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Heat and Thermodynamics question

2023 · Shift 2 · Q51
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  5. /2023 · Shift 2 · Q51

Heat and Thermodynamics question

2023 · Shift 2 · Q51

JEE AdvancedPhysicsHeat and ThermodynamicsNumerical+3 / −1
A cylindrical furnace has height (H)(H)(H) and diameter (D)(D)(D) both 1 m1 \mathrm{~m}1 m. It is maintained at temperature 360 K360 \mathrm{~K}360 K. The air gets heated inside the furnace at constant pressure PaP_aPa​ and its temperature becomes T=360 KT=360 \mathrm{~K}T=360 K. The hot air with density ρ\rhoρ rises up a vertical chimney of diameter d=0.1 md=0.1 \mathrm{~m}d=0.1 m and height h=9 mh=9 \mathrm{~m}h=9 m above the furnace and exits the chimney (see the figure). As a result, atmospheric air of density ρa=1.2 kg m−3\rho_a=1.2 \mathrm{~kg} \mathrm{~m}^{-3}ρa​=1.2 kg m−3, pressure PaP_aPa​ and temperature Ta=300 KT_a=300 \mathrm{~K}Ta​=300 K enters the furnace. Assume air as an ideal gas, neglect the variations in ρ\rhoρ and TTT inside the chimney and the furnace. Also ignore the viscous effects. [Given: The acceleration due to gravity g=10 m s−2g=10 \mathrm{~m} \mathrm{~s}^{-2}g=10 m s−2 and π=3.14\pi=3.14π=3.14] JEE Advanced 2023 Paper 2 Online Physics - Heat and Thermodynamics Question 8 English ComprehensionWhen the chimney is closed using a cap at the top, a pressure difference ΔP\Delta PΔP develops between the top and the bottom surfaces of the cap. If the changes in the temperature and density of the hot air, due to the stoppage of air flow, are negligible then the value of ΔP\Delta PΔP is ‾\underline{\hspace{2cm}}​Nm−2\mathrm{N} \mathrm{m}^{-2}Nm−2.
Numerical answer
View written solutionFree

Correct answer: 20

  1. Given data
  • Furnace temperature: T=360 KT=360\,\text{K}T=360K
  • Atmospheric temperature: Ta=300 KT_a=300\,\text{K}Ta​=300K
  • Atmospheric density: ρa=1.2 kg m−3\rho_a=1.2\,\text{kg m}^{-3}ρa​=1.2kg m−3
  • Furnace height: H=1 mH=1\,\text{m}H=1m
  • Chimney height above furnace: h=9 mh=9\,\text{m}h=9m
  • Thus total height of hot air column from furnace bottom to chimney top: H+h=1+9=10 mH+h=1+9=10\,\text{m}H+h=1+9=10m
  • Atmospheric pressure at furnace inlet and outside air is PaP_aPa​.

We need the pressure difference across the cap when chimney top is closed.


  1. Density of hot air inside furnace/chimney

Since air behaves as an ideal gas and heating is at constant pressure, ρ∝1T\rho \propto \frac{1}{T}ρ∝T1​ So, ρ=ρaTaT\rho = \rho_a\frac{T_a}{T}ρ=ρa​TTa​​ ρ=1.2×300360=1.2×56=1.0 kg m−3\rho = 1.2\times \frac{300}{360} = 1.2\times \frac{5}{6} = 1.0\,\text{kg m}^{-3}ρ=1.2×360300​=1.2×65​=1.0kg m−3

Thus hot air density is ρ=1.0 kg m−3\rho=1.0\,\text{kg m}^{-3}ρ=1.0kg m−3


  1. Pressure at the bottom of furnace

The furnace is open to atmosphere at the bottom inlet, so pressure there is atmospheric: Pbottom=PaP_{\text{bottom}}=P_aPbottom​=Pa​

Inside the closed chimney-furnace system, hot air of density ρ\rhoρ fills the column of height H+h=10 mH+h=10\,\text{m}H+h=10m. So pressure decreases upward hydrostatically by ρg(H+h)\rho g(H+h)ρg(H+h)

Hence pressure just below the cap (inside chimney top) is Pin=Pa−ρg(H+h)P_{\text{in}}=P_a-\rho g(H+h)Pin​=Pa​−ρg(H+h)

Outside the cap, the pressure is the atmospheric pressure at the same height. Starting from pressure PaP_aPa​ at the furnace bottom level, and moving up through outside atmospheric air of density ρa\rho_aρa​ by height 10 m10\,\text{m}10m, Pout=Pa−ρag(H+h)P_{\text{out}}=P_a-\rho_a g(H+h)Pout​=Pa​−ρa​g(H+h)


  1. Pressure difference across cap

The pressure difference between bottom and top surfaces of the cap is ΔP=Pout−Pin\Delta P=P_{\text{out}}-P_{\text{in}}ΔP=Pout​−Pin​

Substitute: ΔP=(Pa−ρag(H+h))−(Pa−ρg(H+h))\Delta P=\left(P_a-\rho_a g(H+h)\right)-\left(P_a-\rho g(H+h)\right)ΔP=(Pa​−ρa​g(H+h))−(Pa​−ρg(H+h)) ΔP=(ρ−ρa)g(H+h)\Delta P=(\rho-\rho_a)g(H+h)ΔP=(ρ−ρa​)g(H+h) In magnitude, ΔP=(ρa−ρ)g(H+h)\Delta P=(\rho_a-\rho)g(H+h)ΔP=(ρa​−ρ)g(H+h)

Now, ρa−ρ=1.2−1.0=0.2 kg m−3\rho_a-\rho = 1.2-1.0=0.2\,\text{kg m}^{-3}ρa​−ρ=1.2−1.0=0.2kg m−3 Therefore, ΔP=0.2×10×10=20 N m−2\Delta P=0.2\times 10\times 10 = 20\,\text{N m}^{-2}ΔP=0.2×10×10=20N m−2


  1. Final answer

20 N m−2\boxed{20\,\text{N m}^{-2}}20N m−2​


  1. Comparison with stored answer

Stored correct answer = 303030

My derived answer is 202020, so I do not agree with the stored answer.

The likely reason is that the pressure difference should be computed over the full hot-air column height from furnace bottom to chimney top, which is H+h=10 mH+h=10\,\text{m}H+h=10m, and using ideal-gas density relation gives ρ=1.0 kg m−3\rho=1.0\,\text{kg m}^{-3}ρ=1.0kg m−3. This yields 20 N m−220\,\text{N m}^{-2}20N m−2, not 30 N m−230\,\text{N m}^{-2}30N m−2.

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