The regional climate feedbacks formulation reveals fundamental biases in a widely - used method for diagnosing climate sensitivity, feedbacks and radiative forcing — the regression of the global top - of -
atmosphere radiation flux on global surface temperature.
I agree that the concept of no feedback sensitivity makes most sense in the context of the top of
the atmosphere radiation fluxes.
Not exact matches
This means that there is an upward surface
flux of LW around (~ 390 W / m2), while the outward
flux at the top of the
atmosphere (TOA) is roughly equivalent to the net solar
radiation coming in (1 - a) S / 4 (~ 240 W / m2).
In that survey, it was almost universal that groups tuned for
radiation balance at the top of the
atmosphere (usually by adjusting uncertain cloud parameters), but there is a split on pratices like using
flux corrections (2 / 3rds of groups disagreed with that).
Refraction, specifically the real component of refraction n (describes bending of rays, wavelength changes relative to a vacuum, affects blackbody
fluxes and intensities — as opposed to the imaginary component, which is related to absorption and emission) is relatively unimportant to shaping radiant
fluxes through the
atmosphere on Earth (except on the small scale processes where it (along with difraction, reflection) gives rise to scattering, particularly of solar
radiation — in that case, the effect on the larger scale can be described by scattering properties, the emergent behavior).
There is non-radiative heat
flux in the
atmosphere though and energy can be transported above the level where the greenhouse effect is dominant but eventually must be lost by thermal
radiation.
Recent accurate laboratory measurements of the absorption in the CO2 band by CLOUD (1952) were used to calculate the
radiation flux in the
atmosphere with the aid of the MIDAC high speed digital computor.»
where is the vertically integrated energy
flux in the
atmosphere, is the net radiative energy input to an atmospheric column (the difference between absorbed shortwave
radiation and emitted longwave
radiation), and is the oceanic energy uptake at the surface.
The other
fluxes (shortwave and longwave
radiation at both surface and top of
atmosphere) show more «normal» cycles (though somewhat higher values).
Sea ice is an important component of the Earth system; it is highly reflective, altering the amount of solar
radiation that is absorbed; it changes the salinity of the ocean where it forms and melts, and it acts as a barrier to the exchange of heat and momentum
fluxes between the
atmosphere and ocean.
Calculation of solar irradiance i.e. shortwave
radiation flux and the
atmosphere's heat
radiation i.e. longwave
radiation flux is important.
Over land, you have a surface energy balance that includes downwelling IR, upwelling IR (Stefan Boltzmann), downwelling solar
radiation minus what is reflected back from the surface, latent heat
flux and sensible heat
flux (these are turbulent
fluxes associated with exchange with the
atmosphere), and conductive
flux from the ground (below the surface).
A SOM is much cheaper and simpler to run compared to a full ocean model, but still reacts to things happening in the
atmosphere, like changes in downwelling
radiation or
fluxes associated with surface wind.
So there is now an increased
radiation flux downward, which will heat up both the lower
atmosphere and also the ground directly (if the optical depth between the photosphere and the ground is not too great).
«Because the solar - thermal energy balance of Earth [at the top of the
atmosphere (TOA)-RSB- is maintained by radiative processes only, and because all the global net advective energy transports must equal zero, it follows that the global average surface temperature must be determined in full by the radiative
fluxes arising from the patterns of temperature and absorption of
radiation.»
Ice significantly reduces the heat
flux between ocean and
atmosphere; through its high albedo it has a strong influence on the
radiation budget of the entire Arctic.
The
atmosphere is analogous to a flexible lens that is shaped by the density distribution of the gas molecules, of the
atmosphere in the space between the sphere holding them, and space; Incoming heat gets collected in many ways and places,, primarily by intermittent solar
radiation gets stored, in vast quantities, and slowly but also a barrage of mass and energy
fluxes from all directions; that are slowly transported great distances and to higher altitudes mostly by oceanic and atmospheric mass flows.
It also balances at the surface including
radiation, latent heat, heat
flux, and it balances within the
atmosphere.
The internal kinetic energy is taken as the upward long wave energy
flux at the top of the
atmosphere, and the potential energy is the upward
radiation flux from the surface.
The cooling rate depends on all the
fluxes, including also conductive / convective, latent heat, and back -
radiation from the
atmosphere.
«in an isotropic non GHG world, the net would be zero, as the mean conduction
flux would equalize, but in our earth it is still nearly zero» if the
atmosphere were isothermal at the same temperature as the surface then exactly the downwelling
radiation absorbed by the surface would be equal to the
radiation of th surface absorbed by the air (or rather by its trace gases) and both numbers would be (1 - 2E3 (t (nu)-RRB--RRB- pi B (nu, T) where t (nu) is the optical thickness, B the Planck function, nu the optical frequency and T the temperature; as the flow from the air absorbed by the surface is equal to the flow from the surface absorbed by the air, the radiative heat transfer is zero between surface and air.
In all of these simple models, we assume the
atmosphere to have a volume as fixed as a bathtub, we assume that the
atmosphere / ocean system is a closed system, we assume that the incoming
radiation from the Sun is constant, we assume no turbulence, we assume no viscosity, we assume radiative equilibrium with no feedback lag, we take no account of water vapor
flux assuming it to be constant, no change in albedo from changes in land use, glacier lengthening and shortening, no volcanic eruptions, no feedbacks from vegetation.
It seems to me that the two papers use at least a similar approach — and one that seems very sensible to me — correlating surface temperature with
radiation fluxes at the top of the
atmosphere.
Many believe that increased water vapor, solar variations in
radiation and magnetic
flux, our relative position in the solar system, the tilt of our planet's axis, the clearing of our
atmosphere of pollutants which allows more sunlight to reach the ground, or our position in the Milky Way galaxy that affects the amount of
radiation reaching our
atmosphere and affecting cloud formation, are also important and are not (and can not be yet) adequately considered in the computer models used by the IPCC consensus.
The climate models create ~ 66 % more than real lower
atmosphere warming by the fake «back
radiation» idea, taught in US Atmospheric Science for ~ 50 years, coupled with the fake single -18 deg C OLR emitter idea, which provides an imaginary negative Down
flux in the bowdlerised two - stream approximation (blame Sagan for this).
Chen, T., and W.B. Rossow, 2002: Determination of top - of -
atmosphere longwave
radiation fluxes: A comparison between two approaches using ScaRaB data.
A significant
flux of solar
radiation was found to penetrate the entire thickness of the
atmosphere, with the amount at the ground 1.5 % of that incident on the top of the
atmosphere.
Abstract Measurements of the
flux of downward solar
radiation through the
atmosphere of Venus and at the planetary surface are reported.
[1] Total absorbed
radiation (TAR), the sum of SNR [shortwave net
radiation] and LDR [longwave downward
radiation], represents the total radiative energy available to maintain the Earth's surface temperature and to sustain the turbulent (sensible and latent) heat
fluxes in the
atmosphere.
So by KT97 if you let the surface be 289K as stated in TFK09 instead of 288K you can take: 67 Wm - 2 absorbed SW by the
atmosphere plus 24 Wm - 2 carried upward by thermals (dry conduction / convection) plus 78 Wm - 2 carried upward by evaporation (convection) plus 66 Wm - 2 actual LW
radiation flux upward (
radiation)------ 235 Wm - 2 detected LW upwelling by satellites above the TOA
Likewise, the emission of CO2 within its absorption bands is just as effective as its interception, therefore this energy is partitioned throughout the
atmosphere and radiated back to earth in its majority (because the escape of energy through the optically thick higher levels of the
atmosphere reduces the
flux, whereas the earth is still optically close by and a ready recipient of IR
radiation.
13) No partitioning of energies into long wave
radiation (from the
atmosphere) and short wave (from the sun), ensuring that no conclusions can be drawn about where the power
fluxes measured are coming from.
We use the 9 climate variables of surface air temperature (SAT), sea level pressure (SLP), precipitation (rain), the top of
atmosphere (TOA) shortwave (SW) and longwave (LW) full - sky
radiation, clear - sky
radiation (CLR, radiative
flux where clouds do not exists), and cloud radiative forcing (CRF, radiative effect by clouds diagnosed from the difference between full - sky and clear - sky
radiation, Cess et al. 1990).