Length contraction and wave length transformation

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SUMMARY

The discussion focuses on the relationship between length contraction and wavelength transformation in the context of special relativity. It establishes that the measured lengths of a rod, moving at speeds U and U' in different inertial frames I and I', can be expressed using the Lorentz factor, leading to the equation L = L'g(V)/(1 + u'V/c²). The participants confirm that this derivation can indeed be applied to the wavelengths of an acoustic wave propagating at speeds U and U' in their respective frames. The distinction between the rest frame of the rod and the rest frame of the medium is also emphasized.

PREREQUISITES
  • Understanding of Lorentz transformations and the Lorentz factor
  • Familiarity with the concept of proper length in special relativity
  • Knowledge of wave propagation in different media
  • Basic principles of acoustic waves and their relationship to mechanical waves
NEXT STEPS
  • Study the derivation of the Lorentz transformations in detail
  • Explore the concept of proper length and its implications in relativistic physics
  • Investigate the relationship between wave speed and wavelength in different inertial frames
  • Learn about the effects of relativistic speeds on acoustic waves and their properties
USEFUL FOR

This discussion is beneficial for physicists, students of relativity, and anyone interested in the interplay between special relativity and wave mechanics, particularly in understanding how motion affects measurements of length and wavelength.

bernhard.rothenstein
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consider a rod of proper length Lo located along the overlapped OX(O'X') axes of the I and I' inertial reference frames in the standard arrangement I' moving relative to I' with speed V. The rod moves with speed U relative to I and with speed U' relative to I'. The measured length of the rod is
L=g(U)Lo (1)
L'=g(U')Lo (2)
in I and in I' respectively. Eliminating Lo between (1) and (2) we obtain
L=L'g(U)/g(U'). (3)
Expressing the right side of (3) as a function of U' only, via the addition law of relativistic velocities we obtain
L=L'g(V)/1+u'V/cc (4)
an equation that relates two non-proper lengths.
Is it correct to consider that the derivation presented above represents a derivtion for the relationship betwee the wavelengths of the same acoustic (mechanical) wave that propagates with speeds U and U' relative to I and I' respectively?
Did you find that derivation somewhere in the literature of the subject?
Thanks.
sine ira et studio
 
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bernhard.rothenstein said:
Is it correct to consider that the derivation presented above represents a derivtion for the relationship betwee the wavelengths of the same acoustic (mechanical) wave that propagates with speeds U and U' relative to I and I' respectively?
Yes. You could consider a rod whose length is one wavelength in the frame where the acoustic medium is at rest and whose velocity is equal to the speed of sound in that frame. Such a rod will have a worldline such that the front of the rod follows the crest of one wave and the rear of the rod follows the crest of another. Thus its length in any given frame corresponds to one wavelength in that frame.

Note, that the rest frame of the rod is not the same as the rest frame of the medium.
 

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