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	<updated>2026-04-25T18:02:02Z</updated>
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		<id>http://wiki.fusenet.eu/fusionwiki/index.php?title=Shafranov_shift&amp;diff=6821</id>
		<title>Shafranov shift</title>
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		<updated>2021-03-15T20:10:31Z</updated>

		<summary type="html">&lt;p&gt;Meritt: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The Shafranov shift&amp;lt;ref&amp;gt;V.D. Shafranov, Atomnaya Énergiya &#039;&#039;&#039;13&#039;&#039;&#039; (1962) 521, [http://dx.doi.org/10.1007/BF01312317 Translated &#039;&#039;Equilibrium of a toroidal pinch in a magnetic field&#039;&#039;, At. Energy &#039;&#039;&#039;13&#039;&#039;&#039;, 6 (1963) 1149]&amp;lt;/ref&amp;gt; is the outward radial displacement &#039;&#039;&amp;amp;Delta;(r)&#039;&#039; of the centre of [[Flux surface|flux surfaces]] with [[Toroidal coordinates|minor radius]] &#039;&#039;r&#039;&#039;, induced by plasma pressure and the hoop force &amp;lt;ref&amp;gt;John Wesson, &#039;&#039;Tokamaks&#039;&#039;, Clarendon Press (2004) ISBN 9780198509226&amp;lt;/ref&amp;gt;.&lt;br /&gt;
Typically, the shift is linear &amp;lt;ref&amp;gt;J.P. Freidberg, &#039;&#039;Plasma physics and fusion energy&#039;&#039;, Cambridge University Press (2007) ISBN 0521851076&amp;lt;/ref&amp;gt; in [[Beta|beta (&amp;amp;beta;)]], and it tends to be more important for [[Tokamak|tokamaks]] than [[Stellarator|stellarators]],&lt;br /&gt;
due to the fact that the magnetic configuration is largely or partly imposed externally in the latter case.&lt;br /&gt;
&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0741-3335/48/6/006 T. Kobuchi, K. Ida, H. Yamada, M. Yokoyama, K.Y. Watanabe, S. Sakakibara, M. Yoshinuma and the LHD Experimental Group, &#039;&#039;Magnetic configuration dependence of the shafranov shift in the Large Helical Device&#039;&#039;, Plasma Phys. Control. Fusion &#039;&#039;&#039;48&#039;&#039;&#039; (2006) 789]&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;/div&gt;</summary>
		<author><name>Meritt</name></author>
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