AcademyMomentum Systems

Academy

Collisions as Momentum Problems

Level 1 - Physics topic page in Momentum Systems.

Principle

A collision is a short interaction where momentum is modeled before kinetic energy.

Notation

\(m_1,m_2\)
colliding masses
\(\mathrm{kg}\)
\(u_1,u_2\)
initial velocities
\(\mathrm{m\,s^{-1}}\)
\(v_1,v_2\)
final velocities
\(\mathrm{m\,s^{-1}}\)
\(\vec{J}_{12}\)
impulse on 1 by 2
\(\mathrm{N\,s}\)
\(K\)
kinetic energy
\(\mathrm{J}\)

Method

During a short collision, internal impulses can be large while external impulse is often negligible.

Choose interval
\[\Delta t_{\mathrm{collision}}\ \text{is short}\]
Neglect external impulse
\[\Delta\vec{P}_{\mathrm{system}}\approx\vec{0}\]
Write momentum
\[m_1u_1+m_2u_2=m_1v_1+m_2v_2\]
Check energy
\[\Delta K=K_f-K_i\]
Use this as a classification check unless the collision is specified elastic.

The diagram compares the total momentum immediately before and after the short interaction.

-1012345-1012pxstatePiPfbeforeafter
The momentum equation compares the total signed momentum immediately before and immediately after the short interaction.

The before-after momentum vectors match for an isolated collision, but kinetic energy may not.

Rules

These are the compact one-dimensional collision relations.

Momentum equation
\[m_1u_1+m_2u_2=m_1v_1+m_2v_2\]
Sticking collision
\[m_1u_1+m_2u_2=(m_1+m_2)v_f\]
Impulse pair
\[\vec{J}_{12}=-\vec{J}_{21}\]
Energy change
\[\Delta K=K_f-K_i\]

Examples

Question
A
\[0.80\,\mathrm{kg}\]
cart moving at
\[5.0\,\mathrm{m\,s^{-1}}\]
sticks to a
\[1.2\,\mathrm{kg}\]
cart at rest. Find final speed.
Answer
\[0.80(5.0)=(0.80+1.2)v_f\]
\[v_f=2.0\,\mathrm{m\,s^{-1}}\]

Checks

  • Momentum conservation is the default collision equation for an isolated pair.
  • Kinetic energy is conserved only for elastic collisions.
  • A stuck-together final state is not elastic.
  • Short collision time does not remove large internal impulses.