Differential Forms and Gradients

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Homework Help Overview

The discussion revolves around the concept of exterior differentiation of 0-forms in the context of differential forms and gradients, specifically in R3 and R2. Participants are exploring the relationship between exterior differentiation and the gradient of a function.

Discussion Character

  • Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants are attempting to relate the exterior differentiation of a 0-form to the gradient, questioning the definitions and properties of differential forms and dual forms. There are discussions about the notation for partial derivatives and the interpretation of differential forms in relation to vectors.

Discussion Status

The conversation is ongoing, with participants providing insights and asking clarifying questions. Some have suggested resources for better understanding, while others are exploring the mathematical definitions and implications of their findings without reaching a consensus.

Contextual Notes

Some participants express a lack of background knowledge in differential forms, indicating that their understanding is based on multivariable calculus. There are mentions of difficulties in finding appropriate references for the definitions being discussed.

TranscendArcu
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Homework Statement


Show that exterior differentiation of a 0-form f on R3 is essentially the same as calculating the gradient of f.

The Attempt at a Solution

Let U be a differentiable 0-form on R3. I think

[tex]dU = \sum _{j=1} ^n \frac{δF_I}{δx_j}dx_j dx_I[/tex]However, since U is a 0-form, I can write U = FI and drop the dxI, right? I would then have,

[tex]dU = \sum _{j=1} ^n \frac{δF_I}{δx_j}dx_j<br /> = \frac{U dx}{δx} + \frac{U dy}{δy} + \frac{U dz}{δz}[/tex]This, I think, has partial derivatives in it, but looks more like [itex]\nabla • U[/itex] than [itex]\nabla U[/itex], the latter of which should be a vector.
 
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You probably want to use '\nabla' for your partial derivative symbol. But no, it's not like a divergence. It's not a scalar sum. dx is the dual form to the basis vector associated with x. To find rate of change along a direction v you dot the gradient vector with v. To find the rate of change using your form, you evaluate the form on the vector. You get the same thing.
 
Okay. First of all, what is a dual form to the basis vector? Also, what do you mean by evaluate the form on the vector? Could you give an example?
 
TranscendArcu said:
Okay. First of all, what is a dual form to the basis vector? Also, what do you mean by evaluate the form on the vector? Could you give an example?

Take e_x=(1,0,0), e_y=(0,1,0), and e_z=(0,0,1). Those are your basis vectors. dx is a linear function on vectors, yes? And dx(e_x)=1, dx(e_y)=0, dx(e_z)=0. Etc. That's what I mean by evaluate the form on vectors. If v=a*e_x+b*e_y+c*e_z, then dx(v)=a, dy(v)=b, dz(v)=c. How did you define 'dx'?
 
The only definition of dx I know is that of the differential distance. That is, taking small (I suppose linear) steps in the direction of x. Is that what you're looking for?

In any case, do I correctly sense that I have to make U into [itex]\vec{U}[/itex]?
 
TranscendArcu said:
The only definition of dx I know is that of the differential distance. That is, taking small (I suppose linear) steps in the direction of x. Is that what you're looking for?

In any case, do I correctly sense that I have to make U into [itex]\vec{U}[/itex]?

If that's your definition of dx as a differential form, I think you may have skipped a chapter. Try and look back in the text and find a real definition. And no, you can't make U into a vector, it's not a vector. It's a real function on R^3, just like any 0-form.
 
Well, truth be told, I only have the mathematical background up to multivariable calculus. That is, the class one might take at the conclusion of BC in high school. What I'm working on here is an extra-credit assignment given our by my instructor. My regular calculus textbook really has nothing in it on either differential k-forms. So I'm trying to piece together what these things k-forms are by googling examples and asking around here.

In other words, I don't have another calculus reference to get a real definition for dx. If you know where I might find one, I'd be very appreciative.
 
TranscendArcu said:
Well, truth be told, I only have the mathematical background up to multivariable calculus. That is, the class one might take at the conclusion of BC in high school. What I'm working on here is an extra-credit assignment given our by my instructor. My regular calculus textbook really has nothing in it on either differential k-forms. So I'm trying to piece together what these things k-forms are by googling examples and asking around here.

In other words, I don't have another calculus reference to get a real definition for dx. If you know where I might find one, I'd be very appreciative.

I'm having a hard time finding one just now. The trouble is that you usually start talking about differential forms when you are dealing with tangent spaces to manifolds. So the language can get hard to deal with pretty quickly. Try starting with this one. http://www.sjsu.edu/faculty/watkins/difforms0.htm I only fished through the first half dozen or so links I found, so there's probably something better as well.
 
Okay. So I took some time to read through the link. I didn't understand everything (even though I have done a bit with vectors, I haven't seen the term "vector space" before). Anyway, let me try a simpler application of these differential forms. Show that exterior differentiation of 0-forms on R1 is essentially the same as ordinary differentiation of smooth functions. So I have,
[tex]dU = \sum _{j=1} ^n \frac{δF_I}{δx_j}dx_j<br /> = \frac{U dx}{δx} + \frac{U dy}{δy} + \frac{U dz}{δz}[/tex]Let U be a differential 0-form such that U=f(x). Thus,
[tex]dU = \sum _{j=1} ^1 \frac{δf(x)}{δx_j}dx_j<br /> = \frac{δf(x)}{δx} dx[/tex]Which I think I can rewrite as

[tex]dU = f'(x) dx[/tex]This is what I wanted to show, right?
 
  • #10
Whoops, I copied that first line of math incorrectly. I should probably just scrap it. I think I should just have:

Let U be a differential 0-form such that U=f(x). Thus,
[tex]dU = \sum _{j=1} ^1 \frac{δf(x)}{δx_j}dx_j<br /> = \frac{f(x)}{δx} dx[/tex]Which I think I can rewrite as

[tex]dU = f'(x) dx[/tex]That's what I wanted, I think.
 
  • #11
TranscendArcu said:
Whoops, I copied that first line of math incorrectly. I should probably just scrap it. I think I should just have:

Let U be a differential 0-form such that U=f(x). Thus,
[tex]dU = \sum _{j=1} ^1 \frac{δf(x)}{δx_j}dx_j<br /> = \frac{f(x)}{δx} dx[/tex]Which I think I can rewrite as

[tex]dU = f'(x) dx[/tex]That's what I wanted, I think.

You should figure out a better way to display partial derivatives, like I said, use \nabla. But the math part looks ok to me.
 
  • #12
http://img338.imageshack.us/img338/8190/skjermbilde20111207kl10.png
I was trying to recreate the loopy d's in the equation you see above. What is the code for those?
 
Last edited by a moderator:
  • #13
Oops, I've been saying the wrong thing. The code is \partial. [tex]\frac{ \partial f }{ \partial x}[/tex]
 
  • #14
Okay. So the next part of the question is "Show that exterior differentiation of a 0-form f on R2 is essentially the same as calculating the gradient of f."

So I have [tex]dU = \sum _{j=1} ^2 \frac{\partial{f(x)}}{\partial{x_j}}dx_j<br /> = \frac{f(x)}{\partial{x}} dx +\frac{f(x)}{\partial{y}} dy[/tex]As a vector, this would be written as [itex]<\frac{f(x)}{\partial{x}},\frac{f(x)}{\partial{y}}>[/itex] right? And is this, then, not just the same as [itex]\nabla U[/itex]?
 
  • #15
TranscendArcu said:
Okay. So the next part of the question is "Show that exterior differentiation of a 0-form f on R2 is essentially the same as calculating the gradient of f."

So I have [tex]dU = \sum _{j=1} ^2 \frac{\partial{f(x)}}{\partial{x_j}}dx_j<br /> = \frac{f(x)}{\partial{x}} dx +\frac{f(x)}{\partial{y}} dy[/tex]As a vector, this would be written as [itex]<\frac{f(x)}{\partial{x}},\frac{f(x)}{\partial{y}}>[/itex] right? And is this, then, not just the same as [itex]\nabla U[/itex]?

Like the question said, it is "essentially the same thing". But it's not the SAME thing. It's not a vector. It's a linear function on vectors.
 
  • #16
[tex]dU = \sum _{j=1} ^2 \frac{\partial{f(x)}}{\partial{x_j}}dx_j<br /> = \frac{\partial{f(x)}}{\partial{x}} dx +\frac{\partial{f(x)}}{\partial{y}} dy[/tex]So, right now, the only similarity I see between this and the gradient is that they both have partial derivatives, and that both require you to calculate partial derivatives. So, yes, computationally I can see the relationship between the two. But is that really the only connection?

Also, notice that I've written [itex]\frac{\partial{f(x)}}{\partial{y}} dy[/itex] Is this bad notation? Would it be better to write f(x,y)?

Also, how come I can't find the edit button anywhere?
 
  • #17
TranscendArcu said:
[tex]dU = \sum _{j=1} ^2 \frac{\partial{f(x)}}{\partial{x_j}}dx_j<br /> = \frac{\partial{f(x)}}{\partial{x}} dx +\frac{\partial{f(x)}}{\partial{y}} dy[/tex]So, right now, the only similarity I see between this and the gradient is that they both have partial derivatives, and that both require you to calculate partial derivatives. So, yes, computationally I can see the relationship between the two. But is that really the only connection?

Also, notice that I've written [itex]\frac{\partial{f(x)}}{\partial{y}} dy[/itex] Is this bad notation? Would it be better to write f(x,y)?

Also, how come I can't find the edit button anywhere?

f(x,y) would certainly be better. Go back and reread post 2 for the connection. And the Edit button has been on and off lately.
 

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