00:01
We have two light sources six meters apart.
00:03
So let's say this is our light source one.
00:08
And let's say it has an intensity of l1.
00:11
The other light source is here.
00:15
We'll call that l2.
00:17
And we're told that this second light has an intensity that's eight times that of the other.
00:23
Okay, so we're going to say that this one is equal to 8l1.
00:28
And we know that the distance in between is six meters.
00:34
So the question is, where in between these two light sources will the total illumination be the least? okay, so let's say this point here.
00:44
So we'll call this the distance between this blue point to l1, x, which means the other one must be 6 minus x.
00:53
And we're told that the intensity at a point, it varies inversely, as the square of the distance between the point and the light source.
01:03
So that means, so let's call the intensity at this point i.
01:10
Well, the total intensity there is going to be the intensity from light source one, which we will call i1, plus the intensity from the second light, which we will call i2.
01:24
So inversely proportional just means that this is equal to the illumination from light one, so that's l1 over the square of the distance and the distance between l1 and our point is x right so this would be x squared and then we multiply by some constant k so this is i1 and we do the same thing for i2 so now this is going to be the intensity from the second light which is l2 over the square of the distance which is six minus x squared and then we multiply by the same constant okay so now we know what l is in terms of l1.
02:15
So let's substitute that in.
02:16
So we get this as equal to.
02:18
And then we can pull the k to the front.
02:21
So that's k times l1 over x squared plus 8l1 over 6 minus x squared.
02:33
Okay.
02:34
And that is equal to the total intensity.
02:37
And this is now only in terms of x.
02:42
Okay.
02:43
And remember that l1 is just a constant.
02:44
Okay...