And witnessed TRUE radiative cooling of the car's hood, roof, until they eventually «dew up»... the reason why FOG FORMS (
surface radiative cooling).
Not exact matches
Results show that the intrusion of dust from the Sahara Desert caused
radiative cooling of Earth's
surface.
During this event, the aerosols stayed close to the
surface due to the presence of a anticyclone hovering over the study region at sea - level, «reducing the amount of shortwave irradiance reaching the
surface and causing greater
radiative cooling,» states Obregón, who likens the effects of desert dust with those resulting from certain forest fires or episodes of high pollution.
That's far from the worst flaw in his calculation, since his two biggest blunders are the neglect of the
radiative cooling due to sulfate aerosols (known to be a critical factor in the period in question) and his neglect of the many links in the chain of physical effects needed to translate a top of atmosphere
radiative imbalance to a change in net
surface energy flux imbalance.
ENSO events, for example, can warm or
cool ocean
surface temperatures through exchange of heat between the
surface and the reservoir stored beneath the oceanic mixed layer, and by changing the distribution and extent of cloud cover (which influences the
radiative balance in the lower atmosphere).
ENSO events, for example, can warm or
cool ocean
surface temperatures through exchange of heat between the
surface and the reservoir stored beneath the oceanic mixed layer, and by changing the distribution and extent of cloud cover (which influences the
radiative balance in the lower atmosphere).
The troposphere is currently
cooling radiatively at about 2K / day, and adding CO2 to the atmosphere generally increases the
radiative cooling (primarily through increases in water vapor, though how these details play out also depend on the details of the
surface budget).
In the case of Concentrated Solar Power that uses heliostats, one ought to be able to boost night time
cooling by providing a low brightness temperature
surface (the mirrors) to enhance
radiative cooling, though the convective
cooling will still dominate.
But the troposphere can still warm with an increased
radiative cooling term because it is also balanced by heating through latent heat release, subsidence, solar absorption, increased IR flux from the
surface, etc..
As far as I know, if the only physical mechanism under consideration is the
radiative cooling of the planet's
surface (which was heated by shortwave solar radiation and reradiated at longer wavelengths in the infrared) via
radiative transport, additional gas of any kind can only result in a higher equilibrium temperature.
Even parabolic troughs might run
radiative cooling through pipes placed halfway between the collector vacuum pipes and the mirror
surface since these pipes would see
cool portions of the sky not occupied by the Sun.
... interestingly in the grey gas case with no solar heating of the stratosphere, increasing the optical thickness of the atmosphere would result in an initial
cooling of and in the vicinity of the skin layer (reduced OLR), and an initial
radiative warming of the air just above the
surface (increased backradiation)-- of course, the first of those dissappears at full equilibrium.
The argument isn't actually as firm a constraint as generally believed, since the infrared
radiative cooling of the atmosphere is affected by the temperature difference between air and the underlying
surface, which can adjust to accommodate any amount of evaporation Nature wants to dump into the atmosphere (as shown in Pierrehumbert 1999 («Subtropical water vapor...» available here)-RRB-.
In full equilibrium, at any given level, there may be some net
radiative heating at some frequencies compensated by some net
radiative cooling at other frequencies, with convection balancing the full spectrum
radiative cooling of the troposphere and heating of the
surface.
This is plainly not true, as can be easily seen by computing the net
radiative cooling in a
radiative - convective model with a consistent
surface energy budget.
In the pure
radiative equilibrium, you can get it into a range where the grey model gives you
surface warming and stratospheric
cooling (that's in one of the problems), but you have to work at it a bit, and also remember to plot things in pressure coord, not optical depth coordinates.
The lapse rate within the troposphere is largely determined by convection, which redistributes any changes in
radiative heating or
cooling within the troposphere +
surface so that all levels tend to shift temperature similarly (with some regional / latitudinal, diurnal, and seasonal exceptions, and some exceptions for various transient weather events).
Re my 441 — competing bands — To clarify, the absorption of each band adds to a warming effect of the
surface + troposphere; given those temperatures, there are different equilibrium profiles of the stratosphere (and different
radiative heating and
cooling rates in the troposphere, etc.) for different amounts of absorption at different wavelengths; the bands with absorption «pull» on the temperature profile toward their equilibria; disequilibrium at individual bands is balanced over the whole spectrum (with zero net LW
cooling, or net LW
cooling that balances convective and solar heating).
The very pretty thermographs prove that the sensor is not affected by the local walls — sensor colour is
cool -(although I am certain Mr. Watts did not normalise the
radiative properties of the sensor and
surface — wrecking the accuracy of this reading — e.g. a glossy
surface can reflect the surrounding temperature and not the
surface temp of the unit).
The very pretty thermographs prove that the sensor is not affectedby the local walls — sensor colour is
cool -(although I am certain Mr. Watts did not normalise the
radiative properties of the sensor and
surface — wrecking the accuracy of this reading — e.g. a glossy
surface can reflect the surrounding temperature and not the
surface temp of the unit).
Knowing the change in the non-
radiative cooling of the Earth
surface is as important as knowing the change in the
radiative cooling, for computing the climate response to increased DWLWIR.
It's because both land and ocean
surfaces are heated by shortwave solar radiation and where aerosols reflect SWR equally well over land or water and where greenhouse gases work by retarding the rate of
radiative cooling which is not equal over land and water.
The water vapor
cooled the Earth, the snow
cooled the atmosphere with resulting increase in
surface albedo which does reflect
radiative heat, meaning the Earth gets less warm, not colder because of it.
Finally, you mention water vapour as a GHG... but water vapour is the main
cooling component in the atmosphere, transporting heat from the
surface to the
radiative layer, so not really a true GHG.
Initially, shallow circulations driven by differential
radiative cooling induce a self - aggregation of the convection into a single band, as has become familiar from simulations over idealized sea
surfaces.
It clearly states that (a) emission of energy by radiation is accompanied with
cooling of the
surface (if no compensating changes prevent it), and (b) the tendency to a
radiative equilibrium means that the emitter with the higher
surface temperature will loose energy due to a negative net radiation balance until this net radiation balance becomes zero.
Consider this: The
surface is
cooled predominantly by non-
radiative heat transfer, while on the other hand the atmosphere is
cooled exclusively by
radiative transfer to space.
The
surface is
cooled predominantly by non-
radiative heat transfer, while on the other hand the atmosphere is
cooled exclusively by
radiative transfer to space.
The IPCC most certainly also claims water vapour warms, doing most of «33 degrees» of warming, whereas, in fact, it
cools the
surface by reducing the temperature gradient whilst still keeping
radiative balance with the Sun.
This
cooling to the
surface can actually be a pretty large source of
cooling.To illustrate how important this is, the authors put this really informative table from some idealized
radiative calculations.
Hard data trends in
radiative flux — trends that are internally consistent, consistent across platforms and consistent with
surface observations of cloud in the Pacific — show strong warming in the SW and
cooling in UV in the period in question.
The more «greenhouse» or IR - active gases in the stratosphere up to the thermosphere / edge of space, the more
radiative surface area is available for
radiative COOLING to space.
The temperature did not change, so the
surface temperature - dependent responses of atmospheric
radiative cooling also did not change.
Here we show that accounting for recent
cooling in the eastern equatorial Pacific reconciles climate simulations and observations.We present a novel method of uncovering mechanisms for global temperature change by prescribing, in addition to
radiative forcing, the observed history of sea
surface temperature over the central to eastern tropical Pacific in a climate model.
You write: «If internal variability (such a a
cool PDO phase) reduces the rate of increase of
surface temperature, while the e [x] ternal forcing still is increasing, this means the
radiative imbalance is impeded from being cancelled by
surface warming.»
The presence of BC resulted in positive
radiative forcing in the atmosphere leading to warming effect (+ 2.1 W / m2) whereas
cooling was observed at the top of the atmosphere (− 0.4 W / m2) and at
surface (− 2.5 W / m2).
If internal variability (such a a
cool PDO phase) reduces the rate of increase of
surface temperature, while the eternal forcing still is increasing, this means the
radiative imbalance is impeded from being cancelled by
surface warming.
I'm always aware that evaporative and convective
cooling near the
surface is contributing to the heating of the atmosphere; but do tend to push it aside, to concentrate on what the purely EM
radiative effects are.
The atmospheric heating and
cooling rates are then passed back to the atmosphere structure module that calculates how much the
surface and atmospheric temperatures would change during the 30 - minute times step given the
radiative heating and
cooling rates.
The DALR is established in Earth's atmosphere by vertically moving macroscopic parcels of air driven by thermal convection between volumes and
surfaces at different temperatures, temperature gradients maintained by diurnal solar forcing and continual
radiative cooling.
The role of
radiative gases in atmospheric
cooling and tropospheric convective circulation far out weighs their role is slowing the
cooling of the land
surface.
Can
radiative gases emit IR to the
surface (land only) and slow it's
cooling rate?
Konrad: It has long been understood that convection
cools the
surface... and that adding convection to a purely
radiative model of the atmosphere reduces the greenhouse effect.
If look look back over my comments on this thread, you will note that I repeatedly state that
radiative gases can slow the
cooling of land
surface and by intercepting
surface IR they can heat gases in the lower troposphere.
Without
radiative cooling at altitude, tropospheric temperatures above the near
surface layer would rise to near
surface Tmax.
Land
surface Tav may be lower under a non
radiative atmosphere, but this does not translate to a
cooler atmosphere.
No, without
radiative cooling (but assuming the same albedo for simplicity), the temperature of the Earth's
surface would not be average 288 K but rather only ~ 255 K (really the average of the square of the temperature over the
surface).
Without
radiative gases, the
surface would be ~ 255 K — which is much
cooler than the
surface or lower atmosphere with
radiative gases.
Konrad says: April 18, 2013 at 8:04 pm
Radiative cooling at altitude is critical for continued convective circulation... Energy loss at altitude is just as important for convective circulation as energy input near the
surface.
Experiment 5 shows why greater
radiative cooling of the night land
surface will not result in significantly greater conductive
cooling of an atmosphere in which the gases are free to move.