Due to personal circumstances I don`t have the luxury to spend a lot of time debating here.
SSDD:
You might find this interesting because there are a number of scientists who have been saying that the 2nd law of thermodynamics also applies to radiative heat transfer.
Included here is their e-mail and other contact information. This is just a small segment of the scientific community that wants to have a free and open debate, which suggests that they would be inclined to answer any questions you have.
Okay here are some examples
Paul S. Braterman,
Regents Professor of Chemistry,
University of North Texas,
Denton, TX 76203 psb@unt.edu
Barrett's paper cited here with approval is erroneous, ignores an important term, and thus violates the second law of thermodynamics, as I have shown (Spectrochim Acta, '97).
The present contribution (unless and until it is accepted by a reputable journal, it should not be referred to as a "paper") appears to commit similar errors, and to ignore, or claim with no evidence to supersede, the voluminous experimental studies on the spectrum of carbon dioxide.
Are we being faced with yet another media pseudo-event?
Volz, Dr. Hartwig" GPRHV@rwedea.de
It seems to me that my understanding of greenhouse physics is completely different from yours. I would like to remind you of the well-known method to measure the temperature of flames. A zirconium dioxide lamp (black body radiator) is placed behind a flame and the black body radiance is measured by a spectrometer through the flame. If the temperature of flame is lower than the lamp's, you will see absorption lines in the black body spectrum. If the flame is hotter, you will see peaks on the black body spectrum at the same wave number positions; if the temperature of lamp and flame equal each other, you will see the ideal black body spectrum.
A similar experiment: in the spectrum of the sun you see Fraunhofer lines (absorption lines). During aneclipse you see emission lines in the chromosphere at the very same wave numbers of the Fraunhofer lines. In both experiments thermodynamics and quantum mechanics are closely interconnected. If you replace the hot lamp by the black radiator earth and the excited states in the flame by the vibration/rotation of gases in the atmosphere, you are in the correct greenhouse physics.
Jarl Ahlbeck AT jahlbeck@ra.abo.fi
Jarl R. Ahlbeck D.Sc.(Chem Eng.)
Abo Akademi University, Finland
Dr. Hartwig's letter pointed out that the second law of thermodynamics is valid also for radiative heat transfer. Of course no radiation can be absorbed by a gas of the same temperature as the radiating surface
All I can add to the above is that I have observed the same disappearance of the Fraunhofer lines using state of the art atomic absorption spectrophotometers with various cathode ray and deuterium arc lamps. Anybody who has been using these analytical tools for quantitative emission and absorption spectroscopic analysis could tell you the same thing.
Have fun with it. I`m curious what happens next after this post is up
SSDD:
You might find this interesting because there are a number of scientists who have been saying that the 2nd law of thermodynamics also applies to radiative heat transfer.
Included here is their e-mail and other contact information. This is just a small segment of the scientific community that wants to have a free and open debate, which suggests that they would be inclined to answer any questions you have.
Okay here are some examples
Paul S. Braterman,
Regents Professor of Chemistry,
University of North Texas,
Denton, TX 76203 psb@unt.edu
Barrett's paper cited here with approval is erroneous, ignores an important term, and thus violates the second law of thermodynamics, as I have shown (Spectrochim Acta, '97).
The present contribution (unless and until it is accepted by a reputable journal, it should not be referred to as a "paper") appears to commit similar errors, and to ignore, or claim with no evidence to supersede, the voluminous experimental studies on the spectrum of carbon dioxide.
Are we being faced with yet another media pseudo-event?
Volz, Dr. Hartwig" GPRHV@rwedea.de
It seems to me that my understanding of greenhouse physics is completely different from yours. I would like to remind you of the well-known method to measure the temperature of flames. A zirconium dioxide lamp (black body radiator) is placed behind a flame and the black body radiance is measured by a spectrometer through the flame. If the temperature of flame is lower than the lamp's, you will see absorption lines in the black body spectrum. If the flame is hotter, you will see peaks on the black body spectrum at the same wave number positions; if the temperature of lamp and flame equal each other, you will see the ideal black body spectrum.
A similar experiment: in the spectrum of the sun you see Fraunhofer lines (absorption lines). During aneclipse you see emission lines in the chromosphere at the very same wave numbers of the Fraunhofer lines. In both experiments thermodynamics and quantum mechanics are closely interconnected. If you replace the hot lamp by the black radiator earth and the excited states in the flame by the vibration/rotation of gases in the atmosphere, you are in the correct greenhouse physics.
Jarl Ahlbeck AT jahlbeck@ra.abo.fi
Jarl R. Ahlbeck D.Sc.(Chem Eng.)
Abo Akademi University, Finland
Dr. Hartwig's letter pointed out that the second law of thermodynamics is valid also for radiative heat transfer. Of course no radiation can be absorbed by a gas of the same temperature as the radiating surface
All I can add to the above is that I have observed the same disappearance of the Fraunhofer lines using state of the art atomic absorption spectrophotometers with various cathode ray and deuterium arc lamps. Anybody who has been using these analytical tools for quantitative emission and absorption spectroscopic analysis could tell you the same thing.
Have fun with it. I`m curious what happens next after this post is up
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