2008: Problem 22

Topic: Collisions
Concepts: Ballistic pendulum, Circular motion, Forces in mechanics


Solution:

By conservation of linear momentum,

m1v0=(m1+m2)vbm_1v_0=(m_1+m_2)v_b
vb=m1m1+m2v0v_b=\frac{m_1}{m_1+m_2}v_0

We conserve energy between the bottom and top of the vertical circle,

12(m1+m2)vb2=12(m1+m2)vt2+2(m1+m2)gL\frac{1}{2}(m_1+m_2)v_b^2=\frac{1}{2}(m_1+m_2)v_t^2+2(m_1+m_2)gL
vb2=vt2+4gLv_b^2=v_t^2+4gL

The minimum velocity at the top of the vertical circle is attained when the tension in the string goes to zero. Only gravity provides the centripetal acceleration so

mg=mvt2Lmg=\frac{mv_t^2}{L}
vt2=gLv_t^2=gL

Substituting this into the equation for vbv_b,

vb2=5gLv_b^2=5gL
m1m1+m2v0=5gL\frac{m_1}{m_1+m_2}v_0=\sqrt{5gL}
v0=(m1+m2)5gLm1v_0=\frac{(m_1+m_2)\sqrt{5gL}}{m_1}

so the answer is E.

Leave a Reply

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

Join 259 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