Inelastic collisions Knowledge-Based Study

Physics · Momentum · Physics · Conservation of Momentum & Collisions

Physics topic explanations on Inelastic collisions.

Study notes

  1. What is an Inelastic Collision?

    In physics, a collision between two or more bodies is classified based on whether mechanical kinetic energy is conserved during the interaction.

    For any isolated system with no net external forces (∑F⃗ext=0\sum \vec{F}_{\text{ext}} = 0), total linear momentum is always conserved:

    p⃗initial=p⃗final\vec{p}_{\text{initial}} = \vec{p}_{\text{final}}

    An inelastic collision is defined as a collision in which the total linear momentum is conserved, but the total kinetic energy is not conserved (Kf<KiK_f < K_i).

    The lost kinetic energy does not vanish; rather, it is transformed into other energy forms such as:

    • Thermal energy (heat generated during the collision)
    • Acoustic energy (sound waves)
    • Work done in permanent structural or plastic deformation of the colliding objects

    Objects Sticking Together

    A completely (or perfectly) inelastic collision represents the extreme case of an inelastic interaction. In this scenario, the colliding bodies stick together upon impact and move forward with a single, shared final velocity (v⃗f\vec{v}_f).

    Consider two masses, m1m_1 and m2m_2, moving along a straight line with initial velocities v1iv_{1i} and v2iv_{2i}:

    m1v1i+m2v2i=(m1+m2)vfm_1 v_{1i} + m_2 v_{2i} = (m_1 + m_2) v_f

    Solving directly for the common final velocity yields:

    vf=m1v1i+m2v2im1+m2v_f = \frac{m_1 v_{1i} + m_2 v_{2i}}{m_1 + m_2}

    Note: Velocities are directional vector quantities. Motion in the chosen negative direction must be entered with a negative sign.

    Quantifying Energy Dissipation

    Although total energy is universally conserved, mechanical kinetic energy decreases in an inelastic event. The change in kinetic energy (ΔK\Delta K) is given by:

    ΔK=Kf−Ki\Delta K = K_f - K_i

    For a completely inelastic collision in one dimension:

    • Initial Kinetic Energy: Ki=12m1v1i2+12m2v2i2K_i = \frac{1}{2}m_1 v_{1i}^2 + \frac{1}{2}m_2 v_{2i}^2
    • Final Kinetic Energy: Kf=12(m1+m2)vf2K_f = \frac{1}{2}(m_1 + m_2) v_f^2

    Because Kf<KiK_f < K_i, ΔK\Delta K is negative. The absolute value ∣ΔK∣|\Delta K| corresponds precisely to the internal energy increase, deformation work, and thermal energy produced by the impact.

    Solving Collision Problems

    1. Identify the system: Confirm that external forces are negligible over the brief duration of the collision so that momentum conservation holds.
    2. Establish a coordinate axis: Assign positive and negative signs consistently according to direction of motion.
    3. Set up momentum conservation: Write m1v1i+m2v2i=m1v1f+m2v2fm_1 v_{1i} + m_2 v_{2i} = m_1 v_{1f} + m_2 v_{2f}. If the objects stick together, set v1f=v2f=vfv_{1f} = v_{2f} = v_f.
    4. Analyze energy if required: Calculate KiK_i and KfK_f separately to determine the amount of dissipated kinetic energy. Never equate initial and final kinetic energies when solving for velocities in an inelastic collision.