Appreciable regional difference sin the chemical composition of cloud water have been observed
for these mountain measurements. The mean concentrations varied greatly not only among different
stations but also within stations. Since each investigator adhered to his/her own standard operating
procedures for cloud/fog collection and analysis, it is difficult to prepare a quantitative summary from the
results to date in Germany. It is clear, however, that cloud/fog water was enriched compared with
precipitation water for all major ions (including those not summarized in Tables Al-1 through Al-3).
The results show that high-elevation forests were exposed to substantial concentrations of chemicals in
clouds/fogs.
A-2
-------
ITALY
A field test to investigate microphysical and chemical characteristics of fog was organized by
FISBAT (Istituto Perlo Studio dei Fenomeni Fisici e Chimici della Bassa e Alta Atmosphera) in the
eastern Po Valley during February and November of 1984 (Fuzzi et al, 1988). Twelve American and
European institutes participated (Atmospheric Sciences Research Center, Albany, NY (USA); Atlanta
University, Atlanta, GA (USA); Italian National Electricity Board (Italy); Lawrence Berkeley Laboratory,
Berkeley, CA (USA); Technical University Vienna (Austria); University of Bologna (Italy); University of
Frankfurt (FRG); University of Padova (Italy) and University of Vienna (Austria). Rotating string
collectors collected fog on an hourly basis. Twenty samples were obtained during February 1984, and 87
samples from six events were obtained during November 1984. The mean, maximum, and minimum
concentrations for the major chemical components in the Po Valley fog are presented in Table Al-4.
The average anion to cation ratio was 0.96, an indication that no important constituents were missed.
Four ions accounted for most of the ionic strength of the fog water solutions: H+, Nrfy+, NO/, and
SO^2'. The average liquid water content (LWC) was 0.08 g/nv3 (maximum 0.29 g/nr*) measured by a
high-volume filter technique.
TABLE Al-4
Hourly Fog Samples Obtained with Rotating String Collectors in Po Valley, Italy
February and November, 1984.
Mean Maximum Minimum
Feb Nov Fcb Nov Feb Nov
H+ 200 160 3600 1200 10 1
SO^- 1000 900 6300 2100 350 150
NO/ 1100 900 8200 3300 290 80
NH^+ 2100 1400 8100 4200 700 300
H2O2 < 0.1
LWC (g/m5) 0.08 0.29
SWEDEN
A ground-based passive string collector sampled water" from stratiform clouds for approximately
five weeks during the summers of 1983 and 1984 in the mountains of central Sweden (Areskutan, 1250
m asl; Ogren and Rodhe, 1986). These measurements were considered representative to air arriving over
central Scandinavia. Cloud liquid water content was measured only in 1984, using a heated-rod impactor
King probe (King et al., 1978). A total of 179 cloud water samples (resolution less than one hour) were
obtained and a wide range of concentrations was encountered; for example, sulfate concentrations ranged
from 1 to 1600 neq/L. Table Al-5 shows the mean ion concentrations classified into four air mass
arrival sectors. Transport of air from the North Atlantic Ocean (NW) was associated with low concentra-
tions, while high concentrations occurred with transport from industrial regions in Europe (S). Long-ra-
nge transport appears to be the primary factor controlling the chemical composition of cloud water at
the sampling site in central Scandinavia.
A-3
-------
TABLE Al-5
Mean Ion Concentrations in Hourly Cloud Water Samples from Four Trajectories
for Areskutan, Sweden, 1250 m asl
A Passive String Collector Sampled Precipitating and Non-precipitating Clouds
in the Summers of 1983 and 1984.
Trajectory
NE NW W S
Ion Species (jieq/L)
H+ 33 13 38 370
34 6 ' 30 700
max 150 max 19 max 220 max 930
NO/ 9 2 10 68
NH4+ 17 0.5 1 NA
LWC Averaged over all directions = 0.16 g/nv*
No. of Samples 47 41 33 4
CANADIAN MONITORING
There are areas of forest at elevations above 600 m scattered throughout southern Quebec, along
the Gaspe Peninsula and in northern New Brunswick. Because higher elevation forests show
unexplained damage symptoms in central Europe and the eastern United States, the Chemistry of High
Elevation Fog (CHEF) program was started in late 1985 to measure wet and dry deposition as well as
the meteorological conditions at several higher altitude sites. The objectives of the CHEF program are
similar to those of the Mountain Cloud Chemistry Project (MCCP) in the USA (Schemenauer, 1986;
Schemenauer et al., 1988; Schemenauer and Winston, 1988). The CHEF program operates 12 months a
year on two mountains (Mt. Tremblant and Roundtop Mountain) and for four months on a third
mountain (Mt. Epaule). Paired fog/cloud water samples are collected with a passive string collector that
is very similar to the MCCP cloud water collector. The program is designed to sample every fog event
on each day of the year. The sampling periods can vary from 1 to 24 hours depending on operator
availability. Because an operator is at the field station only eight hours per day, when fog is expected
overnight a pair of collectors are exposed at the end of the afternoon and the samples collected the next
morning.
The CHEF program is still in the initial stages of data analysis and interpretation. Cloud/fog
samples at Mt. Morency were collected between 25 June and 24 September 1986. The data are
presented as sample means in Table Al-6. The concentration of all ions was 10 to 20 times higher in
non-precipitating cloud water than in precipitation. The precipitating cloud/fog samples had
intermediate values but more closely resembled the precipitation data. The dominant cations were H+
and NH^+ and the dominant anions SO/' and NO/. Fog/cloud samples from Roundtop collected
between 1 May and 25 September 1986 are also shown in Table Al-6. Note that the small number of
A-4
-------
samples precludes any comparison of precipitating and non-precipitating clouds without more recent
CHEF work.
The principal CHEF sampling locations are at altitudes near the typical cloud base heights for
southern Quebec (845 to 970 m). Thus, the main depth of the cloud is usually above the sampling
location and the likelihood of precipitating being mixed with cloud events is high. Any indication of
precipitation at the field sites during the exposure of the passive fog collector results in the sample being
classified as a "precipitation fog/cloud" event. The CHEF data are in agreement with those reported for
northeastern MCCP sites. Schemenauer (1986) reported that the CHEF monitoring sites in Quebec are
in cloud approximately 44% of the year, with lower elevations (about 500 m) experiencing clouds for
about 23% of observations.
Schemenauer et al. (1988) collected paired samples to screen the data for possible
contamination. These results describe the combined experimental precision related to uncertainties in
cloud water collection (ASRC-type passive sampler), chemical analysis, and handling procedures. About
3% of the CHEF samples were eliminated due to a "significant" difference in concentration between the
sample pairs. The remaining 17 pairs of samples had a median difference of 4 neq/L for sulfate (mean
total concentration was 199 jteq/L) and 1.9 jteq/L for nitrate (mean concentration was 65 jieq/L); the
median difference was about 2% of observed concentrations.
Except for the length of the sampling period the CHEF and Mountain Cloud Chemistry Project
(MCCP) protocols are similar. Samples from MCCP and CHEF have been exchanged for comparisons
of analyte concentrations. It is anticipated that for non-precipitating cloud water that the CHEF and
MCCP cloud water concentration data are directly comparable.
TABLE Al-6 .
Mean Ion Concentrations at Two Canadian CHEF Sites in 1986
(from Schemenauer and Winston, 1988).
Morency Roundtop Roundtop
(970 m) (970 m) (845 m)
NP* P NP P NP P
# samples 7 20 3 57 17 81
pH 3.42 3.66 4.52 3.65 3.89 3.71
Ion species (iieq/L)
H+
SOj2'
NOy
NH,+
383
522
87.5
215
218
301
51.1
141
29.9
44
21.9
52.4
224
244
104
116
129
227
72.9
149
197
248
104
125
a NP = non-precipitating clouds
N = precipitating clouds
A-5
-------
APPENDIX B
DATA REPORTS
This section lists the principal data reports and publications from MCCP, ISF, and CHEF cloud
water routine monitoring activities. A brief summary of each is provided.
Mohnen and Kadlecek (1989) presented typical winter and summer events to contrast
time-dependent histories of chemical concentrations for the two seasons. During summer, sufficient
hydrogen peroxide (H2C>2) existed to oxidize available SC>2 to SO^, temporarily depleting the H2C>2. In
winter, H2O2 and oxidation rates were low; thus, sulfate concentrations in cloudwater were generally
independent of SC>2. A chemical cloud climatology for Whiteface Mountain was presented for data from
1982-1987. Summer mean hydrogen ion concentrations ranged from a low of 174 /ieq/L in 1987 to a
high of 331 2 were higher in summer than in fall (0.8 versus 0.15 ppb) and were strongly correlated with ozone,
temperature, and dew point. Daytime H2C>2 exceeded nighttime values by 26%. Cloudwater acidity data
are not presented here. During spring, summer, and fall of 1986 at Whitetop Mountain, the mean
cloudwater [H2O2] was 26 jimol/1 (for 100 samples), while the mean rainwater H2C>2 was 10 ionol/1 (28
samples). A maximum aqueous H2C>2 of 247 /imol/l was observed, the highest value reported to date in
the literature; 13% of summer cloud samples showed greater than 120 junol/l ^C^. Comparison of
rain and cloud H2C>2 during periods of poor vertical mixing in the atmosphere suggested that
levels aloft exceed those at the ground.
B-l
-------
Mueller and Weatherford (1988) computed cloud deposition on Whitetop Mountain, VA for 26
cays in the spring of 1986. Using Lovett's model (Lovett, 1984), the computed cloud deposition for the
study period. The cloudwater SO^ flux was between 5.3 and 9.1 kg/ha/mo, while NOj flux was between
2.8 and 5.4 kg/ha/mo. The ranges reflect projected variation in unmeasured model input data.
Lindberg et al. (1988) used Integrated Forest Study (IPS) data to estimate cloud, precipitation,
and dry deposition at a high-elevation site in the Great Smoky Mountains. Cloudwater SO^2' and NO/
deposition were estimated to be 7.2 and 2.2 kg/ha/mo, respectively, both two to five times greater than
estimates from a nearby low-elevation site for January-April 1986. This is the only published paper from
the IPS cloud water studies.
More recent deposition estimates from IPS appear in discussions by Lovett, Knoerr and Conklin,
and Ragsdale in a draft summary of the IPS that was edited by Lindberg and Johnson (1989). This
report does not present cloud water concentrations and presents cloud deposition only in the form of
graphs. Cloudwater H+ deposition at these two sites was estimated to be 30% to 40% of total H+
deposition. The IPS scientists concluded that the primary sources of uncertainty in cloudwater
deposition were immersion time, cloudwater amount, and ion concentrations.
Other than Lovett's original work at Mt. Moosilauke, the best documented estimates of cloud
water chemical exposure and deposition are from the Mountain Cloud Chemistry Program (MCCP) by
Mohnen and co-workers (1988a; 1988b; 1988c). The CDM-S and CDM-D models (Mueller, 1989;
Krovetz et al., 1989) were used to predict deposition to the spruce-fir forests on five mountains in the
eastern USA. Sigmon et al. (1989) and Joslin et al. (1988) estimated deposition at Shenandoah and
Whitetop Mountain, VA, from canopy throughfall measurements.
B-2
-------
APPENDIX C
SUMMARY OF METEOROLOGICAL DATA
FOR THE MOUNTAIN CLOUD CHEMISTRY PROJECT SITES
1986 - 1988
-------
SUMMARY OF METEOROLOGICAL DATA
SITE: HOWLAND FOREST
Periods of Record
Average Temperature (C)
1987: Apr 11 - Nov 11
1988: Mar 25 - Nov 15
1987
1988
Max
Min
Mean
Average
1987
1988
Mean
APR MAY
8.4 12.1
5.4 13.2
25.6 31.1
-5.4 -2.8
6.6 12.7
Relative Humidity
59.4 57.3
68.9 62.0
65.1 59.6
JUN
16
17
35
1
17
(%)
67
66
67
.9
.0
.9
.6
.0
:
.8
.2
.0
JUL
18
21
33
4
19
73
77
75
.8
. 1*
.0
.9
.7
.6
.5*
. 1
AUG
17.
20.
• 34.
3.
18.
68.
74.
71.
9
0
2
4
9
1
1
0
SEP
13.
13.
28.
-2.
13.
74.
74.
74.
5
7
7
5
6
4
3
3
OCT
7.
6.
26.
-5 .
7.
72.
73.
72.
5
4
9
0
0
2
6
9
Total Precipitation (mm)
1987
1988
Mean
Average
1987
1988
Max Hr.
Mean
55.1 62.7
48.5 13.0
51.1 37.8
Wind Speed (m/s) :
2.8 3.1
3.2 3.1
8.9 10.9
3.1 3.1
Resultant Wind Direction
1987
1988
Mean
Average
1987
1988
Max
Mean
Average
1987
1988
Max
Min
Mean
30.5 258.1
6.3 243.8
15.8 250.9
Solar Radiation (
333.1* 237.5
242.2* 299.0*
869.0 906.3
277.4 263.3
Pressure (mB ) :
1013.8 1012.9
1003.8 1010.8
1025.2 1026.2
973.4 994.2
1007.8 1011.9
54
47
51
2
2
8
2
.9
.2
.0
.7
.8
.4
.7
53
68
59
2
1
6
2
.6
. 8*
.6
.4
. 8*
.7
.2
25.
121.
73.
2.
2.
9.
2.
4
9
6
5
0
0
o
146.
41.
93.
2.
2.
7 .
2.
3
1
7
6
6
Q
6
56.
84-.
70.
2.
2.
8.
2.
1
O
•-J
2
6
6
8
6
(degrees ) :
241
290
285
W/m2
220
340
956
270
1007
1004
1019
987
1006
-- No Data, * Data Recovery
.4
.4
.9
):
.5
.7*
-8.
.3
.8
.5
.6
.2
.2
50%
220
243
230
197
182
954
191
1007
1009
1017
994
1008
.6
. 9*
.0
.6
.0*
.3
.4
.2
.5*
.7
.8
. 1
to 85%,
257.
234.
245.
213.
175.
880.
195.
1007,
1009.
1020.
995,
1008
0
4
7
9
,5
5
,2
.7
.4
.3
.8
.6
264.
264.
264.
140.
203.
801.
167.
1008,
1010.
1026,
984.
1009
2
5
4
3
,9*
7
,2
.3
.5
. 0
,3
.4
# Data Recovery
233.
244.
239.
99.
110.
658.
104.
1010.
1011.
1028.
988.
1010.
9
0
0
8
2*
5
2
.2
4
.6
1
.8
f < 50%
-------
SUMMARY OF METEOROLOGICAL DATA
SUBSITE: MT. MITCHELL 1
Periods of Record:
Average Temperature (C):
1986
1987
1988
Max
Min
Mean
Average
1986
1987
1988
Mean
APR MAY
11.6*
12.8
10.8
20.5
2.0
11.7
Relative Humidity
__
90.2
71.4
79.6
1986;
1987
1988:
JUN
13.
13.
13.
22.
0.
13.
(%):
79.
84.
73.
79.
: May 12
: May 14
: May 10
JUL
3
3
6
1
4
4
7*
4
3
1
14
15
14
23
6
14
82
84
84
83
.0*
. 1
.8
.5
. 1
.8
. 3*
.4
.2
.9
- Nov 20
- Oct 22
- Oct 1
AUG
12
14
15
23
-0
13
90
88
88
88
.2
.6
.2*
.5
.6
.9
.0
.0
.1*
.7
SEP
11
10
12
19
2
11
87
90
88
89
.6
.3
. 0*
.9
.2
.3
. 9*
.8
.5*
.2
OCT
7
4
-
17
-10
6
77
60
-
70
.3
.8
-
.2
.2
.2
.9
.7
-
.5
Total Precipitation (mm):
1986
1987
1988
Mean
Average
1986
1987
1988
Max Hr.
Mean
Resu Itan
1986
1987
1988
Mean
Average
1986
1987
1988
Max
Mean
Average
1986
1987
1988
Max
Min
Mean
57.2
79.2
• -- 26.9
52.4
Wind Speed (m/s):
6.7
4.2
5. .6
21.0
5.6
t Wind Direction
271.9
266.5
284.6
275.0
Solar Radiation (
165.3
162.6
301.1*
1014.8
226.8
Pressure (mB ) :
807.0
810.4
806.1
817.3
798.4
807.7
2.
145.
36.
61.
6.
6.
5.
19.
6.
3
3
8
6
1
5
8
2
1
0
51
96
58
8
5
5
21
6
. 0*
.3
.8
.5
. 3*
.3
.5
.6
.0
4
47
105
49
6
6
5
20
6
.3
.2
. 2*
.4
.4
.5
.6*
.0
.2
22
306
145
161
6
6
6
18
6
.9
.6
.3*
.0
.4
.6
.5*
.9
.5
186
3
-
123
7
7
-
19
7
.9
.3
-
.8
. 7
.4
-
. 9
.6
(degrees) :
293.
289.
292.
291.
W/m2)
220.
231.
355.
1075.
272.
808.
808.
808.
818.
796.
808.
3
7
6
9
6
5#
5
9
1
5
5
5
7
9
5
296
293
270
285
206
-
316
971
266
809
810
811
817
801
810
. 2*
.4
.7
. 1
. 1*
—
. 6*
.3
.7
.4*
.9
.3
. 1
.5
.7
298
349
245
300
140
-
285
946
192
812
810
810
823
802
811
.9
.8
.4*
.8
.9
-
.9*
.6
.0
.8
.2
.3*
.6
.2
.1
284
83
265
206
150
-
269
910
193
815
807
808
828
794
810
.8
.4
.5*
.9
.4
-
.5*
.7
.2
.8
.3
. 9*
. 1
.7
.8
295
297
-
296
135
-
-
860
135
811
804
-
821
793
808
1—1
1
-
• -
c,
-
-
3
• 1
. 3
. 6
-
.4
.0
. 6
-- No Data, * Data Recovery 50% to 85%, # Data Recover < 50%
-------
SUMMARY OF METEOROLOGICAL DATA
SUBSITE: MT. MITCHELL 2
Periods of Record
Average Temperature (C)
1986: Jun 28 - Nov 20
1987: May 18 - Oct 23
1988: May 12 - Sep 30
1986
1987
1988
Max
Min
Mean
Average Re
1986
1987
1988
Mean
Total Free
1986
1987
1988
Mean
APR MAY
— —
15.1
12.3
19.7
5.0
13.4
JUN
17.5
15.6
15.6
24.6
2.2
15.7
JUL
17.2*
17.6
17.0
25.0
8.8
17.3
AUG
—
17.0
17.5
26.3
10. 1
17.3
SEP
14.5*
12.7
13.4
22.1
3.9
13.4
OCT
8.7
3.3*
—
21.0
-7.9
8.0
lative Humidity (%):
__
80.9
66.4
72.3
ipitation (mm)
__
40.6
19.3
28.0
73.8
83.2
67.7
75.1
:
11.4
121.9
40.6
78.7
71. lit
77.6
78. 1
77.2
200.4
54.1
95.8
116.4
--
83.2
83.0
83. 1
--
58.9
122.2
90.5
81.3
87.3
84.5
67.2
23.0*
309.6
126.5
170.5
__
56. 6*
56.6
164.6
0.04*
—
142.4
Average Wind Speed (m/s):
1986
1987
1988
Max Hr.
Mean
Resultant
1986
1987
1988
Mean
Average So
1986
1987
1988
Max
Mean
__
2.8
4.3
12.4
3.7
Wind Direction
__
257.5
261.0
259.6
lar Radiation
__
159.5
229.2
1027.5
200.6
3.3
3.9
3.3
13.0
3.6
(degrees
287.9
277.9
305.6
291.6
(W/m2):
187:7
213.9
252.9
1027.5
231.8
3.8
3.6
3.9
16.6
3.8
):
284.9
281.0
260.8
275.5
221.8
201.8
208.2
1052. 1
210.8
3. 1*
3.7
3.2
11.6
3.4
290. 1*
283.4
260.1
274.8
155.0*
177.7
193.2
979.6
180.3
3.9
4. 1
3.6
13.9
3.9
264.8
251.3
255.8
257. 1
170.2
157.5
152.4
954 . 2
159.9
4.2
5.3*
12.1
4.3
266.5
286.6*
—
269.2
153.0
204. 1*
--
861.9
159.9
Average Pressure (mB):
1986
1987
1988
Max
Min
Mean
__
824.9
820.1
839.3
812.1
822.1
828.6
822.6
823.1
832.8
812.2
823. 1
831.8
825.0
826.3
838.6
815.6
827.7
831.5*
824.5
825.6
835.5
817.6
826. 1
832.5
821.7
824.5
837.5
809.6
826. 1
829.3
817.7*
--
809.6
838.8
827.7
— No Data, * Data Recovery 50% to 85%, * Data Recovery < 50%
-------
SUMMARY OF METEOROLOGICAL DATA
SUBSITE: MT . MITCHELL 3
Periods of Record
Average Temperature (C)
1988: May 14 - Sep 29
1988
Max
Min
Average
1988
APR MAY
17.2
28.2
2.3
Relative Humidity
68.4
JUN
19
31
4
(%)
71
.7
.9
.3
.4
JUL
21.
33.
9.
80.
AUG
6
0
2
2
22
33
12
84
.0
.8
.3
. 1
SEP
18
28
6
85
. 1
.7
.9
.9
Total Precipitation (mm):
1988
Average
1988
Max Hr.
Result an
1988
Average
1988
Max
Average
1988
Max
Min
22.1
Wind Speed (m/s):
1.4
6.1
t Wind Direction
193.8
Solar Radiation (
245.4
1060.7
Pressure (mB ) :
927.3
934.9
920.3
64
1
4
.3
.2
.3
105.
1.
5.
9
1
4
. 71
1
4
.4
.0
.2
117
1
3
.3
. 1
.7
(degrees ) :
222
W/m2
258
1015
929
940
917
.9
):
.9
.8
.5
.3
.8
198.
222.
987.
932.
941.
923.
7
5
2
0
0
7
210
204
957
930
942
921
.5
.6
.9
.6
.9
.7
211
159
892
930
940
917
.8
.6
.4
.9
.3
.3
OCT
-- No Data, * Data Recovery 50% to 85%, # Data Recovery < 50%
-------
SUMMARY OF METEOROLOGICAL DATA
SITE: MT. MOOSILAUKE
Periods of Record
Average Temperature (C)
1986: Jul 12 - Oct 22
1987: Apr 9 - Oct 15
1988: Jun 2 - Oct 18
1986
1987
1988
Max
Min
Mean
Average
1986
1987
1988
Mean
APR MAY
__
6.5 9.9
__
21.7 25.7
-4.5 -3.1
6.5 9.9
Relative Humidity
__
65.4 66.2
— —
65.4 66.2
JUN
—
14.0
14.1*
28.6
2.4
14.0
(%):
--
77.4
61.6*
70.5
JUL
15.9
18.0*
18.9
28.7
4.5
17.8
85.4
80.9*
74.9
79.8
AUG
13.5*
14.7
17.1
28.7
1.2
15.3
82.1*
77.3
82.6
80.6
SEP
9.8
10.9
10.8
20.8
-0. 1
10.5
79.8
84.6
79.3
81.3
OCT
4.7
4.8
4.2
19.4
-5.9
4.6
76.8
76.7
86.0
79.8
Total Precipitation (mm):
1986
1987
1988
Mean
Average
1986
1987
1988
Max Hr.
Mean
Resultan
1986
1987
1988
Mean
Average
1986
1987
1988
Max
Mean
Average
1986
1987
1988
Max
Min
Mean
__
24.6 30.2
__
24.6 30.2
Wind Speed (m/s):
--
4.6 4.6
— —
13.3 13.3
4.6 4.6
t Wind Direction
__
53.5 307.7
__
53.5 307.7
--
163.8
26.4
100.9
--
4.7
4.9*
17.8
4.8
(degrees^
--
306.5
307.5*
306.9
83.3
—
68.8*
74.4
3.2
3.4*
3.3
13.0
3.3
) :
312.0
312.2*
303.4
308.8
101.6
128. 5#
139.7
125.2
4. 1*
4.1
4.0
15.4
4.1
265.0*
305.9
288.6
294.8
82.3*
141.0
51.8
81.4
4.4*
4.7
5.0
15.4
4.7
--
313.4
296. 1
304.8
23.9
46.7
9.1
25.2
4.5
5.3
4.6
21.3
4.8
311.6
327.9
273.7
303.4
Solar Radiation (W/m2):
__
313.1* 227.3
— —
890.3 923.1
313.1 227.3
Pressure (mB ) :
— —
905.5 908.0
— —
915.2 918.3
880.5 892.8
905.5 908.0
--
197.1
259.5*
966.0
224.3
--
905. 1
904.3*
915 .8
887.3
904.8
176.9
209.7*
226.1
968.9
207.3
907.8
908.8*
909.7
919.8
894.4
908.9
183.6*
208.5
225.3*
994.4
206.8
908. 1*
908.4
909.2
918.3
892.0
908.6
144. 1
125.6
151.7
816.8
140.3
908.4
907.3
908.8
921.7
887.1
908.2
102.0
iio.o-
65.9
703.5
92.2
908.0
904.7
907.7
921.0
886.3
906.2
-- No Data, * Data Recovery 50% to 85%, tf Data recovery
50%
-------
SUMMARY OF METEOROLOGICAL DATA
SUBSITE: SHENANDOAH 1
Periods of Record
Average Temperature (C)
1986: Apr 24 - Nov 24
1987: Apr 20 - Nov 15
1988: Apr 14 - Nov 3
1986
1987
1988
Max
Min
Mean
Average
1986
1987
1988
Mean
APR MAY
15.1 14.0
9.6 15.0
6.7 13.7
23.6 27.0
-1.9 -0.4
9.2 14.2
Relative Humidity
48.9 68.4
64.4 64.6
55.4 72.0
57.0 68.5
JUN
18
19
17
29
4
18
(%)
61
68
66
66
. 1#
.4
.4
.8
.2
.3
. 8#
.2
.2
.2
JUL
20
21
21
33
6
21
84
69
69
71
. 2#
. 8*
.6
.9
.5
.5
. 3#
. 9*
. 1
.4
AUG
17
20
21
32
4
19
85
69
72
76
.0
.3
.0
.5
.0
.4
.5
.4
.7
.0
SEP
15
16
14
26
1
15
80
75
79
78
.2
.7
.9
.4
.5
.6
.7
. 2*
.3
.5
OCT
10
8
6
25
-4
8
69
59
64
64
. 1
.2
.4
.4
.0
2
.3
.3
.3
. 2
Total Precipitation (mm):
1986
1987
1988
Mean
Average
1986
1987
1988
Max Hr
Mean
2.3 123.7
19.3 154.2
10.9 217.9
11.9 165.3
Wind Speed (m/s):
5.7 5.0
5.5 4.0
6.4 4.2
15.2 14.1
6.0 4.4
Resultant Wind Direction
1986
1987
1988
Mean
Average
1986
1987
1988
Max
Mean
Average
1986
1987
1988
Max
Min
Mean
301.1 265.0
12.1 259.0
294.1 214.6
208.1 246.2
Solar Radiation (
288.0 243.7
255.1* 230.4
219.5 220.1
979.3 1038.0
242.7 231.4
Pressure (mB ) :
902.0 901.9
901.0 906.1
895.5 903.2
908.3 911.9
884.9 892.2
898.4 903.7
-
91
41
66
4
4
4
12
4
-
.4
.1
.3
.5*
.0
.3
.7
.3
6
49
66
52
4
3
3
10
3
.9*
.0
.5
.4
. Itf
.7
.6
.3
.7
184
40
74
100
4
4
4
13
4
.4
.6
.9
.6
.2
.2
.0
.6
. 1
21
265
66
114
4
4
3
12
4
. 1
.9
.0
o
.2
.4
.9
. 1
.2
30
30
5
24
4
5
4
13
5
.7
.5
.8
- -J
.8
.3
.8
.5
.0
(degrees ) :
283
294
300
293
W/m2
286
258
264
1113
268
903
904
904
916
896
904
-- No Data, * Data Recovery
. 1*
.5
.6
.3
):
.3*
.6
.6
.0
.8
.6*
.2
.6
.8
.3
.2
50%
291
295
273
284
250
240
233
984
238
903
906
907
916
897
906
. 8#
.4
. 1
.4
. 3#
.3
.9
.0
.4
. 0#
. 1
.7
.0
. 1
.5
to 85%,
195
205
236
212
201
228
219
1037
216
905
906
907
914
898
906
.1
.2
.5
.3
.3
.2
.0
.0
.0
.6
.1
.3
.5
.3
.3
# Data
262
209
257
243
173
155
180
915
170
907
904
907
917
890
906
.0
.5
.5
.8
.6
.2
.7
. 1
.2
.3
.7
.7
.2
. 1
.6
Recovery
288
290
284
288
142
167
145
834
151
905
905
904
919
887
905
.4
.6
.9
.0
. 1
. 1
. 1
.8
.4
.8
. 1
.4
.3
.2
. 1
< 50%
-------
SUMMARY OF METEOROLOGICAL DATA
SUBSITE: SHENANDOAH 2
Periods of Record
Average Temperature (C)
1988: May 17 - Nov 22
1987: Apr 22 - Nov 17
1988: Apr 16 - Nov 2
1986
1987
1988
Max
Min
Mean
Average
1986
1987
1988
Mean
APR
—
11.3
9.7
25.5
2.1
10.3
Relative
__
59.4
46.9
51.5
MAY
18.6
17.9
16.8
29.8
3.7
17.6
Humidity
68.0
64.4
61.7
64.0
JUN
21
22
20
32
7
21
(*)
60
64
58
61
.6
.5
.4
.3
.2
.5
.6
.7
.0
. 1
JUL
23.
23.
24.
36.
9.
23.
68.
66.
61.
65.
6
5*
5
1
7
9
6
1*
7
4
AUG
20.
22.
23.
34.
8.
22.
72.
66.
64.
67.
SEP
2
8
9
9
4
3
4
2
3
7
18
19
17
29
6
18
69
73
70
71
.7
.1
.8
.3
. 1
.5
.6
.0
.5
.0
OCT
13.7
10.8
9.6
27.8
-0.6
11.4
60.1
54.0
55.2
56.4
Total Precipitation (mm):
1986
1987
1988
Mean
Average
1986
1987
1988
Max Hr.
Mean
--
16.3
10.2
12.4
98.0
125.2
201.2
149.7
94
89
38
74
.5
.2
.6
.1
1.
19.
86.
47.
5
1*
4
6
--
30.
79.
38.
2
0
4
13
218
76
100
.0
.9
.5
.7
24.6
32.3
31.8
29.6
Wind Speed (m/s):
--
3.6
4.1
12.6
3.9
2.1
2.2
2.9
11.5
2.5
Resultant Wind Direction
1986
1987
1988
Mean
Average
1986
1987
1988
Max
Mean
--
276.3
311.4
298.5
192.6
206.4
165.8
187.9
2
2
2
8
2
.6
.3
.7
.2
.5
2.
2.
2.
10.
2.
6
4*
2
8
4
2.
2.
2.
9.
2.
5
8
6
3
6
2
2
2
9
2
.4
.5
.4
.0
.4
2.3
3.0
3.0
9.9
2.8
(degrees ) :
253
246
285
261
.4
.2
.7
.8
256.
183.
195.
216.
4
4*
1
3
182.
176.
175.
178.
8
0
2
0
195
191
191
192
.1
.0
.7
.6
267.0
274. 1
287.3
276.1
Solar Radiation (W/m2):
--
218.6
184.3
965.6
196.5
217.0
228.2
216.6
1030.5
221.5
272
257
242
1075
257
.5
.2
.7
.4
.5
240.
248.
227.
970.
237.
5
2*
6
8
2
192.
223.
212.
973.
209.
1
7
1
3
0
169
158
169
880
166
.5
.7
.6
. 1
.0
132.5
151. 1
136.0
808.0
139.9
Pressure (mB) :
1986
1987
1988
Max
Min
Mean
--
936.1
934.8
975.6
922. 1
935.3
935.1
940.6
942.2*
969.0
930. 1
939.8
937
937
-
945
929
937
.0
.6
-
.3
.0
.3
937.
939.
938.
947.
927.
938.
9
7*
4*
8 '
4
5
939.
939.
938.
949.
929.
939.
3
8
4
9
2
2
941
938
940
950
922
940
.4
.5
. 1
.5
.3
.0
940.7
940. 1
937.9
955.9
921.4
939.6
-- No Data, * Data Recovery 50% to 85%, # Data Recovery < 50%
-------
SUMMARY OF METEOROLOGICAL DATA
SITE: WHITEFACE
Periods of Record:
Average Temperature (C):
1986
1987
1988
Max
Min
Mean
Average
1986
1987
1988
Mean
APR MAY
— —
15.8
11.7
20.5
2.9
13.0
Relative Humidity
__
86.1
67.5
83.3
1986:
1987
1988:
JUN
8
11
7
23
-2
9
(%)
76
80
72
76
.0*
.0
.3*
.9
.9
.1
;
.4*
.8
.0*
.8
: Jun 19
: May 29
: May 26
JUL
11
13
14
31
0
13
88
85
.81
85
.9
.3
.6*
.3
.5
.2
.1
.5
.6*
.3
- Oct 28
- Oct 13
- Oct 17
AUG
9
11
12
27
-4
11
92
80
89
87
.7
.5
.8
.4
.2
.3
.2
.0
.1
.5
SEP
6
6
6
17
-4
6
89
89
83
87
.4
.2*
.6
.7
.5
.4
.0
.8*
.1*
. 1
OCT
0
-0
-0
13
-10
0
88
82
91
88
.7
.5
.2
.3
.9
.2
. 7*
.9
.7
.2
Total Precipitation (mm):
1986
1987
1988
Mean
Average
1986
1987
1988
Max Hr.
Mean
__
0.0
—
__
Wind Speed (m/s):
__
12.8
9.9
21.9
10.8
Resultant Wind Direction
1986
1987
1988
Mean
Average
1986
1987
1988
Max
Mean
Average
1986
1987
1988
Max
Min
Mean
__
277.0
276.0
276.3
Solar Radiation (
-_
190.1
247.4
934.7
229.6
Pressure (mB ) :
__
849.8
848.1
852.3
843.5
848.7
3
40
-
32
10
9
9
22
9
.3*
.9
-
.8
.3*
.3
.7*
.7
.6
54
66
-
60
8
8
7
23
8
.4
.8
-
.7
.4
.2
.6
.6
.1
47
23
-
39
8
7
8
25
8
.2
.4#
-
.8
.7
.6
.9
.3
.4
62
3
-
34
9
10
10
24
10
.5
.0*
-
.9
.2
.4*
.7
.2
.1
24
1
-
20
9
8
7
30
8
.9
.Ott
-
.5
.4
. 9*
.8
.0
.9
(degrees):
275
297
286
290
W/m2
225
189
248
1018
217
847
846
843
856
831
845
. 9*
.4
.8*
.4
):
.5*
.6
.0*
.5
.9
.7*
.4
.5
.8
.0
.2
283
77
260
200
190
203
174
955
191
848
848
848
859
833
848
.8
.6
.6*
.6
.3
.3
.6*
.9
.7
.9
.6
.8
.2
.4
.8
274
97
263
216
154
184
159
927
165
849
852
846
863
832
849
.9
.3
.9
.2
.0
.0
.0
.9
.0
.2
.6
.9
.7
.6
.4
266
271
263
267
110
100
129
774
114
848
853
845
865
822
848
.3
.5*
.7
.0
.1
. 9*
.5
.6
.0
.7
. 3*
.1
.7
.6
.9
256
257
231
250
77
92
46
669
71
845
849
842
859
821
845
.8
. 1*
.9
.6
. 1
.0
.7
.2
.7
.2
.1
.0
.4
.4
.1
— No Data, * Data Recovery 50% to 85%, # Data Recovery < 50%
-------
SUMMARY OF METEOROLOGICAL DATA
SITE: WHITETOP
Periods of Record:
Average Temperature (C):
1986-
1987
1988
Max
Min
Mean
Average
1986
1987
1988
Mean
APR MAY
7.01* 9.8
1.0* 12.5
4.9 9.9
20.4 21.4
-11.9 -4.7
4.3 10.7
Relative Humidity
62. 6# 83.4
77.6* 81.2
70.6 67.8
70.8 77.5
1986
1987
1988
JUN
14.9
14.4
14. 1
24.0
1.3
14.5
(%):
84.6
85.2
69.1
79.8
: Apr 1
: Apr 1
: Apr 1
JUL
16.7
16.5
16.6
25.3
5.0
16.6
86.9
82.3
75.9
81.6
- Oct 31
- Oct 31
- Oct 31
AUG
13.9
15.9
16.8
25.3
1.2
15.6
91.3
85.6
81.1
85.9
SEP
12.8
13.4*
12.5
19.5
3.0
12.8
91.6
87. 3#
91.2
90.6
OCT
7.1
4.7*
2.9
18.0
-8.6
4.9
86.2
65.2*
71.4*
75.4
Total Precipitation (mm):
1986
1987
1988
Mean
Average
1986
1987
1988
Max Hr.
Mean
48.0 193.0
220.2 93.0
121.7 78.2
128.7 121.4
Wind Speed (m/s) :
2.4# 2.5
3.9* 2.3
3.7 2.8
14.6 10.2
3.5 2.5
Resultant Wind Direction
1986
1987
1988
Mean
Average
1986
1987
1988
Max
Mean
Average
1986
1987
1988
Max
Min
Mean
. 328. 4# 207.9
129.2* 243.6
177.2 240.7
195.2 230.9
Solar Radiation (
232. 8* 176.3
172.8 225.9
197.1 247.0
1068.7 1083.7
194.1 216.8
Pressure (mB ) :
828. 8#
826.0 836.3
826.8 833.1
839.1 842.2
810.3 822.5
826.8 711.0
74.2
152.9
63.5
97.6
2.4
2.5
2.2
8.1
2.4
(degrees
200.2
267.4
121.3
198.0
W/m2):
235.5
228.2
292.1
1090.7
251.2
834.1
835.8
836.2
846.3
824.0
835.4
90.4
66.0
103.4
86.6
1.9
1.9
2.5
7.9
2.1
):
229.3
283.6
241.9
252.0
230.8
235.3
230.7
1083.8
232.3
835.6
838.0
839.0
845.1
827.0
837.6
172.7
57.7
95.8
108.2
2.3*
3.0
2.9
9.5
2.8
191.7*
232.7
272.2
241.6
179.6
193.7
216.7
1013.6
197.0
839. 9#
837.7
838.3
844.1
830.1
838. 1
141.7
85.1
143.3
123.4
2.7*
3.6tt
3.3
10.9
3.2
191.7*
158.8*
2.1
85.3
141.2
151.3
147.7
996.0
146.7
838.1
836. 0*
837.4
844.8
822.6
837.4
95.0
23.6*
83.1
71.9
3.7
3.0
—
13.8
3.4
191.7
97. 1*
188.0
163.9
137.4*
174.6
148.7
871.8
155.1
835.4*
824.3
830.7
846.6
820.0
829.8
-- No Data, * Data Recovery 50% to 85%, * Data Recovery < 50%
-------
SUMMA-RY OF METEOROLOGICAL DATA
SUBSITE: SHENANDOAH 3
Periods of Record
Average Temperature (C)
1986: May 21 - Nov 23
1987: Apr 24 - Nov 18
1988: Apr 15 - Nov 1
1986
1987
1988
Max
Min
Mean
Average
1986
1987
1988
Mean
APR
--
11.4
11.4
25.8
2.6
11.4
Relative
--
52.5
44.9
47.3
MAY
18.5
18.3
17.6
31.2
3.6
18.0
Humidity
68.3
64.7
64.8
65.3
JUN
22.
21.
21.
34.
6.
21.
(%):
61.
62.
59.
61.
JUL
4
8
4
9
6
9
9
3
6
3
24
23
25
38
9
24
74
63
65
66
.0#
.6
.0
.4
.2
.3
.9#
.9
.9
.5
AUG
20.
22.
25.
37.
7.
22.
75.
63.
67.
69.
7
1
0
5
1
6
9
7
9
3
SEP
19
18
19
31
6
18
70
71
71
70
.4'
.3
.0
.5
.0
.9
.5
.1
.1
.9
OCT
14.1
9.6*
10.4
30.5
0.5
11.6
60.4
52.5*
57.0
57.2
Total Precipitation (mm):
1986
1987
1988
Mean
Average
1986
1987
1988
Max Hr.
Mean
Resultan
1986
1987
1988
Mean
Average
1986
1987
1988
Max
Mean
Average
1986
1987
1988
Max
Min
Mean
--
0.0
10.9
7.5
--
123.7
204.0
163.9
--
101.
35.
69.
6
3
0
-
45
85
65
-
.0
.1
.1
180.
31.
75.
93.
8*
5
9
3
29
225
80
110
.0
.0
.3
.7
22.4
33.3*
34.5
29.6
Wind Speed (m/s):
--
2.1
2.4
6.3
2.3
t Wind Di
--
359.6
13. 1
119.9
Solar Rad
--
209.6
205. 1
957.3
206.5
Pressure
--
959.2
954.6
968. 1
942. 1
956.0
1.3
1.6
1.8
5.7
1.6
rection
187.4
179.8
169.8
176.6
iation (
234.7
223.8
227.4
1041. 1
226.9
(mB):
958.5
964.1
961.8
970.7
950.4
962.3
1.
1.
1.
5.
1.
6
5
7
7
6
1
1
1
4
1
.6*
.4
.4
.9
.4
1.
1.
1.
5.
1.
6
7
5
5
6
1
1
1
5
1
.5
.5
.5
.3
.5
1.5
1.9*
1.8
5.5
1.7
(degrees) :
170.
157.
159.
162.
W/m2)
269.
255.
262.
1054.
262.
959.
961.
963.
975.
951.
961.
3
3
2
3
6
3
3
4
4
8
6
2
5
0
5
181
166
188
169
343
243
233
982
250
961
963
965
974
953
964
.2#
.4
.0
.5
.4*
.0
.0
. 1
.4
.2#
.7
.6
.7
.4
.1
182.
166.
166.
172.
224.
220.
221.
973.
222.
962.
963.
965.
973.
954.
963.
4
6
8
1
6
0
7
2
0
6
7
0
2
6
7
179
165
166
170
170
159
177
911
169
964
963
966
977
948
964
.3
.6
.1
.6
.5
.9
.4
.3
. 1
.8
.1
. 1
.9
.1
.6
170.8
91.3*
126.4
135.2
136.2
142.3*
140.4
835.3
139.2
964.4
963.5*
965.4
980.2
947.9
964.6
-- No Data, * Data Recovery 50% to 85%, # Data Recovery < 50%
-------
-------
APPENDIX D
MCCP Publications
-------
Aneja, V.O., Bradow, R.L. and Jayanty, R.K.M., 1988. "Organic Chemical Characterization of Clouds in
High Elevation Spruce-Fir Forests at Mt. Mitchell, North Carolina". Proceedings of the 1988
EPA/APCA International Symposium on Measurement of Toxic and Related Air Pollutants, pp 227-236.
Aneja, V.P., Claiborn, Bradow, R.L., Paur, R.J. and Baumgardner, R.E., 1989. "Dynamic chemical
characterization of montane clouds", Atmospheric Environment, in press.
Aneja, V.P., Claiborn, C.S., Li, Z. and Murthy, A, 1989. "Exceedences of the National Ambient Air
Quality Standard for Ozone Occurring at a Pristine Area Site", Journal of Air Pollution Control and
Waste Management, in press.
Aneja, V.P., Claiborn, Li, Z. and Murthy, A., 1989. "Measurements at high elevations of Oxidants in the
Eastern United States and their role in Forest Decline", in Man and his Ecosystem, L.J. Brasser and
W.C. Mulder, Eds., Elsevier Science Publishers B.V., Amsterdam, Vol. 2, pp 189-194.
Aneja, V.P., Businger, S., Li, Z., Claiborn, C.S. and Murthy, A, 1989. "Ozone Climatology at high
elevations in the Southern Applachians", Journal of Geophysical Research, submitted.
Aneja, V.P., Claiborn, C.S., Murthy, A. and Kim, S.D. "Characterization of the Chemical and Physical
Climatology for evaluation of the role of air pollution in forest decline", in preparation for submission to
Atmospheric Environment.
Aneja, V.P., Businger, S., Li, Z., Claiborn, C, and Murthy, A, 1989. "Ozone Climate at Mt. Mitchell,
North Carolina, and its Association with Synoptic Episodes", Proceedings of the 82nd Annual Meeting of
Air and Waste Management Association, Vol. 89-36.5, pp 1-28.
Aneja, V.P., Sookin, D., Murthy, A, Paur, R.J., Baumgardner, R. and Kronmiller, K., 1990. "Description
and performance of a cloud and rain acidity/conductivity (CRAC) Automated Sampling System",
submitted to the Journal of Air Pollution and Waste Management.
Bailey, B.H. and D.J. Smalley. 1987. Meteorological/climate aspects of mountain cloud chemistry
monitoring. In: Proceedings of the Sixth Symposium on Meteorological Observations and
Instrumentation, Jan. 12-16, 1987. New Orleans, LA American Meteorological Society. Boston, MA
Beltz, N., W. Jaeschke, G.L. Kok, S.N. Gitlin, AL. Lazrus, S. McLaren, D. Shakespeare, and V.A
Mohnen. 1987. A comparison of the enzyme fluorometric and the peroxyoxalate chemiluminescence
methods for measuring ^2^2- J. Atmos. Chem. 5:311-322.
Bradow, R.L. and Viney P. Aneja, 1988. "Aerosol Compositional Effects on Mountain Clouds:
Attributing Sources of Acid Deposition", in Atmospheric Aerosols and Nucleation, Paul E. Wagner and
Gabor Vali, Eds., Chapter 8, pp 40-43, Springer-Verlag, Berlin.
Claiborn, C.S. and Aneja, V.P., 1990. "Measurements of Atmospheric Hydrogen Peroxide in the gas-
phase and in cloudwater at Mt. Mitchell State Park, N.C.", in preparation for submission to Atmospheric
Environment.
Davis, J.M., Seabaugh, S.S., Bradow, R.L., and Monahan, J.F., 1990. "A Trajectory Climatology and Case
Study of Ozone Occurrence at the Mountain Cloud Chemistry Program (MCCP) Site 1 at Mt. Gibbs,
North Carolina", submitted Atmospheric Environment.
DeFelice, T.P. In press. Occurrence of extreme episodes of acidic deposition on coniferous forests in
Mt. Mitchell State Park: aqueous phase. Water. Air. Soil Pollut.
D-l
-------
DeFelice, T.P. 1989. Characterization of extreme deposition of air pollutants in Mt. Mitchell State Park:
potential for forest decline and opportunity for cloud deacidification. Doctoral dissertation. Department
of Marine, Earth, and Atmospheric Sciences, North Carolina State University. 200 pp.
DeFelice, T.P. and V.K. Saxena. 1988. Temporal and spatial distribution of ionic composition and acidity
in clouds: comparison between modeling results and observations, pp. 16. In: Programme International
Congress of Geochemistry & Cosmochemistry, Aug. 29-September 2, Paris, France.
Estes, M.J. and J.T. Sigmon. 1987. Comparisons of chemical compositions of mountain stratiform clouds
and valley fog in the Shenandoah National Park, pp. 59-60. In: Proceedings of the Sixth Symposium on
Meteorological Observations and Instrumentation, Jan. 12-16, New Orleans, LA American
Meteorological Society. Boston, MA.
Fehsenfeld, F.C., J.W. Drummond, U.K. Roychowdhury, P.J. Galvin, E.J. Williams, M.P. Buhr, D.D.
Parrish, G. Hubler, A.O. Langford, J.G. Calvert, B.A. Ridley, F. Grahek, B. Heikes, G. Kok, J. Shelter,
J. Walega, CM. Elsworth, R.B. Norton, D.W. Fahey, P.C. Murphey, C. Hovermale, V.A. Mohnen, K.L.
Demerjian, G.I. Mackay and H.I. Schiff. Intercomparison of NO£ measurement techniques. In press
JGR-Atmospheres. 1989.
Galvin, P.J., V.A. Mohnen and U. Roychowdhury 1987. Advanced mobile measurement laboratory for
mountain cloud chemistry research. Proc. 6th Symposium on Meteorological Observations and
Instrumentation, Jan. 12-16, New Orleans, LA. AMS, Boston, MA.
Galvin, P. and V. Mohnen. 1987. Measurement of ozone and other oxidants at mountain sites in the
eastern U.S., pp. 395-410. In: Proceedings of the North American Oxidant Symposium, Feb. 25-27, 1987,
Quebec, Canada.
Gilliam, F.S. and.J.T. Sigmon. 1987. Relationships between throughfall chemistry and the chemical fluxes
in dry deposition and mountain clouds, pp. 63-65. In: Proceedings of the Sixth Symposium on
Meteorological Observations and Instrumentation, Jan. 12-16, New Orleans, LA. American
Meteorological Society. Boston, MA.
Gilliam, F.S., J.T. Sigmon, M.A Reiter, and D.O. Krovetz. In press. Elevational and spatial variation in
daytime ozone concentrations in the Virginia Blue Ridge mountains: implications for forest exposure.
Can. J. Forest Res.
Harrison, E.A., B.M. Mclntyre, and R.D. Dueser. 1989. Community dynamics and topographic controls
on forest pattern in Shenandoah National Park, Virginia. Bull, of Torrev Bot. Club. 6:1-14.
Hertel, G.D., S.J. Zarnoch, T. Arre, C. Eager, V. Mohnen and S. Medlarz. Status of the Spruce-Fir
Cooperative Research Program. Presented at the 80th Annual Meeting of APCA, New York, NY, June
21-26. 20 pp.
Hornig, J.F., C.J. High, and P.O. Thorne. 1988. Instrumentation for obtaining meteorological and
precipitation information at multiple remote forest sites, pp.183-190. In: G.D. Hertel [Tech. Coordin.]
Effects of Atmospheric Pollutants on the Spruce-Fir Forests of the Eastern United States and the
Federal Republic of Germany. Proceedings of the United States/Federal Republic of Germany Research
Symposium, Oct. 19-23, 1987, Burlington, VT. General Technical Report NE 120, USDA-Forest Service,
Northeastern Forest Experiment Station, Broomall, PA 543 pp.
D-2
-------
Joslin J. D., Mueller S. F. and Wolfe M. H. (1990) The use of artificial and living collectors in the
testing of models of cloud water deposition to forest canopies (submitted to Atmospheric Environment).
Kavender, K.A. 1988. Measurement of a vertical ozone concentration profile in a slash pine forest.
Masters Thesis, Environmental Engineering Sciences Department, University of Florida, Gainesville, FL.
77pp.
Keene, W.C. and J.N. Galloway. 1988. Biogeochemical cycling of formic and acetic acids through the
troposphere: an overview of current understanding. Tellus. 40B:322-334.
Krovetz, D.O., M.A. Reiter, and J.T. Sigmon. 1988. An inexpensive thermocouple probe-amplifier and its
response to rapid temperature fluctuations in a mountain forest. J. Atmos. Oceanic Technol.
5(6):870-874.
Krovetz, D.O., M.A. Reiter, J.T. Sigmon, and L.S. Gilliam. 1988. Assembly and field testing of a
ground-based presence of cloud detector. J. Atmos. Oceanic Technol. 5:579-581.
Krovetz, D.O., J.T. Sigmon, M.A. Reiter, and L.H. Lessard. In press. An automated system for air
sampling with annular denuders at a remote site. Environ. Pollut.
Lefohn, A.S. and V.A. Mohnen 1986. The Characterization of Ozone, Sulfur Dioxide and Nitrogen
Dioxide for Selected Monitoring Sites in the Federal Republic of Germany. JAPCA. Vol. 36, No. 12,
1329-1337.
Lefohn, A.S., D.S. Shadwick and V.A Mohnen. The characterization of ozone and sulfur dioxide
concentrations at a select set of high-elevation sites in the eastern United States. In Press
Environmental Pollution. 1990.
Lefohn, A.S. and V.A Mohnen. 1986. The characterization of ozone, sulfur dioxide and nitrogen dioxide
for selected monitoring sites in the Federal Republic of Germany. JAPCA. 36:1329-1337.
Lefohn, A.S., V.C. Runeckles, S.V. Krupa, and D.S. Shadwick. 1989. Important consideration for
establishing a secondary ozone standard to protect vegetation. JAPCA. 39(8): 1039-1045.
Lessard, L.H. and J.T. Sigmon. 1987. Measurements of concentrations of some reactive atmospheric gases
and fine primary particulates with annular denuder atmospheric samplers, pp.60-62. In: Proceedings of
the Sixth Symposium on Meteorological Observations and Instrumentation, Jan. 12-16, New Orleans, LA.
American Meteorological Society. Boston, MA.
Lin, N.-H. 1988. Investigations on cloud chemistry and acidic deposition at Mt. Mitchell, N.C. Using a
cloud deposition model. Master's Thesis. Department of Marine, Earth, and Atmospheric Sciences,
North Carolina State University. 149 pp.
Mallant, R., K. Elsholz, and B. Bailey. 1989. Fog detection with a low-cost forward scattering optical
device. In: Proceedings of the Symposium on the Role of Clouds in Atmospheric Chemistry and Global
Climate, Jan. 29-Feb. 3, 1989, American Meteorological Society, Anaheim, CA. pp. 221-223.
Markus, M., B. Bailey, and R. Stewart. 1989. Estimation of cloud frequency at high elevation forests in
the eastern United States. In: Proceedings of the Symposium on the Role of Clouds in Atmospheric
Chemistry and Global Climate, Jan. 29-Feb. 3, 1989, American Meteorological Society, Anaheim, CA.
pp. 110-113.
D-3
-------
Markus, M. and B. Bailey. 1989. Cloud frequency determination at high elevations using an optical
detector. In: Proceedings of the Conference on Agricultural and Forest Meteorology, March 7-10, 1989,
American Meteorological Society, Charleston, SC. pp.35-37.
Mclntyre, B.M., M.A Scholl, and J.T. Sigmon. 1990. A quantitative description of a deciduous forest
canopy using a photographic technique. Accepted by Forest Science.
Meagher J. R, Olszyna K. J., Weatherford F. P. and Mohnen V. A. (1990) The availability of H2O2 and
Oj for aqueous phase oxidation of SC«2: the question of linearity. Atmos. Environ, (in press).
Meagher, J.F., K.J. Olszyna, P.P. Weatherford and V.A Mohnen. The availability of H2O2 and Oj for
aqueous phase oxidation of SO2--The question of linearity. Accepted for publication in Atmospheric
Environment.
Mohnen, V.A. 1987. Airborne and ground-based cloud collectors: an overview, pp. 44-46. In: Proceedings
of the Sixth Symposium on Meteorological Observations and Instrumentation, Jan. 12-16, New Orleans,
LA American Meteorological Society. Boston, MA.
Mohnen, V.A. 1988. The mountain cloud chemistry program. In: G.D. Hertel [Tech. Coordin.] Effects of
Atmospheric Pollutants on the Spruce-Fir Forests of the Eastern United States and the Federal Republic
of Germany. Proceedings of the United States/Federal Republic of Germany Research Symposium, Oct.
19-23, 1987, Burlington, VT. General Technical Report NE 120, USDA-Forest Service, Northeast Forest
Experiment Station, Broomall, PA 543
Mohnen, V.A 1989. Mountain Cloud Chemistry Project - Wet, Dry and Cloud Water Deposition,
EPA/600/53-89/009. U.S.EPA Atmospheric Research and Exposure Assessment Laboratory, RTP, N.C.
27711. 77 pp.
Mohnen, V.A. 1989. Exposure of Forests to Air Pollutants, Clouds, Precipitation, and Climatic
Variables. EPA/60/53-89-003. U.S. EPA, Atmospheric Research and Exposure Assessment Laboratory,
RTP, N.C. 27711. 190 pp.
Mohnen, V.A, R.L. Bradow, D. Landsberg, J. Healey, and B.H. Bailey. 1987. Overview of the EPA
mountain cloud chemistry program, pp.47-50. In: Proceedings of the Sixth Symposium on Meteorological
Observations and Instrumentation, Jan. 12-16, New Orleans, LA American Meteorological Society.
Boston, MA.
Mohnen, V.A, K. Leonard, and B.H. Bailey. 1987. Cap cloud frequency and chemistry at Whiteface
mountain, pp. 51-54. In: Proceedings of the Sixth Symposium on Meteorological Observations and
Instrumentation, Jan. 12-16, 1987. New Orleans, LA. American Meteorological Society. Boston, MA.
Mohnen, V.A 1984 Project Director. EPA/NSF Workshop on atmospheric deposition and its impact on
high elevation mountain forest systems, Albany, NY, April 5-7. ASRC/SUNY Pub. No. 981.
Mohnen, V.A. and J.A Kadlecek. Special Problems in Atmospheric Exposure. Part I - Interception;
Part II - Throughfall. MCCP Background Report to Site Directors, November. ASRC/SUNY Pub.
No. 1113.
Mohnen, V.A Mountain Cloud Chemistry. Presented at the Symposium on Cloud Chemistry and Acid
Precipitation, 20 August (XIX General Assembly of the IUGG) Vancouver, Canada. Expand Abstracts
V.3, p. 855, No. Ml 1-9.
D-4
-------
Mohnen, V.A. 1988 The Challenge of Acid Rain. Scientific American. Vol. 259, No. 2, August, 30-38.
Mohnen, V.A. Mountain Cloud Chemistry Project (MCCP). Presented at European Fog Workshop,
University Frankfurt. In: Chemistry and Physics of Fogwater Collection. W. Jaeschke and K.H. Enderle
(Eds.). Proceedings, Workshop Frankfurt am Main, 16-17 December 1986. BPT-Bericht 6/88, 97-121.
Mohnen, V.A Air pollutant distribution patterns: elevational gradients/local chemistry. Proceedings,
15th International Meeting for Specialists in Air Pollution Effects on Forest Ecosystems-Air Pollution
and Forest Decline; Interlaken, Switzerland, October 2-8.
Mohnen, V.A. Exposure of forests to air pollutants, clouds, precipitation and climatic variables. A
preliminary assessment-1987. Annual report submitted to EPA under contract no. CR813934-01-2.
September.
Mohnen, V.A. Quality assurance and quality control procedures for air quality measurements from
airborne platforms. Paper presented at VDI-Workshop "Fluggestutzte Messungen von
Luftverunreinigungen", Vol. 9, 157-166, VDI-Kommission Dusseldorf, Germany. (Workshop on October
13-14, 1988, Trier).
Mohnen, V.A 1989 Elevational gradients/local chemistry. In: Biologic Markers of Air-Pollution Stress
and Damage in Forests. National Academy Press. Washington, DC, 47-56 (Reviewed).
Mohnen, V.A and J.A Kadlecek. Cloud Chemistry Research at Whiteface Mountain. Tellus. 418:79-91.
Mohnen, V.A Acid rain in perspective. The Nelson A Rockefeller Institute of Government Working
Paper Series (Spring, 1989).
Mohnen, V.A Mountain Cloud Chemistry Project Wet, Dry and Cloud Water Deposition.
EPA/600/3-89/009.
Mohnen, V.A and AS. Lefohn. Temporal development of the pollution load of reactive trace gases in
forested areas in the United States. Invited paper presented at the International Congress on Forest
Decline Research: State of Knowledge and Perspectives, Friedrichshafen, Lake Constance, Federal
Republic of Germany, October 2-6. Published in Proceedings, 1990.
Mohnen, V.A Acid Rain. Paper presented at the International Power Technology Conference &
Exhibition, Chicago, IL, October 31, 1989.
Mohnen, V.A Acid rain and urban atmospheric pollution in North America. Presented at The Royal
Institute of International Affairs, Chatham House Conference, Fourth International Energy Conference
"Environmental Challenges: The Energy Response, London, December 4-5, 1989.
Mueller S. F. (1990) Estimating cloud water deposition to subalpine spruce-fir forests - I: modifications
to an existing model (accepted by Atmospheric Environment).
Mueller S. F. and Imhoff R. E. (1989) Inferring cloud deposition to a forest canopy using a passive
cloudwater collector. Geophvs. Res. Let. 16:683-686.
Mueller S. F. and Weatherford F. P. (1988) Chemical deposition to a high elevation red spruce forest.
Water. Air, and Soil Pollution 38:345-363.
D-5
-------
Mueller S. R, Joslin J. D. and Wolfe M. H. (1990) Estimating cloud water deposition to subalpine
spruce-fir forests - II: model testing (accepted by Atmospheric Environment).
Mueller, S.R and RP. Weatherford. 1988. Chemical deposition to a high elevation red spruce forest.
Water. Air. Soil Pollut. 38:345-363.
Murphy, C.E. and J.T. Sigmon. In press. Dry deposition of sulfur and nitrogen oxide gases to forest
vegetation. In: Advances in Environmental Sciences. Springer-Verlag:New York.
Murthy, A. and Aneja, V.P., 1990. "Deposition and Interaction of nitrogen containing pollutants to a
high elevation forest canopy", in preparation for submission to Atmospheric Environment.
Olszyna K. J., Meagher J. R and Bailey E. M. (1988) Gas-phase, cloud and rain-water measurements of
hydrogen peroxide at a high-elevation site. Atmos. Environ. 22(8):1699-1706.
Reisinger L. M. (1989) Particles sampled in the southern Appalachian Mountains. Water. Air, and Soil
Pollut. (in press).
Reisinger L. M. and Imhoff R. E. (1989) Analysis of summertime cloud water measurements made in a
southern Appalachian spruce forest. Water. Air, and Soil Pollut. 45:1-15.
Reisinger L. M., Olszyna K. J. and Hetrick T. L. (1989) Comparison of enhanced and routine methods
for measuring ambient low-level sulfur dioxide. JAPCA. 39:981-983.
Robarge, W.P., R.I. Bruck, and E.B. Cowling. 1988. Throughfall and stemflow measurements at Mt.
Mitchell, North Carolina during the summer of 1986: a preliminary report, pp. 111-116. In: G.D. Hertel
[Tech. Coordin.] Effects of Atmospheric Pollutants on the Spruce-Fir Forests of the Eastern United
States and the Federal Republic of Germany. Proceedings of the United States/Federal Republic of
Germany Research Symposium, Oct. 19-23, 1987, Burlington, VT. General Technical Report NE 120,
USDA-Forest Service, Northeastern Forest Experiment Station, Broomall, PA 543 pp.
Saxena, V.K. 1987. Mountain cloud chemistry project at Mt. Mitchell, NC: strategies and highlights.
Trans. Amer. Geophys. Union (EOS). 68:270.
Saxena, V.K., E.B. Cowling, R.E. Stogner, and R.V. Crum. 1986. 1986:Cloud chemistry measurements at
Mt. Mitchell, North Carolina, pp. 91-94. In: Preprints for the Cloud Physics Conference, American
Meteorological Society, Boston, MA.
Saxena, V.K. and N.-H. Lin. 1988. Cloud capture by a mountain top forest: acidity and dosage duration.
In: Preprint for the 10th International Cloud Physics Conference, Aug. 15-20, 1988, Bad Homburg,
Federal Republic of Germany. 1:232-234. Available from: Deutscher Wetterdienst, Frankfurter Strasse
135, D06050 Offenbach Am Main, FRG.
Saxena, V.K. and N.-H. Lin. 1988. Relative importance of dry, wet and cloud capture mechanisms for
acidic deposition, pp. 237-247. In: S. Hocheiser and R.K.N. Jayenty, eds. Measurements of Toxic and
Related Air Pollutants, EPA/Air Pollution Control Association, Symposium, May 1-4, Raleigh, NC.
Saxena, V.K. and N.-H. Lin. 1989. Contribution of acidic deposition on high elevation forest canopy to
hydrologic cycle, pp. 193-202. In: Proceedings of the International Association Hydrological Science, 3rd.
Science Assembly, May 10-19, Baltimore, MD.
D-6
-------
Saxena, V.K., N.-H.Lin, and T.P.Defelice. In Press. Hydrological and chemical input to fir trees from rain
and clouds during a 1-month study at Clingmans Peak, NC. Atmospheric Environment. 23:, 5pp., 1990.
Saxena, V.K. and R.E. Stogner. 1987. Wet deposition on forest canopy at Mt. Mitchell, North Carolina,
pp. 189-194. In: Measurements of Toxic and Related Air Pollutants, Air Pollution Control Association,
Pittsburgh, PA.
Saxena, V.K., R.E. Stogner, AH. Hendler, T.P. DeFelice, and R.J.-Y. Yeh. 1989. Monitoring the
chemical climate of the Mt. Mitchell State Park for evaluating its impact on forest decline. Tellus.
418:92-109.
Saxena, V.K. and R.J.-Y. Yeh. 1989. Acidic cloud immersion: a possible cause of forest decline. In: Fifth
World Meteorological Organization Scientific Conference on Weather Modification and Applied Cloud
Physics, March 27-31, 1989, Guangzhou, China.
Saxena, V.K. and R.J.-Y Yeh. 1989. Temporal variability in cloud water acidity: physio-chemical
characteristics of atmospheric aerosols and windfield. J. Aerosol Sci. 19:1207-1210.
Sigmon, J.T. and M.J. Estes. 1988. Relationship between cloud chemistry and meteorology in central
Virginia: A preliminary study. Preprints of the 81st Annual Meeting of Air Pollution Control
Association.
Sigmon, J.T., F.S. Gilliam, and M.E. Partin. In press. Precipitation and throughfall chemistry for a
montane hardwood forest ecosystem: potential contributions from cloud water. Can. J. Forest Res.
Sjostedt, D.W. 1987. A characterization of the nocturnal low-level jet in the Carolinas. Masters Thesis.
Department of Environmental Sciences. University of Virginia.
Smalley, D.J. and.B.H. Bailey. 1987. Meteorological/climate aspects of mountain cloud chemistry
monitoring. In: Proceedings of the Sixth Symposium on Meteorological Observations and
Instrumentation, Jan. 12-16, New Orleans, LA American Meteorological Society, Boston, MA pp.
47-50.
Stogner, R.E. 1989. Acidic deposition to Mt. Mitchell, North Carolina area forests resulting from direct
cloud droplet interception. Master's Thesis. Department of Marine, Earth, and Atmospheric Science.
North Carolina State University. 124 pp.
Stogner, R.E. and V.K. Saxena. 1988. Acidic cloud-forest canopy interactions: Mt. Mitchell, NC. Environ.
Pollut. 53:456-458.
Thorne, P.O., Lovett, G.M. and Reiners, W.A (1982). Experimental determination of droplet impaction
on canopy components of balsam fir. Journal of Applied Meteorology 21, 1413-1416.
Valente R. J., Mallant R. K. A, McLaren S. E. and Schemenauer R. S. (1989) Field intercomparison of
ground-based cloud physics instruments at Whitetop Mountain, Virginia. J. Atmos. and Oceanic Tech.
6:396-406.
Vong, R.J., Bailey, B.R., Markus, M.J. and Mohnen, V.A (1989). Factors governing cloud water
composition in the Appalachian Mountains (submitted to Tellus BV
D-7
-------
Vong, R.J., B.H. Bailey, M.J. Markus and V.A Mohnen. Variation in cloud water chemistry with
synoptic type at five mountain sites in the eastern USA. EOS, Vol. 70(43):1007 (October 24, 1989),
Abstract #A11B-13 1130H. Accepted for publication in Tellus (1990).
Yeh, R.J.-Y. 1988. Measurements of cloud water acidity and windfield for evaluating cloud-canopy
interactions in Mt. Mitchell state park. Master's Thesis. Department of Marine, Earth, and
Atmospheric Science, North Carolina State University. 165 pp.
Yeh, R.J.-Y. and V.K. Saxena. 1988. Sulfur and nitrogen emissions along the path of the airmass and
cloud water acidity at Mt. Mitchell, North Carolina, pp. 15. In: 1988 Annual meeting of the American
Association for Aerosol Research, Oct. 10-14, 1988, Chapel Hill, NC.
D-8
-------
APPENDIX E
ADDITIONAL FIGURES
-------
Average Annual Low «2500 m) Cloud Amounts (%) in
Eastern North America, For Land Areas Only, 1971 -
1981, (from Warren et al,, 1986). The Time-Averaged
Cloud Amount is the Product of Frequency of Occurrence
and Amount-When-Present. Values Represent Stratus/
Stratocumulus, Cumulus and Cumulonimbus Cloud Types.
20-29%
30-397.
40-497.
Figure 4-9
E-l
-------
Average Cloud Base Height (m) in Eastern
North America for Stratus/Stratocumulus
Clouds, the Dominant Low Cloud Type, For
Land Areas Only, 1971-81 (From Warren et
al., 1986)
600-690 m 700-790 m
800-890 m
Figure 4-10
E-2
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-------
Probability of Cloud by Height and Season
at Moosilauke, NH, (1985-1987)
All
-•- DJF -•- MAM -o- JJA -a- SON
30%
25%
20%
15%
10%
o
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en
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HEIGHT (m)
Figure 4-13
E-4
-------
Probability of Cloud by Height and Season
at Shenendoah, W, (1985-1987)
— All ••- DJF ••- MAM -o- JJA -a- 5ON
30%
25%
20%
15%
10%
5%
0%
f
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m*
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«!•€•••
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500 1000 1500
HEIGHT (m)
2000
Figure 4-14
E-5
-------
Probability of Cloud by Height and Season
at Whiteface Mountain, NY, (1985-1987)
— All ••-
30%
25%
20%
15%
10%
5%
0%
DJF -•- MAM -o- JJA -n- SON
•
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2000
Figure 4-15
E-6
-------
Low-level Cloud Frequency Departure (%) From
1965-85 Normals For 8 NWS Airports
986 Field Season
Figure 4-17
E-7
-------
Low-level Cloud Frequency Departure (%) From
1965-85 Normals For 8 NWS Airports
1987 Field Season
Figure 4-18
E-8
-------
Low-level Cloud Frequency Departure (%) From
1965-85 Normals For 8 NWS Airports
988 Field Season
Figure 4-19
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Figure 4-23 Cloud droplet size distributions from Whiteface Mountain, NY
calculated by integrating over individual size distributions
and grouping the distributions into three categories by liquid
water content (LWC < 0.5 g/m3, 0.5 < LWC < 1.0 g/m3, and LWC >
1.0 g/m3), and clear air (Mohnen, 1987).
E-12
-------
DROUGHT SEVERITY ( Long Term Palmer) OVER THE EASTERN U.S.
MID-SUMMER 1986
MOIST
NORMAL
MODERATE
SEVERE
EXTREME
Date of Analysis: July 26
Source: NOAA Weekly Weather and Crop Bulletin, July 29, 1986.
Figure 4-25
E-13
-------
DROUGHT SEVERITY ( Long Term Palmer) OVER THE EASTERN U.S.
MID-SUMMER 1987
MOIST
NORMAL
MODERATE
SEVERE
EXTREME
Date of Analysis: August 1
Source: NOAA Weekly Weather and Crop Bulletin, August 4, 1987.
Figure 4-26
E-14
-------
DROUGHT SEVERITY ( Long Term Palmer) OVER THE EASTERN U.S.
MID-SUMMER 1988
MOIST
NORMAL
MODERATE
SEVERE
EXTREME
Date of Analysis: July 30
Source: NOAA Weekly Weather and Crop Bulletin, August 2, 1988.
Figure 4-27
E-15
-------
Midwest
Forested Areas
Q 0%1o20%
EH 21% 10 40%
41% to 60%
61% to 60%
8t%to 100%
South
Mid-Atlantic
Forested Areas
D 0% lo 24%
§3 25% to 49%
E3 50% lo 74%
• 75% to 100%
Source: A.S.L. & Associates
Helena, MT
Figure 4-29 Percent forest cover by county (Regions: Midwest, Northeast,
South, and Mid-Atlantic) .
E-16
-------
Pacific Northwest
Rocky Mountain
West
Forested Areas
D 0%to20%
EJ 21% to 40%
El 41% to 60%
61% to 60%
61% to 100%
Source: A.S.L. & Associates, Helena/ MT
Figure 4-30 Percent forest cover by county (Regions:
Rocky Mountain, and West).
Pacific Northwest,
E-17
-------
Source: EPA (1989)
0.30
CONCENTRATION. PPM
0.05-
0.00
1978 1979 1980 1981 1982 1983 1984 1985 1986 1987
Boxplot comparisons of trends in annual second highest daily maximum
1-hour ozone concentration at 274 sites, 1978-1987.
0.18
0.16-
0.14
0.12
0.10
O.OB
0.06
0.04
0.02
0.00
CONCENTRATION, PPM
• NAMS SfTIS (98) • ALL_S(TES_(274)_
1978 1979 1980 1981 1982 1983 1984 1985 1986 1987
National trend in the composite average of the second highest maximum
1-hour ozone concentration at both NAMS and all sites with 95 percent
confidence intervals, 1978-1987.
Fiuure 4-31
E-18
-------
Source: EPA (1989)
CONCENTRATION, PPM
0.040
0.013-
0.030
0.023
0.020
0.015
O.OtO
0.003
0.000
547 SUES
••——-NAAOS-
1978 1979 1980 1981 1982 1983 1984 1985 1986 1987
Boxplot comparisons of trends in annual mean sulfur dioxide
concentrations at 347 sites, 1978-1987.
O.OJ5
o.oso
0.025-
0.020-
0.013-
0.010-
0.003-
CONCENTRATJON, PPM
0.000
•NAAQS'
• NAMS STCS (105) « AajyjE5_(34
—i i 1 1 1 1 —i 1 1 1—
1978 1979 19BO 1981 1982 1983 1984 1985 1986 1987
National trend in the composite average of the annual average sulfur
dioxide concentration at both NAMS and all sites with 95 percent
confidence intervals, 1978-1987.
Figure 4-32
E-19
-------
Source: EPA (1989)
0.07
CONCENTRATION, PPM
0.06-
0.05-
0.04-
0.03-
0.02-
0.01-
0.00
84 SITES
NAAQS
1978 1979 1980 1981 1982 1983 1984 1985 1986 1987
Boxplot comparisons of trends in annual mean nitrogen dioxide
concentrations at 84 sites, 1978-1987.
0.06
CONCENTRATION, PPM
0.05-
0.04-
0.03-
0.02-
0.01 -
0.00
•NAAQS'
i 1 J
NAMS SfTES (U) o ALLSniSj8_4)_
1978 1979 1980 1981 1982 1983 1984 1985 1986 1987
National trend in the composite average of nitrogen dioxide
concentration at both NAMS and all sites with 95 percent confidence
intervals, .1978-1987.
Figure 4-33
E-20
-------
Source: EPA (1989)
c
o
X
O
z
35
30-
25-
I 20"
1
I ,,H
10-
5-
1979
g:;:;| Transportation
PU*' Combustion
Industrial Processes
Solid Waste and Misc.
888
ilijg
iH
- ^iyffisfr^^
1980
1981 1982 1983 1984
1985
1986
National Trend in Nitrogen Oxide Emissions, 1979-1986.
c
o
O
O
35-
30-
1986
National Trend in Volatile Organic Compound Emissions, 1979-1986.
Figure 4-34
E-21
-------
Source: EPA (1989)
SOM EMISSIONS, K)1 METRIC TONS/YEAR
1978 1979 1980 1981 1982 1983 1984 1985 1986 1987
National trend in sulfur oxide emissions, 1978-1987.
Figure 4-35
E-22
-------
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ROWLAND FOREST -- APR 16 - OCT 15
FREQUENCY OF CONSECUTIVE HOURS OF OZONE GREATER
THAN 70 PPB BETWEEN THE HOURS 7AM AND 6PM
45 -
40 -
35 -
30 -
25 -
20 -
15 -
10 -
.5 -
0
HORIZONTAL BAR: 1986
HASH BAR: 1987
SOLID BAR: 1988
3456
CONSECUTIVE HOURS
Figure 4-37
MT. MOOSILAUKE SUMMIT -- APR 16 - OCT 15
FREQUENCY OF CONSECUTIVE HOURS OF OZONE GREATER
THAN 70 PPB BETWEEN THE HOURS 7AM AND 6PM
>-
z.
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45 -
40 -
35 -
30 -
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20 -
15 -
10 -
5 -
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HORIZONTAL BAR: 1986
HASH BAR: 1987
SOLID BAR: 1988
....
1 1 I [ 1 1 1
3456
CONSECUTIVE HOURS
Figure 4-38
> =
E-24
-------
WHITEFACE MT. SUMMIT -- APR 16 - OCT 15
FREQUENCY OF CONSECUTIVE HOURS OF OZONE GREATER
THAN 70 PPB BETWEEN THE HOURS 7AM AND 6PM
50
45 -
40 -
35 -
30 -
25 -
20 -
15 -
10 -
5 -
0
HORIZONTAL BAR: 1986
HASH BAR: 1987
SOLID BAR: 1988
3456
CONSECUTIVE HOURS
Figure 4-39
w
Gf
a
Cti
b.
WHITEFACE MT. SUBSITE 3 -- APR 16 - OCT 15
FREQUENCY OF CONSECUTIVE HOURS OF OZONE GREATER
THAN 70 PPB BETWEEN THE HOURS 7AM AND 6PM
50
45 -
40 -
35 -
30 -
25 -
20 -
15 -
10 -
5 -
0
HORIZONTAL BAR: 1986
HASH BAR: 1987
SOLID BAR: 1988
3456
CONSECUTIVE HOURS
Figure 4-40
>= 8
E-25
-------
WHITEFACE MT. SUBSITE 4 -- APR 16 - OCT 15
FREQUENCY OF CONSECUTIVE HOURS OF OZONE GREATER
THAN 70 PPB BETWEEN THE HOURS 7AM AND 6PM
0
3
or
w
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JU —
45 -
40 -
35 -
30 -
25 -
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15 -
10 -
5 -
HORIZONTAL BAR: 1986
HASH BAR: 1987
SOLID BAR: 1988
^^
1 1 1
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1 1 1 1 1 1 I
3456
CONSECUTIVE HOURS
Figure 4-41
7 > =
w
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HUNTINGTON, NY -- APR 16 - OCT 15
FREQUENCY OF CONSECUTIVE HOURS OF OZONE GREATER
THAN 70 PPB BETWEEN THE HOURS 7AM AND 6PM
50
45 -
40 -
35 -
30 -
25 -
20 -
15 -
10 -
5 -
0
HORIZONTAL BAR: 1986
HASH BAR: 1987
SOLID BAR: 1988
345
CONSECUTIVE HOURS
Figure 4-42
E-26
-------
HAMPSHIRE COUNTY, MA -- APR 16 - OCT 15
FREQUENCY OF CONSECUTIVE HOURS OF OZONE GREATER
THAN 70 PPB BETWEEN THE HOURS 7AM AND 6PM
uu —
45 -
40 -
35 -
30 ^
25 -
20 -
15 -
10 -
5 -
HORIZONTAL BAR: 1986
HASH BAR: 1987
SOLID BAR: 1988
•
•1 11 J 11 KB! 1 Hi 1
II 1 1
3456
CONSECUTIVE HOURS
Figure 4-43
o-
BEAVER COUNTY, PA -- APR 16 - OCT 15
FREQUENCY OF CONSECUTIVE HOURS OF OZONE GREATER
THAN 70 PPB BETWEEN THE HOURS 7AM AND 6PM
HORIZONTAL BAR: 1986
HASH BAR: 1987
SOLID BAR: 1988
3 4 5
CONSECUTIVE HOURS
Figure 4-44
E-27
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O"
w
Di
SHENANDOAH SUMMIT -- APR 16 - OCT 15
FREQUENCY OF CONSECUTIVE HOURS OF OZONE GREATER
THAN 70 PPB BETWEEN THE HOURS 7AM AND 6PM
50
45 -
40 -
35 -
30 -
25 -
20
15 -
10 -
5 -
0
HORIZONTAL BAR: 1986
HASH BAR: 1987
SOLID BAR: 1988
I
1 I
3456
CONSECUTIVE HOURS
Figure 4-45
SHENANDOAH SUBSITE 2 -- APR 16 - OCT 15
FREQUENCY OF CONSECUTIVE HOURS OF OZONE GREATER
THAN 70 PPB BETWEEN THE HOURS 7AM AND 6PM
-------
o
z
w
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SHENANDOAH SUBSITE 3 -- APR 16 - OCT 15
FREQUENCY OF CONSECUTIVE HOURS OF OZONE GREATER
THAN 70 PPB BETWEEN THE HOURS 7AM AND 6PM
50
45 -
40 -
35 -
30 -
25 -
20 -
15 -
10 -
5 -
0
HORIZONTAL BAR: 1986
HASH BAR: 1987
SOLID BAR: 1988
I I I I
1
3456
CONSECUTIVE HOURS
Figure 4-47
1
2
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P
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BIG MEADOW, VA -- APR 16 - OCT 15
FREQUENCY OF CONSECUTIVE HOURS OF OZONE GREATER
THAN 70 PPB BETWEEN THE HOURS 7AM AND 6PM
HORIZONTAL BAR: 1986
HASH BAR: 1987
SOLID BAR: 1988
3456
CONSECUTIVE HOURS
Figure 4-48
E-29
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SAWMILL RUN, VA -- APR 16 - OCT 15
FREQUENCY OF CONSECUTIVE HOURS OF OZONE GREATER
THAN 70 PPB BETWEEN THE HOURS 7AM AND 6PM
HORIZONTAL BAR: 1986
HASH BAR: 1987
SOLID BAR: 1988
3456
CONSECUTIVE HOURS
Figure 4-49
CJ>
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w
Cti
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DICKEY RIDGE WARREN COUNTY, VA -- APR 16 - OCT 15
FREQUENCY OF CONSECUTIVE HOURS OF OZONE GREATER
THAN 70 PPB BETWEEN THE HOURS 7AM AND 6PM
HORIZONTAL BAR: 1986
HASH BAR: 1987
SOLID BAR: 1988
3456
CONSECUTIVE HOURS
Figure 4-50
E-30
-------
2
Cd
S
Of
W
Qi
WHITETOP MT. SUMMIT -- APR 16 - OCT 15
FREQUENCY OF CONSECUTIVE HOURS OF OZONE GREATER
THAN 70 PPB BETWEEN THE HOURS 7AM AND 6PM
50
45 -
40 -
35 -
30 -
25 -
20 -
15 -
10
5 H
0
HORIZONTAL BAR: 1986
HASH BAR: 1987
SOLID BAR: 1988
3456
CONSECUTIVE HOURS
Figure 4-51
2
Cd
w
a:
GILES COUNTY, TN -- APR 16 - OCT 15
FREQUENCY OF CONSECUTIVE HOURS OF OZONE GREATER
THAN 70 PPB BETWEEN THE HOURS 7AM AND 6PM
HORIZONTAL BAR. 1986
HASH BAR: 1987
SOLID BAR: 1988
3456
CONSECUTIVE HOURS
Figure 4-52
E-31
-------
MARION SMYTH COUNTY, VA -- APR 16 - OCT 15
FREQUENCY OF CONSECUTIVE HOURS OF OZONE GREATER
THAN 70 PPB BETWEEN THE HOURS 7AM AND 6PM
50
45 -
40 -
35 -
30 -
9=1 -
HORIZONTAL BAR: 1986
HASH BAR: 1987
SOLID BAR: 1988
3456
CONSECUTIVE HOURS
Figure 4-53
w
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UH
MT. MITCHELL SUMMIT -- APR 16 - OCT 15
FREQUENCY OF CONSECUTIVE HOURS OF OZONE GREATER
THAN 70 PPB BETWEEN THE HOURS 7AM AND 6PM
50
45 -
40 -
35 -
30 -
25 -
20 -
15 -
10 -
5
0
HORIZONTAL BAR: 1986
HASH BAR: 1987
SOLID BAR: 1988
3456
CONSECUTIVE HOURS
Figure 4-54
E-32
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Figure 4-55: Ozone exposure - total season, Apr 15 - Oct 15, (Daylight hours 7AM - 6PM)
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Hydrogen PeroxWe Concentration (uM)
Dole we lo« Summn
Figure 4-67 Frequency of occurrence for H202 concentrations in cloud water
collected at the Whiteface, NY and Whitetop, VA MCCP sites.
E-41
-------
a,
a.
O
CS1
O
100
90 -
80 -
70 -
60 -
50 -
40 -
30 -
20 -
10
0
ROWLAND FOREST
WARM SEASONS 1986 - 1988
MEAN OZONE VS. 36-HOUR BACK TRAJECTORY
(7278 SAMPLES)
MAXIMUM OZONE VALUE FOR EACH SECTOR BY YEAR
36 33 37 27 32 35 64 34
48 48 54 64 69 76 69 61
41 65 57 58 79 98 90 75
346
360 425
361 1131 2067
1886 702
I I I I
0-45 45-90 90-135 135-180 180-225 225-270 270-315 315-360
MEAN: 28.3 STANDARD DEVIATION: 14.5
36-HOUR BACK TRAJECTORY
Figure 5-1
1986
1987
1988
n,
OH
W
2:
o
tsi
o
100
90
80
70
60
50
40
30
20
10
0
MT. MITCHELL SUMMIT
WARM SEASONS 1986 - 1988
MEAN OZONE VS. 36-HOUR BACK TRAJECTORY
(8684 SAMPLES)
MAXIMUM OZONE VALUE FOR EACH SECTOR BY YEAR
94 98 91 93 92 111 97
90 86 78 83 91 93 85
143 116 123 84 116 115 132
1051
1629
1035 558
560
980
1680
100
105
145
1191
1 T I I I
0-45 45-90 90-135 135-180 180-225 225-270 270-315 315-360
MEAN: 54.9 STANDARD DEVIATION: 18.9
36-HOUR BACK TRAJECTORY
Figure 5-2
E-42
1986
1987
1988
-------
.a
c-
Cd
o
CO
MEAN
MT. MOOSILAUKE SUMMIT
WARM SEASONS 1986 - 1988
OZONE VS. 36-HOUR BACK TRAJECTORY
(5602 SAMPLES)
100
90
80
70
60
5.0
40
30
20
10
0 •
MAXIMUM OZONE VALUE FOR EACH SECTOR BY YEAR
48 31 44 44 48 61 57
63 74 82 94 88 102 98
68 60 71 74 109 127 113
45
67
56
199
321
332
293
758
1212
1702
785
T I I \ \I
0-45 45-90 90-135 135-180 180-225 225-270 270-315 315-360
MEAN: 47.5 STANDARD DEVIATION: 17.8
36-HOUR BACK TRAJECTORY
Figure 5-3
1986
1987
1988
,£>
a,
a,
DJ
z.
o
[S!
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100
90
80
70
60
50
40
30
20
10
0
SHENANDOAH SUMMIT
WARM SEASONS 1986 - 1988
MEAN OZONE VS. 36-HOUR BACK TRAJECTORY
(7944 SAMPLES)
MAXIMUM OZONE VALUE FOR EACH SECTOR BY YEAR
34 32 29 31 45 48 49
98 83 82 75 81 90 99
81 77 79 96 87 135 132
583
474
697
1850
2382
248
224
38
90
140
1486
I I \ \ 1 I I
0-45 45-90 90-135 135-180 180-225 225-270 270-315 315-360
MEAN: 43.7 STANDARD DEVIATION: 19.7
36-HOUR BACK TRAJECTORY
Figure 5-4
E-43
1986
1987
' 1988
-------
ft
a.
2
O
C-J
O
100
90
80
70
60
50
40
30
20
10
0
WHITEFACE MT. SUMMIT
WARM SEASONS 1986 - 1988
MEAN OZONE VS. 36-HOUR BACK TRAJECTORY
(6548 SAMPLES)
MAXIMUM OZONE VALUE FOR EACH SECTOR BY YEAR
57 69 64 69 81 86 70
66 57 72 83 97 104 85
79 58 53 75 102 135 133
623
1960
324
325
166
23 1
54
61
66
I I I I I
0-45 45-90 90-135 135-180 180-225 225-270 270-315 315-360
MEAN: 48.5 STANDARD DEVIATION: 18.1
36-HOUR BACK TRAJECTORY
Figure 5-5
1986
1987
1988
w
•z.
O
IS!
O
100
90
80
70
60
50
40
30
20
10
0
WHITETOP MT. SUMMIT
WARM SEASONS 1986 - 1988
MEAN OZONE VS. 36-HOUR BACK TRAJECTORY
(10319 SAMPLES)
MAXIMUM OZONE VALUE FOR EACH SECTOR BY YEAR
91 82 74 88 96 110 88
102 106 93 98 104 111 124
163 112 103 86 104 105 109
917
736
1058
359
533
2450
2399
103
111
144
1867
I I I I I I T
0-45 45-90 90-135 135-180 180-225 225-270 270-315 315-360
MEAN: 55.4 STANDARD DEVIATION: 22.1
36-HOUR BACK TRAJECTORY
Figure 5-6
E-44
1986
1987
1988
-------
O
2
Cd
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or
cd
K
Ex.
100
90
80
70
60
50
40
30
20
10
0
ROWLAND FOREST
WARM SEASONS 1986 - 1988
FREQUENCY OF OZONE CONCENTRATION VS.
36-HOUR BACK TRAJECTORY
(OZONE >= 70 ppb)
(68 out of 7278 samples)
III! I 1 I
0-45 45-90 90-135 135-180 180-225 225-270 270-315 315-360
36-HOUR BACK TRAJECTORY
Figure 5-7
>-
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2
Cd
Cd
Pi
fc,
100
90
80
70
60
50
40
30
2Q
10
0
MT. MITCHELL SUMMIT
WARM SEASONS 1986 - 1988
FREQUENCY OF OZONE CONCENTRATION VS.
36-HOUR BACK TRAJECTORY
(OZONE >= 70 ppb)
(1585 out of 8684 samples)
I I I 1 I
0-45 45-90 90-135 135-180 180-225 225-270 270-315 315-360
36-HOUR BACK TRAJECTORY
Figure 5-8
E-45
-------
01
100
90
80
70
60
50
40
30
20
10
0
MT. MITCHELL SUMMIT
WARM SEASONS 1906 - 1988
FREQUENCY OF OZONE CONCENTRATION
36-HOUR BACK TRAJECTORY
(OZONE >= 100 ppb)
VS.
(215 out of 8684 samples)
r r i i \^ r i
0-45 45-90 90-135 135-180 180-225 225-270 270-315 315-360
36-HOUR BACK TRAJECTORY
Figure 5-9
CJ>
oz
CL.
100
90 -
80 -
70 -
60 -
50 -
40 -
30 -
20 -
10 -
0
MT. MOOSILAUKE SUMMIT
WARM SEASONS 1986 - 1988
FREQUENCY OF OZONE CONCENTRATION VS.
36-HOUR BACK TRAJECTORY
(OZONE >= 70 ppb)
(638 out of 5602 samples)
I T I
0-45 45-90 90-135 135-180 180-225 225-270 270-315 315-360
36-HOUR BACK TRAJECTORY
Figure 5-10
E-46
-------
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2
w
3
Of
w
ca
100
90 -
80 -
70 -
60 -
50 -
40 -
30 -
20 -
10 -
0
MT. MOOSILAUKE SUMMIT
WARM SEASONS 1986 - 1988
FREQUENCY OF OZONE CONCENTRATION VS.
36-HOUR BACK TRAJECTORY
(OZONE >= 100 ppb)
(66 out of 5602 samples)
I I 1
0-45 45-90 90-135 135-180 180-235 225-270 270-315 315-360
CJ>
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or
ta
ca
36-HOUR BACK TRAJECTORY
Figure 5-11
SHENANDOAH SUMMIT
WARM SEASONS 1986 - 1988
FREQUENCY OF OZONE CONCENTRATION VS.
36-HOUR BACK TRAJECTORY
(OZONE >= 70 ppb)
(806 out of 7944 samples)
0-45 45-90 90-135 135-180 180-225 225-270 270-315 315-360
36-HOUR BACK TRAJECTORY
Figure 5-12
E-47
-------
Cd
100
90
80
70
60
50
40
30
20
10
0
SHENANDOAH SUMMIT
WARM SEASONS 1986 - 1986
FREQUENCY OF OZONE CONCENTRATION VS.
36-HOUR BACK TRAJECTORY
(OZONE >= 100 ppb)
(47 out of 7944 samples)
I I I I
0-45 45-90 90-135 135-180 180-225 225-270 270-315 315-360
36-HOUR BACK TRAJECTORY
Figure 5-13
o
•z.
100
90
80
70
60
50
40
30
20
10
0
WHITEFACE MT. SUMMIT
WARM SEASONS 1986 - 1988
FREQUENCY OF OZONE CONCENTRATION VS.
36-HOUR BACK TRAJECTORY
(OZONE >= 70 ppb)
(840 out of 6548 samples)
[ \ I I I T I
0-45 45-90 90-135 135-180 180-225 225-270 270-315 315-360
36-HOUR BACK TRAJECTORY
Figure 5-14
E-48
-------
w
^>
= 100 ppb)
1 UU —
90 -
80 -
70 -
60 -
50 -
40 -
30 -
20 -
10 -
(84 out of 6548 samples)
Y/////^
%%&
%%%'
mz
•0%%,
Wj^
%£/>>?
1 1 1 1 1 1 1 •
0-45 45-90 90-135 135-180 180-225 225-270 270-315 315-360
36-HOUR BACK TRAJECTORY
Figure 5-15
= 70 ppb)
(2511 out of 10319 samples)
1 I I I I I
0-45 45-90 90-135 135-180 180-225 225-270 270-315 315-360
36-HOUR BACK TRAJECTORY
Figure 5-16
E-49
-------
or
Cd
K
Ci-
ts
100
90 -
80 -
70 -
60 -
50 -
40 -
30 -
20 -
10 -
0
WHITETOP MT. SUMMIT
WARM SEASONS i9ae - 1988
FREQUENCY OF OZONE CONCENTRATION VS.
36-HOUR BACK TRAJECTORY
(OZONE >= 100 ppb)
140 out of 10319 samples)
ii i r^ i i
0-45 45-90 90-135 135-180 180-225 225-270 270-315 315-360
36-HOUR BACK TRAJECTORY
Figure 5-17
E-50
-------
WHITEFACE MT. SUMMIT
WARM SEASONS 1986 - 1988
MEAN H202 VS. 36-HOUR BACK TRAJECTORY
(697 SAMPLES)
— ~
r* -
c~
c
C-J
S
iu -
9 -
8 -
7 -
6 -
-
4 -
3 -
2 -
-
1 -
UAXIUUU H202 VALUE FOR EACH SECTOR BY YEAR
ND ND ND ND ND ND ND ND
2.2 1.2 1.1 2.5 4.3 4.2 3.1 6.5
ND ND 1.2 0.9 4.3 1.6 1.5 1.4
91 136
54 246 96
.,,,,,,. %%$^ %%&'
\^/^/^( V/S/f/ZA W/fXA \%%Z& '%%%' '%%%• \%Z%& \%%%$.
1 1 1 1 1 1 1
1986
1987
1986
MEAN: 0.8 STANDARD DEVIATION: 0.7
36-HOUR BACK TRAJECTORY
ND: No Data Available
Figure 5-18
.0
c.
c.
CM
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O
CO
W
s
10
9
8
7
6
5
4
3
2
1
0
ROWLAND FOREST
WARM SEASONS 1986 - 1988
MEAN S02 VS. 36-HOUR BACK TRAJECTORY
(2426 SAMPLES)
UAX1UUM S02 VALUE FOR EACH SECTOR BY YEAR
ND ND ND ND ND ND ND ND
3.4 2.7 3.1 1.6
2 7 1.8 2 3
71 77 53 59
1 1 1 1
7 8 3.7 2.5
7 6.3 5.4 6.1
431 674 ,_.,
HH HH ^^
1 1 1
1986
1987
1986
0-45 45-90 90-135 135-180 180-325 225-370 270-315 315-360
MEAN: 1 STANDARD DEVIATION: 1
36-HOUR BACK TRAJECTORY
ND: No Data Available
Figure 5-20
o
CO
10
9
8
7
6
5
4
3
2
1
0
MT. MITCHELL SUMMIT
WARM SEASONS 1986 - 1988
MEAN S02 VS. 36-HOUR 'BACK TRAJECTORY
(3623 SAMPLES)-
MAXIMUM
ND ND
58 26
24 7 7.8
S02 VALUE FOR
ND ND
12.6 10.9
12.9 5.8
EACH SECTOR BY YEAR
ND ND ND
10 8.8 5.6
10 13.9 13.9
549
577
365
343 297
ND
8 4
14
429
I I I I I II
0-45 45-90 90-135 135-180 180-325 325-370 270-315 315-360
MEAN: 2.6 STANDARD DEVIATION: 2
36-HOUR BACK TRAJECTORY
ND: No Data Available
Figure 5-21
E-52
1986
1987
1988
-------
.0
C.'
C.
OJ
O
1/3
WHITEFACE MT. SUMMIT
WARM SEASONS 1986 - 1988
MEAN S02 VS. 36-HOUR BACK TRAJECTORY
(4664 SAMPLES)
1 U -
9 -
8 -
7 -
6 -
5 -
4 -
3 -
•
MAXIMUM S02 VALUE FOR EACH SECTOR BY
3 1.8 1.8
1.4 1.7 1.1
6 0.7 0.6
235 I5fi 10g
I 1 1
3.3
6.9
1.6
184
HH
1
8.8
13.1
13.1
496
Up
1
10.1
20.5
16.3
1394
HP
YEAR
1
14.2
11.5
10.4
1575
i^
1 9
4
4.3
51 ^
1 O
T
1986
1987
1988
0-45 45-90 90-135 135-180 180-225 225-270 270-315 315-360
MEAN: 1.2 STANDARD DEVIATION: 1.8
36-HOUR BACK TRAJECTORY
ND: No Data Available
Figure 5-22
CM
O
OJ
10
9
8
7
6
5
4
3
2
1
0
WHITETOP MT. SUMMIT
WARM SEASONS 1986 - 1988
MEAN S02 VS. 36-HOUR BACK TRAJECTORY
(7483 SAMPLES)
MAXIMUM S02 VALUE FOR EACH SECTOR BY YEAR
ND ND ND ND ND ND ND
18.5 10.5 2.5 15.5 21.5 16.5 21.5
30 5 18.5 9.5 3.5 21.5 14.5 30.5
699
ND
47.5
20.5
1462
534 805 1596
259 426
1986
1987
1988
0-45 45-90 90-135 135-180 180-225 225-270 270-315 315-360
MEAN: 8.2 STANDARD DEVIATION: 2.4
36-HOUR BACK TRAJECTORY
ND: No Data Available
Figure 5-23
E-53
-------
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