00:01
As an example of working with coolum's law, electric force and electric field, we'll take a look at two charges that are sitting in space next to each other.
00:12
One is positive and the other is negative.
00:16
And let's just give those some values, a minus 12 nanoculums on the right and a positive three anaculums on the left, separated by 36.
00:30
Centimeters.
00:39
So kulam's law gives us two formulas for both the force of attraction between two charges, and that should be written with an absolute value around those two charges.
00:55
Why? because this equation gives you the magnitude of the interaction.
01:03
The direction comes from basically, knowing what signs of charges there are and whether situated in space.
01:13
So the force always acts on a line joining the bear, and it will act one way if they are attracting each other.
01:24
It will act opposite that on both charges if they repel.
01:29
And the electric field has a similar type of relationship.
01:34
Again, there's a k and the absolute magnitude of a over by, divided by the distance squared.
01:44
But notice that the electric field assumes just one charge sitting there in space, creating a field, whereas the force measures in interaction.
01:55
So let's take a look at this example.
01:58
The two charges will obviously feel an attraction, and that will be a newton's third law pair.
02:07
So those are equal and opposite each other.
02:10
And hence, you don't want to be putting signs on your kulom's law calculation.
02:18
But anyway, we can calculate the magnitude of that interactive force.
02:23
The electrical constant is 9 times 10 to the 9th in si units.
02:30
And remember, we want the absolute magnitudes of those charges.
02:36
So we're going to put them in both with positive signs.
02:43
And really, it makes no sense to have a negative magnitude.
02:51
Only astronomers make that happen.
02:58
But a vector magnitude is not a negative number.
03:05
So let's see what we get in terms of newton's.
03:08
We've used everything in si units.
03:10
So this is 3 .6 times 10 to the minus 6 newtons.
03:22
The next situation we're going to think about is the electric field at a point right in between those two charges.
03:31
So we have our negative and positive charges.
03:36
And we are going to look at a point, we'll call that point p, 15 centimeters from both.
03:48
Centimeters and 15 centimeters...