The upward motion is confined to such a small area, and the subsidence so slow, that one can not ignore
the radiative cooling in the subsiding air.
These three sources speak of three entirely different things: a) the water vapor feedback, b) the carbon cycle feedback, and c) effects on precipitation of reduced longwave
radiative cooling in the tropical lower troposphere.
The strength of
radiative cooling in turn depends on the characteristics of the clouds formed by the condensed vapor.
One might even envision a system in which collector panels similar to trickle style swimming pool panel are glazed during the winter for efficient heat collection (like a Thomason trickle collector), and then the glazing panels are removed in the summer to provide efficient evapro -
radiative cooling in the summer.
Thus, among competing bands, there may be net
radiative cooling in the upper atmosphere or near TOA at longer wavelengths and net heating and shorter wavelengths.
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.
However, global mean precipitation is controlled not by the availability of water vapour, but by a balance between the latent heat of condensation and
radiative cooling in the troposphere.
«In addition to these regions, we can foresee applications for
radiative cooling in off - the - grid areas of the developing world where air conditioning is not even possible at this time.
Not exact matches
The model calculations, which are based on data from the CLOUD experiment, reveal that the
cooling effects of clouds are 27 percent less than
in climate simulations without this effect as a result of additional particles caused by human activity: Instead of a
radiative effect of -0.82 W / m2 the outcome is only -0.60 W / m2.
«No one had yet been able to surmount the challenges of daytime
radiative cooling — of
cooling when the sun is shining,» said Eden Rephaeli, a doctoral candidate
in Fan's lab and a co-first-author of the paper.
Stratospheric
cooling as a result of excess CO2 does influence ozone recovery, and ozone changes
in the troposphere and stratosphere to have effects on
radiative balance of the planet.
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.
You've got the
radiative physics, the measurements of ocean temperature and land temperature, the changes
in ocean heat content (Hint — upwards, whereas if if was just a matter of circulation moving heat around you might expect something more simple) and of course observed predictions such as stratospheric
cooling which you don't get when warming occurs from oceanic circulation.
It provides for the first time a high - fidelity technology demonstration of how you can use
radiative sky
cooling to passively
cool a fluid and,
in doing so, connect it with
cooling systems to save electricity,» said Raman, who is co-lead author of the paper detailing this research, published
in Nature Energy Sept. 4.
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).
Small changes
in oceanic or atmospheric circulation due to small changes
in radiative equilibrium may translate
in flooding here and drying there, warming here and
cooling there, etc..
On the possibility of a changing cloud cover «forcing» global warming
in recent times (assuming we can just ignore the CO2 physics and current literature on feedbacks, since I don't see a contradiction between an internal
radiative forcing and positive feedbacks), one would have to explain a few things, like why the diurnal temperature gradient would decrease with a planet being warmed by decreased albedo... why the stratosphere should
cool... why winters should warm faster than summers... essentially the same questions that come with the cosmic ray hypothesis.
In other words, the same natural forcings that appear responsible for the modest large - scale cooling of the LIA should have lead to a cooling trend during the 20th century (some warming during the early 20th century arises from a modest apparent increase in solar irradiance at that time, but the increase in explosive volcanism during the late 20th century leads to a net negative 20th century trend in natural radiative forcing
In other words, the same natural forcings that appear responsible for the modest large - scale
cooling of the LIA should have lead to a
cooling trend during the 20th century (some warming during the early 20th century arises from a modest apparent increase
in solar irradiance at that time, but the increase in explosive volcanism during the late 20th century leads to a net negative 20th century trend in natural radiative forcing
in solar irradiance at that time, but the increase
in explosive volcanism during the late 20th century leads to a net negative 20th century trend in natural radiative forcing
in explosive volcanism during the late 20th century leads to a net negative 20th century trend
in natural radiative forcing
in natural
radiative forcing).
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.
In the stratosphere, the increased radiative cooling with more CO2 is a ubiquitous feature of double - CO2 simulations and this leads to a drop in the temperature ther
In the stratosphere, the increased
radiative cooling with more CO2 is a ubiquitous feature of double - CO2 simulations and this leads to a drop
in the temperature ther
in the temperature there.
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.
Given the much more rapid respons time of the stratosphere to
radiative forcings, there is (can be) some initial stratospheric
cooling (or at least some
cooling somewhere
in the stratosphere), which consists of a transient component, and a component that remains at full equilibrium.
... 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.
Because latent heat release
in the course of precipitation must be balanced
in the global mean by infrared
radiative cooling of the troposphere (over time scales at which the atmosphere is approximately
in equilibrium), it is sometimes argued that
radiative constraints limit the rate at which precipitation can increase
in response to increasing CO2.
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-.
If you were
in a situation where there was initially more precipitation than
radiative cooling could handle, then the atmosphere could just warm up until the
radiative cooling increased — though then you'd have to worry about how much the warming affects precipitation, etc..
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.
I made the same argument on the slowing of the tropical mass circulation
in a warmer climate, based on Betts and Ridgway (JAS1989) and the difference of the slopes of the Clausius - Clapyron and the
radiative cooling
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 coordinate
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 coordinate
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 coordinate
in pressure coord, not optical depth coordinates.
So a local spike
in precipitation releases a lot of heat — but as the heat increases, this negatively affects the vapor - > water transition (precipitation, or raindrop formation), since warm air holds more water then
cool air — and so the limit on precipitation vis - a-vis the
radiative balance of the atmosphere appears.
In chapter 11.3.6.3 they conclude: ``... it is concluded that the hiatus is attributable, in roughly equal measure, to a decline in the rate of increase in effective radiative forcing (ERF) and a cooling contribution from internal variability (expert judgment, medium confidence)»
In chapter 11.3.6.3 they conclude: ``... it is concluded that the hiatus is attributable,
in roughly equal measure, to a decline in the rate of increase in effective radiative forcing (ERF) and a cooling contribution from internal variability (expert judgment, medium confidence)»
in roughly equal measure, to a decline
in the rate of increase in effective radiative forcing (ERF) and a cooling contribution from internal variability (expert judgment, medium confidence)»
in the rate of increase
in effective radiative forcing (ERF) and a cooling contribution from internal variability (expert judgment, medium confidence)»
in effective
radiative forcing (ERF) and a
cooling contribution from internal variability (expert judgment, medium confidence)».
As I discussed
in # 333, requiring a warmer lower part of the atmosphere, on warming further and emitting more IR, to cause a
cooler part receiving the excess IR to
cool further, violates
radiative transfer principles and / or the Second Law.
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).
In general: even if the stratosphere as a whole cools (in terms of a decrease in total flux going out, to balance radiative forcings + radiative response from below), this doesn't necessarily mean cooling occurs throughout; there could be some portions that war
In general: even if the stratosphere as a whole
cools (
in terms of a decrease in total flux going out, to balance radiative forcings + radiative response from below), this doesn't necessarily mean cooling occurs throughout; there could be some portions that war
in terms of a decrease
in total flux going out, to balance radiative forcings + radiative response from below), this doesn't necessarily mean cooling occurs throughout; there could be some portions that war
in total flux going out, to balance
radiative forcings +
radiative response from below), this doesn't necessarily mean
cooling occurs throughout; there could be some portions that warm.
In the tugging on the temperature profile (by net radiant heating /
cooling resulting from
radiative disequilibrium at single wavelengths) by the absorption (and emission) by different bands, the larger - scale aspects of the temperature profile will tend to be shaped more by the bands with moderate amounts of absorption, while finer - scale variations will be more influenced by bands with larger optical thicknesses per unit distance (where there can be significant emission and absorption by a thinner layer).
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).
«Above about 50 km
in altitude, the ozone heating effect diminishes
in importance because of falling ozone concentrations, and
radiative cooling becomes relatively more important.
@RI: More CO2 raises the optical depth (
in layman speak, the top of the GHG
radiative «fog» above which IR is free to radiate to space and
cool).
The net effect of
radiative gases
in our atmosphere is
cooling at all concentrations above 0.0 ppm.
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.
More CO2 raises the optical depth (
in layman speak, the top of the GHG
radiative «fog» above which IR is free to radiate to space and
cool).
It is virtually certain that anthropogenic aerosols produce a net negative
radiative forcing (
cooling influence) with a greater magnitude
in the NH than
in the SH.
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.
warrenlb, nothing at that site supports your denial of the S - B basis of climate alarm, supports your neglect of the significance of rapid collisional vs. slow
radiative decay of CO2 *
in the troposphere, or supports your dismissal of CO2 *
radiative decay as the source of stratospheric
cooling.
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.
In the tropics net
radiative influx is negative, i.e. radiation
cools the atmospheric column.
Absent
radiative warming it will still warm through conduction and convection and it will
cool radiatively because all matter above absolute zero radiates and I'm pretty sure the nitrogen
in our atmosphere is matter and it has a temperature above absolute zero therefore it radiates a continuous black body spectrum characteristic of that temperature.
The climate sensitivity value tells us how much the planet will warm or
cool in response to a given
radiative forcing change.