touqra
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A plasma is described by the dielectric function
\epsilon (\omega) = \epsilon_0 (1-\frac{\omega_p^2}{\omega^2})
where \omega_p is a constant. Any attempt to establish a voltage
V(t) = V cos \omega t across the plasma generates a region of vacuum called the "sheath" on either side of the plasma volume.
Derive expressions for the uniform electric field E_p (t) = E_p cos \omega t in the plasma and for E_s (t) = E_s cos \omega t in the sheath. Assume that there is no free charge anywhere. Assume that \omega_p is small enough that an electrostatic approximation is always valid.
I don't really understand. Isn't the electric field is stated in the question already ?
\epsilon (\omega) = \epsilon_0 (1-\frac{\omega_p^2}{\omega^2})
where \omega_p is a constant. Any attempt to establish a voltage
V(t) = V cos \omega t across the plasma generates a region of vacuum called the "sheath" on either side of the plasma volume.
Derive expressions for the uniform electric field E_p (t) = E_p cos \omega t in the plasma and for E_s (t) = E_s cos \omega t in the sheath. Assume that there is no free charge anywhere. Assume that \omega_p is small enough that an electrostatic approximation is always valid.
I don't really understand. Isn't the electric field is stated in the question already ?
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