Physics

Conservation of Momentum

Collisions

Physics
NEET UG
Version 1Updated 22 Mar 2026

In physics, a collision is defined as an isolated event in which two or more bodies exert forces on each other for a relatively short period of time, leading to an exchange of momentum and energy. During a collision, the interacting bodies come into direct contact or exert strong forces over a small distance, causing their velocities to change significantly. The fundamental principle governing all…

Quick Summary

Collisions are brief, intense interactions between objects leading to changes in their motion. The most crucial principle is the Conservation of Linear Momentum, which states that for an isolated system, the total momentum before a collision equals the total momentum after.

Momentum is a vector quantity (p=mvp = mv). Collisions are classified based on what happens to kinetic energy.\n\nElastic collisions conserve both momentum and kinetic energy. The coefficient of restitution (ee) is 1.

Objects rebound without deformation. \n\nInelastic collisions conserve momentum but *not* kinetic energy; some kinetic energy is lost (converted to heat, sound, deformation). For these, 0<e<10 < e < 1.

A special case is perfectly inelastic collisions, where objects stick together and move as one, resulting in maximum kinetic energy loss, and e=0e=0.\n\nImpulse (J=FavgΔtJ = F_{avg} \Delta t) is the change in momentum (Δp\Delta p).

It quantifies the effect of force over time during the collision. For 2D collisions, momentum conservation must be applied component-wise (x and y directions). Understanding these types and principles is fundamental to solving collision problems in NEET.

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Key Concepts

Impulse-Momentum Theorem Application

The Impulse-Momentum Theorem, J=Δp\vec{J} = \Delta \vec{p}, is crucial for understanding the forces involved in…

Perfectly Inelastic Collision Calculation

In a perfectly inelastic collision, objects stick together after impact, moving with a common final velocity.…

Elastic Collision Velocity Formulas (1D)

For one-dimensional elastic collisions, specific formulas can be derived for the final velocities of the two…

  • Momentum:p=mv\vec{p} = m\vec{v} (vector quantity)\n- Impulse: J=Δp=FavgΔt\vec{J} = \Delta \vec{p} = \vec{F}_{avg} \Delta t\n- Conservation of Momentum: m1u1+m2u2=m1v1+m2v2m_1\vec{u}_1 + m_2\vec{u}_2 = m_1\vec{v}_1 + m_2\vec{v}_2 (always conserved in isolated system)\n- Elastic Collision: Momentum conserved, Kinetic Energy conserved (e=1e=1)\n - 1D Equal Masses: Velocities exchanged (v1=u2,v2=u1v_1=u_2, v_2=u_1)\n - 1D General: v1=(m1m2)u1+2m2u2m1+m2v_1 = \frac{(m_1 - m_2)u_1 + 2m_2u_2}{m_1 + m_2}, v2=(m2m1)u2+2m1u1m1+m2v_2 = \frac{(m_2 - m_1)u_2 + 2m_1u_1}{m_1 + m_2}\n- Inelastic Collision: Momentum conserved, Kinetic Energy NOT conserved (0<e<10 < e < 1)\n- Perfectly Inelastic Collision: Momentum conserved, Kinetic Energy NOT conserved (max loss), objects stick (e=0e=0)\n - 1D: m1u1+m2u2=(m1+m2)Vm_1u_1 + m_2u_2 = (m_1 + m_2)V\n- Coefficient of Restitution (e): e=(v2v1)(u2u1)e = -\frac{(v_2 - v_1)}{(u_2 - u_1)} or e=relative speed of separationrelative speed of approache = \frac{\text{relative speed of separation}}{\text{relative speed of approach}}\n- Bouncing Ball: e=hrebound/hdrope = \sqrt{h_{rebound}/h_{drop}}

MEPI: Momentum Everywhere, Perfectly Inelastic sticks, Elastic Energy too. (Momentum is conserved in Every collision. Perfectly Inelastic collisions mean objects stick together. Elastic collisions conserve Energy, in addition to momentum.)

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