Contribution to the discussion about Climate Change:
Greenhouse Gas Hypothesis Violates Fundamentals of Physics
by Dipl.-Ing. Heinz Thieme
Deutsche Version siehe: http://real-planet.eu/treibhauseffekt.html
The relationship between so-called greenhouse gases and atmospheric temperature is not yet well understood. So far, climatologists have hardly participated in serious scientific discussion of the basic energetic mechanisms of the atmosphere. Some of them, however, appear to be starting to realise that their greenhouse paradigm is fundamentally flawed, and already preparing to withdraw their theories about the climatic effects of CO2 and other trace gases.
At present, the climatological profession is chiefly engaged in promoting the restriction of CO2 emissions as a means of limiting atmospheric warming. But at the same time, they admit that the greenhouse effect - i.e. the influence of so-called greenhouse gases on near-surface temperature - is not yet absolutely proven (Grassl et al., see: http--www.dmg-ev.de-gesellschaft-aktivitaeten-pdf-treibhauseffekt.pdf ). In other words, there is as yet no incontrovertible proof either of the greenhouse effect, or its connection with alleged global warming.
This is no surprise, because in fact there is no such thing as the greenhouse effect: it is an impossibility. The statement that so-called greenhouse gases, especially CO2, contribute to near-surface atmospheric warming is in glaring contradiction to well-known physical laws relating to gas and vapour, as well as to general caloric theory.
The greenhouse theory proposed by the climatological fraternity runs as follows: Outgoing infra-red radiation from the earth’s surface is somehow re-radiated by molecules of CO2 (mainly) and also O3, NO2, CH4 in the atmosphere. This backradiation produces warming of the lower atmosphere. To convince the public of the greenhouse effect, composites of temperature measurements since the 19th century are exhibited that show a certain warming. Measurements of the CO2 content of the air also show a rise in recent decades (Note CO2). Climatologists then claim that the CO2 rise has caused the temperature rise (see: http://earth.agu.org/eos_elec/99148e.html).
A second source of misconceptions about the relation between temperature and the CO2 content of air arises from an erroneous explanation of conditions on the planet Venus. The Venutian atmosphere is 95% CO2, and its near-surface temperature is approximately 460oC (see also: http://www.uni-erlangen.de/docs/FAU/fakultaet/natIII/geol_appl/klima1.htm ). What climatologists overlook is that atmospheric pressure at the surface of Venus is 90 bar, and that it is this colossal pressure that determines the temperature.
Strict application of physical laws admits no possibility that tiny proportions of gases like CO2 in our atmosphere cause backradiation that could heat up the surface and the atmosphere near it:
1. The troposphere cools as altitude increases: in dry air, at a rate of around 1oC per 100m; under typical atmospheric humidity, by around 0.7oC per 100m. This cooling reflects the decrease of atmospheric pressure as altitude increases. Higher is cooler, both by day and by night.
Backradiation of the heat radiation outgoing from the earth's surface would
only be possible by reflection, similarly to the effect of aluminium foil
under roof insulation. But the CO2
share in our atmosphere cannot cause reflection in any way.
Within homogeneous gases and gas mixtures no reflections occur.
As is well known in optics, reflection and even refraction occur only
at the boundaries of materials of different optical density, or at phase
boundaries of a material or a material mixture (solid-liquid, liquid-gaseous,
solid-gaseous). Thus it occurs
with suspended water drops or ice crystals, or at the boundary between surface
water and air - but never within homogeneous materials, e.g. air, water,
3. If outgoing thermal radiation from the earth’s surface is absorbed in the atmosphere, the absorbing air warms up, disturbing the existing vertical pattern of temperature, density and pressure, i.e. the initial state of the air layers. It is well known that warmed air expands and, because it is then lighter than the non-warmed air around it, rises. The absorbed warmth is taken away by air mass exchange. Just this occurs with near-surface air that is warmed by convection from earth's surface, vegetation, buildings and so on. For the same reason the windows of heated rooms are kept closed in winter – otherwise the warm air would escape.
These facts are slowly but surely dawning on climatologists. Grassl and others state (see above) that radiation absorbed by CO2-molecules will warm the atmosphere if no other reactions occur in the physical (in particular dynamic) processes in the earth/atmosphere system. In these "idealised conditions", they say the greenhouse effect would be inevitable. Such "idealised conditions" must obviously include the proviso that air is stationary. It is really quite absurd that even now something so obvious as that hot air rises is not properly taken into account by the climatological profession. When air is heated up locally, it ascends and the warmth is removed. It also expands with decreasing atmospheric pressure at higher altitude, and cools so that no remaining warming can be observed. The warmth taken over by the absorbing air is transported toward the upper troposphere. The greenhouse effect does not occur.
The same process applies to individual CO2-molecules that absorb outgoing radiant heat from the earth's surface or from lower layers of the troposphere. These individual molecules remain at the same temperature as their surroundings. Due to the high density of molecules in the troposphere, an immediate exchange of absorbed radiated energy takes place by convection with the surrounding molecules of air. The CO2-molecules in the air are not isolated and therefore cannot reach a higher temperature than their environment. If energy is absorbed, the molecules in the immediate vicinity will warm up.
4. A prerequisite for any type of heat transfer is that the emitter is warmer than the absorber. Heat transfer is determined by the ratio of the fourth powers of the temperatures of the emitting and the absorbing bodies. Because temperature is uniform within minute volumes of gas in the air, and temperature decreases with increasing altitude, back transfer to near-surface air of radiation from higher CO2-molecules is impossible. In fact, this is just as impossible as it is to use a cold heat radiator to heat up a warmer area.
5. The energy discharge from the troposphere takes place at its upper boundary layer, at the transition of the atmosphere from its gaseous state to a state approaching a vacuum. Only in this zone do gases start to emit even small quantities of energy by radiation. The other energy transfer mechanisms - thermal conduction and convection - which at denser pressure are far more efficient than radiation, no longer operate because of the low density of the atmosphere there. But from the surface where man lives and up to 10 to 17km altitude (depending on geographical latitude), gases transfer the small quantities of energy they might acquire from absorbed radiation by convection and conduction - not by radiation.
The climatologists derived the theoretical foundation of the greenhouse hypothesis from the concept of radiative equilibrium over the entire gas area of the atmosphere, right down to the earth’s surface. But the fundamental premise of radiative equilibrium - a balance of incoming and outgoing radiation - is correct only as long as it is limited to the vacuum-like zone of the upper atmosphere. In the lower regions of the atmosphere, the heat balance is essentially determined by thermal, i.e. thermodynamic equilibrium, which includes the thermodynamic characteristics of the components of the atmosphere as well as their changes in status.
6. From the upper atmosphere down to earth’s surface, air pressure rises continuously. The determinant of atmospheric pressure is the mass and the weight of that part of the atmosphere above the point in question. And as pressure increases, so does temperature. The rise in temperature is caused by the thermodynamic characteristics of the main components of the atmosphere, i.e. N2 and O2. Everyone knows that compression causes gases to warm: the effect is noticeable even when inflating bicycle tires. The atmosphere is no different.
The relations between temperature, pressure and volume within the gas area of an atmosphere are determined by the following equations:
General gas equitation p x v = R x T
Adiabatic change of state p x v k = constant
or T x v k -1 = constant
k = relation of the specific thermal values cp to cv
Estimates of the effects of CO2 concentrations on air temperature are often – as mentioned before – derived from conditions on Venus. If one assumed that the atmosphere of Venus was similar to that of the earth, rather than being 95% CO2, and that it still had a pressure of 90 bar, then the surface temperature would be about 660°C, i.e. about 200°C more than at present. The difference arises from the somewhat smaller k value for triatomic as against biatomic gases (k Air: 1.4; k CO2: 1.3).
Thus it would actually be somewhat colder on earth if our atmosphere consisted of CO2 rather than air.
7. A special feature of our atmosphere is its water content. Water occurs in three states. The solid and liquid forms (clouds) show radiation characteristics completely different from gases: they reflect radiation. Thus only water in its liquid or solid states shows qualities to some extent comparable to a greenhouse (i.e. mimicking, however locally, the effect of fixed and airtight glass or foil). Naturally clouds do not prevent vertical air exchange. Moreover condensation and solidification of the water in air releases substantial amounts of heat, which largely determines the temperature of the lower atmosphere. By contrast, the heat transport and storage characteristics of trace gases like CO2 are negligible factors in determining air temperature.
An interesting sidelight is that human life and most human activities add humidity to the lower atmosphere. Examples include the spread and intensification of agriculture; irrigation; hydraulic engineering, i.e. dams and reservoirs; burning of fossil fuels; other water use by humans, e.g. in industrial production processes; as well respiration by humans and livestock. It could therefore be assumed that the water content of the atmosphere has increased over the last 100 years. And the resulting cloudier skies, especially at night, would lead to a measurable increase in near-surface air temperature. But climatologists have largely neglected the possible influence on temperature of changes in the water content of the atmosphere.
Commonly held perceptions of the climatic relevance of CO2 and other so-called greenhouse gases rest on a staggering failure to grasp some of the fundamentals of physics. Correct interpretation of the Second Law of Thermodynamics and sound appreciation of the necessary physical conditions for emission of radiation by gases lead to the understanding that within the troposphere no backradiation can be caused by so-called greenhouse gases. Therefore it is not at all correct to speak of a thermal effect of these gases on the biosphere.
The thermal conditions in our and any atmosphere are determined by its pressure and the mass of its main components. Higher concentrations of CO2 in our atmosphere – at least until they reached 2% (a 60-fold increase) and thus became injurious to health – would endanger neither the climate nor mankind. To avoid further misunderstanding, the terms greenhouse effect and greenhouse gases should be avoided in describing the functioning of the atmosphere. A more correct term would be atmosphere effect. The operation of this effect is described in "The Thermodynamic Atmosphere Effect" at http://realplanet.eu/atmoseffect.htm.)
It is completely incomprehensible and unjustified to imagine that mankind can or must protect the climate by attempting to control trace amounts of CO2 in the air.
A question to the reader (similar on http://real-planet.eu/wspeicher.html)
Finally a question, dear reader, why is the surface temperature of the moon during almost perpendicular sun exposure remarkably higher than the ground surface temperature in comparable areas on our Earth, e.g. in the Sahara with likewise comparable conditions concerning the sun exposure? In different sources for the moon surface temperature values of around 130°C are given (the surface temperature at the equator during the day is 134°C (273° F) source: http://lunar.gsfc.nasa.gov/moonfacts.html). Ground surface temperature in comparable areas on the Earth, e.g. in the Sahara, with likewise comparable conditions concerning the sun exposure show lower values. Own measurements during almost perpendicular position of the sun, clear sky, in the northern Sahara led to ground surface temperatures of around 80°C. Other sources give temperatures only around 60°C. Own measurements of ground surface temperature in northern part of Mediterranean Sea area have shown already results of 65°C. And this, compared to the moon surface, poor result for the Earth ground surface temperature, is achieved under the main stream idea that the earth has a heating greenhouse effect. The moon because of lack of an atmosphere is however without such an effect. The reason for the higher temperatures on the moon cannot be that the moon day is longer than Earth day. In the sun at noon the (ground)surface temperature does not rise in Sahara further, if it achieved the highest value, which is reached already some minutes before noon (local time). After further 30 minutes of sun irradiation the value already measured does not continue to rise.
Note CO2: However, doubts about the estimation that the preindustrial CO2-level would have been at 0,028%, at present it is about 0,038%, arose in recent publications: http://www.realco2.de/
Worth to be read: "The Skeptics Handbook" http://joannenova.com.au/globalwarming/the_skeptics_handbook_2-22_lq.pdf .
The above article is an adapted translation of articles that appeared in the German periodicals Elektrizitätswirtschaft No. 20/1999 and Fusion No. 1/2000
And The Thermodynamic Atmosphere Effect - stepwise explained - Using a set of technical models of planets with and without an atmosphere the reasons are explained for differences in surface temperature of the planet without an atmosphere compared with the temperature in the ground layer of atmosphere of the other planet.
It is worth to know the speech of Vaclav Klaus, President of the Czech Republic, at the UN Climate Change Conference 2007: http://www.klaus.cz/klaus2/asp/clanek.asp?id=pnHwpGc13sXM
You can contact the author at firstname.lastname@example.org
The author is co-author and belongs to the initial signers of the Climate Declaration of Heiligenroth (Klimamanifest von Heiligenroth) http://www.klimamanifest-von-heiligenroth.de/klimaman-e.html#Page originally created 16.08.2000, English translation revised by S.Scott, July 2003, recent complement 16.06.2011, move to www.realplanet.eu