1973
DOI: 10.1111/j.1365-246x.1973.tb02407.x
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Representation of the Elastic - Gravitational Excitation of a Spherical Earth Model by Generalized Spherical Harmonics

Abstract: The generalized spherical harmonics, which arise as representations of the rotation group, provide a natural basis for the expansion of tensors of any order in spherical co-ordinates. By using the covariant differentiation rules of Burridge, it is possible to obtain economically the separated differential equations of elastic vibration in a radially symmetric sphere. Derivation of the excitation of an Earth model by a point force or point dislocation is also carried out with the aid of these functions. While a… Show more

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Cited by 226 publications
(232 citation statements)
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“…(B4) where the strain and the rotation are evaluated at the source. The first term due to the symmetric moment tensor has been studied (Phinney and Burridge, 1973;Gilbert and Dziewonski, 1975). The second term is discussed in this appendix.…”
Section: Appendix B Normal-mode Excitationmentioning
confidence: 99%
See 1 more Smart Citation
“…(B4) where the strain and the rotation are evaluated at the source. The first term due to the symmetric moment tensor has been studied (Phinney and Burridge, 1973;Gilbert and Dziewonski, 1975). The second term is discussed in this appendix.…”
Section: Appendix B Normal-mode Excitationmentioning
confidence: 99%
“…Following Phinney and Burridge (1973), the canonical components are defined by (19) The canonical components are expanded in terms of the generalized spherical harmonics of Phinney and Burridge (1973) (20) We may obtain the displacement outside the source radius on which the traction is given in Eq. (20) as a boundary condition.…”
Section: Kinematic Descriptionmentioning
confidence: 99%
“…Formulae of the differentiation for higher order tensors are found in BURRIDGE (1969) and PHINNEY and BURRIDGE (1973).…”
Section: Differentiationmentioning
confidence: 99%
“…To evaluate the elements of the coupling matrix, it is useful to express the strain E and the perturbed elastic stiffness tensor c ijkl (r, θ, ϕ) in terms of generalized spherical harmonics Y N lm (Phinney & Burridge 1973;Dahlen & Tromp 1998, (C.164)):…”
Section: Mode Coupling Selection Rule M = Mmentioning
confidence: 99%