Find a vector field F whose curl is G and use Stokes’ theorem

Colt87

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Find a vector field F whose curl is G and use Stokes’ theorem

Consider the vector fieldG(x, y, z) = xi −y/ 2j + ( 2xy −z/ 2 ) k,and a wire frame described byC = { (x, y, z)|x2 + y2 = 2 and z = 1}

I found the parameters
r(s,t) = (Sqrt 2 cos(s), Sqrt 2 sin(s), t)

from 0<=s<=2pi and

0<=t<=1 (not sure about this bound)

I started with the curl = del X F

but how do i find F(xyz) to get (del X F = G) from that?
 
Frankly I don't know what you mean by "a wire frame described by C = {(x,y,z)x2+y2=2andz=1}\displaystyle \{ (x, y, z)|x^2 + y^2 = 2 and z = 1\}. That is a circle, in the z= 1 plane, with center at (0, 0, 1) and radius 2\displaystyle \sqrt{2}. And, that does not seem to have anything to do with your question. You are given the vector field G=xi+y2k+(2xyz2)k\displaystyle G= x\vec{i}+ \frac{y}{2}\vec{k}+ \left(2xy- \frac{z}{2}\right)\vec{k}. You want to find F such that ×F=G\displaystyle \nabla\times F= G.

Okay, Let F=f(x,y,z)i+g(x,y,z)j+h(x,y,z)k\displaystyle F= f(x,y,z)\vec{i}+ g(x,y,z)\vec{j}+ h(x,y,z)\vec{k}. Then ×F\displaystyle \nabla\times F is
ijkxyzfgh=(hygz)i+(fzhx)j+(gxfy)k\displaystyle \left|\begin{array}{ccc} \vec{i} & \vec{j} & \vec{k} \\ \frac{\partial}{\partial x} & \frac{\partial}{\partial y} & \frac{\partial}{\partial z} \\ f & g & h \end{array}\right|= \left(\frac{\partial h}{\partial y}- \frac{\partial g}{\partial z}\right)\vec{i}+ \left(\frac{\partial f}{\partial z}- \frac{\partial h}{\partial x}\right)\vec{j}+ \left(\frac{\partial g}{\partial x}- \frac{\partial f}{\partial y}\right)\vec{k}.

So we must have hygz=x\displaystyle \frac{\partial h}{\partial y}- \frac{\partial g}{\partial z}= x, fzhx=yx\displaystyle \frac{\partial f}{\partial z}- \frac{\partial h}{\partial x}= \frac{y}{x}, and gxfy=2xyz2\displaystyle \frac{\partial g}{\partial x}- \frac{\partial f}{\partial y}= 2xy- \frac{z}{2}.

Now, what do you want to do with this? You say "use Stokes' theorem". Use Stokes' theorem to do what?
 
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Frankly I don't know what you mean by "a wire frame described by C = {(x,y,z)x2+y2=2andz=1}\displaystyle \{ (x, y, z)|x^2 + y^2 = 2 and z = 1\}. That is a circle, in the z= 1 plane, with center at (0, 0, 1) and radius 2\displaystyle \sqrt{2}. And, that does not seem to have anything to do with your question. You are given the vector field G=xi+y2k+(2xyz2)k\displaystyle G= x\vec{i}+ \frac{y}{2}\vec{k}+ \left(2xy- \frac{z}{2}\right)\vec{k}. You want to find F such that ×F=G\displaystyle \nabla\times F= G.

Okay, Let F=f(x,y,z)i+g(x,y,z)j+h(x,y,z)k\displaystyle F= f(x,y,z)\vec{i}+ g(x,y,z)\vec{j}+ h(x,y,z)\vec{k}. Then ×F\displaystyle \nabla\times F is
ijkxyzfgh=(hygz)i+(fzhx)j+(gxfy)k\displaystyle \left|\begin{array}{ccc} \vec{i} & \vec{j} & \vec{k} \\ \frac{\partial}{\partial x} & \frac{\partial}{\partial y} & \frac{\partial}{\partial z} \\ f & g & h \end{array}\right|= \left(\frac{\partial h}{\partial y}- \frac{\partial g}{\partial z}\right)\vec{i}+ \left(\frac{\partial f}{\partial z}- \frac{\partial h}{\partial x}\right)\vec{j}+ \left(\frac{\partial g}{\partial x}- \frac{\partial f}{\partial y}\right)\vec{k}.

So we must have hygz=x\displaystyle \frac{\partial h}{\partial y}- \frac{\partial g}{\partial z}= x, fzhx=yx\displaystyle \frac{\partial f}{\partial z}- \frac{\partial h}{\partial x}= \frac{y}{x}, and gxfy=2xyz2\displaystyle \frac{\partial g}{\partial x}- \frac{\partial f}{\partial y}= 2xy- \frac{z}{2}.

Now, what do you want to do with this? You say "use Stokes' theorem". Use Stokes' theorem to do what?







Right sorry so i'm pretty sure it's a cylinder. I found F(xyz) = 1/2zyi + x2yj +xyk which G is it's curl.

This is the full question:

Consider the vector field:

G(x, y, z) = xi −y/2j + (2xy −z/2)k,

and a wire frame described by

C = {(x, y, z)|x2 + y2 = sqrt2 and z = 1,

with counter clock wise orientation when viewed from above. Suppose thatS is any smooth surface with boundary C. Compute the flux of G throughS. (Hint: find a vector field F whose curl is G and use Stokes’ theorem.You will need to figure out a parameterization of C to do the resulting lineintegral).
 
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