Question:

A uniform chain of mass $m$ and length $l$ is on a smooth horizontal table with $\left( \frac{1}{n}\right)^{th}$ part of its length is hanging from one end of the table. The velocity of the chain when it completely slips off the table is

Updated On: Apr 4, 2024
  • $\sqrt{gl \left(1- \frac{1}{n^{2}}\right)} $
  • $\sqrt{2 gl \left(1 + \frac{1}{n^{2}}\right)} $
  • $\sqrt{ 2 gl \left(1- \frac{1}{n^{2}}\right)} $
  • $\sqrt{2gl } $
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The Correct Option is A

Solution and Explanation

Taking surface of table as zero level of potential energy, $\bullet$ Potential energy of chain with $\frac{1}{n}$ th part hanging $=\frac{-M g l}{2 n^{2}}$ $\bullet$ Potential energy of chain or it leaves table $=\frac{-M g l}{2}$ Kinetic energy = Loss of potential energy $\Rightarrow \frac{1}{2} M v^{2}=\frac{M g l}{2}\left(1-\frac{1}{n^{2}}\right)$ $\Rightarrow v=\sqrt{g l\left(1-\frac{1}{n^{2}}\right)}$
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Concepts Used:

Work-Energy Theorem

The work and kinetic energy principle (also known as the work-energy theorem) asserts that the work done by all forces acting on a particle equals the change in the particle's kinetic energy. By defining the work of the torque and rotational kinetic energy, this definition can be extended to rigid bodies.

The change in kinetic energy KE is equal to the work W done by the net force on a particle is given by,

W = ΔKE = ½ mv2f − ½ mv2i

Where, 

vi → Speeds of the particle before the application of force

vf → Speeds of the particle after the application of force

m → Particle’s mass

Note: Energy and Momentum are related by, E = p2 / 2m.