Elastic Collisions in Galilean Relativity

According to the principle of relativity, observers in inertial frames, moving at constant velocities relative to a fixed frame of reference, will experience the same laws of physics, although with different values of observables. In this Demonstration, we consider an observer moving at velocity relative to the center of mass of two particles undergoing an elastic collision. Different observers will disagree on the magnitudes of momenta and kinetic energy of the system, but they both will agree on the conservation of momentum and energy.
This Demonstration is based on Galilean relativity, which is an approximation to Einstein's special relativity, accurate only at speeds far slower than the speed of light. You can select the masses and of the two particles and their initial speeds and , as well as two components of the observer's velocity . This velocity vector is shown, along with the speed . The speeds and and the total kinetic energy are also shown on the graphic.


  • [Snapshot]
  • [Snapshot]
  • [Snapshot]


The momentum of an object is a vector quantity defined as for the object's mass and vector velocity . The kinetic energy of an object is a scalar quantity defined as , where is the speed. Both of these values, although they might vary from observer to observer, are seen as conserved in an elastic collision. Note that if other forces such as gravity or electromagnetism were acting on the system, the kinetic energy by itself would not be conserved, but, rather, the total energy of the system.
    • Share:

Embed Interactive Demonstration New!

Just copy and paste this snippet of JavaScript code into your website or blog to put the live Demonstration on your site. More details »

Files require Wolfram CDF Player or Mathematica.