Physic Labs

Newtonian mechanics

Elastic collisions

Verify momentum and kinetic-energy conservation in a one-dimensional collision with adjustable restitution ee. Measure velocities before and after, checking m1u1+m2u2=m1v1+m2v2m_1u_1 + m_2u_2 = m_1v_1 + m_2v_2 and e=(v2−v1)/(u1−u2)e = (v_2 - v_1)/(u_1 - u_2).

High school

Equipment

  • Two virtual carts on a frictionless track
  • Sliders for m₁, m₂, u₁, u₂ and restitution e
  • Readouts for post-collision velocities and total momentum

Procedure

  1. Set up the collision and measure velocities

    Set "Restitution e" to 1.00 (ideal elastic). Choose m₁ = 2 kg, m₂ = 3 kg, u₁ = 5 m/s, u₂ = −1 m/s, watch the collision and read v₁, v₂ in the "After collision" readout. Compute PP before/after and confirm momentum conservation.

  2. Check kinetic-energy conservation

    With the same data, compute K=12m1u12+12m2u22K = \frac{1}{2}m_1u_1^2 + \frac{1}{2}m_2u_2^2 before and after; for e=1e = 1 the two values are equal. Change m₂ so v₂ shifts while PP stays conserved. Verify the formula v1=m1−m2m1+m2u1+2m2m1+m2u2v_1 = \frac{m_1 - m_2}{m_1+m_2}u_1 + \frac{2m_2}{m_1+m_2}u_2 for the e=1e = 1 case.

  3. Scan the restitution coefficient

    Lower e to 0.5 then 0 and repeat the collision. Check e=(v2−v1)/(u1−u2)e = (v_2 - v_1)/(u_1 - u_2) with the new readings: separation speed scales with e. At e=0e = 0 the bodies stick (perfectly inelastic) — compare with the "Inelastic collision" lab. Conclude which e conserves K and which converts K into heat/deformation.

Simulation

Experiment history

The collision problem challenged Descartes and his contemporaries. In 1668 the Royal Society announced a competition on collision laws; the three correct solutions came from John Wallis, Christopher Wren, and Christiaan Huygens — Wallis for soft bodies, Wren for hard elastic ones, Huygens using conservation of "vis viva" mv2mv^2, ancestor of kinetic energy. Newton systematized this in the Principia (1687) via the third law and "quantity of motion" ∑mivi\sum m_iv_i. In the 19th–20th centuries, momentum conservation was elevated by Emmy Noether into a consequence of spatial translation symmetry (1918) — the ideal elastic collision became the standard model of kinetic theory and scattering physics.

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