Standing waves - Wave Equation

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SUMMARY

The discussion focuses on the derivation of equation 4.4.4 in the context of standing waves and the wave equation 4.3.4. The necessity of negative signs in the wave equation is explained, emphasizing that the reflected wave travels in the opposite direction to the incident wave, requiring a sign flip in either the kx or ωt term. The choice to reverse the sign of kx to -kx is justified, while the phase term's sign is deemed arbitrary. The boundary conditions, particularly for fixed ends, influence the phase change ∅, which is crucial for accurate wave representation.

PREREQUISITES
  • Understanding of wave equations, specifically the basic wave equation 4.3.4
  • Familiarity with wave propagation concepts, including incident and reflected waves
  • Knowledge of boundary conditions in wave mechanics
  • Basic trigonometric functions and their application in wave equations
NEXT STEPS
  • Study the derivation of the wave equation 4.3.4 in detail
  • Explore the implications of boundary conditions on standing waves
  • Learn about phase shifts in wave mechanics and their physical significance
  • Investigate the mathematical representation of standing waves and their properties
USEFUL FOR

Students and educators in physics, particularly those focusing on wave mechanics, as well as anyone seeking to deepen their understanding of standing waves and wave equations.

elemis
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I don't completely understand how equation 4.4.4 was derived and determined. I understand the derivation behind the basic wave equation 4.3.4 but not what happened in 4.4.4. Why is there a need for all the negative signs ? Would a simple phase change suffice ?

Please do be a bit detailed in your explanation... Pretend I'm an idiot. Thank you !

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Since the reflected wave travels in the opposite direction as the incident wave, you need to flip the sign on either the kx or the ωt term***. The author chose to reverse the sign of kx to make it -kx. There was already a - sign with -ωt. For the phase term, the choice of sign is arbitrary.

Just changing the phase would express a wave traveling in the same direction as the incident wave, but shifted in phase.

Hope that helps.

EDIT added:
*** This is because a rightward-traveling wave has the form f(kx-ωt) or f(-kx+ωt). A leftward-traveling wave has the form f(kx+ωt) or f(-kx-ωt).
 
Last edited:
So I could equally have written kx+wt ? Why is there a need for the phase change ∅ ?
 
elemis said:
So I could equally have written kx+wt ?
Yes; see the edit added to my earlier post.
Why is there a need for the phase change ∅ ?
As the book says, the type of boundary will determine ∅. Usually the boundary is either fixed or has a maximum amplitude. Also, the location of the boundary plays a role in what ∅ is.

Eg., for a fixed end located at x=x0:

\cos(kx_0 + \phi /2) = 0

You'd solve that for ∅, given k and x0. Your book is taking the fixed end to be at x=0, so that simplifies things somewhat.
 

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