Fine Structure of Infra-Red Absorption in Organic Compounds and the Raman Effect

Nature ◽  
1929 ◽  
Vol 124 (3121) ◽  
pp. 300-301 ◽  
Author(s):  
R. B. BARNES

Assuming first of all for simplicity that the four chlorine atoms are identical, the greatest symmetry the CCl 4 molecule could have is T d . This would lead us to anticipate four fundamentals, v 1 , v 2 , v 3 , v 4 belonging to normal modes A 1 , E , F 2 , F 2 , respectively, using Placzek’s (1934) nomenclature. A 1 is the total symmetric normal mode, and so v 1 is polarized in the Raman effect, and inactive in the infra-red. A 1 is a singlet mode. E is a doublet mode and v 2 is depolarized in the Raman effect, while it is inactive in the infra-red. F 2 is a triplet mode and v 3 and v 4 are depolarized in the Raman effect and are also active in the infra-red. If the Raman spectrum of CCl 4 is examined under coarse dispersion, lines are observed at 217, 314, 459 cm. -1 , identified as v 2 , v 4 and v 1 respectively. Two at 760 and 790 cm. -1 are usually regarded as the result of resonance degeneracy between v 3 and ( v 1 + v 4 ), both in the mode F 2 .


A detailed investigation of the Raman bands for water in the solid and liquid states was first made by the author. Therein it was found that both ice and water give three sets of bands at λλ 4170, 4680 and 5105 A. U. respectively, corresponding to exciting mercury lines at λλ 3650, 4047 and 4358 A. U. The positions of these bands were not identical for ice and water. The former was found to give sharper bands and their shift form the original exciting line was less than for water. The mean infra-red absorptions corresponding to the bands for ice and water were 3·1 μ and 2·99 μ respectively. The above work was done with an instrument of very small dispersion, so that the structure of the band in either case could not be studied at all.


1941 ◽  
Vol 59 (2) ◽  
pp. 171-173 ◽  
Author(s):  
H. M. Foley ◽  
H. M. Randall
Keyword(s):  

1958 ◽  
Vol 11 (4) ◽  
pp. 513 ◽  
Author(s):  
LK Dyall ◽  
AN Hambly

The infra-red spectra of o-nitroanilines do not indicate any intramolecular hydrogen bonding unless there are nitro groups in both positions 2 and 6 to the amino group. An examination of the literature shows that there is no unambiguous evidence from other sources of such bonding in simple o-nitroanilines. An explanation is given of the variation of the stretching frequencies of the nitro group in sterically hindered compounds and in those with electron-donating ortho- and para-substituents.


1949 ◽  
Vol 17 (7) ◽  
pp. 591-594 ◽  
Author(s):  
San‐ichiro Mizushima ◽  
Yonezo Morino ◽  
Itaru Watanabe ◽  
Takehiko Simanouti ◽  
Shigeto Yamaguchi

1881 ◽  
Vol 172 ◽  
pp. 887-918 ◽  

The researches on which this paper is founded, were commenced in February, 1880, but were not sufficiently advanced for any communication to be made regarding them during last session. As an article on the absorption of colourless liquids by Dr. W. Russell, F. R. S., and Mr. Lepraik appeared in ‘Nature’ on the 19th August, 1880, it might have been thought that we were merely following in the steps of those gentlemen, of the scope of whose work we were not aware; we have therefore stated when our work commenced. It will also be seen that our work has been more especially confined to the infra-red region, for reasons which will presently appear, whilst Messrs. Russell and Lepraik turned their attention to the visible portion of the spectrum. Reasons for undertaking the research . The investigations of Professor Tyndall on radiant energy, and its absorption by various organic compounds, led us to believe that if such marked effects were observed by means of the thermopile, at least as much information ought to be gathered from the photographic method recently brought to the notice of the Royal Society. The absorption measured by the thermopile is essentially the integration of all the absorp­tions in the different regions of the spectrum examined, and by this method it is almost impossible to determine the position of the several components, since the face of the instrument has an appreciable breadth. By the photographic method not only can an approximate estimate of the amount of absorption exercised by the compound be judged, but the exact localities of such absorptions can be indisputably fixed.


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