00:01
All right, so here we have a charge particle in red with a velocity.
00:07
And we're going to look at what happens to that charge particle and only a magnetic field, only an electric field, or both electric and magnetic field.
00:17
Because our goal would be that that velocity remains constant for our charge and basically to see if it's possible on each of these fields.
00:27
Okay, so let's take a look at only magnetic field.
00:30
So what happens with a velocity or a charge particle moving with a velocity in a magnetic field, it only feels a force if it has a component perpendicular.
00:47
So if i were to take a magnetic field that is absolutely parallel to the charged particle, then that's the only way that it will not produce.
01:02
A force.
01:03
So if i go ahead and shoot that particle exactly parallel or anti -parallel to the magnetic field, then i can have v be constant.
01:14
So yes, i can do it in a magnetic field, but i have to be parallel, exactly parallel.
01:22
The minute we have any component that's perpendicular, it starts to turn the charge.
01:27
Once you turn the charge, you change a direction and the v is not constant.
01:31
The speed might be constant, but not the v.
01:35
So you have to be exactly parallel to have that unaffected charge.
01:41
Okay, electric field, however, you're always accelerated in the direction of the electric field.
01:52
So let's say i have an electric field this way.
01:54
This before was b.
01:56
Now we've got e.
01:57
Maybe i'll change a color.
01:58
Let's change a color real quick so we can differentiate.
02:01
The two.
02:02
So let's make b field or electric field green.
02:08
Okay, so the blue was for the b field and the green then will be for the electric field.
02:15
Okay, so what happens with the electric field is no matter what, if i have a charged particle in electric field, doesn't matter if it's parallel or perpendicular.
02:26
You will always get a force on that charge in the direction of the electric field...