00:01
We want to find the area of the region that lies inside the cardioid r is equal to 1 plus cosine theta and outside the circle r is equal to 1.
00:10
So i'm going to head and graph to both of those.
00:12
So outside of the circle and inside our cardioid would actually be this region right here that i'm going to shade in red.
00:25
So within this region, we just have to figure out how our radius varies as well as theta.
00:32
Radius will we start from the origin and we go until we intersect our region.
00:36
So the lower bound is going to be one.
00:39
And then we keep on going until we pass through the region, which is going to be our cardioid.
00:46
So r is going to vary 1 up until 1 plus cosine of theta.
00:55
Now the next thing we need to do is figure out how theta varies.
00:59
Well, notice that in this region we would go from here, rotate all the way around, and then exit through here.
01:07
So at least looking at this, it's pretty easy to see that this is going to be negative pi -half to pi -half for our rotation, since it's just the axes.
01:19
But if we weren't given that, what we could do is set these two equations equal to each other and then solve.
01:24
So the algebraic way to do this would just be to let 1 equal to 1 plus cosine theta.
01:31
That gives us 0 is equal to cosine theta.
01:33
And well, we know that would be negative pi half and pi half, or at least for two of the solutions.
01:39
So we have those.
01:42
Now we can go ahead and plug everything into the equation that they give us.
01:48
And that's going to be, so we want to put theta last, since our radius is going to depend on it.
01:56
So it's going to go from negative pi half to pi half.
01:59
And then our radius goes from one to one plus cosine of theta.
02:04
R, dr, d, theta.
02:06
So we can go ahead and integrate this.
02:09
And that's going to give 1 .5r squared.
02:12
So i'm just going to factor that 1 half all the way out.
02:14
So it would be 1 .5 negative pi half to pi half of r squared evaluated from 1 plus cosine theta, or 1 to 1 plus cosine theta.
02:29
Then we have d theta on the outside...