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http://www.mysolutions.tecnico.ulisboa.pt//mysolutions/wiki/api.php?action=feedcontributions&feedformat=atom&user=Ist181114 My Solutions - Contribuições do utilizador [pt] 2025-08-14T05:00:17Z Contribuições do utilizador MediaWiki 1.35.2
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http://www.mysolutions.tecnico.ulisboa.pt//wiki/index.php?title=Debye_shield_/spherical_conductor&diff=3784 Debye shield /spherical conductor 2018-01-20T00:05:54Z <p>Ist181114: </p> <hr /> <div>&lt;div class=&quot;toccolours mw-collapsible mw-collapsed&quot; style=&quot;width:420px&quot;&gt;<br /> &#039;&#039;&#039;Metadata&#039;&#039;&#039;<br /> &lt;div class=&quot;mw-collapsible-content&quot;&gt;<br /> *CONTEXTO : Segundo ciclo universitário<br /> *AREA: Física<br /> *DISCIPLINA: Física e Tecnologia dos Plasmas<br /> *ANO: 4<br /> *LINGUA: en<br /> *AUTOR: Vasco Guerra<br /> *MATERIA PRINCIPAL: Debye shielding and fundamental efects<br /> *DESCRICAO: Debye shield /spherical conductor<br /> *DIFICULDADE: *<br /> *TEMPO MEDIO DE RESOLUCAO: 300 [s]<br /> *TEMPO MAXIMO DE RESOLUCAO: 600 [s]<br /> *PALAVRAS CHAVE: <br /> &lt;/div&gt;<br /> &lt;/div&gt;<br /> (F. F. Chen \(\sim\) 1.10) A spherical conductor of radius \(R\) is immersed in a plasma and charged to a potential \(\phi_0\).<br /> The electrons remain Maxwellian and move to form a Debye shield, but the ions are stationary during the time frame<br /> of the experiment. Assuming \(e\phi_0\ll k T_e\):<br /> <br /> (a) derive an expression for the potential as a function of \(r\);<br /> <br /> (b) calculate the charge in the sphere;<br /> <br /> (c) calculate the sphere capacity for \(R=10\) cm, \(T_e=1\) keV and \(n_0=10^{14}\) and \(10^6\) cm\(^{-3}\), and show that for <br /> high electron densities the plasma behaves as a dielectric.</div> Ist181114 http://www.mysolutions.tecnico.ulisboa.pt//wiki/index.php?title=Debye_shield_/spherical_conductor&diff=3782 Debye shield /spherical conductor 2018-01-20T00:05:37Z <p>Ist181114: </p> <hr /> <div>&lt;div class=&quot;toccolours mw-collapsible mw-collapsed&quot; style=&quot;width:420px&quot;&gt;<br /> &#039;&#039;&#039;Metadata&#039;&#039;&#039;<br /> &lt;div class=&quot;mw-collapsible-content&quot;&gt;<br /> *CONTEXTO : Segundo ciclo universitário<br /> *AREA: Física<br /> *DISCIPLINA: Física e Tecnologia dos Plasmas<br /> *ANO: 4<br /> *LINGUA: en<br /> *AUTOR: Vasco Guerra<br /> *MATERIA PRINCIPAL: Debye shielding and fundamental efects<br /> *DESCRICAO: Debye shield /spherical conductor<br /> *DIFICULDADE: *<br /> *TEMPO MEDIO DE RESOLUCAO: 300 [s]<br /> *TEMPO MAXIMO DE RESOLUCAO: 600 [s]<br /> *PALAVRAS CHAVE: <br /> &lt;/div&gt;<br /> &lt;/div&gt;<br /> (F. F. Chen \(\sim\) 1.10) A spherical conductor of radius $R$ is immersed in a plasma and charged to a potential \(\phi_0\).<br /> The electrons remain Maxwellian and move to form a Debye shield, but the ions are stationary during the time frame<br /> of the experiment. Assuming \(e\phi_0\ll k T_e\):<br /> <br /> (a) derive an expression for the potential as a function of \(r\);<br /> <br /> (b) calculate the charge in the sphere;<br /> <br /> (c) calculate the sphere capacity for \(R=10\) cm, \(T_e=1\) keV and \(n_0=10^{14}\) and \(10^6\) cm\(^{-3}\), and show that for <br /> high electron densities the plasma behaves as a dielectric.</div> Ist181114

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