00:10
In this particular case, you have some time -dependent magnetic field, and you have a coil over here.
00:29
You have connected to an ammeter, and this has got some resistance, r.
00:38
The number of tons in the coil is known, and the area of the coil is known.
00:50
The ammeter was found to register a current of i.
00:59
So in this particular circuit, electric field in the circuit is given by i times r, the resistance of the coil, current times the resistance of the coil.
01:22
And from the loop law, electric field is given by negative change in flux over change in time, which is negative td t of number of tons in the coil, magnetic field, and area.
01:59
In this case, we are assuming that the coil is head on to the magnetic field.
02:06
Checking the constant terms out we have n a and negative d b d t equals i r so from here the only unknown is this so we can figure that out d b d t with a with a negative sign is given by i r over n .a.
03:01
Current is 180 mhz, resistance 25 om, number of tons, 25, and 3 .14 radius square.
03:29
Radius is 0 .3 meter meter square...