Thermal Properties of Matter

JEE Main level, single correct, medium

120 of 126

Question 120 of 126

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)

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

dθdt=−σAeMs(θ4−θ04)\dfrac{d\theta }{dt}=-\dfrac{\sigma Ae}{Ms}\left({\theta }^{4}-{\theta }_{0}^{4}\right)



dθdt=−σAeMαθ3(θ4−θ04)\dfrac{d\theta }{dt}=-\dfrac{\sigma Ae}{M\alpha {\theta }^{3}}\left({\theta }^{4}-{\theta }_{0}^{4}\right)
∫θ3(θ4−θ04)dθ=−σAeMα∫dt\int \dfrac{{\theta }^{3}}{\left({\theta }^{4}-{\theta }_{0}^{4}\right)}d\theta =-\dfrac{\sigma Ae}{M\alpha }\int dt
Let
(θ4−θ04)=x\left({\theta }^{4}-{\theta }_{0}^{4}\right)=x
4θ3dθ=dx4{\theta }^{3}d\theta =dx
∫dx4x=−σAeMα[t]0t\int \dfrac{dx}{4x}=-\dfrac{\sigma Ae}{M\alpha }{\left[t\right]}_{0}^{t}
14[ln⁡x]=MσAeMα[t]0t\dfrac{1}{4}\left[\ln x\right]=\dfrac{M\sigma Ae}{M\alpha }{\left[t\right]}_{0}^{t}
14[ln⁡(θ4−θ04)]2T03T0=−σAeMαt\dfrac{1}{4}\left[\ln \left({\theta }^{4}-{\theta }_{0}^{4}\right)\right]\begin{matrix}2{T}_{0} \\ 3{T}_{0}\end{matrix}=-\dfrac{\sigma Ae}{M\alpha }t
14ln⁡((2T0)4−T04(3T0)4−T04)=−σAeMαt\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{\sigma Ae}{M\alpha }t
t=−αM4σAeln⁡(15T0480T04)t=-\dfrac{\alpha M}{4\sigma Ae}\ln \left(\dfrac{15{T}_{0}^{4}}{80{T}_{0}^{4}}\right)
=−αM4σAeln⁡(316)=-\dfrac{\alpha M}{4\sigma Ae}\ln \left(\dfrac{3}{16}\right)
=−αM4σ(4πR2)eln⁡(316)=-\dfrac{\alpha M}{4\sigma \left(4\pi {R}^{2}\right)e}\ln \left(\dfrac{3}{16}\right) where e=1e=1
t=αM16πσR2ln⁡(163)t=\dfrac{\alpha M}{16\pi \sigma {R}^{2}}\ln \left(\dfrac{16}{3}\right)

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