2013: Problem 18

Topic: System of Masses
Concepts: Conservation of angular momentum, Conservation of linear momentum, Dynamics of CM


Solution:

Since there are no external forces (and torques), we have conservation of linear momentum and angular momentum. The initial linear momentum is

pi=mvrmvr=0p_i=mvr-mvr=0

Since ptot=MtotvCMp_{\text{tot}}=M_{\text{tot}}v_{\text{CM}}, this means vCM=0v_{\text{CM}}=0 so the CM stays at rest at its initial location (1,0)(1, 0). Choosing (1,0)(1, 0) as our axis of rotation, the initial angular momentum is

Li=2mvr=2(1kg)(1m/s)(1m)=2kgm2/sL_i=2mvr=2(1\,\mathrm{kg})(1\,\mathrm{m/s})(1\,\mathrm{m})=2\,\mathrm{kg\,m^2/s}

going counterclockwise. We now go through the possible choices:

  • A) Not correct because the CM moved to (0,0)(0, 0).
  • B) Not correct because the linear momentum is nonzero.
  • C) Not correct because the angular momentum decreased (since the moment arm decreased by a factor of 2\sqrt{2}).
  • D) Not correct because the angular momentum increased (since the moment arm increased by a factor of 22).
  • E) Correct since linear momentum and angular momentum are conserved and the CM stayed at rest.

Thus, the answer is E.

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