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Table of Contents - The Atmospheric Studies Group at TRC

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Section 1: Introduction<br />

1.4 Major Model Algorithms and Options<br />

1.4.1 CALMET<br />

<strong>The</strong> CALMET meteorological model consists <strong>of</strong> a diagnostic wind field module and micrometeorological<br />

modules for overw<strong>at</strong>er and overland boundary layers. <strong>The</strong> major fe<strong>at</strong>ures and options <strong>of</strong><br />

the meteorological model are summarized in <strong>Table</strong> 1-1. When using large domains, the user has the<br />

option to adjust input winds to a Lambert Conformal Projection coordin<strong>at</strong>e system to account for the<br />

Earth's curv<strong>at</strong>ure.<br />

<strong>The</strong> diagnostic wind field module uses a two-step approach to the comput<strong>at</strong>ion <strong>of</strong> the wind fields<br />

(Douglas and Kessler, 1988), as illustr<strong>at</strong>ed in Figure 1-6. In the first step, an initial-guess wind field is<br />

adjusted for kinem<strong>at</strong>ic effects <strong>of</strong> terrain, slope flows, and terrain blocking effects to produce a Step 1<br />

wind field. <strong>The</strong> second step consists <strong>of</strong> an objective analysis procedure to introduce observ<strong>at</strong>ional d<strong>at</strong>a<br />

into the Step 1 wind field to produce a final wind field.<br />

An option is provided to allow gridded prognostic wind fields to be used by CALMET, which may better<br />

represent regional flows and certain aspects <strong>of</strong> sea breeze circul<strong>at</strong>ions and slope/valley circul<strong>at</strong>ions. Wind<br />

fields gener<strong>at</strong>ed by the CSUMM prognostic wind field model can be input to CALMET as either the<br />

initial guess field (p<strong>at</strong>hway A in Figure 1-6) or the Step 1 wind field (p<strong>at</strong>hway B in Figure 1-6).<br />

MM4/MM5, NAM(Eta), WRF, RUC, RAMS and TAPM model output fields can be introduced into<br />

CALMET in one <strong>of</strong> three different ways:<br />

as a replacement for the initial guess wind field (p<strong>at</strong>hway A in Figure 1-6).<br />

as a replacement for the Step 1 field (p<strong>at</strong>hway B); or<br />

as "observ<strong>at</strong>ions" in the objective analysis procedure (p<strong>at</strong>hway C).<br />

<strong>The</strong> techniques used in the CALMET model are briefly described below. <strong>The</strong> recommended approach is<br />

p<strong>at</strong>hway A.<br />

Step 1 Wind Field<br />

Kinem<strong>at</strong>ic Effects <strong>of</strong> Terrain: <strong>The</strong> approach <strong>of</strong> Liu and Yocke (1980) is used to evalu<strong>at</strong>e kinem<strong>at</strong>ic<br />

terrain effects. <strong>The</strong> domain-scale winds are used to compute a terrain-forced vertical velocity, subject to<br />

an exponential, stability-dependent decay function. <strong>The</strong> kinem<strong>at</strong>ic effects <strong>of</strong> terrain on the horizontal<br />

wind components are evalu<strong>at</strong>ed by applying a divergence-minimiz<strong>at</strong>ion scheme to the initial guess wind<br />

field. <strong>The</strong> divergence minimiz<strong>at</strong>ion scheme is applied iter<strong>at</strong>ively until the three-dimensional divergence<br />

is less than a threshold value.<br />

1-19

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