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Question #42868

Difficulty: 8/10 | 🟢 Free

The Question

Two identical satellites, S1S_1 and S2S_2, are located in deep space at 0 K0\text{ K}. Each contains an identical open organ pipe filled with an ideal diatomic gas. The pipes are continuously sounded at their fundamental frequencies. The walls of the pipes have a zero coefficient of thermal expansion, and the heat capacity of the gas is negligible. Satellite S1S_1 is maintained at a constant temperature T0T_0, emitting sound of frequency f0f_0 and constant acoustic intensity I0I_0. Satellite S2S_2 is initially at T0T_0. At t=0t=0, its heating system fails, and it cools by radiating as a perfect black body. S2S_2 has mass MM, specific heat capacity csc_s, and surface area AA. As S2S_2 cools, the local speed of sound drops, modulating the frequency f(t)f(t) of its pipe. Furthermore, the acoustic intensity I(t)I(t) of the pipe in S2S_2 is directly proportional to the absolute temperature of the gas (I(t)∝TI(t) \propto T). An observer counts the acoustic beats between the two pipes. However, the beat detection system automatically shuts off when the intensity I(t)I(t) from S2S_2 drops to I04\frac{I_0}{4}. Find the total number of beats registered by the observer from t=0t=0 until the detection system shuts off. (Assume σ\sigma is the Stefan-Boltzmann constant).

Options

  • A.

    43f0Mcs5σAT03\frac{43 f_0 M c_s}{5 \sigma A T_0^3}

  • B.

    21f0Mcs4σAT03\frac{21 f_0 M c_s}{4 \sigma A T_0^3}

  • C.

    129f0Mcs5σAT03\frac{129 f_0 M c_s}{5 \sigma A T_0^3}

  • D.

    5f0Mcs6σAT03\frac{5 f_0 M c_s}{6 \sigma A T_0^3}

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Correct Answer

Step-by-Step Solution

Explanation

How the Examiner Thinks

Variable_Constraint

Develop pure symbolic logic skills by mastering algebraic constraints without relying on numerical data.

Concepts Behind This Question

Beats and Frequency Difference|Stefan-Boltzmann Power Law|Wave Intensity and Medium

Why This Question Is Tricky

Common Mistakes

This question tests the coupling of thermodynamic cooling with acoustic wave properties, specifically targeting the misconception that beat frequency variations can be approximated linearly or evaluated using simple averages.

Students often fall into the trap of calculating the initial and final beat frequencies and multiplying their average by the total time (Option B).

Furthermore, it tests the correct application of the Stefan-Boltzmann law to find the time-dependent temperature profile T(t)∝(C+t)−1/3T(t) \propto (C + t)^{-1/3}, and recognizing that the speed of sound (and thus the fundamental frequency) scales with T\sqrt{T}.

The integration of the resulting non-linear beat frequency Δf(t)\Delta f(t) over the time interval defined by the intensity threshold rigorously filters out students who rely on kinematic shortcuts instead of setting up the proper differential relationships.

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Question Information

SubjectPhysics
ChapterWaves - Class 11 Part 2
ConceptBeats and Frequency Difference
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree