A particle of mass \( m \) moving with velocity \( v \) collides with a stationary particle of mass \( 2m \). After the collision, they stick together and continue to move with velocity:
Show Hint
For completely inelastic collisions (when objects stick together after collision), use:
\[
m_1 v_1 + m_2 v_2 = (m_1 + m_2) V_f
\]
where \( V_f \) is the common velocity after collision.
Step 1: Applying the Law of Conservation of Momentum.
The total momentum before collision is:
\[
P_{{initial}} = m v + (2m \times 0) = m v
\]
Since the two masses stick together after collision, their combined mass is:
\[
M = m + 2m = 3m
\]
Let the final velocity be \( V_f \). According to conservation of momentum:
\[
m v = (3m) V_f
\]
Step 2: Solving for \( V_f \).
\[
V_f = \frac{m v}{3m} = \frac{v}{3}
\]
Final Answer:
\[
\boxed{\frac{v}{3}}
\]