Let S be the portion of the paraboloid z = 4 -x^2 -y^2 that lies above z= 0. Let F be the vector field F = (z-y)i + (x+z)j - (e^xyz(cosy))k. Using Stoke's Theorem, find the surface integral.
So the hope is that \(\nabla \times \mathbf F\) is a very simple function, if we're using Stokes.
Agreed
Can you calculate it?
Yes. Let me re-calculate to make sure my answer isn't fudged.
\[(xze ^{xyz}cosy -e^{xyz}siny - 1)i -(e^{xyz}cosy - 1)j + 2k\]
What a mess.
Yes
okay, do you know how to parametrize the parabaloid then?
Maybe...
subtract z in the equation, and take the gradient of the expression.
-2x-2y, or -2x-2y-1? I dont quite understand what you meant by subtract z or why it's done that way.
the gradient is a vector
When you have a level set \[ g(x,y,z) = C \]Then the gradient will give you the normal vector to that level set.
So you're saying that \[g(x,y,z) = C = 4 - x^2 -y^2 - z\] \[gradient = (-2x)i - (2y)j - 1k \] ? Sorry, this is again unfamiliar to me.
yes
Ok
you could have even said \[ g(x,y,z)=-4 = -x^2-y^2-z \]It doesn't matter since \(C\) goes away when differentiated.
Excellent
Seems like a tough integral...
Would you use \[\int\limits_{}^{}\int\limits_{S}^{} (curlF) ndS = \int\limits_{C}^{} Fdr \]
Where \[Fdr = (z-y)dx + (x+z)dy + (e^{xyz}cosy)dz\]
In doing so, you are no longer using stokes.
Gotcha
\[dS = \sqrt(4x^2 + 4y^2 +1) ??\]
No, okay, so basically \(\mathbf n\) is the unit normal vector, and \(dS\) is the magnitude of the the normal vector \(d\mathbf S\), which you just calculated.
Well actually, I'm being a bit sloppy here.
Anyway \(d\mathbf S = \langle -2x,-2y,-1\rangle dxdy\)
And \[ \mathbf n~ dS = d\mathbf S \]
Ok
So do we leave the z's as constants the whole time? or set all z's to 0?
Okay, so basically, the \(z\) gets replaced with \(z(x,y)\) when we do this sort of parametrization.
Since \(z=f(x,y)\).
So, for every z, we replace with 4 -x^2 - y^2 ?
yes
Are you sure you wrote the problem down correctly?
Very sure.
Our only hope is that cylindrical coords make things easier.
\[(x(4-x^2-y^2)e^{((4-y^2-x^2)xy)}cosy- e^{(4-x^2-y^2)yx}siny -1 )i -(y(4-x^2-y^2)e^{(4-x^2-y^2)yx}cosy-1)j +2k\]
Doesnt even fit. -_-
How should I go about using cyl coords for this? The only I've been to taught to use this is to convert it to a line integral since Stokes' Theorem allows for you to choose whichever is more convenient, which seems like the line integral would be for this particular instance
I should have said polar coords. \[ r^2 = x^2+y^2\\ \theta = \tan\frac yx\\ x = r\cos\theta\\ y = r\sin\theta \\ dx~dy = r~dr~d\theta \]
Bleh. Either conversion is just... tedious. But given that....\[(\cos(\theta)(4r-r^3) e^{(4r^2-r^4)\cos(\theta)\sin(\theta)}\cos(rsin(\theta)) - e^{(4r^2-r^4)\cos(\theta)\sin(\theta)}\sin(rsin(\theta) - 1)i -(\sin(\theta)(4r-r^3)e^{(4r^2-r^4)\cos(\theta)\sin(\theta)}-1)j +2k\]
There is something wrong with this problem.
lol
I swear that F(x,y,z) = (z-y)i +(x+z)j - (e^xyz (cosy))k. S is the portion of the paraboloid z = 4 - x^2 - y^2 that lies above z=0.
Given Stokes' Theorem, why can't you use a line integral? Stokes' Theorem just equates them. Using it either way is using the theorem. Yes?
http://www.math.ucsd.edu/programs/undergraduate/math_20E_exam/Practice_Test.pdf would be the link to the question also. It's the 3rd question.
|dw:1404104335257:dw|
Join our real-time social learning platform and learn together with your friends!