Verified Solution • 2025–26 Session moderate

QJEEM23Ph7734: JEE Main 2023 Physics - Class 11 JEEM23Ph7734 Solution: A wire of length ' ' and radius ' ' is clamped rigidly at one…

A wire of length ' LL ' and radius ' rr ' is clamped rigidly at one end. When the other end of the wire is pulled by a force ff , its length increases by ' ll '. Another wire of same material of length ' 2 L2 \mathrm{~L} ' and radius ' 2r2 r ' is pulled by a force ' 2f2 f '. Then the increase in its length will be :

Multiple Choice Options

  • A 2l2 l
  • B 4l4 l
  • C ll
  • D l/2l / 2

Step-by-Step Verified Solution

Let AA be the cross-sectional area of the first wire, and let YY be its Young's modulus.

The strain in the wire is given by ϵ=lL\epsilon = \frac{l}{L} , where ll is the increase in length. The stress in the wire is given by σ=fA\sigma = \frac{f}{A} .

According to Hooke's law, the stress is proportional to the strain, so we have σ=Yϵ\sigma = Y \epsilon . Solving for ff , we get f=YAlf = \frac{YA}{l} .

The second wire has twice the length and four times the cross-sectional area of the first wire, so its cross-sectional area is 4A4A and its Young's modulus is still YY .

When a force of 2f2f is applied to this wire, the stress in the wire is σ=2f4A=f2A\sigma = \frac{2f}{4A} = \frac{f}{2A} .

Using Hooke's law again, we have σ=Yϵ\sigma = Y \epsilon . Solving for ϵ\epsilon , we get ϵ=σY=f2AY\epsilon = \frac{\sigma}{Y} = \frac{f}{2AY} .

The increase in length of the second wire is given by Δl=ϵ⋅2L=f⋅2L2AY\Delta l = \epsilon \cdot 2L = \frac{f \cdot 2L}{2AY} .

Substituting the expression for ff that we derived earlier, we get Δl=YL⋅2A⋅l2AY⋅L=l\Delta l = \frac{YL \cdot 2A \cdot l}{2AY \cdot L} = \boxed{l} .

Therefore, the increase in length of the second wire is the same as the increase in length of the first wire, which is ll .

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