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