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eTheses Repository - University of Birmingham

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presence <strong>of</strong> the dome <strong>of</strong> warmer air above the city have been documented in a number <strong>of</strong><br />

experimental and numerical studies (e.g. Bornstein et al. 2000; Lin et al. 2008).<br />

Potential temperature [K]<br />

Figure 4.6: Vertical section at y=0 <strong>of</strong> potential temperature (K) as computed by the<br />

urban_BEP simulation at 12:00 noon <strong>of</strong> the second day <strong>of</strong> the simulation.<br />

Figure 4.7 represents a vertical section <strong>of</strong> the horizontal wind speed at the centre <strong>of</strong> the<br />

urban domain at 12:00 noon. This shows the convergence <strong>of</strong> low level winds over the city,<br />

and divergence al<strong>of</strong>t. The convergence zone is displaced to the east by the geostrophic<br />

wind, as seen in Martilli et al. (2002) and Martilli (2003). This behaviour can be explained<br />

in terms <strong>of</strong> the three competing forces over the urban area: the drag induced by the urban<br />

surface, the pressure gradient due to higher urban temperatures, and advection due to the<br />

general synoptic flow. As seen in Figure 4.5 low winds are observed near the urban surface<br />

due to the dominance <strong>of</strong> the drag effects. Al<strong>of</strong>t (at about 400 m above the ground) however<br />

the pressure gradient and the advection have the same sign, causing a maximum.<br />

96

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