A. Governing equations of the model   d. Radiation up previous next
A.d.vi. Solar flux and zenith angle

The solar flux is integrated over all wavelengths at the top of the atmosphere, , becomes dependent on season, latitude and local time. In this section, we show the formulation of as a function of local time at a specified season and latitude.

Assume that (W m-2) is the solar constant at the mean orbital radius of a planet, and are the radius of its orbit and its mean value, is solar zenith angle, is latitude, is the solar declination angle, is the hour angle (). Then is represented by using the following variables (cf. Ogura, 1999).

(A.52)
(A.53)

and are given as follows.


where ω is the true anomaly, is the semi-major axis of orbit, is eccentricity, is obliquity, is the true anomaly of vernal equinox. longitude of the vernal equinox relative to the perihelion. By introducing the areocentric longitude of the Sun and assuming = , is rewritten as follows.

(A.54)

In this study, = 0.093, = 25.2°, = 100°, and = 591 Wm-2. The value of is derived from Figure 1-1 of Carr (1996). The other parameters are adapted from Scientific Handbook (National Astronomical Observatory of Japan, 2000).


A Numerical Simulation of Thermal Convection in the Martian Lower Atmosphere with a Two-Dimensional Anelastic Model
Odaka, Nakajima, Ishiwatari, Hayashi,   Nagare Multimedia 2001
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