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The Grell–Freitas (GF) convection parameterization: recent developments, extensions, and applications
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Abstract. Recent developments and options in the GF (Grell and
Freitas, 2014; Freitas et al., 2018) convection parameterization are
presented. The parameterization has been expanded to a trimodal spectral
size to simulate three convection modes: shallow, congestus, and deep. In
contrast to usual entrainment and detrainment assumptions, we assume that beta
functions (BFs), commonly applied to represent probability density functions
(PDFs), can be used to characterize the vertical mass flux profiles for the
three modes and use the BFs to derive entrainment and detrainment rates. We
also added a new closure for nonequilibrium convection that improved the
simulation of the diurnal cycle of convection, with a better representation
of the transition from shallow to deep convection regimes over land. The
transport of chemical constituents (including wet deposition) can be treated
inside the GF scheme. The tracer transport is handled in flux form and is
mass-conserving. Finally, the cloud microphysics have been extended to
include the ice phase to simulate the conversion from liquid water to ice in
updrafts with resulting additional heat release and the melting from snow to
rain.
Title: The Grell–Freitas (GF) convection parameterization: recent developments, extensions, and applications
Description:
Abstract.
Recent developments and options in the GF (Grell and
Freitas, 2014; Freitas et al.
, 2018) convection parameterization are
presented.
The parameterization has been expanded to a trimodal spectral
size to simulate three convection modes: shallow, congestus, and deep.
In
contrast to usual entrainment and detrainment assumptions, we assume that beta
functions (BFs), commonly applied to represent probability density functions
(PDFs), can be used to characterize the vertical mass flux profiles for the
three modes and use the BFs to derive entrainment and detrainment rates.
We
also added a new closure for nonequilibrium convection that improved the
simulation of the diurnal cycle of convection, with a better representation
of the transition from shallow to deep convection regimes over land.
The
transport of chemical constituents (including wet deposition) can be treated
inside the GF scheme.
The tracer transport is handled in flux form and is
mass-conserving.
Finally, the cloud microphysics have been extended to
include the ice phase to simulate the conversion from liquid water to ice in
updrafts with resulting additional heat release and the melting from snow to
rain.
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