Checkered Capacitor

A parallel plate capacitor, with plates A \textbf{A} and B \textbf{B} of equal dimensions t × L t \times L at a distance of L L , is filled with square tiles of dielectric to make a chess-board-like capacitor, as shown in the picture above.

Dielectric constant of the dark tile is σ 1 , \sigma_1, that of the light tile is σ 2 , \sigma_2, and ϵ 0 \epsilon_0 is the permittivity of free space. All the dielectric tiles are square cuboids of thickness t t .

Find the capacitance of this capacitor.


Details and Assumptions:

  • Assume that the electric field varies between the plates like an ideal parallel plate capacitor.
2 ϵ 0 σ 1 L 2 ( σ 1 + σ 2 ) t \dfrac{2\epsilon_0 \sigma_1 L^2}{(\sigma_1+\sigma_2)t} 2 ϵ 0 σ 1 L 2 σ 2 t \dfrac{2\epsilon_0 \sigma_1 L^2}{\sigma_2 t} ϵ 0 σ 1 σ 2 t σ 1 + σ 2 \dfrac{\epsilon_0 \sigma_1\sigma_2 t}{\sigma_1+\sigma_2} 2 ϵ 0 σ 1 σ 2 t σ 1 + σ 2 \dfrac{2\epsilon_0 \sigma_1\sigma_2 t}{\sigma_1+\sigma_2}

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.

1 solution

Steven Chase
Mar 9, 2017

In general, the formula for capacitance is (where A A is the cross-sectional area, ϵ \epsilon is the permittivity, and d d is the plate spacing):

C = ϵ A d \large{C = \frac{\epsilon A}{d}}

The individual squares have dimension L 8 \large{\frac{L}{8}} . Treat each individual square as a capacitor. The cross-sectional area is thus A = L t 8 \large{A = \frac{Lt}{8}} . The distance associated with each capacitor is d = L 8 \large{d = \frac{L}{8}} . Thus the capacitance of each square is (when the relative permittivity σ \sigma is accounted for):

C = σ ϵ L t 8 L 8 = σ ϵ t \large{C = \frac{\sigma \epsilon \frac{Lt}{8}}{\frac{L}{8}} =\sigma \epsilon t}

Keep in mind that there are two different values of σ \sigma . Divide the overall checkerboard into 8 columns, each with 8 squares. Each column is equivalent to (4 series σ 1 \sigma_1 capacitors) in series with (4 series σ 2 \sigma_2 capacitors). 4 identical capacitors in series have a capacitance one quarter that of each individual unit. Then the σ 1 \sigma_1 and σ 2 \sigma_2 units in series can be calculated using the general product-over-sum formula for series capacitors. The overall capacitance of a column is given below.

C c o l u m n = σ 1 ϵ t 4 σ 2 ϵ t 4 σ 1 ϵ t 4 + σ 2 ϵ t 4 = σ 1 σ 2 ϵ 2 t 2 4 ϵ t ( σ 1 + σ 2 ) = σ 1 σ 2 ϵ t 4 ( σ 1 + σ 2 ) \large{C_{column} = \frac{\frac{\sigma_1 \epsilon t}{4} \frac{\sigma_2 \epsilon t}{4}}{\frac{\sigma_1 \epsilon t}{4} + \frac{\sigma_2 \epsilon t}{4}} = \frac{\sigma_1 \sigma_2 \epsilon^2 t^2}{4 \epsilon t (\sigma_1 + \sigma_2)} = \frac{\sigma_1 \sigma_2 \epsilon t}{4 (\sigma_1 + \sigma_2)}}

Capacitors in parallel add. Therefore, the 8 columns in parallel yield a total capacitance equal to 8 times the above value.

C t o t a l = 8 C c o l u m n = 8 σ 1 σ 2 ϵ t 4 ( σ 1 + σ 2 ) = 2 σ 1 σ 2 ϵ t σ 1 + σ 2 \large{C_{total} = 8 C_{column} = \frac{8 \sigma_1 \sigma_2 \epsilon t}{4 (\sigma_1 + \sigma_2)} = \frac{2 \sigma_1 \sigma_2 \epsilon t}{\sigma_1 + \sigma_2}}

nice solution !

Sabhrant Sachan - 4 years, 2 months ago

Follow up question: Do all the dark tiles have equal electric field? If yes, what is it? Given that the potential drop across the capacitor is V V .

Rohit Gupta - 4 years, 2 months ago

Log in to reply

Sounds like a good one. Are you going to post it?

Steven Chase - 4 years, 2 months ago

Log in to reply

Are you asking if I am going to post it as a question or am I going to post its solution/answer?

For the solution/answer, I am thinking to wait and let others solve it as well. If no one gives a solution or an answer to this, I'll post one.

Rohit Gupta - 4 years, 2 months ago

Log in to reply

@Rohit Gupta I meant to ask if you would make it into its own problem.

Steven Chase - 4 years, 2 months ago

Interesting. If we had taken 8 rows first, each row would have capacitance C r o w = 4 ( σ 1 + σ 2 ) ϵ L 8 t L 8 C_{row} = \dfrac{4(\sigma_1 + \sigma_2) \epsilon \frac{L}{8} t}{\frac{L}{8}} , and since they are all in series, the total capacitance would be one eighth of this value

C t o t a l = ( σ 1 + σ 2 ) ϵ t 2 C_{total} = \frac{(\sigma_1 + \sigma_2)\epsilon t}{2}

Why is this not correct?

Pranshu Gaba - 4 years, 2 months ago

Log in to reply

Here's my equivalent circuit. What is yours?

Steven Chase - 4 years, 2 months ago

Log in to reply

My equivalent circuit was this:

First parallel, then series.

Edit: I understand now that since σ 1 σ 2 \sigma_1 \neq \sigma_2 , the electric field across each capacitors in a row won't be equal, so they aren't really in parallel.

Pranshu Gaba - 4 years, 2 months ago

This is a good point you brought up. All the dielectrics in the first row beside the plate B B are not in parallel. For the parallel combination, the potential drop across them must be equal. Now, if you consider a dark and a light dielectric, the electric field inside them will be different and hence the potential difference. Therefore, they cannot be considered in parallel.

Rohit Gupta - 4 years, 2 months ago

Awesome problem and solution!:)

Dan Ley - 4 years, 2 months ago

0 pending reports

×

Problem Loading...

Note Loading...

Set Loading...