00:01
Hello, in the question we have given that two cross -sections of a long parallel wires are arranged on the corner of square.
00:08
So, this is the configuration given in the question and the currents, the currents are given i1 and i2 which is 2f and 4g.
00:16
So, now this b1 and b2 i have represented by using the right -hand thumb rule.
00:21
So, if we use the right -hand thumb rule for current i1, so i1 is coming out of the page.
00:27
So, if we place the fingers pointing towards us and call the finger, so we will find that this b1 is pointing in this direction.
00:36
So, b1 is the magnetic field due to this current i1.
00:39
Now, this b2, b2 now this i2, same we will do for i2, i2 is coming out of the page.
00:46
So, we will place the finger in the direction towards us, pointing towards us and we will call the fingers.
00:52
We will find that the magnetic field is along this direction, the tangential one.
00:57
So, now having done this, so we know that for the infinitely long current carrying wire, the magnetic field is given by mu naught i divided by 2 pi r.
01:10
So, b1 will be equal to mu naught i divided by 2 pi r.
01:14
So, current is i1 and b2 will be equal to mu naught i2 divided by 2 pi r.
01:20
R is the distance, that is the edge length of the square.
01:25
So, let us compute b1.
01:27
So, b1 will be equal to mu naught is 4 pi into 10 raised to minus 7 into i1 is 2f divided by 2 pi into r.
01:41
R is how much? 20 centimeters, so which is 0 .2 meters.
01:46
So, if we calculate, so this 2, 2 goes away, this pi goes away, this 2, so this becomes 10.
01:51
So, it gives us b1 as 20f into 10 raised to minus 7 tesla.
01:59
So, similarly, we can find out b2.
02:01
So, b2, what it will be? mu naught 4 pi into 10 raised to minus 7 into b2 is 4g divided by 2 pi r is 0 .2.
02:18
So, if this pi goes away, 2 ones are 2, 2 twos are 4, then this becomes 10.
02:23
So, this becomes 40 into 10 raised to minus 7 and g, g will be there over here multiplied with 40...