00:01
Hi, in this question we are given with a magnetic field in terms of the equation.
00:06
Now we have to convert this magnetic field into spherical coordinates.
00:12
So spherical coordinates.
00:24
So this is given by so in terms of spherical coordinates b is written as r theta comma phi which is given in terms of matrix written as so this is in terms of spherical coordinates where magnetic field is written in terms of r theta and phi.
00:40
Now we have b is given by so b is equal to this sin theta cos phi plus sin theta sin phi into b naught into r cap.
00:58
So a r cap plus cos theta cos phi plus so this is one term cos theta sin phi into b naught a phi.
01:13
So this is the phi component.
01:14
Then we have plus sin phi into so sin phi plus cos phi into a theta.
01:22
So these are the theta components.
01:24
These are the phi components and these are the r components.
01:27
Now we have the surface element ds is equal to it is r square sin theta d phi d theta into a r cap.
01:38
Then we have the flux.
01:40
So magnetic flux phi is given by it is surface integration of so surface aerial integration of the magnetic field.
01:50
So we have phi is equal to double integration of b naught into so this is the amplitude of the magnetic wave.
01:57
It is sin theta into cos phi plus sin phi into sin theta multiplied by r square.
02:07
So d square ds is so taking only components of r.
02:11
So we have r square in terms of ds we have r square sin theta d phi d theta.
02:21
So we have the theta it ranges from 0 to pi by 2 and phi it ranges from 0 to pi by 2.
02:33
So the integration becomes so the integration will be phi is equal to 0 to pi by 2 0 to pi by 2.
02:42
So this is a double integration.
02:43
So b naught into r square is common.
02:46
It is taken outside...