Two identical, parallel, thin metal plates are connected to the terminals of a DC power supply.
a) It can be shown that the electric field produced by a large, thin, metal plate with uniform surface charge density σ, at relatively small distances from the plate, can be expressed as , where is the surface normal unit vector. Derive an expression for the electric field between the plates mentioned above in terms of their charge density σ if the distance d between the plates is much smaller than their dimensions; b) Using integration, derive an expression for the potential difference between
\[E=\frac{ \sigma }{ 2\epsilon _{0} }\eta \]
... can be expressed as (above formula), where n ....
Don't know physics. Sorry.
@UnkleRhaukus
what does eta represent here?
something like the dielectric constant of the material between the plates or something else?
im not sure what eta '\(\eta\) ' means here
uniform surface charge density σ n is the surface normal unit vector
\[\hat{\mathbf n}\]
yes, i couldn't find it
ah ok, so you have to show \[\large\vec E=\frac{ \sigma }{ 2\epsilon _{0} }\hat{\mathbf n}\] ``` \[\large\vec E=\frac{ \sigma }{ 2\epsilon _{0} }\hat{\mathbf n}\] ``
yes, thx
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