Arbitrary travelling wave on string (griffiths 9.5)

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SUMMARY

The discussion focuses on solving a problem from Griffiths 9.5 regarding a traveling wave of arbitrary shape on a string composed of two segments with different mass densities. Key to the solution are the continuity conditions imposed on the wave and its derivatives at the boundary (z=0). The consensus is that these conditions are sufficient to determine the transmitted and reflected waves, regardless of whether the incoming wave is decomposed using Fourier series. Reflection occurs due to changes in the medium, exemplified by transitions between different strings.

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  • Understanding of wave mechanics and boundary conditions
  • Familiarity with the concept of mass density in strings
  • Knowledge of Fourier series for wave decomposition
  • Basic principles of reflection and transmission of waves
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  • Study the application of continuity conditions in wave mechanics
  • Learn about Fourier series and their role in wave analysis
  • Explore the principles of wave reflection and transmission across different media
  • Review examples of traveling waves in strings with varying mass densities
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DE7
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hi all,

i'm in need of a little help with griffiths 9.5 (EM). the problem concerns a traveling wave of arbitrary shape on a string. the string consists of two strings with different mass densities tied together at z=0. given the arbitrary incoming wave, what are the transmitted and reflected waves?

i know i must impose continuity conditions on the wave and its derivatives at z=0. however, are these two equations enough to determine the problem? or should i decompose the incoming wave using Fourier series? I'm not too sure how to go about doing that...any hints?
 
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The problem of wave reflection and transmission is derived simply from the principle of continuity, so yes they are enough. Whether you decompose the wave or not into its fundamental harmonics is irrelevant to the reflected and transmitted wave magnitudes, which is usually the parameter of interest.

Reflection occurs when there is a change in propagating medium, such as air to glass, or string1 to string 2 for mechanical waves.
 

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