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	<id>http://wiki.fusenet.eu/fusionwiki/index.php?action=history&amp;feed=atom&amp;title=TJ-II%3ATransport_and_magnetic_configuration</id>
	<title>TJ-II:Transport and magnetic configuration - Revision history</title>
	<link rel="self" type="application/atom+xml" href="http://wiki.fusenet.eu/fusionwiki/index.php?action=history&amp;feed=atom&amp;title=TJ-II%3ATransport_and_magnetic_configuration"/>
	<link rel="alternate" type="text/html" href="http://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Transport_and_magnetic_configuration&amp;action=history"/>
	<updated>2026-04-16T21:46:09Z</updated>
	<subtitle>Revision history for this page on the wiki</subtitle>
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	<entry>
		<id>http://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Transport_and_magnetic_configuration&amp;diff=4758&amp;oldid=prev</id>
		<title>Admin at 10:05, 25 November 2014</title>
		<link rel="alternate" type="text/html" href="http://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Transport_and_magnetic_configuration&amp;diff=4758&amp;oldid=prev"/>
		<updated>2014-11-25T10:05:36Z</updated>

		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;table style=&quot;background-color: #fff; color: #202122;&quot; data-mw=&quot;interface&quot;&gt;
				&lt;col class=&quot;diff-marker&quot; /&gt;
				&lt;col class=&quot;diff-content&quot; /&gt;
				&lt;col class=&quot;diff-marker&quot; /&gt;
				&lt;col class=&quot;diff-content&quot; /&gt;
				&lt;tr class=&quot;diff-title&quot; lang=&quot;en&quot;&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;Revision as of 12:05, 25 November 2014&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l5&quot;&gt;Line 5:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 5:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;The following issues contribute to the influence of the configuration on confinement:&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;The following issues contribute to the influence of the configuration on confinement:&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* The [[rotational transform]] &amp;lt;ref&amp;gt;E. Ascasíbar et al, &amp;#039;&amp;#039;Magnetic configuration and plasma parameter dependence of the energy confinement time in ECR heated plasmas from the TJ-II stellarator&amp;#039;&amp;#039;, [[doi:10.1088/0029-5515/45/4/009|Nucl. Fusion &amp;#039;&amp;#039;&amp;#039;45&amp;#039;&amp;#039;&amp;#039; (2005) 276-284]]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* The [[rotational transform]] &amp;lt;ref&amp;gt;E. Ascasíbar et al, &amp;#039;&amp;#039;Magnetic configuration and plasma parameter dependence of the energy confinement time in ECR heated plasmas from the TJ-II stellarator&amp;#039;&amp;#039;, [[doi:10.1088/0029-5515/45/4/009|Nucl. Fusion &amp;#039;&amp;#039;&amp;#039;45&amp;#039;&amp;#039;&amp;#039; (2005) 276-284]]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Rational surfaces &amp;lt;ref&amp;gt;D. López-Bruna et al, &#039;&#039;Tracking magnetic resonances in the effective electron heat diffusivity of ECH plasmas of the TJ-II Heliac&#039;&#039;, [[doi:10.1209/0295-5075/82/65002|EuroPhysics Letters &#039;&#039;&#039;82&#039;&#039;&#039; (2008) 65002]]&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;D. López-Bruna et al, &#039;&#039;First dynamic magnetic configuration scans in ECRH plasmas of the TJ-II Heliac&#039;&#039;, [[doi:10.1088/0029-5515/49/8/085016|Nucl. Fusion &#039;&#039;&#039;49&#039;&#039;&#039; (2009) 085016]]&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;D. López-Bruna et al, &#039;&#039;Magnetic Resonances in ECR-Heated Plasmas of the TJ-II Heliac&#039;&#039;, [[doi:10.1002/ctpp.200900005|Contrib. Plasma Phys. &#039;&#039;&#039;50&#039;&#039;&#039; (2010) 600]]&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;D. López-Bruna et al, &#039;&#039;Magnetic resonances and electric fields in the TJ-II Heliac&#039;&#039;, [[doi:10.1088/0741-3335/53/12/124022|Plasma Phys. Control. Fusion 53 (2011) 124022]]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Rational surfaces &amp;lt;ref&amp;gt;D. López-Bruna et al, &#039;&#039;Tracking magnetic resonances in the effective electron heat diffusivity of ECH plasmas of the TJ-II Heliac&#039;&#039;, [[doi:10.1209/0295-5075/82/65002|EuroPhysics Letters &#039;&#039;&#039;82&#039;&#039;&#039; (2008) 65002]]&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;D. López-Bruna et al, &#039;&#039;First dynamic magnetic configuration scans in ECRH plasmas of the TJ-II Heliac&#039;&#039;, [[doi:10.1088/0029-5515/49/8/085016|Nucl. Fusion &#039;&#039;&#039;49&#039;&#039;&#039; (2009) 085016]]&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;D. López-Bruna et al, &#039;&#039;Magnetic Resonances in ECR-Heated Plasmas of the TJ-II Heliac&#039;&#039;, [[doi:10.1002/ctpp.200900005|Contrib. Plasma Phys. &#039;&#039;&#039;50&#039;&#039;&#039; (2010) 600]]&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;D. López-Bruna et al, &#039;&#039;Magnetic resonances and electric fields in the TJ-II Heliac&#039;&#039;, [[doi:10.1088/0741-3335/53/12/124022|Plasma Phys. Control. Fusion 53 (2011) 124022&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;]]&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;D. López-Bruna et al, &#039;&#039;Relationship between MHD events, magnetic resonances and transport barriers in TJ-II plasmas&#039;&#039;, [[doi:10.1088/0029-5515/53/7/073051|Nucl. Fusion &#039;&#039;&#039;53&#039;&#039;&#039;, 7 (2013) 073051&lt;/ins&gt;]]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* [[Magnetic shear]] &amp;lt;ref&amp;gt;J.A. Romero et al, &amp;#039;&amp;#039;Controlling confinement with induced toroidal current in the flexible Heliac TJ-II&amp;#039;&amp;#039;, [[doi:10.1088/0029-5515/43/6/301|Nucl. Fusion &amp;#039;&amp;#039;&amp;#039;43&amp;#039;&amp;#039;&amp;#039; (2003) 387-392]]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;D. López-Bruna et al, &amp;#039;&amp;#039;Effects of ohmic current in the TJ-II stellarator&amp;#039;&amp;#039;, [[doi:10.1088/0029-5515/44/5/008|Nucl. Fusion &amp;#039;&amp;#039;&amp;#039;44&amp;#039;&amp;#039;&amp;#039;, 5 (2004) 645-654]]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* [[Magnetic shear]] &amp;lt;ref&amp;gt;J.A. Romero et al, &amp;#039;&amp;#039;Controlling confinement with induced toroidal current in the flexible Heliac TJ-II&amp;#039;&amp;#039;, [[doi:10.1088/0029-5515/43/6/301|Nucl. Fusion &amp;#039;&amp;#039;&amp;#039;43&amp;#039;&amp;#039;&amp;#039; (2003) 387-392]]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;D. López-Bruna et al, &amp;#039;&amp;#039;Effects of ohmic current in the TJ-II stellarator&amp;#039;&amp;#039;, [[doi:10.1088/0029-5515/44/5/008|Nucl. Fusion &amp;#039;&amp;#039;&amp;#039;44&amp;#039;&amp;#039;&amp;#039;, 5 (2004) 645-654]]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* [[Magnetic well]] &amp;lt;ref&amp;gt;C. Hidalgo et al, &amp;#039;&amp;#039;On the radial scale of fluctuations in the TJ-II stellarator&amp;#039;&amp;#039;, [[doi:10.1088/0741-3335/43/12A/324|Plasma Phys. Control. Fusion &amp;#039;&amp;#039;&amp;#039;43&amp;#039;&amp;#039;&amp;#039; (2001) A313-A321]]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;J. Castellano et al, &amp;#039;&amp;#039;Magnetic well and instability thresholds in the TJ-II stellarator&amp;#039;&amp;#039;, [[doi:10.1063/1.1430435|Phys. Plasmas &amp;#039;&amp;#039;&amp;#039;9&amp;#039;&amp;#039;&amp;#039; (2002) 713]]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;E. Ascasíbar et al, &amp;#039;&amp;#039;Confinement and stability on the TJ-II stellarator&amp;#039;&amp;#039;, [[doi:10.1088/0741-3335/44/12B/322|Plasma Phys. Control. Fusion &amp;#039;&amp;#039;&amp;#039;44&amp;#039;&amp;#039;&amp;#039; (2002) B307-B322]]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* [[Magnetic well]] &amp;lt;ref&amp;gt;C. Hidalgo et al, &amp;#039;&amp;#039;On the radial scale of fluctuations in the TJ-II stellarator&amp;#039;&amp;#039;, [[doi:10.1088/0741-3335/43/12A/324|Plasma Phys. Control. Fusion &amp;#039;&amp;#039;&amp;#039;43&amp;#039;&amp;#039;&amp;#039; (2001) A313-A321]]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;J. Castellano et al, &amp;#039;&amp;#039;Magnetic well and instability thresholds in the TJ-II stellarator&amp;#039;&amp;#039;, [[doi:10.1063/1.1430435|Phys. Plasmas &amp;#039;&amp;#039;&amp;#039;9&amp;#039;&amp;#039;&amp;#039; (2002) 713]]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;E. Ascasíbar et al, &amp;#039;&amp;#039;Confinement and stability on the TJ-II stellarator&amp;#039;&amp;#039;, [[doi:10.1088/0741-3335/44/12B/322|Plasma Phys. Control. Fusion &amp;#039;&amp;#039;&amp;#039;44&amp;#039;&amp;#039;&amp;#039; (2002) B307-B322]]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>http://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Transport_and_magnetic_configuration&amp;diff=4757&amp;oldid=prev</id>
		<title>Admin at 10:00, 25 November 2014</title>
		<link rel="alternate" type="text/html" href="http://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Transport_and_magnetic_configuration&amp;diff=4757&amp;oldid=prev"/>
		<updated>2014-11-25T10:00:31Z</updated>

		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;table style=&quot;background-color: #fff; color: #202122;&quot; data-mw=&quot;interface&quot;&gt;
				&lt;col class=&quot;diff-marker&quot; /&gt;
				&lt;col class=&quot;diff-content&quot; /&gt;
				&lt;col class=&quot;diff-marker&quot; /&gt;
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				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;Revision as of 12:00, 25 November 2014&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l1&quot;&gt;Line 1:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 1:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;A significant part of the research effort at [[TJ-II]] is dedicated to the study of the interaction between transport and the (flexible) magnetic configuration.&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;A significant part of the research effort at [[TJ-II]] is dedicated to the study of the interaction between transport and the (flexible) magnetic configuration.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;ref&amp;gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[[doi:10.1088/0741-3335/41/12B/307|&lt;/del&gt;C. Alejaldre et al, &#039;&#039;Confinement studies in the TJ-II stellarator&#039;&#039;, Plasma Phys. Control. Fusion &#039;&#039;&#039;41&#039;&#039;&#039; (1999) B109]]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;ref&amp;gt;C. Alejaldre et al, &#039;&#039;Confinement studies in the TJ-II stellarator&#039;&#039;, &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[[doi:10.1088/0741-3335/41/12B/307|&lt;/ins&gt;Plasma Phys. Control. Fusion &#039;&#039;&#039;41&#039;&#039;&#039; (1999) B109]]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;ref&amp;gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[[doi:10.1088/0741-3335/45/3/304|&lt;/del&gt;M.A. Ochando et al, &#039;&#039;Emissivity toroidal asymmetries induced by ECRH driven convective fluxes in the TJ-II stellarator&#039;&#039;, Plasma Phys. Control. Fusion &#039;&#039;&#039;45&#039;&#039;&#039; (2003) 221-231]]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;ref&amp;gt;M.A. Ochando et al, &#039;&#039;Emissivity toroidal asymmetries induced by ECRH driven convective fluxes in the TJ-II stellarator&#039;&#039;, &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[[doi:10.1088/0741-3335/45/3/304|&lt;/ins&gt;Plasma Phys. Control. Fusion &#039;&#039;&#039;45&#039;&#039;&#039; (2003) 221-231]]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;ref&amp;gt;[[doi:10.1088/0029-5515/45/10/S22|&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;C. Hidalgo et al, &#039;&#039;Overview of TJ-II experiments&#039;&#039;, &lt;/del&gt;Nucl. Fusion &#039;&#039;&#039;45&#039;&#039;&#039; (2005) S266-S275]]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;ref&amp;gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;C. Hidalgo et al, &#039;&#039;Overview of TJ-II experiments&#039;&#039;, &lt;/ins&gt;[[doi:10.1088/0029-5515/45/10/S22|Nucl. Fusion &#039;&#039;&#039;45&#039;&#039;&#039; (2005) S266-S275]]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;The following issues contribute to the influence of the configuration on confinement:&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;The following issues contribute to the influence of the configuration on confinement:&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* The [[rotational transform]] &amp;lt;ref&amp;gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[[doi:10.1088/0029-5515/45/4/009|&lt;/del&gt;E. Ascasíbar et al, &#039;&#039;Magnetic configuration and plasma parameter dependence of the energy confinement time in ECR heated plasmas from the TJ-II stellarator&#039;&#039;, Nucl. Fusion &#039;&#039;&#039;45&#039;&#039;&#039; (2005) 276-284]]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* The [[rotational transform]] &amp;lt;ref&amp;gt;E. Ascasíbar et al, &#039;&#039;Magnetic configuration and plasma parameter dependence of the energy confinement time in ECR heated plasmas from the TJ-II stellarator&#039;&#039;, &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[[doi:10.1088/0029-5515/45/4/009|&lt;/ins&gt;Nucl. Fusion &#039;&#039;&#039;45&#039;&#039;&#039; (2005) 276-284]]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Rational surfaces &amp;lt;ref&amp;gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[[doi:10.1209/0295-5075/82/65002|&lt;/del&gt;D. López-Bruna et al, &#039;&#039;Tracking magnetic resonances in the effective electron heat diffusivity of ECH plasmas of the TJ-II Heliac&#039;&#039;, EuroPhysics Letters &#039;&#039;&#039;82&#039;&#039;&#039; (2008) 65002]]&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[[doi:10.1088/0029-5515/49/8/085016|&lt;/del&gt;D. López-Bruna et al, &#039;&#039;First dynamic magnetic configuration scans in ECRH plasmas of the TJ-II Heliac&#039;&#039;, Nucl. Fusion &#039;&#039;&#039;49&#039;&#039;&#039; (2009) 085016]]&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[[doi:10.1002/ctpp.200900005|&lt;/del&gt;D. López-Bruna et al, &#039;&#039;Magnetic Resonances in ECR-Heated Plasmas of the TJ-II Heliac&#039;&#039;, Contrib. Plasma Phys. &#039;&#039;&#039;50&#039;&#039;&#039; (2010) 600]]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Rational surfaces &amp;lt;ref&amp;gt;D. López-Bruna et al, &#039;&#039;Tracking magnetic resonances in the effective electron heat diffusivity of ECH plasmas of the TJ-II Heliac&#039;&#039;, &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[[doi:10.1209/0295-5075/82/65002|&lt;/ins&gt;EuroPhysics Letters &#039;&#039;&#039;82&#039;&#039;&#039; (2008) 65002]]&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;D. López-Bruna et al, &#039;&#039;First dynamic magnetic configuration scans in ECRH plasmas of the TJ-II Heliac&#039;&#039;, &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[[doi:10.1088/0029-5515/49/8/085016|&lt;/ins&gt;Nucl. Fusion &#039;&#039;&#039;49&#039;&#039;&#039; (2009) 085016]]&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;D. López-Bruna et al, &#039;&#039;Magnetic Resonances in ECR-Heated Plasmas of the TJ-II Heliac&#039;&#039;, &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[[doi:10.1002/ctpp.200900005|&lt;/ins&gt;Contrib. Plasma Phys. &#039;&#039;&#039;50&#039;&#039;&#039; (2010) 600]]&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;D. López-Bruna et al, &#039;&#039;Magnetic resonances and electric fields in the TJ-II Heliac&#039;&#039;, &lt;/ins&gt;[[doi:10.1088/&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;0741&lt;/ins&gt;-&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;3335&lt;/ins&gt;/&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;53&lt;/ins&gt;/&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;12&lt;/ins&gt;/&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;124022&lt;/ins&gt;|&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;Plasma Phys. Control. Fusion 53 (2011) 124022]]&amp;lt;/ref&amp;gt;&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;* [[Magnetic shear]] &lt;/del&gt;&amp;lt;ref&amp;gt;[[doi:10.1088/&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;0029&lt;/del&gt;-&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;5515&lt;/del&gt;/&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;43&lt;/del&gt;/&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;6&lt;/del&gt;/&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;301&lt;/del&gt;|J.A. Romero et al, &#039;&#039;Controlling confinement with induced toroidal current in the flexible Heliac TJ-II&#039;&#039;, Nucl. Fusion &#039;&#039;&#039;43&#039;&#039;&#039; (2003) 387-392]]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[[doi:10.1088/0029-5515/44/5/008|&lt;/del&gt;D. López-Bruna et al, &#039;&#039;Effects of ohmic current in the TJ-II stellarator&#039;&#039;, Nucl. Fusion &#039;&#039;&#039;44&#039;&#039;&#039;, 5 (2004) 645-654]]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;* [[Magnetic shear]] &amp;lt;ref&amp;gt;&lt;/ins&gt;J.A. Romero et al, &#039;&#039;Controlling confinement with induced toroidal current in the flexible Heliac TJ-II&#039;&#039;, &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[[doi:10.1088/0029-5515/43/6/301|&lt;/ins&gt;Nucl. Fusion &#039;&#039;&#039;43&#039;&#039;&#039; (2003) 387-392]]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;D. López-Bruna et al, &#039;&#039;Effects of ohmic current in the TJ-II stellarator&#039;&#039;, &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[[doi:10.1088/0029-5515/44/5/008|&lt;/ins&gt;Nucl. Fusion &#039;&#039;&#039;44&#039;&#039;&#039;, 5 (2004) 645-654]]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* [[Magnetic well]] &amp;lt;ref&amp;gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[[doi:10.1088/0741-3335/43/12A/324|&lt;/del&gt;C. Hidalgo et al, &#039;&#039;On the radial scale of fluctuations in the TJ-II stellarator&#039;&#039;, Plasma Phys. Control. Fusion &#039;&#039;&#039;43&#039;&#039;&#039; (2001) A313-A321]]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[http://link.aip.org/link/?PHPAEN/9/713/1 &lt;/del&gt;J. Castellano et al, &#039;&#039;Magnetic well and instability thresholds in the TJ-II stellarator&#039;&#039;, Phys. Plasmas &#039;&#039;&#039;9&#039;&#039;&#039; (2002) 713]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[[doi:10.1088/0741-3335/44/12B/322|&lt;/del&gt;E. Ascasíbar et al, &#039;&#039;Confinement and stability on the TJ-II stellarator&#039;&#039;, Plasma Phys. Control. Fusion &#039;&#039;&#039;44&#039;&#039;&#039; (2002) B307-B322]]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* [[Magnetic well]] &amp;lt;ref&amp;gt;C. Hidalgo et al, &#039;&#039;On the radial scale of fluctuations in the TJ-II stellarator&#039;&#039;, &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[[doi:10.1088/0741-3335/43/12A/324|&lt;/ins&gt;Plasma Phys. Control. Fusion &#039;&#039;&#039;43&#039;&#039;&#039; (2001) A313-A321]]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;J. Castellano et al, &#039;&#039;Magnetic well and instability thresholds in the TJ-II stellarator&#039;&#039;, &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[[doi:10.1063/1.1430435|&lt;/ins&gt;Phys. Plasmas &#039;&#039;&#039;9&#039;&#039;&#039; (2002) 713&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;]&lt;/ins&gt;]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;E. Ascasíbar et al, &#039;&#039;Confinement and stability on the TJ-II stellarator&#039;&#039;, &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[[doi:10.1088/0741-3335/44/12B/322|&lt;/ins&gt;Plasma Phys. Control. Fusion &#039;&#039;&#039;44&#039;&#039;&#039; (2002) B307-B322]]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;The picture emerging from these studies is complex. In general, the presence of low-order rational surfaces in the plasma does not seem to be deleterious for transport; rather, local reductions of transport are observed (except at very low shear). Possibly, this is associated with the formation of [[TJ-II:Internal Transport Barriers|internal transport barriers]] at or near such rational surfaces, a consequence of the modification of the radial electric field by the rational surfaces themselves. It is being investigated whether the plasmas where this has been studied have the conditions for a self-healing state of the corresponding magnetic perturbations. On the other hand, the reduction of the magnetic well clearly enhances turbulence levels.&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;The picture emerging from these studies is complex. In general, the presence of low-order rational surfaces in the plasma does not seem to be deleterious for transport; rather, local reductions of transport are observed (except at very low shear). Possibly, this is associated with the formation of [[TJ-II:Internal Transport Barriers|internal transport barriers]] at or near such rational surfaces, a consequence of the modification of the radial electric field by the rational surfaces themselves. It is being investigated whether the plasmas where this has been studied have the conditions for a self-healing state of the corresponding magnetic perturbations. On the other hand, the reduction of the magnetic well clearly enhances turbulence levels.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>http://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Transport_and_magnetic_configuration&amp;diff=3558&amp;oldid=prev</id>
		<title>Admin at 18:50, 8 September 2011</title>
		<link rel="alternate" type="text/html" href="http://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Transport_and_magnetic_configuration&amp;diff=3558&amp;oldid=prev"/>
		<updated>2011-09-08T18:50:19Z</updated>

		<summary type="html">&lt;p&gt;&lt;/p&gt;
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				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;Revision as of 20:50, 8 September 2011&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l4&quot;&gt;Line 4:&lt;/td&gt;
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&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;ref&amp;gt;[[doi:10.1088/0029-5515/45/10/S22|C. Hidalgo et al, &amp;#039;&amp;#039;Overview of TJ-II experiments&amp;#039;&amp;#039;, Nucl. Fusion &amp;#039;&amp;#039;&amp;#039;45&amp;#039;&amp;#039;&amp;#039; (2005) S266-S275]]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;ref&amp;gt;[[doi:10.1088/0029-5515/45/10/S22|C. Hidalgo et al, &amp;#039;&amp;#039;Overview of TJ-II experiments&amp;#039;&amp;#039;, Nucl. Fusion &amp;#039;&amp;#039;&amp;#039;45&amp;#039;&amp;#039;&amp;#039; (2005) S266-S275]]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;The following issues contribute to the influence of the configuration on confinement:&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;The following issues contribute to the influence of the configuration on confinement:&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* The rotational transform &amp;lt;ref&amp;gt;[[doi:10.1088/0029-5515/45/4/009|E. Ascasíbar et al, &#039;&#039;Magnetic configuration and plasma parameter dependence of the energy confinement time in ECR heated plasmas from the TJ-II stellarator&#039;&#039;, Nucl. Fusion &#039;&#039;&#039;45&#039;&#039;&#039; (2005) 276-284]]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* The &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[[&lt;/ins&gt;rotational transform&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;]] &lt;/ins&gt;&amp;lt;ref&amp;gt;[[doi:10.1088/0029-5515/45/4/009|E. Ascasíbar et al, &#039;&#039;Magnetic configuration and plasma parameter dependence of the energy confinement time in ECR heated plasmas from the TJ-II stellarator&#039;&#039;, Nucl. Fusion &#039;&#039;&#039;45&#039;&#039;&#039; (2005) 276-284]]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Rational surfaces &amp;lt;ref&amp;gt;[[doi:10.1209/0295-5075/82/65002|D. López-Bruna et al, &amp;#039;&amp;#039;Tracking magnetic resonances in the effective electron heat diffusivity of ECH plasmas of the TJ-II Heliac&amp;#039;&amp;#039;, EuroPhysics Letters &amp;#039;&amp;#039;&amp;#039;82&amp;#039;&amp;#039;&amp;#039; (2008) 65002]]&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;[[doi:10.1088/0029-5515/49/8/085016|D. López-Bruna et al, &amp;#039;&amp;#039;First dynamic magnetic configuration scans in ECRH plasmas of the TJ-II Heliac&amp;#039;&amp;#039;, Nucl. Fusion &amp;#039;&amp;#039;&amp;#039;49&amp;#039;&amp;#039;&amp;#039; (2009) 085016]]&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;[[doi:10.1002/ctpp.200900005|D. López-Bruna et al, &amp;#039;&amp;#039;Magnetic Resonances in ECR-Heated Plasmas of the TJ-II Heliac&amp;#039;&amp;#039;, Contrib. Plasma Phys. &amp;#039;&amp;#039;&amp;#039;50&amp;#039;&amp;#039;&amp;#039; (2010) 600]]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Rational surfaces &amp;lt;ref&amp;gt;[[doi:10.1209/0295-5075/82/65002|D. López-Bruna et al, &amp;#039;&amp;#039;Tracking magnetic resonances in the effective electron heat diffusivity of ECH plasmas of the TJ-II Heliac&amp;#039;&amp;#039;, EuroPhysics Letters &amp;#039;&amp;#039;&amp;#039;82&amp;#039;&amp;#039;&amp;#039; (2008) 65002]]&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;[[doi:10.1088/0029-5515/49/8/085016|D. López-Bruna et al, &amp;#039;&amp;#039;First dynamic magnetic configuration scans in ECRH plasmas of the TJ-II Heliac&amp;#039;&amp;#039;, Nucl. Fusion &amp;#039;&amp;#039;&amp;#039;49&amp;#039;&amp;#039;&amp;#039; (2009) 085016]]&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;[[doi:10.1002/ctpp.200900005|D. López-Bruna et al, &amp;#039;&amp;#039;Magnetic Resonances in ECR-Heated Plasmas of the TJ-II Heliac&amp;#039;&amp;#039;, Contrib. Plasma Phys. &amp;#039;&amp;#039;&amp;#039;50&amp;#039;&amp;#039;&amp;#039; (2010) 600]]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* [[Magnetic shear]] &amp;lt;ref&amp;gt;[[doi:10.1088/0029-5515/43/6/301|J.A. Romero et al, &amp;#039;&amp;#039;Controlling confinement with induced toroidal current in the flexible Heliac TJ-II&amp;#039;&amp;#039;, Nucl. Fusion &amp;#039;&amp;#039;&amp;#039;43&amp;#039;&amp;#039;&amp;#039; (2003) 387-392]]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;[[doi:10.1088/0029-5515/44/5/008|D. López-Bruna et al, &amp;#039;&amp;#039;Effects of ohmic current in the TJ-II stellarator&amp;#039;&amp;#039;, Nucl. Fusion &amp;#039;&amp;#039;&amp;#039;44&amp;#039;&amp;#039;&amp;#039;, 5 (2004) 645-654]]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* [[Magnetic shear]] &amp;lt;ref&amp;gt;[[doi:10.1088/0029-5515/43/6/301|J.A. Romero et al, &amp;#039;&amp;#039;Controlling confinement with induced toroidal current in the flexible Heliac TJ-II&amp;#039;&amp;#039;, Nucl. Fusion &amp;#039;&amp;#039;&amp;#039;43&amp;#039;&amp;#039;&amp;#039; (2003) 387-392]]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;[[doi:10.1088/0029-5515/44/5/008|D. López-Bruna et al, &amp;#039;&amp;#039;Effects of ohmic current in the TJ-II stellarator&amp;#039;&amp;#039;, Nucl. Fusion &amp;#039;&amp;#039;&amp;#039;44&amp;#039;&amp;#039;&amp;#039;, 5 (2004) 645-654]]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>http://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Transport_and_magnetic_configuration&amp;diff=3557&amp;oldid=prev</id>
		<title>Admin at 18:48, 8 September 2011</title>
		<link rel="alternate" type="text/html" href="http://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Transport_and_magnetic_configuration&amp;diff=3557&amp;oldid=prev"/>
		<updated>2011-09-08T18:48:27Z</updated>

		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;table style=&quot;background-color: #fff; color: #202122;&quot; data-mw=&quot;interface&quot;&gt;
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				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;Revision as of 20:48, 8 September 2011&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l1&quot;&gt;Line 1:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 1:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;A significant part of the research effort at [[TJ-II]] is dedicated to the study of the interaction between transport and the (flexible) magnetic configuration.&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;A significant part of the research effort at [[TJ-II]] is dedicated to the study of the interaction between transport and the (flexible) magnetic configuration.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;ref&amp;gt;[&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;http&lt;/del&gt;:&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;//dx.doi.org/&lt;/del&gt;10.1088/0741-3335/41/12B/307 C. Alejaldre et al, &#039;&#039;Confinement studies in the TJ-II stellarator&#039;&#039;, Plasma Phys. Control. Fusion &#039;&#039;&#039;41&#039;&#039;&#039; (1999) B109]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;ref&amp;gt;[&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[doi&lt;/ins&gt;:10.1088/0741-3335/41/12B/307&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;|&lt;/ins&gt;C. Alejaldre et al, &#039;&#039;Confinement studies in the TJ-II stellarator&#039;&#039;, Plasma Phys. Control. Fusion &#039;&#039;&#039;41&#039;&#039;&#039; (1999) B109&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;]&lt;/ins&gt;]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;ref&amp;gt;[&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;http&lt;/del&gt;:&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;//dx.doi.org/&lt;/del&gt;10.1088/0741-3335/45/3/304 M.A. Ochando et al, &#039;&#039;Emissivity toroidal asymmetries induced by ECRH driven convective fluxes in the TJ-II stellarator&#039;&#039;, Plasma Phys. Control. Fusion &#039;&#039;&#039;45&#039;&#039;&#039; (2003) 221-231]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;ref&amp;gt;[&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[doi&lt;/ins&gt;:10.1088/0741-3335/45/3/304&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;|&lt;/ins&gt;M.A. Ochando et al, &#039;&#039;Emissivity toroidal asymmetries induced by ECRH driven convective fluxes in the TJ-II stellarator&#039;&#039;, Plasma Phys. Control. Fusion &#039;&#039;&#039;45&#039;&#039;&#039; (2003) 221-231&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;]&lt;/ins&gt;]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;ref&amp;gt;[&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;http&lt;/del&gt;:&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;//dx.doi.org/&lt;/del&gt;10.1088/0029-5515/45/10/S22 C. Hidalgo et al, &#039;&#039;Overview of TJ-II experiments&#039;&#039;, Nucl. Fusion &#039;&#039;&#039;45&#039;&#039;&#039; (2005) S266-S275]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;ref&amp;gt;[&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[doi&lt;/ins&gt;:10.1088/0029-5515/45/10/S22&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;|&lt;/ins&gt;C. Hidalgo et al, &#039;&#039;Overview of TJ-II experiments&#039;&#039;, Nucl. Fusion &#039;&#039;&#039;45&#039;&#039;&#039; (2005) S266-S275&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;]&lt;/ins&gt;]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;The following issues contribute to the influence of the configuration on confinement:&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;The following issues contribute to the influence of the configuration on confinement:&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* The rotational transform &amp;lt;ref&amp;gt;[&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;http&lt;/del&gt;:&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;//dx.doi.org/&lt;/del&gt;10.1088/0029-5515/45/4/009 E. Ascasíbar et al, &#039;&#039;Magnetic configuration and plasma parameter dependence of the energy confinement time in ECR heated plasmas from the TJ-II stellarator&#039;&#039;, Nucl. Fusion &#039;&#039;&#039;45&#039;&#039;&#039; (2005) 276-284]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* The rotational transform &amp;lt;ref&amp;gt;[&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[doi&lt;/ins&gt;:10.1088/0029-5515/45/4/009&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;|&lt;/ins&gt;E. Ascasíbar et al, &#039;&#039;Magnetic configuration and plasma parameter dependence of the energy confinement time in ECR heated plasmas from the TJ-II stellarator&#039;&#039;, Nucl. Fusion &#039;&#039;&#039;45&#039;&#039;&#039; (2005) 276-284&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;]&lt;/ins&gt;]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Rational surfaces &amp;lt;ref&amp;gt;[&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;http&lt;/del&gt;:&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;//dx.doi.org/&lt;/del&gt;10.1209/0295-5075/82/65002 D. López-Bruna et al, &#039;&#039;Tracking magnetic resonances in the effective electron heat diffusivity of ECH plasmas of the TJ-II Heliac&#039;&#039;, EuroPhysics Letters &#039;&#039;&#039;82&#039;&#039;&#039; (2008) 65002]&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;[&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;http://&lt;/del&gt;doi:10.1088/0029-5515/49/8/085016 D. López-Bruna et al, &#039;&#039;First dynamic magnetic configuration scans in ECRH plasmas of the TJ-II Heliac&#039;&#039;, Nucl. Fusion &#039;&#039;&#039;49&#039;&#039;&#039; (2009) 085016]&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;[&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;http&lt;/del&gt;:&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;//dx.doi.org/&lt;/del&gt;10.1002/ctpp.200900005 D. López-Bruna et al, &#039;&#039;Magnetic Resonances in ECR-Heated Plasmas of the TJ-II Heliac&#039;&#039;, Contrib. Plasma Phys. &#039;&#039;&#039;50&#039;&#039;&#039; (2010) 600]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Rational surfaces &amp;lt;ref&amp;gt;[&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[doi&lt;/ins&gt;:10.1209/0295-5075/82/65002&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;|&lt;/ins&gt;D. López-Bruna et al, &#039;&#039;Tracking magnetic resonances in the effective electron heat diffusivity of ECH plasmas of the TJ-II Heliac&#039;&#039;, EuroPhysics Letters &#039;&#039;&#039;82&#039;&#039;&#039; (2008) 65002&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;]&lt;/ins&gt;]&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;[&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[&lt;/ins&gt;doi:10.1088/0029-5515/49/8/085016&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;|&lt;/ins&gt;D. López-Bruna et al, &#039;&#039;First dynamic magnetic configuration scans in ECRH plasmas of the TJ-II Heliac&#039;&#039;, Nucl. Fusion &#039;&#039;&#039;49&#039;&#039;&#039; (2009) 085016&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;]&lt;/ins&gt;]&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;[&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[doi&lt;/ins&gt;:10.1002/ctpp.200900005&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;|&lt;/ins&gt;D. López-Bruna et al, &#039;&#039;Magnetic Resonances in ECR-Heated Plasmas of the TJ-II Heliac&#039;&#039;, Contrib. Plasma Phys. &#039;&#039;&#039;50&#039;&#039;&#039; (2010) 600&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;]&lt;/ins&gt;]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* [[Magnetic shear]] &amp;lt;ref&amp;gt;[&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;http&lt;/del&gt;:&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;//dx.doi.org/&lt;/del&gt;10.1088/0029-5515/43/6/301 J.A. Romero et al, &#039;&#039;Controlling confinement with induced toroidal current in the flexible Heliac TJ-II&#039;&#039;, Nucl. Fusion &#039;&#039;&#039;43&#039;&#039;&#039; (2003) 387-392]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;[&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;http&lt;/del&gt;:&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;//dx.doi.org/&lt;/del&gt;10.1088/0029-5515/44/5/008 D. López-Bruna et al, &#039;&#039;Effects of ohmic current in the TJ-II stellarator&#039;&#039;, Nucl. Fusion &#039;&#039;&#039;44&#039;&#039;&#039;, 5 (2004) 645-654]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* [[Magnetic shear]] &amp;lt;ref&amp;gt;[&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[doi&lt;/ins&gt;:10.1088/0029-5515/43/6/301&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;|&lt;/ins&gt;J.A. Romero et al, &#039;&#039;Controlling confinement with induced toroidal current in the flexible Heliac TJ-II&#039;&#039;, Nucl. Fusion &#039;&#039;&#039;43&#039;&#039;&#039; (2003) 387-392&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;]&lt;/ins&gt;]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;[&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[doi&lt;/ins&gt;:10.1088/0029-5515/44/5/008&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;|&lt;/ins&gt;D. López-Bruna et al, &#039;&#039;Effects of ohmic current in the TJ-II stellarator&#039;&#039;, Nucl. Fusion &#039;&#039;&#039;44&#039;&#039;&#039;, 5 (2004) 645-654&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;]&lt;/ins&gt;]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* [[Magnetic well]] &amp;lt;ref&amp;gt;[&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;http&lt;/del&gt;:&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;//dx.doi.org/&lt;/del&gt;10.1088/0741-3335/43/12A/324 C. Hidalgo et al, &#039;&#039;On the radial scale of fluctuations in the TJ-II stellarator&#039;&#039;, Plasma Phys. Control. Fusion &#039;&#039;&#039;43&#039;&#039;&#039; (2001) A313-A321]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;[http://link.aip.org/link/?PHPAEN/9/713/1 J. Castellano et al, &#039;&#039;Magnetic well and instability thresholds in the TJ-II stellarator&#039;&#039;, Phys. Plasmas &#039;&#039;&#039;9&#039;&#039;&#039; (2002) 713]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;[&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;http&lt;/del&gt;:&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;//dx.doi.org/&lt;/del&gt;10.1088/0741-3335/44/12B/322 E. Ascasíbar et al, &#039;&#039;Confinement and stability on the TJ-II stellarator&#039;&#039;, Plasma Phys. Control. Fusion &#039;&#039;&#039;44&#039;&#039;&#039; (2002) B307-B322]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* [[Magnetic well]] &amp;lt;ref&amp;gt;[&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[doi&lt;/ins&gt;:10.1088/0741-3335/43/12A/324&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;|&lt;/ins&gt;C. Hidalgo et al, &#039;&#039;On the radial scale of fluctuations in the TJ-II stellarator&#039;&#039;, Plasma Phys. Control. Fusion &#039;&#039;&#039;43&#039;&#039;&#039; (2001) A313-A321&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;]&lt;/ins&gt;]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;[http://link.aip.org/link/?PHPAEN/9/713/1 J. Castellano et al, &#039;&#039;Magnetic well and instability thresholds in the TJ-II stellarator&#039;&#039;, Phys. Plasmas &#039;&#039;&#039;9&#039;&#039;&#039; (2002) 713]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;[&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;[doi&lt;/ins&gt;:10.1088/0741-3335/44/12B/322&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;|&lt;/ins&gt;E. Ascasíbar et al, &#039;&#039;Confinement and stability on the TJ-II stellarator&#039;&#039;, Plasma Phys. Control. Fusion &#039;&#039;&#039;44&#039;&#039;&#039; (2002) B307-B322&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;]&lt;/ins&gt;]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;The picture emerging from these studies is complex. In general, the presence of low-order rational surfaces in the plasma does not seem to be deleterious for transport; rather, local reductions of transport are observed (except at very low shear). Possibly, this is associated with the formation of [[TJ-II:Internal Transport Barriers|internal transport barriers]] at or near such rational surfaces, a consequence of the modification of the radial electric field by the rational surfaces themselves. It is being investigated whether the plasmas where this has been studied have the conditions for a self-healing state of the corresponding magnetic perturbations. On the other hand, the reduction of the magnetic well clearly enhances turbulence levels.&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;The picture emerging from these studies is complex. In general, the presence of low-order rational surfaces in the plasma does not seem to be deleterious for transport; rather, local reductions of transport are observed (except at very low shear). Possibly, this is associated with the formation of [[TJ-II:Internal Transport Barriers|internal transport barriers]] at or near such rational surfaces, a consequence of the modification of the radial electric field by the rational surfaces themselves. It is being investigated whether the plasmas where this has been studied have the conditions for a self-healing state of the corresponding magnetic perturbations. On the other hand, the reduction of the magnetic well clearly enhances turbulence levels.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>http://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Transport_and_magnetic_configuration&amp;diff=3556&amp;oldid=prev</id>
		<title>Daniellopezbruna at 18:19, 8 September 2011</title>
		<link rel="alternate" type="text/html" href="http://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Transport_and_magnetic_configuration&amp;diff=3556&amp;oldid=prev"/>
		<updated>2011-09-08T18:19:57Z</updated>

		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;table style=&quot;background-color: #fff; color: #202122;&quot; data-mw=&quot;interface&quot;&gt;
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				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;Revision as of 20:19, 8 September 2011&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l5&quot;&gt;Line 5:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 5:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;The following issues contribute to the influence of the configuration on confinement:&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;The following issues contribute to the influence of the configuration on confinement:&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* The rotational transform &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0029-5515/45/4/009 E. Ascasíbar et al, &amp;#039;&amp;#039;Magnetic configuration and plasma parameter dependence of the energy confinement time in ECR heated plasmas from the TJ-II stellarator&amp;#039;&amp;#039;, Nucl. Fusion &amp;#039;&amp;#039;&amp;#039;45&amp;#039;&amp;#039;&amp;#039; (2005) 276-284]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* The rotational transform &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0029-5515/45/4/009 E. Ascasíbar et al, &amp;#039;&amp;#039;Magnetic configuration and plasma parameter dependence of the energy confinement time in ECR heated plasmas from the TJ-II stellarator&amp;#039;&amp;#039;, Nucl. Fusion &amp;#039;&amp;#039;&amp;#039;45&amp;#039;&amp;#039;&amp;#039; (2005) 276-284]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Rational surfaces &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1209/0295-5075/82/65002 D. López-Bruna et al, &#039;&#039;Tracking magnetic resonances in the effective electron heat diffusivity of ECH plasmas of the TJ-II Heliac&#039;&#039;, EuroPhysics Letters &#039;&#039;&#039;82&#039;&#039;&#039; (2008) 65002]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Rational surfaces &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1209/0295-5075/82/65002 D. López-Bruna et al, &#039;&#039;Tracking magnetic resonances in the effective electron heat diffusivity of ECH plasmas of the TJ-II Heliac&#039;&#039;, EuroPhysics Letters &#039;&#039;&#039;82&#039;&#039;&#039; (2008) 65002]&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;[http://doi:10.1088/0029-5515/49/8/085016 D. López-Bruna et al, &#039;&#039;First dynamic magnetic configuration scans in ECRH plasmas of the TJ-II Heliac&#039;&#039;, Nucl. Fusion &#039;&#039;&#039;49&#039;&#039;&#039; (2009) 085016]&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;[http://dx.doi.org/10.&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;1002&lt;/ins&gt;/&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;ctpp.200900005 &lt;/ins&gt;D. López-Bruna et al, &#039;&#039;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;Magnetic Resonances &lt;/ins&gt;in &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;ECR-Heated Plasmas &lt;/ins&gt;of the TJ-II Heliac&#039;&#039;, &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;Contrib. Plasma Phys. &lt;/ins&gt;&#039;&#039;&#039;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;50&lt;/ins&gt;&#039;&#039;&#039; (&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;2010&lt;/ins&gt;) &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;600&lt;/ins&gt;]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;ref&amp;gt;[http://doi:10.1088/0029-5515/49/8/085016 D. López-Bruna et al, &#039;&#039;First dynamic magnetic configuration scans in ECRH plasmas of the TJ-II Heliac&#039;&#039;, Nucl. Fusion &#039;&#039;&#039;49&#039;&#039;&#039; (2009) 085016]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-added&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;ref&amp;gt;[http://dx.doi.org/10.&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;1209&lt;/del&gt;/&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;0295-5075/82/65002 &lt;/del&gt;D. López-Bruna et al, &#039;&#039;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;Tracking magnetic resonances &lt;/del&gt;in &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;the effective electron heat diffusivity of ECH plasmas &lt;/del&gt;of the TJ-II Heliac&#039;&#039;, &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;EuroPhysics Letters &lt;/del&gt;&#039;&#039;&#039;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;82&lt;/del&gt;&#039;&#039;&#039; (&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;2008&lt;/del&gt;) &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;65002&lt;/del&gt;]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-added&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* [[Magnetic shear]] &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0029-5515/43/6/301 J.A. Romero et al, &amp;#039;&amp;#039;Controlling confinement with induced toroidal current in the flexible Heliac TJ-II&amp;#039;&amp;#039;, Nucl. Fusion &amp;#039;&amp;#039;&amp;#039;43&amp;#039;&amp;#039;&amp;#039; (2003) 387-392]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0029-5515/44/5/008 D. López-Bruna et al, &amp;#039;&amp;#039;Effects of ohmic current in the TJ-II stellarator&amp;#039;&amp;#039;, Nucl. Fusion &amp;#039;&amp;#039;&amp;#039;44&amp;#039;&amp;#039;&amp;#039;, 5 (2004) 645-654]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* [[Magnetic shear]] &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0029-5515/43/6/301 J.A. Romero et al, &amp;#039;&amp;#039;Controlling confinement with induced toroidal current in the flexible Heliac TJ-II&amp;#039;&amp;#039;, Nucl. Fusion &amp;#039;&amp;#039;&amp;#039;43&amp;#039;&amp;#039;&amp;#039; (2003) 387-392]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0029-5515/44/5/008 D. López-Bruna et al, &amp;#039;&amp;#039;Effects of ohmic current in the TJ-II stellarator&amp;#039;&amp;#039;, Nucl. Fusion &amp;#039;&amp;#039;&amp;#039;44&amp;#039;&amp;#039;&amp;#039;, 5 (2004) 645-654]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* [[Magnetic well]] &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0741-3335/43/12A/324 C. Hidalgo et al, &amp;#039;&amp;#039;On the radial scale of fluctuations in the TJ-II stellarator&amp;#039;&amp;#039;, Plasma Phys. Control. Fusion &amp;#039;&amp;#039;&amp;#039;43&amp;#039;&amp;#039;&amp;#039; (2001) A313-A321]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;[http://link.aip.org/link/?PHPAEN/9/713/1 J. Castellano et al, &amp;#039;&amp;#039;Magnetic well and instability thresholds in the TJ-II stellarator&amp;#039;&amp;#039;, Phys. Plasmas &amp;#039;&amp;#039;&amp;#039;9&amp;#039;&amp;#039;&amp;#039; (2002) 713]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0741-3335/44/12B/322 E. Ascasíbar et al, &amp;#039;&amp;#039;Confinement and stability on the TJ-II stellarator&amp;#039;&amp;#039;, Plasma Phys. Control. Fusion &amp;#039;&amp;#039;&amp;#039;44&amp;#039;&amp;#039;&amp;#039; (2002) B307-B322]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* [[Magnetic well]] &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0741-3335/43/12A/324 C. Hidalgo et al, &amp;#039;&amp;#039;On the radial scale of fluctuations in the TJ-II stellarator&amp;#039;&amp;#039;, Plasma Phys. Control. Fusion &amp;#039;&amp;#039;&amp;#039;43&amp;#039;&amp;#039;&amp;#039; (2001) A313-A321]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;[http://link.aip.org/link/?PHPAEN/9/713/1 J. Castellano et al, &amp;#039;&amp;#039;Magnetic well and instability thresholds in the TJ-II stellarator&amp;#039;&amp;#039;, Phys. Plasmas &amp;#039;&amp;#039;&amp;#039;9&amp;#039;&amp;#039;&amp;#039; (2002) 713]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0741-3335/44/12B/322 E. Ascasíbar et al, &amp;#039;&amp;#039;Confinement and stability on the TJ-II stellarator&amp;#039;&amp;#039;, Plasma Phys. Control. Fusion &amp;#039;&amp;#039;&amp;#039;44&amp;#039;&amp;#039;&amp;#039; (2002) B307-B322]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Daniellopezbruna</name></author>
	</entry>
	<entry>
		<id>http://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Transport_and_magnetic_configuration&amp;diff=3555&amp;oldid=prev</id>
		<title>Daniellopezbruna at 18:14, 8 September 2011</title>
		<link rel="alternate" type="text/html" href="http://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Transport_and_magnetic_configuration&amp;diff=3555&amp;oldid=prev"/>
		<updated>2011-09-08T18:14:47Z</updated>

		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;table style=&quot;background-color: #fff; color: #202122;&quot; data-mw=&quot;interface&quot;&gt;
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				&lt;col class=&quot;diff-content&quot; /&gt;
				&lt;tr class=&quot;diff-title&quot; lang=&quot;en&quot;&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;Revision as of 20:14, 8 September 2011&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l6&quot;&gt;Line 6:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 6:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* The rotational transform &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0029-5515/45/4/009 E. Ascasíbar et al, &amp;#039;&amp;#039;Magnetic configuration and plasma parameter dependence of the energy confinement time in ECR heated plasmas from the TJ-II stellarator&amp;#039;&amp;#039;, Nucl. Fusion &amp;#039;&amp;#039;&amp;#039;45&amp;#039;&amp;#039;&amp;#039; (2005) 276-284]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* The rotational transform &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0029-5515/45/4/009 E. Ascasíbar et al, &amp;#039;&amp;#039;Magnetic configuration and plasma parameter dependence of the energy confinement time in ECR heated plasmas from the TJ-II stellarator&amp;#039;&amp;#039;, Nucl. Fusion &amp;#039;&amp;#039;&amp;#039;45&amp;#039;&amp;#039;&amp;#039; (2005) 276-284]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Rational surfaces &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1209/0295-5075/82/65002 D. López-Bruna et al, &amp;#039;&amp;#039;Tracking magnetic resonances in the effective electron heat diffusivity of ECH plasmas of the TJ-II Heliac&amp;#039;&amp;#039;, EuroPhysics Letters &amp;#039;&amp;#039;&amp;#039;82&amp;#039;&amp;#039;&amp;#039; (2008) 65002]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Rational surfaces &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1209/0295-5075/82/65002 D. López-Bruna et al, &amp;#039;&amp;#039;Tracking magnetic resonances in the effective electron heat diffusivity of ECH plasmas of the TJ-II Heliac&amp;#039;&amp;#039;, EuroPhysics Letters &amp;#039;&amp;#039;&amp;#039;82&amp;#039;&amp;#039;&amp;#039; (2008) 65002]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-deleted&quot;&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&amp;lt;ref&amp;gt;[http://doi:10.1088/0029-5515/49/8/085016 D. López-Bruna et al, &#039;&#039;First dynamic magnetic configuration scans in ECRH plasmas of the TJ-II Heliac&#039;&#039;, Nucl. Fusion &#039;&#039;&#039;49&#039;&#039;&#039; (2009) 085016]&amp;lt;/ref&amp;gt;&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-deleted&quot;&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1209/0295-5075/82/65002 D. López-Bruna et al, &#039;&#039;Tracking magnetic resonances in the effective electron heat diffusivity of ECH plasmas of the TJ-II Heliac&#039;&#039;, EuroPhysics Letters &#039;&#039;&#039;82&#039;&#039;&#039; (2008) 65002]&amp;lt;/ref&amp;gt;&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* [[Magnetic shear]] &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0029-5515/43/6/301 J.A. Romero et al, &amp;#039;&amp;#039;Controlling confinement with induced toroidal current in the flexible Heliac TJ-II&amp;#039;&amp;#039;, Nucl. Fusion &amp;#039;&amp;#039;&amp;#039;43&amp;#039;&amp;#039;&amp;#039; (2003) 387-392]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0029-5515/44/5/008 D. López-Bruna et al, &amp;#039;&amp;#039;Effects of ohmic current in the TJ-II stellarator&amp;#039;&amp;#039;, Nucl. Fusion &amp;#039;&amp;#039;&amp;#039;44&amp;#039;&amp;#039;&amp;#039;, 5 (2004) 645-654]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* [[Magnetic shear]] &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0029-5515/43/6/301 J.A. Romero et al, &amp;#039;&amp;#039;Controlling confinement with induced toroidal current in the flexible Heliac TJ-II&amp;#039;&amp;#039;, Nucl. Fusion &amp;#039;&amp;#039;&amp;#039;43&amp;#039;&amp;#039;&amp;#039; (2003) 387-392]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0029-5515/44/5/008 D. López-Bruna et al, &amp;#039;&amp;#039;Effects of ohmic current in the TJ-II stellarator&amp;#039;&amp;#039;, Nucl. Fusion &amp;#039;&amp;#039;&amp;#039;44&amp;#039;&amp;#039;&amp;#039;, 5 (2004) 645-654]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* [[Magnetic well]] &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0741-3335/43/12A/324 C. Hidalgo et al, &amp;#039;&amp;#039;On the radial scale of fluctuations in the TJ-II stellarator&amp;#039;&amp;#039;, Plasma Phys. Control. Fusion &amp;#039;&amp;#039;&amp;#039;43&amp;#039;&amp;#039;&amp;#039; (2001) A313-A321]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;[http://link.aip.org/link/?PHPAEN/9/713/1 J. Castellano et al, &amp;#039;&amp;#039;Magnetic well and instability thresholds in the TJ-II stellarator&amp;#039;&amp;#039;, Phys. Plasmas &amp;#039;&amp;#039;&amp;#039;9&amp;#039;&amp;#039;&amp;#039; (2002) 713]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0741-3335/44/12B/322 E. Ascasíbar et al, &amp;#039;&amp;#039;Confinement and stability on the TJ-II stellarator&amp;#039;&amp;#039;, Plasma Phys. Control. Fusion &amp;#039;&amp;#039;&amp;#039;44&amp;#039;&amp;#039;&amp;#039; (2002) B307-B322]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* [[Magnetic well]] &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0741-3335/43/12A/324 C. Hidalgo et al, &amp;#039;&amp;#039;On the radial scale of fluctuations in the TJ-II stellarator&amp;#039;&amp;#039;, Plasma Phys. Control. Fusion &amp;#039;&amp;#039;&amp;#039;43&amp;#039;&amp;#039;&amp;#039; (2001) A313-A321]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;[http://link.aip.org/link/?PHPAEN/9/713/1 J. Castellano et al, &amp;#039;&amp;#039;Magnetic well and instability thresholds in the TJ-II stellarator&amp;#039;&amp;#039;, Phys. Plasmas &amp;#039;&amp;#039;&amp;#039;9&amp;#039;&amp;#039;&amp;#039; (2002) 713]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0741-3335/44/12B/322 E. Ascasíbar et al, &amp;#039;&amp;#039;Confinement and stability on the TJ-II stellarator&amp;#039;&amp;#039;, Plasma Phys. Control. Fusion &amp;#039;&amp;#039;&amp;#039;44&amp;#039;&amp;#039;&amp;#039; (2002) B307-B322]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Daniellopezbruna</name></author>
	</entry>
	<entry>
		<id>http://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Transport_and_magnetic_configuration&amp;diff=2369&amp;oldid=prev</id>
		<title>130.206.11.82 at 19:08, 28 July 2010</title>
		<link rel="alternate" type="text/html" href="http://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Transport_and_magnetic_configuration&amp;diff=2369&amp;oldid=prev"/>
		<updated>2010-07-28T19:08:21Z</updated>

		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;table style=&quot;background-color: #fff; color: #202122;&quot; data-mw=&quot;interface&quot;&gt;
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				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;Revision as of 21:08, 28 July 2010&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l9&quot;&gt;Line 9:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 9:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* [[Magnetic well]] &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0741-3335/43/12A/324 C. Hidalgo et al, &amp;#039;&amp;#039;On the radial scale of fluctuations in the TJ-II stellarator&amp;#039;&amp;#039;, Plasma Phys. Control. Fusion &amp;#039;&amp;#039;&amp;#039;43&amp;#039;&amp;#039;&amp;#039; (2001) A313-A321]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;[http://link.aip.org/link/?PHPAEN/9/713/1 J. Castellano et al, &amp;#039;&amp;#039;Magnetic well and instability thresholds in the TJ-II stellarator&amp;#039;&amp;#039;, Phys. Plasmas &amp;#039;&amp;#039;&amp;#039;9&amp;#039;&amp;#039;&amp;#039; (2002) 713]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0741-3335/44/12B/322 E. Ascasíbar et al, &amp;#039;&amp;#039;Confinement and stability on the TJ-II stellarator&amp;#039;&amp;#039;, Plasma Phys. Control. Fusion &amp;#039;&amp;#039;&amp;#039;44&amp;#039;&amp;#039;&amp;#039; (2002) B307-B322]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* [[Magnetic well]] &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0741-3335/43/12A/324 C. Hidalgo et al, &amp;#039;&amp;#039;On the radial scale of fluctuations in the TJ-II stellarator&amp;#039;&amp;#039;, Plasma Phys. Control. Fusion &amp;#039;&amp;#039;&amp;#039;43&amp;#039;&amp;#039;&amp;#039; (2001) A313-A321]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;[http://link.aip.org/link/?PHPAEN/9/713/1 J. Castellano et al, &amp;#039;&amp;#039;Magnetic well and instability thresholds in the TJ-II stellarator&amp;#039;&amp;#039;, Phys. Plasmas &amp;#039;&amp;#039;&amp;#039;9&amp;#039;&amp;#039;&amp;#039; (2002) 713]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0741-3335/44/12B/322 E. Ascasíbar et al, &amp;#039;&amp;#039;Confinement and stability on the TJ-II stellarator&amp;#039;&amp;#039;, Plasma Phys. Control. Fusion &amp;#039;&amp;#039;&amp;#039;44&amp;#039;&amp;#039;&amp;#039; (2002) B307-B322]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;The picture emerging from these studies is complex. In general, the presence of low-order rational surfaces in the plasma does not seem to be deleterious for transport; rather, local reductions of transport are observed (except at very low shear). Possibly, this is associated with the formation of [[TJ-II:Internal Transport Barriers|internal transport barriers]] at or near such rational surfaces. On the other hand, the reduction of the magnetic well clearly enhances turbulence levels.&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;The picture emerging from these studies is complex. In general, the presence of low-order rational surfaces in the plasma does not seem to be deleterious for transport; rather, local reductions of transport are observed (except at very low shear). Possibly, this is associated with the formation of [[TJ-II:Internal Transport Barriers|internal transport barriers]] at or near such rational surfaces&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;, a consequence of the modification of the radial electric field by the rational surfaces themselves. It is being investigated whether the plasmas where this has been studied have the conditions for a self-healing state of the corresponding magnetic perturbations&lt;/ins&gt;. On the other hand, the reduction of the magnetic well clearly enhances turbulence levels.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;== References ==&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;== References ==&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;references /&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;references /&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>130.206.11.82</name></author>
	</entry>
	<entry>
		<id>http://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Transport_and_magnetic_configuration&amp;diff=982&amp;oldid=prev</id>
		<title>Admin at 07:59, 24 August 2009</title>
		<link rel="alternate" type="text/html" href="http://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Transport_and_magnetic_configuration&amp;diff=982&amp;oldid=prev"/>
		<updated>2009-08-24T07:59:26Z</updated>

		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;table style=&quot;background-color: #fff; color: #202122;&quot; data-mw=&quot;interface&quot;&gt;
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				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;Revision as of 09:59, 24 August 2009&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l6&quot;&gt;Line 6:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 6:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* The rotational transform &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0029-5515/45/4/009 E. Ascasíbar et al, &amp;#039;&amp;#039;Magnetic configuration and plasma parameter dependence of the energy confinement time in ECR heated plasmas from the TJ-II stellarator&amp;#039;&amp;#039;, Nucl. Fusion &amp;#039;&amp;#039;&amp;#039;45&amp;#039;&amp;#039;&amp;#039; (2005) 276-284]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* The rotational transform &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0029-5515/45/4/009 E. Ascasíbar et al, &amp;#039;&amp;#039;Magnetic configuration and plasma parameter dependence of the energy confinement time in ECR heated plasmas from the TJ-II stellarator&amp;#039;&amp;#039;, Nucl. Fusion &amp;#039;&amp;#039;&amp;#039;45&amp;#039;&amp;#039;&amp;#039; (2005) 276-284]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Rational surfaces &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1209/0295-5075/82/65002 D. López-Bruna et al, &amp;#039;&amp;#039;Tracking magnetic resonances in the effective electron heat diffusivity of ECH plasmas of the TJ-II Heliac&amp;#039;&amp;#039;, EuroPhysics Letters &amp;#039;&amp;#039;&amp;#039;82&amp;#039;&amp;#039;&amp;#039; (2008) 65002]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Rational surfaces &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1209/0295-5075/82/65002 D. López-Bruna et al, &amp;#039;&amp;#039;Tracking magnetic resonances in the effective electron heat diffusivity of ECH plasmas of the TJ-II Heliac&amp;#039;&amp;#039;, EuroPhysics Letters &amp;#039;&amp;#039;&amp;#039;82&amp;#039;&amp;#039;&amp;#039; (2008) 65002]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* [[Magnetic shear]] &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0029-5515/44/5/008 D. López-Bruna et al, &#039;&#039;Effects of ohmic current in the TJ-II stellarator&#039;&#039;, Nucl. Fusion &#039;&#039;&#039;44&#039;&#039;&#039;, 5 (2004) 645-654]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* [[Magnetic shear]] &lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0029-5515/43/6/301 J.A. Romero et al, &#039;&#039;Controlling confinement with induced toroidal current in the flexible Heliac TJ-II&#039;&#039;, Nucl. Fusion &#039;&#039;&#039;43&#039;&#039;&#039; (2003) 387-392]&amp;lt;/ref&amp;gt; &lt;/ins&gt;&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0029-5515/44/5/008 D. López-Bruna et al, &#039;&#039;Effects of ohmic current in the TJ-II stellarator&#039;&#039;, Nucl. Fusion &#039;&#039;&#039;44&#039;&#039;&#039;, 5 (2004) 645-654]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* [[Magnetic well]] &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0741-3335/43/12A/324 C. Hidalgo et al, &amp;#039;&amp;#039;On the radial scale of fluctuations in the TJ-II stellarator&amp;#039;&amp;#039;, Plasma Phys. Control. Fusion &amp;#039;&amp;#039;&amp;#039;43&amp;#039;&amp;#039;&amp;#039; (2001) A313-A321]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;[http://link.aip.org/link/?PHPAEN/9/713/1 J. Castellano et al, &amp;#039;&amp;#039;Magnetic well and instability thresholds in the TJ-II stellarator&amp;#039;&amp;#039;, Phys. Plasmas &amp;#039;&amp;#039;&amp;#039;9&amp;#039;&amp;#039;&amp;#039; (2002) 713]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0741-3335/44/12B/322 E. Ascasíbar et al, &amp;#039;&amp;#039;Confinement and stability on the TJ-II stellarator&amp;#039;&amp;#039;, Plasma Phys. Control. Fusion &amp;#039;&amp;#039;&amp;#039;44&amp;#039;&amp;#039;&amp;#039; (2002) B307-B322]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* [[Magnetic well]] &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0741-3335/43/12A/324 C. Hidalgo et al, &amp;#039;&amp;#039;On the radial scale of fluctuations in the TJ-II stellarator&amp;#039;&amp;#039;, Plasma Phys. Control. Fusion &amp;#039;&amp;#039;&amp;#039;43&amp;#039;&amp;#039;&amp;#039; (2001) A313-A321]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;[http://link.aip.org/link/?PHPAEN/9/713/1 J. Castellano et al, &amp;#039;&amp;#039;Magnetic well and instability thresholds in the TJ-II stellarator&amp;#039;&amp;#039;, Phys. Plasmas &amp;#039;&amp;#039;&amp;#039;9&amp;#039;&amp;#039;&amp;#039; (2002) 713]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0741-3335/44/12B/322 E. Ascasíbar et al, &amp;#039;&amp;#039;Confinement and stability on the TJ-II stellarator&amp;#039;&amp;#039;, Plasma Phys. Control. Fusion &amp;#039;&amp;#039;&amp;#039;44&amp;#039;&amp;#039;&amp;#039; (2002) B307-B322]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>http://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Transport_and_magnetic_configuration&amp;diff=981&amp;oldid=prev</id>
		<title>Admin at 06:22, 24 August 2009</title>
		<link rel="alternate" type="text/html" href="http://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Transport_and_magnetic_configuration&amp;diff=981&amp;oldid=prev"/>
		<updated>2009-08-24T06:22:03Z</updated>

		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;table style=&quot;background-color: #fff; color: #202122;&quot; data-mw=&quot;interface&quot;&gt;
				&lt;col class=&quot;diff-marker&quot; /&gt;
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				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;Revision as of 08:22, 24 August 2009&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l3&quot;&gt;Line 3:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 3:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0741-3335/45/3/304 M.A. Ochando et al, &amp;#039;&amp;#039;Emissivity toroidal asymmetries induced by ECRH driven convective fluxes in the TJ-II stellarator&amp;#039;&amp;#039;, Plasma Phys. Control. Fusion &amp;#039;&amp;#039;&amp;#039;45&amp;#039;&amp;#039;&amp;#039; (2003) 221-231]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0741-3335/45/3/304 M.A. Ochando et al, &amp;#039;&amp;#039;Emissivity toroidal asymmetries induced by ECRH driven convective fluxes in the TJ-II stellarator&amp;#039;&amp;#039;, Plasma Phys. Control. Fusion &amp;#039;&amp;#039;&amp;#039;45&amp;#039;&amp;#039;&amp;#039; (2003) 221-231]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0029-5515/45/10/S22 C. Hidalgo et al, &amp;#039;&amp;#039;Overview of TJ-II experiments&amp;#039;&amp;#039;, Nucl. Fusion &amp;#039;&amp;#039;&amp;#039;45&amp;#039;&amp;#039;&amp;#039; (2005) S266-S275]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0029-5515/45/10/S22 C. Hidalgo et al, &amp;#039;&amp;#039;Overview of TJ-II experiments&amp;#039;&amp;#039;, Nucl. Fusion &amp;#039;&amp;#039;&amp;#039;45&amp;#039;&amp;#039;&amp;#039; (2005) S266-S275]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0029-5515/45/4/009 E. Ascasíbar et al, &#039;&#039;Magnetic configuration and plasma parameter dependence of the energy confinement time in ECR heated plasmas from the TJ-II stellarator&#039;&#039;, Nucl. Fusion &#039;&#039;&#039;45&#039;&#039;&#039; (2005) 276-284]&amp;lt;/ref&amp;gt;&lt;/del&gt;&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-added&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;The following issues contribute to the influence of the configuration on confinement:&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;The following issues contribute to the influence of the configuration on confinement:&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-deleted&quot;&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;* The rotational transform &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0029-5515/45/4/009 E. Ascasíbar et al, &#039;&#039;Magnetic configuration and plasma parameter dependence of the energy confinement time in ECR heated plasmas from the TJ-II stellarator&#039;&#039;, Nucl. Fusion &#039;&#039;&#039;45&#039;&#039;&#039; (2005) 276-284]&amp;lt;/ref&amp;gt;&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Rational surfaces &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1209/0295-5075/82/65002 D. López-Bruna et al, &amp;#039;&amp;#039;Tracking magnetic resonances in the effective electron heat diffusivity of ECH plasmas of the TJ-II Heliac&amp;#039;&amp;#039;, EuroPhysics Letters &amp;#039;&amp;#039;&amp;#039;82&amp;#039;&amp;#039;&amp;#039; (2008) 65002]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Rational surfaces &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1209/0295-5075/82/65002 D. López-Bruna et al, &amp;#039;&amp;#039;Tracking magnetic resonances in the effective electron heat diffusivity of ECH plasmas of the TJ-II Heliac&amp;#039;&amp;#039;, EuroPhysics Letters &amp;#039;&amp;#039;&amp;#039;82&amp;#039;&amp;#039;&amp;#039; (2008) 65002]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* [[Magnetic shear]] &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0029-5515/44/5/008 D. López-Bruna et al, &amp;#039;&amp;#039;Effects of ohmic current in the TJ-II stellarator&amp;#039;&amp;#039;, Nucl. Fusion &amp;#039;&amp;#039;&amp;#039;44&amp;#039;&amp;#039;&amp;#039;, 5 (2004) 645-654]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* [[Magnetic shear]] &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0029-5515/44/5/008 D. López-Bruna et al, &amp;#039;&amp;#039;Effects of ohmic current in the TJ-II stellarator&amp;#039;&amp;#039;, Nucl. Fusion &amp;#039;&amp;#039;&amp;#039;44&amp;#039;&amp;#039;&amp;#039;, 5 (2004) 645-654]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
	<entry>
		<id>http://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Transport_and_magnetic_configuration&amp;diff=980&amp;oldid=prev</id>
		<title>Admin at 19:05, 23 August 2009</title>
		<link rel="alternate" type="text/html" href="http://wiki.fusenet.eu/fusionwiki/index.php?title=TJ-II:Transport_and_magnetic_configuration&amp;diff=980&amp;oldid=prev"/>
		<updated>2009-08-23T19:05:15Z</updated>

		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;table style=&quot;background-color: #fff; color: #202122;&quot; data-mw=&quot;interface&quot;&gt;
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				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;Revision as of 21:05, 23 August 2009&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l9&quot;&gt;Line 9:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 9:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* [[Magnetic well]] &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0741-3335/43/12A/324 C. Hidalgo et al, &amp;#039;&amp;#039;On the radial scale of fluctuations in the TJ-II stellarator&amp;#039;&amp;#039;, Plasma Phys. Control. Fusion &amp;#039;&amp;#039;&amp;#039;43&amp;#039;&amp;#039;&amp;#039; (2001) A313-A321]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;[http://link.aip.org/link/?PHPAEN/9/713/1 J. Castellano et al, &amp;#039;&amp;#039;Magnetic well and instability thresholds in the TJ-II stellarator&amp;#039;&amp;#039;, Phys. Plasmas &amp;#039;&amp;#039;&amp;#039;9&amp;#039;&amp;#039;&amp;#039; (2002) 713]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0741-3335/44/12B/322 E. Ascasíbar et al, &amp;#039;&amp;#039;Confinement and stability on the TJ-II stellarator&amp;#039;&amp;#039;, Plasma Phys. Control. Fusion &amp;#039;&amp;#039;&amp;#039;44&amp;#039;&amp;#039;&amp;#039; (2002) B307-B322]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* [[Magnetic well]] &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0741-3335/43/12A/324 C. Hidalgo et al, &amp;#039;&amp;#039;On the radial scale of fluctuations in the TJ-II stellarator&amp;#039;&amp;#039;, Plasma Phys. Control. Fusion &amp;#039;&amp;#039;&amp;#039;43&amp;#039;&amp;#039;&amp;#039; (2001) A313-A321]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;[http://link.aip.org/link/?PHPAEN/9/713/1 J. Castellano et al, &amp;#039;&amp;#039;Magnetic well and instability thresholds in the TJ-II stellarator&amp;#039;&amp;#039;, Phys. Plasmas &amp;#039;&amp;#039;&amp;#039;9&amp;#039;&amp;#039;&amp;#039; (2002) 713]&amp;lt;/ref&amp;gt; &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0741-3335/44/12B/322 E. Ascasíbar et al, &amp;#039;&amp;#039;Confinement and stability on the TJ-II stellarator&amp;#039;&amp;#039;, Plasma Phys. Control. Fusion &amp;#039;&amp;#039;&amp;#039;44&amp;#039;&amp;#039;&amp;#039; (2002) B307-B322]&amp;lt;/ref&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-deleted&quot;&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;The picture emerging from these studies is complex. In general, the presence of low-order rational surfaces in the plasma does not seem to be deleterious for transport; rather, local reductions of transport are observed (except at very low shear). Possibly, this is associated with the formation of [[TJ-II:Internal Transport Barriers|internal transport barriers]] at or near such rational surfaces. On the other hand, the reduction of the magnetic well clearly enhances turbulence levels.&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;== References ==&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;== References ==&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;references /&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;references /&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Admin</name></author>
	</entry>
</feed>