Proving \int curl A.n dS = 0 w/ Stokes Theorem

In summary: Yes, your proof for (1) is correct. As for (2), the proof for the identity div(curl A) = 0 is a bit more involved and requires using the identities for cross and dot products. You can find a detailed proof online or in a calculus or vector calculus textbook.
  • #1
smoothman
39
0
(1)

using stokes theorem and cutting the surface into 2 parts how can we prove that

[tex]\int [/tex] curl A.n dS = 0

assume the surface "S" to be smooth and closed, and "n" is the unit outward normal as usual.

(2)
How can you prove
[tex]\int [/tex] curl A.n dS = 0
using the divergence theorem?
 
Mathematics news on Phys.org
  • #2
What have you attempted? I mean if, in (1), you just follow the hints the answer seems like it is immediate, so how have you tried to use the hints?
 
  • #3
im confused because A hasn't been defined and neither has r(t)??
what shall i assume those to be?
 
  • #4
You were the one who asked the question! What exactly is the statement? It is certainly not true that
[tex]\int \nabla \cross \vec{A}\cdot\vec{n}dS= 0[/itex]
for arbitrary [itex]\vec{A}[/itex]!

What exactly are you asking? If this is homework problem, state exactly what it says. Is [itex]\vec{A}[/itex] a constant vector? It would be easy in that case.

As far as r(t) is concerned, there was no "r(t)" in your original post!
 
  • #5
Whatever A is supposed to be, or the surface, it is clear that (1) wants you to split the surface into two regions (presumably they'll need to be simply connected), then replace the integral over those two surfaces with the line integrals along the boundary - of course we may have to make some leap like taking the closure of the two subsets, but that is immaterial, and then noticing that you reverse the orientation on one, and cancel.
 
  • #6
for part (1)
the only information provided was that :

"assume the surface "S" to be smooth and closed, and "n" is the unit outward normal as usual."

now what do i assume the parameters to be.. i understand that

[itex]\int curl A.ndS = \int A.dr [/itex]

so i assume i have to show : [itex] \int A.dr [/itex] = 0??

but how do i start this off since i haven't been given any parameters etc
 
  • #7
HallsofIvy said:
You were the one who asked the question! What exactly is the statement? It is certainly not true that
[tex]\int \nabla \cross \vec{A}\cdot\vec{n}dS= 0[/itex]
for arbitrary [itex]\vec{A}[/itex]!

What exactly are you asking? If this is homework problem, state exactly what it says. Is [itex]\vec{A}[/itex] a constant vector? It would be easy in that case.

As far as r(t) is concerned, there was no "r(t)" in your original post!


it doesn't state what A is.. all it says is:

S is a smooth closed surface.. n i a unit outward normal to S... that's it..

i haven't been given A... or r(t) or the radius of the curve.. or anythin like that,... so what would i assume the parameters to be
 
  • #8
i think i have managed to work out part 2:

if F = curl A
the div theorem says:
[itex]\int_v div(curlA)dV = \oint Curl A.ndS[/itex]

div(curl A) = 0
So: [itex]\oint CurlA.ndS = 0 [/itex]

i understand that the identity div(curl A)=0 but how is this proved please?
 
  • #9
Tediously. It is just an exercise in manipulating partial derivatives.
 
  • #10
And I still fail to see what is troubling about 1, and I don't get Halls' objections at all. You have a smooth closed surface, like a sphere. Split it into two hemispheres and apply Stokes' theorem, and you're done - you have two line integrals, integrating the same function over the same boundary but with opposite orientations.
 
  • #11
matt grime said:
And I still fail to see what is troubling about 1, and I don't get Halls' objections at all. You have a smooth closed surface, like a sphere. Split it into two hemispheres and apply Stokes' theorem, and you're done - you have two line integrals, integrating the same function over the same boundary but with opposite orientations.

to work out the question i need to work out [itex]\int A.dr = \int A(r(t)). r(t)dt [/itex]
but i don't know the values of r. and I am not given the parameter of r(t)?

so how would i start the question when I am not even given anythin to work with? please start me off here and ill attempt the rest
 
  • #12
Why would you want to actually work out the integral? Change a surface integral into two surface integrals, then turn these into two line integrals. This completes the proof as far as I can tell.
 
  • #13
stokes theorem says that for any smooth oriented surface, that surface integral can be computed as an integral over the boundary of the surface.

if the surface is closed, i.e. the boundary is empty, then the boundary integral is necessarily zero.
 
  • #14
use 2 spheres. simple as. orient them in opposite directions. they cancel out.
 
Last edited:
  • #15
i understand what is being told to me.. but what i need help on is showing this mathematically..

i know the 2 spheres cancel each other out since they are oriented in different directions...

i know i need to show that the 2 line integrals cancel each other out..

but my problem is::::: What Are The Values That I Use For The Line Integrals? since i am not given this in the question.

i was told to prove that [itex]\int curl A.ndS = 0 [/itex] so surely i need to show this mathematically instead of just using words...

so please help me on how to show this mathematically! greatly appreciated..
thnx.. no one seems to hav made that clear to me so far.
 
  • #16
did you understand my post? i have completely answered your question, which has nothing to do with spheres, or cutting anything open.
 
  • #17
kind of.. but the question says that you HAVE to cut the sphere into 2 pieces..

here is what i worked out.. please verify if it is correct..

(1)

so is this proof correct:

[itex]\int curl A.n dS = \int A.dr [/itex]

cutting the sphere horizontally into 2 hemispheres we have...

[itex]\int A.dr - \int A.dr = 0.. [/itex]

therefore, [itex]\int curlA.n ds = 0...[/itex]

is this proof correct??

(2)

for 2 i managed to show

if F = curl A
the div theorem says:
[itex]\int_v div(curlA)dV = \oint Curl A.ndS[/itex]

div(curl A) = 0
So: [itex]\oint CurlA.ndS = 0 [/itex]

i understand that the identity div(curl A)=0 but how is this proved please?
 
  • #18
[itex]curl A= \hat i(\frac{\partial A}{\partial y} - \frac{\partial A}{\partial z}) -\hat j(\frac{\partial A}{\partial x} - \frac{\partial A}{\partial z}) + \hat k(\frac{\partial A}{\partial x} - \frac{\partial A}{\partial y}) [/itex]
then
[itex]div(curl A)= \frac{\partial}{\partial x}(\frac{\partial A}{\partial y} - \frac{\partial A}{\partial z}) + \frac{\partial}{\partial y}(-\frac{\partial A}{\partial x} + \frac{\partial A}{\partial z}) + \frac{\partial}{\partial z}(\frac{\partial A}{\partial x} - \frac{\partial A}{\partial y}) = 0[/itex]
i mean, this happens when A is a C^2 function, so you can use Schwartz theorem: mix the derivatives, and it's zero =)
 
Last edited:
  • #19
do you know how to prove stokes theorem? you paste together the greens theorem in a bunch of rectangles.

i.e. green says the path integral of a one - form over the boundary of a rectangle, equals the integral of the curl of that one form over the interior of the rectangle. then if you have a more extensive region you just cut it up into rectangles and apply greens theorem to each rectangle and add.

the path integrals over the boundaries of those rectangles that share a boundary cancel, while the area integrals over the adjacent areas add, and it leaves you with the desired statement.

i.e. after all the canceling of boundaries traversed in opposite directions, the sum of all the path integrals equals the path integral over those portions of the boundaries only traversed once, i.e. the boundary of the original surface.

hence if it hapens that all the boundaries cancel, i.e. that the original surface has empty boundary, then all the path integrals cancel out leaving zero.

if they had stated the stokes theorem correctly in the first place, i.e. as saying the integral of the curl over the surface equals the path integral of the vector field over the boundary, this is simply zero when that boundary is empty.

so i suggest you try to understand the topic as well as get the answer to the question, since the questioner is perhaps not firing on all cylinders here. i.e. pleasing the teacher is not life's ultimate goal.

or perhaps your teacher is trying to illustrate the methid of proof of the stokes theorem? but then they should have said to deduce it from greens theorem, or maybe they gave you a very preliminary version of stokes theorem?as we say here so often, at some point one wants to get on the freeway, and off the exit ramps, and start making some progress.good luck.
 
Last edited:
  • #20
nice explanation mathwonk... at least, it was useful for me :D

*anyway, i thought that green theorem was a particular case of the stokes theorem... :/, i guess i have to study this again xDD
 
Last edited:
  • #21
smoothman said:
i was told to prove that [itex]\int curl A.ndS = 0 [/itex] so surely i need to show this mathematically instead of just using words.

When did words stop being mathematical explanations?
 
  • #22
smoothman said:
[itex]\int curl A.n dS = \int A.dr [/itex]

what are you integrating over?

cutting the sphere horizontally into 2 hemispheres we have...

[itex]\int A.dr - \int A.dr = 0.. [/itex]

where did this come from? I see no justification for any of that and, again what are the regions you're integrating over?
therefore, [itex]\int curlA.n ds = 0...[/itex]

is this proof correct??

no. All those 'words' you objected to have been ignored. Words are important. As is getting the correct region of integration.

All you've written is X=Y, and Y-Y=0 without explaining what X or Y are and why they are related.
 
  • #23
particular cases are often used to prove general ones. and technically, to use greens as i said, one needs to
pull back" greens from a curved rectangle lying on a surface, to a flat rectangle in the plane. this is called changing coordinates.
 

Related to Proving \int curl A.n dS = 0 w/ Stokes Theorem

1. What is the concept behind Stokes Theorem?

Stokes Theorem is a mathematical tool used in vector calculus to relate the integral of a vector field over a surface to the line integral of the same vector field around the boundary of that surface.

2. How is Stokes Theorem used to prove ∫curl A·n dS = 0?

To prove ∫curl A·n dS = 0 using Stokes Theorem, we first express the integral as a line integral using the divergence theorem. Then, we use the fact that curl A is equal to the line integral of A around the boundary of the surface, which is equal to 0 by the divergence theorem. Therefore, the integral is equal to 0.

3. What is the significance of proving ∫curl A·n dS = 0 using Stokes Theorem?

Proving ∫curl A·n dS = 0 using Stokes Theorem is significant because it allows us to relate the line integral of a vector field to the surface integral of its curl. This relationship is useful in various applications in physics and engineering.

4. Can Stokes Theorem be used to prove other equations in vector calculus?

Yes, Stokes Theorem can be used to prove various other equations in vector calculus, such as the generalized Stokes Theorem and the Kelvin-Stokes Theorem. It is a powerful tool that helps simplify and solve complex integrals.

5. Are there any limitations to using Stokes Theorem?

Stokes Theorem has certain limitations, including the requirement that the surface must be oriented and closed, and the vector field must be continuously differentiable. Additionally, the surface must be able to be parameterized as a function of two variables. These limitations must be considered when applying Stokes Theorem to a problem.

Similar threads

  • General Math
Replies
3
Views
2K
  • Calculus and Beyond Homework Help
Replies
1
Views
635
  • Calculus and Beyond Homework Help
Replies
4
Views
861
  • Calculus and Beyond Homework Help
Replies
2
Views
1K
Replies
1
Views
2K
Replies
2
Views
2K
  • Calculus and Beyond Homework Help
Replies
6
Views
2K
  • General Math
Replies
12
Views
6K
  • Differential Equations
Replies
1
Views
2K
Replies
12
Views
1K
Back
Top