00:03
Okay, so in this problem, we have an experimental setup here.
00:07
It has a resistor connected to some bars with a metal bar freely moved to complete the circuit.
00:13
It's a 6 centimeters long.
00:16
And it's moving on a speed v equals 20 centimeters per second.
00:22
Here's a resistant r, where r is 0 .8 oms.
00:28
The mass of our rod is 0 .2 kilograms.
00:33
And we put this whole thing in a magnetic field that is into the page of the strength.
00:42
We don't know.
00:45
Okay.
00:47
So they give us this chart here, this table of a's and v's.
00:55
So for a's we have 6 .2, 4 .9, 4 .3, 3 .1, and 2 .10, 12, 14, 6 .2, 4 .3, 3 .1, and 2 .10, 12, 14.
01:12
Okay, so it wants us to plot these.
01:15
So let's draw up a plot here and we want to plot as a versus v.
01:20
So a versus v.
01:22
I'm going to make mine pretty big u .s.
01:26
Here.
01:29
Do these by fives and these by twos.
01:37
So now let's find our first one.
01:39
Our first one is at 8.
01:42
8 and 2 .5.
01:46
10 and 3 .1.
01:49
12 and 3 .7, 14 and 4 .3, 16 and 4 .9, and 20 and 6 .2.
02:06
So we look like we have a pretty linear relationship here.
02:10
So for part a, we want to plot it, and then we want to find what the average slope is here.
02:20
So the average slope we can do as the total rise overrun.
02:25
And this is given as 3 .7, that's the max a minus the min a over 12, which is the max v minus the min v.
02:35
And we see that this is 0 .308.
02:39
So that's our slope, which means we have a relationship that looks like, a equals 0 .308 times v.
02:48
This kind of looks like it with some possible y intercept, but this is a slope relationship, which is what we're really care about.
02:57
So now for part b we want to see if we can figure out what b is because that's what we want to know.
03:06
So we got to figure out a relationship between a and v that involves b.
03:12
Okay.
03:13
So to start this, we know the emotional emf is given as bvl.
03:18
And that means the current induced with that motional emf is vbl over r.
03:26
And we also know that the force from that kind of is given as i, l, b.
03:34
So if we put all this together, we see this becomes v, b squared, l squared over r.
03:42
And that is our force...