Die Anwendbarkeit verschiedener Näherungsmethoden zur Berechnung von Kraftkonstanten bei Säkulargleichungen der Ordnung n > 2 / The Applicability of Different Approximation Methods for the Calculation of Force Constants in Secular Equations of Order n > 2

1974 ◽  
Vol 29 (2) ◽  
pp. 332-337 ◽  
Author(s):  
Hans Hermann Eysel ◽  
Walter J. Lehmann ◽  
Kai Lucas ◽  
Achim Müller ◽  
Karlheinz Schmidt

Force constants for molecules with secular equations of order n > 2 have been determined with the help of various approximation methods based on the General Valence Force Field. The applicability of the approximations have been tested empirically. It cannot be predicted with certainty whether any approximation method yields reliable force constants. Some methods have been found to be inapplicable. The calculation of off-diagonal force constants with any approximation method is impossible. The principle of the quasi-determination of off-diagonal force constant matrix elements from the form of the G matrix on which most approximation methods are based, is critically discussed. It is shown that diagonal force constants calculated with approximation methods are more reliable if the coupling between the vibrations in the same species is low. The application of approximation methods for the determination of force constants without critical consideration is not meaningful.

1977 ◽  
Vol 32 (1) ◽  
pp. 76-78 ◽  
Author(s):  
A. K. Dublish ◽  
B. B. Srivastava ◽  
D. K. Sharma ◽  
U. P. Verma ◽  
A. N. Pandey

Abstract Recently reported Coriolis constants of tetrahedral tetramethyls of group IVA metals from the vapour phase IR spectra have been used to determine the pseudo-exact force constants with the aid of the point mass model. The symmetrized force constants for tetramethyls of group IVA and some tetrahedral molecules and ions have also been computed following thhe L-F approximation method. The results are compared with exact or pseudo-exact force constants and with those force constants obtained from different approximation methods. The validity of the method has been tested.


It is shown that the force constants of a solid cannot be deduced from the lattice frequencies alone. The fact that a set of force constants agrees with the frequencies exactly is no guarantee that the force constants are even approximately correct. Detailed eigenvector measurements would resolve the uncertainty. A solid has many more force constants than frequencies. The usual procedure gets round this by retaining only the largest force constants and then using at least as many frequencies as the number of retained force constants to calculate the latter. This procedure is incorrect, because neglecting the small force constants limits the accuracy to which the frequency data can be used to calculate the retained constants. In fact, the number of data that can be extracted from the frequency measurements is always less than the number of force constants one wants to calculate. Therefore, even if all the lattice frequencies were known exactly they could still be satisfied with a very wide range of very different sets of force constants. A large proportion of these sets cannot be rejected on the basis of physical criteria alone. Using the methods of continuous transformation theory, for diamond all the ways are constructed in which the force constant matrix can be changed continuously without altering the agreement with the frequencies. A numerical example is included.


1973 ◽  
Vol 16 (1) ◽  
pp. 149-157 ◽  
Author(s):  
T.R. Ananthakrishnan ◽  
C.P. Girijavallabhan ◽  
G. Aruldhas

1993 ◽  
Vol 48 (3) ◽  
pp. 1050-1055 ◽  
Author(s):  
S. Pittel ◽  
P. Federman ◽  
G. E. Arenas Peris ◽  
R. F. Casten ◽  
W.-T. Chou
Keyword(s):  

1949 ◽  
Vol 16 (2) ◽  
pp. 123-133
Author(s):  
H. Poritsky

Abstract This paper extends the discussion of the approximate method of integrating the equations of compressible fluid flow in the hodograph plane first presented by the author before the Sixth International Congress of Applied Mechanics, Paris, France, September, 1948. As an introduction to the discussion of the polygonal approximation method, fundamental fluid-flow equations are reviewed briefly. Determination of the flow function ψ by the “Method of Reflections” is described and an application of the method illustrated. How flow in the physical plane can be determined by superposition of solutions discussed is shown for the simpler incompressible case.


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