00:01
We have a two charge sheet.
00:03
Let's call this a and this is this contains a charge density of sigma, sigma one, which is negative.
00:19
And plate b or sheet b has got a charge density sigma 2 that has got a positive charge.
00:34
The electric fields then we can write on the left of a will be e1 in this direction and e2 will be in this direction where e1 here between these two plates will be in this direction because of the negative a plate or a sheet and e2 between these plates will be in this direction where this is e1 then on the right of sheet b, electric field, e1 will be in this direction, and e2 will be in this direction.
01:23
We know the field of infinite charge sheet is given by a sigma divided by 2 epsilon.
01:30
Then for part a, so for part a, at a point p.
01:40
So the point p is here.
01:43
Point p at point p the electric field will be e1 plus e2 this is a sigma 1 magnitude plus sigma 2 magnitude divided by 2 epsilon we just added up the fields for two infinite sheets and the total electric field at point p we got is the sum of e1 and e2 because they are in same direction...