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	<title>Effective charge state - Revision history</title>
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	<updated>2026-05-20T12:48:08Z</updated>
	<subtitle>Revision history for this page on the wiki</subtitle>
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		<title>Eldond: Created page with &quot;The effective charge state of ions in a plasma &lt;math&gt;Z_{eff}&lt;/math&gt; is important to many physical processes. :&lt;math&gt;Z_{eff} = \frac{\sum_i n_i Z^2_i}{\sum_i n_i Z_i}&lt;/math&gt; wh...&quot;</title>
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		<updated>2023-03-29T20:22:01Z</updated>

		<summary type="html">&lt;p&gt;Created page with &amp;quot;The effective charge state of ions in a plasma &amp;lt;math&amp;gt;Z_{eff}&amp;lt;/math&amp;gt; is important to many physical processes. :&amp;lt;math&amp;gt;Z_{eff} = \frac{\sum_i n_i Z^2_i}{\sum_i n_i Z_i}&amp;lt;/math&amp;gt; wh...&amp;quot;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;The effective charge state of ions in a plasma &amp;lt;math&amp;gt;Z_{eff}&amp;lt;/math&amp;gt; is important to many physical processes.&lt;br /&gt;
:&amp;lt;math&amp;gt;Z_{eff} = \frac{\sum_i n_i Z^2_i}{\sum_i n_i Z_i}&amp;lt;/math&amp;gt;&lt;br /&gt;
where &amp;lt;math&amp;gt;n_i&amp;lt;/math&amp;gt; is ion density for species &amp;lt;math&amp;gt;i&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;Z_i&amp;lt;/math&amp;gt; is the charge state of species &amp;lt;math&amp;gt;i&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\sum_i n_i Z_i = n_e &amp;lt;/math&amp;gt; by quasi-neutrality, so&lt;br /&gt;
:&amp;lt;math&amp;gt;Z_{eff} = \frac{\sum_i n_i Z^2_i}{n_e}&amp;lt;/math&amp;gt;&lt;br /&gt;
&amp;lt;math&amp;gt;Z_{eff}&amp;lt;/math&amp;gt; would be 1 for a plasma composed purely of hydrogen isotopes, but in practice is always higher due to impurities from plasma facing components.&lt;br /&gt;
&amp;lt;math&amp;gt;Z_{eff}=2&amp;lt;/math&amp;gt; is a common baseline assumption for carbon-walled tokamaks,&amp;lt;ref&amp;gt;[[doi:10.1088/0029-5515/39/11Y/338|T.N. Carlstrom, et al., Nucl. Fusion &amp;#039;&amp;#039;&amp;#039;39&amp;#039;&amp;#039;&amp;#039; (1999) 1941]]&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;[[doi:10.1103/PhysRevLett.107.215001|T. Eich, et al., Phys. Rev. Lett. &amp;#039;&amp;#039;&amp;#039;107&amp;#039;&amp;#039;&amp;#039; (2011) 215001]]&amp;lt;/ref&amp;gt; and some multi-device databases are restricted to cases with low-ish &amp;lt;math&amp;gt;Z_{eff}&amp;lt;/math&amp;gt;&amp;lt;ref&amp;gt;[[doi:10.1063/1.866892|ITER Physics Basis Chapter 2: Plasma confinement and transport, Nucl. Fusion &amp;#039;&amp;#039;&amp;#039;39&amp;#039;&amp;#039;&amp;#039; (1999) 2175]]&amp;lt;/ref&amp;gt;, making their scaling laws valid for &amp;lt;math&amp;gt;Z_{eff}&amp;lt;3&amp;lt;/math&amp;gt; and questionable for higher &amp;lt;math&amp;gt;Z_{eff}&amp;lt;/math&amp;gt;.&lt;br /&gt;
The 1999 ITER physics basis estimates &amp;lt;math&amp;gt;Z_{eff}=1.8-1.9&amp;lt;/math&amp;gt;;&amp;lt;ref&amp;gt;[[doi:10.1088/0029-5515/39/12/301|ITER Physics Basis Chapter 1: Overview and summary, Nucl. Fusion &amp;#039;&amp;#039;&amp;#039;39&amp;#039;&amp;#039;&amp;#039; (1999) 2137]]&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;[[doi:10.1088/0029-5515/39/12/304|ITER Physics Basis Chapter 4: Power and particle control, Nucl. Fusion &amp;#039;&amp;#039;&amp;#039;39&amp;#039;&amp;#039;&amp;#039; (1999) 2391]]&amp;lt;/ref&amp;gt; higher than this will dilute the fuel too much.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;/div&gt;</summary>
		<author><name>Eldond</name></author>
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