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AP® Physics C: Mechanics · Unit 4 · Topic 4.1

Linear Momentum: Revision Notes (Physics C: Mechanics 4.1)

One-page recap of linear momentum for the calculus-based course: p = mv as a vector, system momentum by components, p(t) from x(t), K = p²/2m, and the collision and explosion models.

Short on time? This page is the recap for the calculus-based course (separate from Physics 1, which uses no calculus). For explanations, diagrams and worked examples, use the full study guide.

Recap

  • Linear momentum p = mv. Unit kg·m/s, the same as N·s.
  • Momentum is a vector with the direction of the velocity. In one dimension, p_x has the sign of v_x.
  • The momentum of a system is the vector sum of the momenta of its parts. Opposite momenta cancel; kinetic energies never do.
  • From a position function: p_x(t) = m dx/dt. The p–t graph is the v–t graph scaled by m.
  • A collision is an interaction where the forces between the objects are much larger than the net external force. Only the states just before and just after are compared, so each body can be modelled as an object.
  • An explosion is an interaction where internal forces push parts of the system apart.

Key relationships

Relationship Units Notes
p = mv kg·m/s vector, parallel to v
p_x = mv_x, p_y = mv_y kg·m/s work in components
|p| = √(p_x² + p_y²), tan θ = p_y/p_x kg·m/s, degrees check the quadrant from the signs
p_sys = p₁ + p₂ + … kg·m/s vector sum
p_x(t) = m dx/dt kg·m/s constant mass
K = p²/(2m), |p| = √(2mK) J, kg·m/s same p: lighter object has more K

Assumptions behind the numbers

  • Masses are constant unless a question says otherwise.
  • Velocities are measured in one inertial reference frame. Momentum depends on the frame, just as velocity does.
  • “Just before” and “just after” a collision means close enough in time that external forces have had no noticeable effect.

Mistakes to avoid

  1. Adding sizes of momenta. Add components with signs.
  2. Losing the sign of p_x when an object moves in −x.
  3. Wrong quadrant after an inverse tangent.
  4. Treating p and K as interchangeable. Doubling speed doubles p but quadruples K.
  5. Thinking zero total momentum means everything is at rest.
  6. Using the collision model when external forces act for a long time compared with the interaction.

Quick self-check

  1. Take +x east, +y north. A 0.30 kg ball moves with v = (4.0, −3.0) m/s. Find p and its size. (p = (1.2, −0.90) kg·m/s; size 1.5 kg·m/s, pointing south of east)
  2. A 1.5 kg cart has momentum of size 6.0 kg·m/s. What is its kinetic energy? (K = 6.0² ÷ (2 × 1.5) = 12 J)
  3. A 0.50 kg particle has x(t) = 2.0t² − t³ (x in m, t in s). What is p_x at t = 1.0 s? (v_x = 4.0t − 3t² = 1.0 m/s, so p_x = 0.50 kg·m/s)

Next: practice questions.

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