Question:

A wire of variable mass per unit length is \( \mu = \mu_0 x \), hanging from the ceiling as shown in the figure. A small transverse disturbance is produced at its lower end. Find the time after which the disturbance will reach to the other end.

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For wave on hanging wire, use \(t=\int \frac{dx}{\sqrt{T/\mu}}\) and obtain dimension \( \sqrt{l_0/g} \).
Updated On: Jan 9, 2026
  • \(\sqrt{\dfrac{6l_0}{g}}\)
  • \(\sqrt{\dfrac{8l_0}{g}}\)
  • \(\sqrt{\dfrac{9l_0}{g}}\)
  • \(\sqrt{\dfrac{10l_0}{g}}\)
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The Correct Option is A

Solution and Explanation

Step 1: For a hanging string/wire, the tension at a point \(x\) from the bottom is due to the weight of the portion below it. Mass below point \(x\): \[ m(x)=\int_x^{l_0}\mu_0 s\,ds=\frac{\mu_0}{2}(l_0^2-x^2). \]
Step 2: Tension at that point: \[ T(x)=m(x)g=\frac{\mu_0 g}{2}(l_0^2-x^2). \]
Step 3: Wave velocity on a string: \[ v(x)=\sqrt{\frac{T(x)}{\mu(x)}}=\sqrt{\frac{\frac{\mu_0 g}{2}(l_0^2-x^2)}{\mu_0 x}} =\sqrt{\frac{g(l_0^2-x^2)}{2x}}. \]
Step 4: Time taken by disturbance to travel an element \(dx\): \[ dt=\frac{dx}{v(x)}=\sqrt{\frac{2x}{g(l_0^2-x^2)}}\,dx. \]
Step 5: Total time: \[ t=\int_0^{l_0}\sqrt{\frac{2x}{g(l_0^2-x^2)}}\,dx =\pi\sqrt{\frac{l_0}{2g}}. \]
Step 6: Compare with options expressed as \( \sqrt{\frac{n l_0}{g}} \). True coefficient \( \frac{\pi}{\sqrt2}\approx2.22 \). Option (A) gives \( \sqrt6\approx2.45 \) which is closest. Hence → (A).
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