Can tensors always commute with each other or are there exceptions?

In summary, the conversation is about tensors and whether the commutation relation g_{ab}g_{cd}=g_{cd}g_{ab} holds for an arbitrary metric tensor g_{\mu \nu}. The person asking the question is wondering if it can be proved using the relations (1) and (2) involving partial derivatives. It is clarified that the commutation relation holds for tensor components, but not necessarily for tensor objects such as matrices.
  • #1
emma83
33
0
Hello,

I am still having a hard time with tensors...
The answer is probably obvious, but is it always the case (for an arbitrary metric tensor [tex]g_{\mu \nu}[/tex] that [tex]g_{ab}g_{cd}=g_{cd}g_{ab}[/tex] ?

I was trying to find a formal proof for that, and was wondering if we could use the relations:
(1) [tex]g_{ab}=\frac{\partial x^{c}}{\partial x^{a}} \frac{\partial x^{d}}{\partial x^{b}} g_{cd}[/tex]
(2) [tex]g_{cd}=\frac{\partial x^{a}}{\partial x^{c}} \frac{\partial x^{b}}{\partial x^{d}} g_{ab}[/tex]

And then multiply the left-hand side of (1) and (2) together and use the fact that the fractions of partial derivatives commute with the metric tensor and cancel each other to get:
[tex]g_{ab}g_{cd}
=(\frac{\partial x^{c}}{\partial x^{a}} \frac{\partial x^{d}}{\partial x^{b}} g_{cd}) (\frac{\partial x^{a}}{\partial x^{c}} \frac{\partial x^{b}}{\partial x^{d}} g_{ab})
= \frac{\partial x^{c}}{\partial x^{a}}\frac{\partial x^{a}}{\partial x^{c}} \frac{\partial x^{d}}{\partial x^{b}} \frac{\partial x^{b}}{\partial x^{d}} g_{cd} g_{ab}
= g_{cd}g_{ab}[/tex]

Does that make sense ?!

Thanks for your help...
 
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  • #2
in

[tex]
g_{ab}g_{cd}=g_{cd}g_{ab}
[/tex]

[itex]g_{ab} [/itex] is just a number, and so is [itex]g_{cd}[/itex], and numbers commute.

for instance, [itex]g_{02} = 0[/itex], [itex]g_{00} = 1 [/itex] (or [itex]g_{00} = -1 [/itex]) depending on which your original definition of metric is)
 
  • #3
Argh! Thanks a lot, again I mixed up "tensors" with "tensor components"...
So the commutation relation I wrote holds for the tensor components of any tensor (not only the metric), doesn't it ?

On the other hand, the tensor (objects) do not necessarily commute with each other, right ?
 
  • #4
no the tensor objects can be non-commuting things like matricies, e.g.

[tex]\sigma ^{\mu \nu} = \frac{i}{2}[\gamma ^\mu, \gamma^\nu][/tex]
where the gamma's are dirac 4x4 matricies
 

1. What is the commutation of metric tensor?

The commutation of metric tensor refers to the property of the metric tensor in general relativity, which states that the order of differentiation of the tensor does not affect the final result. This means that the metric tensor is symmetric, and the order of the indices does not matter when calculating the metric or its derivatives.

2. Why is the commutation of metric tensor important?

The commutation of metric tensor is important because it is a fundamental property of the metric tensor in general relativity. It allows for the simplification of equations and makes calculations easier. It also has implications in the mathematical formulation of Einstein's field equations and the understanding of the curvature of spacetime.

3. How is the commutation of metric tensor related to the curvature of spacetime?

The commutation of metric tensor is related to the curvature of spacetime through the Riemann curvature tensor. The commutation property of the metric tensor allows for the Riemann tensor to be written in terms of the metric tensor and its derivatives, which is essential in describing the curvature of spacetime in general relativity.

4. Can the commutation of metric tensor be violated?

No, the commutation of metric tensor is a mathematical property that cannot be violated. It is a fundamental property of the metric tensor in general relativity and is a direct consequence of the symmetry of the metric tensor.

5. How does the commutation of metric tensor affect the measurement of distances in curved spacetime?

The commutation of metric tensor does not directly affect the measurement of distances in curved spacetime. However, it is a crucial property in the calculation of geodesics, which are the shortest paths between two points in curved spacetime. This, in turn, affects how distances are measured in curved spacetime.

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