Page 307 - Fundamentals of Air Pollution
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IV. Local Wind Systems                 263















          Fig. 17-17. Sea breeze due to surface heah'ng over land, resulting in thermals, and subsi-
        dence over water.


        surface out over the water, completing a circular or cellular flow (Fig. 17-
        17). Any general flow due to large-scale pressure systems will be superim-
        posed on the sea breeze and may either reinforce or inhibit it. Ignoring the
        larger-scale influences, the strength of the sea breeze will generally be a
        function of the temperature excess of the air above the land surface over
        that above the water surface.
          Just as heating in the daytime occurs more quickly over land than over
        water, at night radiational cooling occurs more quickly over land. The
        pressure pattern tends to be the reverse of that in the daytime. The warmer
        air tends to rise over the water, which is replaced by the land breeze from
        land to water, with the reverse flow (water to land) completing the circular
        flow at altitudes somewhat aloft. Frequently at night, the temperature
        differences between between land and water are smaller than those during
        the daytime, and therefore the land breeze has a lower speed.



        B. Mountain and Valley Winds
          Solar heating and radiational cooling influence local flows in terrain situa-
        tions. Consider midday heating of a south-facing moutainside. As the slope
        heats, the air adjacent to the slope warms, its density is decreased, and
        the air attempts to ascend (Fig. 17-18). Near the top of the slope, the air
        tends to rise vertically. Along each portion of the slope farther down the
        mountain, it is easier for each rising parcel of air to move upslope, replacing
        the parcel ahead of it rather than rising vertically. This upslope flow is the
        valley wind.
          At night when radiational cooling occurs on slopes, the cool dense air
        near the surface descends along the slope (Fig. 17-19). This is the downslope
        wind. To compensate for this descending air, air farther from the slope
        that is cooled very little is warmer relative to the descending air and rises,
        frequently resulting in a closed circular path. Where the downslope winds
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