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Properties of Matter question

2019 · 12 Apr · Shift 2 · Q51
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Properties of Matter question

2019 · 12 Apr · Shift 2 · Q51

JEE MainPhysicsProperties of MatterMCQ+4 / −1
A uniform cylindrical rod of length L and radius r, is made from a material whose Young’s modulus of Elasticity equals Y. When this rod is heated by temperature T and simultaneously subjected to a net longitudinal compressional force F, its length remains unchanged. The coefficient of volume expansion, of the material of the rod, is (nearly) equal to :
  1. A
    3F(πr2YT){{3F} \over {\left( {\pi {r^2}YT} \right)}}(πr2YT)3F​
  2. B
    6F(πr2YT){{6F} \over {\left( {\pi {r^2}YT} \right)}}(πr2YT)6F​
  3. C
    F(3πr2YT){F \over {\left( {3\pi {r^2}YT} \right)}}(3πr2YT)F​
  4. D
    9F(πr2YT){9F\left( {\pi {r^2}YT} \right)}9F(πr2YT)
View written solutionFree

Correct answer: A

  1. Given data
  • Length of rod =L= L=L
  • Radius =r= r=r
  • Cross-sectional area A=πr2A = \pi r^2A=πr2
  • Young's modulus =Y= Y=Y
  • Rise in temperature =T= T=T
  • Compressive force =F= F=F

The rod is heated and compressed simultaneously, yet its length remains unchanged.


  1. Thermal expansion of length

If the coefficient of linear expansion is α\alphaα, then the increase in length due to heating is

ΔLthermal=αLT\Delta L_{\text{thermal}} = \alpha L TΔLthermal​=αLT


  1. Compression due to force

Longitudinal strain produced by compressive force FFF is

strain=FAY\text{strain} = \frac{F}{AY}strain=AYF​

So decrease in length is

ΔLcompress=FLAY=FLπr2Y\Delta L_{\text{compress}} = \frac{FL}{AY} = \frac{FL}{\pi r^2 Y}ΔLcompress​=AYFL​=πr2YFL​


  1. Condition: net change in length is zero

Since the rod's length remains unchanged,

ΔLthermal=ΔLcompress\Delta L_{\text{thermal}} = \Delta L_{\text{compress}}ΔLthermal​=ΔLcompress​

So,

αLT=FLπr2Y\alpha L T = \frac{FL}{\pi r^2 Y}αLT=πr2YFL​

Cancel LLL:

αT=Fπr2Y\alpha T = \frac{F}{\pi r^2 Y}αT=πr2YF​

Hence,

α=Fπr2YT\alpha = \frac{F}{\pi r^2 Y T}α=πr2YTF​


  1. Coefficient of volume expansion

For an isotropic solid,

γ=3α\gamma = 3\alphaγ=3α

Therefore,

γ=3(Fπr2YT)\gamma = 3\left(\frac{F}{\pi r^2 Y T}\right)γ=3(πr2YTF​)

γ=3Fπr2YT\boxed{\gamma = \frac{3F}{\pi r^2 Y T}}γ=πr2YT3F​​


  1. Match with options

This corresponds to Option A:

3Fπr2YT\boxed{\frac{3F}{\pi r^2 Y T}}πr2YT3F​​


  1. Comparison with stored answer

Stored correct answer: A

Our derived answer: A

So they agree.

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