Physic Labs

Newtonian mechanics

Inelastic collisions

Study the perfectly inelastic collision: two bodies stick together after impact. Verify momentum conservation V=(m1u1+m2u2)/(m1+m2)V = (m_1u_1 + m_2u_2)/(m_1 + m_2) and measure the kinetic energy converted to internal energy ΔK=Kbefore−Kafter\Delta K = K_{before} - K_{after}.

High school

Equipment

  • Two virtual carts that stick together on a track
  • Sliders for m₁, m₂, u₁, u₂ and interaction time
  • Readouts of P and K before/after the collision

Procedure

  1. Measure momentum before impact

    Set m₁ = 2 kg, m₂ = 3 kg, u₁ = 4 m/s, u₂ = −1 m/s. Before running, read "P before" and "K before", compute by hand P=m1u1+m2u2=5P = m_1u_1 + m_2u_2 = 5 kg·m/s and KbeforeK_{before}. Adjust "Interaction time" to see the collision play out fast or slow.

  2. Verify the common velocity

    Watch the two carts stick and read the post-collision velocity. Compare with the prediction V=m1u1+m2u2m1+m2=55=1V = \frac{m_1u_1 + m_2u_2}{m_1+m_2} = \frac{5}{5} = 1 m/s. Repeat with different m₂ and check the formula — P is conserved even though K is not.

  3. Compute the lost energy

    Read "K after" and compute ΔK=Kbefore−Kafter\Delta K = K_{before} - K_{after}: this is the part turned into heat, sound, and deformation. For e=0e = 0 one can show ΔK=12m1m2m1+m2(u1−u2)2\Delta K = \frac{1}{2}\frac{m_1m_2}{m_1+m_2}(u_1-u_2)^2 — the entire kinetic energy of relative motion is lost. Vary u₂ to see ΔK\Delta K follow the squared velocity difference.

Simulation

Experiment history

Inelastic collisions figured early in the 17th-century debate over "vis viva": Leibniz argued that mv2mv^2 is the conserved quantity while the Cartesians held to mvmv. John Wallis (1668) gave the solution for soft bodies — after impact both share the velocity V=∑miui/∑miV = \sum m_iu_i/\sum m_i, i.e., the center-of-mass velocity. The apparent "disappearance" of kinetic energy puzzled physicists until thermodynamics arrived: Joule and Mayer (1840s) showed energy is not lost but converted into heat. Today the ballistic pendulum — a bullet embedding in a suspended wood block — is the classic application for measuring muzzle velocity, invented by Benjamin Robins in 1742.

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