What is the definition of general covariance ?

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SUMMARY

The definition of "general covariance" asserts that the laws of nature must be expressible as equations that hold true across all coordinate systems. It is established that while tensors are necessary for a theory to be generally covariant, they are not sufficient on their own. The theory must also avoid any "prior geometry" that is independent of matter sources. Key references include Einstein's principles and insights from "Gravitation and Spacetime" by Ohanian and Ruffini, which clarify the distinction between covariance and invariance in physical laws.

PREREQUISITES
  • Understanding of tensor calculus
  • Familiarity with covariant derivatives
  • Knowledge of general relativity principles
  • Awareness of coordinate transformations in physics
NEXT STEPS
  • Study the implications of Einstein's principles on general covariance
  • Explore the role of covariant derivatives in physical theories
  • Investigate the differences between covariance and invariance in equations
  • Read "Gravitation and Spacetime" by Ohanian and Ruffini for deeper insights
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Physicists, mathematicians, and students of general relativity seeking to understand the foundational principles of general covariance and its implications in theoretical physics.

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What is the definition of "general covariance"?

What is the definition of "general covariance"?

Is it sufficient for a theory to be written only in terms of tensors for it to be generally covariant? Is it necessary for a theory to be able to be written solely in terms of tensors for it to qualify as generally covariant?
 
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From Einstein: "The general laws of nature are to be expressed by equations which hold good for all systems of co-ordinates, that is, are co-variant with respect to any substitutions whatever (generally co-variant)"

So the definition would appear to be: "laws of nature are generally covariant if the corresponding equations hold good for all systems of co-ordinates".

Your questions:

1) Is it sufficient for a theory to be written only in terms of tensors for it to be generally covariant?

Don't know if this helps but: Can you think of a theory which can be written only in terms of tensors which does not hold good for all systems of coordinates? If not then the answer to your first question is yes, otherwise no.

2) Is it necessary for a theory to be able to be written solely in terms of tensors for it to qualify as generally covariant?

Can you think of a theory which can be written without the use of tensors and nonetheless holds in all systems of coordinates?

Maybe this from Dirac will be useful in answering your question: "Even if one is working with flat space (which means neglecting the gravitational field) and one is using curvilinear coordinates, one must write one's equations in terms of covariant derivatives if one wants them to hold in all systems of coordinates".

So covariant differentiation appears to be a necessary requirement and, as far as I know, you can't have covariant differentiation without introducing tensors.

Dirac elsewhere writes: "The laws of Physics must be valid in all systems of coordinates. They must thus be expressible as tensor equations."

So tensors appear to be a necessary, but perhaps not sufficient, condition for a generally covariant theory.

I hope that was somewhat helpful.
 
pervect said:
What is the definition of "general covariance"?

Is it sufficient for a theory to be written only in terms of tensors for it to be generally covariant?

No, the theory cannot have any "prior geometry" either; i.e., a theory that has absolute
geometric elements independent of matter sources does not qualify as general covariant.
See MTW §17.6.
 
pervect said:
What is the definition of "general covariance"?

Is it sufficient for a theory to be written only in terms of tensors for it to be generally covariant? Is it necessary for a theory to be able to be written solely in terms of tensors for it to qualify as generally covariant?

From Gravitation and Spacetime by Ohanian and Ruffini. page 371 - footnote, which I'm sure you'd agree with it already, but for others
* We have "covariant" vectors, "covariant" derivatives and now "covariant" equations. The word "covariant" is unfortunately much overworked, and which the meaning of the three meanings is intended must be guessed from context.

On general covariance for equations. From page 373
Principle of general covariance: All laws of physics shall bve stated as equations which are covariant with respect to general coordinate transformations.
...
Invariance goes beyond covariance in that it demands that not only the form, but also the content of the equations be left unchanged by the coordinate transformation. Roughly, invariance is achieved by imposing the extra condition that all "constants" in the equation remain exactly the same.

I hope that was of so use pervect.

Best regards

Pete
 
pmb_phy said:
From Gravitation and Spacetime by Ohanian and Ruffini. page 371 - footnote, which I'm sure you'd agree with it already, but for others


On general covariance for equations. From page 373


I hope that was of so use pervect.

Best regards

Pete

Yes, that is helpful, thank you.
 
pervect said:
Yes, that is helpful, thank you.
You're welcome. :smile:

Pete
 

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