Understanding Waves Dispersion: A, B, & C

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SUMMARY

This discussion focuses on the complexities of wave dispersion, specifically addressing three key areas: A) the transverse displacement of a string, B) the dispersion relation in a system, and C) the dependence of wave number on frequency in a beaded string. The equations presented include phi=cos(w1t)+cos(w2t) for transverse displacement and v(sub phi)=c(1+ak^2)^(1/2) for phase velocity. The group velocity is defined as v_g = dω/dk, and the relationship between wave number and frequency is explored through w=w(sub c)cosh(1/2ka).

PREREQUISITES
  • Understanding of wave mechanics and dispersion relations
  • Familiarity with angular frequency and wave number concepts
  • Knowledge of mathematical functions such as cosine and hyperbolic functions
  • Basic principles of superposition in wave theory
NEXT STEPS
  • Study the derivation of the group velocity formula v_g = dω/dk
  • Explore the implications of the dispersion relation w=ak^r in different physical systems
  • Investigate the effects of transverse displacement in wave mechanics using simulations
  • Learn about the mathematical properties of superposition in wave interference
USEFUL FOR

Students preparing for exams in physics, educators teaching wave mechanics, and researchers interested in wave dispersion phenomena.

belleamie
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Hi I'm studying for a test, and in the suggested reading book review has a few equations that they talk about but I'm not don't really understand how it jumps from one thing to another? the book is very vauge... I've broken the parts i don't understand into A,B,C (I used w = omega)

A)IT shows a graph, explain that the end of a string is given a transverse displacement phi=cosw1t+cosw2t where the two frequencies are almost equal and w1>w2 the resultant motion is a traveling wave of angular frequency (w1+w2)/2, modulated by n envelope which is a traveling wave of (w1-w2)/2 There the speed of this envelop is (w1-w2)/(k1-k2) ...? I don't understand how they got that?

B) A system with dipersion relation w=ak^r...a and r are constants because v(sub g)=xv(sub phi) at all wave frequencies. i duno where then got the other variables v(sub g)? i know that v(sub phi) =c(1+ak^2)^1/2 but i don't understand how they relate?

C) a beaded string above cut off, the dependence of k on frequency is given by w=w(sub c) cosh1/2ka showing a graph, How does k depend on the frequency? i know a beaded string can exhibit high freq cut off and that the part od the system vibrates in anti phase with each other...and k=(pi/a)-ik where k can be found as a function by replacing k=pi/a in w/w(sub c)= sin (1/2 Ka-i1/2ka) but I'm not sure how?
 
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These problems are about group velocity [tex]v_g = {\rm d}\omega/{\rm d}k[/tex]. You need to write the superposition as a product of average and beat frequency, using those relations there are for sin a + sin b.

Here is some help, with a nice simulation:
http://webphysics.davidson.edu/faculty/dmb/bernstein/qmwave/section2b.html
 
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