Mechanical Waves & Wave Equation

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SUMMARY

The discussion centers on demonstrating that the wave function y(x,t) = cos(2π/λ * x + φ) * cos(2π * f * t) satisfies the wave equation. To achieve this, one must differentiate the wave function twice with respect to time and space, yielding the second derivatives ∂²y/∂t² and ∂²y/∂x². The ratio of these derivatives results in the expression for the speed of propagation of the wave, specifically v² = λ² * f², confirming that the wave function adheres to the wave equation.

PREREQUISITES
  • Understanding of wave functions and their properties
  • Knowledge of the wave equation in physics
  • Ability to perform partial differentiation
  • Familiarity with concepts of wavelength (λ) and frequency (f)
NEXT STEPS
  • Study the derivation of the wave equation in classical mechanics
  • Learn about standing waves and their characteristics
  • Explore the relationship between wave speed, wavelength, and frequency
  • Practice solving problems involving partial derivatives in wave functions
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Students of physics, educators teaching wave mechanics, and anyone interested in understanding the mathematical foundations of wave behavior.

verd
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Hi, I'm having a little bit of difficulty understanding exactly what to do to get to an answer in section a of this problem. It asks to show that the given function satisfies the wave equation... I have the wave equation. How do I go about 'showing' that it satisfies the wave equation?

Do I just differentiate it twice? ...If so, to which respect to I differentiate it to?


Here's the problem:

You want to measure the mass m of an object, but you don’t have a scale. You therefore decide to attach the object to a string of mass ms and length L, as in the figure, and to generate standing waves on the string (pay attention to the orientation of the axes on the figure!). The wave function that describes the standing wave is given by:
[tex]y(x,t)=\cos(\frac{2\pi}{\lambda}x+\phi)\cos(2\pi ft)[/tex]


where λ is the wavelength, f is the frequency, and φ is the phase.


a) Show that the wave function y(x,t) satisfies the
wave equation and from it derive and expression
for the speed of propagation of the wave in terms of
the given quantities.
 
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verd said:
Hi, I'm having a little bit of difficulty understanding exactly what to do to get to an answer in section a of this problem. It asks to show that the given function satisfies the wave equation... I have the wave equation. How do I go about 'showing' that it satisfies the wave equation?

Do I just differentiate it twice? ...If so, to which respect to I differentiate it to?


Here's the problem:

You want to measure the mass m of an object, but you don’t have a scale. You therefore decide to attach the object to a string of mass ms and length L, as in the figure, and to generate standing waves on the string (pay attention to the orientation of the axes on the figure!). The wave function that describes the standing wave is given by:
[tex]y(x,t)=\cos(\frac{2\pi}{\lambda}x+\phi)\cos(2\pi ft)[/tex]


where λ is the wavelength, f is the frequency, and φ is the phase.


a) Show that the wave function y(x,t) satisfies the
wave equation and from it derive and expression
for the speed of propagation of the wave in terms of
the given quantities.


calculate [itex]{\partial^2 y(x,t) \over \partial t^2}[/itex] and [itex]{\partial^2 y(x,t) \over \partial x^2}[/itex]. The ratio of the first over the second will give you the square of the speed (which will obviously be [itex]\lambda^2 f^2[/itex]).
 

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