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	<title>WEBREVIEW</title>
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		<title>Reflexion/ Transmission of a plane wave on a plane interface</title>
		<link>http://www.webreview.dz/spip.php?article2858</link>
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		<dc:date>2015-12-16T10:31:16Z</dc:date>
		<dc:format>text/html</dc:format>
		<dc:language>fr</dc:language>
		<dc:creator>Aklouche H., Bedrici-Fra&#239; N., Gatignol Ph., Potel C., Rahmi F. </dc:creator>


		<dc:subject>Incidence</dc:subject>
		<dc:subject>Reflection</dc:subject>
		<dc:subject>P waves</dc:subject>
		<dc:subject>Transmission.</dc:subject>

		<description>
&lt;p&gt;On a plane interface between two elastic half-space, P and SV waves propagating in the (x, z) pare related by Snell's law and&lt;br class='autobr' /&gt; the law of continuity of displacement components x u and z u and constraints zz &#963; and zx &#963; on both sides of the interface. An&lt;br class='autobr' /&gt; incident wave P or wave SV generates two P or SV reflected waves and two transmitted waves P or SV. The four continuity&lt;br class='autobr' /&gt; equations are written in the form of a matrix multiplied by a vector transmission-reflection coefficient, defined for (...)&lt;/p&gt;


-
&lt;a href="http://www.webreview.dz/spip.php?rubrique483" rel="directory"&gt;Numero 00&lt;/a&gt;

/ 
&lt;a href="http://www.webreview.dz/spip.php?mot5242" rel="tag"&gt;Incidence&lt;/a&gt;, 
&lt;a href="http://www.webreview.dz/spip.php?mot9051" rel="tag"&gt;Reflection&lt;/a&gt;, 
&lt;a href="http://www.webreview.dz/spip.php?mot10344" rel="tag"&gt;P waves&lt;/a&gt;, 
&lt;a href="http://www.webreview.dz/spip.php?mot10345" rel="tag"&gt;Transmission.&lt;/a&gt;

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 <content:encoded>&lt;div class='rss_chapo'&gt;&lt;p&gt;On a plane interface between two elastic half-space, P and SV waves propagating in the (x, z) pare related by Snell's law and&lt;br class='autobr' /&gt;
the law of continuity of displacement components x u and z u and constraints zz &#963; and zx &#963; on both sides of the interface. An&lt;br class='autobr' /&gt;
incident wave P or wave SV generates two P or SV reflected waves and two transmitted waves P or SV. The four continuity&lt;br class='autobr' /&gt;
equations are written in the form of a matrix multiplied by a vector transmission-reflection coefficient, defined for potential&lt;br class='autobr' /&gt;
movement of the particles. For an planar boundary between fluids with different characteristic impedances, there is continuity of&lt;br class='autobr' /&gt;
z u and zz &#963; on both sides of the interface and the shear zx &#963; in the medium must vanish at the interface (fluid media involving&lt;br class='autobr' /&gt;
only perfect no viscosity, so that was normal stresses, not shear stress 0 xz &#963; = ). As soon as the angle of incidence exceeds a&lt;br class='autobr' /&gt;
critical value of incidence, the wave for which the value of incidence is greater than 30&#176;&lt;br class='autobr' /&gt;
becomes evanescent. The reflectiontransmission&lt;br class='autobr' /&gt;
coefficients become complex.&lt;/p&gt;&lt;/div&gt;
		
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