00:01
Okay, we're given an electric field that looks like this.
00:05
And the first thing i'm going to do is i'm going to use the formulas for some and difference in a cosine to write them out like this.
00:16
When i do that, the sign -sign terms cancel out.
00:22
And these two are the same, so i get twice that.
00:27
It makes life a little easier.
00:29
Then i use my faraday law and ampure law to find out that my by looks like this.
00:38
And my other two components of b, bx and bz, are both zero.
00:48
Then i want to find the components of the pointing vector, which is e cross b over mu not.
00:58
Right away, i can figure out that sx and sy are both zero, because the only components, i only have an x component of e and a c, a y component of b.
01:17
So the only surviving component of the pointing vector is ex, b over a mu not.
01:26
I plug my numbers in...