00:02
Before we started the computation, first we set up some notation.
00:09
So we let this point to be a, let this point to be b, let this point to be c, this point to be d.
00:25
Then we look at the electric field at p, contributed from a, b, c, d separately.
00:35
So if we look at the contribution from b and b.
00:39
And d we know that the contribution from b is this direction, y direction.
00:51
Contribution from d is again only in the y direction or the j direction.
01:12
So now we write down contribution from b and d.
01:24
They are in a wide direction.
01:28
Now we look at contribution from a and c which is less trivial.
01:39
So the contribution from a, it is pointing to a because it is negative charge.
01:46
So we draw this line, ap and the cp.
02:01
Then this is the contribution of electric field from a.
02:07
And the contribution from c is pointing away from c.
02:16
We know that pa and pc are the same distance.
02:22
So, and the charge at a and c are opposite, but the same magnitude.
02:31
So the electric field are the same magnitude.
02:38
So from the symmetry, we know that that ea plus e, c are in x direction.
02:52
So now we know that in x direction, we only need to compute the contribution from a and the contribution from c.
03:08
So the contribution from a in the x direction, it is k -q over r squared, so k and the q, q is negative q, r square.
03:26
So we look at this triangle, the right triangle.
03:34
R is the hypotenuse, so it is r2 is a squared plus a over 2 square...