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Question: An Indian rubber cord \[L\] metre long and the area of cross-section A \[m^2\] is suspended vertical...

An Indian rubber cord LL metre long and the area of cross-section A m2m^2 is suspended vertically. Density of rubber is ρkg/m3\rho \,{\text{kg/m}^3} and Young’s modulus of rubber is YN/m2Y\,{\text{N/m}^2}. If cord extends by ll metre under its own weight, then extension is:

A. L2ρgY\dfrac{{{L^2}\rho g}}{Y}

B. L2ρg2Y\dfrac{{{L^2}\rho g}}{{2Y}}

C. L2ρg4Y\dfrac{{{L^2}\rho g}}{{4Y}}

D. YL2ρg\dfrac{Y}{{{L^2}\rho g}}

Explanation

Solution

Use the formula for density of an object. Also use the formula for the stress, strain and Young’s modulus for the material of the object. Using all these formulas derive the expression for the stress,, strain and the Young’s modulus for the material of the rubber cord. From all these formulae, derive the relation for the extension in the rubber cord.

Formulae used:

The density ρ\rho of an object is given by

ρ=mV\rho = \dfrac{m}{V} …… (1)

Here, mm is the mass of the object and VV is the volume of the object.

The stress on an object is given by

Stress=FA{\text{Stress}} = \dfrac{F}{A} …… (2)

Here, FF is the force acting on the object and AA is the area on which the force is applied.

The strain acting on a wire given by

Strain=ΔLL{\text{Strain}} = \dfrac{{\Delta L}}{L} …… (3)

Here, ΔL\Delta L is the change in length of the wire and LL is the original length of the wire.

The Young’s modulus YY of the material of the object is

Y=StressStrainY = \dfrac{{{\text{Stress}}}}{{{\text{Strain}}}} …… (4)

Complete step by step solution:

We have given that length of the rubber cord is LL, cross-sectional area of the cord is A m2m^2, density of the rubber is ρkg/m3\rho kg/m^3 and Young’s modulus for the material of the rubber cord is YN/m2Y N/m^2.

The cord extends by the length ll because of its own weight. The weight of the rubber cord is given by

F=mgF = mg

According to equation (1), substitute ρV\rho V for mm in the above equation.

F=ρVgF = \rho Vg

Substitute ALAL for VV in the above equation.

F=ρALgF = \rho ALg

The stress acting on the rubber cord is given by equation (2).

Substitute ρALg\rho ALg for FF in equation (2).

Stress=ρALgA{\text{Stress}} = \dfrac{{\rho ALg}}{A}

Stress=ρLg \Rightarrow {\text{Stress}} = \rho Lg

Hence, the stress acting on the rubber cord is ρLg\rho Lg.

Let us now calculate the strain acting on the rubber cord. The extension in the length of the cord is due to its own weight and the weight of the cord is acting at the centre of the rubber cord. Hence, the original length of the rubber cord is half of its original length. Substitute ll for ΔL\Delta L and L/2L/2 for LL in equation (3).

Strain=lL/2{\text{Strain}} = \dfrac{l}{{L/2}}

Strain=2lL \Rightarrow {\text{Strain}} = \dfrac{{2l}}{L}

Hence, the strain on the rubber cord is 2lL\dfrac{{2l}}{L}.

Let us now calculate the Young’s modulus of the material of the rubber cord. Substitute ρLg\rho Lg for stress and 2lL\dfrac{{2l}}{L} for strain in equation (4).

Y=ρLg2lLY = \dfrac{{\rho Lg}}{{\dfrac{{2l}}{L}}}

l=L2ρg2Y \therefore l = \dfrac{{{L^2}\rho g}}{{2Y}}

Therefore, the extension in the length of the rubber cord is L2ρg2Y\dfrac{{{L^2}\rho g}}{{2Y}}.

Hence, the correct option is (B).

Note: The student should keep in mind that the weight of the rubber cord acts at its centre of gravity which is at the centre of the rubber cord. Hence, the original length of the rubber cord while determining the strain acting on the wire must be taken half of the whole length of the rubber cord. Otherwise, the derivation for the extension rubber cord will be incorrect.