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Concepts Of Physics MCQ Edition [Volume 2]
Exam
Concepts Of Physics MCQ Edition [Volume 2]
Subject
Physics
Chapter
Heat Transfer

Concepts Of Physics MCQ Edition [Volume 2] · Physics · Heat Transfer

A cylindrical rod with a length of 50 cm and a cross-sectional area...

A cylindrical rod with a length of 50 cm50 \text{ cm} and a cross-sectional area of 1 cm21 \text{ cm}^2 is positioned between a large ice chamber at 0^{}^{{}^{\circ}}\text{C} and an evacuated chamber kept at 27^{}^{{}^{\circ}}\text{C}, as shown in the figure. Very small portions of the rod extend into the chambers, while the remainder is thermally insulated from the surroundings. The cross section entering the evacuated chamber is blackened, allowing it to completely absorb any incident radiation. Once steady state is achieved, the temperature of this blackened end is 17^{}^{{}^{\circ}}\text{C}. Given the Stefan constant σ=6×10−8 W m−2 K−4\sigma = 6 \times 10^{-8} \text{ W m}^{-2} \text{ K}^{-4}, determine the thermal conductivity of the rod's material.
A cylindrical rod with a length of 50 cm and a cross-sectional area of 1 cm^2 is positioned between a large ice chamber

Options

  1. A4.5 W m−1 K−14.5 \text{ W m}^{-1} \text{ K}^{-1}
  2. B1.8 W m−1 K−11.8 \text{ W m}^{-1} \text{ K}^{-1}
  3. C0.9 W m−1 K−10.9 \text{ W m}^{-1} \text{ K}^{-1}
  4. D3.6 W m−1 K−13.6 \text{ W m}^{-1} \text{ K}^{-1}

Correct answer

B. 1.8 W m−1 K−11.8 \text{ W m}^{-1} \text{ K}^{-1}

Step-by-step solution

In steady state, the net rate of heat absorbed by the blackened end via radiation equals the rate of heat conducted through the rod.

The net rate of heat absorbed by radiation is given by the Stefan-Boltzmann law:
Prad=σA(T04−T14)P_{\text{rad}} = \sigma A (T_0^4 - T_1^4)
where T_0 = 27^{}^{{}^{\circ}}\text{C} = 300 \text{ K} is the temperature of the evacuated chamber, and T_1 = 17^{}^{{}^{\circ}}\text{C} = 290 \text{ K} is the temperature of the blackened end.

The rate of heat conduction through the rod is:
Pcond=kA(T1−T2)LP_{\text{cond}} = \dfrac{k A (T_1 - T_2)}{L}
where T_2 = 0^{}^{{}^{\circ}}\text{C} = 273 \text{ K} is the temperature of the ice chamber, and L=50 cm=0.5 mL = 50 \text{ cm} = 0.5 \text{ m}.

Equating PradP_{\text{rad}} and PcondP_{\text{cond}}:
σA(T04−T14)=kA(T1−T2)L\sigma A (T_0^4 - T_1^4) = \dfrac{k A (T_1 - T_2)}{L}

⇒k=σL(T04−T14)T1−T2\Rightarrow k = \dfrac{\sigma L (T_0^4 - T_1^4)}{T_1 - T_2}

Substituting the given values:
T04−T14=(300)4−(290)4=81×108−70.7281×108=10.2719×108 K4T_0^4 - T_1^4 = (300)^4 - (290)^4 = 81 \times 10^8 - 70.7281 \times 10^8 = 10.2719 \times 10^8 \text{ K}^4

k=6×10−8×0.5×10.2719×108290−273k = \dfrac{6 \times 10^{-8} \times 0.5 \times 10.2719 \times 10^8}{290 - 273}

k=3×10.271917=30.815717≈1.8 W m−1 K−1k = \dfrac{3 \times 10.2719}{17} = \dfrac{30.8157}{17} \approx 1.8 \text{ W m}^{-1} \text{ K}^{-1}

Answer: 1.8 W m−1 K−11.8 \text{ W m}^{-1} \text{ K}^{-1}
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