Components and basis transform differently

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Discussion Overview

The discussion centers on the transformation properties of components and basis vectors under Lorentz and orthogonal transformations. Participants explore the differences in how these entities transform, particularly in the context of geometry and relativity.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • One participant questions why components and basis vectors transform differently under Lorentz transformations, suggesting that basis vectors undergo an inverse transformation compared to components.
  • Another participant raises a question about whether the discussion pertains to group theoretical approaches or differential geometry, indicating a potential mix-up in concepts.
  • A different viewpoint expresses surprise at the idea of transforming basis vectors, suggesting a preference for conserving absolute values instead.
  • One participant asserts that the mathematical treatment of transformations is correct, criticizing physicists for focusing primarily on component behavior in noninertial frames while neglecting basis transformation laws.
  • It is noted that components and basis vectors only transform similarly in specific cases, particularly in orthonormal coordinates, and that generally, all coordinates transform differently than basis vectors.
  • A participant illustrates the transformation difference by discussing the effect of doubling the length of a basis vector, explaining that this leads to an inverse change in the coordinate value.
  • The claim is made that this transformation behavior is not unique to Lorentz transformations, as all coordinates typically transform differently than basis vectors, with orthonormal systems being a notable exception.

Areas of Agreement / Disagreement

Participants express differing views on the nature of transformations for components and basis vectors, with no consensus reached on the implications or correctness of these transformations.

Contextual Notes

The discussion involves complex concepts from geometry and relativity, with potential ambiguities regarding definitions and the context of transformations. Specific assumptions about coordinate systems and their properties are not fully explored.

Ratzinger
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Why do components and basis vectors transform under Lorentz transformation differently (inverse Lorentz for basis), whereas for orthogonal transformation components and basis are transformed by same matrix?

Thank you
 
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Are u talking about the group theoretical approach to relativity,or differential geometry ?I think you're mixing them.Components & basis vectors would imply geometry,while Lorentz transformation & orthogonal transformation would imply [itex]\mbox{O(3)/SO(3)}[/itex] or [itex]SO(3,1)[/itex]...?

So which one would u prefer?

Daniel.
 
Ratzinger said:
Why do components and basis vectors transform under Lorentz transformation differently (inverse Lorentz for basis), whereas for orthogonal transformation components and basis are transformed by same matrix?

Thank you
I´m quite surprised that you want follow the dictatorship of relativism by tranforming even the basis. I expected you to rather conserve absolute values.
o:)
 
Well,that's the correct way to do it.Mathematcally.Physicists are rather sloppy,here,i must say,because are usually interested in how the commponents of (pseudo)tensors behave when a change of noninertial reference frames is done...They have no use for the transformation laws of the basis (co)vectors.

Daniel.
 
Ratzinger said:
Why do components and basis vectors transform under Lorentz transformation differently (inverse Lorentz for basis), whereas for orthogonal transformation components and basis are transformed by same matrix?

Thank you

The basis and the components ony transform in the same manner for a very special set of coordinates - orthonormal coordinates to be precise.

Probably the very simplest way to see why coordinates and vectors transform differently is to look at what happens when you double the length of the basis vector. It should be easy to see that if you double the basis vector, you halve the coordinate value, and vica-versa. That is why coordinates and basis vectors transform differently (oppositely).

Note that when you double one of the basis vectors, you are no longer in an orthonormal basis (you are orthogonal, but not normal).

So there is nothing special about the Lorentz transform - in general ALL coordinates transform differently than basis vectors. (Orthonormal coordinate systems are the exception - of course, they are a very common and important exception).
 

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