Diferenças entre edições de "Debye shield /spherical conductor"
		
		
		
		
		
		Saltar para a navegação
		Saltar para a pesquisa
		
				
		
		
	
| Linha 9: | Linha 9: | ||
*AUTOR: Vasco Guerra  | *AUTOR: Vasco Guerra  | ||
*MATERIA PRINCIPAL: Debye shielding and fundamental efects  | *MATERIA PRINCIPAL: Debye shielding and fundamental efects  | ||
| − | *DESCRICAO:   | + | *DESCRICAO: Debye shield /spherical conductor  | 
*DIFICULDADE: *  | *DIFICULDADE: *  | ||
*TEMPO MEDIO DE RESOLUCAO: 300 [s]  | *TEMPO MEDIO DE RESOLUCAO: 300 [s]  | ||
*TEMPO MAXIMO DE RESOLUCAO: 600 [s]  | *TEMPO MAXIMO DE RESOLUCAO: 600 [s]  | ||
| − | *PALAVRAS CHAVE:   | + | *PALAVRAS CHAVE:    | 
</div>  | </div>  | ||
</div>  | </div>  | ||
| Linha 19: | Linha 19: | ||
The electrons remain Maxwellian and move to form a Debye shield, but the ions are stationary during the time frame  | The electrons remain Maxwellian and move to form a Debye shield, but the ions are stationary during the time frame  | ||
of the experiment. Assuming \(e\phi_0\ll k T_e\):  | of the experiment. Assuming \(e\phi_0\ll k T_e\):  | ||
| + | |||
| + | |||
| + | (a)derive an expression for the potential as a function of \(r$;  | ||
| + | |||
| + | (b) calculate the charge in the sphere;  | ||
| + | |||
| + | (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   | ||
| + | high electron densities the plasma behaves as a dielectric.  | ||
Revisão das 19h44min 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: Debye shield /spherical conductor
 - DIFICULDADE: *
 - TEMPO MEDIO DE RESOLUCAO: 300 [s]
 - TEMPO MAXIMO DE RESOLUCAO: 600 [s]
 - PALAVRAS CHAVE:
 
(F. F. Chen \(\sim\) 1.10) A spherical conductor of radius $R$ is immersed in a plasma and charged to a potential \(\phi_0\). The electrons remain Maxwellian and move to form a Debye shield, but the ions are stationary during the time frame of the experiment. Assuming \(e\phi_0\ll k T_e\):
(a)derive an expression for the potential as a function of \(r$;
(b) calculate the charge in the sphere;
(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 high electron densities the plasma behaves as a dielectric.