Finding the Group Velocity for Shallow Water Wave

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SUMMARY

The group velocity for a shallow water wave is determined using the formula ##v_g = \frac{\frac{\gamma\pi}{\rho \lambda^2}}{v_p \lambda}##, where ##v_p = \sqrt{\frac{2\pi\gamma}{\rho\lambda}}## represents the phase velocity. The correct answer is established as ##\frac{3}{2}v_p## after simplifying the expressions and ensuring the correct differentiation of ##\omega## with respect to ##k##. The discussion highlights the importance of correctly applying the chain rule in calculus to derive the group velocity accurately.

PREREQUISITES
  • Understanding of wave mechanics and shallow water wave theory
  • Familiarity with calculus, specifically differentiation techniques
  • Knowledge of phase and group velocity concepts
  • Basic understanding of the physical parameters involved: density (##\rho##), surface tension (##\gamma##), and wavelength (##\lambda##)
NEXT STEPS
  • Study the derivation of group velocity in different wave contexts, such as sound waves and electromagnetic waves
  • Learn about the implications of group velocity in wave propagation and energy transport
  • Explore advanced calculus techniques for differentiating complex functions
  • Investigate the relationship between phase velocity and group velocity in various media
USEFUL FOR

Students and professionals in physics, particularly those focusing on fluid dynamics, wave mechanics, and applied mathematics. This discussion is beneficial for anyone looking to deepen their understanding of wave behavior in shallow water contexts.

James Brady
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Homework Statement


Find the group velocity for a shallow water wave: ##\nu = \sqrt{\frac{2\pi\gamma}{\rho\lambda^3}}##

Homework Equations


Phase velocity: ##v_p = \nu\lambda##
group velocity: ##v_g = \frac{d\omega}{dk}##

##k=\frac{2\pi}{\lambda}##
##\omega = 2\pi \nu##

The Attempt at a Solution


Get frequency in terms of wave number:

##\nu(k)=\sqrt{\frac{\gamma k}{\rho\lambda^2}}##
##\omega(k) = 2\pi\sqrt{\frac{\gamma k}{\rho\lambda^2}}##

##\frac{d\omega}{dk}=2\pi(\frac{1}{2}(\frac{\gamma k}{\rho \lambda^2})^{-1/2} \frac{\gamma}{\rho \lambda^2})##

We can rewrite the function, getting rid of k. Also did some canceling and moved the pi:##v_g=(\frac{\gamma 2\pi}{\rho \lambda^3})^{-1/2} \frac{\gamma\pi}{\rho \lambda^2}## ##v_g = \frac{\frac{\gamma\pi}{\rho \lambda^2}}{(\frac{\gamma 2\pi}{\rho \lambda^3})^{1/2}}##

Note that given the definition for phase velocity, we can write it as:

##v_p = \sqrt{\frac{2\pi\gamma}{\rho\lambda}}##

##v_g = \frac{\frac{\gamma\pi}{\rho \lambda^2}}{v_p \lambda} = \frac{\frac{\gamma\pi}{\rho \lambda^3}}{v_p}##

So this is where I'm stuck... The correct answer from the book is ##\frac{3}{2}v_p##
 
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James Brady said:
Get frequency in terms of wave number:

##\nu(k)=\sqrt{\frac{\gamma k}{\rho\lambda^2}}##
Try expressing ##\nu(k)## completely in terms of ##k##, rather than a mixture of ##\lambda## and ##k##.
 
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##\frac{d\nu}{dk}=\frac{1}{2}(\frac{\gamma k^3}{4 \pi^2 \rho})^{-1/2}\frac{3k^2\gamma}{4\pi^2\rho}##

So I see we have that nice 3/2 term in there, but if my phase velocity term is correct, ##v_p = \nu\lambda = \sqrt{\frac{2\pi \gamma}{\rho \lambda}} = \sqrt{\frac{\gamma k}{\rho}}##, then every thing other than the 3/2 coefficient must reduce to this...

So maybe this is just some algebra problem right now...?

##\frac{\frac{\gamma k^2}{4\pi^2 \rho}}{\frac{\gamma k^3}{4 \pi^2 \rho}^{1/2}} = \sqrt{\frac{\gamma k}{\rho}}##

Was writing out this question when I figured out that this does reduce to 3/2v_p. Just as long as we do ##\frac{d \omega}{dk}## (include the 2pi), instead of ##\frac{d \nu}{dk}##

I figured I'd post my thoughts anyway. Thanks for tip @TSny.
 

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