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QTCM Approach

All QTCM versions are derived from the nonlinear primitive equations

  equation849

  equation852

  equation855

  equation859

  equation863

where temperature T and specific humidity q are in energy units, tex2html_wrap_inline1877 are the long-wave radiative fluxes depending on T, q and cloudiness over the column, and surface temperature tex2html_wrap_inline1487 . Shortwave fluxes S are positive downward. The operators tex2html_wrap_inline1887 , tex2html_wrap_inline1889 and tex2html_wrap_inline1891 include horizontal diffusion and horizontal advection terms. The vertical fluxes of sensible heat and moisture by nonconvective, diffusive transport, tex2html_wrap_inline1893 and tex2html_wrap_inline1895 , and stress tex2html_wrap_inline1897 , vanish at the top and have drag laws at the surface for tex2html_wrap_inline1899 , evaporation E, and tex2html_wrap_inline1903 . The hydrostatic equation has been used for baroclinic pressure gradients in the momentum equation (gif), where tex2html_wrap_inline1905 is the geopotential at the lowest pressure level tex2html_wrap_inline1907 . tex2html_wrap_inline1909 is surface elevation, tex2html_wrap_inline1911 is surface pressure, tex2html_wrap_inline1913 is atmospheric near-surface density, and tex2html_wrap_inline1915 has been neglected.

An important subsidiary relation that holds for all convective parameterizations is the ``convective heating'' and ``moistening'' terms tex2html_wrap_inline1545 and tex2html_wrap_inline1919 cannot change the vertically integrated moist static energy budget, i.e. tex2html_wrap_inline1921 or

  equation871

where tex2html_wrap_inline1923 , tex2html_wrap_inline1925 , absorbing tex2html_wrap_inline1927 into all fluxes for brevity, and tex2html_wrap_inline1929 denotes vertical averaging over the troposphere, from the surface, tex2html_wrap_inline1911 , to the tropopause, tex2html_wrap_inline1933 .





Johnny Wei-Bing Lin
Thu Sep 9 13:11:12 PDT 1999