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JEE Main 201419 AprilOnline
Exam
JEE Main
Year
2014
Date
19 April
Mode
Online
Subject
Physics
Chapter
Thermal Properties of Matter

JEE Main 2014 · 19 April · Online · Physics · Thermal Properties of Matter

A black coloured solid sphere of radius R and mass M is inside a...

A black coloured solid sphere of radius RR and mass MM is inside a cavity with a vacuum inside. The walls of the cavity are maintained at temperature T0{T}_{0}. The initial temperature of the sphere is 3T03{T}_{0}. If the specific heat of the material of the sphere varies as αT3\alpha{T}^{3} per unit mass with the temperature TT of the sphere, where α\alpha is a constant, then the time taken for the sphere to cool down to temperature 2T02{T}_{0} will be

(σ\sigma is Stefan Boltzmann constant)

A black coloured solid sphere of radius R and mass M is inside a cavity with a vacuum inside. The walls of the cavity

Options

  1. AMα16πR2σln⁡(32)\dfrac{M\alpha}{16\pi{R}^{2}\sigma}\ln \left(\dfrac{3}{2}\right)
  2. BMα16πR2σln⁡(163)\dfrac{M\alpha}{16\pi{R}^{2}\sigma}\ln \left(\dfrac{16}{3}\right)
  3. CMα4πR2σln⁡(32)\dfrac{M\alpha}{4\pi{R}^{2}\sigma}\ln \left(\dfrac{3}{2}\right)
  4. DMα4πR2σln⁡(163)\dfrac{M\alpha}{4\pi{R}^{2}\sigma}\ln \left(\dfrac{16}{3}\right)

Correct answer

B. Mα16πR2σln⁡(163)\dfrac{M\alpha}{16\pi{R}^{2}\sigma}\ln \left(\dfrac{16}{3}\right)

Step-by-step solution

\dfrac{d\theta}{dt} = - \dfrac{\sigmaAe}{Ms}\left({\theta}^{4} - {\theta}_{0}^{4}\right)<br/><br/><imgalt=""src="https://cdn−question−pool.getmarks.app/pyq/jeemain/445148556545.png"style="width:200px;height:400px;"/><br/><br/><br /><br /><img alt="" src="https://cdn-question-pool.Quantrex.app/pyq/jee_main/445148556545.png" style="width: 200px; height: 400px;" /><br /><br />\dfrac{d\theta}{dt} = - \dfrac{\sigmaAe}{M\alpha{\theta}^{3}}\left({\theta}^{4} - {\theta}_{0}^{4}\right)</p><p></p><p>∫ \dfrac{{\theta}^{3}}{\left({\theta}^{4} - {\theta}_{0}^{4}\right)}d\theta = - \dfrac{\sigmaAe}{M\alpha} ∫ dt</p><p>Let(θ4−θ04)=x</p><p>Let \left({\theta}^{4} - {\theta}_{0}^{4}\right) = x

4θ3dθ=dx4{\theta}^{3}d\theta = dx

∫dx4x=−\sigmaAeMα[t]0t∫ \dfrac{dx}{4x} = - \dfrac{\sigmaAe}{M\alpha}{\left[t\right]}_{0}^{t}

14[ln⁡x]=M\sigmaAeMα[t]0t\dfrac{1}{4}\left[\ln x\right] = \dfrac{M\sigmaAe}{M\alpha}{\left[t\right]}_{0}^{t}

14[ln⁡(θ4−θ04)]\dfrac{1}{4}\left[\ln \left({\theta}^{4} - {\theta}_{0}^{4}\right)\right]2T03T0\begin{array}{ll}2{T}_{0} \\ 3{T}_{0}\end{array}=−\sigmaAeMαt= - \dfrac{\sigmaAe}{M\alpha}t

14ln⁡((2T0)4−T04(3T0)4−T04)=−\sigmaAeMαt\dfrac{1}{4}\ln \left(\dfrac{{\left(2{T}_{0}\right)}^{4} - {T}_{0}^{4}}{{\left(3{T}_{0}\right)}^{4} - {T}_{0}^{4}}\right) = - \dfrac{\sigmaAe}{M\alpha}t

t=−\alphaM4\sigmaAeln⁡(15T0480T04)t = - \dfrac{\alphaM}{4\sigmaAe}\ln \left(\dfrac{15{T}_{0}^{4}}{80{T}_{0}^{4}}\right)

=−\alphaM4\sigmaAeln⁡(316)= - \dfrac{\alphaM}{4\sigmaAe}\ln \left(\dfrac{3}{16}\right)

=−\alphaM4σ(4πR2)eln⁡(316)= - \dfrac{\alphaM}{4\sigma\left(4\pi{R}^{2}\right)e}\ln \left(\dfrac{3}{16}\right) where e=1e = 1

t=\alphaM16πσR2ln⁡(163)t = \dfrac{\alphaM}{16\pi\sigma{R}^{2}}\ln \left(\dfrac{16}{3}\right)

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