Understanding the Lie Derivative for Tensor Fields

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Discussion Overview

The discussion revolves around the Lie derivative for tensor fields, particularly focusing on its definition and implications when applied to functions. Participants explore the mathematical formulation of the Lie derivative, its behavior with scalar fields, and the nuances of tensor mappings in the context of diffeomorphisms.

Discussion Character

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

Main Points Raised

  • One participant presents a definition of the Lie derivative and questions why the numerator becomes zero when applied to a function, suggesting a potential inconsistency.
  • Another participant encourages exploration of special cases to reconcile the apparent contradiction in the numerator being zero.
  • A different participant argues that the numerator should be nonzero prior to taking the limit, drawing a comparison to the ordinary derivative of a function.
  • Discussion includes the extension of tangent mappings and the conceptual understanding of scalar fields versus functions, with one participant noting that real-valued functions are not scalar fields.
  • Another participant emphasizes the importance of working with scalar fields and discusses the natural conversion between scalar fields and functions.
  • A participant from an engineering background seeks clarification on using the Lie derivative in a project involving symmetric tensor fields and expresses frustration over understanding the mathematical concepts involved.

Areas of Agreement / Disagreement

Participants express differing views on the behavior of the Lie derivative when applied to functions, with no consensus reached on the implications of the numerator being zero. The discussion remains unresolved regarding the correct application of the Lie derivative in the context of tensor fields.

Contextual Notes

Limitations include the dependence on definitions of scalar fields and functions, as well as the unresolved mathematical steps concerning the behavior of the Lie derivative in specific cases.

jdstokes
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Suppose we define the Lie derivative on a tensor T at a point p in a manifold by

\mathcal{L}_V (T) = \lim_{\epsilon \to 0}\frac{\varphi_{-\epsilon \ast}T(\varphi_\epsilon(p))- T(p)}{\epsilon}

where V is the vector field which generates the family of diffeomorphisms \varphi_t.

If T is just an ordinary function f:M \to \mathbb{R} then it seems like the numerator of the above expression is f(p) - f(p) = 0 which is unusual since I thought the lie derivative of a function was the ordinary derivative \mathcal{L}_V f = V^\mu \partial_\mu f. Can anyone reconcile this?

Thanks
 
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jdstokes said:
it seems like the numerator of the above expression is f(p) - f(p) = 0
...
Can anyone reconcile this?
You've already given yourself a hint! :smile:

Why do you think that numerator seems like that?


Also... have you tried any special cases, to see what happens?
 
I don't understand why the numerator is zero. The numerator should be a small quantity but definitely nonzero. Consider the ordinary derivative of a function f : \mathbb{R} \to \mathbb{R}:

\frac{df}{dx} = \lim_{\epsilon \to 0} \frac{f(x + \epsilon) - f(x)}{\epsilon}.

Note that prior to evaluation of the limit the numerator is nonzero, as it should be. But with the Lie derivative the numerator is already zero before we even evaluate the limit!

\varphi_{-\epsilon\ast}(f(\varphi_\epsilon(p))) - f(p)= f (\varphi_{-\epsilon}\circ \varphi_\epsilon(p)) -f(p)= 0.

My formula for the Lie derivative must not apply when considering functions.
 
The tangent mapping

<br /> \varphi_{-\epsilon *}:T_{\varphi(\epsilon,p)}M\to T_p M<br />

gets extended naturally to

<br /> \varphi_{-\epsilon *}:(T_{\varphi(\epsilon,p)}M)^k\to (T_p M)^k,<br />

but for k=0 you need to stop for a moment to wonder what that mapping is supposed to mean. In fact IMO it doesn't even make fully sense to say that a smooth mapping

<br /> M\to \bigsqcup_{p\in M}(T_p M)^0<br />

would be a real valued M\to\mathbb{R}, but isn't that the convention anyway? And then

<br /> \varphi_{-\epsilon *} (f(\varphi_{\epsilon}(p)})) = f(\varphi_{\epsilon}(p))<br />

is convention too?
 
Last edited:
I see you've noticed that real-valued functions are not scalar fields! Just as (tangent) vector fields are sections of the tangent bundle1, scalar fields are sections of the trivial line bundle1 M \times \mathbb{R} \to M. (note that M \times \mathbb{R} \cong \coprod_{p \in M} \mathb{R})

Recall that \varphi_{\epsilon*} was initially only defined on the tangent spaces; do you recall how you extended it to the entire tensor algebra? That will explain why \varphi_{\epsilon*}(p, x) = (\varphi_\epsilon(p), x) for any point p and scalar x. (I've used (p, x) to denote the element x of the fiber at p of the trivial line bundle)


Generally, you want to work with scalar fields, and not functions M \to R; happily, there is a natural conversion between the two concepts, so it's easy to go back and forth between them when it's convenient to do so.


1: these things are, of course, not unique -- but all such objects are isomorphic.
 
May I ask a couple very basic and simple questions related to this topic? Since I'm currently working on a project requiring advanced tensor math knowlede but I'm from engineering background :(

I need to obtain a diffeomorphism \varphi_t that maps a tensor field T_1 to another tensor field T_2, assume they are symmetric tensors in R^3\times R^3R^3*R^3. The function is to map each tensor in T_1 to the corresponding one in T_2 by translating and rotating the tensor at location p to p', but doesn't change the shape of the tensor.

I think the derivative of T_1(\varphi(p))-T_2(p) should be computed to estimate the function \varphi. Is the Lie derivative the right one to use?

Also during the numerical implimentation, at each iteration, how can I update \varphi? If it's a function from scalar to scalar, then I only need obtain the gradient of some cost function, and update \varphi which only contains translation in R^3.

Sorry if my questions are confusing or totally nonsense. Any suggestion will be appreciated. I've been struggling with this for several weeks, and don't have any clue. I feel so frustrated:frown:
 

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