Calculating Energy and Q of a Vibrating String

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SUMMARY

The discussion focuses on calculating the energy stored in a vibrating string of length 3.2 m and linear mass density 0.008 kg/m, under tension allowing wave propagation at 48 m/s. The string vibrates in its third harmonic with an initial amplitude of 5.0 cm. The energy stored in the system is derived from the potential energy contributions of harmonic oscillators along the string, leading to a total energy calculation. Additionally, the discussion addresses the quality factor (Q) of the system as the amplitude diminishes to 3.0 cm over 1.0 s.

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  • Understanding of wave mechanics and harmonic motion
  • Familiarity with the standing wave equation
  • Knowledge of energy calculations in oscillatory systems
  • Basic calculus for integration of energy contributions
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  • Calculate the total energy stored in a vibrating string using the derived potential energy formula
  • Learn about the concept of quality factor (Q) in oscillatory systems
  • Explore the implications of damping on amplitude and energy in vibrating systems
  • Study the relationship between wave speed, tension, and mass density in strings
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A string 3.2 m long and with a linear mass density of .008 kg/m is kept under tension so that traveling waves propagate at 48 m/s along the string. The ends of the string are clamped and the string vibrates in its third harmonic with an amplitude of 5.0 cm. How much energy is stored in this vibrating system at that time? If the amplitude of the standing wave diminishes to 3.0 cm in 1.0 s, what is the Q of this vibrating system?

I was thinking about starting with

Delta K = .5 U (partial(y)/partial(t))^2 delta x

but this is just a guess; could someone help me with this problem?

Thanks
 
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Start with the standing wave equation$$y(x,t)=2A\sin \left(\frac{2\pi x}{\lambda} \right)\cos (\omega t)$$Here, ##\lambda=\frac{2}{3}L## and ##\omega=\frac{2\pi v}{\lambda}##.

Model the string as a series of harmonic oscillators, each of length ##dx##, mass ##dm=\rho dx## oscillating with same frequency ##\omega## and having variable amplitude ##a(x)=2A\sin \left(\frac{2\pi x}{\lambda} \right)##. At ##t=0## all the oscillators on the string are instantaneously at rest and the contribution of one of them to the potential energy is
$$dU=\frac{1}{2}(\rho dx)\omega^2 a^2= 2 \rho \omega^2 A^2 \sin^2 \left(\frac{2\pi x}{\lambda} \right)dx$$Integrate over the length of the string to get the total stored energy.
 

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