The radiative heating (cooling) term
in Equation
(A.4) is given by the
convergence (divergence) of the net radiative heat flux, which is
calculated by using the radiative transfer equation.
We consider the following radiation processes in our model: absorption
of near infrared solar radiation (NIR), absorption and emission of
infrared radiation associated with atmospheric CO2,
absorption and scattering of solar radiation, and absorption and
emission of infrared radiation associated with dust.
Scattering of NIR and infrared radiation associated with atmospheric
CO2 are not taken into consideration.
Infrared radiative heating due to atmospheric CO2 is a
major radiative heating (cooling) source near the surface
(cf., Savijärvi, 1991b).
Atmospheric temperature in the Martian stratosphere is determined from
a balance between near infrared radiative heating and infrared
cooling associated with atmospheric CO2
(Gierasch and Goody, 1967).
Infrared radiation associated with dust can not be negligible when
calculating nighttime radiative cooling.
is represented as follows.
|
(A.22) |
Qrad,IR and Qrad,NIR are the infrared
and near infrared radiative heating rates associated with
CO2.
Qrad,dust,SR and Qrad,dust,IR are
the solar and infrared radiative heating rates associated with
dust.
The governing equations to calculate these heating rates are described
in the following sections.
- Radiative transfer of atmospheric CO2
- Band parameters of CO2
- Radiative transfer of dust
- Dust opacity
- Optical parameters of dust
- Solar flux and zenith angle
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