Lorentz Transformation: Proving θμ Covariant Vector

In summary, the conversation discusses the transformation of the derivative θμ from a covariant vector to a contravariant vector. It is suggested to try a similar proof to the covariant case shown in an attached image. The speaker also asks for help if they get stuck and to show their work.
  • #1
helpcometk
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Homework Statement



Given that the derivative θμ transforms as a covariant vector ,show that θμ transforms as a contravariant vector.

Homework Equations



Please look the attachement

The Attempt at a Solution


Does anyone know how i should go to prove it ?Is it just a trivial substitution ?
 

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  • #2
helpcometk said:

Homework Statement



Given that the derivative θμ transforms as a covariant vector ,show that θμ transforms as a contravariant vector.

Homework Equations



Please look the attachement

The Attempt at a Solution


Does anyone know how i should go to prove it ?Is it just a trivial substitution ?

What are θμ & θμ supposed to mean exactly? Uf the problem is just to show that [itex]\frac{\partial}{\partial x_\mu}[/itex] transforms as a contravariant vector, just try an analogous proof to the covariant case in your image. If you get stuck, show your work.
 

FAQ: Lorentz Transformation: Proving θμ Covariant Vector

What is the Lorentz Transformation?

The Lorentz Transformation is a set of equations developed by Hendrik Lorentz in the late 19th century to describe the relationship between space and time in special relativity. It is used to transform coordinates and measure physical quantities in one frame of reference to another moving at a constant velocity.

What is a covariant vector?

A covariant vector is a mathematical object that transforms in a specific way under a coordinate transformation. In the context of special relativity, it is a vector that transforms according to the Lorentz Transformation, maintaining its direction and magnitude in different frames of reference.

How is θμ related to Lorentz Transformation?

In special relativity, the θμ vector represents the position of an event in spacetime. The Lorentz Transformation can be used to calculate the coordinates of the same event in a different frame of reference. Proving that θμ is a covariant vector means that it transforms consistently with the Lorentz Transformation.

How is θμ transformed under the Lorentz Transformation?

The Lorentz Transformation can be expressed as a matrix equation, where the θμ vector is multiplied by a matrix representing the transformation. The elements of this matrix are determined by the relative velocity between the two frames of reference. The resulting θμ vector after transformation will have different numerical values, but its direction and magnitude will remain unchanged.

Why is proving θμ a covariant vector important?

Proving that θμ is a covariant vector is important because it provides a mathematical basis for the principles of special relativity. It demonstrates that physical laws and measurements are consistent in different frames of reference and are not dependent on the observer's perspective. This is a fundamental concept in modern physics and has implications for various areas of research, such as high-speed particle physics and cosmology.

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