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Heat and Thermodynamics question

2016 · Shift 0 · Q58
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  5. /2016 · Shift 0 · Q58

Heat and Thermodynamics question

2016 · Shift 0 · Q58

JEE MainPhysicsHeat and ThermodynamicsMCQ+4 / −1
A pendulum clock loses 12s12s12s a day if the temperature is 40∘C{40^ \circ }C40∘C and gains 4s4s4s a day if the temperature is 20∘C.{20^ \circ }C.20∘C. The temperature at which the clock will show correct time, and the co-efficient of linear expansion (α)\left( \alpha \right)(α) of the metal of the pendulum shaft are respectively :
  1. A
    30∘C;  α=1.85×10−3/∘C{30^ \circ }C;\,\,\alpha = 1.85 \times {10^{ - 3}}/{}^ \circ C30∘C;α=1.85×10−3/∘C
  2. B
    55∘C;  α=1.85×10−2/∘C{55^ \circ }C;\,\,\alpha = 1.85 \times {10^{ - 2}}/{}^ \circ C55∘C;α=1.85×10−2/∘C
  3. C
    25∘C;  α=1.85×10−5/∘C{25^ \circ }C;\,\,\alpha = 1.85 \times {10^{ - 5}}/{}^ \circ C25∘C;α=1.85×10−5/∘C
  4. D
    60∘C;  α=1.85×10−4/∘C{60^ \circ }C;\,\,\alpha = 1.85 \times {10^{ - 4}}/{}^ \circ C60∘C;α=1.85×10−4/∘C
View written solutionFree

Correct answer: C

  1. Time period of a pendulum and temperature dependence

For a pendulum, T=2πlgT = 2\pi \sqrt{\frac{l}{g}}T=2πgl​​

If temperature changes, the length changes as l=l0(1+αθ)l = l_0(1+\alpha \theta)l=l0​(1+αθ)

Hence, for small changes, ΔTT=12Δll=12αΔθ\frac{\Delta T}{T} = \frac{1}{2}\frac{\Delta l}{l} = \frac{1}{2}\alpha \Delta \thetaTΔT​=21​lΔl​=21​αΔθ

So the fractional change in period is T′−TT=12α(θ−θ0)\frac{T'-T}{T} = \frac{1}{2}\alpha (\theta-\theta_0)TT′−T​=21​α(θ−θ0​)

A larger period means the clock runs slow (loses time), and a smaller period means it runs fast (gains time).


  1. Relate daily gain/loss to fractional change in period

Let the clock keep correct time at temperature θ\thetaθ.

Then at 40∘C40^\circ C40∘C, it loses 12 s12\text{ s}12 s per day. So, ΔTT=1286400\frac{\Delta T}{T} = \frac{12}{86400}TΔT​=8640012​

Thus, 12α(40−θ)=1286400(1)\frac{1}{2}\alpha (40-\theta)=\frac{12}{86400} \qquad (1)21​α(40−θ)=8640012​(1)

At 20∘C20^\circ C20∘C, it gains 4 s4\text{ s}4 s per day, so its period is smaller than correct. Thus, 12α(20−θ)=−486400(2)\frac{1}{2}\alpha (20-\theta)= -\frac{4}{86400} \qquad (2)21​α(20−θ)=−864004​(2)


  1. Solve for correct temperature

From (1): 12α(40−θ)=1286400\frac{1}{2}\alpha (40-\theta)=\frac{12}{86400}21​α(40−θ)=8640012​

From (2): 12α(20−θ)=−486400\frac{1}{2}\alpha (20-\theta)=-\frac{4}{86400}21​α(20−θ)=−864004​

Divide (1) by (2): 40−θ20−θ=12−4=−3\frac{40-\theta}{20-\theta}=\frac{12}{-4}=-320−θ40−θ​=−412​=−3

So, 40−θ=−3(20−θ)40-\theta = -3(20-\theta)40−θ=−3(20−θ) 40−θ=−60+3θ40-\theta = -60 + 3\theta40−θ=−60+3θ 100=4θ100 = 4\theta100=4θ θ=25∘C\theta = 25^\circ Cθ=25∘C


  1. Find coefficient of linear expansion

Using equation (1): 12α(40−25)=1286400\frac{1}{2}\alpha (40-25)=\frac{12}{86400}21​α(40−25)=8640012​ 12α(15)=1286400\frac{1}{2}\alpha (15)=\frac{12}{86400}21​α(15)=8640012​ 7.5α=12864007.5\alpha = \frac{12}{86400}7.5α=8640012​ α=1286400×7.5\alpha = \frac{12}{86400\times 7.5}α=86400×7.512​

Now, 86400×7.5=64800086400\times 7.5 = 64800086400×7.5=648000

Hence, α=12648000=1.85×10−5/∘C\alpha = \frac{12}{648000} = 1.85\times 10^{-5}/^\circ Cα=64800012​=1.85×10−5/∘C


  1. Check options
  • A: 30∘C30^\circ C30∘C, wrong temperature and wrong α\alphaα
  • B: 55∘C55^\circ C55∘C, wrong
  • C: 25∘C25^\circ C25∘C, α=1.85×10−5/∘C\alpha = 1.85\times 10^{-5}/^\circ Cα=1.85×10−5/∘C ✅
  • D: wrong

Therefore, the correct option is: C\boxed{\text{C}}C​

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