Composition of Lorentz Transformations

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Discussion Overview

The discussion revolves around the composition of Lorentz transformations in the context of relating velocities between multiple inertial frames. Participants explore the mathematical foundations and conceptual understanding of how these transformations are applied and combined, particularly in relation to velocity composition in special relativity.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Conceptual clarification

Main Points Raised

  • One participant expresses confusion about why multiplying the Lorentz transformations of two frames leads to the transformation for a third frame, questioning the derivation of this process.
  • Another participant draws an analogy between Lorentz transformations and rotations in three-dimensional space, suggesting that they can be understood as analogous operations in four-dimensional spacetime.
  • A different participant emphasizes that Lorentz transformations are linear transformations and can be treated similarly to other linear transformations in linear algebra, specifically through matrix multiplication.
  • One participant explains the process of applying successive transformations, detailing how the output of one transformation becomes the input for the next.
  • Another participant references the use of rapidities in spacetime to motivate the velocity composition, mentioning hyperbolic trigonometric identities as a means to understand the relationships between velocities without directly using transformations.
  • A participant reiterates their initial question about composing arbitrary transforms, suggesting that the same principles apply to Lorentz transformations and encouraging others to work through the details for this specific case.

Areas of Agreement / Disagreement

Participants express varying levels of understanding and intuition regarding the composition of Lorentz transformations. There is no consensus on a single method or explanation that resolves the initial confusion, indicating that multiple perspectives and approaches remain in play.

Contextual Notes

Some participants mention the use of rapidities and hyperbolic identities, suggesting that the discussion may depend on specific mathematical frameworks or definitions that are not fully explored within the thread.

Hacky
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It is not intuitive, for me at least, why when relating the velocity of 3 inertial frames (Say F1, F2 moving at v1 with respect to F1, and F3 moving at v2 with respect to F2), one mulitplies the transforms of F2 and F3 to get the transform for F1 with respect to F3 to get v3. I understand why v3 does not equal v1+v2 and have seen some very understandable derivations of the velocity composition formula. But I have not been able to find the derivation of how mupltiplying two transforms leads to the third (and thus leads to v3).

Thanks, Howard
 
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Remember that you can make rotations in 3D multiplying diferent matrix, each one corresponding to a rotation along any selected axis, this is totally analogous, since lorentz transformations corresponds to rotations in four dimensions, with the lorentz metric.
 
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Remember that a Lorentz transformation is just a linear transformation, like the ones you encounter in linear algebra. And the Lorentz transformation, like all linear transformations, has a matrix. You perform successive Lorentz transformations the same way you perform any successive linear transformations: By multiplying their matrices together.
 
Applying the transform once transforms all your vectors to the new co-ordinate system. So:

[tex]\vec{v'} = T_1\vec{v}.[/tex]

The next transform will now transform our new vectors, so:

[tex]\vec{v''} = T_2\vec{v'} = T_2 T_1 \vec{v}.[/tex]

I hope that explains it.
 
The strategy is essentially laid out here [using rapidities in 1+1 spacetime]
https://www.physicsforums.com/showpost.php?p=961838&postcount=13
...but you have to finish it off recognizing that the relative spatial velocity is c*tanh(theta_2-theta_1)... then use the hyperbolic trig identity. If you wish to avoid rapidities, you can use betas and gammas and various identities among them... but they are really hyperbolic trig identities.

The quickest way to motivate the velocity-composition [without explicitly using the transformations] uses the k-calculus.

For non-parallel velocity composition, you'll have to work with a larger more general version of the LT matrices (or else work with infinitesimals, or else do trig on a hyperbolic space).
 
Hacky said:
It is not intuitive, for me at least, why when relating the velocity of 3 inertial frames (Say F1, F2 moving at v1 with respect to F1, and F3 moving at v2 with respect to F2), one mulitplies the transforms of F2 and F3 to get the transform for F1 with respect to F3 to get v3. I understand why v3 does not equal v1+v2 and have seen some very understandable derivations of the velocity composition formula. But I have not been able to find the derivation of how mupltiplying two transforms leads to the third (and thus leads to v3).

Thanks, Howard

Do you understand how, in general, to compose arbitrary transforms?

Say transform T1 maps x->x', and transform T2 maps x'->x'', where x is a vector.

We can say x' = T1(x), and x''=T2(x').

The "composed" transform is a map from x->x''

x'' = T2(T1(x))

All you need to do for the specific case of the Lorentz transforms is work out the details.
 

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