Stoke's theorem rewritten, not in book, but am I right?

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Homework Statement

This is Stoke's theorem in my textbook and I am trying to write it in a new form

\iint_S curl \mathbf{F} \cdot d\mathbf{S}

The Attempt at a Solution



\iint_S curl \mathbf{F} \cdot d\mathbf{S} = \iint_S curl \mathbf{F} \cdot \hat{n} dS = \iint_S curl \mathbf{F} \cdot \frac{(\mathbf{r_u} \times \mathbf{r_v})}{|\mathbf{r_u} \times \mathbf{r_v}|} |\mathbf{r_u} \times \mathbf{r_v}| dA = \iint_S curl \mathbf{F} \cdot (\mathbf{r_u} \times \mathbf{r_v}) dA
 
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... what is \bf{r}_u and \bf{r}_v?
 
The partial derivatives of my parametric surface which I forgot to define...

So r(u,v)
 
flyingpig said:

Homework Statement




This is Stoke's theorem in my textbook and I am trying to write it in a new form

\iint_S curl \mathbf{F} \cdot d\mathbf{S}
No, that is not Stoke's theorem.



The Attempt at a Solution



\iint_S curl \mathbf{F} \cdot d\mathbf{S} = \iint_S curl \mathbf{F} \cdot \hat{n} dS = \iint_S curl \mathbf{F} \cdot \frac{(\mathbf{r_u} \times \mathbf{r_v})}{|\mathbf{r_u} \times \mathbf{r_v}|} |\mathbf{r_u} \times \mathbf{r_v}| dA = \iint_S curl \mathbf{F} \cdot (\mathbf{r_u} \times \mathbf{r_v}) dA
 
Sorry I meant that

\iint_S curl \mathbf{F} \cdot d\mathbf{S} = \oint \mathbf{F} \cdot d\mathbf{r}
 
The idea is correct. Except that n might be either +/-(r_u x r_v)/|r_u x r_v| depending on the direction of the normal implied by the problem.
 
There are two things I don't understand about this problem. First, when finding the nth root of a number, there should in theory be n solutions. However, the formula produces n+1 roots. Here is how. The first root is simply ##\left(r\right)^{\left(\frac{1}{n}\right)}##. Then you multiply this first root by n additional expressions given by the formula, as you go through k=0,1,...n-1. So you end up with n+1 roots, which cannot be correct. Let me illustrate what I mean. For this...
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