Chapter 14: Problem 59
An ideal spring is stretched to a total length \(L_{1} .\) When that length is doubled, the speed of transverse waves on the spring triples. Find an expression for the unstretched length of the spring.
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Chapter 14: Problem 59
An ideal spring is stretched to a total length \(L_{1} .\) When that length is doubled, the speed of transverse waves on the spring triples. Find an expression for the unstretched length of the spring.
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When a \(340-\mathrm{g}\) spring is stretched to a total length of \(40 \mathrm{cm},\) it supports transverse waves propagating at \(4.5 \mathrm{m} / \mathrm{s} .\) When it's stretched to \(60 \mathrm{cm},\) the waves propagate at \(12 \mathrm{m} / \mathrm{s}\). Find (a) the spring's unstretched length and (b) its spring constant.
Two waves have the same angular frequency \(\omega,\) wave number \(k\) and amplitude \(A,\) but they differ in phase: \(y_{1}=A \cos (k x-\omega t)\) and \(y_{2}=A \cos (k x-\omega t+\phi) .\) Show that their superposition is also a simple harmonic wave, and determine its amplitude as a function of the phase difference \(\phi.\)
A rope is stretched between supports \(18.3 \mathrm{m}\) apart; its tension is \(78.6 \mathrm{N} .\) If one end of the rope is tweaked, the resulting disturbance reaches the other end 585 ms later. Find the rope's mass.
If you place a perfectly clear piece of glass in perfectly clear water, you can still see the glass. Why?
If you doubled the tension in a string, what would happen to the speed of waves on the string?
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