00:01
In part a, we're given a vector field f and the curve c, and we're asked the stasis theorem to evaluate the line integral over c of f.
00:13
F is the vector field x squared y i plus one third x -g to j plus x y k, and c is the curved intersection of the hyperbolic paraboloid z equals y squared minus x squared and the cylinder x squared plus y squared equals y squared equals one oriented counterclockwise as viewed from above.
00:44
So we have first of all that s is the part of the surface, which is our hyperbolic paraboloid, c equals y squared minus x squared, that lies above the unit disk, which we'll call d.
01:15
Now the curl of the vector field f that we're given this is x i minus y j plus x squared minus x squared k which reduces to x i minus y j and using previous equation function g of x and y so our surface is a function of y and x so our surface is a function of y and x and x and and we'll take function p to be the first component of the curl of f, which is x, q will be the second component of the curl of f, which is negative y, and r will be 0, the third component.
02:56
Therefore, we have that the line integral over c of f, dystokesis theorem is equal to the surface integral over s of the curl of f, and because of surface is a function of x and y, this is the double integral over the domain of integration d, sorry unit disk, of the opposite of p, so negative x times the partial derivative of g with respect to x, which is negative 2x, minus q, which is negative y, times the partial derivative of g with respect to x, which is negative 2x, minus q, which is negative y, times the partial derivative of g with respect to y, which is 2y, plus r, which is 0, da.
04:03
And simplifying, this is 2 times the double integral over d of x squared plus y squared, da.
04:19
And converting to polar coordinates, this is two times the integral from 0 to pi, integral from 0 to 1, the radius of the disk of r squared, times r is r cubed, d r d theta.
04:42
And taking antiderivatives, you get 2 times 2 pi times 1 fourth, and this simplifies to pi.
05:05
Then in part b, we're asked to graph first the hyperbolic paraboloid and the cylinder, so that we can see the curve c and the surface s using part a.
05:15
To do this, i'm going to use desmosis parametric surface graph...