We need to find an equation that allows factors other than mass, gravity and insolation to affect V without affecting T because according to the Gas Laws T is determined only by the amount of KE needed to keep the mass of the atmosphere off the surface at a given height over and above that required for top of
atmosphere radiative balance.
If anything else tries to disturb the temperature (or more accurately energy content) derived from those 3 characteristics alone then all one sees is a change in circulation adjusting the flow of energy throughput to keep top of
atmosphere radiative balance stable.
No: that is the beauty of using top of
atmosphere radiative balance data — it automatically reflects the flow of heat into the ocean, so thermal inertia of the oceans is irrelevant to the estimate of equilibrium climate sensitivity that it provides, unlike with virtally all other instrumental methods.
Not exact matches
Surface
radiative energy budget plays an important role in the Arctic, which is covered by snow and ice: when the
balance is positive, more solar radiation from the Sun and the Earth's
atmosphere arrives on the Earth's surface than is emitted from it.
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).
Earth's energy
balance In response to a positive
radiative forcing F (see Appendix A), such as characterizes the present - day anthropogenic perturbation (Forsteret al., 2007), the planet must increase its net energy loss to space in order to re-establish energy
balance (with net energy loss being the difference between the outgoing long - wave (LW) radiation and net incoming shortwave (SW) radiation at the top - of -
atmosphere (TOA)-RRB-.
It is the reduced amount of radiation leaving the top of the
atmosphere that changes the earth's
balance of heat, and therefore defines the «direct
radiative forcing» caused by doubling CO2.
But, I think that is likely to affect weather patterns much more than the
radiative balance at the top of the
atmosphere.
For example, we could describe climate change primarily in terms of the physical processes: carbon emissions, the
radiative balance of the
atmosphere, average temperatures, and impacts on human life and ecosystems.
A vast array of thought has been brought to bear on this problem, beginning with Arrhenius» simple energy
balance calculation, continuing through Manabe's one - dimensional
radiative - convective models in the 1960's, and culminating in today's comprehensive
atmosphere - ocean general circulation models.
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
radiative balance over equilibrium timescales — the heat released by raindrop formation will locally warm the
atmosphere, but it takes time for the atmospheric circulation to average this out.
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.
This must warm the
atmosphere in order for
radiative balance to be maintained.
Then, if compositional changes occur, involving changes in the net
radiative balance of the entire
atmosphere the climate zones will shift as the
atmosphere has to work more hard or less hard to maintain top of
atmosphere energy
balance.
Syllabus: Lecture 1: Introduction to Global Atmospheric Modelling Lecture 2: Types of Atmospheric and Climate Models Lecture 3: Energy
Balance Models Lecture 4: 1D
Radiative - Convective Models Lecture 5: General Circulation Models (GCMs) Lecture 6: Atmospheric Radiation Budget Lecture 7: Dynamics of the
Atmosphere Lecture 8: Parametrizations of Subgrid - Scale Physical Processes Lecture 9: Chemistry of the
Atmosphere Lecture 10: Basic Methods of Solving Model Equations Lecture 11: Coupled Chemistry - Climate Models (CCMs) Lecture 12: Applications of CCMs: Recent developments of atmospheric dynamics and chemistry Lecture 13: Applications of CCMs: Future Polar Ozone Lecture 14: Applications of CCMs: Impact of Transport Emissions Lecture 15: Towards an Earth System Model
For instance,
radiative transfer models (measuring heat
balance) are quite well verified, and accurately predict the rise in the temperature (and hence energy) of the
atmosphere as the CO2 level increases.
To evaluate the global effects of aerosols on the direct
radiative balance, tropospheric chemistry, and cloud properties of the earth's
atmosphere requires high - precision remote sensing that is sensitive to the aerosol optical thickness, size istribution, refractive index, and number density.
«
Radiative forcing is a measure of the influence a factor has in altering the
balance of incoming and outgoing energy in the Earth -
atmosphere system and is an index of the importance of the factor as a potential climate change mechanism.
But on larger scales (both in space and time) the earth is a planet of our local star; the sun is our only source of (purely
radiative) energy; we have an
atmosphere which clearly operates to reduce diurnal variations in temperature (which on black body basis would otherwise be huge, on human scale) and the
radiative budget must always be exactly in
balance.
His model of the
atmosphere was advanced for the time, but he did consider the
radiative balance at the surface, whereas we now consider that this is flawed and the
balance at the top of the
atmosphere (TOA) is more appropriate.
Heat melts Rock like ice and this thuderhead of magma rises high in the geo - sky to bring heat to sea level, thus
balancing the core «s heat output when it's
radiative rate is slowed by the R - value of the gas
atmosphere.
He does not look at the top of
atmosphere balance to see how it remains unbalanced under his modified state, so he hasn't looked at
radiative equilibrium, but some kind of transient response, as far as I can tell.
«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.»
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.
Yes, inert gases do absorb incident Solar radiation in the UV and visible spectra, so the
atmosphere warms to
radiative balance, and the temperature at the base of the
atmosphere determines (or «supports») the surface temperature.
As you point out, there is no question that adding CO2 to the
atmosphere affects what I call the «
radiative balance» for want of a better term.
Thus with GHGs in an
atmosphere the circulation can slow down because more of its job of maintaining top of
atmosphere energy
balance is done for it by those
radiative gases.
If all farm animals disappeared, tomorrow, we could not measure the impact on the
radiative balance of the
atmosphere.
The gas constant therefore sets the volume of
atmosphere needed to leave the surface temperature at the level required to both support the
atmosphere AND achieve
radiative balance at the top of the
atmosphere.
T represents the amount of energy available from all sources to maintain the constant flow that keeps the
atmosphere off the surface AND achieves
radiative balance at the top of the
atmosphere.
Additionally, physical phenomena and processes, driven by (1) the net energy that reaches the
atmosphere and surface, (2) redistribution of energy content already within the systems, and (3) activities of human kind, directly affect the
radiative energy
balance from which the hypothesis was developed.
Is the mathematical solution to the fluid flow over the airplane wing simpler than the mathematical solution to the instantaneous
radiative - convective
balance in the
atmosphere?
Aerosols not only affect the
radiative balance at the top of the
atmosphere but also exert a forcing on the hydrological cycle (e.g., Ramanathan et al., 2001a).
The amount of greenhouse gases in the
atmosphere combined with other factors determine the
radiative balance, and / or temperature at which relative thermal equilibrium for a planet occurs based on these factors.
2) Failing to acknowledge that natural variations in the effective radiating height of the
atmosphere occur all the time as a result of the ever changing
balance between different non
radiative processes within the
atmosphere.
In the absence of absorption of terrestrial radiation by the
atmosphere (and with the other caveats about still having the same albedo and such), that average temperature would have to be 255 K at the surface because of
radiative balance and then the temperature would decrease with height at the lapse rate from there.
E.g., given that the net
radiative balance at the top of the
atmosphere remains negative, which certainly indicates continued warming, Trenberth's studies suggest deep ocean uptake of most of the recent heating.
If the
atmosphere contained no IR - absorbing substances, then all the IR emitted by the earth's surface would escape into space and
radiative balance would dictate that the earth's average surface temperature (or really the average of emissivity * T ^ 4 where T is the absolute temperature and the emissivity of most terrestrial materials in the wavelength range of interest is very close to 1) is set by the condition that the earth must radiate as much energy as it absorbs from the sun.
Radiative balance of the earth system then sets the temperature at this level in the
atmosphere and the temperature at the surface basically follows from the lapse rate.
That is determined by consideration of the absorption of the
atmosphere of terrestrial radiation (and radiation emitted by the
atmosphere), which essentially ends up determining at what altitude the temperature has to be determined via
radiative balance between the Earth system (earth +
atmosphere) and the sun and space [which for the earth system with its current albedo is ~ 255 K].
What he shows is that a change in the
radiative balance between the surface and the
atmosphere even by a larger amount, such as 10 W / m ^ 2 would result in only a very small surface temperature change while a change in the greenhouse effect (i.e., the
radiative balance between the earth and space) by 10 W / m ^ 2 results in a much larger surface temperature change (almost 2 orders of magnitude larger if I recall correctly).
Here is a more correct way to say things: When one considers convection, the best quantity to consider is the
radiative balance at the top of the
atmosphere.
A: The volume integral (heat
balance equation) as presented in Pielke (2003) http://blue.atmos.colostate.edu/publications/pdf/R-247.pdf suggests that the changes in ocean heat storage averaged over a year are a snapshot of the
radiative imbalance at the top of the
atmosphere.
Over this five year time span, the latest observations appear to show that the top of the
atmosphere has been in an averaged state of
radiative balance.
The problem of obtaining a realistic value for the absorptivity to emissivity ratio for all the entities at Earth's surface, and in its
atmosphere, that participate in the
radiative balance is a formidable task.
Comparison with independent data, such as the top of
atmosphere (TOA)
radiative balance also provides insight (32).
However, six out of the 19 references in the paper are to Miskolczi himself and the fundamental equations brought up for energy
balance (where
radiative exchange is referenced) rely on his more lengthy 2007 paper, Greenhouse effect in semi-transparent planetary
atmospheres.
But because the
atmosphere blocks infrared, the planet must emit more infrared into the
atmosphere, so that
radiative balance is maintained.