Capacitor with two dielectrics inserted diagonally

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The discussion focuses on calculating the capacitance of a capacitor with square plates and two dielectrics inserted diagonally. Participants emphasize the need for integration to find the capacitance based on varying proportions of the dielectric materials. A method is proposed to form elemental columns of equal dielectric distribution for easier integration. The final capacitance expression is derived, incorporating the dielectric constants and correcting notation for clarity. The conversation concludes with a suggestion to explore the case when both dielectric constants are equal.
carlyn medona

Homework Statement


A capacitor has square plates of length a separated at a distance d. Dielectrics are inserted as shown in the figure. Find the capacitance

Homework Equations

The Attempt at a Solution

[/B]
I know that I have to integrate, but can't get an expression
 

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What would be the capacitance with 100% of material 1? With 50% of material 1 (and 100% of material 2)? With a fraction x of material 1?

What would be the capacitance if half of the length had x% of material 1 and the other half had y%?

These steps should help to find the right expression.
 
carlyn medona said:

Homework Statement


A capacitor has square plates of length a separated at a distance d. Dielectrics are inserted as shown in the figure. Find the capacitance

Homework Equations

The Attempt at a Solution

[/B]
I know that I have to integrate, but can't get an expression
Take an element dx at a distance x from any end for this caculate dc
 
You can form an elemental area dx dy on the bottom plate, extend the area along the z axis
as a column to the top plate, compute the capacitance of this column as the series connection of two capacitors, then add (integrate) the parallel columns to find the total capacitance.

Actually, it is easier to form dx columns of equal dielectric distribution, then there is only one integral to evaluate.

PS thanks @cnh1995 for the vote!
 
Last edited:
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rude man said:
Actually, it is easier to form dx columns of equal dielectric distribution, then there is only one integral to evaluate.
Yes, that is how I solved it.
 
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Okay I got

dc = εa^2k1k2dx ÷(d (xk1 -xk2+k2a) and after integration c
C = εa^2k1k2ln(k1÷k2)÷(d(k1-k2)
 
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You're a bit sloppy with your parentheses, but the result looks good if you make those corrections, replace your ε with ε0 and wind up with C = {ε0κ1κ2a2/D(κ12)} ln(κ1/κ2).
Note that I changed distance from d to D to avoid confusion with the calculus.
It's obvious you went the right way, good going.
 
carlyn medona said:
Okay I got

dc = εa^2k1k2dx ÷(d (xk1 -xk2+k2a) and after integration c
C = εa^2k1k2ln(k1÷k2)÷(d(k1-k2)
As rude man said, replace ε with ε0.

Just for fun, see what happens when you put k1=k2 in that equation.
 
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cnh1995 said:
Just for fun, see what happens when you put k1=k2 in that equation.
Good one, cnh! I wondered about that myself, thought at first I had made an error, finally determined the limit existed and agreed with the degenerate case k1=k2=k.
 
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