00:01
As an example of potential and potential energy for point charges, we are going to figure out the work it will take to drop a positive charge at point p, which is the top vertex in an equilateral triangle.
00:19
And along the bottom are two charges at the vertices.
00:24
There's a positive one micro, which is 10 to the minus 6, coulums, on the left and a negative 2 microculems on the right.
00:37
So the first goal is to find the potential at point p using the potential formula for point charges.
00:47
It's the electrical constant k times charge q over the distance from that charge.
00:55
So we can find the potential at point p due to the positive one microculum.
01:04
K is just 9 times 10 to the 9th in si units.
01:12
And we have one microculum.
01:17
And our separation is given to us as 0 .5 meters.
01:26
So not surprisingly, that's a positive potential.
01:33
And we can do the same for the negative charge.
01:50
And so that's a fairly straightforward.
01:52
It's not surprisingly a negative potential.
02:01
What we know about electric potential is that it just adds.
02:07
So we can find the total potential at point p by just simply adding those two together.
02:18
And if there were many other different charges, we could add them in as well.
02:23
But we get minus 1 .8 times 10 to the 4 volts.
02:32
Now for the work.
02:34
The work done by an external agent, not the field, but an external agent, is going to be positive change in potential energy, which is q times delta v.
02:51
The reminder that what a delta is is a final minus initial...