Use Stokes Theorem to show a relationship

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Homework Statement



Use the Stokes' Theorem to show that

\intf(∇ X A) dS = \int(A X ∇f) dS + \ointf A dl

Homework Equations



Use vector calculus identities. Hint given : Start with the last integral in the above relation.

The Attempt at a Solution


To be honest, I really don't know how to start doing this. I could understand Stokes theorem when needed to evaluate the circulation, vector and surface, but I don't have any idea on how to start to prove this relation. Please help?
 
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Do you know any identities? What does stokes theorem state?
 
ArcanaNoir said:
Do you know any identities? What does stokes theorem state?

The ones that I know are like the ones states in this webpage : http://hyperphysics.phy-astr.gsu.edu/hbase/vecal2.html

Stokes theorem is \ointF.dr = \int∇ X F . n dS
 
Did you know that by convention ##\mathbf n dS## is the same as ##d\mathbf S##?

So what do you get if you set ##\mathbf F = f \mathbf A## and ##\mathbf r = \mathbf l##?

Is there another identity on your web page that you can apply then?
 
I like Serena said:
Did you know that by convention ##\mathbf n dS## is the same as ##d\mathbf S##?

So what do you get if you set ##\mathbf F = f \mathbf A## and ##\mathbf r = \mathbf l##?

Is there another identity on your web page that you can apply then?

Sorry but I still don't get it..quite confused. How should I actually begin proving it?
 
princessme said:
Sorry but I still don't get it..quite confused. How should I actually begin my proving it?

Start with \ointF.dr = \int∇ X F . dS

What do you get if you substitute ##\mathbf F = f \mathbf A## and ##\mathbf r = \mathbf l##?
 
I like Serena said:
Start with \ointF.dr = \int∇ X F . dS

What do you get if you substitute ##\mathbf F = f \mathbf A## and ##\mathbf r = \mathbf l##?

I'll get \ointfA.dl = \int∇ X F . dS
 
princessme said:
I'll get \ointfA.dl = \int∇ X F . dS

Good!
But there's still an ##\mathbf F## in there.
Can you replace that too?
 
I like Serena said:
Good!
But there's still an ##\mathbf F## in there.
Can you replace that too?

So it will be \ointfA.dl = \int∇ X fA . dS
 
  • #10
princessme said:
So it will be \ointfA.dl = \int∇ X fA . dS

Right!
Actually, let's make that \oint(fA).dl = \int∇ X (fA) . dS

Do you have another identity on your web page for something like that?
Perhaps something like ##\nabla \times (u\mathbf A)##?
 
  • #11
I like Serena said:
Right!
Actually, let's make that \oint(fA).dl = \int∇ X (fA) . dS

Do you have another identity on your web page for something like that?
Perhaps something like ##\nabla \times (u\mathbf A)##?

Okay!

Yeah ∇ x (uA) = u∇ x A - A x ∇u
 
  • #12
princessme said:
Okay!

Yeah ∇ x (uA) = u∇ x A - A x ∇u

Good!

Substitute?
 
  • #13
I like Serena said:
Good!

Substitute?

\oint(fA).dl = \int (u∇ x A - A x ∇u ) dS ?

I can see where is this going now..But the original form they wanted is f(∇ x A) dS . so u∇ x A dS is equivalent to that form?
 
  • #14
princessme said:
\oint(fA).dl = \int (u∇ x A - A x ∇u ) dS ?

I can see where is this going now..But the original form they wanted is f(∇ x A) dS . so u∇ x A dS is equivalent to that form?

Yes.
You were supposed to replace u by f as part of the substitution.
 
  • #15
I like Serena said:
Yes.
You were supposed to replace u by f as part of the substitution.

alright. So the it doesn't matter that the f in the original form is outside the bracket and not just stuck with ∇?
 
  • #16
princessme said:
alright. So the it doesn't matter that the f in the original form is outside the bracket and not just stuck with ∇?

In this case it doesn't matter. Both forms are the same.
But as a rule, you should read ##f\nabla \times \mathbf A## as ##f(\nabla \times \mathbf A)##.
 
  • #17
I like Serena said:
In this case it doesn't matter. Both forms are the same.
But as a rule, you should read ##f\nabla \times \mathbf A## as ##f(\nabla \times \mathbf A)##.

Okay thank you for the great help!
 
  • #18
I like Serena said:
In this case it doesn't matter. Both forms are the same.
But as a rule, you should read ##f\nabla \times \mathbf A## as ##f(\nabla \times \mathbf A)##.

Hi there. I have another question. I realized that I made a mistake on my Stokes' Theorem equation at first. The surface integral should be a double integral. But for the one that I need to prove, it is just a single integral. Will that make any difference to my answer?
 
  • #19
princessme said:
Hi there. I have another question. I realized that I made a mistake on my Stokes' Theorem equation at first. The surface integral should be a double integral. But for the one that I need to prove, it is just a single integral. Will that make any difference to my answer?

That's not really a mistake.
You are integrating with ##d\mathbf S## which is an infinitesimal surface element.
You can either use one or two integral symbols - it means the same thing.

Formally, it should be a single integral symbol, since there is only one infinitesimal specified.
It should only be a double integral if your integrating with the infinitesimals ##dx dy## or some such.
 

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