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Question: A material has Poisson's ratio of 0.5. lf a uniform rod suffers a longitudinal strain of \[2\times {...

A material has Poisson's ratio of 0.5. lf a uniform rod suffers a longitudinal strain of 2×1032\times {{10}^{-3}}, the percentage increase in its volume is:
A. 2%
B. 0.5%
C. 4%
D. 0%

Explanation

Solution

To find the percentage increase in volume, we use the relation between the volume change of a material due to strain and the Poisson’s ratio. The ratio of the change in length to the original length is termed as longitudinal strain.
Formula used:
The relationship between change in volume and Poisson’s ratio is given by,
ΔVV=(12σ)(ΔLL)\dfrac{\Delta V}{V}=\left( 1-2\sigma \right)\left( \dfrac{\Delta L}{L} \right)
where, ΔV\Delta V is change in volume, V is original volume, σ\sigma is Poisson’s ratio, ΔL\Delta L is change in length and L is original length.

Complete answer:
Given,
σ=0.5\sigma =0.5
Longitudinal strain = 2×1032\times {{10}^{-3}}
Therefore,
ΔLL=2×103\dfrac{\Delta L}{L}=2\times {{10}^{-3}}
Substituting these values in ΔVV=(12σ)(ΔLL)\dfrac{\Delta V}{V}=\left( 1-2\sigma \right)\left( \dfrac{\Delta L}{L} \right), we get,
ΔVV=(12σ)(ΔLL)\dfrac{\Delta V}{V}=\left( 1-2\sigma \right)\left( \dfrac{\Delta L}{L} \right)
ΔVV=(12(0.5))(2×103)\dfrac{\Delta V}{V}=\left( 1-2\left( 0.5 \right) \right)\left( 2\times {{10}^{-3}} \right)
ΔVV=(11)(2×103)\dfrac{\Delta V}{V}=\left( 1-1 \right)\left( 2\times {{10}^{-3}} \right)
ΔVV=0×(2×103)\dfrac{\Delta V}{V}=0\times \left( 2\times {{10}^{-3}} \right)
ΔVV=0\dfrac{\Delta V}{V}=0
Since, the ratio between change in volume and original volume is zero, the percentage increase in volume will be 0%

The answer is option D.

Note:
The relationship between change in volume and Poisson’s ratio is derived as follows:
Volume of the rod is given by,
V=πr2lV=\pi {{r}^{2}}l
Where, r is radius and l is length.
Differentiating both sides, we get,
dV=πr2dl+π2rldrdV=\pi {{r}^{2}}dl+\pi 2rldr
Dividing both sides by volume, we get,
dVV=πr2dlπr2l+π2rldrπr2l\dfrac{dV}{V}=\dfrac{\pi {{r}^{2}}dl}{\pi {{r}^{2}}l}+\dfrac{\pi 2rldr}{\pi {{r}^{2}}l}
Cancelling out common terms,
dVV=dll+2drr\dfrac{dV}{V}=\dfrac{dl}{l}+\dfrac{2dr}{r}
Now, Poisson’s ratio is given by,
σ=(drr)dll\sigma =\dfrac{-\left( \dfrac{dr}{r} \right)}{\dfrac{dl}{l}}
Therefore,
drr=σdll\dfrac{dr}{r}=-\sigma \dfrac{dl}{l}
Substituting this value in dVV=dll+2drr\dfrac{dV}{V}=\dfrac{dl}{l}+\dfrac{2dr}{r}, we get,
dVV=dll+2drr\dfrac{dV}{V}=\dfrac{dl}{l}+\dfrac{2dr}{r}
dVV=dll2σdll\dfrac{dV}{V}=\dfrac{dl}{l}-2\sigma \dfrac{dl}{l}
dVV=(12σ)dll\dfrac{dV}{V}=\left( 1-2\sigma \right)\dfrac{dl}{l}
The radius of the rod decreases as length increases, hence it is taken as negative.