00:01
In this problem, we're asked to consider a circular loop of wire moving in the xy plane with constant velocity in the negative x direction, and it enters a uniform magnetic field which covers the region in which x is less than zero.
00:17
The surface normal vector of the loop points in the direction of the magnetic field.
00:24
Knowing this, which statement is correct.
00:28
Statement a says, induced potential difference.
00:33
In the loop is at a maximum as the edge of the loop just enters the region with magnetic field.
01:31
Okay.
01:36
Okay.
01:36
So we're going to be observing the conductive loop moving in the x, y plane, as shown in the figure below.
01:45
So let me do a little thinking here.
01:49
I'm going to go get a black, and i'm going to have my y direction.
02:02
Here i've got a circular loop.
02:04
Here's my x direction.
02:08
And i've got all of these charges.
02:11
I'm not going to draw all my charges in.
02:15
And we've got this.
02:17
Okay, the magnetic field lines are represented.
02:25
These are magnetic fields lines.
02:41
And they're directed from the drawing towards us, and they're parallel to the normal vector of the loop of the wire.
02:49
And we're determining which position of the loop of the wire, of the loop of wire relative to the region of uniform magnetic field is a potential difference induced in the maximum loop.
03:05
The loop is divided into four quarters since we need to determine under which overlap.
03:13
Okay.
03:14
So let me draw my four quarters better.
03:26
Okay.
03:29
So we'll look at faraday's law of induction and in its qualitative form states that the potential difference.
03:57
I'm going to abbreviate a little bit.
03:58
This is a long one.
03:59
It's induced in a loop when the number of magnetic fields, field lines passing through the loop changes with time.
04:52
So we're going to count the field lines passing through the loop when the loop just enters the region of the magnetic field.
05:06
Okay...