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Heat and Thermodynamics question

2019 · 9 Jan · Shift 1 · Q49
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Heat and Thermodynamics question

2019 · 9 Jan · Shift 1 · Q49

JEE MainPhysicsHeat and ThermodynamicsMCQ+4 / −1
A rod, of length L at room temperature and uniform area of cross section A, is made of a metal having coefficient of linear expansion α\alphaα/oC. It is observed that an external compressive force F, is applied on each of its ends, prevents any change in the length of the rod, when its temperature rises by Δ\DeltaΔ TK. Young's modulus, Y, for this metal is :
  1. A
    FAαΔT{F \over {A\alpha \Delta T}}AαΔTF​
  2. B
    FAα(ΔT−273){F \over {A\alpha (\Delta T - 273)}}Aα(ΔT−273)F​
  3. C
    F2AαΔT{F \over {2A\alpha \Delta T}}2AαΔTF​
  4. D
    2FAαΔT{{2F} \over {A\alpha \Delta T}}AαΔT2F​
View written solutionFree

Correct answer: A

  1. Free thermal expansion of the rod

If the rod were allowed to expand freely for a temperature rise of ΔT\Delta TΔT, then the change in length would be

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

So the thermal strain is

ϵthermal=ΔLthermalL=αΔT\epsilon_{\text{thermal}} = \frac{\Delta L_{\text{thermal}}}{L} = \alpha \Delta Tϵthermal​=LΔLthermal​​=αΔT
  1. Effect of compressive force

A compressive force FFF is applied at each end. The internal compressive stress developed in the rod is

σ=FA\sigma = \frac{F}{A}σ=AF​

The corresponding compressive strain is

ϵcompressive=σY=FAY\epsilon_{\text{compressive}} = \frac{\sigma}{Y} = \frac{F}{AY}ϵcompressive​=Yσ​=AYF​

This strain acts opposite to thermal expansion.

  1. Condition for no change in length

The problem states that the rod does not change its length when temperature rises by ΔT\Delta TΔT. Hence,

ϵthermal=ϵcompressive\epsilon_{\text{thermal}} = \epsilon_{\text{compressive}}ϵthermal​=ϵcompressive​

So,

αΔT=FAY\alpha \Delta T = \frac{F}{AY}αΔT=AYF​

Rearranging,

Y=FAαΔTY = \frac{F}{A\alpha \Delta T}Y=AαΔTF​
  1. Matching with options

Thus the correct option is

FAαΔT\boxed{\frac{F}{A\alpha \Delta T}}AαΔTF​​

which is Option A.

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