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Table of Contents - The Atmospheric Studies Group at TRC

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Section 1: Introduction<br />

Slope Flows: Slope flows are computed based on the shooting flow parameteriz<strong>at</strong>ion <strong>of</strong> Mahrt (1982).<br />

Shooting flows are buoyancy-driven flows, balanced by adjective <strong>of</strong> weaker momentum, surface drag,<br />

and entrainment <strong>at</strong> the top <strong>of</strong> the slope flow layer. <strong>The</strong> slope flow is parameterized in terms <strong>of</strong> the terrain<br />

slope, distance to the crest and local sensible he<strong>at</strong> flux. <strong>The</strong> thickness <strong>of</strong> the slope flow layer varies with<br />

the elev<strong>at</strong>ion drop from the crest.<br />

Blocking Effects: <strong>The</strong> thermodynamic blocking effects <strong>of</strong> terrain on the wind flow are parameterized in<br />

terms <strong>of</strong> the local Froude number (Allwine and Whiteman, 1985). If the Froude number <strong>at</strong> a particular<br />

grid point is less than a critical value and the wind has an uphill component, the wind direction is adjusted<br />

to be tangent to the terrain.<br />

Step 2 Wind Field<br />

<strong>The</strong> wind field resulting from the adjustments described above <strong>of</strong> the initial-guess wind is the Step 1 wind<br />

field. <strong>The</strong> second step <strong>of</strong> the procedure involves the introduction <strong>of</strong> observ<strong>at</strong>ional d<strong>at</strong>a into the Step 1<br />

wind field through an objective analysis procedure. An inverse-distance squared interpol<strong>at</strong>ion scheme is<br />

used which weighs observ<strong>at</strong>ional d<strong>at</strong>a heavily in the vicinity <strong>of</strong> the observ<strong>at</strong>ional st<strong>at</strong>ion, while the Step 1<br />

wind field domin<strong>at</strong>es the interpol<strong>at</strong>ed wind field in regions with no observ<strong>at</strong>ional d<strong>at</strong>a.<br />

<strong>The</strong> resulting wind field is subject to smoothing, an optional adjustment <strong>of</strong> vertical velocities based on the<br />

O'Brien (1970) method, and divergence minimiz<strong>at</strong>ion to produce a final Step 2 wind field.<br />

Introduction <strong>of</strong> Prognostic Wind Field Results<br />

<strong>The</strong> CALMET model contains an option to allow the introduction <strong>of</strong> gridded wind fields gener<strong>at</strong>ed by<br />

MM4/MM5, NAM(Eta), WRF, RUC, RAMS and TAPM (or the CSUMM model) as input fields. <strong>The</strong><br />

procedure permits the prognostic model to be run with a significantly larger horizontal grid spacing and<br />

different vertical grid resolution than th<strong>at</strong> used in the diagnostic model. This option allows certain<br />

fe<strong>at</strong>ures <strong>of</strong> the flow field such as the sea breeze circul<strong>at</strong>ion with return flow al<strong>of</strong>t, which may not be<br />

captured in the surface observ<strong>at</strong>ional d<strong>at</strong>a, to be introduced into the diagnostic wind field results. An<br />

evalu<strong>at</strong>ion with CAPTEX tracer d<strong>at</strong>a indic<strong>at</strong>ed th<strong>at</strong> the better sp<strong>at</strong>ial and temporal resolution <strong>of</strong>fered by<br />

the hourly MM4 fields can improve the performance <strong>of</strong> the dispersion modeling on regional scales (EPA,<br />

1995).<br />

If the prognostic wind d<strong>at</strong>a are used as the initial guess field, the coarse grid scale d<strong>at</strong>a are interpol<strong>at</strong>ed to<br />

the CALMET fine-scale grid. <strong>The</strong> diagnostic module in CALMET will then adjust the initial guess field<br />

for kinem<strong>at</strong>ic effects <strong>of</strong> terrain, slope flows and terrain blocking effects using fine-scale CALMET terrain<br />

d<strong>at</strong>a to produce a Step 1 wind field. A second approach is to use prognostic wind d<strong>at</strong>a directly as the Step<br />

1 wind field. This field is then adjusted using observ<strong>at</strong>ional d<strong>at</strong>a, but additional terrain adjustments are<br />

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