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

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For long range transport applications > 50km, <strong>the</strong> CTSG option is not usually considered as<br />

impacts on far-field receptors is of <strong>the</strong> most interest. In near-field applications involving complex<br />

flows, <strong>the</strong> grid spacing should usually be sufficiently small enough to resolve both <strong>the</strong> dominant<br />

<strong>and</strong> small terrain features adequately.<br />

However, on both near <strong>and</strong> far field applications, if a terrain feature, such as a mine dump that is<br />

too small to be resolved by <strong>the</strong> chosen grid cell resolution is expected to directly influence <strong>the</strong><br />

plume <strong>the</strong>n <strong>the</strong> CTSG scheme may be invoked to explicitly detail <strong>the</strong> flow of plume material<br />

around that terrain obstacle.<br />

3.3 Shoreline Fumigation<br />

Fumigation is classified into two types depending on whe<strong>the</strong>r it is a temporal or spatial<br />

phenomenon. The <strong>for</strong>mer process, termed “nocturnal inversion breakup fumigation,” occurs when<br />

pollutants from an elevated stack are entrained into <strong>the</strong> growing convective boundary layer as it<br />

breaks up <strong>the</strong> nocturnal inversion in <strong>the</strong> morning. The spatial phenomenon, termed “shoreline<br />

fumigation,” occurs when a <strong>the</strong>rmal internal boundary layer growing with downstream distance<br />

entrains pollutants from an elevated stack near a shoreline. Both phenomena are discussed.<br />

3.3.1 Sub-grid Scale TIBL<br />

The majority of cities in New South Wales are located within a few kilometers of <strong>the</strong> coastline<br />

such that many sources are affected by complex 3-D flow patterns typical of coastal regions. As<br />

well as sea <strong>and</strong> l<strong>and</strong> breeze circulation systems, <strong>the</strong> significant differences between <strong>the</strong> boundary<br />

layers of marine <strong>and</strong> overl<strong>and</strong> means distinct changes occur to a dispersing plume moving from<br />

l<strong>and</strong> to sea <strong>and</strong> vice versa. The <strong>CALPUFF</strong> modeling system is well suited to h<strong>and</strong>ling <strong>the</strong>se<br />

complex phenomena <strong>and</strong> will do so on a grid by grid cell basis without any invocation by <strong>the</strong><br />

modeler as long as CALMET supplies <strong>the</strong> meteorology to <strong>CALPUFF</strong>.<br />

Briefly, <strong>the</strong>re are important differences in <strong>the</strong> structure of <strong>the</strong> marine <strong>and</strong> continental boundary<br />

layers which can have significant effects on plume dispersion in <strong>the</strong> overwater <strong>and</strong> coastal<br />

environments. The sensible heat flux over <strong>the</strong> open water is typically more than an order of<br />

magnitude less than that over l<strong>and</strong>. The reasons <strong>for</strong> this are; water has a higher heat capacity <strong>and</strong><br />

is partially transparent to solar radiation resulting in a small diurnal temperature difference; <strong>the</strong><br />

sea is more uni<strong>for</strong>m, <strong>and</strong>, <strong>the</strong>re is a constant supply of moisture in <strong>the</strong> marine boundary layer. As<br />

a result of <strong>the</strong>se differences <strong>the</strong> mixing heights overwater are much lower. At <strong>the</strong> l<strong>and</strong> sea<br />

interface, rapid changes in <strong>the</strong> dispersion characteristics occur which can significantly affect <strong>the</strong><br />

ground-level concentrations from coastal sources. For stacks emitting into <strong>the</strong> stable zone above<br />

<strong>the</strong> shallow marine boundary layer, narrow plumes are intercepted by a growing Thermal Internal<br />

20

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