Diferenças entre edições de "Plasma frequency"

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(D. R. Nicholson ~ 1.3) In the deduction of the electron plasma frequency, suppose the ions are not infinitely massive, but have a mass \(m_i\) and can moce.
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(D. R. Nicholson ~ 1.3) In the deduction of the electron plasma frequency, suppose the ions are not infinitely massive, but have a mass \(m_i\) and can move. Modify the discussion to show that the coupled oscillation of the electron and ion " slabs " is made with the total plasma frequency  
Modify the discussion to show that the coupled oscillation of the electron and ion ``slabs'' is made with the total plasma frequency  
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\((\omega_p^2 = \omega_{pe}^2 + \omega_{pi}^2)\).
\((\omega_p^2 = \omega_{pe}^2 + \omega_{pi}^2)\).
 

Edição atual desde as 21h02min de 2 de março de 2017

Metadata

  • CONTEXTO : Segundo ciclo universitário
  • AREA: Física
  • DISCIPLINA: Física e Tecnologia dos Plasmas
  • ANO: 4
  • LINGUA: en
  • AUTOR: Vasco Guerra
  • MATERIA PRINCIPAL: Debye shielding and fundamental efects
  • DESCRICAO: Plasma frequency
  • DIFICULDADE: *
  • TEMPO MEDIO DE RESOLUCAO: 300 [s]
  • TEMPO MAXIMO DE RESOLUCAO: 600 [s]
  • PALAVRAS CHAVE:

(D. R. Nicholson ~ 1.3) In the deduction of the electron plasma frequency, suppose the ions are not infinitely massive, but have a mass \(m_i\) and can move. Modify the discussion to show that the coupled oscillation of the electron and ion " slabs " is made with the total plasma frequency \((\omega_p^2 = \omega_{pe}^2 + \omega_{pi}^2)\).