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that performance evaluation be based on comparisons <strong>of</strong> <strong>the</strong> full set <strong>of</strong> predicted/observed<br />

data pairs as well as <strong>the</strong> highest predicted <strong>and</strong> observed values per event <strong>and</strong> <strong>the</strong> highest N<br />

values (e.g., N=10) unpaired in space or time that represents <strong>the</strong> highest end <strong>of</strong> <strong>the</strong><br />

concentration distribution.<br />

Six <strong>of</strong> <strong>the</strong> eight LRT models were applied to both <strong>the</strong> GP80 <strong>and</strong> SRL75 experiments. The ARRPA<br />

model could only be applied to <strong>the</strong> GP80 database <strong>and</strong> <strong>the</strong> MTDDIS model could only be<br />

applied to <strong>the</strong> SRL75 database. Model performance was generally consistent between <strong>the</strong> two<br />

tracer databases <strong>and</strong> was characterized by three features:<br />

• A spatial <strong>of</strong>fset <strong>of</strong> <strong>the</strong> predicted <strong>and</strong> observed patterns.<br />

• A time difference between <strong>the</strong> predicted <strong>and</strong> observed arrival <strong>of</strong> <strong>the</strong> plumes to <strong>the</strong><br />

receptors.<br />

• A definite angular <strong>of</strong>fset <strong>of</strong> <strong>the</strong> predicted <strong>and</strong> observed plumes that could be as much as<br />

20‐45 degrees.<br />

The LRT models tended to underestimate <strong>the</strong> horizontal spreading <strong>of</strong> <strong>the</strong> plume at ground level<br />

resulting in too high peak (centerline) concentrations when compared to <strong>the</strong> observations. For<br />

<strong>the</strong> Lagrangian models this is believed to be due to using sigma‐y dispersion (Turner) curves<br />

that are representative <strong>of</strong> near‐source <strong>and</strong> are applied for longer (> 50 km) downwind<br />

distances. The spatial <strong>and</strong> angular <strong>of</strong>fsets resulted in poor correlations <strong>and</strong> large bias <strong>and</strong> error<br />

between <strong>the</strong> predicted <strong>and</strong> observed tracer concentrations when paired by time <strong>and</strong> location.<br />

However, when comparing <strong>the</strong> maximum predicted <strong>and</strong> observed concentrations unmatched<br />

by time <strong>and</strong> location, <strong>the</strong> models performed much better. For example, <strong>the</strong> average <strong>of</strong> <strong>the</strong><br />

highest 25 predicted <strong>and</strong> observed concentrations (unpaired in location <strong>and</strong> time) were within<br />

a factor <strong>of</strong> two for six <strong>of</strong> <strong>the</strong> eight models evaluated (MESOPUFF, MESOPLUME, MESOPLUME,<br />

MTDDIS, ARRPA <strong>and</strong> RTM‐II). The study concluded that <strong>the</strong> LRT models’ observed tendency to<br />

over‐predict <strong>the</strong> observed peak concentrations errs on <strong>the</strong> conservative side for regulatory<br />

applications. However, this over‐prediction must be weighed against <strong>the</strong> general tendency <strong>of</strong><br />

those models to underestimate horizontal spreading <strong>and</strong> to predict a plume pattern that is<br />

spatially <strong>of</strong>fset from <strong>the</strong> observed data.<br />

2.3.2 Rocky Mountain Acid Deposition Model Assessment Project – Western Atmospheric<br />

Deposition Task Force<br />

A second round <strong>of</strong> LRT model evaluations was conducted as part <strong>of</strong> <strong>the</strong> Rocky Mountain Acid<br />

Deposition Model Assessment (EPA, 1990). In this study, <strong>the</strong> eight models from <strong>the</strong> 1986<br />

evaluation were compared against a newer model, <strong>the</strong> Acid Rain Mountain Mesoscale Model<br />

(ARM3) (EPA, 1988). The statistical evaluation considered data paired in time/space <strong>and</strong> also<br />

unpaired in time/space equally. In this study, it was found that <strong>the</strong> MESOPUFF‐II (Scire et al.,<br />

1984a, <strong>and</strong> 1984b) model performed best when using unpaired data, <strong>and</strong> that <strong>the</strong> ARM3 model<br />

performed best when using paired data. A final model score was assigned on <strong>the</strong> basis <strong>of</strong> a<br />

model’s performance relative to <strong>the</strong> o<strong>the</strong>rs in each <strong>of</strong> <strong>the</strong> areas (paired in time/space, unpaired<br />

in time/space, <strong>and</strong> paired in time, not space) for each <strong>of</strong> two tracer releases considered.<br />

The primary objective was to assemble a mesoscale air quality model based primarily on<br />

models or model components available at <strong>the</strong> time for use by state <strong>and</strong> federal agencies to<br />

assess acid deposition in <strong>the</strong> complex terrain <strong>of</strong> <strong>the</strong> Rocky Mountains.<br />

8

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