How Do Electric Fields Differ Between Plasma and Vacuum Sheaths?

touqra
Messages
284
Reaction score
0
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 ?
 
Last edited:
Physics news on Phys.org
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.
 
##|\Psi|^2=\frac{1}{\sqrt{\pi b^2}}\exp(\frac{-(x-x_0)^2}{b^2}).## ##\braket{x}=\frac{1}{\sqrt{\pi b^2}}\int_{-\infty}^{\infty}dx\,x\exp(-\frac{(x-x_0)^2}{b^2}).## ##y=x-x_0 \quad x=y+x_0 \quad dy=dx.## The boundaries remain infinite, I believe. ##\frac{1}{\sqrt{\pi b^2}}\int_{-\infty}^{\infty}dy(y+x_0)\exp(\frac{-y^2}{b^2}).## ##\frac{2}{\sqrt{\pi b^2}}\int_0^{\infty}dy\,y\exp(\frac{-y^2}{b^2})+\frac{2x_0}{\sqrt{\pi b^2}}\int_0^{\infty}dy\,\exp(-\frac{y^2}{b^2}).## I then resolved the two...
Hello everyone, I’m considering a point charge q that oscillates harmonically about the origin along the z-axis, e.g. $$z_{q}(t)= A\sin(wt)$$ In a strongly simplified / quasi-instantaneous approximation I ignore retardation and take the electric field at the position ##r=(x,y,z)## simply to be the “Coulomb field at the charge’s instantaneous position”: $$E(r,t)=\frac{q}{4\pi\varepsilon_{0}}\frac{r-r_{q}(t)}{||r-r_{q}(t)||^{3}}$$ with $$r_{q}(t)=(0,0,z_{q}(t))$$ (I’m aware this isn’t...
Hi, I had an exam and I completely messed up a problem. Especially one part which was necessary for the rest of the problem. Basically, I have a wormhole metric: $$(ds)^2 = -(dt)^2 + (dr)^2 + (r^2 + b^2)( (d\theta)^2 + sin^2 \theta (d\phi)^2 )$$ Where ##b=1## with an orbit only in the equatorial plane. We also know from the question that the orbit must satisfy this relationship: $$\varepsilon = \frac{1}{2} (\frac{dr}{d\tau})^2 + V_{eff}(r)$$ Ultimately, I was tasked to find the initial...
Back
Top