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Showing posts with the label Raman

Will Happer should include Raman measurements

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I think Professor  Happer has it absolutely wrong , sadly.  This curve was made redundant by quantum mechanics. In the 1920s, more spectral modes of molecules were discovered/ identified through Raman scattering experiments by Rasetti and others. The two CO2 modes at 1288 and 1338 cm-1 shown here are both Raman only, as are the H2O and the N2O near to them. Raman Lidars can measure the temperature of all of the gases from these modes. The last CO2 mode on the right at 2349cm-1 is right by N2's single 2338cm-1 mode. From this mode, the atmosphere's temperature is measured by Lidars, and the N2-CO2 laser radiates it by infrared photons (or electron discharge). I have written to Happer, and he sadly dismisses the/my Raman measurements.   Raman spectrometers measure in reference to the blackbody radiation ground surface temperature Max value (thin black line).  Blue modes are Raman active modes , and  green lines are both IR (thermo transductive) and Raman active mo...

The gassy messenger: N2 and O2 are also greenhouse gases

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Update May 2015 I have recently (and finally) published my findings: Reinterpreting and Augmenting John Tyndall’s 1859 Greenhouse Gas Experiment with Thermoelectric Theory and Raman Spectroscopy  at:  academia.edu/   and  http://vixra.org/abs/1504.0165   . Abstract Climate science's fundamental premise – assumed by all parties in the great climate debate – says the greenhouse gases – constituting less than 2% of Earth’s atmosphere, first derived by John Tyndall in his 1859 thermopile experiment and demonstrated graphically today by infrared spectroscopy – are unique because of their IR (heat) absorbing property. From this, it is – paradoxically – assumed the (remaining 98%) non-greenhouse gases N 2  nitrogen and O 2  oxygen are non-heat absorbent. This paper reveals, by elementary physics, the (deceptive) role thermopiles play in this paradox . It was found that for a speci...