00:01
Our magnetic field region is sketched in this figure.
00:06
Firstly, let's apply ampere's law.
00:10
So this says that the closed loop integral, the magnetic field b .d .l, the enclosed path, must be equal to zero in this case, since there are no currents in the region.
00:25
So using the figure, let's let our magnetic field b equal to b0 in the i direction, when y is less than 0 and equal to 0 for y greater than 0.
00:52
So the integral as written by amper's law is actually the integral across the closed path from a to b to c to d and back to a again, as you can see in our region, of b dot d equals to 0 and this integral is the magnetic field b across ab times l minus the magnetic field b across cd, margified by l, and that's also equal to 0.
01:37
But we know from the diagram that the magnetic field across c and d is 0.
01:47
So b, c, d is equal to 0...