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Question #42159

Difficulty: 8/10 | 🟢 Free

The Question

A thermally isolated radioactive sample of initial mass m0m_0 and constant specific heat capacity cc is placed in a vacuum at absolute zero. The sample generates heat at a rate Pin(t)=P0e−λtP_{\text{in}}(t) = P_0 e^{-\lambda t} due to radioactive decay, and its mass decreases as m(t)=m0e−λtm(t) = m_0 e^{-\lambda t}. The sample loses energy via Stefan-Boltzmann radiation from its constant surface area AA, such that Pout(t)=σAT4P_{\text{out}}(t) = \sigma A T^4. The temperature TT of the sample is governed by the energy balance Pin(t)=Pout(t)+m(t)cdTdtP_{\text{in}}(t) = P_{\text{out}}(t) + m(t) c \frac{dT}{dt}. If the initial temperature of the sample is 0 K0\text{ K}, what is the value of d2Tdt2\frac{d^2T}{dt^2} at t=0t=0?

Options

  • A.

    00

  • B.

    −λP0m0c- \frac{\lambda P_0}{m_0 c}

  • C.

    λ216(P0σA)1/4\frac{\lambda^2}{16} \left( \frac{P_0}{\sigma A} \right)^{1/4}

  • D.

    λP0m0c\frac{\lambda P_0}{m_0 c}

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Correct Answer

Step-by-Step Solution

Explanation

How the Examiner Thinks

Multi-Concept_Bridge

Master problems that require linking physics and math concepts to solve complex competitive questions.

Concepts Behind This Question

Stefan-Boltzmann Power Law|Radioactive Decay Law Dynamics|Differential Calculus

Why This Question Is Tricky

Common Mistakes

This question tests the student's ability to correctly set up and differentiate the energy balance equation for a system with time-varying mass and temperature.

The primary trap is treating the mass m0m_0 as a constant in the thermal capacity term mc(dT/dt)mc(dT/dt).

If a student forgets to apply the product rule to m(t)=m0e−λtm(t) = m_0 e^{-\lambda t}, they will miss the −λm0c(dT/dt)-\lambda m_0 c (dT/dt) term and incorrectly arrive at −λP0/(m0c)-\lambda P_0 / (m_0 c).

Another trap is assuming a quasi-steady state (Pin=PoutP_{\text{in}} = P_{\text{out}}), which ignores thermal inertia entirely.

By asking for the second derivative at t=0t=0, the problem elegantly bypasses an unsolvable non-linear integration while strictly enforcing the mathematical consequences of the decaying mass.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterThermal Properties of Matter - Class 11 Part 2
ConceptStefan-Boltzmann Power Law
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree