Photoacoustic infrared spectra (250–10 000 cm−1) of partially deuterated kaolinite #9

1987 ◽  
Vol 65 (6) ◽  
pp. 1420-1423 ◽  
Author(s):  
K. H. Mlchaelian ◽  
K. Bukka ◽  
D. N. S. Permann

Partial deuteration of kaolinite #9 was accomplished by grinding lumps to a size of 9 μm and refluxing a D2O suspension for periods ranging from 8 to 146 h. Photoacoustic infrared spectra were obtained and compared with previously published infrared and Raman spectra of undeuterated kaolinite and with infrared spectra of deuterated kaolinite. Data from this investigation indicate an extent of deuteration of about 20%; with the exception of the OD stretching bands near 2700 cm−1, most of the bands observed are attributable to undeuterated kaolinite. The infrared band at 2718 cm−1, which was previously assigned to uncoupled inner surface OD stretching, is the analogue of the 3684 cm−1 band observed in Raman and photoacoustic infrared spectra of undeuterated kaolinite. The results support assignment of the 3684 cm−1 band to uncoupled inner surface hydroxyl stretching vibrations.


1971 ◽  
Vol 49 (14) ◽  
pp. 2459-2462 ◽  
Author(s):  
R. Savoie ◽  
M. Pézolet

The Raman and far-infrared spectra of crystalline cyanogen iodide have been recorded. High-frequency shoulders alongside the Raman bands confirm the piezoelectric nature of this solid and allow an estimate to be made of the frequencies of the longitudinal modes associated to the fundamental vibrations. Dipole derivatives calculated from these frequencies agree qualitatively with those obtained from infrared band intensity measurements.



1980 ◽  
Vol 34 (1) ◽  
pp. 60-65 ◽  
Author(s):  
J. R. Durig ◽  
W. J. Natter ◽  
M. Johnson-Streusand

The Raman spectra (0 to 3300 cm−1) of (CH3)3Si(CHCH2) and (CD3)3Si(CHCH2) in the gaseous, liquid and solid states have been recorded. The infrared spectra (20 to 3300 cm−1) of the same two compounds in the gaseous and solid states have also been recorded. A vibrational assignment based upon depolarization ratios, frequency shifts with isotopic substitution, infrared band contours, and group frequencies is proposed. The SiC3 torsion was observed at 55 and 50 cm−1 for the “light” and “heavy” molecules, respectively, and the barriers to internal rotation were calculated to be 0.73 kcal/mol and 0.64 kcal/mol for the light and heavy compounds, respectively. These results are compared to the corresponding data for similar molecules.



1990 ◽  
Vol 55 (6) ◽  
pp. 1485-1490 ◽  
Author(s):  
Peter Schwendt ◽  
Milan Sýkora

The infrared and Raman spectra of M2[V2O2(O2)4(H2O)]·xH2O and M2[V2O2(O2)4(D2O)]·xD2O (M = N(CH3)4, Cs) were measured. In the region of the vanadium-oxygen stretching vibrations, the spectra were interpreted based on normal coordinate analysis, employing empirical correlations between the bond lengths and force constants.



1992 ◽  
Vol 291 ◽  
Author(s):  
Charles C. Kim ◽  
M. I. Bell ◽  
D. A. McKeown

ABSTRACTThe normal modes of vibration and their frequencies are calculated for benitoite, a mineral whose crystal structure (space group D23h) consists of three-membered silicate rings (Si3O9) linked by Ba+2 and Ti+4 ions. The calculation unambiguously assigns the normal modes to the lines in the Raman and infrared spectra and determines the atomic interactions. On the assumption that mode mixings and splittings due to inter-ring interactions are small, the normal frequencies of the isolated ring of C3h, symmetry are determined. The identification of normal modes characteristic of three-membered silicate rings may prove to be a valuable guide in the interpretation of the infrared and Raman spectra of amorphous silicates, potentially leading to new information on the ring statistics of these materials.



1972 ◽  
Vol 26 (5) ◽  
pp. 540-542 ◽  
Author(s):  
G. R. Burns ◽  
D. G. McGavin

Infrared and Raman spectra have been measured for spiropentane-H8. Raman spectra for the liquid have enabled the b1 species ring twist to be assigned. Previous assignments of this mode were based on calorimetric data and on the assignment of a band in the infrared spectrum to a combination band involving the ring twist mode. Infrared spectra of low temperature crystalline films have provided sufficient information that, when taken with the Raman data and gas phase infrared spectra, we have assignments for all of the fundamental modes.



1964 ◽  
Vol 42 (3) ◽  
pp. 690-695 ◽  
Author(s):  
James E. Griffiths ◽  
Donald E. Irish

Infrared spectra (250–2000 cm−1) and Raman displacements (Δv = 100–1800 cm−1) with qualitative polarization measurements are reported for cyanuric fluoride. All of the active fundamentals are assigned on the basis of a planar D3h model: a1′ = 1496, 999, 642; e′ = 1617, 1424, 1087, 576, 378; a2″ = 817, 436; e″ = 743 and 226 cm−1.



1957 ◽  
Vol 35 (9) ◽  
pp. 969-979 ◽  
Author(s):  
J. K. Wilmshurst ◽  
H. J. Bernstein

The Raman spectra of liquid (CD3)3CH and (CD3)3CD were obtained photoelectrically together with depolarization ratios, and the infrared spectra of the corresponding gases were obtained from 3 to 35 μ. A vibrational assignment consistent with depolarization ratios and band contours has been made for the molecules on the basis of C3v symmetry. The spectra have been correlated with the spectra of (CH3)3CH and (CH3)3CD and modified assignments for two modes have been given for these molecules. Tentative assignments have been made for the 'inactive' A2 modes (which are 'active' if the molecule has symmetry C3) to explain some of the observed frequencies around 1000 cm.−1 which could not be satisfactorily assigned as summation or difference tones.



1966 ◽  
Vol 19 (9) ◽  
pp. 1603 ◽  
Author(s):  
GB Deacon ◽  
JHS Green ◽  
W Kynaston

The infrared spectra (500-40 cm-1) of crystalline (Me4N)2HgCl4, Me4NHgCl3, and (Et4As)2HgI4, and the Raman spectra of the first two compounds, have been recorded. Assignments of the vibrational frequencies are made and discussed in relation to the structure of the anions.



1977 ◽  
Vol 31 (3) ◽  
pp. 230-236 ◽  
Author(s):  
R. N. Bhargava ◽  
R. A. Condrate

Infrared and Raman spectra were measured and interpreted for two crystalline VPO5 phases (α- and β-VPO5) and several related vanadium phosphate glasses. The spectral results for the crystalline phases were consistent with those predicted by factor group analysis using the previously determined space groups. Empirical band assignments were made for the observed bands on the basis of the bands observed earlier for related phosphate and oxyvanadium compounds. Also, the band assignments made for the infrared spectra of the glasses were consistent with the assignments for crystalline V2O5 and the two crystalline VPO5 phases. No Raman spectra were observed for the glasses because processes involving adsorption and Rayleigh scattering dominated over Raman scattering. The infrared spectra of vanadium phosphate glasses with high P2O5 concentrations possessed many features resembling those observed in the infrared spectra of α-VPO5, suggesting similarities in the short range order for the two materials. Analyses of the vibrational spectra of hydrated α-VPO5 samples suggests that the water molecules are adsorbed in the interlamellar spaces of the crystals, complexing to vanadium ions. Initial steps in the hydration of vanadium phosphate glasses apparently involve physical adsorption of water on their surfaces. No water adsorption could be detected for β-VPO5 under normal conditions from its infrared and Raman spectra.



1982 ◽  
Vol 47 (8) ◽  
pp. 2027-2036 ◽  
Author(s):  
Jiří Dybal ◽  
Jan Štokr ◽  
Bohdan Schneider

Infrared and Raman spectra of methyl acetate, tert-butyl acetate, methyl pivalate and tert-butyl pivalate were measured in the liquid and crystalline states and solutions of different dielectric constants. In these molecules, the bands of the C=O str. vibrations are not affected by conformational structure. The shape and position of the band of the C=O str. vibration in methyl acetate are primarily determined by intermolecular order created by interactions of the permanent dipoles of the molecules. In methyl pivalate and in tert-butyl acetate, the shape of the carbonyl band is mainly determined by Fermi resonance.



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