Definition of Form-Invariant Function: Q&A

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Discussion Overview

The discussion revolves around the definition of a 'form-invariant function' as presented in Weinberg's 'Gravitation and Cosmology'. Participants explore the implications of the definition in the context of metric transformations and coordinate systems.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant questions whether the condition for form-invariance implies that the transformed metric ##g_{\mu\nu}^\prime## is simply the same function as ##g_{\mu\nu}##.
  • Another participant asserts that the definition indeed means that the metrics are the same function, noting the use of the symbol "y" to avoid confusion with coordinates.
  • A different participant argues that the condition ##g'_{\mu\nu}(x')=g_{\mu\nu}(x)## would imply the functions are different due to the different values assigned by the coordinate transformations, contrasting it with the condition ##g'_{\mu\nu}(y)=g_{\mu\nu}(y)## which suggests they yield equal results for the same numerical inputs.
  • One participant acknowledges the clarification regarding the distinction between points in different coordinate systems.

Areas of Agreement / Disagreement

Participants express differing interpretations of the definition of form-invariance, with some agreeing that the metrics are the same function while others argue that the conditions imply they are different functions. The discussion remains unresolved regarding the implications of the definitions.

Contextual Notes

The discussion highlights the potential confusion arising from the notation and the implications of coordinate transformations on the definition of form-invariance. There are unresolved nuances regarding the interpretation of the metrics and their relationships under transformation.

Einj
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Hello everyone. I'm reading Weinberg's 'Gravitation and Cosmology' and I'm having some problems understanding the definition of a 'form-invariat function'. He says:
A metric ##g_{\mu\nu}## is said to be form-invariant under a given coordinate transformation ##x\to x^\prime##, when the transformed metric ##g^\prime_{\mu\nu}(x^\prime)## is the same function of its argument ##x^{\prime\mu}## as the original metric ##g_{\mu\nu}(x)## was of its argument ##x^\mu##, that is,
\begin{equation}
g^\prime_{\mu\nu}(y)=g_{\mu\nu}(y) \; \text{ for all }y.
\end{equation}
If the previous condition was true doesn't this simply mean that ##g_{\mu\nu}^\prime## is the same function as ##g_{\mu\nu}##? Should we ask for:
\begin{equation}
g^\prime_{\mu\nu}(x^\prime)=g_{\mu\nu}(x)
\end{equation}
?

Thanks a lot!
 
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Einj said:
If the previous condition was true doesn't this simply mean that ##g_{\mu\nu}^\prime## is the same function as ##g_{\mu\nu}##?

That is precisely what he means, that they are the same function.
I think that's why he used the symbol "y" instead of x's, so that it wouldn't be confused as having something to do with the coordinates x and x'.
 
Last edited:
The problem with g'_{\mu\nu}(x')=g_{\mu\nu}(x) is that it means the two functions have same value in a single point. But because x' associates different numbers to that point compared to x, g'_{\mu\nu}(x')=g_{\mu\nu}(x) necessarily means g and g' are different functions and don't have the same form.
But g'_{\mu\nu}(y)=g_{\mu\nu}(y) means that if we give the two functions, the same numbers, they will give equal results which means they're the same function. Note that y in the right refers to a different point than y in the left because they are same numbers in different coordinate systems.
 
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Shyan said:
Note that y in the right refers to a different point than y in the left because they are same numbers in different coordinate systems.
Oh I see. That is clear. Thanks!
 

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