Elastic Collisions

Physics
NEET UG
Version 1Updated 22 Mar 2026

An elastic collision is a type of collision in which the total kinetic energy of the system of colliding bodies is conserved, in addition to the conservation of total linear momentum. This implies that there is no net loss of kinetic energy in the form of heat, sound, or permanent deformation during the collision process. While kinetic energy may temporarily convert into potential energy of deform…

Quick Summary

Elastic collisions are fundamental interactions where two key quantities are conserved: total linear momentum and total kinetic energy. This means that the 'push' and the 'energy of motion' of the system remain unchanged before and after the collision.

While momentum conservation applies to all collisions (elastic or inelastic), kinetic energy conservation is the defining characteristic of an elastic collision. In such collisions, objects deform temporarily during contact but fully regain their original shape, ensuring no permanent energy loss to heat, sound, or deformation.

The coefficient of restitution, a measure of 'bounciness', is exactly 1 for elastic collisions. Key scenarios include one-dimensional head-on collisions, where specific formulas predict final velocities based on masses and initial velocities.

Special cases, like equal masses exchanging velocities or a light object bouncing off a heavy one, are particularly important for NEET. Though idealizations in the macroscopic world, elastic collisions are crucial models in microscopic physics.

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Key Concepts

Conservation Laws in 1D Elastic Collisions

In a one-dimensional elastic collision between two bodies, say m1m_1 and m2m_2, with initial velocities u1u_1

Special Case: Equal Masses and One at Rest

When two bodies of equal mass (m1=m2=mm_1 = m_2 = m) undergo a 1D elastic collision, and one of them is initially…

Special Case: Light Body Colliding with Massive Body at Rest

Consider a very light body (m1m_1) colliding elastically with a much heavier body (m2m_2) that is initially…

  • Definition:Total linear momentum and total kinetic energy are conserved.
  • Coefficient of Restitution:e=1e=1.
  • 1D Momentum Conservation:m1u1+m2u2=m1v1+m2v2m_1 u_1 + m_2 u_2 = m_1 v_1 + m_2 v_2
  • 1D Kinetic Energy Conservation:rac12m1u12+12m2u22=12m1v12+12m2v22rac{1}{2} m_1 u_1^2 + \frac{1}{2} m_2 u_2^2 = \frac{1}{2} m_1 v_1^2 + \frac{1}{2} m_2 v_2^2
  • Relative Velocity Relation:u1u2=v2v1u_1 - u_2 = v_2 - v_1 (relative speed of approach = relative speed of separation)
  • Final Velocities (General 1D):

- v_1 = left(\frac{m_1 - m_2}{m_1 + m_2}\right)u_1 + left(\frac{2m_2}{m_1 + m_2}\right)u_2 - v_2 = left(\frac{2m_1}{m_1 + m_2}\right)u_1 + left(\frac{m_2 - m_1}{m_1 + m_2}\right)u_2

  • Special Case ($m_1=m_2, u_2=0$):v1=0,v2=u1v_1=0, v_2=u_1 (velocities exchange)
  • Special Case ($m_1 ll m_2, u_2=0$):v1approxu1,v2approx0v_1 approx -u_1, v_2 approx 0 (light body bounces back, heavy body at rest)
  • Special Case ($m_1 gg m_2, u_2=0$):v1approxu1,v2approx2u1v_1 approx u_1, v_2 approx 2u_1 (heavy body continues, light body moves with double speed)

For Elastic Collisions, remember 'MKE': Momentum is conserved. Kinetic energy is conserved. Equals 1 (Coefficient of Restitution, e=1e=1).

And for the relative velocities: 'Approach = Separation' (u1u2=v2v1u_1 - u_2 = v_2 - v_1).

For equal masses, 'Swap Speeds!'

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