Slowing the escape of
radiation to space means the planet is warmer than it would have been otherwise.
Not exact matches
Thinner air thus
means fewer molecules
to deflect incoming cosmic rays —
radiation from outer
space.
Alas, as Smith notes, that is where the similarities end; the «Earth - sized» world orbiting HD 10180 is too close
to its star,
meaning it is a roasted exoplanet where any atmosphere is blasted into
space by the star's powerful
radiation and stellar winds.
The fact that there is a natural greenhouse effect (that the atmosphere restricts the passage of long wave (LW)
radiation from the Earth's surface
to space) is easily deducible from i) the
mean temperature of the surface (around 15ºC) and ii) knowing that the planet is roughly in radiative equilibrium.
Because the lapse rate is not zero, changing the altitude near the top of the atmosphere where infrared
radiation escapes freely
to space allows adjustment of the surface temperature by
means of the addition of greenhouse gases.
The term «photosphere» for a star has essentially the same
meaning as any of the six terms «Effective -LCB- Emission
Radiation Radiating -RCB--LCB- Height Level -RCB-» for the atmosphere of a planet, being the altitude at which the gas above has an optical depth of 2/3, i.e. at which about 50 % of the
radiation leaving that altitude vertically upwards escapes
to space.
If the troposhere is cold, that
means sea surface also is cold, and it is still gaining shortwave energy from the Sun at the same rate while it radiates a lesser amount longwave
radiation to space.
Part Six — Nonlinearity and Dry Atmospheres — demonstrating that different distributions of water vapor yet with the same
mean can result in different
radiation to space, and how this is important for drier regions like the sub-tropics
Under those conditions, there will always be a lapse rate in the atmosphere (in the troposphere) as long as it can find some
means to lose energy
to interstellar
space by
radiation or loss of mass.
Therefore, if you work from the layer at which the
radiation escapes into
space (about 6 km) down
to the ground, the negative lapse rate
means that surface temperature has
to be higher than the non-GHG temperature.
If Earth's
mean energy imbalance today is +0.5 W / m2, CO2 must be reduced from the current level of 395 ppm (global -
mean annual -
mean in mid-2013)
to about 360 ppm
to increase Earth's heat
radiation to space by 0.5 W / m2 and restore energy balance.
Somehow, largely by conduction, convection and latent heat, and such
means other than by
radiation, heat flows from the earth's surface
to somewhere, where it is then radiated into
space.
However, even though surface temperatures of land and ocean may experience feedback effects, there are few possible feedbacks posited for the level of the atmosphere where the net
radiation to space takes place, and this
means that the 1.2 degrees C heating effect must be absorbed within the boundaries of the atmosphere somewhere.
It also
means less longwave
radiation escaping
to space.
Without atmosphere the surface of the ocean or land would lose o (T ^ 4 — Ts ^ 4)(1) where Ts is the temperature of the
space (about 4K) while in the presence of the atmosphere the heat losses are hc * (T — Tl)(2) and o (T ^ 4 — Tl ^ 4)(3) where (2) represents the heat transfer by convection (inclusive conduction) through the air layer and (3) corresponds
to the net flow due
to the heat exchange by
radiation, Tl being the
mean temperature of the air layer.
5) Thus the presence of water vapour and CO2
means that less energy is radiated into
space from within their characteristic
radiation bands so the temperature of the earth's surface has
to increase in order for energy radiated at other wavelengths
to increase
to compensate.
This
means the Earth absorbed more energy from solar
radiation than it emitted as heat back
to space.
That goes for GHGs as much as it does for other gases, which
means that
radiation will gain more free access
to space above in close step with the decrease in opaque gas molecules.
Therefore, since energy may leave the Earth System only by
radiation out
to Space, the
mean energy output of the Earth System is about 240 Watts / m ^ 2.
The violet curve (above right) shows that, assuming a
mean temperature of 255 K, Earth System
radiation to Space is in a squat, wide «longwave» range, from about 5μm
to beyond 40μm, which we call mid - and far - infrared.
Notice that the Earth System
mean temperature I had
to use
to provide 240 Watts / m ^ 2 of
radiation to Space to balance the input absorbed from by the Earth System from the Sun was 255 K. However, the actual
mean temperature at the Surface is closer
to 288 K.
Heat always moves from warmer
to colder, so it must move, through whatever
means, from the tropics
to the arctic or, via
radiation,
to outer
space.
Ira said: «Notice that the Earth System
mean temperature I had
to use
to provide 240 Watts / m ^ 2 of
radiation to Space to balance the input absorbed from by the Earth System from the Sun was 255 K. However, the actual
mean temperature at the Surface is closer
to 288 K.
If you
mean by «the atmosphere heats the earth» that the atmosphere causes the earth
to be at a higher steady - state temperature than if all of the
radiation that the earth emitted went back out into
space, then yes, that is what I am claiming; however, it doesn't violate the 2nd Law because the heat still goes from the earth
to the atmosphere.
The first part of Secretary Langley's instruction required me
to procure or design and construct the best instruments and
means for determining the intensity of the sun's
radiation in free
space at the earth's
mean solar distance.
«The Planck feedback parameter [equivalent
to κ — 1] is negative (an increase in temperature enhances the long - wave emission
to space and thus reduces R [the Earth's
radiation budget]-RRB-, and its typical value for the earth's atmosphere, estimated from GCM calculations (Colman 2003; Soden and Held 2006), is ~ 3.2 W m2ºK — 1 (a value of ~ 3.8 W m2ºK — 1 is obtained by defining [κ — 1] simply as 4σT3, by equating the global
mean outgoing long - wave
radiation to σT4 and by assuming an emission temperature of 255 ºK).»
It will be convenient here
to define the term radiative exchange equilibrium between two specified regions of
space (or bodies) as
meaning that for the two regions (or bodies) A and B, the rate of flow of
radiation emitted by A and absorbed by B is equal
to the rate of flow the other way, regardless of other forms of transport that may be occurring.
The atmosphere is in long - term equilibrium which
means that all thermally emitted
radiation is in balance with the loss at the top of the atmospher
to space.
Meanwhile, he continued, higher cloud tops in effect thicken the total column of cloud, and that
means more trapping of infrared or heat
radiation that would otherwise exit
to space.