Line Integral - Stokes theorem

AwesomeTrains
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Homework Statement


Hello
I was given the vector field: \vec A (\vec r) =(−y(x^2+y^2),x(x^2+y^2),xyz) and had to calculate the line integral \oint \vec A \cdot d \vec r over a circle centered at the origin in the xy-plane, with radius R, by using the theorem of Stokes.

Another thing, when calculating ∇× \vec A I used Cartesian coordinates but when doing the integration I changed to polar coordinates, is that okay? Or do I have to do it all in Cartesian coordinates, because I did curl in Cartesian coordinates?

Homework Equations


Stokes equation:
5f65e93751487f9350c194aa5f2bb8de.png


The Attempt at a Solution


My result is: 2R^4π Is that correct ? I evaluated both sides and got the same.

Kind regards Alex
 
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AwesomeTrains said:
Another thing, when calculating ∇× \vec A I used Cartesian coordinates but when doing the integration I changed to polar coordinates, is that okay? Or do I have to do it all in Cartesian coordinates, because I did curl in Cartesian coordinates?
It's fine to change coordinates to make evaluating the integral easier whenever you want.

My result is: 2R^4π Is that correct ? I evaluated both sides and got the same.
I didn't actually do the integral on paper so I might have missed something, but the answer looks right to me.
 
Okay, thanks for the reply :)
 
I got 4πR4.

del x A = 4R2 k
dA = R2/2 k
∫2R2R2dθ from 0 to 2π = 4πR4.
 
Last edited:
Thanks for doing the calculation but why is dA=\frac{R^2}{2} d \theta. My curl vector is the same.
I was using dxdy=rdrd \theta
 
AwesomeTrains said:
Thanks for doing the calculation but why is dA=\frac{R^2}{2} d \theta. My curl vector is the same.
I was using dxdy=rdrd \theta

I took the differential area as that of a triangle of area 1/2 bh = 1/2 R Rrdθ = 1/2 R2
b = base
h = height
Proof: A = ∫dA = 1/2 R2∫dθ from 0 to 2π = πR2. :smile:

You can do it your way too! Just requires integrating twice instead of once:
dA = r dr dθ
A = ∫∫r dr dθ= R2/2 (2θ) = πR2.
So how about showing how you got 2πR4? One of us must have stumbled a bit in the dA department.
 
rude man said:
I got 4πR4.

del x A = 4R2 k
dA = R2/2 k
∫2R2R2dθ from 0 to 2π = 4πR4.
The curl is ##\nabla\times\vec{A} = 4r^2 \hat{k}##. It depends on variable ##r##, not constant ##R##, so you can't use that area element.
 
Thanks for the replies guys. I'll write out my calculation then you can see where the mistake lies.
\nabla \times \vec A = (xz - 0)i + (0 - yz)j + (3x^2+y^2 - (-x^2 - 3y^2))k
Chose a vektor normal to the circle:
d \vec f = 0i+0j+k
The dot product is then:
\nabla x \vec A \cdot d \vec f = 4x^2+4y^2 = 4r^2
Then I integrated over the circle, and changed to spherical coordinates where I used the area element: dA =rdrd \phi:
\int_{0}^{2\pi} \int_{0}^R 4r^2rdrd \phi = \int_{0}^{2Pi} \int_{0}^R 4r^3drd \phi = 2R^4\pi
 
Last edited:
I agree, I should not have made r constant in the curl expression.
 
  • #10
Is 2R^4\pi then the correct result?
 
  • #11
Yes.
 
  • #12
AwesomeTrains said:
Is 2R^4\pi then the correct result?
Yes, I say it is, and you were right to use r dr dθ as the elemental area.
 
  • #13
Okay, thanks for the help, will be back with some more problems :)
 
  • #14
AwesomeTrains said:
Okay, thanks for the help, will be back with some more problems :)
Please do! I'll try not to mess up next time ... o:)
 
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