2016: Problems 21-22

Topic: System of Masses
Concepts: Center of mass, Dynamics of CM


Solution:

There are no external forces on the system in the horizontal direction. Thus, the CM does not move in the horizontal direction. Setting the final position of mm as the origin, the CM is located a distance

x=m(0)+3m(L)m+3m=3L4x=\frac{m(0)+3m(L)}{m+3m}=\frac{3L}{4}

to the left. Thus, the answer is A.

Topic: System of Masses
Concepts: Conservation of energy, Velocity constraints


Solution:

Just before the top ball hits the ground, it is moving directly downward. This is because if it had a velocity component parallel to the rod, then the bottom ball would also have the same parallel component to keep the rod length fixed. But the system would then violate conservation of momentum.

Thus, the bottom ball is at rest in the end and the top ball has all the kinetic energy. Conserving energy from the beginning,

mgL=12mv2mgL=\frac{1}{2}mv^2
v=2gLv=\sqrt{2gL}

so the answer is A.

Leave a Reply

This site uses Akismet to reduce spam. Learn how your comment data is processed.

Join 261 other subscribers

F=ma Training Program
Group (2026)
Individual (2026)

1D elastic collision 1D inelastic collision 5 kinematics equations Angular kinematics Atwood machine Buoyant force Circular motion Circular orbits Conservation of angular momentum Conservation of energy Conservation of linear momentum Dimensional analysis Effective spring constant Elliptical orbits Energy dissipation Error propagation Fictitious forces Fma: Collisions Fma: Dynamics Fma: Energy Fma: Fluids Fma: Gravity Fma: Kinematics Fma: Oscillatory Motion Fma: Other Fma: Rigid Bodies Fma: System of Masses Forces in mechanics Free fall Inclined plane Kinetic energy Limiting cases Mass-spring system Moments of inertia Motion graphs Newton's laws Power Projectile motion Relative velocity Rolling motion Simple harmonic motion Statics Torque Torque from weight Work-energy theorem

Discover more from Kevin S. Huang

Subscribe now to keep reading and get access to the full archive.

Continue reading