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JEE Advanced 2023 Paper 2 · Physics · Calorimetry and Heat Transfer · medium

A planet of negligible atmospheric heat capacity orbits a star at distance d=1.5×10^11 m. The star is a black body of radius 7×10^8 m and surface…

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A planet of negligible atmospheric heat capacity orbits a star at distance d=1.5×1011 md=1.5\times10^{11}\ \mathrm{m}. The star is a black body of radius 7×108 m7\times10^{8}\ \mathrm{m} and surface temperature 5800 K5800\ \mathrm{K}. The planet reflects 30%30\% of the incident radiation and, being a fast rotator, radiates as a black body uniformly from its whole surface. Using Wien's constant 2.898×10−3 m K2.898\times10^{-3}\ \mathrm{m\,K}, the wavelength at which the planet's emission peaks in steady state is nearest to
  1. A. 8.0 μm8.0\ \mu\mathrm{m}
  2. B. 10.3 μm10.3\ \mu\mathrm{m}
  3. C. 11.3 μm11.3\ \mu\mathrm{m}
  4. D. 12.4 μm12.4\ \mu\mathrm{m}
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Answer: (C) 11.3 μm11.3\ \mu\mathrm{m}

Power absorbed by the planet (radius rpr_p): intensity at distance dd is σTs4 Rs2d2\sigma T_s^4\,\dfrac{R_s^2}{d^2}, intercepted over the cross-section πrp2\pi r_p^2, and only (1−0.3)(1-0.3) is absorbed. Power radiated: 4πrp2σT44\pi r_p^2\sigma T^4. Balancing, T4=0.74 Ts4Rs2d2T^4=\dfrac{0.7}{4}\,T_s^4\dfrac{R_s^2}{d^2}, so T=TsRs2d (0.7)1/4=5800×0.0483×0.9147≈256 KT=T_s\sqrt{\dfrac{R_s}{2d}}\,(0.7)^{1/4}=5800\times0.0483\times0.9147\approx256\ \mathrm{K}. Wien's law gives λm=2.898×10−3256.3≈11.3 μm\lambda_m=\dfrac{2.898\times10^{-3}}{256.3}\approx11.3\ \mu\mathrm{m}. Without the albedo one gets 280 K280\ \mathrm{K} and 10.3 μm10.3\ \mu\mathrm{m}; using Rs/dR_s/d instead of Rs/2dR_s/2d gives 8.0 μm8.0\ \mu\mathrm{m}; applying 0.71/20.7^{1/2} gives 12.4 μm12.4\ \mu\mathrm{m}.
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