The desert air is likewise
heated at altitude, by latent heat.
Not exact matches
Traditional old varieties of arabica coffee don't grown
at this
altitude with the
heat and humidity.
In a study supported by the Office of Biological and Environmental Research's Atmospheric System Research program, scientists used the Community Atmosphere Model version 4 to examine the relative importance of
heating at different
altitudes to the MJO.
At higher
altitudes it is relatively harder to retain this energy as more
heat is lost to space.
At low
altitudes, about half the energy of such a bomb is released in the air blast, 35 percent as
heat and 15 percent as nuclear radiation.
Normally, titanium oxide in the atmospheres of hot Jupiters absorbs light and reradiates it as
heat, making the atmosphere grow warmer
at higher
altitudes.
When the lander jettisons its
heat shield
at a 1 - kilometer
altitude, data transmission switches from an antenna on the shield to one on the lander.
As the satellite dips down into the atmosphere, STATIC identifies the cold ionosphere
at closest approach and subsequently measures the
heating of this charged gas to escape velocities as MAVEN rises in
altitude.
Hours outdoors in
heat humidity, or now
at altitude in the mountains strong sunshine can be tough on an active girl's skin.
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The change in radiation balance is more
heating of the oceans
at one side (specifically high in the subtropics, as expected), but more
heat released
at higher
altitudes, thus somewhere acting as a net negative feedback to higher sea surface temperatures.
In the absence of solar
heating, there is an equilibrium «skin temperature» that would be approached in the uppermost atmosphere (above the effective emitting
altitude) which is only dependent on the outgoing longwave (LW) radiation to space in the case where optical properties in the LW part of the spectrum are invariant over wavelength (this skin temperature will be colder than the temperature
at the effective emitting
altitude).
Now, I think it was in 1956 that atmospheric physicist and sometimes - weapons designer Gilbert Plass (who needed to know about IR to fire
heat - seeking missiles up the tailpipes of jet fighter
at high
altitude) noted that CO2 in the upper troposphere could block the escape of IR to space: The Carbon Dioxide Theory of Climate Change, Gilbert Plass (1955)(abstract) In the full paper, available
at the above link, Plass spells out the previous notion which his research overturned:
In 1896 Swedish chemist and Nobel laureate Svante Arrhenius used Langley's bolometer to measure the
heat from the Moon
at various
altitudes above the horizon in order to estimate the dependence of atmospheric
heat trapping on amount of water vapor and CO2 along the line of sight to the Moon, a much longer path near the horizon than
at 45 degrees.
And there was NO effect on temperatures
at lower
altitudes over that time, even from this massive
heating event where about 20 % of the entire atmosphere warmed.
The effects of very short wavelength UV on photochemical reactions in the stratosphere leading to
heating at very high
altitudes is something that is under appreciated in the climate science community but the meterologists would have likely let them know when to look for these affects.
orgConsider David Keith's idea, presented in an article published in the Proceedings of the National Academy of Sciences, of deploying a fleet of thermostatically self - regulating, mirror - coated, nanotechnology flying saucers, which would be programmed to assemble
at the latitude and
altitude appropriate to reflect back the precise amount of sun light necessary to offset the global
heating associated with human - caused CO2 emissions.
When clouds condense back to water they give up the Latent
Heat of Vaporisation at that altitude and the radiant energy is closer to top of atmosphere to pass to that great heat sink in the sky: Sp
Heat of Vaporisation
at that
altitude and the radiant energy is closer to top of atmosphere to pass to that great
heat sink in the sky: Sp
heat sink in the sky: Space.
That fluctuation is amplified by land surface temperatures in the same latitude band of about the same area, because the land surface temperatures are
at a higher average
altitude with a lower average specific
heat capacity and the (Tmax + Tmin) / 2 method of determining «average» amplifies the variance.
«Classic thermodynamics», tempterrain include the original Clausius statement of the Second Law of Thermodynamics, which only related to
heat transfer
at the same
altitude, so that there was no change in potential energy.
CO2 radiation
at high above is cold (depends on
altitudes, latitudes, and longitudes, say from 0degreeC to -60 degreeC) can not radiate net
heat back to the Earth which is
at a higher temperature.
It is
heated at the bottom and it loses its
heat in
altitude.
In order to force a temperature decline
at the adiabatic lapse rate, there must be some combination of both
heating from below and cooling from above that would otherwise drive the rate of cooling with
altitude beyond the effective lapse rate.
Does not your thought experiment fail, because most of the molecules in the atmosphere are all
at the same
heat (kinetic energy), while the difference in temperature with
altitude (on a thermometer) is simply an effect of the number of molecules you meet (pressure and density).
The black soot soaks up
heat and when the snow gets dirty it melts more quickly and,
at such high
altitudes, the effect is magnified.
Since warm air is being moved poleward
at low
altitudes, the wind flow is no longer associated with the direct
heat engine of the Hadley cell.
Thus the warm wire
at the top of the collumn (
at say +30 oc) can not «
heat the air»
at high
altitude, because the individual molecules
at altitude are already
at something like +30 oc (in terms of their individual kinetic energy)..
That might give a bit of pause for thought about density and its effect on the ability of air packets
at different
altitudes to retain the
heat of the Sun.
If the atmosphere of Venus became truly opaque to incoming solar radiation
at some
altitude above the surface, the atmosphere below that point would be isothermal assuming no
heat input to the surface from the core of the planet.
An atmosphere in which
heated gases can rise to
altitude, but can not lose energy and descend runs far hotter than an atmosphere in which energy loss
at altitude can occur.
-- convective circulation in the troposphere is driven by
heating at low
altitude and energy loss
at high
altitude.
However, it is much easier to figure out what happens when you add more radiative gases to an atmosphere that already has them: And, the answer is that it increases the IR opacity of the atmosphere, which increases the
altitude of the effective radiating level and hence means the emission is occurring from a lower - temperature layer, leading to a reduction of emission that is eventually remedied by the atmosphere
heating up so that radiative balance
at the top - of - the - atmosphere is restored.
The mechanism which prevents H2O vapour from overheating the world is cloud cover, due to the easily provable fact that
heated moist air rises, expanding, cooling and condensing into cloud cover in the rarified air
at higher
altitudes.
Studying Chinese summer thunderclouds the researchers found that an increase in aerosols led to larger and more persistent convective cloud systems, with larger anvils
at several kilometers of
altitude that may reflect more sunlight, but trap even more
heat — as their high - resolution model showed.
The outflow temperature does not depend just on the local state but rather on conditions throughout the tropics, since the tropical general circulation redistributes
heat efficiently
at high
altitudes.
By seeing for the first time how these eddies accelerate the jet streams
at two different
altitudes, scientists found the eddies were weak
at the higher
altitudes where previous researchers had found that most of the sun's
heating occurs.
This
heating of the air «from above» explains the fact that the lapse rate is between - 5 K / km to — 8 K / km depending on the exact value of Ch
at the place,
altitude and time considered and not the adiabatic lapse rate of -9.8 K / km.
(Any higher and they start to suffer stratospheric
heating due to the vertical temperature profile reversing
at the tropopause — the lapse rate changes sign and the air gets warmer instead of colder with
altitude.)
Convection
at lower
altitudes will punch through the thicker lower layers allowing a much more direct path for radiative effects to become efficient and unhindered in delivering the
heat to space.
The crowd of government - financed alarmists artificially introduced this signal by excluding Canadian, Siberian, high -
altitude and other «inconvenient» measurements from data sets, by various «adjustments» fitting the desired outcome, by placing meteorological stations on airport tarmacs,
at air conditioners» exhausts and in other artificially
heated places, and by blatantly omitting, negating, and even reversing (as in prof. Mann's case) actual results.
At higher
altitudes radiation
heat transfer becomes more significant and OLR is emitted and the parcel cools.
By looking
at atmospheric profiles above Gan Island, they could see how clouds and moisture changed which
altitudes were
heated over the course of each cycle of the MJO.
A drying of the atmosphere — that the researchers note — takes place in the subtropical subsidence zone (the 30 degrees latitude) but expands towards the 30 - 45 degrees latitude — Earth's Meditteranean climates, where their model suggests net cloud cover would actually decrease most (see dotted line in first image in this article,
at top)-- most notably around 500 hPa (roughly translating to a height of around 5 kilometers of
altitude in the troposphere) decreasing albedo and increasing solar
heat absorption, therefore net climate warming.
To that you answer if the temperature ever starts to rise, due to say volcanic
heat, or upwelling to water's surface, the
heat is immediately removed by the power of evaporation as infrared - resonant gases chug
heat straight up through the atmospheric mix to belch it out radiatively
at higher
altitude; while simultaneously dragging other, non-infrared resonant gases upward with them, to also dump THEIR
heat radiatively, from a higher position than they would have, had the refrigerative cycle not taken place.
One of the key insights in Lindzens 2001 adaptive iris hypothesis, the others being the latent
heat left
at altitude upon water vapor condensation thanks to convection and the temperature lapse rate, and the lowering of humidity (so water vapor feedback) from the resulting precipitation.
The basic idea was that reducing the difference in temperature between the ocean (
at some fixed depth below the skin) and the atmosphere (
at some fixed low
altitude) through warming the atmosphere reduces the
heat loss.
However, the large difference in dry vs wet lapse rate is not due to the presence of water vapor changing the average Cp, but instead due to the progressive condensation of vapor to liquid or solid
at altitude (
heat of condensation being released).
He doesn't mention that the radiosonde datasets are regarded as questionable for climatological purposes
at higher
altitude due to radiative
heating / cooling effects on the instrument packages.
I just tried jotting down, step by step, a sequence of events beginning with evaporation from the sea surface, absorption of latent
heat, subsequent condensation
at altitude into opaque liquid droplets and the release of selfsame latent
heat.