Before that could happen, the atmosphere would be so full of cloud, which would prevent solar
flux reaching the surface, that the maximum surface temperature would be much less than 100C.
You said» on average
the flux reaching the surface is about 320W / M2 in the daytime» No.
Not exact matches
Leblanc et al. (2003), through simulations of SEP trajectories inside Mercury's magnetosphere, showed that significant SEP
fluxes can
reach Mercury's
surface not only into the cusps footprint, as in the case of solar wind, but also at the planet's equator, elongated toward dawn.
It is found with both methods that the heat
flux is maximum at the center of the nanowire, while it decreases when
reaching the exterior
surfaces of nanowires.
How these cyclical climate take place is still unknown, but they «are most likely caused by variations in the solar wind and associated magnetic fields that affect the
flux of cosmic rays incident on cloudiness, and thereby control the amount of sunlight
reaching the earth's
surface and thus the climate.»
The temperature at various locations in the atmosphere and on the
surface of the earth is determined by the net
flux of energy at that location (and never
reaches true equilibrium because the energy input from the sun changes with night / day and the seasons).
The difference is in timing: the equilibrium between ocean
surface and atmosphere is
reached in 1 - 3 years half life time, but the deep oceans - atmosphere exchanges are limited in
flux and need much longer periods to
reach equilibrium (half life time ~ 40 years).
Precipitation: increased freshwater / iceberg
flux cools ocean mixed layer, increases sea ice area, causing increase of precipitation that falls before it
reaches Antarctica, adding to ocean
surface freshening and reducing ice sheet growth.
That
flux is dominated by insolation (solar energy
reaching the
surface) but the temperature is also (notionally) influenced by thermodynamic state and the magnitude of currents and circulations, both horizontal and vertical.
On average, at all stations, the sensitivity of
surface shortwave
flux to changes in cloud cover is about -0.5 ± 0.1 W m - 2 % -1 in winter according to both ground - based and satellite observations but in summer
reaches -1.5 ± 0.3 and -1.8 ± 0.2 W m - 2 % -1 according to ground - based and satellite observations, respectively.
whereF is radiant - energy
flux at the emitting
surface; εis emissivity, set at 1 for a blackbody that absorbs and emits all irradiance
reaching its emitting
surface (by Kirchhoff's law of radiative transfer, absorption and emission are equal and simultaneous), 0 for a whitebody that reflects all irradiance, and (0, 1) for a graybody that partly absorbs / emits and partly reflects; and σ ≈ 5.67 x 10 — 8 is the Stefan - Boltzmann constant.