United States
Environmental Protection
Agency
Environmental Sciences
Research Laboratory
Research Triangle Park NC 27711
Research and Development
EPA-600/S3-84-079  Aug. 1984
Project  Summary
An  Evaluation  of Alternative
Gaussian  Plume  Dispersion
Modeling Techniques  in
Estimating  Short-Term Sulfur
Dioxide  Concentrations
Thomas E. Pierce
  A  routinely  applied  atmospheric
dispersion  model was  modified  to
evaluate alternative modeling tech-
niques  that allow for  more detailed
source  data,  onsite meteorological
data, and several dispersion methodol-
ogies. These techniques were evaluated
using hourly measured SO2 concentra-
tions at fixed receptors around coal-
fired power  plants  near  Paradise,
Kentucky,  during  1976,  and near
Johnsonville, Tennessee, during 1977.
A significant finding of the evaluation
was that the more sophisticated models
did  not appreciably outperform the
routinely applied models. The models
using   airport  meteorological  data
performed as well as the models using
onsite wind data. With the Pasquill-
Gifford and Briggs dispersion schemes,
small differences in model performance
were observed. More substantial differ-
ences occurred  with  models using
onsite turbulence measurements. The
model using Pasquill's recommenda-
tions  tended to  overpredict  peak
concentrations. The models based  on
Draxler's  and  Cramer's approaches
using onsite turbulence yielded mixed
results, perhaps  in part because the
lateral  standard deviation  of  wind
direction available was the 1 -h average
of 5-min values (rather than a 1 -h value),
thus  eliminating the  longer  period
fluctuations that are  important  in
estimating 1-h concentrations  in
addition  to  the shorter  period
fluctuations.  Additional research is
recommended  to  improve  the
application  of onsite turbulence
measurements  and to provide more
accurate estimates of plume trajector-
ies for input to atmospheric dispersion
models.
  This Project Summary was developed
by EPA 's Environmental Sciences Re-
search Laboratory, Research Triangle
Park, NC. to announce key findings of
the research project that is fully docu-
mented in a separate report of the same
title (see Project Report ordering in-
formation at back).
Introduction
  The  EPA routinely  uses Gaussian
plume models to make decisions having
important environmental and economic
impacts on air quality. Despite  the
economic and environmental importance
placed on air quality modeling, the predic-
tions from dispersion models are often no
better than within a factor of two of the
observations. Recognizing the limitations
of these models, the EPA and the Ameri-
can Meteorological Society (AMS) have
initiated steps  to  improve  current
modeling  practices.  The general
consensus is that more validations of air
quality simulation models are needed to
improve existing models and to guide the
development of future models.

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  In the current study, a Gaussian plume
dispersion model incorporating alterna-
tive techniques was evaluated using a
comprehensive data base developed for
two  Tennessee  Valley Authority coal-
fired  power  plants:  Johnsonville and
Paradise.  Alternative  modeling  tech-
niques  were  included in  a  routinely
applied  Gaussian dispersion model,  in-
cluding  different approaches for emis-
sions, meteorology, and dispersion.
  The benchmark model from which the
alternatives  were  developed  was  the
MPTER  algorithm.   Multiple  Point
Gaussian  Dispersion  Algorithm  with
Optional Terrain  Adjustment,  an  air
quality simulation model that is used by
EPA  in  regulatory  applications.  The
MPTER  was  especially suited for this
study because  actual coordinates for
each monitoring site could  be specified,
along  with  the  physical  separation
between  stacks.  Furthermore,  the
author's  in-depth experience  with
MPTER allowed for careful and expedient
inclusion of the alternative  models.

Modeling  Alternatives Used
  In modeling for regulatory applications,
the design  capacity  or  the  maximum
operating  capacity  of  resulting  SO2
emissions and source parameters are
often required as model inputs. The daily
and   seasonal  operating  rates  vary
significantly at  most  coal-fired power
plants. Furthermore,  maximum surface
concentrations at a power plant can occu r
under  less  than  full-load conditions.
Thus, for the Johnsonville and Paradise
locations,  hourly S02 emissions, stack
gas temperatures, and gas exit velocities
were computed for comparison to full-
load conditions.
  The meteorological data  required  for
EPA regulatory applications are often
selected from the National  Weather
Service (NWS) stations  that  are  most
representative of the site being modeled.
In  this study,  the airport data  from
Nashville, Tennessee (BNA) were used as
model  inputs  for  the  Paradise  and
Johnsonville sites.  Evansville,  Indiana
(EW) surface data were also included for
comparison at the Paradise site. Because
the use of onsite meteorological data is
preferred, the hourly average 110-m
onsite wind data were used at both power
plants.
  An accurate estimate of  dispersion is
critical  in air quality analysis.  In  this
regard,   much  effort  was   made   in
developing the alternative models in this
study. The MPTER uses Pasquill-Gifford
(PG)  dispersion  coefficients.  As  one
alternative,   Pasquill's   approach  for
estimating buoyancy-induced dispersion
(BID) was evaluated. Briggs' rural disper-
sion coefficients combined  with  Pas-
quill's1, Draxler's2,  and Cramer's3 that
use  onsite  turbulence measurements
were evaluated for the Johnsonville site.
  A  matrix  of  model alternatives was
developed for use in Paradise in 1976 and
for use in Johnsonville in 1977. These
matrices are shown in  Tables 1 and 2
respectively.  In the development of the
alternative models, an effort was made to
keep each change in a  technique inde-
pendent of the other techniques.

Accomplishments
  Short-term S02 concentrations were
evaluated at Paradise with seven model-
ing alternatives and at Johnsonville with
eleven modeling  alternatives.  The
accomplishments of this study included
the following:

  1) The development  of  two years of
    data (one year for Paradise and one
    year for Johnsonville) consisting of
    hourly S02 emission rates and stack
    characteristics, hourly S02 concen-
    trations  monitored  at ten to twelve
    receptor sites, hourly average onsite
    meteorological   parameters,  and
    hourly  NWS  meteorological  data
    collected at BNA, and EW;

  2) The  incorporation  of  alternative
    modeling techniques into the EPA
    Gaussian plume dispersion model,
    MPTER,  including modifications of
    MPTER to allow for the input  of
    onsite  meteorological   data,  the
    development of an algorithm  for
    calculating dispersion using Briggs'
    rural interpolation  formulae,  and
    adaptations of  onsite  turbulence
    schemes using methods described
    by Pasquill, Draxler, and Cramer;

  3) The  implementation   of  these
    models using the available data on
    EPA's UNIVAC computer; and
'Pasquill, F. 1976. Atmospheric Dispersion Parame-
 ters in Gaussian Plume Modeling Part II Possible
 Requirements  for  Change in Turner Workbook
 Values. EPA-600/4-76-030b. Environmental Pro-
 tection Agency Research Triangle Park, North Caro-
 lina. 53 p.
2Draxler, R. 1976. "Determination of Atmospheric
 Diffusion Parameters."Atmos. Environ. 10: 99-105.
3Cramer, H. E. 1976 "Improved Techniques for Mod-
 eling the Dispersion of Tall Stack Plumes." In: Pro-
 ceedings of the Seventh International Technical
 Meeting on Air Pollution Modeling and Its Applica-
 tion. N. 51, NATO/CCMS Airlie House, Virginia, pp.
 731-780.
  4) The analysis of the model's results
     and observed  S02 concentrations
     using relatively straightforward sta-
     tistical comparisons.


Results
Paradise
  At the Paradise plant, greater differ-
ences  in predicted  SO2 concentrations
resulted  from using various emissions
data than from using alternative disper-
sion schemes and  meteorological data.
Furthermore, the "conservative"full-load
emissions models compared more favor-
ably to  peak observed concentrations
than the "more realistic"  models using
hourly emissions data, which underpre-
dicted  peak concentrations by about a
factor of two. This unexpected result was
attributed  to  inaccuracies  associated
with estimating stability, mixing heights,
wind vectors, and/or S02 emission rates.
  Another  unexpected  feature  of the
Paradise analysis was that the  models
incorporating onsite wind  data  did not
show significant improvements over the
models using airport meteorological data.
  Although the concentrations from the
two modeling alternatives differed hour
to hour, the overall results, especially for
the peak concentrations, were similar.
  Although   emissions  input   and
meteorological   data  have  been
recognized as having important effects in
dispersion modeling, dispersion schemes
are usually discussed as a primary basis
for  model  differences. The concentra-
tions predicted with the three dispersion
schemes at Paradise,  however, resulted
in average differences of less than 10
percent.  Buoyancy-induced  dispersion
did seem to increase concentrations with
the  models  using  the  Briggs and  PG
dispersion  coefficients,  although  the
Briggs coefficients  potentially can yield
lower   concentrations  for  downwind
distances  up to  two   kilometers.
Furthermore, measurements taken from
receptors closer to the source than those
located at Paradise should be examined
for  comparison with the Briggs  and PG
curves.
Johnsonville
  With the  11 Johnsonville alternative
models, the principal  emphasis  was on
the  prediction  of peak concentrations,
especially the concentrations related to
the National Ambient Air Quality Stand-
ards for SO2. Some additional analyses
were used to diagnostically evaluate the
models.
    The significant differences between
the emissions data alternatives that were

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Table 1.   Modeling Alternative Matrix Used for Paradise


                                             Model Number
Technique
Emissions input
  Full-load conditions
  Hourly averages

Meteorology input
  BNA airport data
  EVV airport data
  Onsite wind data

Dispersion scheme
  PG
  PC with BID
  Briggs formulae with BID
Table 2.   Mode/ing Alternative Matrix for Johnsonville
                                           Model Number
Technique
                            2     3
                               10   11
Emissions input
  Full-load conditions
  Daily averages
  Hourly averages

Meteorology input
  BNA airport data
  BNA, exclude calms
  Onsite wind data

Dispersion scheme
  PG
  PG with BID
  Briggs with BID
  Pasquill's 1976 scheme
  Draxler's scheme
  Cramer's scheme
XXXXXXXX
           X    X    X    X    X   X
noted in the Paradise analysis were not
evident in the Johnsonville analysis. In
fact, the models using full-load emissions
data compared similarly to the models
using hourly and daily emission data for
the peak concentrations. The differences
between  the  models  using  daily and
hourly emissions data seemed insignifi-
cant; in retrospect, it probably would have
been more cost effective to use the daily
emission rates rather than  the hourly
emission rates. The similar performance
noted  for the  models  using  full-load,
daily, and hourly emission rates may have
been  due to  the  increased plume rise
associated  with  full-load  stack
parameters, which would cause a reduc-
tion in maximum surface concentrations.
  It appeared that the procedure to elim-
inate calm winds had little effect on peak
concentrations. At other power plant
sites  where  the  receptors are located
  closer to the source and where A- and B-
  stability has a  greater effect  on  peak
  concentrations,  the elimination of calm
  winds  might be  an  important
  consideration.
    As with Paradise, little additional bene-
  fit was gained by using onsite wind data
  in  preference to  airport  data.  This  is
  probably because the airport site,  BNA,
  and the Johnsonville site are similar in
  topography. In the diagnostic evaluation,
  the  model  using onsite wind  data did
  show better performance over the airport
  model, resulting in  higher correlations
  and mean fractional errors closer to zero.
    The  differences between the models
  using different dispersion schemes were
  again small in contrast to the differences
  noted with the emission and meteorolog-
  ical  alternatives. In predicting the peak
  concentrations,  the three basic disper-
  sion models (PG,  PG  with  buoyancy-
 induced  dispersion,   and  Briggs)
 performed  about equally. The models
 using on-site turbulence data, however,
 did not perform as well as expected. The
 Pasquill scheme overpredicted most peak
 concentrations.  The  modeling
 alternatives  using   the  Cramer  and
 Draxler dispersion schemes gave results
 that  were  comparable  to the models
 using  the  PG  curves  but   differed
 substantially,  on occasion, from the
 observations. Because the Cramer and
 Draxler models limited dispersion during
 nighttime hours, further work is needed
 to develop  a  scheme  to  practically
 estimate  dispersion  using  routine
 meteorological measurements during all
 meteorological regimes.' In this study, the
 PG model appeared to perform as well as
 the other dispersion  schemes.

 Conclusions and
 Recommendations
   In studies of this kind, the results often
 suggest a need for improving modeling
 techniques and for obtaining more so-
 phisticated input data. This study did not
 deviate from this tradition. The  alterna-
 tive modeling approaches  used with the
 Johnsonville and Paradise plants yielded
 results  that  were within an order of
 magnitude  of the  peak SO2 concentra-
 tions.  Yet,  further  improvements  are
 possible with more accurate source term
 data,  more  site-specific meteorological
 data,   and   more  refined   dispersion
 schemes.
   The major differences in model per-
 formance resulted from  differences in
 emission rates and to a lesser extent from
 the use of different meteorological data.
 The   use  of alternative dispersion
 schemes  was  not  as significant.
 However, efforts to improve the measure-
 ments of the  standard   deviations  of
 horizontal and vertical wind direction (as
 well  as  other turbulence parameters)
 could provide a more  reliable  means for
 estimating dispersion.
   The task of model  evaluation in this
 study was  especially  onerous, because
 slight  differences in  predicted plume
trajectories overwhelmed the statistical
comparison  used  to examine  the
 alternative  modeling  approaches.  This
further  substantiates  the observation
that   the  Gaussian  plume  dispersion
 model is especially sensitive to the input
of wind direction. Model evaluations
could perhaps be simplified by following
the advice of Calder and Johnson, i.e.,
that each model component be separately
 evaluated. Otherwise,  it  is  difficult  to
compare the  strengths and weaknesses

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   of different modeling  techniques. The
   difficulty in performing model evaluation
   is further  compounded by lack of field
   data. The  availability of field data from
   studies such as Cinder Cone Butte, Idaho,
   and Kincaid, Illinois, will hopefully make
   the tasks of model evaluation and model
   improvement less formidable.
          The EPA author Thomas £. Pierce was on assignment to the Environmental
            Sciences Research Laboratory, Research Triangle Park, NC 27711 from NOAA,
            U. S. Department of Commerce {presently with NUS Corporation, Gaithersburg,
            MD).
          D. Bruce Turner is the EPA Project Officer (see beiow).
          The complete report, entitled "An Evaluation of Alternative Gaussian Plume
            Dispersion Modeling Techniques in Estimating Short-Term Sulfur Dioxide
            Concentrations," (Order No. PB 84 -223 62 7; Cost: $16.00, subject to change)
            will be available only from:
                  National Technical Information Service
                  5285 Port Royal Road
                  Springfield. VA 22161
                  Telephone: 703-487-4650
          The EPA Project Officer can be contacted at:
                  Environmental Sciences Research Laboratory
                  U.S. Environmental Protection Agency
                  Research Triangle Park, NC 27711
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