What kind of tensor is the gradient of a vector Field?

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SUMMARY

The gradient of a tangent vector field, represented as a type (1,0) tensor, results in a type (1,1) tensor when differentiated using the covariant differential operator. Conversely, the gradient of a dual vector field yields a type (0,2) tensor. The discussion emphasizes that while vector spaces and their duals are isomorphic, this isomorphism is not canonical. The integrability condition for a vector field to be a gradient field is also highlighted, indicating that closed curves must yield zero.

PREREQUISITES
  • Understanding of tensor types (e.g., (1,0), (1,1), (0,2))
  • Familiarity with covariant differentiation and differential operators
  • Knowledge of vector spaces and dual vector spaces
  • Basic concepts of integrability in vector fields
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  • Explore the properties of covariant derivatives in differential geometry
  • Study the implications of the integrability condition for vector fields
  • Learn about the relationship between vector spaces and their duals in linear algebra
  • Investigate the concept of natural versus canonical isomorphisms in mathematics
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Mathematicians, physicists, and students in advanced calculus or differential geometry, particularly those interested in tensor analysis and vector field theory.

  • #31
PrecPoint said:
(ie a metric tensor field)
No, not necessarily a metric tensor field. A non-degenerate bilinear form. This is not the same thing. A metric tensor is a bilinear form but a bilinear form is not necessarily a metric (or even a pseudo-metric). Again, the typical example would be the (fully anti-symmetric) symplectic form in symplectic geometry.

PrecPoint said:
Please pay attention to the bold words
Please pay attention to the bold words:
martinbn said:
All tangent spaces to all points on a manifold are isomorphic
 
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  • #32
A vector space and its dual differ in the way their elements transform under linear maps. If a linear map ##L## maps the vector space ##V## into the vector space ##W## then by definition elements of ##V## are sent to elements of ##W##.

However elements of the dual space ##V^{*}## are not sent to elements of ##W^{*}##. Instead it is the other way around. Elements of ##W^{*}## are sent to elements of ##V^{*}##.

Schematically this transformation difference can be represented by two diagrams:

##L:V→V## ##L^{*}:W^{*}→V^{*}##

This difference in transformation direction distinguishes a vector space and its dual. I would guess that this automatically excludes the possibility of a natural transformation between the identity functor and the "dual"" functor that maps each vector space to its dual and each linear map to its induced map on dual spaces. A natural transformation would seem always to preserve the direction of transformation. @fresh_42 is this correct?

This is a purely algebraic consideration and does not require manifolds or tensors or anything else. However, on a smooth manifold, the differential of a smooth map ##f:M→N## between two manifolds ##df:TM→TN## maps tangent vector in ##TM## to tangent vectors in ##TN## while the dual of the differential ##df^{*}:TN^{*}→TM^{*}## maps ##TN^{*}## back in the opposite direction to ##TM^{*}##. The direction of ##df## is called "covariant" while the direction of ##df^{*}## is called "contravariant".

In the language of what is sometimes called "abstract nonsense" the differential is a covariant functor from the category of smooth manifolds and smooth maps to the category of smooth vector bundles and smooth vector bundle morphisms while the dual of the differential defines a contravariant functor to the category of smooth vector bundles and smooth vector bundle morphisms. This is the origin of the terms "push forward" and "pullback".

Notes:
-The coordinates of a vector with respect to a basis are dual vectors when they are viewed as linear functionals that assign a coordinate to each vector. Similarly, the coordinates of dual vectors are dual dual vectors and under the canonical isomorphism are identified with vectors.
 
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  • #33
lavinia said:
A natural transformation would seem always to preserve the direction of transformation. @fresh_42 is this correct?
If I read nLab correctly, and there is no better online source I am aware of when it comes to homological algebra then there is no distinction between covariant or contravariant functors in the definition of a natural transformation between categories, i.e. it is valid in both cases.

Assume we would have two different functors ##\tau,\dagger \, : \,\text{Vec}\longrightarrow \text{Vec}^*.## A transformation ##\alpha \, : \, \tau \longmapsto \dagger ## is natural if it is compatible with the morphisms: Say ##\varphi : V^\tau \longrightarrow W^\tau ## and ##\psi : V^\dagger \longrightarrow W^\dagger ## then we demand that
$$
\alpha (W)\circ \varphi^\tau = (V^\tau\stackrel{\varphi^\tau}{\longrightarrow }W^\tau \stackrel{\alpha }{\longrightarrow } W^\dagger) =(V^\tau\stackrel{\alpha }{\longrightarrow }V^\dagger \stackrel{\psi^\dagger}{\longrightarrow }W^\dagger)= \psi^\dagger \circ \alpha (V)
$$
Hence being natural says something about the mapping ##\tau \longmapsto \dagger## rather than the direction of ##\varphi ## or ##\psi.## I think that makes sense as we are interested how ##V^*\cong V^\tau ## and ##V^*\cong V^\dagger## are related, and not how morphisms in either category are defined. If I'm not mistaken, then ##\varphi,\psi \, : \,W\longrightarrow V## is not ruled out.

There is another interesting note on that page:
A transformation which is natural only relative to isomorphisms may be called a canonical transformation.

At least this explains the difficulty to distinguish the terms with the example ##\text{Vec}## and ##\text{Vec}^*.##
 
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  • #34
fresh_42 said:
If I read nLab correctly, and there is no better online source I am aware of when it comes to homological algebra then there is no distinction between covariant or contravariant functors in the definition of a natural transformation between categories, i.e. it is valid in both cases.

Assume we would have two different functors ##\tau,\dagger \, : \,\text{Vec}\longrightarrow \text{Vec}^*.## A transformation ##\alpha \, : \, \tau \longmapsto \dagger ## is natural if it is compatible with the morphisms: Say ##\varphi : V^\tau \longrightarrow W^\tau ## and ##\psi : V^\dagger \longrightarrow W^\dagger ## then we demand that
$$
\alpha (W)\circ \varphi^\tau = (V^\tau\stackrel{\varphi^\tau}{\longrightarrow }W^\tau \stackrel{\alpha }{\longrightarrow } W^\dagger) =(V^\tau\stackrel{\alpha }{\longrightarrow }V^\dagger \stackrel{\psi^\dagger}{\longrightarrow }W^\dagger)= \psi^\dagger \circ \alpha (V)
$$
Right. What I meant to say more clearly was there is no idea of a natural transformation between a covariant functor and a contravariant functor.

The thinking was whether one could choose isomorphisms ##J_{V}## between each vector space ##V## an its dual so that for every linear map ##L:V→W##, ##L^{*} \circ J_{W} \circ L =J_{V}##. This cannot be done by choosing a basis for each vector space.

This seems to illustrate a difference between the idea of a natural/canonical isomorphism and a natural transformation.
 
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  • #35
martinbn said:
Why not?
As an example, take a Banach space that is not reflexive but still linearly isomorphic to its second continuous dual space.
 
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  • #36
S.G. Janssens said:
As an example, take a Banach space that is not reflexive but still linearly isomorphic to its second continuous dual space.
How is that in contradiction to what I said!
 
  • #37
martinbn said:
How is that in contradiction to what I said!
Is the above a question?

If yes, then it can be answered by looking up reflexivity and, for example, James' theorem.
 

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