00:01
Alright, hello, in this question we're given this charge setup.
00:02
We have an equilateral triangle, which means that each of these angles is 60 degrees, and they have a side length of 20 centimeters.
00:09
We have three negative charges, and we're interested in the net electric field at this point c, which is halfway between charges 1 and 3.
00:19
So in order to figure out what this is going to be, i'm going to start by drawing the vectors that are each of the electric fields from these.
00:26
So i know that for a negative point charge, i'm going to have an electric field that is pointing towards it radially.
00:33
So for charge 1, which i'll draw here in black, i'm going to have an electric field, sorry, charge 3, not charge 1.
00:40
I'm going to have e3, which is pointing directly towards charge 3.
00:44
For charge 1, i'm going to have the same thing.
00:47
I'm going to have e1 is pointing directly towards it.
00:49
And then e2, this blue one, is going to be pointing directly towards that, and that's going to be e2.
00:56
Now if i want to just find the magnitude, i can set my axes to be whatever i want.
01:02
And so i'm going to make a very clever choice of axes here.
01:04
I'm going to say that that is the positive x direction, and then that is the positive y direction.
01:09
And because i know these are at right angles to one another, this is just going to make my life a lot easier, since i'm only asked for the magnitude.
01:17
So i know that my electric field in the x direction is going to be, well, i have e3 pointing in the positive direction, and i have e1 pointing in the negative direction, so that's going to be a negative.
01:29
What is the electric field generated by a point charge? well, it's going to be k times that point charge.
01:36
So for charge 3, it's going to be kq3 over the distance it is away squared.
01:41
So in this case, it's a distance a over 2 away, and that's going to be squared.
01:47
And then for e1, i have k times q1 over a over 2 squared as well.
01:53
Note here, i've accounted for the fact that these are negative charges already by just having the direction of my electric fields point towards those point charges.
02:04
So when i plug in q1 and q3, i don't need to plug in the sine.
02:11
I can go ahead and reduce this down, factor out some like terms, and i'll get q3 minus q1.
02:16
So that's going to be e in the x direction...