Quick
Search: 
 
advanced search
 GSW Home    GeoRef Home    My GSW Alerts    Contact GSW    About GSW    Journals List    Help 
Bulletin of the Seismological Society of America Don't get GSW? Talk to your librarian.
JOURNAL HOME HELP CONTACT PUBLISHER SUBSCRIBE ARCHIVE SEARCH TABLE OF CONTENTS

Bulletin of the Seismological Society of America; October 1997; v. 87; no. 5; p. 1288-1296
© 1997 Seismological Society of America
This Article
Right arrow Full Text (PDF)
Right arrow References
Right arrow Alert me when this article is cited
Right arrow Alert me if a correction is posted
Right arrow Citation Map
Services
Right arrow Email this article to a friend
Right arrow Similar articles in this journal
Right arrow Alert me to new issues of the journal
Right arrow Download to citation manager
Right arrow reprints & permissions
Citing Articles
Right arrow Citing Articles via HighWire
Right arrow Citing Articles via Google Scholar
Google Scholar
Right arrow Articles by Deichmann, N.
Right arrow Search for Related Content
GeoRef
Right arrow GeoRef Citation

Far-field pulse shapes from circular sources with variable rupture velocities

Nicholas Deichmann

Swiss Seismological Service Institute of Geophysics, ETH-Hönggerberg, CH-8093 Zürich, Switzerland

Abstract

Recently, Sato (1994) developed a simple earthquake source model of a circular rupture expanding outward from the center of a fault with constant stress drop. In contrast to previous models, the rupture velocity is allowed to vary over the duration of faulting. This model is used to synthesize apparent moment-rate functions for a three-stage source process: first, the rupture starts out with a gradually increasing velocity, then, it continues to expand uniformly until, finally, it slows to a gradual stop. Synthetic velocity seismograms are obtained from a convolution of the apparent moment-rate functions with a causal Q-operator and an appropriate instrument response. Comparisons with an example of an earthquake signal show that, in the context of the proposed model, the observed emergent P-wave onset, which is not compatible with a constant rupture velocity, can be explained by a gradually accelerating rupture front. Systematic departures from the generally expected scaling relationship between seismic moment and rupture duration are often interpreted as evidence for a dependence of stress drop on seismic moment. However, the trade-off between stress drop and rupture velocity inherent in all kinematic source models implies that such deviations can just as well be attributed to systematic variations of rupture velocity. Whereas, in general, the total duration of the far-field displacement pulse is shorter for P waves than for S waves, the model predicts that the rise time, {tau}1/2, of the displacement pulse should be longer for P waves than for S waves. This feature could constitute a critical test of the model and also provide a constraint on the rupture velocity.




This article has been cited by other articles:


Home page
Bulletin of the Seismological Society of AmericaHome page
N. Deichmann
Local Magnitude, a Moment Revisited
Bulletin of the Seismological Society of America, August 1, 2006; 96(4A): 1267 - 1277.
[Abstract] [Full Text] [PDF]


Home page
Bulletin of the Seismological Society of AmericaHome page
The Colima, Mexico, Earthquake (MW 5.3) of 7 March 2000: Seismic Activity Along the Southern Colima Rift
Bulletin of the Seismological Society of America, August 1, 2003; 93(4): 1458 - 1467.



Home page
Bulletin of the Seismological Society of AmericaHome page
N. Deichmann
Empirical Green's functions: A comparison between pulse width measurements and deconvolution by spectral division
Bulletin of the Seismological Society of America, February 1, 1999; 89(1): 178 - 189.
[Abstract] [PDF]




JOURNAL HOME HELP CONTACT PUBLISHER SUBSCRIBE ARCHIVE SEARCH TABLE OF CONTENTS
Copyright © 2009 by Seismological Society of America