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QTCM Approach

All QTCM versions are derived from the nonlinear primitive equations

  equation942

  equation945

  equation948

  equation952

  equation956

where temperature T and specific humidity q are in energy units, tex2html_wrap_inline2955 are the long-wave radiative fluxes depending on T, q and cloudiness over the column, and surface temperature tex2html_wrap_inline2421 . Shortwave fluxes S are positive downward. The operators tex2html_wrap_inline2965 , tex2html_wrap_inline2967 and tex2html_wrap_inline2969 include horizontal diffusion and horizontal advection terms. The vertical fluxes of sensible heat and moisture by nonconvective, diffusive transport, tex2html_wrap_inline2971 and tex2html_wrap_inline2973 , and stress tex2html_wrap_inline2975 , vanish at the top and have drag laws at the surface for tex2html_wrap_inline2977 , evaporation E, and tex2html_wrap_inline2981 . The hydrostatic equation has been used for baroclinic pressure gradients in the momentum equation (5.3), where tex2html_wrap_inline2983 is the geopotential at the lowest pressure level tex2html_wrap_inline2985 . tex2html_wrap_inline2987 is surface elevation, tex2html_wrap_inline2989 is surface pressure, tex2html_wrap_inline2991 is atmospheric near-surface density, and tex2html_wrap_inline2993 has been neglected.

An important subsidiary relation that holds for all convective parameterizations is the ``convective heating'' and ``moistening'' terms tex2html_wrap_inline2995 and tex2html_wrap_inline2997 cannot change the vertically integrated moist static energy budget, i.e. tex2html_wrap_inline2999 or

  equation964

where tex2html_wrap_inline3001 , tex2html_wrap_inline3003 , absorbing tex2html_wrap_inline3005 into all fluxes for brevity, and tex2html_wrap_inline3007 denotes vertical averaging over the troposphere, from the surface, tex2html_wrap_inline2989 , to the tropopause, tex2html_wrap_inline3011 .





Climate Systems Interaction Group
Tue Aug 13 18:22:11 PDT 2002