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Question #43690

Difficulty: 8/10 | 🟢 Free

The Question

A radioactive sample of instantaneous mass mm is attached to a light horizontal spring of spring constant kk. The system oscillates on a smooth horizontal surface in a viscous medium that exerts a drag force Fd=−cvF_d = -cv, where vv is the instantaneous velocity of the sample and cc is a positive constant. The sample undergoes radioactive decay with a decay constant λ\lambda, such that its mass decreases according to dmdt=−λm\frac{dm}{dt} = -\lambda m. The decay products are continuously ejected such that they are left completely stationary with respect to the horizontal surface. If E=12mv2+12kx2E = \frac{1}{2}mv^2 + \frac{1}{2}kx^2 represents the instantaneous mechanical energy of the oscillating sample, which of the following expressions gives the rate of change of this mechanical energy, dEdt\frac{dE}{dt}?

Options

  • A.

    (λm2−c)v2\left( \frac{\lambda m}{2} - c \right) v^2

  • B.

    −(λm2+c)v2-\left( \frac{\lambda m}{2} + c \right) v^2

  • C.

    −cv2-c v^2

  • D.

    (λm−c)v2\left( \lambda m - c \right) v^2

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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

Radioactive Decay Law Dynamics|Mechanical Energy Conservation|Integration

Why This Question Is Tricky

Common Mistakes

This question tests the application of Newton's Second Law to variable mass systems and its intersection with the Work-Energy Theorem.

Students commonly fall into the trap of writing Fnet=ma  ⟹  mdvdt=−kx−cvF_{net} = ma \implies m\frac{dv}{dt} = -kx - cv, ignoring the thrust force arising from the ejected mass.

This leads to the incorrect energy derivative −(λm2+c)v2-\left(\frac{\lambda m}{2} + c\right)v^2.

Another common mistake is assuming the rate of change of mechanical energy is simply the power of the non-conservative drag force (−cv2-cv^2), failing to account for the energy carried away by the lost mass and the work done by the thrust force.

The correct approach requires using mdvdt=Fext+ureldmdtm\frac{dv}{dt} = F_{ext} + u_{rel}\frac{dm}{dt} to properly account for the momentum transfer.

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Question Information

SubjectPhysics
ChapterNuclei - Class 12
ConceptRadioactive Decay Law Dynamics
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree