00:01
So in this question, we're going to be using gauss's law, and we're told that we have a cylinder of radius a.
00:08
So i'm drawing this in cross section.
00:12
So that's an a.
00:13
And then outside that, and this is carrying a charge plus q.
00:18
And then outside that, we have a cylinder, a concentric cylinder of radius b.
00:23
So it's meant to be a circle.
00:25
And it's carrying a total charge minus 2q.
00:29
And we're told that these cylinders are conducting.
00:31
And what that means is that the charge is going to be, uh, homogeneously distributed.
00:38
So let's remember that gauss's law is that the integral of e over a surface, so the integral of the flux of the e field through a surface, is equal to the charge enclosed by that surface divided by epsilon.
00:59
So let's think first of a gaussian surface with r less than a.
01:04
This surface contains no charge, and that means that the...
01:09
Well, first of all, let's think, because we have a symmetric situation, this integral, because e is going to be the same at all points of a given radius, because we have circular symmetry, this is going to come down to 2 pi r times the modulus of the e field, equals q enclosed over epsilon naught.
01:38
So here, inside the first cylinder, so for r less than a, q enclosed is zero.
01:48
So we have that e is equal to zero.
01:51
Now let's think about a radius between a and b...