![]() However, according to my initial arguments, how can frequency of the wave change if there is no change in $\omega$?ġ.In the case where the observer is moving, is it true that the apparent wavelength does not change from the case where both source and observer are stationary? And in the case where the source is moving, is it true that both wavelength and frequency are changing from the normal case? And if so, why is it that the relative motion is not what matters?Ģ.In the case where the source is moving, how can frequency change when $\omega$ remains constant?Įdit: Clarified that I am talking about longitudinal waves propagating in a stationary medium. This must mean that there is an inherent change in the wavelength and frequency of the wave, visible to any stationary observer. Examine how frequency compression and the observers motion combine to influence the. However, in the case where the source is moving with respect to the observer, which is stationary, (scene 7 of 8) the state of motion of the observer is the same as in the case where both the observer and the source are stationary(scene 3 of 8). The Doppler shift is a phenomenon that occurs when sound waves are moving towards or away from the observer. Now, as can be seen from the Appendix, by taking as the variations of p and q the. However, this animation (scenes 4 and 5 of 8) helped me realise(?) that, in the case of the observer moving and the source remaining stationary, the wave itself does not change, but the apparent frequency of the wave as seen by the observer changes.Īlso, as there is relative velocity between the source and the wave I thought that the apparent change in frequency would be due to the apparent change in velocity and wavelength $(v=\nu*\lambda)$ which means that $\lambda$ would be constant. We summarize the Extended Doppler shift formulas for the simplest cases of the non-uniformly moving observer, source/observer, and Mirror/reflector variations. Parametric representation of ray path for calculation of Doppler shift. My initial doubt was how the frequency and the time period of the wave could change if $\omega$ did not change. ![]() Now the Doppler effect shows us that if the source of the wave or the observer is in motion the frequency$(\nu)$ of the wave changes(Here I am talking about longitudinal waves propagating in a stationary medium). ![]() Also, velocity of propagation of a wave $v = \nu*\lambda$. The time period ($T$) of the (harmonic) wave is then $2*\pi/\omega$. For a transverse wave(or for pressure waves required to produce longitudinal waves), the motion perpendicular to the direction of propagation of the wave is governed by an equation like $y = Asin(\omega t)$ in case of harmonic waves(here $\omega$ is angular frequency of simple harmonic motion). ![]()
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