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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 central hole of radius r_1 is created in a uniform circular disc...

A central hole of radius r1r_1 is created in a uniform circular disc having thickness dd and radius r2r_2. The inner surface (a cylinder of length dd and radius r1r_1) is kept at a temperature θ1\theta_1, while the outer surface (a cylinder of length dd and radius r2r_2) is kept at a temperature θ2\theta_2 (with θ1>θ2\theta_1 > \theta_2). Given that the thermal conductivity of the disc's material is KK, determine the heat flowing per unit time through the disc.

Options

  1. AπK(r22−r12)(θ1−θ2)d\dfrac{\pi K (r_2^2 - r_1^2) (\theta_1 - \theta_2)}{d}
  2. BπKd(θ1−θ2)ln⁡(r2/r1)\dfrac{\pi K d (\theta_1 - \theta_2)}{\ln(r_2 / r_1)}
  3. C2πKd(θ1−θ2)r2−r1\dfrac{2\pi K d (\theta_1 - \theta_2)}{r_2 - r_1}
  4. D2πKd(θ1−θ2)ln⁡(r2/r1)\dfrac{2\pi K d (\theta_1 - \theta_2)}{\ln(r_2 / r_1)}

Correct answer

D. 2πKd(θ1−θ2)ln⁡(r2/r1)\dfrac{2\pi K d (\theta_1 - \theta_2)}{\ln(r_2 / r_1)}

Step-by-step solution

Consider a cylindrical shell of radius randthicknessr and thicknessdrwithinthedisc.<br><br>Thesurfaceareaofthisshellthroughwhichheatflowsradiallyiswithin the disc.<br><br>The surface area of this shell through which heat flows radially isA = 2\pi r d.<br><br>Thethermalresistanceofthiselementalshellisgivenby.<br><br>The thermal resistance of this elemental shell is given bydR = \dfrac{dr}{KA} = \dfrac{dr}{K(2\pi r d)}.<br><br>Thetotalthermalresistanceofthediscisobtainedbyintegratingfrom.<br><br>The total thermal resistance of the disc is obtained by integrating fromr = r_1totor = r_2:<br><br>:<br><br>R = \int_{r_1}^{r_2} \dfrac{dr}{2\pi K r d} = \dfrac{1}{2\pi K d} \ln \left(\dfrac{r_2}{r_1}\right)

The rate of heat flow is given by H=H =\dfrac{\Delta \theta}{R}, where Δθ=θ1−θ2\Delta \theta = \theta_1 - \theta_2.

H=H =\dfrac{\theta_1 - \theta_2}{\dfrac{1}{2\pi K d} \ln\left(\dfrac{r_2}{r_1}\right)} = \dfrac{2\pi K d (\theta_1 - \theta_2)}{\ln(r_2 / r_1)}
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