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 />
Sensitivity to ∆t; ∆x = 1 km<br />
Vertical Velocity x-section through Manhattan<br />
∆t=6 s<br />
∆t=1 s<br />
∆t=0.66 s<br />
∆t=0.11 s<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 />
Terra Incognita<br />
LES and mesoscale limits<br />
From Wyngaard<br />
•If the (integral) scale <strong>of</strong> the turbulence is l, then in the LES limit, i.e., ∆ ≪ l, the numerical grid resolves all <strong>of</strong> the<br />
energy-containing turbulence.<br />
•The subgrid model is responsible only for energy transfer from the resolved scales. The standard Smagorinsky<br />
(or Lilly) subgrid model produces this transfer at the correct mean rate.<br />
•In the mesoscale limit, ∆ ≫ l, no turbulence is resolved. Turbulence effects are represented through a subgrid<br />
model, typically <strong>of</strong> the ensemble-mean type. In principle the subgrid model can be adjusted to perform well in this<br />
limit.<br />
•Between these two limits lies the Terra Incognita where the subgrid model carries significant fluxes and<br />
transfers energy. In principle neither ensemble mean nor the traditional LES closures are appropriate there.<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 />
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