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

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4.4 MODEL PERFORMANCE EVALUATION FOR THE SRL75 TRACER EXPERIMENT<br />

The Irwin (1997) plume fitting evaluation approach was used to evaluate <strong>CALPUFF</strong> for <strong>the</strong> SRL75<br />

field experiment. There are two components to <strong>the</strong> Irwin plume fitting evaluation approach:<br />

1. A temporal analysis that examines <strong>the</strong> time <strong>the</strong> tracer arrives, leaves <strong>and</strong> resides on <strong>the</strong><br />

receptor arc; <strong>and</strong><br />

2. A plume fitting procedures that compares <strong>the</strong> predicted observed peak <strong>and</strong> average plume<br />

concentrations <strong>and</strong> <strong>the</strong> width <strong>of</strong> <strong>the</strong> plume by fitting a Gaussian plume through <strong>the</strong><br />

predicted or observed concentrations across <strong>the</strong> arc <strong>of</strong> receptors or monitors that lie on<br />

<strong>the</strong> 100 km receptor arc.<br />

Because only long‐term integrated average observed SF6 samples were available, <strong>the</strong> timing<br />

component <strong>of</strong> <strong>the</strong> evaluation could not be compared against observed values in <strong>the</strong> SRL75<br />

experiments.<br />

Most <strong>of</strong> <strong>the</strong> <strong>CALPUFF</strong> sensitivity tests estimated that <strong>the</strong> tracer arrived at <strong>the</strong> 100 km arc on<br />

hour 13 LST, 2½ hours after <strong>the</strong> beginning to <strong>the</strong> tracer release. The exceptions to this are <strong>the</strong><br />

<strong>CALPUFF</strong>/MMIF simulations using <strong>the</strong> 4 km MM5 data <strong>and</strong> <strong>CALPUFF</strong>/MMIF using <strong>the</strong> 36 km <strong>and</strong><br />

PG dispersion that estimated <strong>the</strong> plume arrives at hour 14 LST. With one exception, <strong>the</strong><br />

<strong>CALPUFF</strong> simulations estimated that <strong>the</strong> tracer resided ei<strong>the</strong>r 5 or 6 hours on <strong>the</strong> arc. And with<br />

two exceptions, it was <strong>the</strong> meteorological data ra<strong>the</strong>r than <strong>the</strong> dispersion option that defined<br />

<strong>the</strong> residence time <strong>of</strong> <strong>the</strong> estimated tracer on <strong>the</strong> 100 km receptor arc. The exceptions were<br />

for <strong>the</strong> PG dispersion sensitivity test that in two cases predicted <strong>the</strong> tracer would remain one<br />

less hour on <strong>the</strong> arc; <strong>the</strong> <strong>CALPUFF</strong>/CALMET BASE sensitivity test using <strong>the</strong> PG dispersion<br />

estimated that <strong>the</strong> tracer would reside only 4 hours on <strong>the</strong> 100 km receptor arc. Without any<br />

observed tracer timing statistics, <strong>the</strong>se results are difficult to interpret.<br />

Table 4‐9 displays <strong>the</strong> model performance evaluation for <strong>the</strong> various <strong>CALPUFF</strong> sensitivity tests<br />

using <strong>the</strong> Irwin plume fitting evaluation approach. The observed values were taken from <strong>the</strong><br />

1998 EPA <strong>CALPUFF</strong> tracer test evaluation report data (EPA, 1998a). Also shown in Table 4‐4 are<br />

<strong>the</strong> statistics from <strong>the</strong> 1998 EPA report for <strong>the</strong> <strong>CALPUFF</strong> V4.0 modeling using Pasquill‐Gifford<br />

(PG) <strong>and</strong> similarity (CAL) dispersion. Note that <strong>the</strong> EPA 1998 <strong>CALPUFF</strong> modeling used CALMET<br />

with just observations so is analogous to <strong>the</strong> BASE sensitivity scenario that used <strong>CALPUFF</strong> V5.8.<br />

There are five statistical parameters evaluated using <strong>the</strong> Irwin plume fitting evaluation<br />

approach:<br />

• Cmax, which is <strong>the</strong> plume fitted centerline concentration.<br />

• Omax, which is <strong>the</strong> maximum observed value at <strong>the</strong> ~40 monitoring sites or maximum<br />

predicted value across <strong>the</strong> ~200 receptors along <strong>the</strong> 100 km arc.<br />

• Sigma‐y, which <strong>the</strong> second moment <strong>of</strong> <strong>the</strong> Gaussian distribution <strong>and</strong> a measure <strong>of</strong> <strong>the</strong><br />

plume spread.<br />

• Plume Centerline, which is <strong>the</strong> angle <strong>of</strong> <strong>the</strong> plume centerline from <strong>the</strong> source to <strong>the</strong> 100<br />

km arc.<br />

• CWIC, <strong>the</strong> cross wind integrated concentration (CWIC) across <strong>the</strong> predicted <strong>and</strong> observed<br />

fitted Gaussian plume.<br />

The first thing we note in Table 4‐9 is that <strong>the</strong> maximum centerline concentration <strong>of</strong> <strong>the</strong> fitted<br />

Gaussian plume to <strong>the</strong> observed SF6 tracer concentrations across <strong>the</strong> 12 monitors (2.739 ppt) is<br />

almost half <strong>the</strong> observed maximum at any <strong>of</strong> <strong>the</strong> monitors (5.07 ppt). As <strong>the</strong> centerline<br />

concentrations in a Gaussian plume represents <strong>the</strong> maximum concentration, this means that<br />

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