Molekūlstrukturen von Phoshorverbindungen / Molecular Structure of Phosphorus Compounds. 1. Trimethylphosphate

1973 ◽  
Vol 28 (7) ◽  
pp. 1140-1144
Author(s):  
I. Trimethylphosphat ◽  
H. Oberhammer

The molecular structure of Trimethylphosphate O = P(OCH3)3 has been determined in the vapour phase by electron diffraction. The best fit of the experimental scattering intensity was obtained by assuming two rotational isomers with C3-symmetry occuring in a ratio of approximately 3:1. The geometric parameters and mean square amplitudes are given in the article.

1974 ◽  
Vol 29 (6) ◽  
pp. 901-904 ◽  
Author(s):  
O. Oberhammer ◽  
O. Glemser ◽  
H. Klüver

The molecular structure of ClNSOF2 was determined by electron diffraction of gases. The following geometric parameters were obtained:Cl-N=1.715(5), S=N=1.484(7), S=O=1.394(3), S-F=1.548(3) Å, ∢ ClNS=114.7 (8), ∢ FSF=92.6(.8), ∢ NSF=111.8(.9) ∢ NSO=117.4 (3.1) and ∢ OSF=108.6 (.8)°. The results for the mean square amplitudes of vibration are given in the paper and an attempt is made to explain differences in corresponding parameters of some related molecules.


1975 ◽  
Vol 30 (7-8) ◽  
pp. 506-512 ◽  
Author(s):  
H. Oberhammer ◽  
J. Grobe

The molecular structures of the two trifluoromethyl phosphoranes (CF3)2PCl3 and (CF3)3PCl2 have been determined by electron diffraction of gases. The structure of (CF3)2PCl3 was found to be a regular trigonal bipyramid with both CF3 groups in axial positions (D3h symmetry) and the fluorine atoms staggered to the equatorial chlorine atoms. The following geometric parameters (ra-values) were obtained: r(C-F) = 1.331(2) Å, r(P-C) = 1.950(II) Å, r(P-Cl) = 2.036(2) Å and ⦓ FCF = 108.3°(0.4). (CF3)3PCl2 possesses the structure of a distorted trigonal bipyramid with two CF3 groups in axial and one in equatorial position. Again the fluorine atoms of the axial CF3 groups are staggered to the equatorial atoms. The ra-values for the geometric parameters are: r(C-F)= 1.329(2) Å, r(P-C)eq= 1.938(31) Å, r(P-C)ax = 1.946(14) Å, r(P-Cl) = 2.053(6) Å, ⦓ FCF = 108.5°(0.3), ⦓ ClPCl = 133.0°(1.7) and ⦓ CaxPCeq = 95.5°(1.9). The average P-C bond length was found to be r(P-C)av = 1.943(5) A. The results for the mean square amplitudes are given in the article. It was shown that in both molecules the torsional amplitudes of the CF3 groups around the P-C bond directions are small, indicating high potential barriers to internal rotation.


1972 ◽  
Vol 26 ◽  
pp. 3468-3474 ◽  
Author(s):  
Birgit Andersen ◽  
R. Srinivasan ◽  
Per J. Garegg ◽  
Ulla Rudén ◽  
Åke Pilotti

1978 ◽  
Vol 33 (10) ◽  
pp. 1236-1238 ◽  
Author(s):  
Jon Brunvoll ◽  
István Hargittai ◽  
Mária Kolonits

Abstract An electron diffraction investigation yielded the following geometric parameters for trifluoromethyl sulphonyl chloride rg(C-F ) 1.326(4), rg(S=0 ) 1.416(7), rg(S-Cl) 2.016(5), rg(S-C) 1.857(6) Å, ∢ O= S - C 108.3(7)°, ∢ C-S-Cl 98.7(4)°, ∢ O = S = O 122.4(10),° ∢ O = S - Cl 108.3(3)°, ∢ F -C-F 109.9(3)°. The S - C bond is in CF3SO2Cl by almost 0.1 Å longer than in CH3SO2Cl.


1969 ◽  
Vol 18 (2) ◽  
pp. 337-344 ◽  
Author(s):  
I.A. Ronova ◽  
D.A. Bochvar ◽  
A.L. Chistjakov ◽  
Yu.T. Struchkov ◽  
N.V. Alekseev

1973 ◽  
Vol 27 ◽  
pp. 1950-1956 ◽  
Author(s):  
G. Schrumpf ◽  
R. Stölevik ◽  
Kjell-Ivar Dahlquist ◽  
Jacques M. Waisvisz ◽  
Marcel G. van der Hoeven ◽  
...  

1974 ◽  
Vol 28a ◽  
pp. 1150-1154 ◽  
Author(s):  
M. Trætteberg ◽  
G. Paulen ◽  
I. Grenthe ◽  
L. Henriksen ◽  
Bernt Klewe ◽  
...  

1964 ◽  
Vol 18 ◽  
pp. 603-611 ◽  
Author(s):  
A. Almenningen ◽  
B. Andersen ◽  
M. Trætteberg ◽  
Hans Halvarson ◽  
Lennart Nilsson

1971 ◽  
Vol 24 (6) ◽  
pp. 1183 ◽  
Author(s):  
JK Wilmshurst ◽  
JF Horwood

The infrared spectrum of methyl pyruvate in the liquid phase in the vapour phase, in solution, and as a glassy and crystalline solid has been obtained from 4000 to 200 cm-1, together with the Raman spectrum of the liquid. The data are consistent with the assumption of a planar pseudo-trans isomer in the crystalline state, and a mixture of this isomer with a less stable planar pseudo-cis isomer in the other phases investigated. The energy difference between the two isomers in the liquid state was found to be c. 650 cal mol-1. A complete assignment, with the exception of the torsional modes, has been made for both rotational isomers.


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