00:01
So if we were to draw the trajectory of the electron, it's going to go through a half circle.
00:08
And so the velocity is always tangent to the curve.
00:15
And perpendicular to the velocity is always the magnetic force.
00:21
Here it would be going down.
00:26
And the velocity would be going straight to the right.
00:30
So here, the magnetic field must be directed into the page.
00:36
So we can label this.
00:42
So again, the magnetic field is always into the page.
00:45
And we know that the force is equaling mass times acceleration.
00:50
And the only force here would be the magnetic force.
00:55
And in this case, the acceleration is centripetal.
00:58
So we can say that the magnetic force equals the mass times the centripetal acceleration.
01:04
Or we can say that the absolute value of the charge times the velocity times the magnitude of the magnetic field times sine of phi is going to be equal to mv squared divided by r now here we know that phi is 90 degrees so this term is going to be equal to one it can be eliminated and we know that the magnitude of the magnetic field is going to be equal to the mass times the velocity divided by the absolute value of of the charge times the radius.
01:36
So at this point for part a, when we're trying to find b, we can simply say that this is going to be equal to 9 .11 times 10 to the negative 31st kilogram, and then the velocity of the electron is 1 .41 times 10 to the 6 meters per second.
01:56
And this will be divided by the charge of an electron, 1 .6 times 10 to the negative 19.
02:05
Kulams and then times the radius of 0 .05 meters.
02:15
And we find that the magnitude of the magnetic field is equaling 1 .61 times 10 to the negative 4th tesla's.
02:23
So this will be your answer for part a.
02:29
So that'll be your answer for a day.
02:31
And then for part b, they're asking us for a time...