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Solved: When a transverse sinusoidal wave is present on a
Chapter 15, Problem 57P(choose chapter or problem)
When a transverse sinusoidal wave is present on a string, the particles of the string undergo SHM. This is the same motion as that of a mass attached to an ideal spring of force constant \(k^{\prime}\), for which the angular frequency of oscillation was found in Chapter 14 to be \(\omega=\sqrt{k / m}\). Consider a string with tension and mass per unit length \(\mu\), along which is propagating a sinusoidal wave with amplitude A and wavelength \(\lambda\). (a) Find the “force constant” \(k^{\prime}\) of the restoring force that acts on a short segment of the string of length \(\Delta x) (where \(\Delta x \ll \lambda\)). (b) How does the “force constant” calculated in part (b) depend on , \(\mu\), , and \(\lambda\)? Explain the physical reasons this should be so.
Equation Transcription:
Text Transcription:
K’
omega=sqrtk/m
U
Lambda
K’
Deltax
deltax<<lambda
U
Lambda
Questions & Answers
QUESTION:
When a transverse sinusoidal wave is present on a string, the particles of the string undergo SHM. This is the same motion as that of a mass attached to an ideal spring of force constant \(k^{\prime}\), for which the angular frequency of oscillation was found in Chapter 14 to be \(\omega=\sqrt{k / m}\). Consider a string with tension and mass per unit length \(\mu\), along which is propagating a sinusoidal wave with amplitude A and wavelength \(\lambda\). (a) Find the “force constant” \(k^{\prime}\) of the restoring force that acts on a short segment of the string of length \(\Delta x) (where \(\Delta x \ll \lambda\)). (b) How does the “force constant” calculated in part (b) depend on , \(\mu\), , and \(\lambda\)? Explain the physical reasons this should be so.
Equation Transcription:
Text Transcription:
K’
omega=sqrtk/m
U
Lambda
K’
Deltax
deltax<<lambda
U
Lambda
ANSWER:
Solution 57P
Step 1