On the Separation Property of the Roots of the Secular Equation

1930 ◽  
Vol 52 (4) ◽  
pp. 843 ◽  
Author(s):  
E. T. Browne
2015 ◽  
Vol 37 (4) ◽  
pp. 303-315 ◽  
Author(s):  
Pham Chi Vinh ◽  
Nguyen Thi Khanh Linh ◽  
Vu Thi Ngoc Anh

This paper presents  a technique by which the transfer matrix in explicit form of an orthotropic layer can be easily obtained. This transfer matrix is applicable for both the wave propagation problem and the reflection/transmission problem. The obtained transfer matrix is then employed to derive the explicit secular equation of Rayleigh waves propagating in an orthotropic half-space coated by an orthotropic layer of arbitrary thickness.


2021 ◽  
pp. 881-922
Author(s):  
Zhanfeng Ju ◽  
El‐Sayed M. El‐Sayed ◽  
Daqiang Yuan
Keyword(s):  

2021 ◽  
pp. 922-952
Author(s):  
Zhanfeng Ju ◽  
El‐Sayed M. El‐Sayed ◽  
Daqiang Yuan
Keyword(s):  

1982 ◽  
Vol 1 (5) ◽  
pp. 309-311 ◽  
Author(s):  
A. Isidori ◽  
A. Ruberti

2013 ◽  
Vol 31 (20) ◽  
pp. 2149-2156
Author(s):  
W. Caiping ◽  
L. Shaoping ◽  
Z. Liqun ◽  
Z. Lijuan

1966 ◽  
Vol 21 (9) ◽  
pp. 1377-1384
Author(s):  
A. V. Willi

Kinetic carbon-13 and deuterium isotope effects are calculated for the SN2 reaction of CH3I with CN-. The normal vibrational frequencies of CH3I, the transition state I · · · CH3 · · · CN, and the corresponding isotope substituted reactants and transition states are evaluated from the force constants by solving the secular equation on an IBM 7094 computer.Values for 7 force constants of the planar CH3 moiety in the transition state (with an sp2 C atom) are obtained by comparison with suitable stable molecules. The stretching force constants related to the bonds being broken or newly formed (fCC, fCC and the interaction between these two stretches, /12) are chosen in such a way that either a zero or imaginary value for νʟ≠ will result. Agreement between calculated and experimental methyl-C13 isotope effects (k12/ k13) can be obtained only in sample calculations with sufficiently large values of f12 which lead to imaginary νʟ≠ values. Furthermore, the difference between fCI and fCC must be small (in the order of 1 mdyn/Å). The bending force constants, fHCI and fHCC, exert relatively little influence on k12/k13. They are important for the D isotope effect, however. As soon as experimental data on kH/kD are available it will be possible to derive a value for fHCC in the transition state if fHCI is kept constant at 0.205 mdynA, and if fCI, fCC and f12 are held in a reasonable order of magnitude. There is no agreement between experimental and calculated cyanide-C13 isotope effects. Possible explanations are discussed. — Since fCI and fCC cannot differ much it must be concluded that the transition state is relatively “symmetric”, with approximately equal amounts of bond making and bond breaking.


1961 ◽  
Vol 68 (9) ◽  
pp. 906 ◽  
Author(s):  
Harry Lass ◽  
Carleton B. Solloway
Keyword(s):  

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