00:06
In this case what is happening is i have two parallel rods.
00:12
They are connected by a resistor, by a resistor r.
00:20
The distance between the rods are l and a metal cart moves in this direction with a speed of v.
00:43
So we have to figure out what the area is over here and other than that, there's a magnetic field.
00:54
The magnetic field, this is the top view of the of my setup.
01:02
Now if i look at the side view of the setup then you will realize that if this is the horizontal, magnetic field is 68 degree below horizontal.
01:19
So this is the magnetic field and the vertical component of the magnetic field will be given by.
01:25
B sine 68 degree using the value of b to be 5 times 10 to the minus 5 tesla multiplied by sine 68 is 0 .93 and that comes out to be 4 .64 4 .6 4 times 10 to the minus 5 tesla.
02:57
So let us call this b perpendicular.
03:05
Now in this particular case what's happening is b perpendicular b perpendicular goes into the plane just because the area through which the magnetic field passes is reducing, the flux is changing and there will be an emf induced in the system let us tell let us first find the emf induced emf equals we don't care about the direction at this point negative d fee dt be perpendicular dot area or multiplied by area now let us assume that the rod moves to the right by an amount of x which makes the whole area to be oh by the way we can call this to be l prime the horizontal distance to be l prime so the area becomes the vertical l and the horizontal l prime l l now if you look at the system carefully you should be able to understand that the perpendicular value of magnetic field is constant, l stays constant, and dl prime, d t is l prime is on the time -dependent term, and the rate of change of l -prime is simply given by v.
05:27
So, p perpendicular, l -v.
05:33
Let us just put the numbers in now...