Guest Post by Willis Eschenbach
A couple of apparently related theories have been making the rounds lately. One is by Nikolov and Zeller (N&Z), expounded here and replied to here on WUWT. The other is by Hans Jelbring, discussed at Tallblokes Talkshop. As I understand their theories, they say that the combination of gravity plus an atmosphere without greenhouse gases (GHGs) is capable of doing what the greenhouse effect does—raise the earth at least 30°C above what we might call the “theoretical Stefan-Boltzmann (S-B) temperature.”
So what is the S-B temperature, theoretical or otherwise?
A curious fact is that almost everything around us is continually radiating energy in the infrared frequencies. You, me, the trees, the ocean, clouds, ice, all the common stuff gives off infrared radiation. That’s how night-vision goggles work, they let you see in the infrared. Here’s another oddity. Ice, despite being brilliant white because it reflects slmost all visible light, absorbs infrared very well (absorptivity > 0.90). It turns out that most things absorb (and thus emit) infrared quite well, including the ocean, and plants (see Note 3 below). Because of this, the planet is often treated as a “blackbody” for IR, a perfect absorber and a perfect emitter of infrared radiation. The error introduced in that way is small for first-cut calculations.
The Stefan-Boltzmann equation specifies how much radiation is emitted at a given temperature. It states that the radiation increases much faster than the temperature. It turns out that radiation is proportional to absolute temperature to the fourth power. The equation, for those math inclined, is
Radiation = Emissivity times SBconstant times Temperature^4
where the Stefan-Boltzmann constant is a tiny number, 0.0000000567 (5.67E-8). For a blackbody, emissivity = 1.
This “fourth-power” dependence means that if you double the absolute temperature (measured in kelvins), you get sixteen (2^4) times the radiation (measured in watts per square metre, “W/m2”). We can also look at it the other way, that temperature varies as the fourth root of radiation. That means if we double the radiation, the temperature only goes up by about 20% (2^0.25)
Let me call the “theoretical S-B temperature” the temperature that an evenly heated stationary blackbody planet in outer space would have for a given level of incoming radiation in W/m2. It is “theoretical”, because a real, revolving airless planet getting heated by a sun with the same average radiation will be cooler than that theoretical S-B temperature. We might imagine that there are thousands of mini-suns in a sphere around the planet, so the surface heating is perfectly even.
Figure 1. Planet lit by multiple suns. Image Source.
On average day and night over the planetary surface, the Earth receives about 240 W/m2 of energy from the sun. The theoretical S-B temperature for this amount of radiation (if it were evenly distributed) is about -18°C, well below freezing. But instead of being frozen, the planet is at about +14°C or so. That’s about thirty degrees above the theoretical S-B temperature. So why isn’t the planet a block of ice?
Let me take a short detour on the way to answering that question in order to introduce the concept of the “elevator speech” to those unfamiliar with the idea.
The “elevator speech” is simply a distillation of an idea down to its very basics. It is how I would explain my idea to you if I only had the length of an elevator ride to explain it. As such it has two extremely important functions:
1. It forces me to clarify my own ideas on whatever I’m discussing. I can’t get into handwaving and hyperbole, I can’t be unclear about what I’m claiming, if I only have a few sentences to work with.
2. It allows me to clearly communicate those ideas to others.
In recent discussions on the subject, I have been asking for that kind of “elevator speech” distillation of Jelbring’s or Nikolov’s ideas, so that a) I can see if whoever is explaining the theory really understands what they are saying and, if so, then b) so that I can gain an understanding of the ideas of Jelbring or Nikolov to see if I am missing something important.
Let me give you an example to show what I mean. Here’s an elevator speech about the greenhouse effect:
The poorly-named “greenhouse effect” works as follows:
• The surface of the earth emits energy in the form of thermal longwave radiation.
• Some of that energy is absorbed by greenhouse gases (GHGs) in the atmosphere.
• In turn, some of that absorbed energy is radiated by the atmosphere back to the surface.
• As a result of absorbing that energy from the atmosphere, the surface is warmer than it would be in the absence of the GHGs.
OK, that’s my elevator speech about why the Earth is not a block of ice. Note that it is not just saying what is happening. It is saying how it is happening as well.
I have asked, over and over, on various threads, for people who understand either the N&Z theory or the Jelbring theory, to give me the equivalent elevator speech regarding either or both of those theories. I have gotten nothing scientific so far. Oh, there’s the usual handwaving, vague claims of things like ‘the extra heat at the surface, is just borrowed by the work due to gravity, from the higher up regions of the atmosphere‘ with no mechanism for the “borrowing”, that kind of empty statement. But nothing with any meat, nothing with any substance, nothing with any explanatory value or scientific content.
So to begin with, let me renew my call for the elevator speech on either theory. Both of them make my head hurt, I can’t really follow their vague descriptions. So … is anyone who understands either theory willing to step forward and explain it in four or five sentences?
But that’s not really why I’m writing this. I’m writing this because of the claims of the promoters of the two theories. They say that somehow a combination of gravity and a transparent, GHG-free atmosphere can conspire to push the temperature of a planet well above the theoretical S-B temperature, to a condition similar to that of the Earth.
I hold that with a transparent GHG-free atmosphere, neither the hypothetical “N&Z effect” nor the “Jelbring effect” can possibly raise the planetary temperature above the theoretical S-B temperature. But I also make a much more general claim. I hold it can be proven that there is no possible mechanism involving gravity and the atmosphere that can raise the temperature of a planet with a transparent GHG-free atmosphere above the theoretical S-B temperature.
The proof is by contradiction. This is a proof where you assume that the theorem is right, and then show that if it is right it leads to an impossible situation, so it cannot possibly be right.
So let us assume that we have the airless perfectly evenly heated blackbody planet that I spoke of above, evenly surrounded by a sphere of mini-suns. The temperature of this theoretical planet is, of course, the theoretical S-B temperature.
Now suppose we add an atmosphere to the planet, a transparent GHG-free atmosphere. If the theories of N&K and Jelbring are correct, the temperature of the planet will rise.
But when the temperature of a perfect blackbody planet rises … the surface radiation of that planet must rise as well.
And because the atmosphere is transparent, this means that the planet is radiating to space more energy than it receives. This is an obvious violation of conservation of energy, so any theories proposing such a warming must be incorrect.
Q.E.D.
Now, I’m happy for folks to comment on this proof, or to give us their elevator speech about the Jelbring or the N&Z hypothesis. I’m not happy to be abused for my supposed stupidity, nor attacked for my views, nor pilloried for claimed errors of commission and omission. People are already way too passionate about this stuff. Roger Tattersall, the author of the blog “Tallbloke’s Talkshop”, has banned Joel Shore for saying that the N&Z hypothesis violates conservation of energy. Roger’s exact words to Joel were:
… you’re not posting here unless and until you apologise to Nikolov and Zeller for spreading misinformation about conservation of energy in their theory all over the blogosphere and failing to correct it.
Now, I have done the very same thing that Joel did. I’ve said around the web that the N&Z theory violates conservation of energy. So I went to the Talkshop and asked, even implored, Roger not to do such a foolish and anti-scientific thing as banning someone for their scientific views. Since I hold the same views and I committed the same thought-crimes, it was more than theoretical to me. Roger has remained obdurate, however, so I am no longer able to post there in good conscience. Roger Tallbloke has been a gentleman throughout, as is his style, and I hated to leave. But I did what Joel did, I too said N&Z violated conservation of energy, so in solidarity and fairness I’m not posting at the Talkshop anymore.
And more to the point, even if I hadn’t done what Joel did, my practice is to never post at or even visit sites like RealClimate, Tamino’s, and now Tallbloke’s Talkshop, places that ban and censor scientific views. I don’t want to be responsible for their page views counter to go up by even one. Banning and censorship are anathema to me, and I protest them in the only way I can. I leave them behind to discuss their ideas in their now cleansed, peaceful, sanitized, and intellectually sterile echo chamber, free from those pesky contrary views … and I invite others to vote with their feet as well.
But I digress, my point is that passions are running high on this topic, so let’s see if we can keep the discussion at least relatively chill …
TO CONCLUDE: I’m interested in people who can either show that my proof is wrong, or who will give us your elevator speech about the science underlying either N&K or Jelbring’s theory. No new theories need apply, we have enough for this post. And no long complicated explanations, please. I have boiled the greenhouse effect down to four sentences. See if you can match that regarding the N&K or the Jelbring effect.
w.
NOTE 1: Here’s the thing about a planet with a transparent atmosphere. There is only one object that can radiate to space, the surface. As a result, it is constrained to emit the exact amount of radiation it absorbs. So there are no gravity/atmospheric phenomena that can change that. It cannot emit more or less than what it absorbs while staying at the same temperature, conservation of energy ensures that. This means that while the temperature can be lower than the theoretical S-B temperature, as is the case with the moon, it cannot be more than the theoretical S-B temperature. To do that it would have to radiate more than it is receiving, and that breaks the conservation of energy.
Once you have GHGs in the atmosphere, of course, some of the surface radiation can get absorbed in the atmosphere. In that case, the surface radiation is no longer constrained, and the surface is free to take up a higher temperature while the system as a whole emits the same amount of radiation to space that it absorbs.
NOTE 2: An atmosphere, even a GHG-free atmosphere, can reduce the cooling due to uneven insolation. The hottest possible average temperature for a given average level of radiation (W/m2) occurs when the heating is uniform in both time and space. If the total surface radiation remains the same (as it must with a transparent atmosphere), any variations in temperature from that uniform state will lower the average temperature. Variations include day/night temperature differences, and equator/polar differences. Since any atmosphere can reduce the size of e.g. day/night temperature swings, even a transparent GHG-free atmosphere will reduce the amount of cooling caused by the temperature swings. See here for further discussion.
But what such an atmosphere cannot do is raise the temperature beyond the theoretical maximum average temperature for that given level of incoming radiation. That’s against the law … of conservation of energy.
NOTE 3: My bible for many things climatish, including the emissivity (which is equal to the absorptivity) of common substances, is Geiger’s The Climate Near The Ground, first published sometime around the fifties when people still measured things instead of modeling them. He gives the following figures for IR emissivity at 9 to 12 microns:
Water, 0.96 Fresh snow, 0.99 Dry sand, 0.95 Wet sand, 0.96 Forest, deciduous, 0.95 Forest, conifer, 0.97 Leaves Corn, Beans, 0.94
and so on down to things like:
Mouse fur, 0.94 Glass, 0.94
You can see why the error from considering the earth as a blackbody in the IR is quite small.
I must admit, though, that I do greatly enjoy the idea of some boffin at midnight in his laboratory measuring the emissivity of common substances when he hears the snap of the mousetrap he set earlier, and he thinks, hmmm …
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My elevator speech to fellow engineers is this: GH gasses are qualitatively like applying insulation on a hot pipe — it impedes heat-loss to the environment (outer space in earth’s case). Once applied, the pipe’s insulation surface (tropopause) is cooler than the bare pipe is (earth’s surface). So it’s losing less heat when insulated & the heated pipe surface (earth’s surface) is warmer than w/o the “insulation”.
That’s where the proposed 33K GHG rise (insulation effect) comes from — 288K (earth surface) – 255K (tropopause surface). Not a bad approximation, but valid IMO for an atmosphere w/only non-condensible GH gasses.
There, Willis… Is everything clear now?
I recently watched a Horizon program on the BBC that mentioned the ‘South Atlantic Anomaly’. A strange depression in the earths magnetic field that affected the Hubble Space telescope. If this is the case then according to the Svensmark hypothesis then surely there should be an increase in cloudiness in this area. Does anybody now whether this is the case ? An interesting little study for some enterprising research student.
Planet without atmosphere warms to S-B temperature. Energy out = energy in. Everyone happy.
Wrap planet in an atmosphere (GHG free if you wish), atmosphere provides a insulation effect, ‘slowing’ the release of the out going energy, temperature of planet rises to a sufficient level that the original energy out figure is reached.
Planet plus atmosphere give same energy out = energy in but with the planets near surface warmer than before. Everyone happy.
In both cases the energy in and out are the same, no rules broken.
Specifying which heat transport mechanism is in use and by how much does not help the basic explanation.
Hunter raised questions regarding snow as a blackbody. Between temperatures of
250 and 273 K, reasonable for snow, the emissivity is about 0.98. You’ll notice that snow around trees- picking up the infrared radiation from the tree, melts a lot faster than snow further from the trees.
Nature is not in any way influenced by the logic of argument. What may seem completely rational and logical has been shown time and time again to be wrong. If your argument describes nature, then it will have predictive power. If there exists a single case where this prediction fails, this is evidence that the argument does not describe nature, simply coincidence.
Willis, you responded to one post as valid. Your response did not mae sense to me. here is the assertion you rejected…
4. The thicker and denser the atmosphere, the higher the near surface atmospheric temperature will be.
Willis responded…
I don’t think so. The dry adiabatic lapse rate is g / Cp, where g is gravity and Cp is the specific heat of the atmosphere. The lapse rate does not vary with elevation, which means that Cp doesn’t vary with density, so I don’t see how a denser atmosphere would perforce be warmer.
—————————————
I am not certain Willis’s response makes sense to me. The lapse rate may be constant, but it is a constant VARIATION,which appears to be predicated on g and Cp. (IE, the greater the gravity, the higher the specific heat of the atmosphere) What does “specific heat emanate from? If specific heat, which is the heat capacity per unit mass of a material, then the more materials there are per volume, then the greater heat per volume. Therefore an atmosphere of more (denser) material, will have a higher specific heat content then a thinner atmosphere. The lapse rate will be the same in both atmosphers, just the starting point or temperature will be different.
What am I missing here?
More blue box replies please… Thank you.
Willis
interesting post as always.
There seems to be some confusion about the roles of conduction and convection in the GHG free atmosphere. I think the point is that when the GHG free atmosphere is ‘added’ it will take some time for the system to reach equilbrium. During this period the atmosphere will be heated by conduction and I think it therefore follows that during this period the outgoing radiation will be LESS than the incoming radiation simply because some of that energy is being used to heat the atmosphere by conduction. Once the system reaches equilibrium I think you are quite correct -incoming radiation will equal outgoing radiation. The outgoing radiation from the surface will pass through the atmosphere as if it was not there.
Roy Spencer says that in this model convection has no role to play. I would not argue with Roy. But even if there was convection all it would do is assist in raising the atmosphere to equilibrium temperature.
Willis Eschenbach listed a book as a reference. More convenient would be online sites.
Years ago, I was searching the web trying to get at least a highschool science understanding of the greenhouse effect, as opposed to heuristic handwaving,. The firs numerical site I found was the late John Daly’s site: Here’s a good link describing the greenhouse effect.
http://www.john-daly.com/miniwarm.htm
From there, it was guest papers like this,
http://www.john-daly.com/artifact.htm,
other sites like this,
http://www.geo.utexas.edu/courses/387H/Lectures/chap2.pdf
and finally links to other sites, leading to “Climate Audit”, and finally to the promised land-
“Watts Up With That?”
Willis, excellent elevator pitch!
I agree completely, as the gas, which can’t radiate or absorb, will gain energy from contact with the surface, causing the surface temperature to drop. Since the gas can’t radiate the energy away, and the surface temperature has dropped, the next contact of a gas molecule with the surface will exchange energy in the other direction. Initially, the temperature will drop, but in the steady state, the temperature of the surface will remain at the non-atmospheric level. The mass at the steady state temperature has increased, but the temperature has not. The “missing radiation” from the surface was used to increase the gas temperature to that previously enjoyed by the surface. As soon as that has be accomplished, the system is once again in equilibrium.
Michael Reed,
I believe you have made a profound point. Engineers such as myself struggle for years with expert help to understand these devilishly complex technical questions/issues. Without having gone through that, you must rely on someone who has. Find one you trust and ask him or her.
Failing that, I will answer. No, we are not. The earth has been far warmer and far cooler than now, with far higher, but not much lower, concentrations of CO2. There is no correlation between the two according to data from many sources. The “average temperature of the earth” is nearly impossible to ascertain, and we have only been recording temperature data in more than just a few places since 1851, and not accurately enough to determine whether changes mean anything. For example, climate scientists debate changes on the order of 0.01 degrees C, using data from weather thermometers accurate to +-1 degree C, obviously ridiculous. Despite this, most of them agree that the average temperature of the Earth probably has risen 0.7 degrees C since 1851! Does that seem like a lot? Not to me. Has it changed more than that and faster than that many times? Yes it has.
There, glad I could clear that up for you!
I haven’t had time to carefully read all the replies, but several comments and conclusions in the posts seem to forget one important fact.
Air cools as it rises.
Rising air is gaining gravitational potential energy and must be losing other energy. It does this by expanding and cooling. This is the physical reason behind the lapse rate. So even if we had a planet with a uniform temperature of 255 K at the surface, only the bottom layers of the atmosphere would warm to this temperature. Temperature in the the upper layers would drop off at approximately the lapse, so the “average temperature” of a transparent atmosphere will always be less than the surface temperature.
COROLLARY. The idea that “falling air will get heated by gravity as it falls” ignores the fact that gravity had equally cooled the air as it rose. If you added NEW air at the top (perhaps from a small comet hitting the earth), then this new air falling would have warming effect (at least temporarily).
**********************************
A second very minor point is that the energy balance must also include geothermal energy. On earth this is a minor effect (on the order of 1 W/m^2), so the energy emitted will be slightly larger than the energy absorbed. On the moon this would be an even smaller effect. On Jupiter, however, this is a significant effect, warming the “surface” well above the SB temperature. (http://en.wikipedia.org/wiki/Internal_heating#Gas_giants)
********************************
Finally, I want to reiterate that I agree with Willis and his overall conclusions.
I have to say, it’s pretty darn thrilling to see WUWT folks taking such an interest in thermodynamics and transport theory! There is perhaps no better subject than transport theory to unite mathematics, physics, engineering, biology, ecology, and economics. And conversely, an solid grasp of transport theory makes it far easier to appreciate these topics as aspects of a unified whole … which is perhaps why three of the greatest scientists of the 20th century were attracted to it:
(1) Albert Einstein for Brownian motion and black-body radiation,
(2) Paul Dirac for a (still largely classified) theory of U235 isotope transport in centrifuges, and
(3) John von Neumann for the computational theory of detonation waves and
boundary layer transport (H-bombs, aircraft, and missiles)
Regarding Alexander Feht’s dubious assertions, it is true that Boltzmann killed himself, and it is true too that Boltzmann faced opposition to his ideas. But opposition is very commonly encountered in science, and perhaps a more likely explanation is Boltzmann’s lifelong history of depression, worsened by grief over the unexpected death of his eldest son (from appendicitis).
On the other hand, perhaps it is well to reflect upon the celebrated opening lines of David Goodstein’s physics textbook States of Matter:
So if you should find yourself starting to feel a bit “down” reading this particular WUWT topic … then please take a break! 🙂
Only got partway thru the replies so if this has been said before ……”never mind!”.
W’s argument only applies if the absorptivity and emissivity (albedo) of the planet’s surface are identical. He is correct if his ideal atmosphere, where convection, conduction, adiabatic lapse rate (thus gravity) play no part, has zero absorptivity and emissivity. Also not stated and assumed (I assume) is that any H2O is inert, like the atmosphere, and must have zero heat of vaporization/crystallization, and absorptivity = emissivity.
If these apply W’s simplistic argument is correct and gravity cannot play a part but in the real world Willis has previously shown here that excess heat is transferred to the upper atmosphere by condensing water vapor in thunderheads and radiated into space to keep the Earth’s temp withing a narrow range. Brilliant Willis!!!!!!
Now looking at N&Z’s and HJ’s argument that gravity (adiabatic lapse rate) plays a part; the elevator explanation is: Assume that the air is dry. All other properties are the same. It warms from contact with the warmer surface. A warm bubble breaks away and rises. As it rises it cools thru expansion, radiating some of that heat energy, as long wave IR, into space or warming some of trace GHGs. (These then radiate some of that miniscule energy, as LWIR, into space as they cool.) As the cold air bubble sinks back to the ground it cools the surrounding warmer air and surface absorbing the remaining energy NOT radiated into space. So N&Z and HJ are correct; gravity plays a part in transmission of some energy into space.
Now add water vapor. As Willis explained previously, the amount of energy transferred to space thru LWIR is dramatically increased because of the large amount of energy released when the water vapor condenses into clouds, driving the clouds to ever higher altitudes and ever more efficient transmission of the released energy into space. N&Z and HJ are still correct but the overall contribution by gravity now becomes a far smaller proportion of the total heat removed, possibly insignificantly small.
BC
My roof stored negative energy last night. It was covered in frost. When the sun hit it in the morning, energy that would otherwise have heated the tiles was used up in melting the ice and evaporating the resulting wet surface.
simpleseekeraftertruth says:
January 14, 2012 at 6:10 am ,
Your description was based on the idea of an IR photon from the sun being absorbed on the way in, and showing that 50% will be reflected back into space. The idea is that, in agregate, the co2 will have a cooling effect.
However, you have ignored the fact that most of the energy reaching the Earth from the sun is not in the IR, but in the visible spectrum. This bulk of energy goes straight through the CO2 and reaches the surface. It is then absorbed by the ground and the oceans and is emitted as IR. So, although the CO2 has intercepted the small amount of incoming IR and sent it back into space, there is a much larger flow of outgoing IR on which to act. This means the cooling effect is much less than the warming effect.
Not only integrating sphere, Michael, but also thermal IR sensors and cameras. One has to know the true emissivity in order to sense temperature accurately.
It is quite a lot more complicated, which is why in engineering we do two things to simplify. To avoid having to integrate emitted power throughout the entire volume of gas onto the point of interest, we resort to a “effect length” of path through the gas that depends on the geometry of the enclosure, which makes the problem quasi-one dimensional. For example, the effective length of path to one surface in an enclosure between infinite planes is 1.8 times the distance between the planes.
Second, we find the “emissivity” of the gas as a function of partial pressure of H2O and CO2 (the two common gases involved in IR) and temperature from a chart, or from a program that represents the chart. Problems in which there is a temperature gradient in the gas are more complex yet. Active gas in an enclosure is not a simple problem.
I agree quite generally with Willis on this post. One general comment I would make is about the common use of the term “radiation” as in radiation=sigma*T^4. What we actually calculate is emitted power; i.e. power (watts) emitted per unit area of surface into a hemisphere above that surface. Not keeping in mind the units of things leads to a lot of confusion.
Willis says he disagrees with this notion:
“somehow a combination of gravity and a transparent, GHG-free atmosphere can conspire to push the temperature of a planet well above the theoretical S-B temperature, to a condition similar to that of the Earth.”
Wayne says: “No Bill, if the air was ever warmer than the surface the air would transfer by conduction that energy from the air TO the surface, always warmer to cooler. It would not just accumulate. Eventually an equilibrium would be established.”
Peter Sorenson says: “Willis has forgotten about the convective heat transfer. and the mass transfer modes of moving heat.”
There is no planet that derives heat from a multitude of surrounding suns. [snip: My friend, it’s called a “thought experiment”. -w]
The argument that theory trumps observation is what has led so many astray. Here is a practical demonstration of a device that is theoretically impossible.
First, let’s clear up two separate uses of the term “lapse rate”. Willis refers to the dry adiabatic lapse rate. This is a decrease in temperature per height gain in a rising air parcel. It is a process — adiabatic decompression.
Second, the term “lapse rate” in the atmosphere is the general decline in temperature of the troposphere with altitude. It is the end result of a whole series of processes that contribute to a final temperature distribution — one of these processes is adiabatic sinking or lifting of air, so is radiant emission.
When we use the term specific heat, we are not speaking of heat, but rather how much heat is needed to raise the temperature of one kilogram of material one degree celsius.
Cp is a measure based one-kilogram mass of material. If you increase density by jamming more kilograms into a volume, the specific heat remains the same because it is per unit mass. The heat capacity per unit volume increases, but not the specific heat. So thinner air has less heat capacity, but not less specific heat.
Oh, and let’s not forget the ocean.
I’m not sure about lapse rate warming being the answer as lapse rate cooling in the convection cycle would tend to cancel it out however… does gravity (which can do work) add energy to the equation such that radiation in + work done by gravity = radiation out? (Where the heck does gravity come from anyway?)
Willis is right, but they might quibble (though they didn’t think to make this suggestion) that clouds radiate at colder temperatures, so this effect goes in the right direction to balance the energy. However, the cloud-top distribution that is observed does not help to close the energy balance.
Conservation of energy dictates that the amount of energy radiated from the Earth’s system must be equal to the energy it receives. Under the GHG hypothesis, it is argued that this balance occurs at a place called “top of atmosphere”, while any level below this is allowed to be at a higher temperature.
The gravity hypothesis must similarly involve a TOA radiation that is equal to the incoming radiation, and would allow that the temperature at the Earth’s surface be higher than this. Willis premise is that there cannot be a TOA radiating less that the surface, because to do so, the atmosphere would need to absorb outgoing IR, and without GHG’s it cannot do so.
But, if the lower atmosphere is warmed by the gravity effect, there would indeed by a temperature gradient, with temperature declining as you go higher. At this point, it could be imagined that there is a TOA higher up radiating the same amount of energy that is received from the Sun.
But. . .the crucial point is, these molecules in the atmosphere cannot radiate. To do so would require molecules of N2 and O2 to emit photons. As far as I am aware, they do not. The only way energy can leave the Earth is by radiation, and only the surface can radiate. This does lead to the violation that Willis states – the ground is supposedly warmed by a gravity compressed atmosphere, yet the energy can only leave the planet by radiating from the surface, which implies more energy radiating than being received.
However. . . What if we imagine some GHG’s are added to the atmosphere (just like our good ol’ Earth, actually). What happens if we suppose the gravity hypothesis to be correct? The ground is warmed by compression, and this extra outgoing radiation is absorbed by the GHG’s in the atmosphere. There can now be a TOA effect, radiating exactly the same amount of energy into space as is received.
Does this sound as if GHG’s and gravity both play a role in regulating the Earth’s temperature? Could be. The moral is – never thow out the baby with the bath water, Willis.