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JEE Advanced 2021 Paper 2 · Physics · Simple Harmonic Motion · medium

JEE Advanced 2021 Paper 2 Physics: Paragraph 1

A block of mass 2 kg2\ \mathrm{kg} is attached to a horizontal spring of force constant 200 N m−1200\ \mathrm{N\,m^{-1}} and executes simple harmonic motion with amplitude 10 cm10\ \mathrm{cm} on a smooth horizontal table. At the instant the block is 5 cm5\ \mathrm{cm} from the equilibrium position and moving away from it, a lump of putty of mass 2 kg2\ \mathrm{kg}, falling vertically with negligible horizontal velocity, lands on the block and sticks to it. The surface remains smooth.

Question 1

Single correct option

The new amplitude of oscillation of the combined system is closest to
  1. A. 7.07 cm7.07\ \mathrm{cm}
  2. B. 7.91 cm7.91\ \mathrm{cm}
  3. C. 8.66 cm8.66\ \mathrm{cm}
  4. D. 10.0 cm10.0\ \mathrm{cm}
Show answer and solution

Answer: (B) 7.91 cm7.91\ \mathrm{cm}

Just before the collision, ω=k/m=10 rad s−1\omega=\sqrt{k/m}=10\ \mathrm{rad\,s^{-1}} and at x=5x=5 cm the speed is v=ωA2−x2=10×0.0866=0.866 m s−1v=\omega\sqrt{A^2-x^2}=10\times0.0866=0.866\ \mathrm{m\,s^{-1}}. The putty has no horizontal momentum, so horizontal momentum conservation gives v′=24v=0.433 m s−1v'=\tfrac{2}{4}v=0.433\ \mathrm{m\,s^{-1}}, while the position x=5x=5 cm is unchanged. The new angular frequency is ω′=200/4=7.07 rad s−1\omega'=\sqrt{200/4}=7.07\ \mathrm{rad\,s^{-1}}. The new total energy is 12kx2+12Mv′2=0.25+0.375=0.625 J\tfrac12kx^2+\tfrac12Mv'^2=0.25+0.375=0.625\ \mathrm{J}, and equating to 12kA′2\tfrac12kA'^2 gives A′=2×0.625/200=0.0791 m=7.91 cmA'=\sqrt{2\times0.625/200}=0.0791\ \mathrm{m}=7.91\ \mathrm{cm}. The value 7.077.07 cm results from wrongly assuming the collision happens at the mean position, and 8.668.66 cm is the pre-collision speed-based amplitude A2−x2\sqrt{A^2-x^2}.

Question 2

Single correct option

The maximum speed of the block after the putty sticks is closest to
  1. A. 0.43 m s−10.43\ \mathrm{m\,s^{-1}}
  2. B. 0.50 m s−10.50\ \mathrm{m\,s^{-1}}
  3. C. 0.56 m s−10.56\ \mathrm{m\,s^{-1}}
  4. D. 0.87 m s−10.87\ \mathrm{m\,s^{-1}}
Show answer and solution

Answer: (C) 0.56 m s−10.56\ \mathrm{m\,s^{-1}}

After the collision the system is a mass M=4 kgM=4\ \mathrm{kg} on the same spring, with total mechanical energy E=12kx2+12Mv′2E=\tfrac12kx^2+\tfrac12Mv'^2 where x=0.05 mx=0.05\ \mathrm{m} and v′=0.433 m s−1v'=0.433\ \mathrm{m\,s^{-1}}. Thus E=12(200)(0.0025)+12(4)(0.1875)=0.25+0.375=0.625 JE=\tfrac12(200)(0.0025)+\tfrac12(4)(0.1875)=0.25+0.375=0.625\ \mathrm{J}. The block is fastest at the equilibrium position, where all this energy is kinetic: 12Mvmax2=0.625\tfrac12Mv_{max}^2=0.625, giving vmax=2×0.625/4=0.3125=0.559 m s−1v_{max}=\sqrt{2\times0.625/4}=\sqrt{0.3125}=0.559\ \mathrm{m\,s^{-1}}. Equivalently vmax=ω′A′=7.07×0.0791=0.559 m s−1v_{max}=\omega'A'=7.07\times0.0791=0.559\ \mathrm{m\,s^{-1}}. The value 0.430.43 is the speed immediately after the collision, which is not the maximum, and 0.870.87 is the speed before sticking. Hence option (C) is the only one consistent with energy conservation after the sticking collision; the energy lost in the inelastic collision is irrelevant for what follows.
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