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<oai_dc:dc xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
  <dc:contributor>P. Spudich</dc:contributor>
  <dc:contributor>G. C. Beroza</dc:contributor>
  <dc:creator>Mariagiovanna Guatteri</dc:creator>
  <dc:date>2001</dc:date>
  <dc:description>&lt;p&gt;&lt;span&gt;We consider the applicability of laboratory-derived rate-and state-variable friction laws to the dynamic rupture of the 1995 Kobe earthquake. We analyze the shear stress and slip evolution of&amp;nbsp;&lt;/span&gt;&lt;i&gt;Ide and Takeo's&lt;/i&gt;&lt;span&gt;&amp;nbsp;[1997] dislocation model, fitting the inferred stress change time histories by calculating the dynamic load and the instantaneous friction at a series of points within the rupture area. For points exhibiting a fast-weakening behavior, the Dieterich-Ruina friction law, with values of&amp;nbsp;&lt;/span&gt;&lt;i&gt;d&lt;sub&gt;c&lt;/sub&gt;&lt;/i&gt;&lt;span&gt;&amp;nbsp;= 0.01–0.05 m for critical slip, fits the stress change time series well. This range of&amp;nbsp;&lt;/span&gt;&lt;i&gt;d&lt;sub&gt;c&lt;/sub&gt;&lt;/i&gt;&lt;span&gt;&amp;nbsp;is 10–20 times smaller than the slip distance over which the stress is released,&amp;nbsp;&lt;/span&gt;&lt;i&gt;D&lt;sub&gt;c&lt;/sub&gt;&lt;/i&gt;&lt;span&gt;, which previous studies have equated with the slip-weakening distance. The limited resolution and low-pass character of the strong motion inversion degrades the resolution of the frictional parameters and suggests that the actual&amp;nbsp;&lt;/span&gt;&lt;i&gt;d&lt;sub&gt;c&lt;/sub&gt;&lt;/i&gt;&lt;span&gt;&amp;nbsp;is less than this value. Stress time series at points characterized by a slow-weakening behavior are well fitted by the Dieterich-Ruina friction law with values of&amp;nbsp;&lt;/span&gt;&lt;i&gt;d&lt;sub&gt;c&lt;/sub&gt;&lt;/i&gt;&lt;span&gt;≥0.01–0.05 m. The apparent fracture energy&amp;nbsp;&lt;/span&gt;&lt;i&gt;G&lt;sub&gt;c&lt;/sub&gt;&lt;/i&gt;&lt;span&gt;&amp;nbsp;can be estimated from waveform inversions more stably than the other friction parameters. We obtain a&amp;nbsp;&lt;/span&gt;&lt;i&gt;G&lt;sub&gt;c&lt;/sub&gt;&lt;/i&gt;&lt;span&gt;&amp;nbsp;≈ 1.5×l0&lt;/span&gt;&lt;sup&gt;6&lt;/sup&gt;&lt;span&gt;&amp;nbsp;J m&lt;/span&gt;&lt;sup&gt;−2&lt;/sup&gt;&lt;span&gt;&amp;nbsp;for the 1995 Kobe earthquake, in agreement with estimates for previous earthquakes. From this estimate and a plausible upper bound for the local rock strength we infer a lower bound for&amp;nbsp;&lt;/span&gt;&lt;i&gt;D&lt;sub&gt;c&lt;/sub&gt;&lt;/i&gt;&lt;span&gt;&amp;nbsp;of about 0.008 m.&lt;/span&gt;&lt;/p&gt;</dc:description>
  <dc:format>application/pdf</dc:format>
  <dc:identifier>10.1029/2001JB000294</dc:identifier>
  <dc:language>en</dc:language>
  <dc:publisher>American Geophysical Union</dc:publisher>
  <dc:title>Inferring rate and state friction parameters from a rupture model of the 1995 Hyogo-ken Nanbu (Kobe) Japan earthquake</dc:title>
  <dc:type>article</dc:type>
</oai_dc:dc>