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11.2  General Gaussian Dispersion Model                         321

            temperatures, and humidity. Less obvious, but equally important, are vertical
            motions that influence air parcel motion. Atmospheric stability affects the vertical
            motion of air parcels. The temperature difference between the air parcel and
            atmosphere causes vertical motion, at least near the emission source, but the con-
            vective circulation thus established is affected directly by the stability of the
            atmosphere. Winds tend to be turbulent and gusty when the atmosphere is unstable,
            and this type of weather causes air pollutants to disperse erratically. Subsidence
            occurs in larger scale vertical circulation as air from high-pressure areas replaces
            that carried aloft in adjacent low-pressure systems. This often brings very dry air
            from a high altitude to a low level.



            11.2.4 Adiabatic Lapse Rate of Temperature


            In the analysis above, we assumed constant air temperature and molar weight,
            however, both temperature T and molar weight M change with elevation, and the
            change in M is not as important as that of temperature. For an adiabatic air parcel in
            the atmosphere, it may produce work to the surroundings. The rate of temperature
            change over elevation can be derived from the first law of thermodynamics [21]as

                                  dT            g
                                     ¼                                  ð11:10Þ
                                   dz    c p;a þ h dw=dTð  Þ
                                               fg
            where c p;a is the air heating capacity, w is the water vapor mass fraction in the air
            (kg vapor/air). Since most air contains less than a few percent of water vapor,
            except for those in cloud or fogs, the effect of water vapor can be ignored and we
            can use a simpler equation that is meant to be for dry air

                                        dT      g
                                           ¼                            ð11:11Þ
                                        dz     c p;a
            This is also called the adiabatic lapse rate of dry air temperature. Temperature
            decreases with elevation and it is a straight line in a plot of elevation versus
            temperature (Fig. 11.4). With a typical air heating capacity of c p;a ¼ 1;006 J/kg.K
                          2
            and g ¼ 9.81 m/s , we can estimate the adiabatic lapse rate of dry air temperature
            dT  ¼ 0.975 or 9.75 K/km. This is an estimation for guidance only. The actual value
            dz
            changes with location and time. As dry air moves vertically, its temperature
            changes at about 1 °C per 100 m [21]. For air with moisture, the temperature change
            could be 5–10 °C per km, depending on its water content, and air up in the sky
            reaches saturation easily to form clouds.
              The change of temperature over elevation is the main reason behind atmospheric
            stability, which is an important factor in air dispersion.
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