Capacitor and Dielectric story

A parallel plate capacitor with plate area A A and separation d d ( d < < l d<<l lateral dimensions ) ) is filled with a dielectric of dielectric constant k = e α x k=e^{\alpha x} where α \alpha is a constant ( α > 0 ) (\alpha>0) and plate is at x = 0 x=0 . The capacitor is charged to a potential V V .
Calculate the capacitance ( C ) (C)
Answer comes in the form of C = ϵ 0 A β α γ δ e α d C=\frac{\epsilon_{0}A^{\beta}\alpha}{\gamma- \delta e^{-\alpha d}}
Type your answer as β + γ + δ = ? \beta+\gamma+\delta=? Bonus
1) Sketch C C vs d d
2) Obtain the charge on the plates.
3) Obtain the electric field E ( x ) \vec{E}(x)

Details and Assumptions
1) Don't forget to solve bonus problem.
2) Remember the 1 s t 1^{st} point of Details and Assumptions .

The problem is not original.


The answer is 3.

This section requires Javascript.
You are seeing this because something didn't load right. We suggest you, (a) try refreshing the page, (b) enabling javascript if it is disabled on your browser and, finally, (c) loading the non-javascript version of this page . We're sorry about the hassle.

2 solutions

E ( x ) = d V d x = Q ϵ 0 ϵ A = Q ϵ 0 A e α x E(x)=-\dfrac{dV}{dx}=\dfrac{Q}{\epsilon_0\epsilon A}=\dfrac{Q}{\epsilon_0 A}e^{-αx}\implies

V = Q ϵ 0 α A 0 d e α x d x = V=\dfrac{Q}{\epsilon_0 αA}\displaystyle \int_0^d e^{-αx}dx=

Q ϵ 0 α A ( 1 e α d ) \dfrac{Q}{\epsilon_0 αA}(1-e^{-αd})\implies

Q = ϵ 0 α A 1 e α d × V Q=\dfrac{\epsilon_0 αA}{1-e^{-αd}}\times V\implies

C = Q V = ϵ 0 α A 1 e α d C=\dfrac{Q}{V}=\dfrac{\epsilon_0 αA}{1-e^{-αd}} .

So β = 1 , γ = 1 , δ = 1 β=1,\gamma=1,\delta=1 , and β + γ + δ = 3 β+\gamma+\delta=\boxed 3 .

Sahil P.
May 13, 2020

Capacitors in series add like resistors in parallel, so C = ϵ 0 A 0 d d x e α x C=\frac{\epsilon_{0}A}{\int_{0}^{d} \frac{dx}{e^{\alpha x}}} . This yields the desired answer.

0 pending reports

×

Problem Loading...

Note Loading...

Set Loading...