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	<title>OR/17/062 Focal mechanism - Revision history</title>
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		<id>http://earthwise-staging.bgs.ac.uk/index.php?title=OR/17/062_Focal_mechanism&amp;diff=36720&amp;oldid=prev</id>
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		<summary type="html">&lt;p&gt;1 revision imported&lt;/p&gt;
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		<title>Ajhil at 13:43, 21 March 2018</title>
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		<updated>2018-03-21T13:43:02Z</updated>

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&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;__NOTOC__&lt;br /&gt;
{{OR/17/062}}&lt;br /&gt;
Local mechanisms for the earthquake were determined from measured first motion polarities on the vertical component of ground motion and SH/P amplitude ratios using three different methods: FOCMEC, the grid search method of Snoke et al. (1984)&amp;lt;ref name=&amp;quot;Snoke 1984&amp;quot;&amp;gt;SNOKE, J, MUNSEY, J, TEAGUE, A, and BOLLINGER, G. 1984. A program for focal mechanism determination by combined use of polarity and P-SV amplitude ratio data. &amp;#039;&amp;#039;Earthquake Notes 55&amp;#039;&amp;#039;, 3–15.&amp;lt;/ref&amp;gt;; HASH (Hardebeck and Shearer, 2003&amp;lt;ref name=&amp;quot;Hardebeck 2003&amp;quot;&amp;gt;HARDEBECK, J L, and SHEARER, P M. 2003. Using S/P Amplitude Ratios to Constrain the Focal Mechanisms of Small Earthquakes. &amp;#039;&amp;#039;Bulletin of the Seismological Society of America&amp;#039;&amp;#039;, 93:2434–2444.&amp;lt;/ref&amp;gt;); and, FPFIT, Reasenberg and Oppenheimer [1985]&amp;lt;ref name=&amp;quot;Reasenberg 1985&amp;quot;&amp;gt;REASENBERG, P, and OPPENHEIMER, D. 1985. FPFIT, FPPLOT, and FPPAGE: Fortran computer programs for calculating and displaying earthquake fault plane solutions. Technical report, U.S. Geol. Survey.&amp;lt;/ref&amp;gt;. Both FOCMEC and HASH use both polarities and SH/P amplitude ratios. FPFIT uses only polarities. The 1-D velocity model and the best fitting hypocentre were used to determine take-off angles.&lt;br /&gt;
&lt;br /&gt;
We measured 11 first motion polarities and 5 SH/P amplitude ratios. The stations where these were measured are shown in Figure 8(a) and (b). Sampling of the focal sphere is quite poor as a result of the large azimuthal gap with all the measurements from either the east of the epicentre.&lt;br /&gt;
&lt;br /&gt;
For the grid search method of Snoke et al. (1984)&amp;lt;ref name=&amp;quot;Snoke 1984&amp;quot;&amp;gt;&amp;lt;/ref&amp;gt;, we used a grid spacing of 2° and a maximum amplitude ratio error of 0.1. 21 solutions were found that fitted the data. These were all very similar and we selected the one with the smallest amplitude ratio error as representative. We also used a grid spacing of 2° for HASH along with a maximum average error in the amplitude ratio of 0.1.&lt;br /&gt;
&lt;br /&gt;
The source mechanisms given by the three different methods are shown in Figure 8(c), (d) and (e). All three methods show a right-lateral predominantly strike-slip fault that strikes north-northwest south-southeast and dips by varying amounts to the west. The second fault plane calculated by both FOCMEC and FPFIT strikes approximately east-west and dips north. However, HASH calculates a second fault plane that is near vertical and strikes northeast-southwest (d). These results suggest that the mechanism is not very well constrained.&lt;br /&gt;
&lt;br /&gt;
[[Image:OR17062fig8.jpg|thumb|center|500px|  &amp;#039;&amp;#039;&amp;#039;Figure 8&amp;#039;&amp;#039;&amp;#039;&amp;amp;nbsp;&amp;amp;nbsp;&amp;amp;nbsp;&amp;amp;nbsp;Stations where first motion polarities (a) and SH/P amplitude ratios were measured. Source mechanisms determined using (c) FOCMEC, (d) HASH and (e) FPFIT.    ]]&lt;br /&gt;
==References==&lt;br /&gt;
{{reflist}}&lt;br /&gt;
[[Category: OR/17/062 The Moidart earthquakes of 4 August 2017  | 05]]&lt;/div&gt;</summary>
		<author><name>Ajhil</name></author>
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