00:01
Here we're going to find the electric field at a point, a distance, certain distance 2d, away from a conducting plane, and there is a charge plus q sitting on top of that conducting plane.
00:19
And the method we're going to use is a nice little trick called the method of images.
00:25
What that method relies on is that you're putting.
00:30
Potential in a region is unique as long as you have the potential specified on a boundary.
00:39
So i'm going to go ahead and pretend that we know that conductor plane is grounded so that we have a very unique potential sitting there.
00:50
And the idea is that as long as you do something to recreate the potential on the boundary, you're good to go.
01:00
So the idea is why where the image comes in is you can imagine an image charge.
01:11
It's not really there, but you can imagine it there of negative q.
01:17
And then everywhere along that conductor is equidistant from both charges, as long as you put that imaginary charge one distance away.
01:28
But the conductor everywhere along it is equidistant from those two -point charges, and so the potentials add up to zero everywhere along there.
01:47
And so you've kind of matched the uniqueness of that boundary.
01:53
But once you put that image charge there, then it is a simple matter to figure out the electric field at any point.
02:02
You so choose as long as it's in the region of the real charge off limits...