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Generic Guidance and Optimum Model Settings for the CALPUFF ...

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In <strong>CALPUFF</strong>, by default, a calm period is defined as that when <strong>the</strong> puff transport speed is less<br />

than <strong>the</strong> user-supplied threshold speed which has a current default value of 0.5 m/s. The default<br />

calm threshold speed is used to identify periods when <strong>the</strong> transport distances are minimal, but not<br />

zero.<br />

In <strong>CALPUFF</strong>, several adjustments are automatically made to <strong>the</strong> normal algorithms to simulate<br />

calm periods. These adjustments affect <strong>the</strong> way <strong>the</strong> slugs are released, <strong>the</strong> way gradual plume<br />

rise is addressed, <strong>the</strong> way near-source effects are simulated <strong>and</strong> <strong>the</strong> way <strong>the</strong> puff size changes<br />

during each sampling step. Conceptually, under calm conditions it is expected that a fresh release<br />

will rise virtually straight up from <strong>the</strong> source <strong>and</strong> disperse as a function of time due to wind<br />

fluctuations about a mean of zero.<br />

The following adjustments are made to puffs released into a calm period<br />

� Slugs are released as puffs, <strong>the</strong> length of <strong>the</strong> slug is zero<br />

� All mass <strong>for</strong> <strong>the</strong> period (typically one hour) is placed into one puff<br />

� The distance to final rise is set to zero (<strong>the</strong>re<strong>for</strong>e no gradual plume rise)<br />

� Building downwash effects are not included<br />

� The growth of σy <strong>and</strong> σz is based on time, ra<strong>the</strong>r than distance traveled during <strong>the</strong><br />

sampling step, regardless of <strong>the</strong> dispersion option chosen by <strong>the</strong> user in <strong>the</strong> control file<br />

� Minimum values of turbulence velocities <strong>for</strong> σv <strong>and</strong> σw are imposed.<br />

When CALMET has been used, u* <strong>and</strong> w* may be available even when <strong>the</strong> puff transport speed is<br />

less than <strong>the</strong> threshold, so that turbulence can be estimated. However, it is recognized that this<br />

may not be a robust procedure if <strong>the</strong> wind data used by CALMET includes true calms, since<br />

under <strong>the</strong>se conditions estimates of turbulence velocities σv <strong>and</strong> σw can be indeterminate.<br />

<strong>CALPUFF</strong> relies on <strong>the</strong>se velocities to grow <strong>the</strong> puffs using time dependent dispersion <strong>for</strong>mulas<br />

during periods that are calms which can occur under both stable <strong>and</strong> convective conditions.<br />

There are two ways to improve <strong>CALPUFF</strong>’s behaviour in calm conditions, <strong>the</strong> first is to use subhourly<br />

meteorological data <strong>and</strong> <strong>the</strong> second is to use sub hourly meteorological data combined<br />

with true measured turbulence parameters, σv <strong>and</strong> σw. This is discussed below;<br />

3.6.1 Sub hourly meteorological data <strong>and</strong> its usage in <strong>CALPUFF</strong><br />

Steady state Gaussian regulatory models are traditionally limited to a one hour time step <strong>and</strong> one<br />

hour meteorological data even though sub-hourly meteorological data is typically recorded <strong>and</strong><br />

stored at most Automatic wea<strong>the</strong>r stations around <strong>the</strong> world. Of <strong>the</strong> currently available regulatory<br />

models <strong>CALPUFF</strong> is <strong>the</strong> only regulatory model that is able to use sub hourly meteorological <strong>and</strong><br />

emissions data. The consequences of this <strong>for</strong> realistically modelling calm conditions are<br />

significant.<br />

True calm/stagnation events seldom last longer than several consecutive hours at a time be<strong>for</strong>e<br />

some instability, mechanical or convective destroys’ <strong>the</strong> event. Traditional models with <strong>the</strong>ir<br />

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