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QJEEAdv13Phbe44: JEE Advanced 2013 Physics - Class 11 JEEAdv13Phbe44 Solution: One end of a horizontal thick copper wire of length 2L and…

One end of a horizontal thick copper wire of length 2L and radius 2R is welded to an end of another horizontal thin copper wire of length L and radius R. When the arrangement is stretched by applying forces at two ends, the ratio of the elongation in the thin wire to that in the thick wire is

Multiple Choice Options

  • A 0.25
  • B 0.5
  • C 2
  • D 4

Step-by-Step Verified Solution

To solve this problem, we need to use Hooke's Law, which states that the elongation (or stretch) of a material is directly proportional to the force applied and the length of the material, and inversely proportional to the cross-sectional area and the Young's modulus of the material. Mathematically, this relation can be expressed as:

ΔL=F⋅LA⋅Y\Delta L = \frac{F \cdot L}{A \cdot Y}

where:

  • ΔL\Delta L is the elongation
  • FF is the force applied
  • LL is the original length of the material
  • AA is the cross-sectional area of the material
  • YY is the Young's modulus of the material

In this problem, the Young's modulus ( YY ) and the force ( FF ) are the same for both wires because they are made of the same material (copper) and the forces applied are equal. Therefore, the elongation is dependent on the length and cross-sectional area of each wire.

For the thick wire with length 2L2L and radius 2R2R , the cross-sectional area A1A_1 is given by:

A1=π(2R)2=4πR2A_1 = \pi (2R)^2 = 4\pi R^2

For the thin wire with length LL and radius RR , the cross-sectional area A2A_2 is given by:

A2=πR2A_2 = \pi R^2

Using the formula for elongation for both wires, we get:

Elongation of the thick wire ( ΔLthick\Delta L_\text{thick} ):

ΔLthick=F⋅2L4πR2⋅Y=F⋅2L4πR2Y=FL2πR2Y\Delta L_\text{thick} = \frac{F \cdot 2L}{4\pi R^2 \cdot Y} = \frac{F \cdot 2L}{4\pi R^2 Y} = \frac{FL}{2\pi R^2 Y}

Elongation of the thin wire ( ΔLthin\Delta L_\text{thin} ):

ΔLthin=F⋅LπR2⋅Y=FLπR2Y\Delta L_\text{thin} = \frac{F \cdot L}{\pi R^2 \cdot Y} = \frac{FL}{\pi R^2 Y}

To find the ratio of the elongation in the thin wire to that in the thick wire, we divide ΔLthin\Delta L_\text{thin} by ΔLthick\Delta L_\text{thick} :

Ratio=ΔLthinΔLthick=FLπR2YFL2πR2Y=FLπR2Y⋅2πR2YFL=2\text{Ratio} = \frac{\Delta L_\text{thin}}{\Delta L_\text{thick}} = \frac{\frac{FL}{\pi R^2 Y}}{\frac{FL}{2\pi R^2 Y}} = \frac{FL}{\pi R^2 Y} \cdot \frac{2\pi R^2 Y}{FL} = 2

Therefore, the ratio of the elongation in the thin wire to that in the thick wire is 2. The correct answer is:

Option C: 2.00

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