00:02
In this example, we are going to look at forces and electric field of point charges and see how the force on point charges affects their motion.
00:17
So the situation that we have are two equally charged point charges.
00:26
We'll treat them like point charges, and they're tied together with a lightweight string.
00:31
Both of them have a charge of minus 4 nanoculums, which is times 10 to the minus 9 quulums.
00:49
We'll call this one charge 1 and charge 2.
00:54
So they're held together by the string, and what we know is that there's a repulsion that acts equally and oppositely on both of these charges.
01:07
So the force of repulsion is acting on both of those, and that's going to create a tension in the string that's equal and opposite as long as that string is lightweight.
01:27
So each of those charges is going to be held in equilibrium by that interactive tension.
01:36
Okay.
01:38
And what we see from this diagram is the tension has to be equal in magnitude to the cholome force of repulsion between the two charges.
01:50
So that's where our electrostatics equation is going to come into play.
01:55
Kulam's law says that the force between two charges is k times the absolute magnitude of the two charges interacting over their separation squared.
02:13
Here we're given that the separation is 2 centimeters.
02:17
So 0 .02 meters is r d.
02:28
And we can work this out, kulom's law, simply by using the values we have in the electrical constant k in the appropriate units.
02:46
Si is 9 times 10 to the 9th.
02:52
Charges have equal magnitudes 4 times 10 to the minus 9th.
02:58
We'll square that and divide by the distance squared.
03:04
And that will come out to be in newton's.
03:09
Working that out, we see this force is, 3 .6 times 10 to the minus 4th newton's.
03:25
This is also equal to the tension that's pulling back on, equally on both sides of the string.
03:37
And we may want to show the electric field in the vicinity around those two charges.
03:45
Let's go ahead and do that, two negative charges, equal signs, equal magnitudes.
03:53
But basically, the electric field shows the lines of force that a positive charge would experience.
04:02
So let me draw those in blue.
04:07
And what i'm thinking of is the total electric field coming from both of those charges.
04:13
If you're near one of the charges on the side opposite, the other charge, the electric field will simply point straight into each charge.
04:24
Charge representing the attraction of a positive charge.
04:29
You'd have a fairly strong, straight electric field on that side.
04:35
As you get into the middle, though, a positive charge is going to have a hard time figuring out whether it's going to attract to the left charge or the right charge.
04:48
And those electric fields are actually going to partially cancel in that space in between.
04:56
And so you get kind of this saddle.
05:01
A saddle always kind of represents an ambiguity in direction.
05:12
And i really should be showing those electric field lines really spaced out in the area, in between the two charges, representing a weak electric field in that region...