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Documentation of the Evaluation of CALPUFF and Other Long ...

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2.3.3 Comparison <strong>of</strong> <strong>CALPUFF</strong> Modeling Results to Two Tracer Field Experiments<br />

The <strong>CALPUFF</strong> dispersion model (<strong>CALPUFF</strong> Version 4) was compared against tracer<br />

measurements from <strong>the</strong> GP80 <strong>and</strong> SRL75 field study experiments in a study conducted by<br />

James O. Paumier <strong>and</strong> Roger W. Brode (EPA, 1998a). The evaluation approach adopted <strong>the</strong><br />

method used by Irwin (1997) that examined fitted predicted <strong>and</strong> observed plume<br />

concentrations across an arc <strong>of</strong> receptors. Meteorological inputs for <strong>the</strong> <strong>CALPUFF</strong> model were<br />

based on CALMET using observed surface <strong>and</strong> upper‐air meteorological data. The study found<br />

that for <strong>the</strong>se three tracer releases, <strong>the</strong>re was overall agreement between <strong>the</strong> observed times<br />

<strong>and</strong> modeled times for both <strong>the</strong> time required for <strong>the</strong> plume to reach <strong>the</strong> receptor arc, as well<br />

as <strong>the</strong> time to pass completely by <strong>the</strong> arc. However, <strong>the</strong> transport direction had an angular<br />

<strong>of</strong>fset. For <strong>the</strong> GP80 100 km arc, <strong>CALPUFF</strong> underestimated <strong>the</strong> lateral dispersion <strong>of</strong> <strong>the</strong> plume<br />

<strong>and</strong> overestimated <strong>the</strong> plume peak as well as <strong>the</strong> cross wind integrated concentration (CWIC)<br />

average concentrations across <strong>the</strong> plume; <strong>the</strong> lateral dispersion <strong>and</strong> CWIC were within a factor<br />

<strong>of</strong> two <strong>of</strong> <strong>the</strong> observed value <strong>and</strong> <strong>the</strong> <strong>CALPUFF</strong> fitted plume centerline concentrations was 2 to<br />

2½ times greater than observed. Very different model performance was seen at <strong>the</strong> 600 km arc<br />

<strong>of</strong> receptors with simulated maximum <strong>and</strong> CWIC that were 2 to 2 ½ times lower than observed<br />

<strong>and</strong> lateral dispersion that was 2½ to 3½ times greater than observed.<br />

2.3.4 ETEX <strong>and</strong> ATMES‐II<br />

After <strong>the</strong> Chernobyl accident in April 1986, <strong>the</strong> Atmospheric Transport Model <strong>Evaluation</strong> Study<br />

(ATMES) was initiated to compare <strong>the</strong> evolution <strong>of</strong> <strong>the</strong> radioactive cloud from Chernobyl with<br />

predictions by ma<strong>the</strong>matical models for atmospheric dispersion, using as input <strong>the</strong> estimated<br />

source term <strong>and</strong> <strong>the</strong> meteorological data for <strong>the</strong> days following <strong>the</strong> accident. Considerable<br />

work was undertaken by ATMES in order to identify <strong>and</strong> make available <strong>the</strong> databases <strong>of</strong><br />

radionuclide concentration in air measured after <strong>the</strong> Chernobyl accident <strong>and</strong> <strong>of</strong> meteorological<br />

conditions that occurred. The ATMES LRT dispersion modeling <strong>and</strong> model evaluation was<br />

conducted in <strong>the</strong> 1989‐1990 time period. The performance <strong>of</strong> <strong>the</strong> LRT models to predict <strong>the</strong><br />

observed radionuclides was hampered by <strong>the</strong> poor characterization <strong>of</strong> <strong>the</strong> emissions release<br />

from Chernobyl.<br />

In May 1989, it was proposed to carry out a massive tracer experiment in Europe designed to<br />

address <strong>the</strong> weaknesses <strong>of</strong> ATMES modeling. In <strong>the</strong> following year <strong>the</strong> proposal was analyzed<br />

<strong>and</strong> modified to adapt it to <strong>the</strong> European context, <strong>and</strong> to take account <strong>of</strong> <strong>the</strong> ATMES results, as<br />

<strong>the</strong>y became available. The experiment was named ETEX 16 , European Tracer Experiment. It<br />

was designed to test <strong>the</strong> readiness <strong>of</strong> interested services to respond in <strong>the</strong> case <strong>of</strong> an<br />

emergency, to organize <strong>the</strong> tracer release <strong>and</strong> compile a data set <strong>of</strong> measured air<br />

concentrations <strong>and</strong> to investigate <strong>the</strong> performance <strong>of</strong> long range atmospheric transport <strong>and</strong><br />

dispersion models using that data set.<br />

The period 15 October‐15 December 1994 was selected as <strong>the</strong> possible window for <strong>the</strong> two<br />

tracer experiments as part <strong>of</strong> ETEX. The first release started at 1600 UTC on October 23, 1994,<br />

<strong>and</strong> lasted 11 hours <strong>and</strong> 50 minutes. 340 kg <strong>of</strong> PMCH (perfluoromethylcyclohexane) tracer were<br />

released in Monterfil, France (48° 03’ 30’’ N, 2° 00’ 30’’ W) at an average flow rate <strong>of</strong> 8.0 g/s.<br />

The second ETEX tracer experiment started at 1500 UTC on November 14, 1994 <strong>and</strong> lasted for 9<br />

hours <strong>and</strong> 45 minutes <strong>and</strong> released 490 kg <strong>of</strong> PMCP (perfluromethlcyclopentane) from<br />

Monterfil for an average release rate <strong>of</strong> 11.58 g/s.<br />

16 http://rem.jrc.ec.europa.eu/etex/<br />

9

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