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Fine Scale Meteorology & Air Quality Models - School of Architecture ...

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ASI2_Lecture 3_7/12/2011<br />

erturbations nique inks to etup xploration<br />

Taking the model’s<br />

• <strong>Fine</strong> scale modeling enters the “Terra Incognita” regime<br />

• Given that mesoscale modeling systems have many<br />

operating options, how are the resulting simulation<br />

dependent on the user selection <strong>of</strong> model options.<br />

• Need to understand the properties <strong>of</strong> modeling systems<br />

dependence on the properties <strong>of</strong> their individual<br />

components and their linkages.<br />

• Ad hoc modeling group is currently undertaking this study,<br />

preliminary results follows.<br />

• Perform & explore model sensitivity studies including:<br />

Model physics, numerics, time steps, grid size, filtering<br />

ASI 2: URBAN CLIMATE AND AIR POLLUTION <strong>School</strong> <strong>of</strong> <strong>Architecture</strong>, The Chinese University <strong>of</strong> Hong Kong, Hong Kong, 7-8 Dec 2011<br />

Numerical Considerations: Horizontal Diffusion<br />

Standard configuration <strong>of</strong> WRF has in the horizontal the Smagorinsky scheme<br />

K<br />

h<br />

s<br />

C x<br />

2<br />

s<br />

C 0.4<br />

2<br />

u<br />

v<br />

<br />

0.25<br />

2 2 <br />

<br />

<br />

x<br />

y<br />

<br />

ASI 2: URBAN CLIMATE AND AIR POLLUTION <strong>School</strong> <strong>of</strong> <strong>Architecture</strong>, The Chinese University <strong>of</strong> Hong Kong, Hong Kong, 7-8 Dec 2011<br />

2<br />

2<br />

u<br />

v<br />

<br />

<br />

<br />

y<br />

x<br />

<br />

<br />

In Martilli’s simulations, with DX=1km, this gives K h values <strong>of</strong> the order <strong>of</strong> 100-200 m2/s<br />

Standard MM5 has in the horizontal (see Xu et al. MWR 2001)<br />

K<br />

K<br />

h<br />

H 0<br />

K<br />

H 0<br />

3. 10<br />

2<br />

2<br />

<br />

2 2 u<br />

v<br />

u<br />

v<br />

<br />

Cs<br />

x<br />

0.25<br />

2 2 <br />

<br />

<br />

x y<br />

<br />

<br />

y x<br />

<br />

<br />

3<br />

x<br />

t<br />

2<br />

2<br />

600.<br />

m 2 //s<br />

s<br />

For Dx=1000.m and Dt=5s (Martilli’s case)<br />

“the background term K H0 is dominant at all levels and locations<br />

throughout the simulation time” Xu et al. MWR 2001<br />

21

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