SR & Lorentz Scalar Fields: Covariant Diff. & Wave Amplitude

In summary, the conversation discusses the use of covariant differentiation in GR and SR, with a focus on non-Cartesian coordinate systems. It is noted that some texts use this as an introduction to Christoffel symbols. The conversation also brings up the question of how wave amplitudes are treated as Lorentz scalar fields and why they are not Lorentz contracted.
  • #1
dyn
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Hi. In GR , covariant differentiation is used because the basis vectors are not constant. But , what about in SR ? If the basis vectors are not Cartesian then they are not constant. Does covariant differentiation exist in SR ? And are for example spherical polar basis vectors which are not constant treated differently to Cartesian basis vectors in SR ?

Another question I have is regarding Lorentz Scalar Fields. I have read that a wave can be treated as a Lorentz scalar field which means that its amplitude in one frame is the same as measured in any other inertial frame but why is the wave amplitude not Lorentz contracted ?
Thanks
 
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  • #2
dyn said:
But , what about in SR ? If the basis vectors are not Cartesian then they are not constant.
Yes, it is needed with non-Cartesian coordinate systems. Some texts use that as a gentle way to introduce the Christoffel symbols. IIRC, Schutz does that in 'A first course in General Relativity', with a chapter introducing Christoffel symbols et al, mostly focusing on polar coordinate systems, before he introduces curvature in the following chapter.
 
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  • #3
Just to clarify further, this is nothing particular for Minkowski space - it is the case for any set of non-affine coordinates on a regular euclidean space as well.
 
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Likes PWiz
  • #4
Thanks. So if I was working with spherical polars in Minkowski space I would use covariant differentiation as the basis vectors are not constant.
Any thoughts on my problem with wave amplitudes and Lorentz scalar fields ?
 

Related to SR & Lorentz Scalar Fields: Covariant Diff. & Wave Amplitude

1. What is a Lorentz scalar field?

A Lorentz scalar field is a type of field in theoretical physics that is invariant under Lorentz transformations. This means that the value of the field remains the same regardless of the observer's frame of reference. Examples of Lorentz scalar fields include temperature and mass density.

2. What is the significance of a covariant differential in SR?

In special relativity, the covariant differential is used to describe how quantities change between different frames of reference. It takes into account the effects of time dilation and length contraction, allowing for consistent calculations and equations in different frames of reference.

3. How does a Lorentz scalar field differ from a vector field?

A Lorentz scalar field is a field that has one value at every point in space, while a vector field has both a magnitude and direction at each point. Additionally, vector fields are not invariant under Lorentz transformations, while Lorentz scalar fields are.

4. What is wave amplitude in the context of SR and Lorentz scalar fields?

Wave amplitude refers to the maximum displacement of a wave from its equilibrium position. In the context of SR and Lorentz scalar fields, it is used to describe the strength of the field at a given point in space and time. The amplitude of a Lorentz scalar field remains the same in all frames of reference.

5. How are covariant differential and wave amplitude related in SR?

In special relativity, the covariant differential is used to describe the change in a Lorentz scalar field between different frames of reference. This change can also be seen as the wave amplitude of the field, as it is the measure of the field's strength at a specific point in space and time. Therefore, the covariant differential and wave amplitude are closely related in the context of SR and Lorentz scalar fields.

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