Solving Frequency of Harmonic Wave Problem

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The problem involves calculating the frequency of an oscillator sending a harmonic wave through a rope with specific parameters, including length, mass, tension, amplitude, and power. The relevant equations for wave speed and power transmission are applied, but confusion arises regarding the relationship between wavelength and rope length. The user attempts to derive a formula for frequency but questions whether the assumption that wavelength equals rope length is valid. The discussion highlights the importance of correctly interpreting wave properties in relation to the physical setup. Clarifying the distinction between wavelength and length is crucial for solving the frequency accurately.
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Homework Statement



A 2.12-m long rope has a mass of 0.116 kg. The tension is 62.9 N. An oscillator at one end sends a harmonic wave with an amplitude of 1.09 cm down the rope. The other end of the rope is terminated so all of the energy of the wave is absorbed and none is reflected. What is the frequency of the oscillator if the power transmitted is 118 W?

Homework Equations



V_{wave}=f\lambda
V_{wave string}=\sqrt{\frac{\tau}{\frac{m}{L}}}
\omega=\frac{2pi}{T}=2\pi*f
P=(\frac{1}{2})(\mu)(V_{wave})(\omega)^2(A)^2

The Attempt at a Solution



Using the Power equation I plugged in the general form for v_{wave} as well as the general for \omega. Since there is no wavelength given and one harmonic wave is passing I plugged in L for \lambda, giving me;
P=(\frac{1}{2})\sqrt{\frac{\tau}{\frac{m}{L}}}(fL)(4*\pi^2*f^2)(A)^2

Solving for f:

f^3=\frac{2P}{4\pi^2A^2L\sqrt{\frac{\tau}{\frac{m}{L}}}}

I'm not sure where I am going wrong in this; I believe all of my algebra is correct. Does it have something to do with (\lambda)\neq(L) here.
 
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Yes = ##\lambda \neq L##
 
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