00:02
Hi, so we are given a problem of parallel platy capacitor.
00:06
So we have an air capacitor which is made by two metal plates, each having area a and are separated by distance t.
00:15
So let me draw the metal plates here.
00:19
So we have two parallel metal plates, each having area of air and these two pender plates are separated by distance t.
00:33
Now it's given that in between the two metal plates, a metal slab of thickness a which is less than d is inserted so we have a metal slab of thickness a this thickness is less than the separation d and it is inserted in between the two plates and in the first part of the problem we need to find the net capacitance of this arrangement now note that in between the two parallel plates so in between these two plates we have a metal slab insert it so this is a metal slab and not a dialectic slab that is why this arrangement is like an arrangement of two capacitors connected in series so we have a capacitor consisting of the upper so let me write it like this so we have a capacitor consisting of the upper plate and the metal slab so let's call this capacitor 7 and then we have another capacitor consisting of the middle metal slab and the lower plate so this is capacitors c2 which is filled with so this two capacitors are filled with eo and the distance as you can see between the upper plate and the metaslav and the metaslav and the lower plate let's see this let's call this distance bt prime and for both the capacitors the distance is same and if you will see the distance d prime is going to be equal to total distance which is d minus the distance where we have the metal slab.
02:33
So the thickness of the metal slab which is a divided by 2.
02:38
So this is the thickness or the distance between the two capacitors, t prime.
02:46
Now having found that, so in the first part of the problem, we need to find the equivalent capacitance of this arrangement of the capacitors which is in which in series so the equivalent capacitance can be written as one over c because since it's like a series combination so 1 over c c equals 1 over c1 plus 1 over c2 now note that c1 and c2 they are they are separated by the same distance so and they have the same area so c1 is indeed equals to c2 which is equal to x0 a divided by the distance which we have already calculated here d prime which is d minus a or divided by or divided by 2 so that's c1 and c2 now since c1 is equal to c2 which is going to imply the capacitance c is nothing but it's going to be equal to half times c1.
04:10
So the equivalent capacitance is half of c1 and we have already calculated c1 which is equal to c2.
04:18
So from this, we find that the equivalent capacitance for this combination is going to be epsilon not a divided by d minus a...