Calculating Energy and Q of a Vibrating String

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To calculate the energy stored in a vibrating string, the standing wave equation is used, incorporating the string's length, tension, and amplitude. The energy can be derived by modeling the string as harmonic oscillators and integrating the potential energy contributions along its length. The Q factor, which measures the damping of the wave, can be determined by analyzing the change in amplitude over time. Specifically, if the amplitude decreases from 5.0 cm to 3.0 cm in 1.0 second, the Q factor can be calculated using the formula related to amplitude decay. This discussion emphasizes the application of wave mechanics and energy principles in understanding vibrating 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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