In many Mediterranean climates there is a strong diurnal character to daily temperatures in the warm summer months, due to the great loss of ultraviolet
radiation from the sun at night.
Atmospheres absorb incident
radiation from the Sun at all altitudes, and radiate it away until they cool to the predetermined thermal profile.
Not exact matches
Darin Toohey, a professor
at the University of Colorado's atmospheric and oceanic sciences department and one of the paper's authors, says black carbon absorbs shortwave
radiation from the
sun, causing the atmosphere to heat up.
It's found out that natural UV
radiation from the
sun may increase by about 25 %
at the beach, as it is reflected by the water and yellow sand.
The UV index is an international standard measurement of how strong the ultraviolet (UV)
radiation from the
sun is
at a particular place on a particular day.
And while ozone high in the atmosphere helps shield Earth
from the
sun's ultraviolet
radiation,
at ground level, it mixes with fine particulates to form breath - choking smog.
This is where
radiation from distant stars is brought to a focus by the
Sun's gravitational field, which would allow a visiting probe to resolve objects
at the centre of...
The gauntlet Juno ran
at Jupiter held many chances for catastrophe: The spacecraft might have been knocked out by intense magnetic fields (
at that distance, 20 times stronger than Earth's), ionizing
radiation (a total dose of 265 rads — more than enough to kill a human being), dust particles
from Jupiter's rings (
from which the main engine was completely unshielded) or loss of power if the solar arrays were unable to reorient to the
sun.
Mark Loeffler
at Northern Arizona University irradiated ammonium hydrosulphide, commonly found in Jupiter's atmosphere, with high - energy protons that mimic
radiation coming
from the
sun.
The
Sun's
radiation pressure and solar wind accelerate materials away
from the comet's head
at differing velocities according to the size and mass of the materials.
A dog's fur is quite effective
at preventing the
sun's
radiation from reaching his skin.
Over time, the
sun bleached away the color, leaving behind ghostly impressions, the brightest in the center where the glass of the skylight shone the light of the
sun most directly, fading along the sides where it cast in
at angles, and dimmest along the edges where the fabric was concealed
from the
sun's
radiation.
The stratosphere absorbs short wave (UV)
radiation from the
sun but is not hot enough to radiate much
at short wavelengths.
The paragraph in the OP you quote
from as well as the one above it in full are saying that the ice age cycles result
from the Earth's changing orbit round the
sun which creates changes in the «incoming solar
radiation (insolation)
at high latitudes» (Roe (2006) PDF).
Actually, though, most of the OLR originates
from below the tropopause (can get up around 18 km in the tropics, generally lower)-- with a majority of solar
radiation absorbed
at the surface, a crude approximation can be made that the area emitting to space is less than 2 * (20/6371) * 100 % ~ = 0.628 % more than the area heated by the
sun, so the OLR per unit area should be well within about 0.6 % of the value calculated without the Earth's curvature (I'm guessing it would actually be closer to if not less than 0.3 % different).
Now, when the energy received directly
from the
Sun at the surface of Venus is less than 10 % of what we receive on Earth, then there is less than 10 % coming back as back
radiation — far less in fact.
Waters
at this depth can not be warmed directly by the
sun or greenhouse effect as solar
radiation penetrates only to 100 metres depth, while infra - red
radiation from the greenhouse effect can only warm the immediate surface «skin» of the ocean.
Although only 1 percent of the
sun's energy is emitted
at ultraviolet wavelengths between 200 and 300 nanometers, the decrease in this
radiation from 1 July 1981 to 30 June 1985 accounted for 19 percent of the decrease in the total irradiance over the same period.»
Total solar irradiance - The amount of solar
radiation received outside the Earth's atmosphere on a surface normal to the incident
radiation, and
at the Earth's mean distance
from the
Sun.
No publication discusses a greenhouse effect specifically
at the poles, so don't bother me with links to all the «runaway greenhouse» garbage (which I've studied for thousands of hours) because there's only 1W / m ^ 2 going in
from the
Sun, and so no more coming out into the atmosphere, and so no more coming down again as back
radiation.
At one point Dr. Chu thought that painting roofs and other structures white would help reflect the
sun's
radiation and save the nation and the world
from global warming.
Memphis October 14, 2012
at 5:24 pm Myrrh's basic problem is that he doesn't seems to understand that
radiation from the
sun warms the earth.
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.
Memphis October 17, 2012
at 10:56 am Myrr when are you going to realise that NOBODY thinks that only visible
radiation comes
from sun.
Memphis October 16, 2012
at 1:43 am Myrrh So you are nowfinally going to stop pretending that
radiation from the
sun can not warm us?
The latter gives rise to a strong negative feedback between the surface temperature Ts and the temperature of «absolutely black body» Tbb, which is determined by the solar
radiation S reaching the Earth's surface
at its distance
from the
Sun.
This measure is available for the US
from the BEST data set... The reconfirmation now of a strong
sun - temperature relation based specifically upon the daytime temperature maxima adds strong and independent scientific weight to the reality of the
sun - temperature connection... This suggests strongly that changes in solar
radiation drive temperature variations on
at least a hemispheric scale... Close correlations like these simply do not exist for temperature and changing atmospheric CO2 concentration.»
This must result in about 85 times as much infrared
radiation from the
Sun,
at 3.3 microns wavelength, being sent back into space by the absorption and re-
radiation from methane molecules in the upper atmosphere as could be re-radiated into the lower atmosphere for infrared
radiation sourced
from the warmed Earth.
Radiation comes in
from the
sun (solar
radiation at short wavelengths), and every body radiates according to its temperature (proportional to the fourth power of absolute temperature), so that on Earth we, and the surface and atmosphere radiate
at infrared wavelengths.
The
radiation situation
from the outer shell is complex because the
sun only heats one half
at a time and the flux is not uniform.
The temperature climbs much higher (than on Earth) so long as the lunar surface is basking in the
sun, and drops much lower while the back
radiation from outer space is only
at 4 kelvins.
northern Scandinavia) cloudy days in November and December are typically warmer than cloud - free days because the Earth's surface has a net
radiation loss
at the time (i.e. outgoing heat loss exceeds
radiation received
from the
sun).
Testimony to this assumption is the term that has been employed for more than a century to describe the
radiation in all wavelengths received
from the
Sun: the so - called «solar constant,» whose value
at the mean
Sun - Earth distance is a little over 1 1/3 kilowatts per square meter of surface.
The increase of CO2 gives both the higher value of Tl due to the increased absorption of the outgoing surface
radiation and the higher value of T after the
radiation from the
Sun is «switched off»
at the evening.
If the
radiation into space is
at a lower rate than the arrival of radiant energy
from the
sun the planet heats up.
Now the
sun would be expected to set up an undisturbed gradient
from cold
at the bottom to warm
at the top but it does not because upward
radiation from the surface plus energy drawn upwards by evaporation
at the surface creates a layer 1 mm deep near the surface (the subskin) which is 0.3 C cooler than the water below it.
If the
Sun were a massive ball of hydrogen, heated by a H - fusion reactor
at its core, then changes
at the solar core would be delayed by about 30 My (million years), the diffusion time for
radiation from the core of the
Sun to its surface [See William A. Fowler, «What cooks with solar neutrinos?»
However, the point is simply this: As long as you have an IR - absorbing atmosphere that is
at a nonzero temperature, the earth's surface will have to be
at a warmer temperature (in order to radiate away the energy that it receives
from the
sun) than it would be if the atmosphere did not absorb any of the IR
radiation that the earth emits.
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.
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.
Otherwise, such a hypothesis does not even satisfy the First Law of Thermodynamics (basically, conservation of energy): Without substances in the atmosphere that absorb terrestrial
radiation, the earth's surface
at its present temperature would be emitting back out into space way more energy than it receives
from the
sun and hence would rapidly cool down.
Conclusion, CO2 (and its «back
radiation») makes LITTLE difference, because
at the same level of pressure on BOTH planets, the only thing that seems to matter is planetary distance
from the
sun.
In the experiment, cosmic
radiation was passed through a large reaction chamber containing a mixture of lower atmospheric gases
at realistic concentrations that was exposed to ultraviolet
radiation from lamps that mimic the action of the
sun's rays.
At sunrise, the sun's angle is 0 degrees, at noon 90 degrees, at sunset 0 degrees again, so the amount of radiation the equator is getting is 1368 watts / meter ^ 2 cos x. Integrate that cos x from sunrise, pi / 2, to sunset, - pi / 2, and you get 2 / pi for the average radiatio
At sunrise, the
sun's angle is 0 degrees,
at noon 90 degrees, at sunset 0 degrees again, so the amount of radiation the equator is getting is 1368 watts / meter ^ 2 cos x. Integrate that cos x from sunrise, pi / 2, to sunset, - pi / 2, and you get 2 / pi for the average radiatio
at noon 90 degrees,
at sunset 0 degrees again, so the amount of radiation the equator is getting is 1368 watts / meter ^ 2 cos x. Integrate that cos x from sunrise, pi / 2, to sunset, - pi / 2, and you get 2 / pi for the average radiatio
at sunset 0 degrees again, so the amount of
radiation the equator is getting is 1368 watts / meter ^ 2 cos x. Integrate that cos x
from sunrise, pi / 2, to sunset, - pi / 2, and you get 2 / pi for the average
radiation.
Multiple sources suggest that the energy
from BB
radiation at ~ 5700 K (eg
from the
sun) will be ~ 10 UV, ~ 40 % visible, ~ 45 % IR - A & IR - B (0.7 — 3 um), and ~ 5 % «thermal IR» (3 um and longer).
The «back
radiation» component
from GHG's and clouds is only about 140 W / m ^ 2 while the peak solar input exceeds 1000 W / m ^ 2
at the equator and even the mid morning
Sun exceeds 300 W / m ^ 2 in most places across the planet.