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252                  17. The Physics of the Atmosphere

       These equations combine Boyle's law, which states that when temperature
       is held constant the volume varies inversely with the pressure, and the
       law of Guy-Lussac, which states that when pressure is held constant the
       volume varies in proportion to the absolute temperature.


       A. First Law of Thermodynamics
         If a volume of air is held constant and a small amount of heat A/i is
       added, the temperature of the air will increase by a small amount AT. This
       can be expressed as



       where c v is the specific heat at constant volume. In this case, all the heat
       added is used to increase the internal energy of the volume affected by the
       temperature. From the equation of state (Eq. 17-8), it can be seen that the
       pressure will increase.
         If, instead of being restricted, the volume of air considered is allowed to
       remain at an equilibrium constant pressure and expand in volume, as well
       as change temperature in response to the addition of heat, this can be
       expressed as


       By using the equation of state, the volume change can be replaced by a
       corresponding pressure change:


       where c p is the specific heat at constant pressure and equals c v + R d/ where
       R d is the gas constant for dry air.


        B. Adiabatic Processes
          An adiabatic process is one with no loss or gain of heat to a volume of
       air. If heat is supplied or withdrawn, the process is diabatic or nonadiabatic.
       Near the earth's surface, where heat is exchanged between the earth and
       the air, the processes are diabatic.
          However, away from the surface, processes frequently are adiabatic. For
       example, if a volume (parcel) of air is forced upward over a ridge, the
       upward-moving air will encounter decreased atmospheric pressure and
       will expand and cool. If the air is not saturated with water vapor, the
       process is called dry adiabatic. Since no heat is added or subtracted, &h in
       Eq. (17-13) can be set equal to zero, and introducing the hydrostatic equation



       and combining equations results in
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