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QTCM Approach

All QTCM versions are derived from the nonlinear primitive equations

  equation862

  equation865

  equation868

  equation872

  equation876

where temperature T and specific humidity q are in energy units, tex2html_wrap_inline1891 are the long-wave radiative fluxes depending on T, q and cloudiness over the column, and surface temperature tex2html_wrap_inline1499 . Shortwave fluxes S are positive downward. The operators tex2html_wrap_inline1901 , tex2html_wrap_inline1903 and tex2html_wrap_inline1905 include horizontal diffusion and horizontal advection terms. The vertical fluxes of sensible heat and moisture by nonconvective, diffusive transport, tex2html_wrap_inline1907 and tex2html_wrap_inline1909 , and stress tex2html_wrap_inline1911 , vanish at the top and have drag laws at the surface for tex2html_wrap_inline1913 , evaporation E, and tex2html_wrap_inline1917 . The hydrostatic equation has been used for baroclinic pressure gradients in the momentum equation (gif), where tex2html_wrap_inline1919 is the geopotential at the lowest pressure level tex2html_wrap_inline1921 . tex2html_wrap_inline1923 is surface elevation, tex2html_wrap_inline1925 is surface pressure, tex2html_wrap_inline1927 is atmospheric near-surface density, and tex2html_wrap_inline1929 has been neglected.

An important subsidiary relation that holds for all convective parameterizations is the ``convective heating'' and ``moistening'' terms tex2html_wrap_inline1559 and tex2html_wrap_inline1933 cannot change the vertically integrated moist static energy budget, i.e. tex2html_wrap_inline1935 or

  equation884

where tex2html_wrap_inline1937 , tex2html_wrap_inline1939 , absorbing tex2html_wrap_inline1941 into all fluxes for brevity, and tex2html_wrap_inline1943 denotes vertical averaging over the troposphere, from the surface, tex2html_wrap_inline1925 , to the tropopause, tex2html_wrap_inline1947 .





Hui Su
Thu Nov 16 00:53:31 PST 2000