Little Spivak-Winding Number: Integrating Forms over Chains

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Discussion Overview

The discussion revolves around the integration of differential forms over chains, specifically in the context of problems from Little Spivak's text. Participants explore the nature of integrals defined in the problems, the properties of covering maps, and the implications of the change of variables theorem in relation to integrals of forms.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants question whether the integral defined in the problems is indeed the integral of a differential form over a chain, as the book has not yet defined this concept.
  • One participant describes their solution using the polar coordinate map and discusses the lifting property of covering maps.
  • Another participant seeks clarification on the necessity of n being an integer in problem 4-24, suggesting that the integral of dθ over the circle results in 2πn for some integer n.
  • There is a discussion about the computations involving pullbacks and the conditions under which the change of variables theorem applies.
  • Some participants express uncertainty about the relationship between the integral of a closed curve and the winding number around the circle.
  • One participant proposes that the exercise aims to show that the integral of any closed curve around the circle corresponds to a constant speed curve that winds around n times.
  • Another participant questions the assumption that the integral of c*dθ is n/2π, expressing confusion about this being a given in the problem.
  • A later reply discusses the existence of a 2-cube with a specific boundary condition and relates it to the fundamental group of the plane.

Areas of Agreement / Disagreement

Participants express various viewpoints regarding the nature of the integrals and the properties of the curves involved. There is no consensus on several points, including the necessity of certain conditions for the integrals and the interpretation of the results in the context of the problems.

Contextual Notes

Some participants note limitations in their understanding of covering maps and the change of variables theorem, which may affect their interpretations of the integrals discussed. There is also mention of the need for positive determinants in certain computations, indicating potential restrictions in the application of theorems.

sammycaps
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So I'm working on Little Spivak and I found a solution to problem 4-24 at http://www.ms.uky.edu/~ken/ma570/homework/hw18/html/ch4c.htm. My question is, is the integral defined there the integral of a differential form over a chain, or something else?

I only ask because the book did not reach the point of defining integration of forms over chains until 1 page later.

Thanks
 
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sammycaps said:
So I'm working on Little Spivak and I found a solution to problem 4-23 at http://www.ms.uky.edu/~ken/ma570/homework/hw18/html/ch4c.htm. My question is, is the integral defined there the integral of a differential form over a chain, or something else?

I only ask because the book did not reach the point of defining integration of forms over chains until 1 page later.

Thanks
Do you mean #24?
 
Yes, sorry about that.
 
my solution used the polar coordinate map, and lifted the chain through the convex domain space of that map. no integration needed. do you know about covering maps?
 
mathwonk said:
my solution used the polar coordinate map, and lifted the chain through the convex domain space of that map. no integration needed. do you know about covering maps?

I've seen a bit of covering maps, but I don't know too much about them. I took a course that studied the fundamental group (but oddly skipped covering maps). Is your solution online?

As an aside, is the c* in the link I posted the pullback operator, or something else (once I know that I can rest and check out your solution).
 
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the point is the "polar coordinate" map P taking (r,t) to (e^rcos(t), e^rsin(t)), has the "lifting property".. I.e. any map f from a closed interval into the complement of (0,0) in the plane, factors through P.

I.e. given f:I-->R^2 - (0,0), there is a map g:I-->R^2, such that f = Pog. That let's you work in R^2 instead of R^2 - (0,0). and in R^2 you have convexity to let you fill things in.
 
Hmmm, I'll have to review covering spaces. So, then you would just fill the closed curve in and use that to get the 2-cube with boundary the difference of the two curves?
 
Also, in the link I posted at the beginning of the thread, can anyone explain why n in problem 4-24 is necessarily an integer?
 
sammycaps said:
Also, in the link I posted at the beginning of the thread, can anyone explain why n in problem 4-24 is necessarily an integer?

the form d\theta integrates to 2\pi over the circle. The formul in the exercise is just a change of variables.
 
  • #10
sammycaps said:
So I'm working on Little Spivak and I found a solution to problem 4-24 at http://www.ms.uky.edu/~ken/ma570/homework/hw18/html/ch4c.htm. My question is, is the integral defined there the integral of a differential form over a chain, or something else?

I only ask because the book did not reach the point of defining integration of forms over chains until 1 page later.

Thanks

Yes it is an integral over a chain. The author is asking you to verifiy that any closed curve along the circle integrates to 2\pin for some integer n. intuitively it wraps around the curcle n times.
 
  • #11
lavinia said:
the form d\theta integrates to 2\pi over the circle. The formul in the exercise is just a change of variables.

Maybe I'm just not used to the computations with pullbacks. I get ∫c*d\theta=∫f1(c)det(c')+f2(c)det(c'), where f1 and f2 are the component functions of d\theta. Is this right? Why does this get you an integer (once you normalize it by 2∏)

And for it to be change of variables, don't we have to assume det(c') is positive?
 
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  • #12
sammycaps said:
Maybe I'm just not used to the computations with pullbacks. I get ∫c*d\theta=∫f1(c)det(c')+f2(c)det(c'), where f1 and f2 are the component functions of d\theta. Is this right? Why does this get you an integer (once you normalize it by 2∏)

And for it to be change of variables, don't we have to assume det(c') is positive?

I spoke a little loosely. Because of the change of variables theorem, the integral of a form over a smooth simplex can be defined as the integral of any pull back. Two different pull backs are connected by a change of variables.

The form d\theta is dual to the tangent unit length vector field of the circle. Its integral is just the length of the circle. As Mathwonk pointed out its integral is the same as integrating dx over an interval of length 2\pi.
 
  • #13
lavinia said:
I spoke a little loosely. Because of the change of variables theorem, the integral of a form over a smooth simplex can be defined as the integral of any pull back. Two different pull backs are connected by a change of variables.

The form d\theta is dual to the tangent unit length vector field of the circle. Its integral is just the length of the circle. As Mathwonk pointed out its integral is the same as integrating dx over an interval of length 2\pi.

I think I sort of understand, but I'm not sure how to see that it must integrate to 2\pin, for some n, explicitly. I'm on a pretty basic level, since I just started learning about this stuff.
 
  • #14
sammycaps said:
I think I sort of understand, but I'm not sure how to see that it must integrate to 2\pin, for some n, explicitly. I'm on a pretty basic level, since I just started learning about this stuff.

The point of the exercise is to show that every integral of a closed curve around the circle is the same same as the integral of a constant speed curve that winds around the circle n times. n can be any integer, positive, negative, or zero. That is why the integral is always an integer.
 
  • #15
lavinia said:
The point of the exercise is to show that every integral of a closed curve around the circle is the same same as the integral of a constant speed curve that winds around the circle n times. n can be any integer, positive, negative, or zero. That is why the integral is always an integer.

I understand (or maybe not), but the solution that I posted asks that you first take as given that ∫c*dθ is n/2∏. I don't see this (especially if the goal of the entire problem is essentially to prove this).

Am I completely missing the point?
 
  • #16
So I might have worked it out (or at least thought about it a bit more), so I have another question (answers to the above are also very welcome). It is possible to find a 2-cube which has boundary = c1,n-c1,m if n≠m, if you allow the 2-cube to map to (0,0)? Or, does no 2-cube exist with such boundary (here c1,n(t)=(cos(2∏nt),sin(2∏nt))).

If I'm thinking about it correctly, one should exist since the fundamental group of the plane is trivial (so we can just linearly interpolate). But, I wasn't sure.
 
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  • #17
Maybe this will be helpful.

In polar coordinates in the plane dθ is a closed 1 form in the plane minus the origin.

By Stokes theorem its integral over any closed curve that bounds a smooth rectangle is zero. Note that such a rectangle does not to contain the origin and this means that its bounding curve does not wind around the origin.

Note also that this rectangle does not seen to be a geometric rectangle but only the smooth image of one, a smooth singular 2 cube. This follows from the change of variables theorem and the relation

fc* = f*d for any smooth function,f.

Now suppose you have a curve that does wind around the origin. If you retrace it exactly backwards, then the one followed by its reverse no longer winds around the origin. And it is clear that the integral of c*dθ over the combined curve is zero since the first half is negated by the second.But you do not need to exactly retrace the curve backwards to unwind it. If it winds around the origin n times, then any curve that winds around -n times will undo it. For instance the curves

R(cos-nθ,sin-nθ) will unwind a curve that winds around the origin +n times. In your problem you are asked to show this.

The method is to show that the original curve followed by one the the R(cos-nθ,sin-nθ)'s is the boundary of a smooth singular 2 cube then apply Stokes theorem. Since ddθ = 0 the integral is zero so the integral over the boundary is zero. But the integral over the boundary is the sum of the integrals of dθ over the original curve and R(cos-nθ,sin-nθ) so their integrals are negatives of each other.
 
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