I Stokes' theorem and surface integrals

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The discussion focuses on computing the integral of the curl of a vector field over a 2-dimensional surface using Stokes' theorem. The antisymmetric tensor, defined as the difference of partial derivatives, is introduced to facilitate this computation. The user expresses confusion about an extra factor of 2 in their final equation, which is clarified by another participant who points out that the integral is symmetric in its indices, leading to double counting. The conversation also touches on the concept of differential forms and the proper definition for surface elements to avoid this issue. The resolution emphasizes the importance of correctly accounting for the symmetry in the indices when setting up the integral.
dRic2
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Compute the integral of the "curl" of the vector field ##A_i(x_i)## over a 2-dimensional surface.
Hi,

So my goal is to compute the integral of the "curl" of the vector field ##A_i(x_i)## over a 2-dimensional surface. Following a physics book that I am reading, I introduce the antisymmetric 2-nd rank tensor ##\Omega_{ij}##, defined as:
$$\Omega_{ij} = \frac {\partial A_i}{\partial x_j} - \frac {\partial A_j}{\partial x_i}$$
then, from what I gather reading the Wikipedia page (https://en.wikipedia.org/wiki/Surface_integral), if the surface can be parametrized by a set of 2 variables ##u## and ##v## I should be able to write the surface element as ##dudv## times the determinant of the jacobian:
$$ \frac {\partial x_i}{\partial u} \frac {\partial x_j}{\partial v} - \frac {\partial x_j}{\partial u} \frac {\partial x_i}{\partial v}$$
Putting all together I get:
$$\int_S \left( \frac {\partial A_i}{\partial x_j} - \frac {\partial A_j}{\partial x_i} \right) \left( \frac {\partial x_i}{\partial u} \frac {\partial x_j}{\partial v} - \frac {\partial x_j}{\partial u} \frac {\partial x_i}{\partial v} \right) dudv$$
Using the chain rule, I can simplfy the expression to yield:
$$ \int_S \left( \frac {\partial A_i}{\partial v} \frac {\partial x_i}{\partial u} - \frac {\partial x_i}{\partial v} \frac {\partial A_i}{\partial u} - \frac {\partial A_j}{\partial u} \frac {\partial x_j}{\partial v} + \frac {\partial x_j}{\partial u} \frac {\partial A_j}{\partial v} \right) dudv = 2 \int_S \left( \frac {\partial A_i}{\partial v} \frac {\partial x_i}{\partial u} - \frac {\partial x_i}{\partial v} \frac {\partial A_i}{\partial u} \right) dudv
$$
But I am pretty sure there should not be a 2 in the last equation. Is my reasoning wrong?

Thanks
Ric
 
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I think you should check your distributions from the second-to-last line. From what I got, the terms on the last line should all be distinct.

This is assuming that your reasoning is correct, though. Algebraically, your final answer does not look right.
 
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In the last line ##u## and ##v## were swapped. I corrected the OP for clarity.
 
dRic2 said:
Summary:: Compute the integral of the "curl" of the vector field ##A_i(x_i)## over a 2-dimensional surface.

Hi,

So my goal is to compute the integral of the "curl" of the vector field ##A_i(x_i)## over a 2-dimensional surface. Following a physics book that I am reading, I introduce the antisymmetric 2-nd rank tensor ##\Omega_{ij}##, defined as:
$$\Omega_{ij} = \frac {\partial A_i}{\partial x_j} - \frac {\partial A_j}{\partial x_i}$$
then, from what I gather reading the Wikipedia page (https://en.wikipedia.org/wiki/Surface_integral), if the surface can be parametrized by a set of 2 variables ##u## and ##v## I should be able to write the surface element as ##dudv## times the determinant of the jacobian:
$$ \frac {\partial x_i}{\partial u} \frac {\partial x_j}{\partial v} - \frac {\partial x_j}{\partial u} \frac {\partial x_i}{\partial v}$$
Putting all together I get:
$$\int_S \left( \frac {\partial A_i}{\partial x_j} - \frac {\partial A_j}{\partial x_i} \right) \left( \frac {\partial x_i}{\partial u} \frac {\partial x_j}{\partial v} - \frac {\partial x_j}{\partial u} \frac {\partial x_i}{\partial v} \right) dudv$$
Using the chain rule, I can simplfy the expression to yield:
$$ \int_S \left( \frac {\partial A_i}{\partial v} \frac {\partial x_i}{\partial u} - \frac {\partial x_i}{\partial v} \frac {\partial A_i}{\partial u} - \frac {\partial A_j}{\partial u} \frac {\partial x_j}{\partial v} + \frac {\partial x_j}{\partial u} \frac {\partial A_j}{\partial v} \right) dudv = 2 \int_S \left( \frac {\partial A_i}{\partial v} \frac {\partial x_i}{\partial u} - \frac {\partial x_i}{\partial v} \frac {\partial A_i}{\partial u} \right) dudv
$$
But I am pretty sure there should not be a 2 in the last equation. Is my reasoning wrong?

Thanks
Ric

There are n(n-1) possible off-diagonal values of (i,j). The way you have set your integral up, you only need the \frac12 n(n-1) terms where i < j. After changing variables to u and v your integrand is symmetric in i and j; hence your answer is twice as large as it should be.
 
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Oh I see. Since ##dx_i \wedge dx_j = - dx_j \wedge dx_i## I was counting the same surface twice!

Even though I don't know differential geometry at all, I read on Wikipedia (https://en.wikipedia.org/wiki/Differential_form) that the "differential 2-form" (whatever that is...) is defined for i<j in order to give the correct surface element. I didn't understand most of the article but it seems to me that it says the same thing that you said. Thanks!
 
dRic2 said:
Oh I see. Since ##dx_i \wedge dx_j = - dx_j \wedge dx_i## I was counting the same surface twice!

Even though I don't know differential geometry at all, I read on Wikipedia (https://en.wikipedia.org/wiki/Differential_form) that the "differential 2-form" (whatever that is...) is defined for i<j in order to give the correct surface element. I didn't understand most of the article but it seems to me that it says the same thing that you said. Thanks!

Note that <br /> \int \partial_jA_i\,dx_i \wedge dx_j = \int (\partial_2A_1-\partial_1A_2)\,dx_1 \wedge dx_2 <br /> + \int (\partial_3A_2-\partial_2A_3)\,dx_2 \wedge dx_3 <br /> + \int (\partial_3A_1-\partial_1A_3)\,dx_1 \wedge dx_3