Not exact matches
Blackbody radiation was an extension clarifying further details about heat,
emission and
temperature.
So while, in the isothermal
blackbody surface approximation, if the starting surface
temperature is 288 K and we know the OLR is reduced from surface
emission by 150 W / m2 via GHE, we know that removing all greenhouse agents will have a TOA forcing of -150 W / m2, (and some forcing at the tropopause, etc.) which will cool the surface
temperature to about 255 K at equilibrium, absent non-Planck feedbacks.
For a small amount of absorption, the
emission upward and downward would be about the same, so if the upward (spectral) flux from below the layer were more than 2 * the (average)
blackbody value for the layer
temperature (s), the OLR at TOA would be reduced more than the net upward flux at the base of the layer, decreasing CO2 TOA forcing more than CO2 forcing at the base, thus increasing the cooling of the base.
Emissivity = proportion of
emission with reference to a
blackbody (it's a ratio)
Emission = emissivity x what a
blackbody would emit at that
temperature (it's an absolute value)
It seems to me that any layer from the surface to the highest limits of the atmosphere is radiating some roughly
blackbody looking spectrum corresponding to its own
Temperature; and much of that spectrum exits directly to space (assuming cloudless skies for the moment) with a spectrum corresponding to the emission temperature of that surface; but now with holes in it from absorption by GHG molecules or the atmospheric gases
Temperature; and much of that spectrum exits directly to space (assuming cloudless skies for the moment) with a spectrum corresponding to the
emission temperature of that surface; but now with holes in it from absorption by GHG molecules or the atmospheric gases
temperature of that surface; but now with holes in it from absorption by GHG molecules or the atmospheric gases themselves.
The infrared radiation hangs around longer than it would have done, some being absorbed by matter, causing heating, which causes higher re-emission (the
blackbody spectrum of the whole Earth's
emissions moves slightly to a higher energy -
temperature profile, in order to balance out the radiation budget of the Earth).
After all, it makes perfect sense that something that is nearly a
blackbody at a
temperature of about 15 C will emit only 50 W / m ^ 2 of
emission (gross)... at least once you repeal a few laws of physics that were never much use to us anyway!
To be clear, the Hottel average is across the entire
blackbody emission for that
temperature.
This is called the Planck feedback because it is fundamentally due to the Planck
blackbody radiation law (warmer
temperatures = higher
emission).