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Linear Momentum, Impulse, and Collisions

Momentum becomes especially powerful when forces are large, complicated, and short-lived — collisions, explosions, catches, impacts.

Force-time curves with equal impulse areas and before-after momentum vectors for a cart collision.
Local explanatory diagram

Linear momentum is:

p⃗ = mv⃗.

It is a vector.

Impulse changes momentum

Newton's second law can be written:

F⃗net=frac{dp⃗{dt}.

Integrating over time:

J⃗ = ∈t F⃗ dt = Δp⃗.

For an approximately constant force:

J⃗ ≈ F⃗avgΔt.

The area under a force-versus-time graph is therefore impulse.

Why airbags and crumple zones help

To stop a person, their momentum must change.

For the same Δp:

Favg ≈ Δp/Δt.

Increasing the stopping time reduces the average force.

That is the mechanical idea behind airbags, padding and vehicle crumple zones. They do not eliminate the required momentum change; they spread it over more time and often more distance.

Conservation of momentum

For a chosen system:

Δp⃗system = J⃗external.

If external impulse is negligible:

p⃗before=p⃗after.

Internal collision forces can be enormous and momentum can still be conserved, because the internal interaction forces exchange momentum within the system.

Collision types

Elastic collision

  • momentum conserved
  • kinetic energy conserved

Inelastic collision

  • momentum conserved for an isolated system
  • kinetic energy is not conserved as kinetic energy

Perfectly inelastic collision

  • objects stick together afterward

Kinetic energy that disappears from the translational bookkeeping may become deformation, sound, thermal energy, vibration, rotation, or other internal energy.

Center of mass

For particles:

r⃗꜀M=
Σᵢ mᵢr⃗ᵢ/Σᵢ mᵢ.

The center of mass of a system responds to net external force as though the total mass were concentrated there for translational motion:

F⃗ext=Ma⃗꜀M.

This is why an exploding firework's fragments can fly in many directions while the system's center of mass continues along the trajectory determined by external forces.

Example: catching a ball

A 0.15 kg baseball moving at 40 m/s has momentum magnitude:

p=mv=6.0 kg m/s.

Stopping it in 0.010 s requires an average force magnitude around:

F≈6.0/0.010=600 N.

If the glove and arm move backward so stopping takes 0.050 s:

F≈120 N.

Same momentum change; five times the stopping time; one fifth the average force.

Physics C bridge

The force-time graph idea becomes exact through:

Δp⃗ = ∈t F⃗ext dt.

Calculus also makes variable-mass and continuous-system mechanics possible, although those are beyond the normal AP Physics C: Mechanics core.

Takeaway: Momentum is the natural bookkeeping quantity for interactions over time.

part of

sources

College Board — AP Physics 1 Course and Exam DescriptionOpenStax College Physics 2e — Linear MomentumOpenStax University Physics Volume 1