The Idealized greenhouse model article on Wikipedia gives the following solution for finding the global surface temperature on an idealized planet with an atmosphere:
$$T_s = \left[ \frac{S_0(1 - \alpha_p)}{4\sigma} \frac{1}{1 - \frac{\epsilon}{2}} \right]^{1/4} $$
- $T_s$ is the surface temperature on the planet,
- $S_0$ is the solar constant, in this case for Mars,
- $\alpha_p$ is the planetary albedo,
- $\sigma$ is the Stefan-Boltzmann constant,
- $\epsilon$ is the emissivity or absorptivity of the atmosphere.
The number 4 in the denominator is accounting for the fact that the surface area of a sphere is 4 times the area of its intercept (its shadow), so the average incoming radiation is $S_0/4$.
But for a local area near the equator that would stretch $y$ km along its longitude, for a full day/night cycle the total surface area for the incoming radiation along its latitude would be $2\pi ry$ km², while the intercept (or shadow) of that total surface area would be $2ry$ km², $r$ being the radius of the circle at that latitude of the planet.
So couldn't one use the expression above for a local area near the equator when the number 4 in the denominator would be replaced by $\pi$, and also take into account the latitude of the local area and the axial tilt of Mars ?
It still would be an idealized model of course, not accounting for the winds for example.
And could this adjusted model be still more refined, or localized ?
And are there other models to predict the average local temperatures on Mars ?