The pattern of eigenfrequencies of radial overtones which is predicted for a specified Earth-model
In 1974 Anderssen and Cleary examined the distribution of eigenfrequencies<br />of radial overtones in torsional oscillations of Earth-models.<br />They pointed out that according to Sturm-Liouville theory this distribution<br />should approach asymptoticall...
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Istituto Nazionale di Geofisica e Vulcanologia (INGV)
1977-06-01
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doaj-6019cf5464c54251af7f84fbd48c925d2020-11-24T22:30:20ZengIstituto Nazionale di Geofisica e Vulcanologia (INGV)Annals of Geophysics1593-52132037-416X1977-06-01303-445946910.4401/ag-4832The pattern of eigenfrequencies of radial overtones which is predicted for a specified Earth-modelE. R. LAPWOODR. SATOIn 1974 Anderssen and Cleary examined the distribution of eigenfrequencies<br />of radial overtones in torsional oscillations of Earth-models.<br />They pointed out that according to Sturm-Liouville theory this distribution<br />should approach asymptotically, for large overtone number m,<br />the value nnz/y, where y is the time taken by a shear-wave to travel<br />along a radius from the core-mantle interface to the surface, provided<br />elastic parameters vary continuously along the radius. They found that,<br />for all the models which they considered, the distributions of eigenfrequencies<br />deviated from the asymptote by amounts which depended on<br />the existence and size of internal discontinuities. Lapwood (1975) showed<br />that such deviations were to be expected from Sturm-Liouville theory,<br />and McNabb, Anderssen and Lapwood (1976) extended Sturm-Liouville<br />theory to apply to differential equations with discontinuous coefficients.<br />Anderssen (1977) used their results to show how to predict the pattern<br />of deviations —called by McNabb et al. the solotone effect— for a<br />given discontinuity in an Earth-model.<br />Recently Sato and Lapwood (1977), in a series of papers which will<br />be referred to here simply as I, II, III, have explored the solotone effect<br />for layered spherical shells, using approximations derived from an exacttheory which holds for uniform layering. They have shown how the<br />form of the pattern of eigenfrequencies, which is the graph of<br />S — YMUJI/N — m against m, where ,„CJI is the frequency of the m"'<br />overtone in the I"' (Legendre) mode of torsional oscillation, is determined<br />as to periodicity (or quasi-periodicity) by the thicknesses and velocities<br />of the layers, and as to amplitude by the amounts of the discontinuities<br />(III). The pattern of eigenfrequencies proves to be extremely sensitive<br />to small changes in layer-thicknesses in a model.<br />In this paper we examine a proposed Earth-model with six surfaces<br />of discontinuity between core boundary and surface, and predict its<br />pattern of eigenfrequencies. When seismological observations become<br />precise enough, and can be subjected to numerical analysis refined<br />enough, to identify the radial overtones for large m, this pattern of<br />eigenfrequencies will prove to be a severe test for any proposed model,<br />including he one which we discuss below.http://www.annalsofgeophysics.eu/index.php/annals/article/view/4832 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
E. R. LAPWOOD R. SATO |
spellingShingle |
E. R. LAPWOOD R. SATO The pattern of eigenfrequencies of radial overtones which is predicted for a specified Earth-model Annals of Geophysics |
author_facet |
E. R. LAPWOOD R. SATO |
author_sort |
E. R. LAPWOOD |
title |
The pattern of eigenfrequencies of radial overtones which is predicted for a specified Earth-model |
title_short |
The pattern of eigenfrequencies of radial overtones which is predicted for a specified Earth-model |
title_full |
The pattern of eigenfrequencies of radial overtones which is predicted for a specified Earth-model |
title_fullStr |
The pattern of eigenfrequencies of radial overtones which is predicted for a specified Earth-model |
title_full_unstemmed |
The pattern of eigenfrequencies of radial overtones which is predicted for a specified Earth-model |
title_sort |
pattern of eigenfrequencies of radial overtones which is predicted for a specified earth-model |
publisher |
Istituto Nazionale di Geofisica e Vulcanologia (INGV) |
series |
Annals of Geophysics |
issn |
1593-5213 2037-416X |
publishDate |
1977-06-01 |
description |
In 1974 Anderssen and Cleary examined the distribution of eigenfrequencies<br />of radial overtones in torsional oscillations of Earth-models.<br />They pointed out that according to Sturm-Liouville theory this distribution<br />should approach asymptotically, for large overtone number m,<br />the value nnz/y, where y is the time taken by a shear-wave to travel<br />along a radius from the core-mantle interface to the surface, provided<br />elastic parameters vary continuously along the radius. They found that,<br />for all the models which they considered, the distributions of eigenfrequencies<br />deviated from the asymptote by amounts which depended on<br />the existence and size of internal discontinuities. Lapwood (1975) showed<br />that such deviations were to be expected from Sturm-Liouville theory,<br />and McNabb, Anderssen and Lapwood (1976) extended Sturm-Liouville<br />theory to apply to differential equations with discontinuous coefficients.<br />Anderssen (1977) used their results to show how to predict the pattern<br />of deviations —called by McNabb et al. the solotone effect— for a<br />given discontinuity in an Earth-model.<br />Recently Sato and Lapwood (1977), in a series of papers which will<br />be referred to here simply as I, II, III, have explored the solotone effect<br />for layered spherical shells, using approximations derived from an exacttheory which holds for uniform layering. They have shown how the<br />form of the pattern of eigenfrequencies, which is the graph of<br />S — YMUJI/N — m against m, where ,„CJI is the frequency of the m"'<br />overtone in the I"' (Legendre) mode of torsional oscillation, is determined<br />as to periodicity (or quasi-periodicity) by the thicknesses and velocities<br />of the layers, and as to amplitude by the amounts of the discontinuities<br />(III). The pattern of eigenfrequencies proves to be extremely sensitive<br />to small changes in layer-thicknesses in a model.<br />In this paper we examine a proposed Earth-model with six surfaces<br />of discontinuity between core boundary and surface, and predict its<br />pattern of eigenfrequencies. When seismological observations become<br />precise enough, and can be subjected to numerical analysis refined<br />enough, to identify the radial overtones for large m, this pattern of<br />eigenfrequencies will prove to be a severe test for any proposed model,<br />including he one which we discuss below. |
url |
http://www.annalsofgeophysics.eu/index.php/annals/article/view/4832 |
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