ChemInform Abstract: THE CALCULATION OF BOND DISTANCES FROM VALENCE FORCE CONSTANTS (SIEBERT-BADGER-JENSOVSKY ITERATION)

1978 ◽  
Vol 9 (12) ◽  
Author(s):  
A. FADINI ◽  
S. KEMMLER-SACK
Keyword(s):  
Force Constants ◽  
Valence Force

Schwingungsspektren und Kraftkonstanten der Hexacyano-Komplexe des Mangan(I), Technetium(I) und Rhenium(I) / Vibrational Spectra and Force Constants of the Hexacyano Complexes of Mangan(l), Technicium(I) and Rhenium(l)

1972 ◽  
Vol 27 (8-9) ◽  
pp. 1193-1196 ◽  
Author(s):  
W. Krasser ◽  
K. Schwochau
Keyword(s):  
Force Field ◽  
Raman Spectra ◽  
Vibrational Spectra ◽  
Point Group ◽  
Force Constants ◽  
Irreducible Representations ◽  
Infrared And Raman Spectra ◽  
Valence Force ◽  
Valence Force Field ◽  
Complex Salts

The infrared and Raman spectra of the complex salts K5[Mn(CN)6], K5[Tc(CN)6] and K5[Re(CN)s] have been recorded in the range from 4000 to 40 cm-1. All expected fundamental vibrations have been observed and could be assigned to the irreducible representations of the sym­metry point group Oh . The calculation of the force constants is based on the concept of the generalized valence force field. The low CN-valence force constants indicate the relatively strong Π-bonding character of the metal carbon bond, which is especially pronounced for K5[Tc(CN)6).

Semiempirical Calculations of Valence Force Constants in C2X4, C3X4 and C4X4 Compounds

1981 ◽  
Vol 36 (7) ◽  
pp. 759-762 ◽  
Author(s):  
G. Díaz Fleming ◽  
W. Kosmus ◽  
K. Kalcher
Keyword(s):  
Point Charge ◽  
Electron Distribution ◽  
Force Constants ◽  
Semiempirical Calculations ◽  
Point Charge Model ◽  
Valence Force ◽  
Charge Model ◽  
Static Electron

Abstract e m ie m p iric a l C a lc u la tio n s o f V a le n c e F o rc e C o n s ta n ts in C 2X 4 , C3X4 a n d C 4X 4 C o m p o u n d s Valence force constants were calculated for C2X4, C3X4 and C4X4 (X = H, F, Cl, Br) with a point charge model using CNDO data. The magnitude of the valence force constants is discussed in terms of the polarization of the static electron distribution.

Notizen:Schwingungseigenschaften des TeO42- -Ions/ Vibrational Properties of the TeO42--Ion

1978 ◽  
Vol 33 (10) ◽  
pp. 1226-1227
Author(s):  
Enrique J. Baran
Keyword(s):  
Force Field ◽  
Related Species ◽  
Force Constants ◽  
Vibrational Properties ◽  
Bond Orders ◽  
Mean Amplitudes Of Vibration ◽  
Valence Force ◽  
Valence Force Field ◽  
Complete Assignment

Abstract A complete assignment of the fundamental vibrations of the tetrahedral TeO42- ion is proposed and its principal force constants have been calculated using the modified valence force field. Mean amplitudes of vibration and bond orders are also estimated. The results are briefly discussed and some comparisons with related species are made.

On the application of OVFF to MX6 type ions

1972 ◽  
Vol 27 (5) ◽  
pp. 867-869 ◽  
Author(s):  
J. N. Rai ◽  
S. N. Tiwary ◽  
S. N. Rai
Keyword(s):  
Force Field ◽  
Point Group ◽  
Force Constants ◽  
Valence Force ◽  
Valence Force Field

AbstractForce constants for nine ions belonging to Oh point group have been evaluated by using Orbital Valence Force Field. The constants have been compared with their values obtained by using Urey-Bradley Force Field. The validity of the two methods has been discussed

Gitterschwingungsspektren

1976 ◽  
Vol 31 (7) ◽  
pp. 847-852 ◽  
Author(s):  
H. D. Lutz ◽  
P. Willich ◽  
H. Haeuseler
Keyword(s):  
Force Field ◽  
Long Range ◽  
Force Constants ◽  
The Other ◽  
Valence Force ◽  
Normal Coordinates ◽  
Valence Force Field ◽  
Symmetry Coordinates ◽  
Ir Frequencies ◽  
Good Agreement

Abstract Force constants and normal coordinates of MnS2 , FeS2 , RuS2, RuSe2, RuTe2, OsS2 and PtP2 are calculated based on the five ir active vibrations of the pyrite lattice. By setting up a valence force field consisting of short and long range M -X, X2 -X2 and M -M stretching constants it has proved possible to obtain good agreement between experimental and calculated frequencies with expection of FeS2 and RuS2 . The force constants corresponding to the shortest metal chalcogen distances (MnS2: 0.30, RuSe2: 0.88, RuTe2: 0.62, OsS2: 1.32, PtP2: 1.22 mdyn/Å) are mainly responsible for the ir frequencies. For RuSe2 and RuTe2, the forces between adjacent X2 groups are not negligible. Whereas the force constants of OsS2 and PtP2 are of comparable strength, the forces in MnS2 are significantly weaker than those in the other compounds. The normal coordinates of MnS2, OsS2 and PtP2 , and RuSe2 and RuTe2 show significant differences according to both the contribution of the 6 symmetry coordinates to the 5 ir active vibrations and the assignment of the spectra.

Darstellung und Schwingungsspektren von cis- und trans-[OsXY(acac)2], X ≠ Y = Cl, Br, I sowie Normalkoordinatenanalyse von trans-[OsClBr(acac)2]/Synthesis and Vibrational Spectra of cis- and trans-[OsXY(acac)2], X ≠ Y = Cl, Br, I, and Normal Coordinate Analysis of trans-[OsClBr(acac)2]

1998 ◽  
Vol 53 (2) ◽  
pp. 227-231
Author(s):  
K. Dallmann ◽  
W. Preetz
Keyword(s):  
Normal Coordinate Analysis ◽  
Force Constants ◽  
Vibrational Modes ◽  
Normal Coordinate ◽  
Valence Force ◽  
Valence Force Field ◽  
Stretching Vibrations ◽  
Cis And Trans ◽  
Ir And Raman ◽  
Good Agreement

Abstract In the reaction of K2[OsX3 Y3] with boiling water/acetylacetone (1:1) the six mixed com­plexes cis-and trans-[OsX2 (acac)2] (X ≠ Y = Cl, Br, I) are formed, which have been purified by column chromatography with toluene on silica gel. The IR and Raman spectra (10K) show the intraligand vibrations of the acac groups with nearly constant frequencies and the stretching vibrations of OsO in the range 460-696, of OsCl at 315-345, of OsBr at 210-225, and of Osl at 160-175 cm-1 . A normal coordinate analysis based on a modified valence force field was performed for trans-[OsClBr(acac)2] and the vibrational modes have been assigned. With a set of 32 force constants, taking into account the intraligand vibrations, a good agreement between observed and calculated frequencies has been achieved. The valence force constants are fd (OsCl•) = 1.75, fd(OsBr′) = 1.63 and fd (OsO) = 3.27 mdyn/Å.

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