How Do Electric Fields Differ Between Plasma and Vacuum Sheaths?

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Homework Help Overview

The discussion revolves around the differences in electric fields between plasma and vacuum sheaths, focusing on the dielectric function of plasma and the implications of applying a voltage across it. Participants are tasked with deriving expressions for the electric fields in both regions under specific assumptions.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Some participants question the initial understanding of the electric field as stated in the problem. Others suggest deriving constants related to the electric fields in terms of voltage and the dielectric function. There are mentions of starting with the Laplace equation and considering the geometry of the setup.

Discussion Status

Participants are actively exploring the relationships between the electric fields in the plasma and sheath, as well as how these relate to the applied voltage. There is a recognition of the need for further specifications regarding the geometries involved, indicating a productive direction in the discussion.

Contextual Notes

Assumptions include the absence of free charge and the validity of the electrostatic approximation due to a small plasma frequency. The geometry involves two electrodes with one grounded and the other at a specified voltage, separated by a distance that includes the plasma and sheath sizes.

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 ?
 
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touqra said:
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 ?

I would say that your task is to find the constants E_s and E_p in terms of V and \epsilon(\omega)

I'd say start with the Laplace equation - but unless you have some futher specification of the geometries involved like a sketch og something, that might prove tricky
 
Troels said:
I would say that your task is to find the constants E_s and E_p in terms of V and \epsilon(\omega)

I'd say start with the Laplace equation - but unless you have some futher specification of the geometries involved like a sketch og something, that might prove tricky

It's two plate of electrodes, one grounded, another at voltage V, separated by a distance
H + 2h, where h is the size of the sheath at each end of the electrode and H the size of plasma.
 
You have two different types of dielectric, one is vacuum, the other given by the plasma equation... Given the obvious direction of the electric field, what is the relationship between Es & Ep?

Now what is the relationship between the fields and the potential?
Solve to get the absolute fields.
 

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