EPA-600/4-79-039
June 1979
RAPID TECHNIQUES FOR CALCULATING
THE POLLUTANT STANDARDS INDEX' (PSI)
Revised June 1979
by
Lance A. Wallace
and
Wayne R. Ott
Monitoring Technology Division
OFFICE OF MONITORING AND TECHNICAL SUPPORT
OFFICE OF RESEARCH AND DEVELOPMENT
U.S. ENVIRONMENTAL PROTECTION AGENCY
WASHINGTON, D.C. 20460
-------
DISCLAIMER
This report has been reviewed by the Office of Research and Development,
U.S. Environmental Protection Agency, and approved for publication. Mention
of trade names or commercial products does not constitute endorsement or
recommendation for use.
ii
-------
FOREWORD
Monitoring activities provide the most important quantitative information
available on the state-of-the-environment, thereby providing a scientific
measure of the impact of environmental regulatory actions. To generate valid
monitoring data, research is necessary to evaluate and improve measuring
instruments and techniques, develop criteria for designing monitoring networks,
carry out effective statistical analyses of monitoring data, and give technical
support to field monitoring activities. The Environmental Protection Agency's
(EPA's) Office of Research and Development (ORD) carries forward a broadly
based national research program in air pollution, water pollution, and other
environmental topic areas. Within ORD, the Office of Monitoring and Technical
Support oversees research and policies concerned with monitoring quality
assurance, measurement methods evaluation, advanced monitoring techniques, and
improved methods for analyzing and handling environmental data.
This report is intended to provide technical aids that will assist State
and local agencies in computing a nationally uniform air pollution index, the
Pollutant Standards Index. Use of this index by air pollution control agencies
is covered under regulations promulgated by EPA in August 1978, as required
by the Clean Air Act Amendments of 1977 (P.L. 95-95).
The report was first issued in March 1978. With EPA's decision to amend
the National Ambient Air Quality Standard for ozone (Federal Register,
February 8, 1978), this report was revised and reissued in June 1979.
iii
-------
ABSTRACT
Rapid techniques for calculating the Pollutant Standards Index (PSI) for
daily public reporting of air quality are discussed. A complete set of
original nomograms for calculating the PSI in gravimetric or volumetric units
is presented. The nomograms are recommended for use by all State and local
air pollution control agencies as ammeans of determining the PSI rapidly and
accurately. Examples of linear and logarithmic graphs for calculating the
PSI are also included.
Tables for rapidly identifying the critical pollutant on a given day and
automatically determining its PSI value to the nearest unit are listed in
Appendix A. Tables A-2 and A-4 list the precise pollutant concentrations
corresponding to consecutive unit values of PSI between 1 and 500, and can,
therefore, provide the definitive verification of estimates of PSI obtained
from the nomograms or other graphs. Computer programs for creating these or
similar tables appear in Appendix B.
The first edition of this report covered the period from July 1977 to
February 1978 and work was completed March 1978. The revised edition covered
the period through May of 1979 and work was completed in June of 1979.
iv
-------
CONTENTS
Foreword ill
Abstract iv
List of Figures vii
List of Examples vii
I. Introduction 1
II. Structure of the PSI 3
III. Graphical Techniques 6
Linear Graphs 6
Logarithmic Graphs 6
Nomograms 8
IV. Tabular Forms 21
"Rapid Survey" Tables (A-l and A-3) 21
"Working" Tables (A-2 and A-4) 22
"Reference" Tables (A-5 through A-15) 24
References 26
Appendix A - Tables for Computing the Pollutant Standards
Index (PSI) 27
Tables
A-l "Rapid Survey" Table: Pollutant Concentrations for
PSI = 5-200 in Steps of 5 28
A-2 "Working" Table: Pollutant Concentrations for
PSI = 0.5-199.5 29
A-3 "Rapid Survey" Table: Pollutant Concentrations for
PSI = 200-500 in Steps of 5 33
A-4 "Working" Table: Pollutant Concentrations for
PSI = 200.5-499.5 35
A-5 "Reference" Table. PSI Values for CO (pg/m3) at
Equally Spaced Concentrations 45
A-6 "Reference" Table: PSI Values for CO (ppm) at
Equally Spaced Concentrations 46
A-7 "Reference" Table: PSI Values for 03 (yg/m3) at
Equally Spaced Concentrations 47
A-8 "Reference" Table: PSI Values for 03 (ppm) at
Equally Spaced Concentrations 48
A-9 "Reference" Table: PSI Values for N02 (yg/m3) at
Equally Spaced Concentrations 49
A-10 "Reference" Table: PSI Values for N02 (ppm) at
Equally Spaced Concentrations 50
-------
Appendix A - Tables for Computing the Pollutant Standards
Index (PSI) [cont'd]
Tables
A-ll "Reference" Table: PSI Values for S02 (ppm) at
Equally Spaced Concentrations 51
A-12 "Reference" Table: PSI Values for SCg (yg/m3) at
Equally Spaced Concentrations 52
A-13 "Reference" Table: PSI Values for TSP (yg/m3) at
Equally Spaced Concentrations 53
A-14 "Reference" Table: PSI Values for TSP x S02 (ppm yg/m3) at
Equally Spaced Concentrations 54
A-15 "Reference" Table: PSI Values for TSP x S02 (yg/m3) at
Equally Spaced Concentrations 55
Appendix B - Computer Programs for Calculating the Pollutant
Standards Index (PSI) Tables 56
B-l. Program for Producing "Rapid Survey" and
"Working" Tables (Tables A-l to A-4, or
desired variations) for Rapid Calculation
of PSI 57
B-2. Program for Producing "Reference" Tables of PSI
Values for Individual Pollutants (Tables A-5
through A-15, or desired variations) 60
vi
-------
LIST OF FIGURES
Number Page
1 Example of PSI subindex function for CO plotted on
linear graph paper ... 7
2 Example of log-log plot of PSI subindex for
TSP 9
3 PSI nomogram for CO, 03, S02 , and TSP in gravimetric units . . 11
4 PSI nomogram for N02 , TSP x S02, COH, and COH x S02 in
gravimetric units 13
5 PSI nomogram for CO, 03, S02, and TSP in volumetric units . . 15
6 PSI nomogram for N02, TSP x S02, COH, and COH x S02 in
volumetric units 17
7 Illustration of nomogram: TSP concentration of 277 yg/m3
corresponds to PSI value of 115, to the nearest unit .... 20
LIST OF EXAMPLES
1 Comparison of Standard Tables (requiring interpolation)
With Half-Integer Tables Allowing Immediate Determination
of PSI 23
2 How to Use Tables A-2 and A-4 24
vii
-------
I. INTRODUCTION
In May 1974, Thorn and Ott1 began a national survey of existing air
pollution indicesthose in the literature and those in use by air pollution
control agencies throughout the United States and Canada. The survey,
published in 1976, identified the structural characteristics of a candidate
national uniform air pollution index.2'3 In September 1976, the Environmental
Protection Agency (EPA) formally adopted an air pollution index based upon
this structure, the Pollutant Standards Index (PSI).1*'5
The PSI was intended to be used by State and local air pollution control
agencies for reporting air quality data to the public on a daily basis. At
that time, its use by air pollution agencies was completely optional, and a
number of agencies adopted it.6 With passage of the Clean Air Act Amendments
of 1977, the PSI has been given greater importance. Section 309 of the
Clean Air Act Amendments requires that a national air quality monitoring
system be established using a uniform air quality index.
Air pollution index reports generally should be made as current as
possible, since the public has little interest in reports that are more
than a day old. Thus, a need arises for effective techniques to assist the
engineer, data analyst, or field technician in rapidly calculating the PSI on
a routine basis.
When the PSI was initially published,5 graphs of its subindices were
included to aid in its calculation. Subsequent reports from air pollution
control agencies made it apparent that other computational aids for the PSI
were needed. In February 1977, Severn developed a PSI manual containing
logarithmic plots for use by the Baltimore Division of Air Pollution Control.
The manual consisted of over 20 pages of explanatory materials and graphs
for calculating the PSI. In April 1977, Zorbini9 presented an 11-page
table compiled by the North Ohio Valley Air Authority (NOVAA). The table
contained integer PSI values and the corresponding concentration values for
each pollutant. Other agencies throughout the United States have indicated
a similar need for a means of computing the PSI accurately and conveniently
from available air monitoring data.
To meet these needs, we have prepared several new computational aids.
Foremost among these is the PSI nomogram, which enables the PSI to be
calculated rapidly using a pair of charts. This report presents the PSI
nomograms for all combinations of pollutants and concentration units.
A second computational approach of importance is the use of tables.
A novel departure from most tables has been employed here that unambiguously
denotes the PSI to the nearest unit. This approach is somewhat different than
that originally proposed by NOVAA, although their original effort contributed
-------
many ideas to the approach taken in this report. Although tables are some-
times unwieldy, they provide the highest precision of any computational aids
available, and are useful as references. Finally, computers, minicomputers,
and programmable hand calculators afford still another way for computing the
index. A FORTRAN computer program to assist the engineer and computer
programmer in adapting the PSI to a particular installation is presented in
another report. ^ Computer approaches are extremely rapid and precise, but
they require data processing equipment that may not be available at some
installations.
Within EPA, we have experimented with a variety of techniques for
calculating the PSI. The remainder of this report describes each technique,
discusses its advantages and disadvantages, and provides a complete
presentation of graphs, nomograms, and tables for reference purposes.
Additional documentation, including computer programs for making tables, is
given in the appendices.
Readers seeking additional information on PSI can obtain the EPA
guideline report,5 or the report on the computer program,-^ by writing to
the Environmental Protection Agency Library, MD-35, Research Triangle Park,
North Carolina 27711. The history of PSl's development, along with examples
of the application of PSI to actual data and the theoretical basis of various
air and water pollution index structures, have been summarized in a book.l-'-
Although this report was first issued in March 1978 as "Rapid Techniques
for Computing the Pollutant Standards Index," the revision of the National
Ambient Air Quality Standard for Ozone has necessitated some changes in the
nomograms and tables. These changes have been incorporated into this revised
edition.
-------
II. STRUCTURE OF THE PSI
The PSI is based upon the Federal National Ambient Air Quality Standards
(NAAQS); Episode criteria (Alert, Warning, and Emergency); and Significant
Harm levels that have been established for the various air pollutants. It
includes six pollutants: carbon monoxide (CO) , sulfur dioxide (SC>2 ), total
suspended particulates (TSP), photochemical oxidants (principally Os),
nitrogen dioxide (NC^), and Coefficient of Haze (COH). Combinations of
pollutants as they appear in the Code of Federal Regulations are also
included: S02 x TSP and COH x SC^ . Each pollutant is represented mathemati-
cally in the index by a segmented linear function* called a "subindex." Each
subindex relates the observed short-term (24 hours or less) concentration to
the subindex value in Table 1:
Table 1
BREAKPOINTS FOR PSI SUBINDICES
Concentration Subindex Value
50% of NAAQS** 50
NAAQS 100
Alert 200
Warning 300
Emergency 400
Significant Harm 500
One set of breakpoints - TSP x SC>2 in (pg/m3) (ppm) - does not appear
in the Federal Register and was newly calculated for the PSI. The
conversion factor employed in determining the TSP x S02 breakpoints was the
following:
1 ppm SOj = 2619 yg/m3
(at 25°C and 760mm)
*A segmented linear function consists of successive straight line segments
joined at their end points, or "breakpoints."
**For S02 and TSP, the annual NAAQS are used at this level and are interpreted
on a 24-hour basis.
-------
This value was based in turn on the following physical constants:
Absolute zero = -273.15°C
Atomic wt. of 0 = 15.9994
Atomic wt. of S = 32.06
Gas constant R = 0.08205 atm-liters/mole °K
The resulting breakpoints for TSP x S02, correct to 4 significant figures are:
Episode Level PSI TSP x SO (ppm pg/m3)
"- ' 2
Alert 200 24.82
Warning 300 99.66
Emergency 400 150.1
Significant Harm 500 187.1
All other breakpoints are found in the Federal Register and also appear
in Tables A-l and A-3. (However, the breakpoints for COH are based upon the
"standard" conversion factor between COH and TSP and should be used only if
no site-specific conversion factor is available.)
For any given day, the value of the PSI is simply the largest value of
the subindices. Mathematically,
PSI = Max
j Ij , Ij , ...
where Ij denotes the first subindex, I2 denotes the second subindex, and so
on. Usually, n = 5. In the current version of the proposed Federal
regulation on PSI, a pollutant can be deleted if measurements indicate that
PSI values are below PSI = 50 for an extended time period (for example, a
season or a year). When the PSI is reported, the pollutant responsible, or
the "critical" pollutant, also is identified. If two or more subindices
exceed 100, all such pollutants should be identified.
The PSI values are characterized by five health-related terms (Table 2):
Table 2
Range Descriptor Category
0
-------
A typical report on radio or television might consist of the following
statement: "Today's air quality index is 120; the air quality is 'unhealthful';
and the pollutant responsible is carbon monoxide." The index also can be fore-
cast a day in advance using such language as, "no significant change,"
"increase," or "decrease."
Units
Two sets of units are commonly used in air quality measurements
gravimetric and volumetric. Gravimetric units are mass per unit volume,
usually expressed as micrograms of substance per cubic meter of air (ug/m3);
volumetric units are volume of gaseous pollutant per unit volume of air, often
expressed as parts per million (ppm) .
The conversion factors between these sets of units are known to about four
significant figures (limited, in the case of SO^, by the variable isotopic
abundance of sulfur in the earth's crust.) However, the standards and episode
levels appearing in the Federal Register have been rounded off to only one or
two (sometimes three) significant figures. Thus, the conversion factors at
these levels are inexact, and there is even a small possibility that a
concentration reported in one set of units will exceed a standard, while if it
is converted correctly to another set of units, it will not exceed the
standard. For example, a CO value of 29.8 ppm measured at reference conditions
is below the "warning" level of 30 ppm, but, when converted correctly to
34.12 mg/m3, exceeds the "warning" level of 34 mg/m3.
Since the PSI is based upon the Federal Register values, it shares this
potential ambiguity. However, there is some indication that the
Federal Register values may be revised in the future to remove this potential
ambiguity. If the Federal Register numbers are revised, then, at that time,
the PSI can be altered to agree with whatever new standards and episode levels
are adopted.
We have provided tables and nomograms in both sets of units for the
convenience of the many agencies measuring gases in volumetric units (ppm).
Many State and local agencies use mixtures of units and will wish to "cut and
paste" the nomograms here to achieve a custom nomogram for their own use.
-------
III. GRAPHICAL TECHNIQUES
Three main graphical techniques are available for calculating the PSI:
linear graphs
logarithmic graphs
nomograms
Each technique has characteristics that may make it desirable for a given
application. The following discussion outlines major advantages and
disadvantages of each method.
Linear Graphs
The most straightforward approach is simply to plot the PSI subindex
values for each pollutant on ordinary graph paper. Since the PSI is a
segmented linear index, only the five or six breakpoints (occurring at PSI
-values of 50, 100, 200, 300, 400, and 500) for each pollutant need to be
plotted. They are then connected by straight lines. For ease of identifying
the proper descriptive word for any pollutant concentration, horizontal lines
may be drawn at the breakpoints to divide the graph into regions corresponding
to the "Good," "Moderate," "Unhealthful," "Very Unhealthful," and "Hazardous"
descriptors. These labels should be written directly on the graph to make
identification of each region as easy and rapid as possible. An example of
such a graph, the CO subindex in ppm, is included in Figure 1.
One advantage of the linear graph is that it can be made with the
simplest materials and is very easy to understand by all users. A disadvan-
tage is that it gives the same space to the seldom-attained upper levels of
the PSI values as to the the more common lower levels. This defect may be
corrected by changing the scale at selected breakpoints, expanding it
between, say, 0 and 100, and compressing it between 200 and 500. However,
such changes of scale increase the complexity of the graph and may cause
occasional misinterpretations.
Logarithmic Graphs
The logarithmic plot has the advantage of expanding the region in which
most readings occur (i.e., PSI<100) thereby increasing the precision in that
region. Before preparing a logarithmic plot for any pollutant, it would be
desirable to inspect its historical valuesif these never go below, say,
10 on the PSI scale, it becomes unnecessary to include the region below
PSI = 10.
-------
500
LU
Q
Z
OQ
ID
CO
V)
a.
400
300
200
100
0
VERY UNHEALTHFUL
0
20 30
CO CONCENTRATION, ppm
(8-hour running average)
40
50
Figure 1. Example of PSI subindex function for CO plotted on linear
graph paper.
-------
In Baltimore, Severn8 prepared logarithmic plots of the PSI for all of
the pollutants. The resulting graphs were enclosed in plastic sheets for
protection and daily use by station personnel. By using two or more scales
along the horizontal axis of the logarithmic graph, two or more pollutants
may be plotted on a single diagram. Figure 2 shows a plot of TSP on
logarithmic graph paper.
Logarithmic graphs may be useful for some applications. However, some
users may find them difficult or time-consuming to prepare and read. In
addition, a number of charts will be required if many pollutants are reported.
Nomograms
Both types of graphs mentioned above have the disadvantage of requiring
the user to locate a concentration on one axis, travel vertically to the
curve of interest, and then travel horizontally to the corresponding PSI
subindex value. This requires considerable attention, and leaves room for
error in both of the "traveling" procedures. A device offering greater
precision with less chance for error is the nomogram.
A nomogram "collapses" the two scales involved (in this case, the PSI
subindex values and the pollutant concentrations) to give a direct represen-
tation on a single line of the relationship between the two sets of numbers.
Each pollutant concentration occurs immediately adjacent to its correspond-
ing PSI subindex, eliminating the "traveling" error described above.
Because the nomogram eliminates much of the wasted space in an ordinary
graph, it has the additional advantage of being able to display a number of
pollutants and their corresponding subindex relationships on a single page.
The major disadvantage of the nomogram is the time it takes to prepare. The
tick marks must be determined precisely, their length and number must be
chosen carefully for maximum ease and rapidity of use, and the draftsmanship
must be painstaking. Since these requirements might be too exacting to allow
many air pollution control agencies to prepare such nomograms, we have
prepared a model nomogram for all pollutants and all systems of units
presently contained in the PSI (See Figures 3-6).
-------
500
400
300
HAZARDOUS
VERY UNHEALTHFUL
UNHEALTHFUL
It
X K
fy 90
Q 80
Z 70
MODERATE
Z
S30
2
GOOD
« mil IIHI mil MIII inn inn ii ii
S
TOTAL SUSPENDED PARTICULATES (TSP), M9/m3
(24-hour average)
Figure 2. Example of log-log plot of PSI subindex for TSP, from Severn.8
-------
PSI
CO
(mg/m3)
NOMOGRAM
S02
(ug/m
(jug/m
5OU-=
3 450-=
o
g 400
< -^
< 350-=
X
300
280-4
_J =
3 270;
^ 260-1
< .=.
UJ =
240=
>- =
230Hi
220-4
210=
190i
180 i
170 |
3 160 i
u_ =
x ;
< =
HI
^ 140-4
D 4
130;
120 =
fc 1
oc ;
U) ~
D 70;
O E
2 1
60 E
GO -
O E
0 1
-o ^
= 67.5
55
50
46
Er-40
=^34
33
32
31
-30
28
27
26
25
23
22
21
20
18
~ 16
: 15
~ 14
~~ 13
1 '2
r 1 1
r
; 6
oou
_=
450^H
300^1
280-4
:
;
260=
;
~
~
:
;
220 i
:
210;
;
:
180;
170=
160-4
:
=
140 =
130 ;
;
110 =
J
80 E
:
60 E
~
=
:
20 E
o =
=1200 -
11000
=900
=800
750
650
~ (inn
550
~" 450
L 390
r 380
i- 370
- 360
r 350
j- 340
'- 330
-
''- 310
: 300
i- 280
1- 270
j- 260
- 250
1- 230
1- 220
'- 210
^200
\- 180
1- 160
H- 150
^- 140
=- 130
'- 120-
i- 110
E 100
- 90
U 80
h 60
- 50
i_ 40
^ 30
^ 20
;- 10
1=
=:
450-^
400
350-=
. _ _ 300 ~
r
280=
I
260-4
r;
220-4
210-E
190i
180 =
170 =
-
160-|
140 E
_^
^
130-^
r
120 E
110 i
~
90^
i
60-^
i
r
==zo*u
2500
2400
=^2300
2200
2100
2000
1800
1700
1600
^1500
S 1300
=1100
E^
~
~ 900
^_
~ 75°
650
~
~ 450
365
=- 350
r~30o
200
=- 150
^ 100
80
- 70
60
= 50
r 40
30
r_ 20
~ 10
450-=
400
350
300-=
J80 I
-
260=
220 |
210;
190i
180 i
170=
160-4
150 =
140-4
130 ;
120-4
110-4
i
90=
;
:
60-^
^=
i
r
30-^
900
875
800
750
Z_ 700
_ 625
~ 450
-400
r 390
I~ 375
- 370
- 360
-
350
- 340
- 330
-
320
_ 31
^300
- 290
-
- 280
-
260
250
E-200
~
^ 80
- 70
50
- 40
- 20
- 10
Report No. EPA-600/4- 79-039
Figure 3. PSI nomogram for CO,
Og, SC>2, and TSP, expressed in gravimetric units.
11
-------
PSI NOMOGRAM
ZARDOUS
VERY UNHEALTHFUL HA
NO2
400
300^
290 6
280
:
270
260 i
240 --3
230
220
3500
=~ 3000
2500
2260
r 2200
[-- 2100
1 2000
J 1900
i 1800
l~ 1 700
= 1500
r 1400
1 uoo
= 1200
TSP
(iig/m
450
400
300
290
280
270
260
250
240
230
220
210
?nn
x SO2
2
) (OOO's)
_.., >ian
=:
..T.
\
=
450
-- 393
350
^ 300
__- 261
= 250
i- 240
' 230
- 220
=- 210
= 200
\~ 190
§- ISO
|- 170
~ 160
\ 150
=- 140
f- 130
=~ 120
E- 110
r 100
;- 90
~ 80
r- 70
~ fi
-------
PSI NOMOGRAM
CO
(ppm)
600 __ SO
Z> 450-=
0 -=
O
tr 400-=
< -EE
< 360-=
I -=
300^
-
-
~E
i
1 =
LJ. Jj
I E
< H
Z -i
> J
DC E
^ E
i
E
-
z
180;
-
170 f
_J _=.
O E
< 150 -
2 ^
i 14°-i
3 --
130 |
ODERATE |
1
03 to <
O O <
mlMiiiiiiilmiliiiiliml
60-4
40 =
§ 304
o -E
0 20-|
10 i
ES 45
EE 40
EE 35
=30
29
28
26
25
23
- 22
20
19
17
i 16
-
E M
_
E 13
-
E 11
-
-
I 10
-
r.
:=
i a
h
i 7
1 6
i 5
1 4
h~ 3
| 2
i 1
<>3
(ppm)
600-= 0.60-
450-=
400-=
350-=
300-=.
190 i
-
180 E
;
170 |
~
~
;
-
140 E
I
130 i
:
=
90 |
80 |
60=
40=
30|
20 |
10 I
n =
0.55
0.50
0.45
=0.40 -
=- 0.37
p- 0.33
p- 0.31
S- 0.29
S- 0.27
S 0.25
r
E- 0.19
: 0.18
§-
E- 0.17
\_
-
^~
E 0.15
i-
I
E 0.13
~
| o.n
i-
| o.io
! 0.08
EL.
| 0.07
1 0.04
I 0.02
=-
|- 001
= n n
S02
(ppm)
KOO . 1 .0
450-=
400-=
35O
300-=
E
=
-
-
z
-
-
180 E
170-^
~
~E
Z
140E
130=
:
90 f
80 |
60 |
40 =
30 |
20 |
io|
o =
EEEH0.90
EEE-0 80
0.70
0.60
E MO
EEo^o
=^-0.35
|- 0^9
E- 0^8
E- 0^7
^-H125
=- 0.24
=- 023
5~ 0.21
= tt20
=- 0.19
1- 0.16
E 0.15
0.13
0.12
0.11
0.10
0.09
0.08
0.07
0.06
0.05
0.04
' 0.02
-
' 0.01
-
TSP
(jug/m3)
50°^ 100°
450 ^=j
400^
350-=
300-^=
180^
170^
160 E
140=
130=
90-^
80 |
-
60 |
40
30 i
20-|
10-^
o =
950
900
- 875
- 800
750
700
- 625
P~
390
~ 375
370
_ 360
-
350
- 340
- 330
- 320
- 310
- 290
- 280
- ?70
£7 250
~- 100
- 80
- 70
- 60
50
- 40
- 30
- 20
- 10
o
Report No. EPA-600/4-79-039
Figure 5. PSI nomogram for CO, 03,
S02, and TSP, expressed in volumetric units.
15
-------
NO.
PSI NOMOGRAM
TSPxSO2 COM
COHxSO
(ppm)
CO ^
0 450^
Q ==
OC 400
< 3
N 350-=
< 350 _
I
290-^
3 4
i 27H
< J
UJ =
I 250 _
z -=
>- ,, =
oc 23° =
> 220=
onn
19
1.8
I./
1 6
1.5
r_ , |
~ 10
f
~_ 07
n s
(ppm- jjg/m^)
450^
400
~_
290 i
270=
-
220^
180
170
160
150 1
140
~ 130
120
no
=- 95
E 90
= 80
^- 75
B- 65
~ 60
~ 45
5 40
=- 35
~ 30
74 ft
450^=
400^?
'290-=
270:
220 f
9nn -
75
7 0
i- 9
S- 8
=- 7
- 5
=r- 4
i- 3
%~ '
E- 39
=- 37
=- 34
=- 33
=r~ 3 1
(ppm)
450^
400-^
-=
290-^
270 i
220
210
1 4
1 2
1 1
H- 0.75
07
I- 065
E 0 6
055
0 45
r
r- 0.3
r 0.25
" 0 2
Report No. EPA-600/4-79-039
Figure 6. PSI nomogram for NO2, TSP x S02, COM, and COM x S02, expressed
in volumetric units.
17
-------
Uses of the Nomogram
The main use of the nomogram is expected to be as a calculational aid.
Daily readings of pollutant concentrations would be checked against the PSI
subindex scales to determine the highest reading. The information would be
written down elsewhere, the nomogram remaining unmarked for use on succeeding
days.
A second possible use of the nomogram has been suggested. Some agencies
may wish to use copies of the nomogram as permanent records of each day's
pollutant concentrations. All pollutants measured that day would have their
levels checked or circled on the nomogram. The PSI value for that day would
be determined from the highest subindex and reported elsewhere in the usual
fashion. Copies of the nomogram could be carried on a clipboard for use at
the monitoring station. Each copy would then be dated and signed by the
technician making the reading. The copies could be kept in a binder to form
a permanent record of a year's air quality at each station. Then, if ques-
tions came up regarding possible errors, or knowledge of the PSI subindex
for a particular pollutant was felt to be important, the complete record
would be available. However, it is recognized that this procedure may be
somewhat wasteful of space.
How to Use the NomogramThe basic use of the nomogram is to
determine the PSI value for any given pollutant concentration. The left-
hand side of each strip contains tick marks corresponding to each unit
between 1 and 500 on the PSI scale (or between 200 and 500 for those
pollutants that have no national ambient air quality standards). Since
levels above 300 are rarely achieved, the range between 300 and 500
has been compressed so that each tick mark corresponds to five PSI units.
(If greater precision is required in this 300-500 range, the user may
consult Table A-4.)
The right-hand side of each strip contains tick marks corresponding
to intervals of different sizes, depending upon the pollutant. To deter-
mine the PSI value corresponding to an observed pollutant concentration,
locate the two values just above and below the observed value by interpo-
lation, and read the PSI value off the left-hand side. Figure 7 illustrates
the technique of using the nomogram. In the Figure, assume that an observed
concentration of TSP is 277 yg/m3. Since 277 is about two-fifths of the way
between 275 and 280 (the closest values explicitly indicated on the nomogram),
then the nearest PSI value would be 115 (the number corresponding to this
interpolated value).
19
-------
TSP
1
ID
LL
X
r-
LU
I
z
D
LU
h-
<
DC
LU
Q
O
S
Q
O
O
e?
(jug/m3)
-
130 E
-E
1 *» «
PSI = 115 ^J-J> -i
,* 1^^
1^ ^^ ~~
1 0 -=
inn -
IUU _
90 E
80 |
-=
70 |
..
60 |
50 =
a r\
4O _
E:
30 |
*? n ~
^U _
10 |
_ z:
r» ^
300
- 290
- 280
_^ TSP = 277 jug/m3
- 270
ofin
_ £Dw
=7 250
r 200
5-
E- 150
1/^ /^
0 0
- 80
- 70
f f*i
60
50
- 40
if\
JU
- 20
- 10
n
Figure 7. Illustration of nomogram: TSP concentration of 277 pg/m3 corresponds to
PSI value of 115, to the nearest unit.
20
-------
IV. TABULAR FORMS
Tables provide the definitive values for the PSI subindices and are,
therefore, necessary for reference purposes. Well designed tables can be
used also for rapid calculation of the PSI, although highly detailed tables
take up several pages and may be unwieldy compared to the nomogram. Appendix
A includes three sets of tables:
Tables A-l and A-3
"Rapid Survey" tables for finding the critical pollutant
(the one with the highest PSI value) for any one day.
Tables A-2 and A-4
"Working" tables for determining the PSI to the nearest
unit rapidly and unambiguously.
Tables A-5 through A-15
"Reference" tables giving values of the PSI associated
with a range of concentrations for each pollutant
individually.
How to Use the Tables
"Rapid Survey" Tables
Table A-l. This table gives values of the PSI from 5-200 (in incre-
ments of five) for all of those pollutants with National Ambient Air Quality
Standards: CO, 03, S02, and TSP. The table provides a swift way of
comparing concentrations for each, pollutant on any one day and determining
which pollutant has the maximum PSI value for that day. To determine the
exact PSI value for that day, the user can then look up that pollutant
only in the more detailed "Working" Table A-2. For example, assume the
following values for the four pollutants on a certain day: CO = 4.0 ppm,
Os = 0.048 ppm, S02 = 0.028 ppm, and TSP = 67.5 yg/m3. Table A-l shows
that the PSI subindices for the four pollutants are as follows: CO = less
than 45; 03 =40; SCv> = more than 45; and TSP, exactly 45. Thus SOs is
the critical pollutant for that day and a look at Table A-2 shows that
the PSI value for that day is 47.
Table A-3. This table gives values of the PSI from 200-500, also in
increments of five for all pollutants with episode levels as defined in the
Federal Register. On those occasions when Alert levels are exceeded,
Table A-3 may be used to determine the pollutant or combination of
21
-------
pollutants with the highest PSI subindex. For example, if the values on
one day were TSP = 300 yg/m3, S02 = .10 ppm, and N02 = 1190 yg/m3, then the
table would show that the N02 subindex was just above 205, while the
TSP x S02 subindex (corresponding to 30 yg/m3- ppm) was well above 205.
To determine the exact value of the PSI, the user would then turn to the
TSP x S02 column in Table A-4.
"Working" Tables--
Tables A-2 and A-4. In these tables, the values of the PSI, correct to
the nearest integer, can be found immediately and unambiguously without the
need for interpolation.
The normal approach to creating tables is to choose integer values for
one variable and calculate the corresponding values of the second variable.
This approach has one drawbackfor the numbers about halfway between two
table entries, it may take extra time, with the attendant possibilities of
error, to determine the proper value by interpolation.
To avoid this drawback, Tables A-2 and A-4 list the half-integer values
of the PSI for each pollutant. For each of the 500 PSI values, the tables
list explicitly the upper and lower boundaries of the pollutant concentra-
tions corresponding to that value. These are the "cut-off" points that
determine the proper PSI value for any pollutant concentration; by listing
them explicitly, we remove any need for interpolation or estimation.
Thus, the pollutant concentrations corresponding to a PSI value of 50
are all of those contained in the range from 49.5 to 50.5; and the table
lists only these "half-unit" values. For instance, Example 1 shows a section
of an "ordinary" (integer-value) table next to a corresponding section of a
half-integer table. Using the "ordinary" table, it would be quite
difficult to say whether an observed concentration for SOg of 415 yg/m3
corresponded to a PSI value of 111 or 112. Using the half-integer table,
however, it is easy to see that 415 yg/m3 is smaller than the value of
415.03 yg/m3 that marks the dividing line between 111 and 112; thus the
correct value of 111 can be selected rapidly with confidence.
22
-------
Example 1
Comparison of Standard Tables (requiring interpolation) With
Half-Integer Tables Allowing Immediate Determination of PSI.
STANDARD INTEGER- "WORKING" HALF-
VALUE TABLE INTEGER TABLE
PSI j>02
111 412.85
112 417.20
113 421.55
Standard tables require calculation to determine the closest
column entry to a given value. For example, an observed concentra-
tion for S02 of 415 pg/m3 could not immediately be assigned a PSI
value, since 415 is nearly midway between the column entries of 412.85
and 417.20. Two subtractions would have to be performed and the
results compared before the nearest PSI integer could be determined.
On the other hand, the table showing only the half-integer values
of the PSI requires no calculationit is at once evident that 415 is
less than 415.03 (the dividing line between PSI = 111 and PSI = 112)
so that PSI = 111.
PSI
110.5
111.5
112.5
SO?
410.68
415.03
419.38
23
-------
To determine the PSI value corresponding to any pollutant concentration,
travel down the proper column to the two values bracketing the observed
concentration. Then travel horizontally at the level of the smaller
concentration (the upper row) to the value in the left-hand or right-hand
column marked "PSI (nearest unit)" (See Example 2).
Example 2
How to Use Tables A-2 and A-4*
PSI
(Nearest CO
Unit) PSI (mg/m3) 03 SO,,
41
42
^""^-s^43
44
45
40.5 4.05
41.5 4.15
42.5 4.25
^"""\^43.5 4.35
44.5 4.45
*Assume an observed value
locate the values just above
and
(the
the
then locate the PSI value
*
97.20 64.80
99.60 66.40
102.00 68.00
104.40 69.60
106.80 71.20
for TSP of 65pg/m3 . In
and below this value (63
level with the smaller
upper of the two rows) in the left-hand column.
proper PSI value is 43.
TSP
60.75
62.25
63.75
65.25
66.75
the TSP column,
.75 and 65.25),
concentration
In the example,
ExceptionsThe only exceptions to the above procedure occur at the
Federally-set pollutant concentration standards corresponding to the PSI
values 100, 200,...500. At these points, it would be misleading to report a
PSI value of 100, say, for a concentration that corresponds to a value of
99.9such a concentration is below the standard and, therefore, the PSI
value should be reported as 99. The values corresponding to 100, 200,...500
are listed explicitly in Tables A-l and A-3. Only if the observed concentra-
tion exceeds these values may the PSI value be reported as 100, 200,...500.
"Reference" Tables
Tables A-5 through A-15. These tables were originally designed to
aid in constructing the PSI nomogram. They may find further use with
agencies wishing to construct their own nomograms. These tables also
provide a check on the accuracy of the nomogram provided here.
24
-------
For each pollutant, about 250-300 equal Increments have been selected
spanning the range from PSI = 0 to PSI = 500. This ensures a sufficient
number of values to construct a nomogram accurate to the nearest PSI unit.
AmbiguitiesWhat if a reading falls exactly on a half-integer value
of the PSI? This should happen very seldom, but when it does, the user may
wish to round off to the nearest odd number. This has two advantages:
(1) over the long run, the user will be rounding upward about as often as
downward; and (2) in those cases involving readings near the Federal standards
(PSI values of 100, 200, etc.), a reading of 99.5, say, will be correctly
rounded downward to 99, while a reading at 100.5 will be rounded upward to
101. In each case, there will be no ambiguity concerning whether or not a
standard was surpassed.
Programs for Creating Tables
Some agencies may desire to modify these tables for their own purposes.
Possible modifications include:
different breakpoints for COH based upon site-
specific conversion factors.
more (or less) detail for certain pollutants.
different formatting for special purposes.
To assist such efforts, we have included in Appendix B the main program
for Table A-3 and the main program and all subroutines for Tables A-5
through A-15. Table A-3 was selected to represent the entire group of
Tables A-l through A-4, which are basically similar (differing only in the
range of the PSI values and the size of the increment). Tables A-5
through A-15, however, required inverting each of the 41 equations used in
Tables A-l through A-4 to relate pollutant concentrations to their PSI
values. Rather than require each agency to go through the exercise of
inverting these equations, it appeared preferable to list them in one
place for future reference. Therefore, the 11 subroutines containing these
41 inverted equations have been included with the main program in Appendix B.
25
-------
REFERENCES
1. Thorn, Gary C., and Wayne R. Ott, "Air Pollution Indices: A Compendium
and Assessment of Indices Used in the United States and Canada,"
Ann Arbor Science Publishers, Ann Arbor, MI, 1976.
2. Thorn, Gary C., and Wayne R. Ott, "A Proposed Uniform Air Pollution Index,"
Atmospheric Environment, vol. 10, 1976. p. 261.
3. Ott, Wayne R., and Gary C. Thorn, "A Critical Review of Air Pollution
Index Systems in the United States and Canada," Journal of the Air
Pollution Control Association, vol. 26, no. 5, May 1976. pp. 460-470.
4. U.S. Environmental Protection Agency, "Guideline for Public Reporting of
Daily Air Quality," Federal Register, vol. 41, no. 174, September 7, 1976.
p. 37660.
5. Hunt, William F., Jr., Wayne R. Ott, John Moran, Raymond Smith,
Gary Thorn, Neil Berg, and Barry Korb, "Guideline for Public Reporting
of Daily Air QualityPollutant Standards Index (PSI)," Office of Air
Quality Planning and Standards, U.S. Environmental Protection Agency,
EPA 450/2-76-013, Research Triangle Park, NC, August 1976.
6. Hunt, William F., Jr., Raymond Smith, Wayne R. Ott, and Wilson B. Riggan,
"The Pollutant Standards Index CPSI)An Early Warning System for Air
Pollution," presented at the Eighth International Scientific Meeting of
the International Epidemiological Association, Las Croabas, Puerto Rico,
September 18-23, 1977.
7. Clean Air Act Amendments of 1977 (P.L. 95-95). August 7, 1977. 42USC7401
8. Severn, Harry A., Chief, Division of Air Pollution Control, City of
Baltimore, Health Department, letter to Wayne R. Ott, February 22, 1977.
9. Zorbini, Dan, Chemist, North Ohio Valley Air Authority, Steubenville, OH,
letter to Wayne R. Ott, April 27, 1977.
10. Ott, Wayne R., "A FORTRAN Program for Computing the Pollutant Standards
Index CPSI)," U.S. Environmental Protection Agency, Washington, DC,
EPA-600/4-78-001, May 1978.
11. Ott, Wayne R., Environmental Indices; Theory and Practice, Ann Arbor
Science Publishers, Ann Arbor, MI, 1978.
26
-------
RAPID SURVEY TABLE:
Table A-1
POLLUTANT CONCENTRATIONS FOR PSI = 5-200 IN STEPS OF 5
PSI
5
10
15
20
25
30
35
40
45
50
55
60
65
70
75
80
85
90
95
100
105
110
115
120
125
130
135
140
145
150
155
160
165
170
175
180
185
190
195
200
UNITS
CO
(MG/M3)
0.50
1.00
1.50
2.00
2.50
3.00
3.50
4.00
4.50
5.00
5.50
6.00
6.50
7.00
7.50
8.00
8.50
9.00
9.50
10.00
10.35
10.70
11.05
11.40
11.75
12.10
12.45
12.80
13.15
13.50
13.85
14.20
14.55
14.90
15.25
15.60
15.95
16.30
16.65
17.00
IN MICROGRAMS/CUBIC
03
12.00
24.00
36.00
48.00
60.00
72.00
84.00
96.00
108.00
120.00
132.00
144.00
156.00
168.00
180.00
192.00
204.00
216.00
228.00
240.00
248.00
256.00
264.00
272.00
280.00
288.00
296.00
304.00
312.00
320.00
328.00
336.00
344.00
352.00
360.00
368.00
376.00
384.00
392.00
400.00
S02
8.00
16.00
24.00
32.00
40.00
48.00
56.00
64.00
72.00
80.00
108.50
137.00
165.50
194.00
222.50
251.00
279.50
308.00
336.50
365.00
386.75
408.50
430.25
452.00
473.75
495.50
517.25
539.00
560.75
582.50
604.25
626.00
647.75
669.50
691.25
713.00
734.75
756.50
778.25
800.00
METER
TSP
7.50
15.00
22.50
30.00
37.50
45.00
52.50
60.00
67.50
75.00
93.50
112.00
130.50
149.00
167.50
186.00
204.50
223.00
241.50
260.00
265.75
271.50
277.25
283.00
288.75
294.50
300.25
306.00
311.75
317.50
323.25
329.00
334.75
340.50
346.25
352.00
357.75
363.50
369.25
375.00
UNITS IN
CO
0.4500
0.9000
1.3500
1.8000
2.2500
2.7000
3.1500
3.6000
4.0500
4.5000
4.9500
5.4000
5.8500
6.3000
6.7500
7.2000
7.6500
8.1000
8.5500
9.0000
9.3000
9.6000
9.9000
10.2000
10.5000
10.8000
11.1000
11.4000
11.7000
12.0000
12.3000
12.6000
12.9000
13.2000
13.5000
13.8000
14.1000
14.4000
14.7000
15.0000
PARTS PER
03
0.0060
0.0120
0.0180
0.0240
0.0300
0.0360
0.0420
0.0480
0.0540
0.0600
0.0660
0.0720
0.0780
0.0840
0.0900
0.0960
0.1020
0.1080
0.1140
0.1200
0.1240
0.1280
0.1320
0.1360
0.1400
0.1440
0.1480
0.1520
0.1560
0.1600
0,1640
0.1680
0.1720
0.1760
0.1800
0.1840
0.1880
0.1920
0.1960
0.2000
MILLION
S02
0.0030
0.0060
0.0090
0.0120
0.0150
0.0180
0.0210
0.0240
0.0270
0.0300
0.0410
0.0520
0.0630
0.0740
0.0850
0.0960
0.1070
0.1180
0.1290
0.1400
0.1480
0.1560
0.1640
0.1720
0.1800
0.1880
0.1960
0.2040
0.2120
0,2200
0.2280
0.2360
0.2440
0.2520
0.2600
0.2680
0.2760
0.2840
0.2920
0.3000
PSI
5
10
15
20
25
30
35
40
45
50
55
60
65
70
75
80
85
90
95
100
105
110
115
120
125
130
135
140
145
150
155
160
165
170
175
180
185
190
195
200
28
-------
WORKING TABLE:
Table A-2
POLLUTANT CONCENTRATIONS FOR PSI = 0.5-199.5
PSI
(NEAREST
UNIT)
1
2
3
4
5
6
7
8
9
10
11
12
13
14
15
16
17
18
19
20
21
22
23
24
25
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
PSI
0.5
1.5
2.5
3.5
4.5
5.5
6.5
7.5
8.5
9.5
10.5
11.5
12.5
13.5
14.5
15.5
16.5
17.5
18.5
19.5
20.5
21.5
22.5
23.5
24.5
25.5
26.5
2.7.5
28.5
29.5
30.5
31.5
32.5
33.5
34.5
35.5
3C.5
37.5
38.5
UNITS
CO
(MG/M3)
0.05
0.15
0.25
0.35
0.45
0.55
0.65
0.75
0.85
0.95
1.05
1.15
1.25
1.35
1.45
1.55
1.65
1.75
1.85
1.95
2.05
2.15
2.25
2.35
2.45
2.55
2.65
2.75
2.85
2.95
3.05
3.15
3.25
3.?5
3.45
.1.55
?,65
3.7£
3.35
39. £ 3.y'j
*0,5 . 4.'jb
41.5
42.5
43.5
44.5
45.5
46.5
47.5
43.5
49.5
4.15
4.25
4.35
4.4j
4,55
4.65
4.75
4.86
t ,95
IN MICRO&RAMS/CUBIC
03
1.20
3.60
6.00
8.40
10.80
13.20
15.60
18.00
20.40
22.80
25.20
27,60
30.00
32.40
34.80
3/.20
39.60
42. QO
44.40
46.80
49. 2J
51,60
54,00
56.40
L,8.30
61.20
63.60
66.00
63.40
70. bU
73.20
75.60
78.00
80.40
S2.80
8o.I\;
V.50
3 j.JO
St .4'.'
94. fO
j/ ?(
99.60
IJ2.00
104.40
1%.80
30S,^0
111. CO
114.00
116.40
113 hQ
S02
0.80
2.40
4.00
5.60
7.20
8.80
10.40
12.00
13.60
15.20
16.80
18.40
20,00
21.60
23,20
24.80
26,40
28,00
29.60
31,20
32.80
34.40
36,00
37.60
39.20
40.60
42.40
44,00
45,60
47 . 20
48,80
50.40
52,00
53.50
55.20
56 . 30
"o,-"C
60 . 00
Ci GC
'3,1\>
K,f;n
65^0
68,00
69.60
71 ?C
7 -.-'JO
74 40
76. "
-7 (_,-,
79.. 0
METER
TSP
0.75
2.25
3.75
5.25
6.75
8.25
9.75
11.25
12.75
14.25
15.75
17.25
18.75
20.25
21.75
23,25
24.75
26.25
27.75
29.25
30.75
32. 2b
33.75
35.25
36.75
38.25
39.75
41.25
42.75
4^.25
45. 7 c
47. ?b
48.75
50.25
51.75
^3,2^
5-1 . 75
r , " r
,;u , CO
UNITS IN
0
0
0
0
0
0
0
0
0
0
0
1
1
1
1
I
1
1
1
1
1
I
2
2
2
2
2
2
2
2
2
2
2
3
3
3
j
^
37 , 75 3
??.?' i 3
60 7: i 3
62.25 i 3
63 »,
65.25
F:6J-,
63.25
69.75
71. V.
3
3
4
4
4
4
1 i , i i
?A,'T | 4
CO
.0450
.1350
.225C
.3150
.4050
,4950
.5850
.6750
.7650
.8550
.9450
.0350
.1250
.2150
.3050
.3950
.4850
.5750
.6650
.7550
.8450
.9350
.0250
.1150
.2050
2950
.3850
.4750
,5650
.6550
.7450
.8350
.9250
.0150
.1050
.1950
.28bO
.3750
.4650
.505U
.6450
360
,8250
.915C
.0050
.0950
.1850
?750
.36^)0
455U
PARTS PER
03
0.0006
0.0018
0.0030
0.0042
0.0054
O.C066
0.0078
0.0090
0.0102
0.0114
0.0126
O.Oj.38
0.0150
0,0162
0.0174
0.0185
0.0198
0.0210
0.0222
0,0234
U.0246
0.0258
0,0270
Q.02&2
0.0294
0.030&
0.0318
0.0330
0.0342
0.0354
j.0366
0.0378
0.0390
0.0402
0.0414
0.0126
n.0433
0,0^50
0 Q')b2
j.0474
O.C486
0.0493
0.0510
0.0522
0.053*
0.0546
O.U558
0,0570
O.G5S2
0.0534
MILLION
S02
0.0003
0.0009
0.0015
0.0021
0.0027
0,0033
0.0039
0.0045
0.0051
0.0057
0.0063
0.0069
0.0075
0.0081
0.0087
0.0093
0.0099
0.0105
0.0111
0.0117
0.0123
0.0129
0.0135
0.0141
0.0147
0.0153
0.0159
0.0165
o.om
0.0177
0.0183
0.0189
0.0195
0.0201
0.0207
0,0213
0.0239
0.0225
0.0231
0.0';?-7
0.0243
0.0249
0.0255
0.0261
0.0267
0.0273
PSI
0.5
1.5
2.5
3.5
4.5
5.5
6.5
7.5
8.5
9.5
10.5
11.5
12.5
13,5
14,5
15.5
16.5
17.5
18.5
19.5
20.5
21.5
22.5
23.5
24.5
25.5
26.5
27.5
28.5
29.5
30,'
31.5
32.5
33.5
34.5
35. 5
J6.5
37.5
38.5
39, G
40.5
41.5
42.5
"3.5
44.5
45.5
0.0279 46.5
0.0285
47. 5
0.0291 48.5
0.0297 i 49.5
PSI
(NEAREST
UNIT)
1
2
3
4
5
6
7
8
9
10
11
12
13
14
15
16
17
18
19
20
21
22
23
24
25
26
27
28
es
3C
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
-------
Table A-2 (Continued)
WORKING TABLE: POLLUTANT CONCENTRATIONS FOR PSI = 0.5-199.5
PSI
(NEAREST
UNIT)
51
52
53
54
55
56
57
58
59
60
61
62
63
64
65
66
67
68
69
70
71
72
73
74
75
76
77
78
79
80
81
82
83
84
85
86
87
88
83
90
91
92
93
94
95
96
97
98
99
100
PSI
50.5
51.5
52.5
53.5
54.5
55.5
56.5
57.5
58.5
59.5
60.5
61.5
62.5
63.5
64.5
65.5
66.5
67.5
68.5
69.5
70.5
71.5
72.5
73.5
74.5
75.5
76.5
77.5
78.5
79.5
80.5
81.5
82.5
83.5
84.5
85.5
86.5
87.5
88.5
89.5
90.5
91.5
92.5
93.5
94.5
95.5
96,5
97,5
98.5
99.5
UNITS
CO
(MG/M3)
5.05
5.15
5.25
5.35
5.45
5.55
5.65
5.75
5.85
5.95
6.05
6.15
6.25
6.35
6.45
6.55
6.65
6.75
6.85
6.95
7.05
7.15
7.25
7.35
7.45
7.55
7.65
7.75
7.85
7.95
8.05
8.15
8.25
8.35
8.45
8.55
8.65
8.75
8.85
8.95
9.05
9.15
9.25
9.35
9.45
9.55
9.65
9.75
9.85
9.95
IN MICROGRAMS/CUBIC
03
121.20
123.60
125.00
128.40
130.80
133.20
135.60
138.00
140.40
142.80
145.20
147.60
150.00
152.40
154.80
157.20
159.60
162.00
164.40
166.80
169.20
171.60
174.00
176.40
178.80
181.20
183.60
186.00
188.40
190.80
193.20
195.60
198.00
200.40
202.80
205.20
207.60
210.00
212.40
214.80
217.20
219. nO
222.00
224.40
226.80
229.20
231.60
234.00
236.40
238.80
S02
82.85
88.55
94.25
99.95
105.65
111.35
137.05
122.75
128.45
134.15
139.85
145.55
151.25
156.95
162.65
168.35
174.05
179.75
185.45
191.15
196.85
202.55
208.25
213.95
219.65
225.35
231.05
236.75
242.45
248.15
253.85
259.55
265.25
270.95
276.65
282.35
288.05
293.75
299.45
305.15
310.85
316.55
322.25
327.95
333.65
339.35
345.05
350.75
356.45
362.15
METER
TSP
76.85
80.55
84.25
87.95
91.65
95.35
99.05
102.75
106.45
110.15
113.85
117.55
121.25
124.95
128.65
132.35
136.05
139.75
143.45
147.15
150.85
154.55
158.25
161.95
165.65
169.35
173.05
176.75
180.45
184.15
187.85
191.55
195.25
198.95
202.65
206.35
210.05
213.75
217.45
221.15
224.85
228. 55
232.25
235.95
239.65
243.35
247.05
250.75
254.45
258.15
UNITS IN
CO
4.5450
4.6350
4.7250
4.8150
4.9050
4.9950
5.0850
5.1750
5.2650
5.3550
5.4450
5.5350
5.6250
5.7150
5.8050
5.8950
5.9850
6.0750
6.1650
6.2550
6.3450
6.4350
6.5250
6.6150
6.7050
6.7950
6.8850
6.9750
7.0650
7.1550
7.2450
7.3350
7.4250
7.5150
7.6050
7.6950
7.7850
7.3750
7.9C50
8.0550
8.1450
8.2350
8.3250
8.4150
8.5050
8.5950
8.6850
8.7750
8.8650
8.9550
PARTS PER
03
0.0606
0.0618
0.0630
0.0642
0.0654
0.0666
0.0678
0.0690
0.0702
0.0714
0.0726
0.0738
0.0750
0.0762
0.0774
0.0786
0.0798
0.0810
0.0822
0.0834
0.0846
0.0858
0.0870
0.0882
0.0894
0.0906
0.0918
0.0930
0.0942
0.0954
0.0966
0.0978
0.0990
0.1002
0.1014
0.1026
0.1038
0.1050
0.1062
0.1074
0.1086
O.J098
0.1110
0.1122
0.1134
0.1146
0.1158
0.1170
0.1182
0.1194
MILLION
S02
0.0311
0.0333
0.0355
0.0377
0.0399
0.0421
0.0443
0.0465
0.0487
0.0509
0.0531
0.0553
0.0575
0.0597
0.0619
0.0641
0.0663
0.0685
0.0707
0.0729
0.0751
0.0773
0.0795
0.0817
0.0839
0.0861
0.0883
0.0905
0.0927
0.0949
0.0971
0.0993
0.1015
0.1037
0.1059
0.1081
0.1103
0.1125
0.1147
0.1169
0.1191
0.1213
0.1235
0.1257
0.1279
0.1301
0.1323
0.1345
0.1367
0.1389
PSI
50.5
51.5
52.5
53.5
54.5
55.5
56.5
57.5
58.5
59.5
60.5
61.5
62.5
63.5
64.5
65.5
66.5
67.5
68.5
69.5
70.5
71.5
72.5
73.5
74.5
75.5
76.5
77.5
78.5
79.5
80.5
81.5
82.5
83.5
84.5
85.5
86.5
87.5
88.5
89.5
90.5
91.5
92.5
93.5
94.5
95.5
96.5
97.5
98.5
99.5
PSI
(NEAREST
UNIT)
51
52
53
54
55
56
57
58
59
60
61
62
63
64
65
66
67
68
69
70
71
72
73
74
75
76
77
78
79
80
81
82
83
84
85
86
87
88
89
90
91
92
93
94
95
96
97
98
99
100
-------
Table A-2 (Continued)
WORKING TABLE: POLLUTANT CONCENTRATIONS FOR PSI = 0.5-199.5
PSI
(NEAREST
UNIT)
101
102
103
104
105
106
107
108
109
110
111
112
113
114
115
116
117
118
119
120
121
122
123
124
125
126
127
128
129
130
131
132
133
134
135
136
137
138
139
140
141
142
143
144
145
146
147
148
149
150
PSI
100.5
101.5
102.5
103.5
104.5
105.5
106.5
107.5
108.5
109.5
110.5
111.5
112.5
113.5
114.5
115.5
116.5
117.5
118.5
119.5
120.5
121.5
122.5
123.5
124.5
125.5
126.5
127.5
128.5
129.5
130.5
131.5
132.5
133.5
134.5
135.5
136.5
137.5
138.5
139.5
140.5
141.5
142.5
143.5
144.5
145.5
146.5
147.5
148.5
149.5
UNITS
CO
(M6/M3)
10.04
10.11
10.18
10.25
10.32
10.39
10.46
10.53
10.60
10.67
10.74
10.81
10.88
10.95
11.02
11.09
11.16
11.23
11.30
11.37
11.44
11.51
11.58
11.65
11.72
11.79
11.86
11.93
12.00
12.07
12.14
12.21
12.28
12.35
12.42
12.49
12.56
12.63
12.70
12.77
12.84
12-91
12.98
13.05
13.12
13.19
13.26
13.33
13.40
13.47
IN MICROGRAMS/CUBIC
03
240.80
242.40
244.00
245.60
247 '.20
248.80
250.40
2S2.00
253.60
255.20
256.80
258.40
260.00
261.60
263.20
264.80
266.40
268.00
269.60
271.20
272.80
274.40
.276.00
277.60
279.20
280.80
282.40
284.00
285.60
287.20
288.80
290.40
292.00
293.60
295.20
296.80
298.40
300.00
301.60
303.20
304.80
306.40
308.00
309.60
311.20
312.80
314.40
316.00
317.60
319.20
S02
367.18
371.53
375.88
380.23
384.58
388.93
393.28
397.63
401.98
406.33
410.68
415.03
419.38
423.73
428.08
432.43
436.78
441.13
445.48
449.83
454.18
458.53
462.88
467.23
471.58
475.93
480.28
484.63
488.98
493.33
497.68
502.03
506.38
510.73
515.08
519.43
523.78
528.13
532.48
536.83
541.18
545.53
549.88
554.23
558.58
562.93
567.28
571.63
575.98
580.33
METER
TSP
260.58
261.73
262.88
264.03
265.18
266.33
267.48
268.63
269.78
270.93
272.08
273.23
274.38
275.53
276.68
277.83
278.98
280.13
281.28
282.43
283.58
284.73
285.88
287.03
288.18
289.33
290.48
291.63
292.78
293.93
295.08
296.23
297.38
298.53
299.68
300.83
301.98
303.13
304.28
305.43
306.58
307.73
308.88
310.03
311.18
312.33
313.48
314.63
315.78
316.93
UNITS IN
CO
9.0300
9.0900
9.1500
9.2100
9.2700
9.3300
9.3900
9.4500
9.5100
9.5700
9.6300
9.6900
9.7500
9.8100
9.8700
9.9300
9.9900
10.0500
10.1100
10.1700
10.2300
10.2900
10.3500
10.4100
10.4700
10.5300
10.5900
10.6500
10.7100
10.7700
10.8300
10.8900
10.9500
11.0100
11.0700
11.1300
11.1900
11.2500
11.3100
11.3700
11.4300
11.4900
11.5500
11.6100
11.6700
11.7300
11.7900
11.8500
11.9100
11.9700
PARTS PER
03
0.1204
0.1212
0.1220
0.1228
0.1236
0.1244
0.1252
0.1260
0.1268
0.1276
0.1284
0.1292
0.1300
0.1308
0.1316
0.1324
0.1332
0.1340
0.1348
0.1356
0.1364
0.1372
0.1380
0.1388
0.1396
0.1404
0.1412
0.1420
0.1428
0.1436
0.1444
0.1452
0.1460
0.1468
0.1476
0.1484
0.1492
0.1500
0.1508
0.1516
0.1524
0.1532
0.1540
0.1548
0.1556
0.1564
0.1572
0.1580
0.1588
0.1596
MILLION
S02
0.1408
0.1424
0.1440
0.1456
0.1472
0.1488
0.1504
0.1520
0.1536
0.1552
0.1568
0.1584
0.1600
0.1616
0.1632
0.1648
0.1664
0.1680
0.1696
0.1712
0.1728
0.1744
0.1760
0.1776
0.1792
0.1808
0.1824
0.1840
0.1856
0.1872
0.1888
0.1904
0.1920
0.1936
0.1952
0.1968
0.1984
0.2000
0.2016
0.2032
0.2048
0.2064
0.2080
0.2096
0.2112
0.2128
0.2144
0.2160
0.2176
0.2192
PSI
100.5
101.5
102.5
103.5
104.5
105.5
106.5
107.5
108.5
109.5
110.5
111.5
112.5
113.5
114.5
115.5
116.5
117.5
118.5
119.5
120.5
121.5
122.5
123.5
124.5
125.5
126.5
127.5
128.5
129.5
130.5
131.5
132.5
133.5
134.5
135.5
136.5
137.5
138.5
139.5
140.5
141.5
142.5
143.5
144.5
145.5
146.5
147.5
148.5
149.5
PSI
(NEAREST
UNIT)
101
102
103
104
105
106
107
108
109
110
111
112
113
114
115
116
117
118
119
120
121
122
123
124
125
126
127
128
129
130
131
132
133
134
135
136
137
138
139
140
141
142
143
144
145
146
147
148
149
150
31
-------
Table A-2 (Continued)
WORKING TABLE: POLLUTANT CONCENTRATIONS FOR PSI = 0.5-199.5
PSI
(NEAREST
UNIT)
151
152
153
154
155
156
157
158
159
160
161
162
163
164
165
166
167
168
169
170
171
172
173
174
175
176
177
178
179
180
181
182
183
184
185
186
187
188
189
190
191
192
193
194
195
196
197
198
199
200
PSI
150.5
151.5
152.5
153.5
154.5
155.5
156.5
157.5
158.5
159.5
160.5
161.5
162.5
163.5
164.5
165.5
166.5
167.5
168.5
169.5
170.5
171.5
172.5
173.5
174.5
175.5
176.5
177.5
178.5
179.5
180.5
181.5
182.5
183.5
184.5
185.5
186.5
187.5
188.5
189.5
190.5
191.5
192.5
193.5
194.5
195.5
196.5
197.5
198.5
199..5
UNITS
CO
(M6/M3)
13.54
13.61
13.68
13.75
13.82
13.89
13.96
14.03
14.10
14.17
14.24
14.31
14.38
14.45
14.52
14.59
14.66
14.73
14.80
14.87
14.94
15.01
15.08
15.15
15.22
15.29
15.36
15.43
15.50
15.57
15.64
15.71
15.78
15.85
15.92
15.99
16.06
16.13
16.20
16.27
16.34
16.41
16.48
16.55
16.62
16.69
16.76
16.83
16.90
16.97
IN MICROGRAMS/CUBIC
03
320.80
322.40
324.00
325.60
327.20
328,80
330.40
332.00
333.60
335.20
336.80
338.40
340.00
341.60
343.20
344.80
346.40
348 . 00
349.60
351.20
352.80
354.40
356.00
357.60
359.20
360.80
362.40
364.00
365.50
367.20
368.80
370.40
372.00
373.60
375.20
376.80
378.40
380.00
331.60
383.20
384.80
386.40
388.00
389.60
391.20
392.30
394.40
396.00
397.60
399.20
S02
584.68
589.03
593.38
597.73
602.08
606.43
610.78
615.13
619.48
623.83
628.18
632.53
636.88
641.23
645.58
649.93
654.28
658.63
662.98
667.33
671.68
676.03
680.38
684.73
689.08
693.43
697.78
702.13
706.48
710.83
715.18
719.53
723.88
728.23
732.58
736.93
741.28
745.63
749.98
754.33
758.68
763.03
767.38
771.73
776.08
780.43
784.78
789.13
793.48
797.83
METER
TSP
318.08
319.23
320.38
321.53
322.68
323.83
324.98
326.13
327.28
328.43
329.58
330.73
331.88
333.03
334.18
335.33
336.48
337.63
338.78
339.93
341.08
342.23
343.38
344.53
345.68
346.83
347.98
349.13
350.28
351.43
352.58
353.73
354.88
356.03
357.18
358.33
359.48
360.63
361.78
362.93
364.08
365.23
366.38
367.53
368.68
369.83
370.98
372.13
373.28
374.43
UNITS IN
CO
12.0300
12.0900
12.1500
12.2100
12.2700
12.3300
12.3900
12.4500
12.5100
12.5700
12.6300
12.6900
12.7500
12.8100
12.8700
12.9300
12.9900
13.0500
13.1100
13.1700
13.2300
13.2900
13.3500
13.4100
13.4700
13.5300
13.5900
13.6500
13.7100
13.7700
13.8300
13.8900
13.9500
14.0100
14.0700
14.1300
14.1900
14.2500
14.3100
14.3700
14.4300
14.4900
14.5500
14.6100
14.6700
14.7300
14.7900
14.8500
14.9100
14.9700
PARTS PER
03
0.1604
0.1612
0.1620
0.1628
0.1636
0.1644
0.1652
0.1660
0.1668
0.1676
0.1684
0.1692
0.1700
0.1703
0.1716
0.1724
0.1732
0.1740
0.174S
0.1756
0.1754
0.1772
0.1780
0.1788
0.1796
0.1804
0.1812
0.1820
0.1328
0.1836
0.1844
0.1852
0.1860
0.1868
0.1376
0.1884
0.1392
0.1900
G.I 908
0.1916
0.1924
0.1932
0.1940
0.1948
0.1956
C.I 964
0.1972
0.19SO
0.1983
0.1996
MILLION
SO 2
0.2208
0.2224
0.2240
0.2256
0.2272
0.2288
0.2304
0.2320
0.2336
0..2352
0.2368
0.2384
0.2400
0.2416
0.2432
0.2448
0.2464
0.2480
0.2496
0.2512
0.2528
0.2544
0.2560
0.2576
0.2592
0.2608
0.2624
0.2640
0.2656
0.2672
0.2688
0.2704
0.2720
0.2736
0.2752
0.2768
0.2784
0.2800
0.2816
0.2832
0.2848
0.2864
0.2880
0.2896
0.2912
0.2928
0.2944
0.2960
0.2976
0.2992
PSI
150.5
151.5
152.5
153.5
154.5
155.5
156.5
157.5
158.5
159.5
160.5
161.5
162.5
163.5
164.5
165.5
166.5
167.5
168.5
169.5
170.5
171.5
172.5
173.5
174.5
175.5
176.5
177.5
178.5
179.5
180.5
181.5
182.5
183.5
184.5
185.5
186.5
187.5
188.5
189.5
190.5
i'91.5
192.5
193.5
194.5
.195.5
196.5
197.5
198. 5
1P9.5
PSI
(NEAREST
UNIT)
151
152
153
154
155
156
157
158
159
160
161
162
163
164
165
166
167
168
169
170
171
172
173
174
175
176
177
178
179
180
181
182
183
184
185
186
187
188
189
190
191
192
193
194
195
196
197
198
199
200
32
-------
LL
O
00
a.
LU
00
z
o
o
i
CM
00
D.
cc.
LL
co
«?P
Table A
CENTRA^
H
O
O
I-
z
<
_J
_J
O
_J
CO
<
l_
>-
UJ
>
C£
00
Q
Q-
<
cc
CO
i i
z.
=>
Q
UJ
i i
s:
o
_i
!
i i
s:
CC
UJ
1/1
fe
14
2:
o:
LU
UJ
s:
o
CO
=3
O
co
CD
cc
CJ>
s:
*r.
K 1
CO
f
t s
ZD
CM E:
0 0-
OO CU
X 1
O 1C
00
CJ
CO
re ic
CJ CJ
CO
CM s:
o ^
CO CD
a- i
co s:
t Q.
CL-
IO
s^
xs:
0- 1
CM
o
^-
CM
CO
co
CJ
CM
o
0-
H~
CM
O
CO
co
O
co
CJ CD
t i
CO
Q_
00 00 0 O
O CO VO en CM in
CM CM CM CM CO CO
O O O O O O
0 0 0 0 OO
o t-i CM co «* tn
n co ro co co co
O CM -3- CO OO O
CM CO O * CO CO
to in co o r~. LO
«3" 00 CM VO 01 CO
CM CM CO CO CO **
O 00 WO «* CM O
in «a- !*- «3- ~r =*
vo r- co en o i
O CO CO en CM If)
CM o r~-
in in vo r-~ co oo
t-H i t t 1 » 1 i 1 t 1
O r~ CO O VD CO
co co «a- o in ,-H
r-H ^H CM CO CO «3-
o o o o o o
O in CD LO o in
in i o CM in i
r~. oo o rn CM ro
CO CO -S3- «* ^1- «*
O O OO OO
O «* CO CM IO O
co co oo cr> en o
O C3 O O O O
CD CM «3- IO OO O
^ =! - ^f * -ej- in
o m o un o m
o oo i~- in * CM
r~- i~- co cr> o i
r-4 t~H «-H »-H CM CM
o LO o ur> o in
O O >-l t-t CM CM
CM CM CV! CJ CM CM
OOO O 0
oo <-i «± r-~ o
co <*«*<* in
C3 O O O O
o o o o o
vo r^. oo en o
co co co co =!-
CM ^- VO CO CD
t^ i i in en *i-
CM O l»» * CM
l~- < 1 ^- CO CM
* in in in vo
OO VO ^ CM O
co co co co co
CM ro <- in vo
OO *-t «* t^ O
r^ oo oo co cr>
O CD O CD CD
o in o in o
CT> O CM CO in
co *a- «* ^- <3-
O CD O O O
o o o o o
vo r-^ oo ch o
CM CM CM CM CO
o in o m CD
in CM o r>. in
Cn O i I t-H CM
. 1 CM CM CM CM
en vo CM en in
vo CM co co en
«* in m 10 vo
CD CD O O O
CD in CD in o
CD CM in r^ CD
tn vo t^ oo CD
* «3- *3- «3- in
O 0 O 0 0
<* OO CM VO O
O O r-H ^H CM
O O CD O O
CM <3- CO CO O
in in tn LO vo
o in o LO o
r-i en oo vo tn
CM CM co «a- in
CM CM CM CM CM
o LO o m o
co co *i- ^r in
CM CNJ CM CM CM
ooooo
co vo en CM in
in LO LO vo vo
ooooo
O O O O CD
i 1 CM CO * LO
«a- *r «a- «a- *
CM * VO OO O
oo CM vo O in
en t~- * CM en
in en co r-. o
CO VO !-» t-^ OO
CO CO «* CM CD
CM CM CM CM CM
r-~- oo en o r-i
co vo en CM in
en en en CD CD
in o in o in
vo co en r-t CM
^j- tr «* in in
o o o o CD
ooooo
r-t CM CO <3" LO
CO CO CO CO CO
ooooo
LO O LO O LO
CM O r»- LO CM
co «d- «S- in co
CM CM CM CM CM
CM OO LO i 1 CO
in o vo CM r^
r-~ oo oo en en
O O CD O CD
in CD in o LO
CM LO 1^. CD CM
i i CM co in vo
in LO in in LO
CD O O O CD
*a- oo CM vo CD
CM CM CO CO **
ooooo
CM * VO OO O
vo vo vo vo r^
LO o in o LO
co CM CD en r-»
vo r-. oo oo en
CM CM CM CM CM
LO o LO o in
LO VO VO l~~ I-~
CM CM CM CM CM
OOOOO
CO r-H «* 1 CD
OOOOO
ooooo
vo r~* co en o
^j* ^~ ^f* *5t~ in
CM ^ VO CO O
en co t-^ i-i vo
VO ^- rH CTl VO
<- oo CM in en
oo co en en en
OO VO «* CM CD
CM co ^t- in vo
co i i «* r~ o
O t ' i-H 1 CM
o in CD in o
* in r-. co o
in LO in LO vo
o o CD o CD
ooooo
vo t^. oo en o
CO CO CO CO ^J"
ooooo
o in o LO o
o r~- in CM o
r-~. r~- oo en o
CM CM CM CM CO
«3" r- 1 1^. *S- CD
co en »3- o vo
O CD 1 CM CM
O CD OO O
O LO O LO O
LO r~- o CM in
r-~ oo o I-H CM
in in vo vo vo
O O O CD O
«d- OO CM vo O
«» «* in in vo
ooooo
CM *^-
ooooo
ooooo
o in o in o
co co «tr «i- in
co co co co co
CM en vo co o
oo t i in en co
«d- in in in vo
ooooo
CD m o in o
o CM in i~- o
o < i CM co in
o in o in o
in r~ o CM in
r~ r-~ oo oo oo
ooooo
vo r~. oo en o
co oo oo oo en
CD O CD O O
VO CM CO ** CD
r~. co oo en o
co co co co si-
CD in CD in CD
CO CO * * LO
co co co co co
33
-------
in
LL
O
i
t? 2
< m
^ O
J2 Z
CO
Ul
>
cc
z
o
I
00 s"
o a.
co a.
X 1
x: (/>
o ac
0 O
o
CO
:c ic
to o o
1 ^^^
1 1
r> 'try
CM JE
a 0~-~
UJ CO O
X X O
> i a. i
E: to :c
IX
<£>
S^
to to
t :z>
z: CM
0 0
* 2*"
_l
_J
i i
E:
a:
UJ CM
to
to
£
«£
a.
ro
14
t/O
1 1
z.
o
CM
C£ 0
uj zi
tj
O O-
03 (-
o
to
rf CM
2 o
CD CO
§
o
* s
1 1
to - «
1 «»>
-« s
r> o CD
» «
to
a.
ooooo
CM **- to oo o
O O O O r-t
ooooo
r-i CM co <* in
IO IO tO IO 1O
CM «* VOCO O
o CM O>
1 1 1-4 t 1 «4 i 1
OOOOO
rH CM CO o> o
co co co ro *^
CM en vo co o
in OOCM to O
oo oo o> en o
CM CM CM CM CO
ooooo
o in o m o
in r-^ocM in
CM co into r««
CO OO 00 OO OO
8 in o m o
CM lOt*. O
OOOO 1-1
CM CM CM CM CM
SOO O O
r^ OOOt O
t-«
OOOOO
to CM oo^ o
ro ^^m to
o inoino
oo oo 01 o> o
CO CO CO CO <^
in o in o in
T-t co ^r «o r^.
CM CM CM CM CM
1-1 1-1 l-« «-H 1-1
in o in o in
O i-l i-H CM CM
ooooo
mo in o in
01 co to in ro
r-«ro in r-. o»
in in in in in
en r- to «* co
r»>cM I>^CM r>»
Ot OO rH r-4
ro«*«a-«l- ^~
CM«*l£)OO O
to to to to r^
ooooo
r-« CM CO * in
oo co oo oo oo
ooooo
in CD m o m
Oi-l i-i CM CM
in in in in in
ooooo
ooooo
in CD m o m
O i t i-l CM CM
** «*«*«*«*
oo m co o op
roi~. T-H in oo
O O i 1 i-< » I
ro ro ro ro ro
in o in o in
CM in r--. o CM
-i r~ co o to
oo co en o o
co CO co en en
to CM oo«*- o
CM in r-. o co
f-l i-l i-l CM CM
CM CM CM CM CM
OOOOO
1-1 CM ro «d- m
co in coo oo
in i-i i-. co oo
u>r^r»cooo
«* «* * ^»- *f
in o in o in
O rH i-l CM CM
O in o in o
en O CM co m
CM CO CO CO CO
O in o in o
co co** «* in
8 OOOO
mo in o
CM O O\ Is- IO
-i CO «S- tO CO
10 to to to to
-toco !» in
CM r»> r-t 10 i-i
CM CM CO CO «d-
co «s- to co o
ooooo
to r-. oo en o
oo co oo oo en
ooooo
o mo m o
ro ro »* *a- in
in in in in in
ooooo
§0000
in o m o
co co a- *i- m
^ ** «* ^f ^J-
in ro ooo in
CM to o co i^
CM CM CO OO CO
ro ro co ro co
O in o in o
in r*. o CM in
CM oo in 1-1 r».
r-i I-H CM ro co
en en en en en
tO CM CO *3-O
in coo co to
CM CM CO CO CO
CM CM CM CM CM
ooooo
SoooS
in co o co m
<» O IO !-HI-»
en o o i < T-t
3- if) in in in
O in o in o
co oo «3- * in
«t- <* ^J- ^f «*
in o in o in
«O CO Cf> r-> CM
ro co ro «3- =!-
in o in o in
in to to r>- 1
f*. r^ t^. r~~ r>-
ooooo
in o m o in
* CO r-l O OO
OCM »s- to r--
«* CM I-H en co
to rn to o in
«* in in to to
CM «no co o
oo oo co oo en
ooooo
rH CM CO «3- in
en en en en en
ooooo
in o in o in
in to to r-. rx
in in in in in
ooooo
ooooo
in o in o in
in to to i~, t-^
** ^J- ^r «a- ^~
ro o co in ro
-i in co CM to
*3-«d- * in in
ro co co co oo
in o m o in
i^ o CM in r-
ro o to CM oo
T*- in in to to
en en en en en
to CM oo «3- o
00 rH ro to en
co «d- «* «1- ^t-
CM CM CM CM CM
OOOOO
i-i CM oo «» in
II 1 1 l-H T-H 1 1
ro o oo in co
ro en st- o to
CM CM CO «J- *
in in in in in
in o in o in
in to to P~. i^
ej- «! ^t- * *
t
o in o 'o o
si- to i-- co o
. r>- r^. r--. CD
ooooo
o in o m cs
i~» in «d- c\J 1-1
cn rH oo in r^
I-N oo co oo co
to in co CM o
o in o in o
r** r^ co co en
CM ^J- to CO CD
en en en en o
O O CD O O
to r-. co en o
en en en en CD
o o o o I-H
o in o in o
CO oo en en o
in m in in to
O o o CD o
ooooo
o m o in o
co co en cr> CD
=J- «3- «* * u->
J
o oo in ro o
o oo r^ ii in
to to to i-. t-^
co co co ro ro
o in o in CD
O CM in r-. o
lf> r-t r*. CO CD
r- oo oo 01 o
en en cr> 01 o
i i
t£> CM CO >>f O
I-H ^j- to cn cj
in in in ir> to
CM CM CM CJ CM
ooooo
to Is-. co en o
r-t i-H r-t r-t r-l
o oo in ro o
CM r~» oo en in
in m to to t~~
10 in in in in
O in o in o
oo co en en o
«3~ ^t* ^*~ "3~ m
34
-------
i
in
CM
ii
DC
O
u.
(A
z
JD O
O
a.
UJ
_J
3
C3
IT
O
O-
CM O-
O 1
oo to
1C 0
o o
o
00
;c DC
o o
to co
1 CMS
I-H O --~
z to to
D_ 1
O OO S
UJ 10.
X D.
s:
vo
CMS:
o
toes
CM
0
0
1 1
_J
_J
f- 1
CM
UJ to
0.
to
f
-H
oo cn in T-H r~.
O CD T-H CM CM
CM CM CM CM CM
O O O O O
T-H oo in r~ cn
O 00 0 0
co co oo co co
si- co ii cn oo
cn si- cn co co
r-t en vo si- T-H
in in vo r~. oo
CM CM CM CM CM
o cn cn cn co
vo i~- cn I-H ro
vo vo vo r~. r~.
ro en in T-I r~.
O O T-H CM CM
vo vo vo vo vo
O O O O O
T-I si-r~. o oo
O o o 1 1 i
ro ro oo co co
O 0 00 0
-H oo in r~- en
O 00 0 O
CM CM CM CM CM
O CD O O O
OO CO OO CO OO
O CM co in vo
in in in in in
vo r-. oo o I-H
co st- in i oo
in in in in in
CM r-. CM I CM
vo oo <-H co vo
r~. r~. oo oo oo
ro oo co co co
«a- CM o co vo
O 1 CM CM CO
CO OO OO CO OO
CM VO O «=»- CO
CD CD T-I T-H T-H
cn vo ro o r-~
CD CM sj- vo r-.
r~.r~r~.r~.r~.
in in in in in
o I-H CM co sr
0 0 0 0 O
CM CM CM CM CM
r-H CM CO sf- in
CM CM CM CM CM
oo cn in i i r~.
oo oo si- in in
CM CM CM CM CM
00000
T-H co in i cn
T-H T-H 1 t-H i-H
co co ro ro ro
vo in co T-H o
ro oo oo oo co
cn vo si- T-H cn
CO cn O i-H T-H
CM CM 00 OO 00
oor-~r-.r~.vo
in i cn i i co
r~.r~.r~.oooo
oo ai m T-H r~-
co oo sj- in in
vo vo vo vo vo
00000
vo cn CM in oo
i-H T-I CM CM CM
CO CO CO OO CO
0 0 0 0 O
T-H co in r~. cn
i-H T-H i-H i-H T-H
CM CM CM CM CM
O CD O O O
CO OO OO CO CO
OO CT> T-I CM sj-
in in vo vo vo
CM ro in vo r~-
m o T-H CM co
i-H CM CM CM CM
in in in in in
r~ CM r~. CM r~.
CO T-H CO VO OO
oo cn cn cn cn
co co ro ro co
si- CM o co vo
si- in 10 vo r~-
OO CO CO CO OO
CM VO O si- CO
CM CM OO CO CO
si- T-H co in CM
en I-H CM si- vo
r~ co co co co
in in in in in
in vo r~. oo cn
o o o o o
CM CM CM CM CM
vo r~- co en o
CM CM CM CM CM
co cn in i i r~.
vo vo r~- oo oo
CM CM CM CM CM
00000
T-H co in r~- cn
CM CM CM CM CM
co co ro co ro
co r~. in ro CM
vo si- i i cn vo
CM ro si- si- in
oo co co oo oo
vo in in in «*
in r~. cn T-H co
oo oo oo cn cn
co cn in T i r~«
vo vo r~- co oo
vo vo vo vo vo
o o o o o
ro oo oosj-sj"
ro co co ro co
o o oo o
CM CM CM CM CM
CM CM CM CM CM
O O O O O
OO CO 00 CO OO
in r~- ooo I-H
vo vo vo r~- r~-
cn o T-I co sj-
s»- vo r~-co en
CM CM CM CM CM
in in in in in
CM r~- CM r~- CM
il OO VO OO T-H
o o o o I-H
si- CM O OO VO
oo cn o CD T-H
oo co cn cn cn
CM VO O si- OO
si- si- in in in
cn vo ro o r~.
r~* m T-H co sj-
co oo cn cn cn
in in in in in
o I-H CM co sr
T-H i 1 r- 1 T-i T-H
CM CM CM CM CM
T-H CM OO si- in
CM CM CM CM CM
co cn in T-H i
cn cn CD T-H T i
CM CM co co ro
CD CD O CD CD
I-H co in r~- en
co co oo oo co
oo co ro ro co
CD cn r~- in si-
CM VO T-H VO II
si- T-H cn vo sr
vo i r~- co cn
ro co co oo co
sj- co ro ro CM
in r~- en T-H co
cn cn cn CD CD
ro cn LO T-H i~.
cn cn o T-H T-H
CD O O O O
vo cn CM in co
st- si- in in in
ro ro co co ro
O O O o O
i i co in r~- en
ro oo co co co
CM CM CM CM CM
0 0 0 O O
co oo ro oo oo
ro si- vo i cn
r^ ^~ r~« r~. r~.
in vo co cn CD
CD T-H CM co in
ro ro ro co ro
in in in in in
r~- CM r~, CM r~-
co vo oo T-I co
I i 1 i-H CM CM
^1- CM O CO VO
CM 00 si- si- LO
en cn cn cn cn
CM VO O si- CO
vovor~.r~.r~.
si- T-I oo in CM
vo oo cn T-H oo
cn cn cn o o
in in in in in
in vo r-~ oo en
T-H T-H I-H T-H I 1
CM CM CM CM CM
vo t-~ oo cn o
CM CM CM CM CM
ro cn in r-i i
CM CM OO sj- si-
ro oo co ro ro
CD CD O O O
T-H co in r-- cn
oo co co co oo
CM i i cn f~ vo
vo T-H in o in
T-H cn vo si- T-H
O O T-I CM OO
CM T-H T-H T-H O
in r~- cn ii ro
co cn Ln T-H r
CM CM CO si" sj-
0 O 0 0 0
vo vo vo r*~- r~.
co co ro co co
O CD O O O
i i co in i cn
CM CM CM CM CM
O 00 0 0
CO OO CO CO 00
O CM ro in vo
oo oo oo oo oo
CM co si- vo r~-
vo r~. co cn o
CO CO CO CO sj-
in in in in in
CM r~. CM r~- CM
VO OO T-H OO VO
CM CM CO CO ro
si- CM O OO VO
vo r~. oo oo cn
cn o> cn cn cn
CM VO O si- OO
co oo cn cn cn
cn vo oo o i
si- VO 00 O T-H
0 O 0 T-I T-I
in in in in in
O t-H CM CO «*
CM CM CM CM CM
CM CM CM CM CM
T-H CM co si- in
CM CM CM CM CM
ro cn in I-H r-~
in in vo r~- r~.
ro ro ro ro oo
CD O O O CD
T-H ro in i en
in in in in in
co oo co co ro
sj- oo i i cn co
o in o si- cn
cn vo si- T-H oo
co si- in vo vo
o cn cn cn co
in vo oo o CM
co cn in T-H r~.
in in vo r~- 1~.
o o o o o
vo cn CM in oo
r~. r~. co oo co
co co co co ro
o o o o o
ti ro in r~. cn
in in in in in
CM CM CM CM CM
00000
co co co co ro
co cn T-I CM si-
co oo cn cn cn
oo cn I-H CM co
i i CM si- in vo
in in in in in
r~- CM r~- CM i~.
OO i-H CO VO OO
OO s^ si* sj* sl"
sl- CM O 00 VO
O T-H CM CM OO
00000
I 1 T 1 I-H I 1 1 1
CJ VO CD si- CO
O O T-H T-H i-H
in in in in in
si- T-H oo in CM
co in vo co o
T-I i 1 i 1 i 1 CM
in in in in in
in vo r~. oo en
CM CM CM CM CM
CM CM CM CM CM
VI.T r~. co cn o
CM CM CM CM CM
-------
i
in
8
oc
o
LL
GO
_ g
a) r*
3 <
.£ oc
§ z
^ z
*s
I- ^
LU
_l
<
C3
cn
O
E
CM Q-
O 1
CO CO
X IE
:c o
O 0
cj
CO
-T- 7j-
00
"ii
co co
1- CMS:
I-H O^
z: co CD
3 X =>
a. i
Q co s:
LU 1 O_
X Q.
s: __^
VO
CM :E
o *v.
(/> CD
£=F
CO CD
1 ^
CM
o
z. z
o
11
_l
_J
1 1
= CM
a: o
Lul CO
a.
CO
I
ce:
«t CO
a. o
z.
I-H
CO
1-1 o
Z. CJ
ID
C£ CM
LU O
t z:
LU
S
CJ
1-1 a.
ca co
3 -
^~
§ CM
CD O
0 CO
CJ
CO
Z 0
11
00
t «
'z. 2:
=5 o?;
CJ CD
i i
Q.
CO
LU^^
1-1 Of. h-
CO
ro cn in T-I r-.
co co cn o o
OO OO OO ^- <*
O 0 0 0 0
I-H OO in 1 cn
V0 ict to m in
CO co CO co co
vo m oo r-H o
«* cn «* cr> -3-
VO CO i-H OO VO
r*-» co cn cn co
«* «* «* ** in
co i>. r-~ r-. vo
«* vo co o CM
CM CM CM CO CO
oo cn in I-H r^
00 00 Cn 0 0
o o o o o
i i * Is- o co
Cn Cn cn CO O
co co co «* «*
0 0 OO 0
i-i co in r~» cn
CM CM CM CM CM
CO O O O O
OO CO CO CO OO
m i oo o i i
Cn Cn Cn O O
i-H i-l r-H CM CM
in u> r cn o
r~- co en o CM
«* =! *J- 10 in
in in 10 in in
CM I--. CM r^ CM
t-i CO <£> OO ^H
m in in in vo
«3- «J- ^s- ^- =*
^- CM o oo ID
^f in vo vo r^
o o o o o
CM *O O * OO
CM CM CO CO CO
10 in 10 in in
o> u> co o r~
1-1 co in i-x oo
CM CM CM CVJ CM
CM CM CM CM CM
in in in in in
O «-H CM CO *i-
CO CO CO CO CO
CM CM CM CM CM
i-l CM CO «S" if>
co co co co co
CM CM CM CM CM
co an in i-i r-.
I i 1 CM CO CO
* sf si- «l- »s-
o o oo o
t-i co in r-^ o>
i i r-~ i-- h-
co co co co co
oo f- ir> co CM
00 CO OO CO OO
CO r-1 OO ID CO
i 1 CM CM CO *i"
in in in in in
10 in ir> in «d-
«* CM if> oo
O O « < f-H « *
OO 00 0
i i co in i^ cr>
CM CM CM CM CM
00 OO O
CO 00 CO GO CO
co «3- ID r^ en
OO O 0 0
CM CM CM CM CM
fH CM «3" in ID
co ^- in 10 r~-
tr> ID in in in
in in in in in
p^ CM r-» CM r-
CO VO 00 r-* CO
«D 10 ua r- r-^
«* «=l- ^l- * *
«* CM O 00 «O
oo en o o I-H
CM U3 O * OO
«j- *a- in in in
in in in in in
«3- «-n oo in CM
o CM co in r-
co co co co co
CM CM CM CM CM
in in in in in
in 10 r-» oo a>
co co co co co
CM CM CM CM CM
ID i--. oo cn o
CO CO CO CO «3-
CJ CM CM CM CM
co cn in i i r~-
*3- »d- in 10 VD
^f «*«* «a- ^~
o o o o o
t i co in i*» en
CO OO OO CO CO
co co co co co
o en t^ in *
co r»» CM i CM
> i oo ~
in in in tr) in
en ID co o r~.
oo o CM «d- in
co < ^i- ^- ^i-
CM CM CM CM CM
in in in m in
O i-l CM CO "51-
«i- «i- «* * ^r
CM CM CM CM CM
T-4 CM CO *3" in
«*«*«!'*-*
CM CM CM CM CM
co en m r-i r-~
r*. r^ oo en en
«s- «d- 1-^-«*
o o o oo
w-i co in r-. en
en en en en en
co co co co co
CM i-i en r-. vo
I^» CM o i-H t-i
in in vo VD 10
CM r- i i I t 1 O
*1" IO CO O CM
in in in ID ID
ro cy> m i 1 1
r- r-. co en en
CO CO CO CO CO
o o o o o
ID en CM in co
CO CO ^f- «d- *3-
o o o oo
I-H co in i--. en
CM CM CM CM CM
CO O CD O O
CO CO CO CO CO
CO en I-H CM i CM CM
cn cn cn cn cn
o O o o o
t-i «d- r>- o co
in in in VD vo
o o o o o
I-H oo in r^ cn
CO CO CO CO CO
o o o o o
co co co oo co
in r-~ oo o i-i
CM CM CM CO CO
CM CM CM CM CM
t-i CM co in vo
O i-H CM CO «3-
in 10 in in in
CM r-- CM i-- CM
i i co vo oo t-i
O O O O i-H
in in in in in
»3- CM o co vo
CO i CM CM CO
CM CM CM CM CM
CM VO O * CO
O CO I-H rH T-I
VD VO VD VD VO
cn VD co o i^
in r-. cn i i CM
in in in vo vo
CM CM CM CM CM
in in in in in
O t-4 CM OO "Sf
in in in in in
CM CM CM CM CM
"H CM CO «* LO
LO in in in in
CM CM CM CM CM
co cn in i r^
co co «3- in in
in in in in in
o o co o o
I-H co in r~. cn
vo in co i i o
in o in o in
CO I-H CO VO CO
vo r>- r»- oo cn
VD VO VD VO VD
oo r-» r-v f-. vo
co in r~ cn I-H
co cn in I-H r-~
co co ti- in in
cn cn cn cn cn
o o o o o
VD cn CM in co
vo vo r~~ !>. r^
o o o o o
i i oo in i cn
co co co co co
OO 0 0 O
co co co co ro
oo «* vo i cn
CO OO CO CO CO
CM CM CM CM CM
I-~ OO O t-l CM
in VD oo cn co
1 t-~ 1 t-^ CO
LO in in in in
r~- CM r»- CM r^
OO VD OO t 1 CO
i 1 1 i-H CM CM
in in in in in
^l- CM o co vo
^l- in vo vo r~
CM CM CM CM CM
CM VO O ^f OO
CM CM OO CO OO
VO VD VD VO VD
sj- r-n co in CM
si- vo r-~ cn I-H
vo vo vo vo r^
CM CM CM CM CM
in in in in in
in vo r^ co cn
in in in in in
CM CM CM CM CM
vo i-~ oo cn o
in in in in vo
CM CM CM CM CM
36
-------
in
cri
3
in
d
cc
o
< o
g
_l
_l
2
QQ
2
o
tr
i
Q.
CM IX
0 1
CO CO
x n:
31 O
o o
o
co
:c ic
o o
(J O
to ro
1 CMS:
I-H O -^
2: co cs
:z> x rs
D- 1
Q co s:
LU t O-
X D-
E: ^__^
tO
S^
CO Cfl
xs:
0- 1
co en
li^
CM
2: z.
o
1
_J
_l
1 i
21 CM
oc o
LU CO
O.
CO
fe
et oo
CL 0
z.
1 1
CO
1
M O
z. o
:z>
o: CM
UJ o
I 2:
LU
E:
o
1 « O_
03 CO
s *-
^
CO
S CM
13 O
O CO
C£
O
* 1
21
CO
z 0
i i
CO
l-< CO
2= s:
=3 0---.
O C3
^
HH
CO
Q-
co
LU-
>- OH
CO
t-l CM CO ST LO
CO OO CO OO 00
LO IO LO LO IO
CM r-» CM l*» CM
tO OO i 1 CO \O
CM CM CO CO CO
to LO LO LO LO
SCM O OO tO
cn o o 1-1
CM CM CO CO CO
CM VO O *J- OO
*a- «a- LO 10 LO
to to to to to
i^ r^ r^ t-~ r^
CM CM CM CM CM
IO LO LO LO LO
O i-l CM CO ^f
to to to to to
CM CVJ CM CM CM
i 1 CM CO * LO
to to to to to
CM CM CM CM CM
CO O> LO -! r»-
cn o> o i i >
LO 10 to to to
o o o o o
t-H CO LO 1 Cf>
CO CO CO CO CO
*d" *3- «3- "9- <*
O Cn !* LO ^1-
* OO CO OO CO
OO LO CO O OO
co -d- LO to to
si- co co co CM
co LO r^ cn i i
cr» en cy» o* o
CO CTl LO i-l r-
cn cn o «-H i i
cn cn o o o
O O t-l i 1 i 1
to cn CM LO oo
cn cn o o o
«a- «a- to to LO
o o o o o
r-i co to r-». cn
co co co ro co
co co co co co
o o o o o
CO OO CO OO CO
00 Cn rH CM «*
st si" LO LO LO
CM CM CM CM CM
O i-H CO «* LO
r-. oo cn o t-i
oo 00 oo cn cn
LO LO IO LO LO
r-. CM i-- CM r-.
OO .-1 CO ID CO
co ^- ^i- ^- «*
LO LO LO IO LO
* CM O OO to
CM CO si" ** IO
co co co co ro
CM to o ^r co
to to r^ r-. r~.
to to to to to
«* «-i CO 10 CM
i-H CO -st tO CO
OO OO OO CO OO
CM CM CM CM CM
LO LO LO LO LO
LO to i-- oo cn
to to to to to
CM CM CM CM CM
to r- oo cn o
to to to to P
CM CM CM CM CM
co cnio 1-1 1-^
CM CM CO *f 1-
to to to to to
O OO O O
rH co LO r-». cn
«s- «* <* «« **-
«d- <*«*'* SI-
CM >-icn i^. to
oo co r>» CM r^
LO COO CO LO
r^ co cn cn o
CM i 1 r-H 1 O
co LO i^. cn i
o oo o 1-1
co cn to I-H r^
CM CM CO «* ^J-
O O 0 0 O
t-H i 1 i 1 i 1 t 1
i-i st-r^ o co
i 1 i-H i 1 CM CM
LO LO LO LO LO
O OO O O
I-H co 10 t-»- cn
<*«*«*«*«*
OO CO CO CO CO
O OO O O
00 CO CO CO 00
to r-^oo o T-H
LO LO LO tO VO
CM CM CM CM CM
r>. oocn t-i CM
CM co^r to r^
cn cn cn cn cn
LO LO LO LO LO
CM r»» CM 1 CM
i-i CO IO OO «-l
IO LO LO LO U3
LO LO LO LO LO
«* CM O CO IO
to 1^.00 oo cn
ro co co co co
CM to O «* OO
co oo cn cn oS
to to to to to
cn to co o r-.
cn 1-1 co to to
oo cn cn cn cn
CM CM CM CM CM
LO LO LO LO LO
O i-l CM CO *d-
p*"1* ^* p** r^ i^^
CM CM CM CM CM
i-H CM CO «* LO
r*^ f^* p*^ f*^ ^^
CM CM CM CM CM
^7
co cn to I-H r>-
10 to to r-. r-~
to to to to to
o o o o o
-i co to r-. cn
LO IO LO LO LO
^- ^- ^- ^- ^-
sf co i i cn oo
CM l»» CM IO r-H
CO O OO 10 CO
T-I CM CM CO ^J-
OO OO 00 OO 00
o en cn en oo
co «* to oo o
co cn 10 i i r-»
to to to r~ r~-
o o o o o
i 1 i 1 i 1 i 1 i-H
to cn CM LO oo
CM CM CO CO CO
LO LO LO IO LO
o o o o o
t-i co 10 i-» cn
IO LO LO IO LO
co co co co co
O O O 0 O
CO OO CO OO CO
co «a- to r~- cn
to to to to to
CM CM CM CM CM
CO «S- to 1^. OO
oo cn o 1-1 CM
cn cn o o o
LO LO LO LO LO
r-» CM rv. CM r»«
CO IO OO i-H CO
to to to r-. t-v
IO LO IO LO LO
sj- CM o oo to
CD T-I CM CM CO
*3- vi- «a- -a- **
CM to o «a- oo
O O i 1 1 i 1
t-. t~- ix. r^ r-^
»* i-l CO 10 CM
00 O r-H CO IO
cn o o o o
CM CO CO CO CO
LO IO LO LO IO
10 to r- oo cn
r-~ t~- r-~ r^ r^
CM CM CM CM CM
to !». oo cn o
r^ r-» r~ r^ oo
CM CM CM CM CM
OO O> IO i-l 1^.
oo co cn o o
to to to i r»-
o o o o o
i-i co LO r-, cn
to to to to to
to 10 co i i o
IO «-H tO i 1 to
O OO IO CO O
10 to tor^ co
OO CO OO OO CO
co r>. r-. r^ to
CM ^ to 00 O
CM CM CM CM OO
co cn to i i r-
goo cn O o
1-1 «a-r-- o co
«3- «d- sf IO LO
LO IO LO LO LO
O CD O CD O
i i co to r-. cn
to to to to to
co oo co co co
0 OO O O
OO CO 00 CO OO
O CM CO LO IO
CM CM CM CM CM
o i i CM *r LO
«d- to to r~- oo
o o o o o
LO LO LO IO tO
CM I-- CM l-» CM
to co *-t co to
r-- r-. oo oo oo
LO LO LO IO IO
sfr CM O OO to
«* 10 to to r-~
«a- «d-«**4- *a-
CM to O «* CO
CM CM CO CO OO
cn to co o r~.
IO OO O CM OO
OO OO CO CO OO
LO IO LO LO LO
§-1 CM OO si-
00 00 0000
CM CM CM CM CM
i 1 CM CO
-------
CD
cn
i
in
d
IT
O
LL
CO
ll
~~ o
O- 1
o co E:
UJ 1 O_
X Q.
s: ___^
vo"
2^
co cr>
£=?
CO CO
1 3
CM
o
o
1*
_J
_l
1 1
* CM
cc. o
LU CO
Q.
CO
h-
cc
xf. CO
CC 0
zz
t 1
CO
1
1-1 0
z: o
:r>
a:
1 1
5:
CO
ZT O
1 1
CO
1 1 CO
^ y
= 0^.
<_> CD
CO
O-
CO
LU^-
1-1 OC 1
OO . oo o I-H
oo co oo en en
CM CM CM CM CM
ro <* in r-. 00
in vo r-~ oo en
CM CM CM CM CM
in in in in in
CM f-. CM t-~ CM
i l CO VO OO i '
0 0 O 0 i-i
IO IO CO IO l£>
*f CM O OO IO
CM co «* ^f in
in in in in in
CM IO O «d" 00
10 ID r~- r^ t~-
i t~~ i~~ t~~ r
en vo co o r-~
co in i~- cr> o
CM CM CM CM CO
CO CO CO CO CO
in in in in in
O t-i CM ro «d-
CM CM CM CM CM
t i CM co «* in
CD en en en en
CM CM CM CM CM
co o> in t-i r-
(^ ^ co CT» ex»
r~« hx r^ r^ r^
OO 0 0 O
t-i ro in r-x
O> CTk O% CD CD
«* «* ^*- *3- -SI-
CM r-H CD r- vo
CD «i- CO CO 00
CM O l*»- in CM
vo i r-» oo CD
CD CD CD CD CD
CM c-H <-H i-l O
CM «1- ID OO O
in in in in «o
CM CM CM CM CM
co CD in r-i r~
r~ Is* co en CD
IO CD CM in CO
in in in in in
oo oo o
i i co in r*. CD
co co co ro ro
OO OO O
co oo co oo ro
co «* 10 i-» cri
CD CD CD CD CD
CM CM CM CM CM
CD O CM CO ^»-
OCM CO ^j- in
CM CM CM CM CM
in in in in in
i-. CM I--CM r-»
CO «3 OO > l CO
< 1 < 1 rH CM CM
ID IO ^D *O CD
sf CM O CO U3
«3 r-» OO CO CD
in in in in in
CM U3 O * CO
OO OO CD CD CD
p** ^^ p"* r*^ ^^
^»- > i co m CM
CM *j- in r^ CD
co co co co ro
co co co co ro
in in in in in
in 10 r^ oo CD
CM CM CM CM CM
<£> l~- CO CD O
CD Ol CD CD O
CM CM CM CM CO
CM 10 O *1-CO
O O 1 i 1 «-H
CO CO OO 00 CO
o o o o o
i i co in i~v CD
o o o o o
in in in in in
CM i-~. t i in o
i-H r-H CM CM CO
CD *t* CD ^" CT»
CD O O i I « 1
CD O O O O
r-» o co vo CD
r-l CO ^t" in VO
VO VO VO VO VO
CM CM CM CM CM
CM VO O -sf CO
O O r-l fH r-H
CM CM CM CM CM
t-H CO in 1 CD
vo vo 10 vo vo
o o o o o
O r-l CM CO ^J-
«r *i- «d- *i- «s-
o oo o o
in in in in in
O r-H CM CO «*
o o o o o
co co co ro co
«=f r-< CD VO CO
vo r>. r-~. co CD
CM CM CM CM CM
in in in in in
CM r CM t^ CM
vo oo r-i ro vo
CM CM ro ro oo
vo vo vo vo vo
ro co co oo ro
O O l i l CM
vo vo vo vo vo
i-H CO in !->. CD
o o o o o
oo oooo co oo
VO OO O CM ^1"
o t i co «* in
** «d- «d- «d- <<3-
co co co co ro
in in in in in
O r-l CM CO «tf-
co co co co ro
I-H CM CO *3- in
0 0 O OO
co co co co co
CM VO O *J" CO
CM CM ro co co
00 CO CO 00 00
o o o o o
i-< co in h~ CD
i 1 i 1 r- i r-l l 1
in in in in in
* CD co r^. CM
co co ^J- ^f in
<* CD *»- CD "3-
CM CM ro co «*
o o o o o
co vo CD CM in
OO CD O CM CO
vo vo r~» r>. r»
CM CM CM CM CM
CM VO O *i- 00
CM CM CO CO CO
CM CM CM CM CM
r-l CO in t-^ CD
vo vo vo vo vo
CD O O O O
in vo r^ co CD
«*«* «* «3- ^1-
o o o o o
in in in in in
in vo r-. co CD
o o o o o
co co co co ro
r-l OO VO CO O
O O r-l CM CO
CM CM CM CM CM
in in in in in
i^ CM r~- CM r-.
CO rH CO VO CO
ro ^j- =* «i- ^~
vo vo vo vo vo
CO CO CO CO OO
CM co co ^r «s-
vo vo vo vo vo
i i co in r CD
CO OO CO 00 CO
VO CO O CM <-
vo r-. CD o i i
<( ^- < in in
co co co co co
in in in in in
in vo r-» co CD
ro co ro co ro
vo i-~ oo CD o
O O O O t-H
co co co co co
CNJ VO O «* 00
'* ^c in in in
00 CO OOOO 00
o o o o o
i i co m i CD
CM CM CM CM CM
in in in in in
vo i i in CD «*
in vo vo vo i^
CD «^~ CD *3* CD
^- in in vo vo
o o o o o
cr> CM in oo r-i
«* VO l*» OO O
CM CM CM CM CM
CM VO O ^f CO
^- «d- in in in
CM CM CM CM CM
r-i co in r^. CD
vo vo vo vo vo
O O O O CD
O tl CM CO *3"
«i- «d- *J- ^- *
o o o o o
in in in in in
O «l CM CO *
ro co co co co
oo in ro o i~~
co «3- in vo vo
CM CM CM CM CM
in in in in in
CM r~- CM r^ CM
r-i CO VO OO 1
in in in in vo
vo vo vo vo vo
ro oo co co ro
in in vo vo r^
vo vo vo t*"1 vo
r-i ro in i CD
CM CM CM CM CM
CO OO 00 00 00
VO OO O CM «3-
CM co in vo r-
in in in in in
oo ro ro ro ro
in in in in in
O r-l CM CO "*
co co co ro co
i i CM co ^f in
r-H t 1 r-H r-l r-l
co ro ro co ro
CM vo o vr oo
vo vo h- r^ rv
OO CO OO 00 CO
o o o o o
r-i ro m i-~ en
ro co co co co
in in in in in
co ro r~ i < vo
r~- oo co CD en
«3- CD «S- CD ^~
r-. t^. oo oo CD
00000
in co > i «j- r-»
t-t CM ^t- in vo
00 CO CO OO 00
CM CM CM CM CM
CM VO O ^- 00
vo vo r^ r^ i-^
CM CM CM CM CM
r-i ro in t^. CD
vo vo vo vo vo
o o o o o
m vo r^ co CD
^- ^- ^- sj- sj-
o o o o o
in in in in in
in vo i oo CD
co co co co co
in CM o r^ ^l-
r~> co CD CD CD
CM CM CM CM CM
in in in in in
i^ CM i^ CM r-~
co vo oo 1-4 ro
vo vo vo i~- i
vo vo vo vo vo
OO CO OO CO OO
r~ oo co CD CD
vo m vo vo vo
rH CO in 1-^ CD
co co co ro ro
00 CO 00 00 00
VO OO CD CM «3-
00 CD rH CM CO
in in vo vo vo
co co co co ro
in in in in in
in vo r-» co CD
co co co co ro
vo r~. co CD o
rH rH rH I 1 CM
co co co ro co
-------
If)
£
EC
O
oo
O
%
<
cc
31
JB
J3
co
LU
-J
CD
O
2
cc
i
Q-
CM (X
O 1
CO CO
x 3;
2C O
O <_J
O
to
:E :E
O 0
O O
to ro
h- CM s:
1-1 O -v,
z: co t5
:=> x :r>
d. 1
Q CO 2:
U4 I Q_
X 0.
i i *
s: _^
VO
2^
to o
x E:
IX 1
to o
^"S
CM
,_ O
a
t i
_j
_j
i i
CM
o; o
UJ CO
0-
co
o;
=c co
Q- O
z.
I-H
CO
r-
I-H O
^: o
=>
j
gig
-i
O i
m < a-
= : £
0
v,,^
co ;
1 ~
1 8
O
II
CO
£ °
CO
t .
r-i oo
^ s:
=3 O -^
O CD
ST_
I-H
CO
0.
I
CO
LU- .
t~t OH
CO r-» ^j- 1-<
»-l i-H CM OO «*
<* ^i- «d- ^t- *
CM CM CM CM CM
ir> in in in in
CM |v. CM r^ CM
00 «-i CO >O
r-~ r^ oo oo oo
^O WD 4£> yO iO
CO OO CO OO CO
O O <-< t-i CM
r». r^ t^. r^ r-.
-i co in t~. cr>
<4- ^t- «a- * *
00 00 00 00 00
VO OO O CM *d-
«* in t^. oo en
l£) IO IO IO ^O
CO CO CO CO CO
in in in in in
O t-H CM CO "3-
CM CM CM CM CM
CO CO CO CO CO
r-l CM CO «3" in
CM CM CM CM CM
CO CO CO CO CO
CM VO O «3- 00
O O «-H r-1 ,-t
<7) o> o^ crv en
0 00 OO
i-i co in r-. en
in in in in in
in in in in in
CM r-^ t-4 m o
CM CM CO CO «*
in o in o in
CM CO CO «* «*
« 1 r-4 i-l r-l T-I
r~ o co vo en
«d- <£>r~oocn
CM CM CM CM CM
CM VO O <5f CO
O O I 1 «-H « 1
CO CO CO CO CO
rH r- 1 r-i r-i r-4
t-i co in r^.o>
in in in in in
10 10 *^ vo 10
o o o o o
in to i»« co en
CM CM CM CM CM
o oo oo
in in in in in
in «o r-. co en
CM CM CM CM CM
CO CO CO CO CO
en vo«a- r-< oo
«* in vo r^ t^
«* «*^-«d-«a-
CM CM CM CM CM
in in in in in
r^ CM r-- CM r>-
§«-( CO U3 OO
en en en en
VD UD CD *£> 1O
CO CO 00 CO OO
CM CO CO *i-«3-
r-i co in i^. en
in in in in in
oo co co co GO
SCO O CM «*
r-i co <* in
r>. r~. r~- (^ !>.
CO CO CO CO CO
in in in in in
in 10 r>» co en
CM CM CM CM CM
CO CO CO CO PO
10 r-. co en o
CM CM CM CM CO
CO CO CO CO CO
CM IOO*3- CO
CM CM CO CO CO
en en en en en
ooooo
»-«co in r^ en
10 IO 10 IO 10
in in in in in
^- en co iv. CM
* ^i- in in 10
o m o m o
in in to 10 iv.
co vo en CM in
r-l CM CO in IO
CO CO CO CO CO
CM vo o «a- oo
CM CM CO CO CO
CO CO CO CO CO
1 1 1 1 1 1 «-( t 1
r-i PO in iv. er»
IO 10 VO IO 10
10 IO 10 IO IO
ooooo
O r-l CM CO «*
CO CO CO CO CO
ooooo
in in in in in
O r-l CM CO ^-
CO CO CO CO CO
CO CO CO CO CO
to co r-i co in
co cno O r-i
«
cn cn cn cr\ cn
in in in in LO
o in cn co oo
rH t-H rH CM CM
VO rH VO rH VO
CM CO CO =* cn
CO CO CO CO CO
rH rH i 1 rH i 1
i i co in rv. cn
cn cn cn cn cr»
vo vo vo vo vo
CD O O O O
in vo rv. co cn
«a- «a- *i-
-------
Lf)
O>
3
in
d
o
CM
to
q.
cc
O
UL.
JL?
~~ o
0)
S
to
o
<
_J
O
Q.
CJ
cc
O
E
CM O_
O 1
if) in
X 3"
3C O
0 0
O
CO
31 3C
O O
O
CM 10 O =! CO
O O r * i I r-H
O O O O O
T i co in r~ en
o o o o o
tO IO IO IO IO
CM i T-H in o
oo co «* «* in
i 1 tO i 1 IO i-H
in in to to r--
CM CM CM CM CM
r-v o co to o\
r~~ en a I-H CM
CM CM CO CO CO
co co co co co
CM to o e- oo
O O 1 1 I-H r I
«d- ^- «* «* **
t i co in r-. en
o o o o o
o o o o o
O i 1 CM OO ^T
LO in m LO m
<3- <* "* * *
00000
in in in in in
in in in in in
co co co co co
>3- I-H en to co
oo * cy» cr> ot
to OO O CM "*
o I-H co >* in
o o o o o
«* ^- ^1- «d- ^1-
in in in in in
O < i CM co
f 1 i-H rH r 1 t 1
to to to to to
«* en co i-~- CM
m m to to i^
to 1-4 to i i to
r~ oo oo CT> CT>
CM CM CM CM CM
co to cr> CM in
^- in to oo en
CO CO CO CO CO
co co co co co
CM to O «d- OO
CM CM CO CO CO
^f <* «d- =!- *
i 1 t-H t-H i 1 r-t
t i co in r~- CT>
i-H ii f-H r-l i<
o o o o o
in to r- oo CM
in in in in in
o o o o o
in in in in in
in to r-^ oo CTI
in in in in in
co co co co co
il OO to CO O
I-- r>- oo en o
10 to to to r^
CM CM CM CM CM
in in in in in
r-~ CM i~- CM !-»
co to oo I-H co
to to to r^ r
OO CO OO CO CD
t1^* oo oo cr»
oo oo oo oo co
-H co in r-- en
I-H I 1 I 1 I 1 f-H
cr> cn 01 cri o>
tO OO O CM «d-
to r-~ 01 o t-i
O O O i-H r-H
3- * -sf «d- «d-
in in in in in
in to t~- oo cr>
in in in in in
co co co co ro
to r- oo CD CD
in in in in to
co co co co co
CM IO O M- 00
3- «d- in in in
o o o o o
I-H co in r^ cr>
CM CM CM CM CM
to to to to to
to i i in en «a-
l~>. OO 00 OO CTl
i I to i-i to 1
O O «-H 1 CM
CO CO CO CO CO
cr> CM tn oo I-H
o CM co «d- to
«* *!- * »l- ^(-
co co co co co
CM tO O * OO
*j- «d- in in in
>a- * «*«*>*
t-H co in r-* en
CM CM CM CM CM
O O O O CD
CD I-H CM CO *
to to to to to
~ 1 1^.1 1^
CM CM CVJ CM CM
tn in in in in
CM r~~ CM r~- CM
to co I-H co to
r-~ i~- oo oo oo
co oo co oo co
O O i-H i 1 CM
CM o> en en en
r-n co in r*. en
CM CM CM CM CM
CTi CT* CT> *
in in in in in
O 1-1 CM CO - oo o r-t CM
^l- ^j- in in in
co co co co co
CM to O «3- CO
to to r~. i^ r^
^j- < <- ^- «a-
I-H co in r-x CD
co co co co co
CD O O O O
in to i oo en
to to to to to
o o o o o
in m in in in
in to i^ co en
to to to to to
co co co co co
=j- in to to r^
CM CM CM CM CM
in in in in in
l-v. CM 1^ CM I^.
CO r-H CO tO 00
co en en en en
^«v i^^ r^. i^ r^
CO CO OO CO OO
CM CO CO *d- ^f
en en en en en
I-H co in i en
co co co co co
en en en en en
to oo o CM «3-
oo en I-H CM co
i-H r-H CM CM CM
* -3- * *a- «a-
in in in in in
in to r^ oo en
to to to to to
co co co co co
to r co en CD
to to to to r--
CO CO CO CO CO
CM to o =* CO
co oo en en en
CD O O CD CD
i i oo in r^. en
<3- r in r>- co en
CM CM CM CM CM
«3- * «* «!- «*
in in in in in
CD I-H CM CO ^1-
r-- i~~ r^~ r~~ r-^
CO CO CO CO CO
I-H CM co * in
i t-x r^ r~- r~-
CO CO CO CO CO
CM tO O M- CO
CD O «-H r-H (~H
r-H I"H r-l I-H r-H
I-H co in I-*-, en
in LO in in in
to to to to t.o
CM r-~- I-H in o
«3- <* in in to
r~- CM r^ CM r^.
r-~ co co en en
CO CO CO CO CO
i o co to en
o CM co * in
to to to to to
CO CO CO CO CO
CM t£> O >=f OO
O O t-H t-H I-H
in to in in in
r-i co m r~- en
in in in in m
i^. r^ r^. r^ r^
O CD CD O O
tn to r-^ co en
«3- ^i- «* «d- ^
O CD O O O
in LO in in in
in to r-^ oo en
r**- r^>- 1**» r**^ r***
co co co co co
en to >d- I-H co
I-H CM CO <=* ^f
CO CO OO CO CO
CM CM CM CM CM
in in in in in
r- CM i CM r^
CO IO CO I-H CO
i-H r-H i-H CM CM
CO CO CO CO CO
CO CO OO CO CO
r^ co oo en en
en en en en en
i i co in r- en
in in in in in
en en en en en
to co o CM >sj-
O r-H CO -3" in
CO CO CO CO CO
d- ^i- «* «3- «a-
in in in in in
in to t~- co en
r-. r-» i~>. r i-»
co co co ro ro
to r^» co en o
r i^ f^ i*-^ co
oo co co ro co
-------
I
in
o
cc
o
LL.
CO
i 2
§ H-
c <
+: cc
§ Z
B 5
< o
JQ I-
H 1
OJ Q-
0 1
OO CO
x a:
a: o
o <->
o
co
T~ *T"
0 O
O O
to ro
1 CM IE
1-1 0^-
?" CO C9
ID X :D
O- 1
o if> y
LU h O-
X 0.
2- ^
VO
S^
CO CS
S^
CO CO
1 ID.
OJ
0
j*- 7"
O
H-I
_J
_1
i i
= OJ
CC 0
LU CO
Q_
CO
cm.
HH
CQ O.
3 00
0 1
CO
rf
cs c\i
o o
cc co
«->
1 i
s:
5 S
£
i i * *
i S
O C5
I-H
Q.
1
CO
UJ^^
1-10:1
CO «£ I-H
O- UJ z:
2: =D
OJ VO O * CO
oj oj co ro co
. 1 CO LO 1^ Cn
^Q ID VO VO vo
VO VO VO VO VO
«3- cn co r^ oj
10 vo r^ r^ co
CM i CM r~- CM
O O i-H 1-4 OJ
«* «*- «3- ^- «*
co vo cn CM in
r~ co en i i CM
vo vo vo r>- r-.
CO CO CO CO CO
OJ VO O "=J- OO
OJ OJ CO CO CO
LO LD LO LO LO
i i co in i^. cn
VO VO VO VO VO
O O O O O
SI-H OJ CO ^f
CO CO CO CO
o o o o o
LO LO LO LO LO
O i-l OJ CO *J-
00 CO CO CO CO
co co co co co
ID CO t 1 CO LO
in vo i r~- co
CO CO CO CO CO
OJ OJ OJ OJ OJ
LO LO If) in LO
OJ t< OJ 1 OJ
VO CO i I CO VO
OJ oj co co co
CO CO CO OO CO
CO CO CO CO CO
O O i 1 I-H OJ
o o o o o
OJ OJ OJ OJ OJ
I-H co if) r~- cn
VO VD O*» O"» CX» O^
ID CO O OJ **
ID r>. CT> C3 i I
CO CO CO «3- ^1-
^- < «* ^- «d-
LO UD ID LO LO
SI-H OJ CO «d"
CO CO OO CO
co co co co co
i i oj co *i- 10
CO CO CO CO OO
co co co co co
OJ ID O «* CO
^- ^- LO LO LO
t i co in i en
rs. r^ r~~ r~ [^
*D ID *JD 1JD VO
10 t-i 10 cr> ^l-
co cr> en en CD
iv. 00 t-- oj co
oj co co ^i- «a-
«* ^- «a- «* ^i-
cn oj LO oo «-i
co LO vo i en
i-v. r-^ r-» f^ r~
co co co co co
OJ ^D O «* CO
^J- ^t- LO LO IO
LO LO LO LO ID
*-< co LO r-» en
tv. r^ r^ r^ r-^
00000
LO vo r^ oo en
CO OO CO CO CO
«a- ^t- «a- «a-
** * 'i- *J- ^~
LO LO LO LO LO
LO ID r^ co en
CO CO CO 00 CO
co co co co co
VD r~ co en o
co co co co en
co co co co co
OJ VD O ^f OO
10 vo r-. r>- 1
I-H co in r^ en
CO CO CO CO CO
VO IO VD ID VD
oo co r-~ <-> VD
O «-H r-t OJ OJ
CO OO CO OO CO
LO LO VD VD r^
LO OO <-> «3- t^
O i 1 CO * IO
OO OO 00 CO CO
co co co co co
OJ VO O ^1- CO
VD VO 1 I~« l~~
LO LO LO IO LO
rn co LO r^ en
CO CO 00 CO 00
O O O O CD
O t I OJ CO ^f
cn en en en en
*j- ^J- «* * sj-
O O O O CD
LO IO LO LO IO
O i-H OJ CO «*
cn cn en en cn
co co co co oo
o r~. LO oj cn
CO CO *f LO LO
cn cn cn cn cn
OJ OJ OJ OJ OJ
LO LO LO LO LO
OJ t1^ OJ l~v OJ
-4 CO ID CO i-l
LO LO LO LO VD
COCO CO 00 CO
CO CO CO 00 CO
IO IO VO VO C~
CD CD CD O O
OJ OJ OJ OJ OJ
I-H co LO I en
CO CO CO CO CO
cn cn cn cn cn
VD CO CD OJ «3-
co cn i i oj co
3" 'd' LO LO LO
* <* * ^- *
LO LO LO LO LO
O i-lOJ CO «3-
cn cn cn cn cn
co co co co co
i-H OJ CO «3- LO
cn cn cn en cn
co co ro co co
oj VD o *r co
co co Ch en cn
.-H oo LO t-^ cn
cn cn cn cn en
VO VD VO VD VD
CD 10 en co oo
co co co «*=*
00 CO OO CO CO
f^ co co cn cn
. i ^- r>. o co
i^co cn I-H oj
co co co en cn
co co co co co
OJ VO O «* CO
co co cn cn cn
LO LO LO LO LO
i-i co in i en
cn cn cn cn cn
o o oo o
in VD t-^ co cn
cn cn en cn cn
* T ^t- * <*
00000
in in LO in LO
in vo f^ co cn
cn cn cn en cn
co co co co co
i^ ^- oj cn vo
vo i co oo cn
cn cn en cn cn
OJ OJ OJ OJ OJ
LO LO LO LO LO
r-» oj i^ oj i~-
CO VO OO i I CO
ID vo VD rv. r^
CO CO CO OO CO
OO CO CO CO CO
r-~ co co cn cn
o ooo o
OJ OJ OJ OJ OJ
i-i co LO i cn
cn cn cn cn cn
cn cn cn cn cn
vo oo ooj «s-
«3- inr-».co cn
in in in LO in
«a- «3- «3- * ^r
LO LO LO LO LO
LO vo r^. co cn
cn cn cn cn cn
co co co co co
VD r-^cocn o
cn cn cn cn CD
CO CO CO CO ^J"
i i *i- r~. o co
o o o *-H i i
CM OJ OJ OJ OJ
i i OJ CO M- LO
OO 0 0 O
LO LO in in in
oo in oj cn VD
oj vo o co t~^
CD O i 1 i l 1
LO 10 LO in in
in in «a- *a- *a-
CO ^J- LO VO 1^-
cn cn cn cn cn
CO CO CO CO CO
OJ VO O <=1- CO
CD O i 1 i I I-H
VO VO VO VO VD
i-H i 1 i-H t-H i-H
i i co LO i-^. cn
CD CD O CD CD
OO OO CO CO CO
CD O O O O
O i 1 OJ CO «*
O 0 0 0 0
in in LO LO LO
o o o o o
LO LO LO lO LO
CD i 1 CM CO «d"
O O O CD O
** «a- * * *i-
i 1 OJ CO * LO
OO CD O O
*a- «* ^i- «* «*
VD cn CM in co
-H i-H CM OJ CM
CM CM CM CM CM
I 1 I 1 II I 1 I-H
vo t-~- co cn CD
CD O O O i-H
LO IT) LO LO LO
co CD r «d- 1 i
i i in oo oj vo
CM CM OJ CO CO
LO in LO LO in
co co co oj oj
OO cn o i i oj
en cn o CD o
CM VO O ^1- 00
OJ OJ CO CO CO
VO VO VD VD VD
I-H I! i-H r t I-H
I-H co in t^ en
OO CO CO COCO
O O O CD CD
in vo I-- oocn
o o o o o
LO in LO in in
O CD O OO
LO LO lO LO LO
LO vo r^ co en
00000
d- «tf- * -d- *d-
I-H cn vo *i- I-H
^- -3- in vo r^
o o o OCD
co co co co co
CO CO CO CO CO
CO i-H CO VO OO
i 1 CO «3" LO ID
CO CO CO CO OO
CO CO CO CO GO
cn *3- cn %J- cn
oj co co «3- «3-
I 1 I-H I-H I-H I-H
OJ OJ OJ OJ OJ
i i co in i cn
I-H i-H I-H i-H , 1
CD OO OO
co LO vo co cn
vo t^ co cno
vo vo VD vor^
*3- «d- *J- ^t- sj-
LO LO LO LO LO
in vo r-. co en
0 O 0 0 0
<* ^t- «* «* ^t-
vo i^ co cn o
O O O CDi-H
-------
in
CT>
5
DC
O
u.
e/3
fl
2 <
~ o
* z
<8
CD
I-
LU
8
cc
i
§
CM O-
O 1
CO CO
xac
aco
Sii
CO
OO
°ii
co co
1 CM;E
1-1 0-^
0 £=?
i > CO 2T
UJ 1-0.
X O-
1 1 V---
s: ^_^
to"
0^
CO C5
of ^
coca
*~S
OJ
o
1£ ifi
0
1 (
_l
_1
» 1
21 CM
OL O
LU CO
O_
CO
1
CC
eC CO
0- O
» 1
CO
1
i-t o
ZL 0
=>
S g
t §
o
* o-
§ £
0
£
§ CM
CS 0
0 CO
0
1 )
co
z: o
i i
CO
1 *-*
S S
=3 o^:
C_) 15
i-
CX.
co
LU-
1-1 C£ 1
oo «c *-"
o- LU z:
z ra
*-_^
1-1 >sr r-> o co
CO CO CO *J" ^"
CM OJ CM CM CM
-H CM co «* in
LO LO LO in in
oo in CM en to
en co r-» o<-
co <* «* in in
in in in in in
CM CM i 1 i 1 i 1
co ^*- in to r-.
«a- "3- ^- «a- *
O4 tO O *S- 00
«d- »o «d- <-> en
t~^oo cr> o O
CO CO CO CO CO
CO CO CO CO CO
< I CO VD CO i 1
OO O> O i-l CO
OO OO OO CO OO
in o in o in
in «o toi^r-^
CM CM CM CM CM
i i co in i crv
CM CM CM CM CM
O O OO O
t-i CM ^r in i^
CM ro sf in to
"d- ^- «s- «* CM CM in CO
«d- «3- in m in
CM CM CM CM CM
VOP»- OO CTi CD
r**» i^ r^* r^* r**»
in in in in in
co o r-. «d- 1-1
co CM in en co
in vo vo 10 r-.
in in in in in
oo o o>o»
oo en o Oi-i
CM ID O «* OO
10 vo t~-. r^ r^-
LO iO LO lO LO
^H co in r^cr>
CO CO CO CO CO
COCO CO COCO
OO OOO
in 10 r-- CO en
in in in in in
ooooo
in in in in in
LOIO r-. co en
*****
io*J- r-i en 10
i t CM CO CO«3"
CO CO CO CO CO
CO CO OO CO CO
CO ID CO i-t CO
*j-m 10 co en
CO CO CO CO CO
.-I IO t t U> > I
co co en en o
CM CM CM CM CM
r-t co in r»-cn
CO CO CO COCO
CD CD OOO
CO O i-» CO<*-
r>.cn o i-iCM
t^i^ co coco
* *& 1 CO CO
<£> vo » r** p^^ f*1** f^*
LO to m to to
co c^ r*^ *^ »~i
in en CM to o
en en o o I-H
in in to to to
r-». i r^. to to
i-^ co en o <-i
CM to O «* CO
O O I < rH i-H
r-~ i-~- r^ r^ i^
I-H co in r~ en
in in in in in
CO OO CO 00 CO
ooooo
LO to p*. oo en
in in in in in
ooooo
in in in in in
in to r- co en
-i en to «* 1-1
en en o i i CM
CO CO CO CO CO
OO CO 00 CO 00
OO i-H CO to CO
to co en o i-i
en en en en en
co co co co co
co co «* *3- in
CM CM CM CM CM
i i oo in r-». en
in in in in in
ooooo
i-H rH i 1 i-< i 1
co in to co en
en o I-H CM co
co en en en en
«* «1- «d- * ^l-
LO in in in in
in to r^ oo en
* «* «d- «* ^J-
to r^ oo en o
CM CM CM CM CO
^1- «* «* ^1- »*
I-H =!- 1~^ o ro
en en en o o
CM CM CM CO CO
i-H CM CO sj- LO
co co co co co
i^ !>. i^- r^. i-~
in in to in in
oo m CM en to
co r^» I-H >* oo
i-l i 1 CM CM CM
to to to to to
to to LO in LO
CM co «* in to
«* «* -st- «d- <3-
CM to O «d" CO
CM CM CO CO CO
1-^. P». |^ |-^ |-^
i i co LO r>- cn
to to to to to
CO CO CO CO CO
ooooo
O i-H CM CO ^1-
LO LO in LO in
ooooo
in to in in in
O i-5 CM CO «*
* cn
in to to i~~- r-.
CM OJ CM CM CM
i i co in r~» cn
to to to to to
ooooo
i 1 i-H rH i 1 t 1
rH OJ «S- 10 I-,
in to i co cn
cn cn cn cn cn
*
to en CM in oo
O O I-H i-l i I
co co co co co
to r>. co cn o
co co co co "3-
i--. r^ i-^ r~. r-.
m to in in in
co o r>- ^- I-H
CM to en co t^
co co co «d- <*
LT* tO tO tO LO
^- ^* ^J* co co
I co cn CD I-H
^t- ^- »* «* ^1-
CM to O < CO
*3- ^1- LO LO LO
i>» r~ i r~. f».
I-H co in r~- cn
CO CO CO COCO
O CD O O O
in to r^ co cn
in in in in in
CD O CD O O
in in in in in
in to i-». co cn
* «!»<* ^- *
to «d- 1 i cn to
to r-. oo oo cn
CO OO CO CO CO
OO CO 00 CO OO
CO VO CO i 1 CO
CT> O r-i CO ^fr
cft cr* o^ o> cr*
in o to o LO
oo cr» cr» C3 o
CVJ Cxi C\J C\i OJ
f- 1 co LO r-* cn
p""* i**"* r^* P*N. r**1*
ooooo
CO 0 i-H CO <*
O CM CO ^ LO
ooooo
LO in in in LO
in ur> LO in in
LO to r~- co cr>
-------
IT)
cn
in
§
CM
cc
o
LL.
CO
~ O
g <
H
^ g
LU
_l
ca
cc
i
£
CO D-
O 1
co in
X 3C
Z 0
O 0
o
^-^
co
3: DC
O O
co n
1 CM s:
1-1 O '
2: co co
O- 1
a co s
X 0_
s:
co
S^
£=F
CO 13
1 ZD
CM
O
?* ~^-
0
» i
_!
_1
I I
21 CM
LU CO
a.
CO
§ co
2:
1 1
CO
z o
ra
« g
£ i
UJ
~ a
1
CO
S 00
1 1
Q.
CO
LU--*
-> C£ 1
CO < >-i
O- LU Z
Z 13
i i *d- r-. o co
CM CM CM CO CO
CO CO CO CO CO
i 1 CM CO «* LO
«* «a- «d- «**»
in in in to in
oo m CM cn co
0*3- oo --H in
in LO LO VO VO
VO I© VO to VO
CO CO CM CM CVI
CM co «* in vo
co co co co co
*J- *J-«a- «3- si-
CM VO O «* CO
CD to P-- r^. r*-.
t--. r-. r-~ i-~ i^
i i co m i en
CO CO OO OO 00
COCO 0000 00
o o o o o
O i 1 CM CO «*
LO ID If) IT) IT)
00000
LO ID in ir> un
O i-l CM CO sj"
«* * «d- "si- «* <*
<£> O» CM tn OO
CO CO * «!l- «*
CO CO CO CO CO
vo r~ oo CT> CD
»a- «a- **** in
r*^ r*^ ^^ r^» f^
LO in in in to
co o t^ *a- t-i
CO VO O ^1-
10 r~~ r>- oo oo
v£> CO VO VO CO
r-H t 1 » 1 O O
f-. OO CT> O i 1
CO CO CO *d" *^"
CM VO O f OO
oo oo en cr> en
f"*-. r^- 1^ i^^ !**«
-i co in r-» en
en en en en en
00 OO OO 00 OO
o o o o o
ir> vo i oo cr>
»*<* =* «a- »d-
in co in in ir>
o o o o CD
in in in in in
in co i-~- oo en
*J- »i- «*'* -d-
-H en vo * t-H
*3- »s- in co r~.
co co co co co
CO CO CO CO CO
OO CO OO CO OO
OO i-H CO VO OO
.-i co «» in 10
co co co co co
en o*> en o^ en
r CM r^ CM i
co «3- «d- in in
co co co co co
CM CM CM CM CM
I-H co in r-. en
en en en en en
0 OOO 0
co in to co en
CM CO -=J- LO 1O
in in in uo in
in in in in en
in co r-- oo c«
«* * «a- ^j- «a-
co i^ oo en o
* ^- «d- ^j- in
st- ^- «f ^t- *
-< «* i--. o co
in in in vo 10
CO CO CO CO CO
I-H CM co -H
OO 00 COCO 00
i-i co in r~ CTI
00000
en en en en en
O 0 000
O > 1 CM CO «3-
in LO in in LO
LO in in in in
0 00 OO
in in in to en
O -! CM CO «»
in in in in in
«* «a- «a- »i- «a-
en vo * C-H CT>
t-~. oo en O O
CO CO CO «* ^1"
co co co co co
CO 00 CO OO CO
i-t CO VO OO -<
oo en o i co
co co «=» ^- »a-
cn cr> en en en
CO OO CO OO CO
vo vo r-x r-- co
co co co co co
CM CM CM CM CM
i i co in r~ cn
o o o o o
i 1 CM =! LO r^
co en o t i CM
in in in LO in
in LO in in in
O I-H CM CO <4-
LO in LO LO in
^- «* «d- «* i-
t-l CM CO * CO
in in in LO LO
<* ^r en vo
>-H CM CO CO ^1-
co co co co co
OO CO OO CO OO
co co oo « i co
»* in vo oo en
en en cn Ch en
en *i* cn ^ en
oo en en o o
co co co "sf ^~
CM CM CM CM CM
i i co LO r«. cn
f I 1-1 I I r- 1 1 1
00 O i-H CO «*-
co in vo t*~ oo
CM CM CM CM CM
in in LO in in
in LO LO in LO
in vo r-», oo cn
LO LO LO LO LO
«* «* «* 'i- >=r
vo r^ oo cn o
in in in in vo
««r 'J- *i- «
CM CM CM CM CM
cn cn cn cn cn
O CD O O O
O i-l CM CO ^h
vo vo vo vo vo
LO in in in in
o o o o o
LO LO LO LO LO
O i 1 CM CO ^f
vo LO vo vo vo
^r i i cn vo o o o
co co ** sr *
vo i OD cn o
vo vo vo vo r^.
in in in in in
co CD r-- «a- r-i
cor-, o * oo
«d- * in in LO
(^^ r^» t*** r*»» rs^
in LO in >3- *
vo i~- oo cn o
in in in in vo
CM VO O «* OO
vo vo i-- i~~ r~
OO 00 OO 00 OO
i 1 i 1 i-H T * r t
i i co LO r cn
co co co co co
en en cn cn cn
O CD O O O
in 10 i^. co cn
vo vo co vo vo
in in in LO in
OO CD CD O
in in LO LO in
in vo t~^ oo cn
vo vo vo vo vo
I-H cn vo ^h it
cn cn o i-i CM
«* ^l- in LO in
co co co co co
OO CO CO CO OO
CO i-l CO VO 00
vo OO cn o i
in LO in vo vo
cn cn cn cn cn
i-H VO i 1 VO i-H
*a- *j- ir, LO vo
«3- *i- *J- sj- ^j-
CM CM CM CM CM
»-H co in rv. cn
co co co co co
rH rH i 1 I 1 r-i
co in 10 co cn
LO vo i oo vn
co co co oo co
in in in in in
in in in in in
ir> vo t-^ co cn
vo vo vo vo vo
* «=f «* *J- <*
vo rv. oo cn o
vo vo vo vo r-
«* <* sj- ** -cj-
-------
tn
OJ
«
i
LO
1
II
S
(L
O
UL
(0
intinued)
TPATION
Og
^ s
< g
a> °
3 (~
2
H <
h-
_J
_J
O
Q.
ui
03
<
(-
/ORKiNC
:>
to
1
r-«
z:
o
tu
X
1 1
z:
o
14
_J
_J
»«4
£
C£.
UJ
C-
to
&
-.
CO
ac a:
oo
o o
co
CMS:
o-^.
GO CD
X =3
a. i
to 3E
H-a:
O-
to
S5
CO tS
£=F
CO O
! ^
CM
O
CM
O
to
oo
o
o
o
CM
O
n.
to
CM
O
OO
CO
0
,"">
s:
o »«.
<_> C3
i i
a.
oo
UJ ^
»-i cr i
to *i > i
c. uj 2:
2: r>
ii «* 1 o ro
r-i t 1 i l CM C\J
«* «d- «3- * «tf-
t 1 CM CO *i- LO
I c^ i-^ r-~ r--.
i i r~. r^ r--.
in in '.n in in
oo in CM cn vo
i-l LO CTl CM VQ
vo if) in ir>
o o o o o
m LO ir> in in
CD < 1 CM O «*
=* «a- «* vf W-
CTi tjD 1- t 1 CM
CM co *3- ID in
in ir> LD 10 in
ro co co ro ro
ro oo ro oo co
1 CO tO OO i-H
ro «si- in 10 co
10 *^ vo 10 ^o
£T» CT^ C7> CT> CJ1
r~. CM i^. CM c^
«D l~^ t~- OO OO
«* ^»- »* *J «1-
CM CM CM CM CM
r-t CO IO 1 Ol
r-l CM «3" in hv
i i CM ro «d- in
«d- «* * ^l- «3-
in to in in in
u> in in in tn
O i-t CM 00 <*
r-» r^ r~- r-^ r~~
<* ^t- =f «d- *
^H CO CO «* UT
^f ^f "* «* «*
ID cy> CM in oo
CM CM ro CO CO
* «3 vo r^
<*<** *a- ^r
CM Cn CTi
i-i ro in r~- ov
in in in in in
en en CTI 01 en
o o cs o o
in 10 r^ oo en
f^ r^. r»- r- i^.
in in in in m
O O CD O O
in in ix> in LO
m vo r~. oo en
r-»- f~~ r^ i^. i-^
=1- «a- »* * *
10 <(- 1 i en to
<£> r~~ oo oo en
in in in in m
oo ro co ro ro
oo ro oo ro oo
oo vo oo t-i ro
en Q I-* ro «*
10 i r^. t~- r-~
en en cr* cr» en
oo oo co oo ro
CT> CM C3 O i-<
«3- <^ in in in
CM CNJ CM CM CM
-i co no r-. en
in to in in in
*i « ! i < «-H r-H
CO O «-i OO «3-
>J3 CO CT> O r-l
«* TJ- <* in in
in in in in in
LO in in in in
*r> u> rv. co en
r-* r^. ^-^ f f^-.
=r
«* * «a- ^f <=»
<i CM oo -=t in
oo oo oo oo oo
r-» r^ r^ i-^. r-
in in in m in
oo m CM en «3
OO CM l£> CT> 00
en CD o a f-n
r-- oo oo oo oo
r-t t-4 O CD O
I-H CM oo «^- in
r-» t-~ r~^ r~» r
«* * ^J- «* «*
CM tD O «* OO
CM CNJ ro oo co
en en en en en
r--iOOI.ni-~.Ch
in vo vo UD 10
en cr> en en en
O CD O O O
O i-i *
oo oo co oo oo
in in LO in in
00000
in in in LO in
O «-l CM CO *
CO CO CO OO CO
* * «=* «=* <*
d- I-H en vo *j-
O i-H t-H CM CO
us 10 vo vo vo
oo oo ro oo co
oo oo co oo oo
vo oo r- > oo vo
in to oo en o
r^- i r*- &**- oo
en en en en en
on «* en *3- en
i 1 CM CM CO OO
tn in in in in
CM CM CM CM CM
r-t CO LT5 f^ «T»
vo vo vo vo >o
vo I en o CM
CM co ^j- vo r^
in in in in in
in m in in in
in LO to in LO
O r-i-CM 00 sl- «d- «*
r-< CM CO ^- in
oo oo oo co co
sr «* «* «* «a-
*-O O'l CM U~> OO
ir> in us vo VD
* * ft «a- -q-
10 r^ oo cr. o
O3 CO 00 CO CT»
f^. r f^. r^. r^
in 10 in LO LO
co o r-^. «a- r-<
r^. T-i -sj- oo CM
f-H CM CM CM CO
CO OO OO 00 OO
en en en co oo
in vo r~- oo en
r-~ r-^ i^. r^- 1^
* ir> in LO in
in vo r-. OO en
00 00 00 CO CO
* «JT =! * <*
i-i en vo <=* r-t
«* * in vo r-v.
^n vo vo vo vo
ro ro ro co co
CO . r- r--
cn en en en en
r-i co in i~^ en
oo oo oo oo oo
en en en en en
o o o o o
O -: CM CO ^T
en en en en en
in in in in in
o o o o o
in LO uo LO in
O r-l CM CO *?
en en en en en
*J- ** * -* ^J-
cn vo *s- ,-- 1 en
r-. co en o o
vo vo vo f*^ r^
CO CO CO OO CO
CO OO CO OO CO
<-H CO VO CO i-H
co en o < < oo
co oo en en cr>
en en en en en
r-l VO r-l VO *~t
r-~. f^- oo en
in in in in in
CM CO CM CM CM
.~i co in r-- en
oo oo oo co oo
i CM * to r--
^r in vo i^ oo
vo to vo vo vo
in in in in in
LO in in in LO
O <-H CM CO <3-
en en en en en
«3- <- >3- «t- cn cr^
CD CD O O CD
LO vo r-~ oo cn
cn cn cn cn cn
tn in m in in
00000
in in in in in
in to r»- co cn
CTS cn cn cn o>
=*=*«*<* «d-
VO "S- r-l CT> VO
t 1 CM CO CO >*
i-^ i r^ r~- r-^
co ro co co co
CO CO CO CO OO
CO VO OO i 1 OO
«d- uo to oo cn
cn cn cn cn cn
cn en cn cn cn
cn CD O r-i I-H
to vo 10 vo vo
CM CM CM CM CM
I-H co LO r». cn
cn cn cv« cn cn
r-l r~l t-f r-J i 1
CO O t-i CO i*-
cn I-H CM co «*
vo i^- r^ t^ t^
LO in to LO in
LO in LO in LO
LO vo r-- co cn
cn cn cn en cn
** «a- «* «* «d-
VD 1*- CO O1 O
cn cn cn cn o
* ^j- «a- sj- m
-------
Table A-5
REFERENCE TABLE: PSI VALUES FOR CO Wm3) AT EQUALLY SPACED CONCENTRATIONS
CO PSI
0.200 2.0
0.400 4.0
0.600 6.0
0.800 8.0
1.000 10.0
1.200 12.0
1.400 14.0
1.600 16.0
1.800 18.0
2.000 20.0
2.200 22.0
2.400 24.0
2.600 26.0
2.800 28.0
3.000 30.0
3.200 32.0
3.400 34.0
3.600 36.0
3.800 38.0
4.000 40.0
4.200 42.0
4.400 44.0
4.600 46.0
4.800 48.0
5.000 50.0
5.200 52.0
5.400 54.0
5.600 56.0
5.800 58.0
6.000 60.0
6.200 62.0
6.400 64.0
6.600 66.0
6.800 68.0
7.000 70.0
7.200 72.0
7.400 74.0
7.600 76.0
7.800 78.0
8.000 80.0
8.200 82.0
8.400 84.0
8.600 86.0
8.800 88.0
9.000 90.0
9.200 92.0
9.400 94.0
9.600 96.0
9.800 98.0
10.000 100.0
CO PSI
10.200 102.9
10.400 105.7
10.600 108.6
10.800 111.4
11.000 114.3
11.200 117.1
11.400 120.0
11.600 122.9
11.800 125.7
12.000 128.6
12.200 131.4
12.400 134.3
12.600 137.1
12.800 140.0
13.000 142.9
13.200 145.7
13.400 148.6
13,600 151.4
13.800 154.3
14.000 157.1
14.200 160.0
14.400 162.9
14.600 165.7
14.800 168.6
15.000 171.4
15.200 174.3
15.400 177.1
15.600 180.0
15.800 182.9
16.000 185.7
16.200 188.6
16.400 191.4
16.600 194.3
16.800 197.1
17.000 200.0
17.200 201.2
17.400 202.4
17.600 203.5
17.800 204.7
18.000 205.9
18.200 207.1
18.400 208.2
18.6CO 209.4
18.800 210.6
19.000 211.8
19.200 212.9
19.400 214.1
19.600 215.3
19.800 216.5
20.000 217.6
CO PSI
20.200 218.8
20.400 220.0
20.600 221.2
20.800 222.4
21.000 223.5
21.200 224.7
21.400 225.9
21.600 227.1
21.800 228.2
22.000 229.4
22.200 230.6
22.400 231.8
22.600 232.9
22.800 234.1
23.000 235.3
23.200 236.5
23.400 237.6
23.600 238.8
23.800 240.0
24.000 241.2
24.200 242.4
24.400 243.5
24.600 244.7
24.800 245.9
25.000 247.1
25.200 248.2
25.400 249.4
25.600 250.6
25.800 251.8
26.000 252.9
26.200 254.1
26.400 255.3
26.600 256.5
26.800 257.6
27.000 258.8
27.200 260.0
27.400 261.2
27.600 262.4
27.800 263.5
28.000 264.7
28.200 265.9
28.400 267.1
28.600 268,2
28.800 269.4
29.000 270.6
29.200 271.8
29.400 272.9
29.600 274.1
29.800 275.3
30.000 276.5
CO PSI
30.200 277.6
30.400 278.8
30.600 280.0
30.800 281.2
31.000 282.4
31.200 283.5
31.400 284.7
31.600 285.9
31.800 287.1
32.000 288.2
32.200 289.4
32.400 290.6
32.600 291.8
32.800 292.9
33.000 294.1
33.200 295.3
33.400 296.5
33.600 297.6
33.800 298.8
34.000 300.0
34.200 301.7
34.400 303.3
34.600 305.0
34.800 306.7
35.000 308.3
35.200 310.0
35.400 311.7
35.600 313.3
35.800 315.0
36.000 316.7
36.200 318.3
36.400 320.0
36.600 321.7
36.800 323.3
37.000 325.0
37.200 326.7
37.400 328.3
37.600 330.0
37.800 331.7
38.000 333.3
38.200 335.0
38.400 336.7
38.600 338.3
38.800 340.0
39.000 341.7
39.200 343.3
39.400 345.0
39.600 346.7
39.800 348.3
40.000 350.0
CO PSI
W.200 351.7
40.400 353.3
40.600 355.0
40.800 356.7
41.000 358.3
41.200 360.0
41.400 361.7
41.600 363.3
41.800 365.0
42.000 366.7
42.200 368.3
42.400 370.0
42.600 371.7
42.800 373.3
43.000 375.0
43.200 376.7
43.400 378.3
43.600 380.0
43.800 381.7
44.000 383.3
44.200 385.0
44.400 386.7
44.600 388.3
44.800 390.0
45.000 391.7
45.200 393.3
45.400 395.0
45.600 396.7
45.800 398.3
46.000 400.0
46.200 401.7
46.400 403.5
46.600 405.2
46.800 407.0
47.000 408.7
47.200 410.4
47.400 412.2
47.600 413.9
47.800 415.7
48.000 417.4
48.200 419.1
48.400 420.9
48.600 422.6
48.800 424.3
49.000 426.1
49.200 427.8
49.400 429.6
49.600 431.3
49.800 433,0
50.000 434.8
CO PSI
50.200 436.5
50.400 438.3
50.600 440.0
50.800 441.7
51.000 443.5
51.200 445.2
51.400 447.0
51.600 448.7
51.800 450.4
52.000 452.2
52.200 453.9
52.400 455.7
52.600 457.4
52.800 459.1
53.000 460.9
53.200 462.6
53.400 464.3
53.600 466.1
53.800 467.8
54.000 469.6
54.200 471.3
54.400 473.0
54.600 474.8
54.800 476.5
55.000 478.3
55.200 480.0
55.400 481.7
55.600 483.5
55.800 485.2
56.000 487.0
56.200 488.7
56.400 490.4
56.600 492.2
56.800 493.9
57.000 495.7
57.200 497.4
57.400 499.1
57.600 500.9
57.800 502.6
58.000 5C4.3
58.200 506.1
58.400 507.8
58.600 509.6
58.800 511.3
59.000 513.0
59.200 514.8
59.400 516.5
59.600 518.3
59.800 520.0
60.000 521.7
45
-------
Table A-6
REFERENCE TABLE: PSI VALUES FOR CO (ppm) AT EQUALLY SPACED CONCENTRATIONS
CO PSI
0.200 2.2
0.400 4.4
0.600 6.7
0.800 8.9
1.000 11.1
1.200 13.3
1.400 15.6
1.600 17.8
1.800 20.0
2.000 22.2
2.200 24.4
2.400 26.7
2.600 28.9
2.800 31.1
3.000 33.3
3.200 35.6
3.400 37.8
3.600 40.0
3.800 42.2
4.000 44.4
4.200 46.7
4.400 48.9
4.600 51,1
4.800 53.3
5.000 55.6
5.200 57.8
5.400 60.0
5.600 62.2
5.800 64.4
6.000 66.7
6.200 68.9
6.400 71.1
6.600 73.3
6.800 75.6
7.000 77.8
7.200 30.0
7.400 82.2
7.600 84.4
7.800 86.7
8.000 88.9
8.200 91,1
8.400 93.3
8.600 95.6
8.800 97.8
9.000 100.0
9.200 103.3
9.400 106.7
9.600 110.0
9.300 113.3
10.000 116.7
CO PSI
10.200 120.0
10.400 123.3
10.600 126.7
10.800 130.0
11.000 133.3
11.200 136.7
11.400 140.0
11.600 143.3
11.800 146.7
12.000 150.0
12.200 153.3
12.400 156.7
12.600 160.0
12.800 163.3
13.000 166.7
13.200 170.0
13.400 173.3
13.600 176.7
13.800 180.0
14.000 183.3
14.200 186.7
14.400 190.0
14.600 193.3
14.800 196.7
15.000 200.0
15.200 201.3
15.400 202.7
15.600 204.0
15.800 205.3
16.000 206.7
16.1.00 208.0
16.400 209.3
16.600 210.7
16.800 212.0
17.000 213.3
17.200 214,7
17.400 ?J6.0
17.600 ?17.3
17.800 213.7
18.000 220.0
18.200 '21.3
18.400 ^22.7
18.600 224.0
18.800 225.3
19.000 226.7
19.200 2?8.0
19.400 229.3
19.600 230.7
1Q.800 232.0
20.000 233.3
CO PSI
20.200 234.7
20.400 236.0
20.600 237.3
20.800 238.7
21.000 240.0
21.200 241.3
21.400 242.7
21.600 244.0
21.800 245.3
22.000 246.7
22.200 248.0
22.400 249.3
22.600 250.7
22.800 252.0
23.000 253.3
23.200 254.7
23.400 256.0
23.600 257.3
23.800 258.7
24.000 260.0
24.200 261.3
24.400 262.7
24.600 264.0
24.800 265.3
25.000 266.7
25.200 268.0
25.400 269.3
25.600 270.7
25.800 272.0
26.000 273.3
26.200 274.7
26.400 276.0
26.600 277.3
26.800 278.7
27.000 280.0
27.200 281.3
27.400 282.7
27.600 284.0
27.800 285.3
28.000 286.7
26.200 288.0
28.400 28S.3
28.600 290.7
28.800 292.0
29.000 293.3
29.200 294.7
29.400 296.0
29.600 297.3
25.800 298.7
| 30,000 300.0
CO PSI
30.200 302.0
30.400 304.0
30.600 306.0
30.800 308.0
31.000 310.0
31.200 312.0
31.400 314.0
31.600 316.0
31.800 318.0
32.000 320.0
32.200 322.0
32.400 324.0
32.600 326.0
32.800 328.0
33.000 330.0
33.200 332.0
33.400 334.0
33.600 336.0
33.800 338.0
34.000 340.0
34.200 342.0
34.400 344.0
34.600 346.0
34.800 348.0
35.000 350.0
35.200 352.0
35.400 354.0
35.600 356.0
35.800 358.0
36.000 360.0
36.200 362.0
36.400 364.0
36.600 366.0
36.800 368.0
37.000 370 0
37.200 372.0
37.400 374.0
37.600 376.0
37. SCO 3/8.0
38. OOC 380,0
3ft. ZOO 3o?.C
3?. 400 384.0
33.600 386.0
38.800 388,0
39.000 390.0
39.20C 392.0
39.400 ,,94.0
39.600 396.0
39.800 :98.0
40.000 400.0
CO PSI
40.200 402.0
40.400 404.0
40.600 406.0
40.800 408.0
41.000 410.0
41.200 412.0
41.400 414.0
41.600 416.0
41.800 418.0
42.000 420.0
42.200 422.0
42.400 424.0
42.600 426.0
42.800 428.0
43.000 430.0
43.200 432.0
43.400 434.0
43.600 436.0
43.800 438.0
44.000 440.0
44.200 442.0
44.400 444.0
44.600 446.0
44.800 448.0
45.000 450.0
45.200 452.0
45.400 454.0
45.600 456.0
45.800 458.0
46.000 460.0
46,200 462.0
46.400 464.0
46.600 466.0
46.800 468.0
47.000 470.0
47.200 472. 0
47.400 474.0
47.600 476.0
47.800 478, n
48.000 480,0
8.200 4^2.0
48.400 484.0
48.600 486.0
48.800 488.0
49.000 490.0
49.2GO 492.0
49.400 494.0
49.600 496.0
49.800 498.0
50.000 500.0
CO PSI
50.200 502.0
50.400 504.0
50.600 506.0
50.800 508.0
51.000 510.0
51.200 512.0
51.400 514.0
51.600 516.0
51.800 518.0
52.000 520.0
52.200 522.0
52.400 524.0
52.600 526.0
52.800 528.0
53.000 530.0
53.200 532.0
53.400 534.0
53.600 536.0
53.800 538.0
54.000 540.0
54.200 542.0
54.400 544.0
54.600 546.0
54.800 548.0
55.000 550.0
55.200 552.0
55.400 554.0
55.600 556.0
55.800 558.0
56.000 560.0
56.200 562.0
56.400 564.0
56.600 566.0
56.800 568.0
57.000 570.0
57.200 572.0
57.400 574.0
57.600 576.0
57.800 578.0
58.000 580.0
58.200 582.0
58.400 584.0
58.600 586.0
58.800 588.0
59.000 590.0
59.200 592.0
59.400 594.0
59.600 596.0
59.300 598.0
60.000 600.0
-------
Table A-7
REFERENCE TABLE: PSI VALUES FOR O3 (jufl/m3) AT EQUALLY SPACED CONCENTRATIONS
03 PSI
4.000 1.7
8.000 3.3
12.000 5.0
16.000 6.7
20.000 8.3
24.000 10.0
28.000 11.7
32.000 13.3
36.000 15.0
40.000 16.7
44.000 13.3
48.000 20.0
52.000 21.7
56.000 23.3
60.000 25.0
64.000 26.7
68.000 28.3
72.000 30.0
76.000 31.7
80.000 33.3
84.000 35.0
88.000 36.7
92.000 38.3
96.000 40.0
100.000 41.7
104.000 43.3
108.000 45.0
112.000 46.7
116.000 48.3
120.000 50.0
124.000 51.7
128.000 53.3
132.000 55.0
136.000 56.7
140.000 58.3
144.000 60.0
148.000 61.7
152.000 63.3
156.000 65.0
160.000 66.7
164.000 68.3
168.000 70.0
172.000 71.7
176.000 73.3
180.000 75.0
184.000 76.7
188.000 78.3
192.000 80.0
196.000 81.7
200.000 83.3
03 PSI
204.000 85.0
208.000 86.7
212.000 88.3
216.000 90.0
220.000 91.7
224.000 93.3
228.000 95.0
232.000 96.7
236.000 98.3
240.000 100.0
244.000 102.5
248.000 105.0
252.000 107.5
256.000 110.0
260.000 112.5
264.000 115.0
268.000 117.5
272.000 120.0
276.000 122.5
280.000 125.0
284.000 127.5
288.000 130.0
292.000 132.5
296.000 135.0
300.000 137.5
304.000 140.0
308.000 142.5
312.000 145.0
316.000 147.5
320.000 150.0
324.000 152.5
328.000 155.0
332.000 157.5
336.000 160.0
340.000 162.5
344.000 165.0
348.000 167.5
352.000 170.0
356.000 172.5
360.000 175.0
364.000 177.5
368.000 180.0
372.000 182.5
376.000 185.0
380.000 187.5
384.000 190.0
388.000 192.5
392.000 195.0
396.000 197.5
400.000 200.0
03 PSI
404.000 201.0
408.000 202.0
412.000 203.0
416.000 204.0
420.000 205.0
424.000 206.0
428.000 207.0
432.000 208.0
436.000 209.0
440.000 210.0
444.000 211.0
448.000 212.0
452.000 213.0
456.000 214.0
460.000 215.0
464.000 216.0
468.000 217.0
472.000 218.0
476.000 219.0
480.000 220.0
484.000 221.0
488.000 222.0
492.000 223.0
496.000 224.0
500.000 225.0
504.000 226.0
508.000 227.0
512.000 228.0
516.000 229.0
520.000 230.0
524.000 231.0
528.000 232.0
532.000 233.0
536.000 234.0
540.000 235.0
544.000 236.0
548.000 237.0
552.000 238.0
556.000 239.0
550.000 240.0
564.000 241.0
568.000 242.0
572.000 243.0
576.000 244.0
580.000 245.0
584.000 246.0
588.000 247.0
592.000 248.0
596.000 249.0
600.000 250.0
03 PSI
604.000 251.0
608.000 252.0
612.000 253.0
616.000 254.0
620.000 255.0
624.000 256.0
628.000 257.0
632.000 258.0
636.000 259.0
640.000 260.0
644.000 261.0
648.000 262.0
652.000 263.0
656.000 264.0
660.000 265.0
664.000 266.0
668.000 267.0
672.000 268.0
676.000 269.0
680.000 270. Q
684.000 271.0
688.000 272.0
692.000 273.0
696.000 274.0
700.000 275.0
704.000 276.0
708.000 277.0
712.000 278.0
716.000 279.0
720.000 280.0
724.000 281.0
728.000 282.0
732.000 283.0'
736.000 284.0
740.000 285.0
744.000 286.0
748.000 237.0
752.000 288.0
756.000 289.0
760.000 290.0
764.000 291.0
768.000 292.0
772.000 293.0
776.000 294.0
780.000 295.0
784.000 296.0
788.000 297.0
792.000 298.0
796.000 299.0
800.000 300.0
03 PSI
804.000 302.0
808.000 304.0
812.000 306.0
816.000 308.0
820.000 310.0
824.000 312.0
828.000 314.0
832.000 316.0
836.000 318.0
840.000 320.0
844.000 322.0
848.000 324.0
852.000 326.0
856.000 328.0
860.000 330.0
864.000 332.0
868.000 334.0
872.000 336.0
876.000 338.0
880.000 340.0
884.000 342.0
888.000 344.0
892.000 346.0
896.000 348.0
900.000 350.0
904.000 352.0
908.000 354.0
912.000 356.0
916.000 358.0
920.000 360.0
924.000 362.0
928.000 364.0
932.000 366.0
936.000 368.0
940.000 370.0
944.000 372.0
948.000 374.0
952.000 376.0
956.000 378.0
960.000 380.0
964.000 382.0
968.000 384.0
972.000 386.0
976.000 388.0
980.000 390.0
984.000 392.0
988.000 394.0
992.000 396.0
996.000 398. C
1000.000 400.0
03 PSI
1004.000 402.0
1008.000 404.0
1012.000 406.0
1016.000 408.0
1020.000 410.0
1024.000 412.0
1028.000 414.0
1032.000 416.0
1036.000 418.0
1040.000 420.0
1044.000 422.0
1048.000 424.0
1052.000 426.0
1056.000 428.0
1060.000 430.0
1064.000 432.0
1068.000 434.0
1072.000 436.0
1076.000 438.0
1080.000 440.0
1084.000 442.0
1088.000 444.0
1092.000 446.0
1096.000 448.0
1100.000 450.0
1104.000 452.0
1108.000 454.0
1112.000 456.0
1116.000 458.0
1120.000 460.0
1124.000 462.0
1128.000 464.0
1132.000 466.0
1136.000 468.0
1140.000 470.0
1144.000 472.0
1148.000 474.0
1152.000 476.0
1156.000 478. 0
1160.000 480.0
1164.000 482.0
1168.000 484.0
1172.000 486.0
1176.000 488.0
1180.000 490.0
1184.000 492.0
1188.000 494.0
1192.000 496.0
1196.000 498.0
1200.000 500.0
47
-------
Table A-8
REFERENCE TABLE: PSI VALUES FOR 03 (ppm) AT EQUALLY SPACED CONCENTRATIONS
03 PSI
0.002 1.7
0.004 3.3
0.006 5.0
0.008 6.7
0.010 8.3
0.012 10.0
0.014 11.7
0.016 13.3
0.018 15.0
0.020 16.7
0.022 18.3
0.024 20.0
0.026 21.7
0.028 23.3
0.030 25.0
0.032 26.7
0.034 28.3
0.036 30.0
0.038 31.7
0.040 33.3
0.042 35.0
0.044 36.7
0.046 38.3
0.048 40.0
0.050 41.7
0.052 43.3
0.054 45.0
0.056 46.7
0.058 48.3
0.060 50.0
0.062 51.7
0.064 53.3
0.066 55.0
0.068 56.7
0.070 58.3
0,072 60.0
0.074 61.7
0.076 63.3
0.073 65.0
0.080 66.7
0.082 68.3
0.084 70.0
0.086 71.7
0.088 73.3
0.090 75.0
0.092 76.7
0.094 78.3
0.096 80.0
0.098 81.7
0.100 83.3
03 PSI
0.102 85.0
0.104 86.7
0.106 88.3
0.108 90.0
0.110 91.7
0.112 93.3
0.114 95.0
0.116 96.7
0.118 98.3
0.120 100.0
0.122 102.5
0.124 105.0
0.126 107.5
0.128 110.0
0.130 112.5
0.132 115.0
0.134 117.5
0.136 120.0
0.138 122.5
0.140 125.0
0.142 127.5
0.144 130.0
0.146 132.5
0.148 135.0
0.150 137.5
0.152 140.0
0.154 142.5
0.156 145.0
0.158 147.5
0.160 150.0
0.162 152.5
0.164 155.0
0.166 157.5
0.168 150.0
0.170 162.5
0.172 165.0
0.174 167.5
0.176 170.0
0.178 172.5
0.180 175.0
0.182 177.5
0.184 180.0
0.186 182.5
0.188 185.0
0.190 187.5
0.192 190.0
0.194 192.5
0.196 195.0
0.198 197.5
0.200 200.0
03 PSI
0.202 201.0
0.204 202.0
0.206 203.0
0.208 204.0
0.210 205.0
0.212 206.0
0.214 207.0
0.216 208.0
0.218 209.0
0.220 210.0
0.222 211.0
0.224 212.0
0.226 213.0
0.228 214.0
0.230 215.0
0.232 216.0
0.234 217.0
0.236 218.0
0.238 219.0
0.240 220.0
0.242 221.0
0.244 222.0
0.246 223.0
0.248 224.0
0.250 225.0
0.252 226.0
0.254 227.0
0.256 228.0
0.258 229.0
0.260 230.0
0.262 231.0
0.264 232.0
0.266 233.0
0.268 234.0
0.270 235.0
0.272 236.0
0.274 237.0
0.276 238.0
0.278 239.0
0.280 240.0
0.282 241.0
0.284 242.0
0.286 243.0
0.288 244.0
0.290 245.0
0.292 246.0
0.294 247.0
0.295 248.0
0.298 249.0
0.300 250.0
03 PSI
0.302 251.0
0.304 252.0
0.306 253.0
0.308 254.0
0.310 255.0
0.312 256.0
0.314 257.0
0.316 253.0
0.318 259.0
0.320 260.0
0.322 261.0
0.324 262.0
0.326 263.0
0.328 264.0
0.330 265.0
0.332 266.0
0.334 267.0
0.336 268.0
0.338 269.0
0.340 270.0
0.342 271.0
0.344 272.0
0.346 273.0
0.348 274.0
0.350 275.0
0.352 276.0
0.354 277.0
0.356 278.0
0.358 279.0
0.360 280.0
0.362 281.0
0.364 282.0
0.366 283.0
0.368 284.0
0.370 285.0
0.372 286. 0
0.374 287.0
0.376 283.0
0.378 289.0
0.380 290.0
0.382 291.0
0.384 292.0
0.386 293.0
0.388 294.0
0.390 295.0
0.392 296.0
0.394 297.0
0.396 298.0
0.398 299.0
0.400 300.0
03 PSI
0.402 302.0
0.404 304.0
0.406 306.0
0.408 308.0
0.410 310.0
0.412 312.0
0.414 314.0
0.416 316.0
0.418 318.0
0.420 320.0
0.422 322.0
0.424 324.0
0.426 326.0
0.428 328.0
0.430 330.0
0.432 332.0
0.434 334.0
0.436 336.0
0.433 338.0
0.440 340.0
0.442 342.0
0.444 344.0
0.446 346.0
0.443 348.0
0.450 350.0
0.452 352.0
0.454 354.0
0.456 356.0
0.458 358.0
0.460 360.0
0.462 362.0
0.464 364.0
0.466 366.0
0.468 368.0
0.470 370.0
0.472 372.0
0.474 374.0
0.476 376.0
0.478 378.0
0.480 380.0
0.482 382. 0
0.484 334.0
0.486 386.0
0.488 388.0
0.490 390.0
0.492 392.0
0.494 394.0
0.496 396.0
0.493 393.0
0.500 400.0
03 PSI
0.502 402.0
0.504 404.0
0.506 406.0
0.508 408.0
0.510 410.0
0.512 412.0
0.514 414.0
0.516 416.0
0.518 418.0
0.520 420.0
0.522 422.0
0.524 424.0
0.526 426.0
0.528 428.0
0.530 430.0
0.532 432.0
0.534 434.0
0.536 436.0
0.538 438.0
0.540 440.0
0.542 442.0
0.544 444.0
0.546 446.0
0.548 448.0
0.550 450.0
0.552 452.0
0.554 454.0
0.356 456.0
0.558 458.0
0.560 460.0
0.562 462.0
0.564 464.0
0.566 466.0
0.568 468.0
0.570 470.0
0.572 472.0
0.574 474.0
0.576 476.0
0.578 478.0
0.580 480.0
0.582 482.0
0.584 484.0
0.586 4S6.0
0.538 488.0
0.590 490.0
0.592 492.0
0.594 494.0
0.596 496.0
0.593 498. 0
0.600 500.0
48
-------
Table A-9
REFERENCE TABLE: PSI VALUES FOR N02 (M9/m3) AT EQUALLY SPACED CONCENTRATIONS
N02 PSI
1130.000 200.0
1140.000 200.9
1150.000 201.8
1160.000 202.7
1170.000 203.5
1180.000 204.4
1190.000 205.3
1200.000 206.2
1210.000 207.1
1220.000 208.0
1230.000 208.8
1240.000 209.7
1250.000 210.6
1260.000 211.5
1270.000 212.4
1280.000 213.3
1290.000 214.2
1300.000 215.0
1310.000 215.9
1320.000 216.8
1330.000 217.7
1340.000 218.6
1350.000 219.5
1360.000 220.4
1370.000 221.2
1380.000 222.1
1390.000 223.0
1400.000 223.9
1410.000 224.8
1420.000 225.7
1430.000 226.5
1440.000 227.4
1450.000 228.3
1460.000 229.2
1470.000 230.1
1480.000 231.0
1490.000 231.9
1500.000 232.7
1510.000 233.6
1520.000 234.5
1530.000 235.4
1540.000 236.3
1550.000 237.2
1560.000 238.1
1570.000 238.9
1580.000 239.8
1590.000 240.7
1600.000 241.6
1610.000 242.5
1620.000 243.4
N02 PSI
1630.000 244.2
1640.000 245.1
1650.000 246.0
1660,000 246.9
1670.000 247.8
1680.000 248.7
1690.000 249.6
1700.000 250.4
1710.000 251.3
1720.000 252.2
1730.000 253.1
1740.000 254.0
1750.000 254.9
1760.000 255.8
1770.000 256.6
1780.000 257.5
1790.000 258.4
1800.000 259.3
1810.000 260.2
1820.000 261.1
1830.000 261.9
1840.000 262.8
1850.000 263.7
1860.000 264.6
1870.000 265.5
1880.000 266.4
1890.000 267.3
1900.000 268.1
1910.000 269.0
1920.000 269.9
1930.000 270.8
1940.000 271.7
1950.000 272.6
1960.000 273.5
1970.000 274.3
1980.000 275.2
1990.000 276.1
2000.000 277.0
2010.000 277.9
2020.000 278.8
2030.000 279.6
2040.000 280.5
2050.000 281.4
2060.000 282.3
2070.000 283.2
2080.000 284.1
2090.000 285.0
2100.000 285.8
2110.000 286.7
2120.000 287.6
N02 PSI
2130.000 288.5
2140.000 289.4
2150.000 290.3
2160.000 291.2
2170.000 292.0
2180.000 292.9
2190.000 293.8
2200.000 294.7
2210.000 295.6
2220.000 296.5
2230.000 297.3
2240.000 298.2
2250.000 299.1
2260.000 300.0
2270.000 301.4
2280.000 302.7
2290.000 304.1
2300.000 305.4
2310.000 306.8
2320.000 308.1
2330.000 309.5
2340.000 310.8
2350.000 312.2
2360.000 313.5
2370.000 314.9
2380.000 316.2
2390.000 317.6
2400.000 318.9
2410.000 320.3
2420.000 321.6
2430.000 323.0
2440.000 324.3
2450.000 325.7
2460.000 327.0
2470.000 328.4
2480.000 329.7
2490.000 331.1
2500.000 332.4
2510.000 333.8
2520.000 335.1
2530.000 336.5
2540.000 337.8
2550.000 339.2
2560.000 340.5
2570.000 341.9
2580.000 343.2
2590.000 344.6
2600.000 345.9
2610.000 347.3
2620.000 348.6
N02 PSI
2630.000 350.0
2640.000 351.4
2650.000 352.7
2660.000 354.1
2670.000 355.4
2680.000 356.8
2690.000 358.1
2700.000 359.5
2710.000 360.8
2720.000 362.2
2730.000 363.5
2740.000 364.9
2750.000 366.2
2760.000 367.6
2770.000 368.9
2780.000 370.3
2790.000 371.6
2800,000 373.0
2810.000 374.3
2820.000 375.7
2830.000 377.0
2840.000 378.4
2850.000 379.7
2860.000 381.1
2870.000 382.4
2880.000 383.8
2890.000 385.1
2900.000 386.5
2910.000 387.8
2920.000 389.2
2930.000 390.5
2940.000 391.9
2950.000 393.2
2960.000 394.6
2970.000 395.9
2980.000 397.3
2990.000 398.6
3000.000 400.0
3010.000 401.3
3020.000 402.7
3030.000 404.0
3040.000 405.3
3050.000 406.7
3060.000 408.0
3070.000 409.3
3080.000 410.7
3090.000 412.0
3100.000 413.3
3110.000 414.7
3120.000 416.0
N02 PSI
3130.000 417.3
3140.000 418.7
3150.000 420.0
3160.000 421.3
3170.000 422.7
3180.000 424.0
3190.000 425.3
3200.000 426.7
3210.000 428.0
3220.000 429.3
3230.000 430.7
3240.000 432.0
3250.000 433.3
3260.000 434.7
3270.000 436.0
3280.000 437.3
3290.000 438.7
3300.000 440.0
3310.000 441.3
3320.000 442.7
3330.000 444.0
3340.000 445.3
3350.000 446.7
3360.000 448.0
3370.000 449.3
3380.000 450.7
3390.000 452.0
3400.000 453.3
3410.000 454.7
3420.000 456.0
3430.000 457.3
3440.000 458.7
3450.000 460.0
3460.000 461.3
3470.000 462.7
3480.000 464.0
3490.000 465.3
3500.000 466.7
3510.000 468.0
3520.000 469.3
3530.000 470.7
3540.000 472.0
3550.000 473.3
3560.000 474.7
3570.000 476.0
3580.000 477.3
3590.000 478.7
3600.000 480.0
3610.000 481.3
3620.000 482.7
N02 PSI
3630.000 484.0
3640.000 485.3
3650.000 486.7
3660.000 488.0
3670.000 489.3
3680.000 490.7
3690.000 492.0
3700.000 493.3
3710.000 494.7
3720.000 496.0
3730.000 497.3
3740.000 498.7
3750.000 500.0
3760.000 501.3
3770.000 502.7
3780.000 504.0
3790.000 505.3
3800.000 506.7
3810.000 508.0
3820.000 509.3
3830.000 510.7
3840.000 512.0
3850.000 513.3
3860.000 514.7
3870.000 516.0
3880.000 517.3
3890.000 518.7
3900.000 520.0
3910.000 521.3
3920.000 522.7
3930.000 524.0
3940.000 525.3
3950.000 526.7
3960.000 528.0
3970.000 529.3
3980.000 530.7
3990.000 532.0
4000.000 533.3
4010.000 534.7
4020.000 536.0
4030.000 537.3
4040.000 538.7
4050.000 540.0
4060.000 541.3
4070.000 542.7
4080.000 544.0
4090.000 545.3
4100.000 546.7
4110.000 548.0
4120.000 549.3
-------
Table A-10
REFERENCE TABLE: PSI VALUES FOR NO2 (ppm) AT EQUALLY SPACED CONCENTRATIONS
N02 PSI
0.600 200.0
0.605 200.8
0.610 201.7
0.615 202.5
0.620 203.3
0.625 204.2
0.630 205.0
0.635 205.8
0.640 206.7
0.645 207.5
0.650 208.3
0.655 209.2
0.660 210.0
0.665 210.8
0.670 211.7
0.675 212.5
0.680 213.3
0.685 214.2
0.690 215.0
0.695 215.8
0.700 216.7
0.705 217.5
0.710 218.3
0.715 219.2
0.720 220.0
0.725 220.8
0.730 221.7
0.735 222.5
0.740 223.3
0.745 224.2
0.750 225.0
0.755 225.8
0.760 226.7
0.765 227.5
0.770 228.3
0.775 229.2
0.780 230.0
0.785 230.8
0.790 231.7
0.795 232.5
0.800 233.3
0.805 234.2
0.810 235.0
0.815 235.8
0.820 236.7
0.825 237.5
0.830 238.3
0.835 239.2
0.840 240.0
0.845 240.8
N02 PSI
0.850 241.7
0.855 242.5
0.860 243.3
0.865 244.2
0.870 245.0
0.875 245.8
0.880 246.7
0.885 247.5
0.890 248.3
0.895 249.2
0.900 250.0
0.905 250.8
0.910 251.7
0.915 252.5
0.920 253.3
0.925 254.2
0.930 255.0
0.935 255.8
0.940 256.7
0.945 257.5
0.950 258.3
0.955 259.2
0.960 260.0
0.965 260.8
0.970 261.7
0.975 262.5
0.980 263.3
0.985 264.2
0.990 265.0
0.995 265.8
1.000 266.7
1.005 267.5
1.010 268.3
1.015 269.2
1.020 270.0
1.025 270.8
1.030 271.7
1.035 272.5
1.040 273.3
1.045 274.2
1.050 275.0
1.055 275.8
1.060 276.7
1.065 277.5
1.070 278.3
1.075 279.2
1.080 280.0
1.085 280.8
1.090 281.7
1.095 282.5
N02 PSI
1.100 283.3
1.105 284.2
1.110 285.0
1.115 285.8
1.120 286.7
1.125 287.5
1.130 288.3
1.135 289.2
1.140 290.0
1.145 290.8
1.150 291.7
1.155 292.5
1.160 293.3
1.165 294.2
1.170 295.0
1.175 295.8
1.180 296.7
1.185 297.5
1.190 298.3
1.195 299.2
1.200 300.0
1.205 301.2
1.210 302.5
1.215 303.7
1.220 305.0
1.225 306.2
1.230 307.5
1.235 308.7
1.240 310.0
1.245 311.2
1.250 312.5
1.255 313.7
1.260 315.0
1.265 316.2
1.270 317.5
1.275 318.7
1.280 320.0
1.285 321.2
1.290 322.5
1.295 323.7
1.300 325.0
1.305 326.2
1.310 327.5
1.315 328.7
1.320 330.0
1.325 331.3
1.330 332.5
1.335 333.7
1.340 335.0
1.345 336.2
N02 PSI
1.350 337.5
1.355 338.7
1.360 340.0
1.365 341.2
1.370 342.5
1.375 343.7
1.380 345.0
1.385 346.2
1.390 347.5
1.395 348.7
1.400 350.0
1.405 351.2
1.410 352.5
1.415 353.7
1.420 355.0
1.425 356.2
1.430 357.5
1.435 358.7
1.440 360.0
1.445 361.2
1.450 362.5
1.455 363.7
1.460 365.0
1.465 366.2
1.470 367.5
1.475 368.7
1.480 370.0
1.485 371.2
1.490 372.5
1.495 373.7
1.500 375.0
1.505 376.2
1.510 377.5
1.515 378.7
1.520 380.0
1.525 381.2
1.530 382.5
1.535 383.7
1.540 385.0
1.545 386.2
1.550 387.5
1.555 388.7
1.560 390.0
1.565 391.2
1.570 392.5
1.575 393.7
1.580 395.0
1.585 396.2
1.590 397.5
1.595 398.7
N02 PSI
1.600 400.0
1.605 401.2
1.610 402.5
1.615 403.7
1.620 405.0
1.625 406.2
1.630 407.5
1.635 408.7
1.640 410.0
1.645 411.2
1.650 412.5
1.655 413.7
1.660 415.0
1.665 416.2
1.670 417.5
1.675 418.7
1.680 420.0
1.685 421.2
1.690 422.5
1.695 423.7
1.700 425.0
1.705 426.2
1.710 427.5
1.715 428.7
1.720 430.0
1.725 431.2
1.730 432.5
1.735 433.7
1.740 435.0
1.745 436.2
1.750 437.5
1.755 438.7
1.760 440.0
1.765 441.2
1.770 442.5
1.775 443.7
1.780 445.0
1.785 446.2
1.790 447.5
1.795 448.7
1.800 450.0
1.805 451.2
1.810 452.5
1.815 453.7
1.820 455.0
1.825 456.2
1.830 457.5
1.835 458.7
1.840 460.0
1.845 461.2
N02 PSI
1.850 462.5
1.855 463.7
1.860 465.0
1.865 466.2
1.870 467.5
1.875 468.7
1.880 470.0
1.885 471.2
1.890 472.5
1.895 473.7
1.900 475.0
1.905 476.2
1.910 477.5
1.915 478.7
1.920 480.0
1.925 481.2
1.930 482.5
1.935 483.7
1.940 485.0
1.945 486.2
1.950 487.5
1.955 488.7
1.960 490.0
1.965 491.2
1.970 492.5
1.975 493.7
1.980 495.0
1.985 496.2
1.990 497.5
1.995 498.7
2.000 500.0
2.005 501.2
2.010 502.5
2.015 503.7
2.020 505.0
2.025 506.2
2.030 507.5
2.035 508.7
2.040 510.0
2.045 511.2
2.050 512.5
2.055 513.7
2.060 515.0
2.065 516.2
2.070 517.5
2.075 518.7
2.080 520.0
2.085 521.2
2.090 522.5
2.095 523.7
50
-------
Table A-11
REFERENCE TABLE: PSI VALUES FOR SO2 (ppm) AT EQUALLY SPACED CONCENTRATIONS
S02 PSI
0.004 6.7
0.008 13.3
0.012 20.0
0.016 26.7
0.020 33.3
0.024 40.0
0.028 46.7
0.032 50.9
0.036 52.7
0.040 54.5
0.044 56.4
0.048 58.2
0.052 60.0
0.056 61.8
0.060 63.6
0.064 65.5
0.068 67.3
0.072 69.1
0.076 70.9
0.080 72.7
0.084 74.5
0.088 76.4
0.092 78.2
0.096 80.0
0.100 81.8
0.104 83.6
0.108 85.5
0.112 87.3
0.116 89.1
0.120 90.9
0.124 92.7
0.128 94.5
0.132 96.4
0.136 98.2
0.140 100.0
0.144 102.5
0.148 105.0
0.152 107.5
0.156 110.0
0.160 112.5
0.164 115.0
0.168 117.5
0.172 120.0
0.176 122.5
0.180 125.0
0.184 127.5
0.188 130.0
0.192 132.5
0.196 135.0
0.200 137.5
S02 PSI
0.204 140.0
0.208 142.5
0.212 145.0
0.216 147.5
0.220 150.0
0.224 152.5
0.228 155.0
0.232 157.5
0.236 160.0
0.240 162.5
0.244 165.0
0.248 167.5
0.252 170.0
0.256 172.5
0.260 175.0
0.264 177.5
0.268 180.0
0.272 182.5
0.276 185.0
0.280 187.5
0.284 190.0
0.288 192.5
0.292 195.0
0.296 197.5
0.300 200.0
0.304 201.3
0.308 202.7
0.312 204.0
0.316 205.3
0.320 206.7
0.324 208.0
0.328 209.3
0.332 210.7
0.336 212.0
0.340 213.3
0.344 214.7
0.348 216.0
0.352 217.3
0.356 218.7
0.360 220.0
0.364 221.3
0.368 222.7
0.372 224.0
0.376 225.3
0.380 226.7
0.384 228.0
0.388 229.3
0.392 230.7
0.396 232.0
0.400 233.3
S02 PSI
0.404 234.7
0.408 236.0
0.412 237.3
0.416 238.7
0.420 240.0
0.424 241.3
0.428 242.7
0.432 244.0
0.436 245.3
0.440 246.7
0.444 248.0
0.448 249.3
0.452 250.7
0.456 252.0
0.460 253.3
0.464 254.7
0.468 256.0
0.472 257.3
0.476 258.7
0.480 260 .'0
0.484 261.3
0.488 262.7
0.492 264.0
0.496 265.3
0.500 266.7
0.504 268.0
0.508 269.3
0.512 270.7
0.516 272.0
0.520 273.3
0.524 274.7
0.528 276.0
0.532 277.3
0.536 278.7
0.540 280.0
0.544 281.3
0.548 282.7
0.552 284.0
0.556 285.3
0.560 286.7
0.564 288.0
0.568 289.3
0.572 290.7
0.576 292.0
0.580 293.3
0.584 294.7
0.588 296.0
0.592 297.3
0.596 298.7
0.600 300.0
S02 PSI
0.604 302.0
0.608 304.0
0.612 306.0
0.616 308.0
0.620 310.0
0.624 312.0
0.628 314.0
0.632 316.0
0.636 318.0
0.640 320.0
0.644 322.0
0.648 324.0
0.652 326.0
0.656 328.0
0.660 330.0
0.664 332.0
0.668 334.0
0.672 336.0
0.676 338.0
0.680 340.0
0.684 342.0
0.688 344.0
0.692 346.0
0.696 348.0
0.700 350.0
0.704 352.0
0.708 354.0
0.712 356.0
0.716 358.0
0.720 360.0
0.724 362.0
0.728 364.0
0.732 366.0
0.736 368.0
0.740 370.0
0.744 372.0
0.748 374.0
0.752 376.0
0.756 378.0
0.760 380.0
0.764 382.0
0.768 384.0
0.772 386.0
0.776 388.0
0.780 390.0
0.784 392.0
0.788 394.0
0.792 396.0
0.796 398.0
0.800 400.0
S02 PSI
0.804 402.0
0.808 404.0
0.812 406.0
0.816 408.0
0.820 410.0
0.824 412.0
0.828 414.0
0.832 416.0
0.836 418.0
0.840 420.0
0.844 422.0
0.848 424.0
0.852 426.0
0.856 428.0
0.860 430.0
0.864 432.0
0.868 434.0
0.872 436.0
0.876 438.0
0.880 440.0
0.884 442.0
0.888 444.0
0.892 446.0
0.896 448.0
0.900 450.0
0.904 452.0
0.908 454.0
0.912 456.0
0.916 458.0
0.920 460.0
0.924 462.0
0.928 464.0
0.932 466.0
0.936 468.0
0.940 470.0
0.944 472.0
0.948 474.0
0.952 476.0
0.956 478.0
0.960 480.0
0.964 482.0
0.968 484.0
0.972 486.0
0.976 488.0
0.980 490.0
0.984 492.0
0.988 494.0
0.992 496. C
0.996 498.0
1.000 500.0
S02 PSI
1.004 502.0
1.008 504.0
1.012 506.0
1.016 508.0
1.020 510.0
1.024 512.0
1.028 514.0
1.032 516.0
1.036 518.0
1.040 520.0
1.044 522.0
1.048 524.0
1.052 526.0
1.056 528.0
1.060 530.0
1.064 532.0
1.068 534.0
1.072 536.0
1.076 538.0
1.080 540.0
1.084 542.0
1.088 544.0
1.092 546.0
1.096 548.0
1.100 550.0
1.104 552.0
1.108 554.0
1.112 556.0
1.116 558.0
1.120 560.0
1.124 562.0
1.128 564.0
1.132 566.0
1.136 568.0
1.140 570.0
1.144 572.0
1.148 574.0
1.152 576.0
1.156 578.0
1.160 580.0
1.164 582.0
1.168 584.0
1.172 586.0
1.176 588.0
1.180 590.0
1.184 592.0
1.188 594.0
1.192 596.0
1.196 598.0
1.200 600.0
51
-------
Table A-12
REFERENCE TABLE: PSI VALUES FOR SO2 (jug/m3) AT EQUALLY SPACED CONCENTRATIONS
S02 PSI
10.000 6.3
20.000 12.5
30.000 18.8
40.000 25.0
50.000 31.3
60.000 37.5
70.000 43.8
80.000 50.0
90.000 51.8
100.000 53.5
110.000 55.3
120.000 57.0
130.000 58.8
140.000 60.5
150.000 62.3
160.000 64.0
170.000 65.8
180.000 67.5
190.000 69.3
200.000 71.1
210.000 72.8
220.000 74.6
230.000 76.3
240.000 78.1
250.000 79.8
260.000 81.6
270.000 83.3
280.000 85.1
290.000 86.8
300.000 88.6
310.000 90.4
320.000 92.1
330.000 93.9
340.000 95.6
350.000 97.4
360.000 99.1
370.000 101.1
380.000 103.4
390.000 105.7
400.000 108.0
410.000 110.3
420.000 112.6
430.000 114.9
440.000 117.2
450.000 119.5
460.000 121.8
470.000 124.1
480.000 126.4
490.000 128.7
500.000 131.0
S02 PSI
510.000 133.3
520.000 135.6
530.000 137.9
540.000 140.2
550.000 142.5
560.000 144.8
570.000 147.1
580.000 149.4
590.000 151.7
600.000 154.0
610.000 156.3
620.000 158.6
630.000 160.9
640.000 163.2
650.000 165.5
660.000 167.8
670.000 170.1
680.000 172.4
690.000 174.7
700.000 177.0
710.000 179.3
720.000 181.6
730.000 183.9
740.000 186.2
750.000 188.5
760.000 190.8
770.000 193.1
780.000 195.4
790.000 197.7
800.000 200.0
810.000 201.3
820.000 202.5
830.000 203.8
840.000 205.0
850.000 206.3
860.000 207.5
870.000 208.8
880.000 210.0
890.000 211.3
900.000 212.5
910.000 213.8
920.000 215.0
930.000 216.3
940.000 217.5
950.000 218.8
960.000 220.0
970.000 221.3
980.000 222.5
990.000 223.8
1000.000 225.0
S02 PSI
1010.000 226.3
1020.000 227.5
1030.000 228.8
1040.000 230.0
1050.000 231.3
1060.000 232.5
1070.000 233.8
1080.000 235.0
1090.000 236.3
1100.000 237.5
1110.000 238.8
1120.000 240.0
1130.000 241.3
1140.000 242.5
1150.000 243.8
1160.000 245.0
1170.000 246.3
1180.000 247.5
1190.000 248.8
1200.000 250.0
1210.000 251.3
1220.000 252.5
1230.000 253.8
1240.000 255.0
1250.000 256.3
1260.000 257.5
1270.000 258.8
1280.000 260.0
1290.000 261.3
1300.000 262.5
1310.000 263.8
1320.000 265.0
1330.000 266.3
1340.000 267.5
1350.000 268.8
1360.000 270.0
1370.000 271.3
1380.000 272.5
1390.000 273.8
1400.000 275.0
1410.000 276.3
1420.000 277.5
1430.000 278.8
1440.000 280.0
1450.000 281.3
1460.000 282.5
1470.000 283.8
1480.000 285.0
1490.000 286.3
1500.000 287.5
S02 PSI
1510.000 288.8
1520.000 290.0
1530.000 291.3
1540.000 292.5
1550.000 293.8
1560.000 295.0
1570.000 296.3
1580.000 297.5
1590.000 298.8
1600.000 300.0
1610.000 302.0
1620.000 304.0
1630.000 306.0
1640.000 308.0
1650.000 310.0
1660.000 312.0
1670.000 314.0
1680.000 316.0
1690.000 318.0
1700.000 320.0
1710.000 322.0
1720.000 324.0
1730.000 326.0
1740.000 328.0
1750.000 330.0
1760.000 332.0
1770.000 334.0
1780.000 336.0
1790.000 338.0
1800.000 340.0
1810.000 342.0
1820.000 344.0
1830.000 346.0
1840.000 348.0
1850.000 350.0
1860.000 352.0
1870.000 354.0
1880.000 356.0
1890.000 358.0
1900.000 360.0
1910.000 362.0
1920.000 364.0
1930.000 366.0
1940.000 368.0
1950.000 370.0
1960.000 372.0
1970.000 374.0
1980.000 376.0
1990.000 378.0
2000.000 380.0
S02 PSI
2010.000 382.0
2020.000 384.0
2030.000 386.0
2040.000 388.0
2050.000 390.0
2060.000 392.0
2070.000 394.0
2080.000 396.0
2090.000 398.0
2100.000 400.0
2110.000 401.9
2120.000 403.8
2130.000 405.8
2140.000 407.7
2150.000 409.6
2160.000 411.5
2170.000 413.5
2180.000 415.4
2190.000 417.3
2200.000 419.2
2210.000 421.2
2220.000 423.1
2230.000 425.0
2240.000 426.9
2250.000 428.8
2260.000 430.8
2270.000 432.7
2280.000 434.6
2290.000 436.5
2300.000 438.5
2310.000 440.4
2320.000 442.3
2330.000 444.2
2340.000 446.2
2350.000 448.1
2360.000 450.0
2370.000 451.9
2380.000 453.8
2390.000 455.8
2400.000 457.7
2410.000 459.6
2420.000 461.5
2430.000 463.5
2440.000 465.4
2450.000 467.3
2460.000 469.2
2470.000 471.2
2480.000 473.1
2490.000 475.0
2500.000 476.9
S02 PSI
2510.000 478.8
2520.000 480.8
2530.000 482.7
2540.000 484.6
2550.000 486.5
2560.000 488.5
2570.000 490.4
2580.000 492.3
2590.000 494.2
2600.000 496.2
2610.000 498.1
2620.000 500.0
2630.000 501.9
2640.000 503.8
2650.000 505.8
2660.000 507.7
2670.000 509.6
2680.000 511.5
2690.000 513.5
2700.000 515.4
2710.000 517.3
2720.000 519.2
2730.000 521.2
2740.000 523.1
2750.000 525.0
2760.000 526.9
2770.000 528.8
2780.000 530.8
2790.000 532.7
2800.000 534.6
2810.000 536.5
2820.000 538.5
2830.000 540.4
2840.000 542.3
2850.000 544.2
2860.000 546.2
2870.000 548.1
2880.000 550.0
2890.000 551.9
2900.000 553.8
2910.000 555.8
2920.000 557.7
2930.000 559.6
2940.000 561.5
2950.000 563.5
2960.000 565.4
2970.000 567.3
2980.000 569.2
2990.000 571.2
3000.000 573.1
52
-------
Table A-13
REFERENCE TABLE: PSI VALUES FOR TSP Wm3) AT EQUALLY SPACED CONCENTRATIONS
TSP PSI
4.000 2.7
8.000 5.3
12.000 8.0
16.000 10.7
20.000 13.3
24.000 16.0
28.000 18.7
32.000 21.3
36-. 000 24.0
40.000 26.7
44.000 29.3
48.000 32.0
52.000 34.7
56.000 37.3
60.000 40.0
64.000 42.7
68.000 45.3
72.000 48.0
76.000 50.3
80.000 51.4
84.000 52.4
88.000 53.5
92.000 54.6
96.000 55.7
100.000 56.8
104.000 57.8
108.000 58.9
112.000 60.0
116.000 61.1
120.000 62.2
124.000 63.2
128.000 64.3
132.000 65.4
136.000 66.5
140.000 67.6
144.000 68.6
148.000 69.7
152.000 70.8
156.000 71.9
160.000 73.0
164.000 74.1
168.000 75.1
172.000 76.2
176.000 77.3
180.000 78.4
184.000 79.5
188.000 80.5
192.000 81.6
196.000 82.7
200.000 83.8
TSP PSI
204.000 84.9
208.000 85.9
212.000 87.0
216.000 88.1
220.000 89.2
224.000 90.3
228.000 91.4
232.000 92.4
236.000 93.5
240.000 94.6
244.000 95.7
248.000 96.8
252.000 97.8
256.000 98.9
260.000 100.0
264.000 103.5
268.000 107.0
272.000 110.4
276.000 113.9
280.000 117.4
284.000 120.9
288.000 124.3
292.000 127.8
296.000 131.3
300.000 134.8
304.000 138.3
308.000 141.7
312.000 145.2
316.000 148.7
320.000 152.2
324.000 155.7
328.000 159.1
332.000 162.6
336.000 166.1
340.000 169.6
344.000 173.0
348.000 176.5
352.000 180.0
356.000 183.5
360.000 187.0
364.000 190.4
368.000 193.9
372.000 197.4
376.000 200.4
380.000 202.0
384.000 203.6
388.000 205.2
392.000 206.8
396.000 208.4
400.000 210.0
TSP PSI
404.000 211.6
408.000 213.2
412.000 214.8
416.000 216.4
420.000 218.0
424.000 219.6
428.000 221.2
432.000 222.8
436.000 224.4
440.000 226.0
444.000 227.6
448.000 229.2
452.000 230.8
456.000 232.4
460.000 234.0
464.000 235.6
468.000 237.2
472.000 238.8
476.000 240.4
480.000 242.0
484.000 243.6
488.000 245.2
492.000 246.8
496.000 248.4
500.000 250.0
504.000 251.6
508.000 253.2
512.000 254.8
516.000 256.4
520.000 258.0
524.000 259.6
528.000 261.2
532.000 262.8
536.000 264.4
540.000 266.0
544.000 267.6
548.000 269.2
552.000 270.8
556.000 272.4
560.000 274.0
564.000 275.6
568.000 277.2
572.000 278.8
576.000 280.4
580.000 282.0
584.000 283.6
588.000 285.2
592.000 286.8
596.000 288.4
600.000 290.0
TSP PSI
604.000 291.6
608.000 293.2
612.000 294.8
616.000 296.4
620.000 298.0
624.000 299.6
628.000 301.2
632.000 302.8
636.000 304.4
640.000 306.0
644.000 307.6
648.000 309.2
652.000 310.8
656.000 312.4
660.000 314.0
664.000 315.6
668.000 317.2
672.000 318.8
676.000 320.4
680.000 322.0
684.000 323.6
688.000 325.2
692.000 326.8
696.000 328.4
700.000 330.0
704.000 331.6
708.000 333.2
712.000 334.8
716.000 336.4
720.000 338.0
724.000 339.6
728.000 341.2
732.000 342.8
736.000 344.4
740.000 346.0
744.000 347.6
748.000 349.2
752.000 350.8
756.000 352.4
760.000 354.0
764.000 355.6
768.000 357.2
772.000 358.8
776.000 360.4
780.000 362.0
784.000 363.6
788.000 365.2
792.000 366.8
796.000 368.4
800.000 370.0
TSP PSI
804.000 371.6
808.000 373.2
812.000 374.8
816.000 376.4
820.000 378.0
824.000 379.6
828.000 381.2
832.000 382.8
836.000 384,4
840.000 386.0
844.000 387.6
848.000 389.2
852.000 390.8
856.000 392.4
860.000 394.0
864.000 395.6
868.000 397.2
872.000 398.8
876.000 400.8
880.000 404.0
884.000 407.2
888.000 410.4
892.000 413.6
896.000 416.8
900.000 420.0
904.000 423.2
908.000 426.4
912.000 429.6
916.000 432.8
920.000 436.0
924.000 439.2
928.000 442.4
932.000 445.6
936.000 448.8
940.000 452.0
944.000 455.2
948.000 458.4
952.000 461.6
956.000 464.8
960.000 468.0
964.000 471.2
968.000 474.4
972.000 477,6
976.000 480.8
980.000 484.0
984.000 487.2
988.000 490.4
992.000 493.6
996.000 496.8
1000.000 500.0
TSP PSI
1004.000 503.2
1008.000 506.4
1012.000 509.6
1016.000 512.8
1020.000 516.0
1024.000 519.2
1028.000 522.4
1032.000 525.6
1036.000 528.8
1040.000 532.0
1044.000 535.2
1048.000 538.4
1052.000 541.6
1056.000 544.8
1060.000 548.0
1064.000 551.2
1068.000 554.4
1072.000 557.6
1076.000 560.8
1080.000 564.0
1084.000 567.2
1088.000 570.4
1092.000 573.6
1096.000 576.8
1100.000 580.0
1104.000 583.2
1108.000 586.4
1112.000 589.6
1116.000 592.8
1120.000 596.0
1124.000 599.2
1128.000 602.4
1132.000 605.6
1136.000 608.8
1140.000 612.0
1144.000 615.2
1148.000 618.4
1152.000 621.6
1156.000 624.8
1160.000 628.0
1164.000 631.2
1168.000 634.4
1172.000 637.6
1176.000 640.8
1180.000 644.0
1184.000 647.2
1188.000 650.4
1192.000 653.6
1196.000 656.8
1200.000 660.0
53
-------
Table A-14
REFERENCE TABLE: PSI VALUES FOR TSPxS02 (ppm-/ig/m3) AT EQUALLY SPACED CONCENTRATIONS
TSPXS02 PSI
25.000 200.2
26.000 201.6
27.000 202.9
28.000 204.3
29.000 205.6
30.000 206.9
31.000 208.3
32.000 209.6
33.000 210.9
34.000 212.3
35.000 213.6
36.000 214.9
37.000 216.3
38.000 217.6
39.000 219.0
40.000 220.3
41.000 221.6
42.000 223.0
43.000 224.3
44.000 225.6
45.000 227.0
46.000 228.3
47.000 229.7
48.000 231.0
49.000 232.3
50.000 233.7
51.000 235.0
52.000 236.3
53.000 237.7
54.000 239.0
55.000 240.4
56.000 241.7
57.000 243.0
58.000 244.4
59.000 245.7
60.000 247.0
61.000 248.4
62.000 249.7
63.000 251.0
64.000 252.4
65.000 253.7
66.000 255.1
67.000 256.4
68.000 257.7
69.000 259.1
70.000 260.4
71.000 261.7
72.000 263.1
73.000 264.4
74.000 265.8
TSPXS02 PSI
75.000 267.1
76.000 268.4
77.000 269.8
78.000 271.1
79.000 272.4
80.000 273.8
81.000 275.1
82.000 276.4
83.000 277.8
84.000 279.1
85.000 280.5
86.000 281.8
87.000 283.1
88.000 284.5
89.000 285.8
90.000 287.1
91.000 288.5
92.000 289.8
93.000 291.2
94.000 292.5
95.000 293.8
96.000 295.2
97.000 296.5
98.000 297.8
99.000 299.2
100.000 300.7
101.000 302.7
102.000 304.6
103.000 306.6
104.000 308.6
105.000 310.6
106.000 312.6
107.000 314.5
108.000 316.5
109.000 318.5
110.000 320.5
111.000 322.5
112.000 324.5
113.000 326.4
114.000 328.4
115.000 330.4
116.000 332.4
117.000 334.4
118.000 336.3
119.000 338.3
120.000 340.3
121.000 342.3
122.000 344.3
123.000 346.3
124.000 348,2
TSPXS02 PSI
125.000 350.2
126.000 352.2
127.000 354.2
128.000 356.2
129.000 358.2
130.000 360.1
131.000 362.1
132.000 364.1
133.000 366.1
134.000 368.1
135.000 370.0
136.000 372.0
137.000 374.0
138.000 376.0
139.000 378.0
140.000 380.0
141.000 381.9
142.000 383.9
143.000 385.9
144.000 387.9
145.000 389.9
146.000 391.8
147.000 393.8
148.000 395.8
149.000 397.8
150.000 399.8
151.000 402.4
152.000 405.1
153.000 407.8
154.000 410.5
155.000 413.2
156.000 415.9
157.000 418.7
158.000 421.4
159.000 424.1
160.000 426.8
161.000 429.5
162.000 432.2
163.000 434.9
164.000 437.6
165.000 440.3
166.000 443.0
167.000 445.7
168.000 448.4
169.000 451.1
170.000 453.8
171.000 456.5
172.000 459.2
173.000 461.9
174.000 464.6
TSPXS02 PSI
175.000 467.3
176.000 470.0
177.000 472.7
178.000 475.4
179.000 478.1
180.000 480.8
181.000 483.5
182.000 486.2
183.000 488.9
184.000 491.6
185.000 494.3
186.000 497.0
187.000 499,7
188.000 502.4
189.000 505.1
190.000 507.8
191.000 510.6
192.000 513.3
193.000 516.0
194.000 518.7
195.000 521.4
196.000 524.1
197.000 526.8
198.000 529.5
199.000 532.2
200.000 534.9
201.000 537.6
202.000 540.3
203.000 543.0
204.000 545.7
205.000 548.4
206.000 551.1
207.000 553.8
208.000 556.5
209.000 559.2
210.000 561.9
211.000 564.6
212.000 567.3
213.000 570.0
214.000 572.7
215.000 575.4
216.000 578.1
217.000 580.8
218.000 583.5
219.000 586.2
220.000 588.9
221.000 591.6
222.000 594.3
223.000 597.0
224.000 599.8
TSPXS02 PSI
225.000 602.5
226.000 605.2
227.000 607.9
228.000 610.6
229.000 613.3
230.000 616.0
231.000 618.7
232.000 621.4
233.000 624.1
234.000 626.8
235.000 629.5
236.000 632.2
237.000 634.9
238.000 637.6
239.000 640.3
240.000 643.0
241.000 645.7
242.000 648.4
243.000 651.1
244.000 653.8
245.000 656.5
246.000 659.2
247.000 661.9
248.000 664.6
249.000 667.3
250.000 670.0
251.000 672.7
252.000 675.4
253.000 678.1
254.000 680.8
255.000 683.5
256.000 686.2
257.000 689.0
258.000 691.7
259.000 694.4
260.000 697.1
261.000 699.8
262.000 702.5
263.000 705.2
264.000 707.9
265.000 710.6
266.000 713.3
267.000 716.0
268.000 718.7
269.000 721.4
270.000 724.1
271.000 726.8
272.000 729.5
273.000 732.2
274.000 734.9
TSPXS02 PSI
275.000 737.6
276.000 740.3
277.000 743.0
278.000 745.7
279.000 748.4
280.000 751.1
281.000 753.8
282.000 756.5
283.000 759.2
284.000 761.9
285.000 764.6
286.000 767.3
287.000 770.0
288.000 772.7
289.000 775.4
290.000 778.1
291.000 780.9
292.000 783.6
293.000 786.3
294.000 789.0
295.000 791.7
296.000 794.4
297.000 797.1
298.000 799.8
299.000 802.5
300.000 805.2
301.000 807.9
302.000 810.6
303.000 813.3
304.000 816.0
305.000 818.7
306.000 821.4
307.000 824.1
308.000 826.8
309.000 829.5
310.000 832.2
311.000 834.9
312.000 837.6
313.000 840.3
314.000 843.0
315.000 845.7
316.000 848.4
317.000 851.1
318.000 853.8
319.000 856.5
320.000 859.2
321.000 861.9
322.000 864.6
323.000 867.3
324.000 870.1
54
-------
Table A-15
REFERENCE TABLE: PSI VALUES FOR TSP x SO2 l/jg/m3)2 AT EQUALLY SPACED CONCENTRATIONS*
TSPXS02 PSI
64.000 0.0
66.000 200.5
68.000 201.5
70.000 202.6
72.000 203.6
74.000 204.6
76.000 205.6
78.000 206.6
80.000 207.7
82.000 208.7
84.000 209.7
86.000 210.7
88,000 211.7
90.000 212.8
92.000 213.8
94.000 214.8
96.000 215.8
98.000 216.8
100.000 217.9
102.000 218.9
104.000 219.9
106.000 220.9
108.000 221.9
110.000 223.0
112.000 224.0
114.000 225.0
116.000 226.0
118.000 227.0
120.000 228.1
122.000 229.1
124.000 230.1
126.000 231.1
128.000 232.1
130.000 233.2
132.000 234.2
134.000 235.2
136.000 236.2
138.000 237.2
140.000 238.3
142.000 239.3
144.000 240.3
146.000 241.3
148.000 242.3
150.000 243.4
152.000 244.4
154.000 245.4
156.000 246.4
158.000 247.4
160.000 248.5
162.000 249.5
TSPXS02 PSI
164.000 250.5
166.000 251.5
168.000 252.6
170.000 253.6
172.000 254.6
174.000 255.6
176.000 256.6
178.000 257,7
180.000 258.7
182.000 259.7
184.000 260.7
186.000 261.7
188.000 262.8
190.000 263.8
192.000 264.8
194.000 265.8
196.000 266.8
198.000 267.9
200.000 268.9
202.000 269.9
204.000 270.9
206.000 271.9
208.000 273.0
210.000 274.0
212.000 275.0
214.000 276.0
216.000 277.0
218.000 278.1
220.000 279.1
222.000 280.1
224.000 281.1
226.000 282.1
228.000 283.2
230.000 284.2
232.000 285.2
234.000 286.2
236.000 287.2
238.000 288.3
240.000 289.3
242.000 290.3
244.000 291.3
246.000 292.3
248.000 293.4
250.000 294.4
252.000 295.4
254.000 296.4
256.000 297.4
258.000 298.5
260.000 299.5
262.000 300.8
TSPXS02 PSI
264.000 302.3
266.000 303.8
268.000 305.3
270.000 306.8
272.000 308.3
274.000 309.8
276.000 311.4
278.000 312.9
280.000 314.4
282.000 315.9
284.000 317.4
286.000 318.9
288.000 320.5
290.000 322.0
292.000 323.5
294.000 325.0
296.000 326.5
298.000 328.0
300.000 329.5
302.000 331.1
304.000 332.6
306.000 334.1
308.000 335.6
310.000 337.1
312.000 338.6
314.000 340.2
316.000 341.7
318.000 343.2
320.000 344.7
322.000 346.2
324.000 347.7
326.000 349.2
328.000 350.8
330.000 352.3
332.000 353.8
334.000 355.3
336.000 356.8
338.000 358.3
340.000 359.8
342.000 361.4
344.000 362.9
346.000 364.4
348.000 365.9
350.000 367.4
352.000 368.9
354.000 370.5
356.000 372.0
358.000 373.5
360.000 375.0
362.000 376.5
TSPXS02 PSI
364.000 378.0
366.000 379.5
368.000 381.1
370.000 382.6
372.000 384.1
374.000 385.6
376.000 387.1
378.000 388.6
380.000 390.2
382.000 391.7
384.000 393.2
386.000 394.7
388.000 396.2
390.000 397.7
392.000 399.2
394.000 401.0
396.000 403.1
398.000 405.2
400.000 407.2
402.000 409.3
404.000 411.3
406.000 413.4
408.000 415.5
410.000 417.5
412.000 419.6
414.000 421.6
416.000 423.7
418.000 425.8
420.000 427.8
422.000 429.9
424.000 432.0
426.000 434.0
428.000 436.1
430.000 438.1
432.000 440.2
434.000 442.3
436,000 444.3
438.000 446.4
440.000 448.5
442.000 450.5
444.000 452.6
446.000 454.6
448.000 456.7
450.000 458.8
452.000 460.8
454.000 462.9
456.000 464.9
458.000 467.0
460.000 469.1
462.000 471.1
TSPXS02 PSI
464.000 473.2
466.000 475.3
468.000 477.3
470.000 479.4
472.000 481.4
474.000 483.5
476.000 485.6
478.000 487.6
480.000 489.7
482.000 491.8
484.000 493.8
486.000 495.9
488.000 497.9
490.000 500.0
492.000 502.1
494.000 504.1
496.000 506.2
498.000 508.2
500.000 510.3
502.000 512.4
504.000 514.4
506.000 516.5
508.000 518.6
510.000 520.6
512.000 522.7
514.000 524.7
516.000 526.8
518.000 528.9
520.000 530.9
522.000 533.0
524.000 535.1
526.000 537.1
528.000 539.2
530.000 541.2
532.000 543.3
534.000 545.4
536.000 547.4
538.000 549.5
540.000 551.5
542.000 553.6
544.000 555.7
546.000 557.7
548.000 559.8
550.000 561.9
552.000 563.9
554.000 566.0
556.000 568.0
558.000 570.1
550.000 572.2
562.000 574.2
TSPXS02 PSI
564.000 576.3
566.000 578.4
568.000 580.4
570.000 582.5
572.000 584.5
574.000 586.6
576.000 588.7
578.000 590. 7
580.000 592.8
582.000 594.8
584.000 596.9
586.000 599.0
588.000 601.0
590.000 603.1
592.000 605.2
594.000 607.2
596.000 609.3
598.000 611.3
600.000 613.4
602.000 615.5
604.000 617.5
606.000 619.6
608.000 621.6
610.000 623.7
612.000 625.8
614.000 627.8
616.000 629.9
618.000 632.0
620.000 634.0
622.000 636.1
624.000 638.1
626.000 640.2
628.000 642.3
630.000 644.3
632.000 646.4
634.000 648.5
636.000 650.5
638.000 652.6
640.000 654.6
642.000 656.7
644.000 658.8
646.000 660.8
648.000 662.9
650.000 664.9
652.000 667.0
654.000 669.1
656.000 671.1
658.000 673.2
660.000 675.3
662.000 677.3
'Expressed in 1000's.
55
-------
APPENDIX B
COMPUTER PROGRAMS FOR CALCULATING THE
POLLUTANT STANDARDS INDEX (PSI) TABLES
56
-------
B1. Program for Producing "Rapid Survey" and "Working" Tables (Tables A-1,
A-2, A-3, A-4, or desired variations) for Rapid Calculation of PSI.
C THIS PROGRAM PRODUCES A TABLE Of- POLLUTANT
C CONCENTRATIONS CORRESPONDING TO ANY DESIRED
C . . . . VALUES AND INCREMENTS OF THE POLLUTANT
C STANDARDS INDEX (PSI). CHANGING A SINGLE
C . . . . STATEMENT ALLOWS INTEGER OR HALF-INTEGER
C . . . . VALUES OF PSlt IN INCREMENTS OF ONE, FIVE,
C .... OR TEN UNITS, TO BE CHOSEN FUR DISPLAY.
IMPLICIT REAL*8(A-h,U-Z)
WRITE (6,200)
200 FORMAT UHl»20x*
* 'TABLE FOK SAPID CALCULATION OF POLLUTANT STANDARDS INDEX*f,
+ 1X,*PSI = 1-200'/)
WRITE (6,2001)
2001 FORMAT (*0,22X,'UNITS IN MICROGRAMS/CUB1C METERf,
* 12X, «UNITS IN PARTS PER MILLION*)
WRITE (6,201)
201 FORMAT (1H0.5X ,«PSl ,9 7X , »pSI )
WRITE (6,202)
202 FORMAT (1H ,2X , (NEARE ST * ,2X , 'FSlf ,8X,«CO , 7x,' 03» ,fcX,' SU2 ,
* 7X,'TSP»,13X, CO«,6X,»Q3»,7X,»S02», 7X,
+ »PSI«,2X, '(NEAREST*)
WRITE (6,203)
203 FORMAT (1H ,<*X,«UN1 T ) , 9X,2X , ' (MG/M3 ) ,77* , 'UN IT) /)
C . . . . SELECT NUMBER OF LINES IN TABLE
D0*10*i«l*,20l
REALI - DFLUATU )
C . . . . SELECT STARTING VALUE AND INCREMENTS FOR PSI
PSI - l.*REALl-0.5
IF (PSI.G1.&0.) GO TO 5Q
CONTINUE
S02 « 80.*PS1/50.
S02PPM s 0.03*PS1/50.
TSP = 75.*PSI/50.
CO * PSI/10.
COPPM * 9.*PSI/100.
03 * 160.*PSI/100.
03PPM * 0.06*PSI/100.
GO TO 5000
50 CONTINUE
57
-------
IF (PSI.GT.100.) GO TO 60
802 * 2d5,*(PSI-50.)/50, + 80.
S02PPM s ,n*(PSI"50.)/SO. t 0.03
TSP 9 185,*(PSI-50.)/50. + 75,
CO s PSI/10,
COPPM s 9,*PSI/100,
03 s 240,*PST/100.
OJPPM * 0,12*PSI/100,
GO TO 5000
60 CONTINUE
IF (PSI.GT.aOQ.) GO TO 70
S02 = 435,*(PSI-100.)/10Q. + 365,
S02PPM s Q,16*(PSI-100.)/100, + 0,14
TSP * U5.*(PSI-tOO,)/lOO. * 260.
CO » 7,*PSI/100, * 3.
COPPM a 6.*(PSI-100.)/1QO. + 9,
03 a 160.*(P5I-100,)/100. * 240.
03PPM « 0.08*(PSI-100.)/100. + 0,i2
GO TO 5000
70 CONTINUE
IF (PSI.&T.300.) GO TO 80
S02 * 800.*(PSI-200.)/100. + 80C.
S02PPM * 0.30 * (PSI-200.)/100. + 0.30
TSP = 500.*(PSI-200.)/200. * 375.
CO - 17.*{PSl-200.)/IOO. + 17.
COPPM * 15.*(PSI-2GO.}/100. + 15.
03 » 400.*{PSI-2QQ.)/100. + ^.00.
03PPM » .2*(PSI-200.)/100. + .2
N02 « 1130.*(PSI-2CO.)/100. + 1130.
N02PPM - 0.6*{PSI-200.)/10C. *0.6
TS = 19&.*(PSr-20G.)/lQG. + 65.
TSPPM - 74.fc<»*{PSI-200.)/100. + 2^.82
GO TO 5000
80 CONTINUE
IF (PSI.GT.403) GO TO 90
S02 » 500.*(pSI-300.)/100. + 1600.
S02PPM * 0.2*(PS1-300.)/100. * .6
TSP « 50Q.*(PS1-200.)/200. + 375.
CO « 12.*(PSI-300.)/10a. * 34.
COPPM* 10.*
-------
S02 = 520.*(PSI-400.)/100. + 2100.
S02PPM - 0.2*(PSI-300.)/10C. + .6
TSP » 125.*(PSI-40Q.)/1CO. + 875.
CO * 11.5*(PSl-400.)/100. * 46.
COPPM* lo.*(PSl-300.)/100. * 30.
03 * 20C.*(HSl-30Q.)/100. + 800.
03PPM - . 1*(PSI-300.)/100. + .<»
N02 * 75o.*(PSl-^»00.)/100. + 3000.
N02PPM * .<»*(PSI-3QO.)/100. » 1.2
TS = 97.*(PSI - ^»00.)/100. * 393.
TSPPM » 37. *(PSI-^00. 1/100. + 1&0.1
5000 CONT 1NUE
c . . . . SELECT 'SPACING AND NUHBER OF LINES PER PAGL
J « i
IF (K/5*5.Nt.K) GO TO 6^70
IF (K.EQ.O) GO TO 6470
6450 WRITE (6,650)
650 FORMAT (lH )
IF(K/40*<»O.NE.K> GO TO 647C
WRITE (6,640)
640 FORMAT (1H1)
WRITE (6,2001)
WRITE(6,201)
WRITE (6,202)
WRITE (6,203)
6470 CONTINUE
WRITE (6,302)J, PSI ,CO,03, S02, TSP, COPPM,03PPM,S02PPM,PSI , J
302 FORMAT {1H ,5X ,I3,2X, F6 .1 ,4F 10.2, 6X» 3F 10.4,3X ,Fe-l ,4X, 13 )
10 CONTINUE
END
59
-------
B2. Program for Producing "Reference" Tables of PSI Values for Individual
Pollutants (Tables A-5 through A-15, or desired variations).
c ........ THIS PROGRAM PRODUCES A TABLE OF PSI
C ........ VALUES CORRESPONDING TO ANY DESIRED
C ......... POLLUTANT CONCENTRATIONS AND INCREMENTS.
C ......... ELEVEN SUBROUTINES COVER ALL POLLUTANTS
C ......... AND POSSIBLE COMBINATIONS OF UNITS.
IMPLICIT REAL*8(A-H,0-Z), INTEGER (1-N)
C . . . . SELECT SIZE DF TABLE: (# OF LINES, H OF COLUMNS)
DIMENSION SINDEX (so, 12)
DO 60 M*l ,11
IF (M.EO.l) WRITE (6,101 )
101 FORMAT (HI, 55X,'CO(UG/M3)»//' ,1X ,6(3X, 'CO' ,6*, 'PSI ' , 5X ) )
IF(H.EQ.Z) WRITE (6,102)
102 FORMAT (1H1 ,55X, »CO ( PPM) //* ,1X,6( 3X, 'CO' ,6X, »PSI f ,5X } )
IF (M.E0.3) WRITE (6,1003)
1003 FORMAT ( 1H1 ,&5X , D3(UG/M3) // ,1X,6(3X, »U3' ,6X, 'PSI f ,5X) )
IF (M.EQ.4) WRITE (6,104)
1 04 FORMAT (!Hl,b5X,'03(PPM) '//' ' » IX, 6 (3X, '03* ,6X, 'PSI ,5X ) )
IF (M.E0.5) WRITE (6,105)
105 FORMAT (1H1 ,55X , 'N02 (UG/M3) '//' ' ,1X ,6(3X, f N02' ,5X , *PS1 « ,i>X ) )
IF (M.EQ.6) WRITE <6,1D6)
106 FORMAT (HI ,55X , «N02 (PPM ) //' " ,1X, 6 (3X, "NU2 ,5X , »PSI ' , 5X ) )
IF (M.E0.7) WRITE (6,107)
107 FORMAT (1H1,55X, «S02( UG/M3 ) ' //' ', 1X,6(3X, * S02 * ,5X , 'PSI ,5X )
IF (M.EQ.6) WRITE (6,138)
108 FORMATdHI ,55X,'S02(PPM) V/' », 1X,6 (3X, »S02 ,5X, »PS1 ,5X ) )
IF (M.E0.9) WRITE (6,109)
109 FORMAT ( HI , 55X , »TSP (UG/M3) ' // ' ' ,1X ,6(3X, TSP* ,5X , »PS1 ,i>X) )
IF (M.E0.1D) rfRlTE (6,110)
110 FORMAT (lr(l,^2X, 'T SPX S02(UG/M3) (UG/M3) ( IN THOUSANDS)')
IF (M.E0.10) ^klTE (6,1110)
1110 FORMAT (I0I,1X,6(*TSPXS02» ,
-------
IF
F
F
F
F
F
F
F
F
(M,
(M,
(M,
(M,
(M,
(M,
(M,
(M,
(M,
CO(REALI,T,SUBCO,PSI )
COPPM(lvEALl ,T,SUBCO,PS1 )
03(REALI»T,SUB03,PSI)
03PPM(KEALI,T»SUB03,PS1)
N02(REALI ,T,SUBN02,PSI)
N02PPM(kEALl,T,SUBN02,PSl)
S02(R£AL1 ,T,SUBS02,PSI)
S02PPM(RtALI,T,SUBS02,PSI)
TSPtREALI ,T,SUBTSP,PSI )
TS(REALI,T, S.PS1)
TSPPM{RtALI,T,S,PSI)
T * 0.0
PSl » 0.0
DO 10 I = 1,300
= DFLOAT(I
EQ.l) CALL
EQ.2) CALL
EQ.3) CALL
EQ.4) CALL
EQ.5) CALL
EQ.6) CALL
EQ.7) CALL
EQ.fc) CALL
LQ.9) CALL
F(M.EC.IO) CALL
F (M.EQ.ll)CALL
J « J + I
S INDEX (J,K) * T
SINDEX (J,L) = PSl
IF (J.EQ.bO) < * K+2
IF (J.EQ.50) J = 0
10 CONTINUE
DO 25 N = l ,10
DO 20 JDNE =1,5
J = 5 *(N-1) * JONE
WRITE (6,1002) (SINDEXt J,K),K«1.12>
1002 FORMAT (IX, 6 (FB.3 ,2X ,F 6.1 ,3X ) )
20 CONTINUE
WRITE (5,103)
25 CONTINUE
60 CONTINUE
END
SUBROUTINE CO(REAL1,T,SUBCO,PSI)
T = 0.2*REALI
IF(T
JF(T
1F(T
IF(T
IF(T
pSl * SyBCQ
RETURN
END
SUBRoUTINE COPPM(REALI,T,SUBCG.PSI)
T = 0-2*REALI
IF( T.GE.O.O.AND.T.LT .9.0)
lF(T.Gt.9.o.AND.T.LT.15.0)
IF(T.GE.15.0.AND. T.LT.30.0)
1F(T.GE.30.0)
PSl = SUBCO
RETURN
END
.GE.O.O.AND.T.LT .10.0)
,GE.10.0.AND.T
,GE.17.0.AND.T
.GE.34.0.AND.T
.GE.46.0)
.LT.
.LT.
.LT.
17.
34,
46.
0)
0)
0)
sueco«io.o*T
sUBCO*14.28S>71
-------
SUBROUTINE 03(R£ALI,T,SUB03,PSI)
T * + 200.0
2*(T-1600.0) + 300.0
19230S*(T-2100.0) 4
IF( T.
1F(T.
IF( T.
IF(T.
GE.
GE.
GL.
GE.
SUBS02=1666.66667*T
SUBS02=454.545456*(1-0.03) * 50.0
SUbS02=625.0*(T-0.14) + 100.
0.3.AND.1.LT .0.6)
IF(T.GE.0.6)
SU8S02=333.333333*(T-0.3) + 200.0
SUB$02*500.0*(T-0.6) * 300.0
62
-------
PSI = SUBS02
RETURN
END
SUBROUTINE ISP(REALI,T,SUBTSP,PS1)
T = 4.*REALI
,GE.0.0.AND.T.LT.75.0)
Gt.75.0.AND.T.LT.260.0)
,GE.260.0.AND.T.LT.375.0)
,GE.375.0.AND.T.LT.875.0)
O.AND.T
o)
(REAL1,
*RLAL I
65000.0.AND.
261000.0.AND
IF(T
1F(T
IF(T
IF(T
IF(T.GE.875
pSI = SjBTSP
RETURN
END
SUBROUTINE TS
T = 62000. * 2000
61 IFU.GE
IFU.GE
IF{T.GE.393000.0)
PSI * S
T = T/lOOO.
RETURN
END
SUBROUTINE TSPPM
T * 24.0 *1.0*REAL1
62 1F(T.GE.24.82
IF(T.OE.99.66
IF(T.GE.15G.l
PS] = S
RETURN
END
SUB TSP=. 666666667*1
SUbTSP = G.27C27027*(T-75.) + t
SUbTSP=.B695652l7*(l-260.0)
SUBTSP=0.^*(T-375.0) + 200.0
SUetSP=G.6*(T-B75.C) + ^00. 0
ICO-
T,S,PS1)
T.LT.261300.0) S«.00051020«»*( T-65000.0 ) + 20u.
.T.LT.393000.0) S=.000757576*(T-261000.0)+300.
S=0.001C309278*(T-393000.0) +
(REAL!, T,S,PsI)
.AND.T.LT.99.66
.AND.T.LT.150.1
) 5=1.337
) 5=1.962
S=2.703
*(T-2«..b2) + 2C c
*(T-99.66 ) +
63
-------
TECHNICAL REPORT DATA
(Please read Instructions on the reverse before completing)
1. REPORT NO.
EPA-600/4-79-039
3. RECIPIENT'S ACCESSION-NO.
4. TITLE AND SUBTITLE
RAPID TECHNIQUES FOR CALCULATING THE POLLUTANT
STANDARDS INDEX (PSI)
REVISED JUNE 1979
5. REPORT DATE
June 1979
6. PERFORMING ORGANIZATION CODE
ORD/OMTS/MTD (RD-680)
7. AUTHOR(S)
Lance Wallace and Wayne R. Ott
8. PERFORMING ORGANIZATION REPORT NO.
9. PERFORMING ORGANIZATION NAME AND ADDRESS
10. PROGRAM ELEMENT NO.
1HD621
N/A
11. CONTRACT/GRANT NO.
N/A
12. SPONSORING AGENCY NAME AND ADDRESS
Office of Research and Development
U.S. Environmental Protection Agency
401 M Street, S.W.
Washington, D.C. 20A60
13. TYPE OF REPORT AND PERIOD COVERED
In-house
14. SPONSORING AGENCY CODE
EPA/600/19
15. SUPPLEMENTARY NOTES
N/A
16. ABSTRACT
Rapid techniques for calculating the Pollutant Standards Index (PSI) for daily
public reporting of air quality are discussed. A complete set of original nomograms
for calculating the PSI in gravimetric or volumetric units is presented. The
nomograms are recommended for use by all State and local air pollution control
agencies as a means of determining the PSI rapidly and accurately. Examples of
linear and logarithmic graphs for calculating the PSI are also included.
Tables for rapidly identifying the critical pollutant on a given day and
automatically determining its PSI value to the nearest unit are listed in Appendix A.
Tables A-2 and A-4 list the precise pollutant concentrations corresponding to
consecutive unit values of PSI between 1 and 500, and can, therefore, provide the
definitive verification of estimates of PSI obtained from the nomograms or other
graphs. Computer programs for creating these or similar tables appear in Appendix B.
This revised edition includes all the changes in tables and nomograms required
by the 1979 revision of the National Ambient Air Quality Standard for ozone.
17.
KEY WORDS AND DOCUMENT ANALYSIS
DESCRIPTORS
b.IDENTIFIERS/OPEN ENDED TERMS C. COSATI Field/Group
Mathematical models, -Computer simulation,
Systems analysis, Statistical analysis,
Pollution - Air pollution, Sanitary
engineering, Environmental engineering,
Civil engineering
Environmental indices
Air quality indices,
Data analysis, Computer
techniques, Environmen-
tal monitoring
04B
05C
06F
12A
12B
13B
IS. DISTRIBUTION STATEMENT
RELEASE TO PUBLIC
19. SECURITY CLASS (ThixReport)
UNCLASSIFIED
21. NO. OF PAGES
64
20. SECURITY CLASS (Thispage)
UNCLASSIFIED
22. PRICE
EPA Form 2220-1 (9-73)
64
4U.S. GOVERNMENT PRINTING OFFICE: 1980 311-132/11 1-3
------- |