3.3

linear momentum and its conservation

principle of conservation of momentum

in an isolated system where no external resultant force acts, the total momentum remains constant.

  • momentum is a vector quantity
  • direction must be considered when solving problems
  • total momentum before a collision equals total momentum after the collision

total momentum before = total momentum after

collisions

in any collision, momentum is conserved provided the system is isolated.

two-object collision (one dimension)

  • consider motion along a straight line
  • choose one direction as positive
  • assign signs carefully to velocities

if two objects of masses m₁ and m₂ have initial velocities u₁ and u₂, and final velocities v₁ and v₂:

m₁u₁ + m₂u₂ = m₁v₁ + m₂v₂

momentum and impulse

  • impulse is the product of force and the time for which it acts
  • impulse equals the change in momentum

impulse = FΔt = Δp

  • unit: N s
  • 1 N s = 1 kg m s⁻¹

elastic and inelastic collisions

collisions are classified based on what happens to kinetic energy.

perfectly elastic collision

  • momentum is conserved
  • kinetic energy is conserved
  • relative speed of approach equals relative speed of separation

inelastic collision

  • momentum is conserved
  • kinetic energy is not conserved
  • some kinetic energy is converted to heat, sound, or deformation

energy in collisions

total kinetic energy before collision:

½m₁u₁² + ½m₂u₂²

total kinetic energy after collision:

½m₁v₁² + ½m₂v₂²

in a perfectly elastic collision:

½m₁u₁² + ½m₂u₂² = ½m₁v₁² + ½m₂v₂²

even when kinetic energy is not conserved, total energy and total momentum are always conserved in an isolated system.