00:01
For this problem, we are told to let f of xy be the piecewise defined function, xy minus 1 divided by x squared plus y squared minus 2, if x squared plus y squared does not equal to, and 1 over 2 if x squared plus y squared equals 2.
00:16
We are then asked to show that the partial derivatives, with respect to x and y, at the point 1 -1, each exist, but that f is not differentiable at the point 1 -1.
00:28
So to begin with finding those partial derivatives, we know that by definition, fx of 1 -1, should be equal to the limit as delta -x approaches 0 of f of 1 plus delta -x, 1 minus f -of -1 -1 -1, all divided by delta -x.
00:54
We know that f -1 -1 equals 1 over 2.
00:57
So we can write this then as the limit, as delta x approaches zero, of, now f of 1 plus delta x, 1 would be, let's see here.
01:09
I'll write it down as 1 plus delta x times 1 minus 1, divided by 1 plus delta x all squared, plus 1 squared, so plus 1, minus 2.
01:25
So we can just write that as minus 1.
01:29
And we have minus 1 over 2, and we divide everything through by delta x.
01:35
So this will then be equal to the limit as delta x approaches 0 of, one moment here.
01:45
So simplifying the numerator, we can write that down as negative delta x over 4 plus 2 delta x, and then we're still dividing by delta x or multiplying by one over delta x.
01:59
So we can see that the delta x is divided out.
02:01
We're left with negative 1 over 4 plus 2 delta x, or the limit of that, as delta x approaches 0.
02:13
So we clearly get a result of negative 1 over 4 as the partial derivative.
02:17
Then taking the partial derivative with respect to y, we'll get that this will be the limit as delta y approaches 0.
02:25
Of f of, or it would be f of 1, then 1 plus delta y, minus f of 1 1, which we already know, that's 1 half, all divided by delta y.
02:43
Now, substituting in 1 plus delta y in place of y, we'd get 1 plus delta y minus 1 divided by 1 plus delta y, all squared, plus 1 minus 2, so minus 1, minus 1 over 2, all over delta y.
03:03
And i'll note we're still taking a limit as delta y approaches 0 here.
03:09
Oops, let me fix that line that showed up there.
03:15
Now we can see that the overall form of what we are looking at here is identical to what we saw for delta, or for the partial derivative with respect to x.
03:27
So we can conclude that we'll arrive at the same point, particularly being that partial derivative equals negative 1 over 4...