<?xml version='1.0' encoding='utf-8'?>
<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>T.-F. Wong</dc:contributor>
  <dc:contributor>S.H. Hickman</dc:contributor>
  <dc:creator>N.M. Beeler</dc:creator>
  <dc:date>2003</dc:date>
  <dc:description>&lt;div class="margin-size-16-b margin-size-16-t"&gt;&lt;div class="margin-size-4-t margin-size-16-b"&gt;&lt;p class="typography serif indefinite-width"&gt;&lt;span&gt;We consider&amp;nbsp;expected&amp;nbsp;relationships&amp;nbsp;between&amp;nbsp;apparent&amp;nbsp;stress&amp;nbsp;τ&lt;sub&gt;a&lt;/sub&gt;&amp;nbsp;and&amp;nbsp;static&amp;nbsp;stress&amp;nbsp;drop&amp;nbsp;Δτ&lt;sub&gt;s&lt;/sub&gt;&amp;nbsp;using a standard&amp;nbsp;energy&amp;nbsp;balance and find τ&lt;sub&gt;a&lt;/sub&gt;&amp;nbsp;= Δτ&lt;sub&gt;s&lt;/sub&gt;&amp;nbsp;(0.5 - ξ), where ξ is&amp;nbsp;stress&amp;nbsp;overshoot. A simple implementation of this balance is to assume overshoot is constant; then&amp;nbsp;apparent&amp;nbsp;stress&amp;nbsp;should vary linearly with&amp;nbsp;stress&amp;nbsp;drop, consistent with spectral theories (Brune, 1970) and dynamic crack models (Madariaga, 1976). Normalizing this expression by the&amp;nbsp;static&amp;nbsp;stress&amp;nbsp;drop&amp;nbsp;defines an&amp;nbsp;efficiency&amp;nbsp;η&lt;sub&gt;sw&lt;/sub&gt;&amp;nbsp;= τ&lt;sub&gt;s&lt;/sub&gt;a/Δτ&lt;sub&gt;s&lt;/sub&gt;&amp;nbsp;as follows from Savage and Wood (1971). We use this measure of&amp;nbsp;efficiency&amp;nbsp;to analyze data from one of a number of observational studies that find&amp;nbsp;apparent&amp;nbsp;stress&amp;nbsp;to increase with seismic moment, namely earthquakes recorded in the Cajon Pass borehole by Abercrombie (1995). Increases in&amp;nbsp;apparent&amp;nbsp;stress&amp;nbsp;with event size could reflect an increase in seismic&amp;nbsp;efficiency; however, η&lt;sub&gt;sw&lt;/sub&gt;&amp;nbsp;for the Cajon earthquakes shows no such increase and is approximately constant over the entire moment range. Thus,&amp;nbsp;apparent&amp;nbsp;stress&amp;nbsp;and&amp;nbsp;stress&amp;nbsp;drop&amp;nbsp;co-vary, as&amp;nbsp;expected&amp;nbsp;from the&amp;nbsp;energy&amp;nbsp;balance at constant overshoot. The median value of η&lt;sub&gt;sw&lt;/sub&gt;&amp;nbsp;for the Cajon earthquakes is four times lower than η&lt;sub&gt;sw&lt;/sub&gt;&amp;nbsp;for laboratory events. Thus, these Cajon-recorded earthquakes have relatively low and approximately constant&amp;nbsp;efficiency. As the&amp;nbsp;energy&amp;nbsp;balance requires η&lt;sub&gt;sw&lt;/sub&gt;&amp;nbsp;= 0.5 - ξ, overshoot can be estimated directly from the Savage-Wood&amp;nbsp;efficiency; overshoot is positive for Cajon Pass earthquakes. Variations in&amp;nbsp;apparent&amp;nbsp;stress&amp;nbsp;with seismic moment for these earthquakes result primarily from systematic variations in&amp;nbsp;static&amp;nbsp;stress&amp;nbsp;drop&amp;nbsp;with seismic moment and do not require a relative decrease in sliding resistance with increasing event size (dynamic weakening). Based on the comparison of field and lab determinations of the Savage-Wood&amp;nbsp;efficiency, we suggest the criterion η&lt;sub&gt;sw&lt;/sub&gt;&amp;nbsp;&amp;gt; 0.3 as a test for dynamic weakening in excess of that seen in the lab.&lt;/span&gt;&lt;/p&gt;&lt;/div&gt;&lt;/div&gt;</dc:description>
  <dc:format>application/pdf</dc:format>
  <dc:identifier>10.1785/0120020162</dc:identifier>
  <dc:language>en</dc:language>
  <dc:publisher>Seismological Society of America</dc:publisher>
  <dc:title>On the expected relationships among apparent stress, static stress drop, effective shear fracture energy, and efficiency</dc:title>
  <dc:type>article</dc:type>
</oai_dc:dc>