Solving Frequency of Harmonic Wave Problem

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SUMMARY

The discussion centers on calculating the frequency of a harmonic wave transmitted through a rope with specific parameters: a length of 2.12 m, mass of 0.116 kg, and tension of 62.9 N. The power transmitted is given as 118 W, and the amplitude of the wave is 1.09 cm. The user attempts to derive the frequency using the power equation and the wave velocity formula, ultimately expressing frequency in terms of power, amplitude, and other constants. The confusion arises from the relationship between wavelength and rope length, indicating that the wavelength does not equal the length of the rope in this scenario.

PREREQUISITES
  • Understanding of harmonic waves and wave properties
  • Familiarity with tension in strings and wave velocity equations
  • Knowledge of power transmission in wave mechanics
  • Basic algebra and manipulation of equations
NEXT STEPS
  • Study the relationship between wavelength and harmonic frequencies in strings
  • Learn about the effects of tension and mass per unit length on wave speed
  • Explore the derivation of power equations in wave mechanics
  • Investigate the implications of boundary conditions on wave behavior
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Students in physics, particularly those studying wave mechanics, as well as educators and anyone involved in solving problems related to harmonic waves and their properties.

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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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