00:01
Let's say we have a red conducting sphere as you can see in the diagram there in the middle as a radius of a.
00:08
In a charge of plus q.
00:11
And that red conducting sphere is surrounded by empty space, but it's also inside of a larger green conducting sphere.
00:19
Right? and this fear is hollow.
00:22
So it has an inner radius of b.
00:24
And an outer radius of c.
00:27
Um and this outer sphere, like the green one, there has no charge on it, no net charge.
00:33
So let's find the electric field at a few different points.
00:36
And and to do this, we're gonna be using what's called god's law, right? and god's law for electric fields basically says that the integral of the electric field in terms of the area d.
00:53
A.
00:54
Is equal to the charge enclosed.
00:57
So q.
00:58
E.
00:58
N.
00:59
C.
01:01
I'm trouble getting to see there right over the constant e.
01:05
Not right.
01:07
Which is the primitive itty of free space.
01:09
So the first thing to know is that the electric field inside of any conductor is always zero.
01:19
So that means we don't even need god's law for inside the red conductor.
01:24
This is just going to be zero.
01:26
And also inside the green conductor.
01:28
So between the radi i.
01:30
B and c, those are also going to be zero.
01:32
We don't even need god's law for for those because anytime you have any conductor, the electric field inside of is zero.
01:41
Now between the conductors, this is where we do have to use galaxies long for galaxies law.
01:49
We need a calcium surface.
01:52
So if we're using between the conductors, let's say we have our read conductor here and we have our inner radius here.
02:00
So this will be radius b.
02:04
Right? and then of course we have radius a.
02:06
Inside.
02:08
So actually we're going to choose a galaxy in surface in between those.
02:12
It's just gonna be a circle here and that's going to have a radius r.
02:17
Right? so what that radius are? we know that.
02:21
Um because we're dealing with spheres, we we we like know that that d...