Momentum and Collisions
Misconceptions
| Misconception | Correction |
|---|---|
| "Heavier objects have more momentum" | Momentum depends on both mass AND velocity: p = mv |
| "Momentum is the same as kinetic energy" | Momentum is a vector (p = mv), KE is a scalar (½mv²); they're conserved differently |
| "In a collision, the heavier object always wins" | Momentum is always conserved; the lighter object changes velocity more |
| "Momentum is always conserved" | Momentum is conserved only when external forces are negligible |
| "Elastic collisions conserve energy, inelastic don't" | Both conserve momentum; elastic also conserves KE, inelastic doesn't |
Key Concepts
Momentum
Momentum is mass times velocity:
- •p = mv
- •Vector quantity (has direction)
- •Unit: kg·m/s (no special name)
- •Total momentum of a system: p_total = Σmᵢvᵢ
Impulse
Impulse is the change in momentum caused by a force:
- •J = FΔt = Δp = p_f - p_i
- •Vector quantity
- •Unit: N·s = kg·m/s
- •Area under F-t graph equals impulse
Impulse-Momentum Theorem
The impulse equals the change in momentum:
- •FΔt = mΔv = mv_f - mv_i
- •Derived from Newton's second law: F = ma = m(Δv/Δt)
Conservation of Momentum
In an isolated system (no external forces), total momentum is conserved:
- •Σp_before = Σp_after
- •m₁v₁ᵢ + m₂v₂ᵢ = m₁v₁f + m₂v₂f
Types of Collisions
Elastic Collision:
- •Momentum is conserved
- •Kinetic energy is conserved
- •Objects bounce off each other
- •Examples: billiard balls, atomic collisions
Inelastic Collision:
- •Momentum is conserved
- •Kinetic energy is NOT conserved (some converts to heat, sound, deformation)
- •Most real collisions are inelastic
Perfectly Inelastic Collision:
- •Objects stick together after collision
- •Maximum KE loss (consistent with momentum conservation)
- •m₁v₁ᵢ + m₂v₂ᵢ = (m₁ + m₂)v_f
Center of Mass
The point where total mass can be considered concentrated:
- •x_cm = (m₁x₁ + m₂x₂)/(m₁ + m₂)
- •Velocity of center of mass: v_cm = (m₁v₁ + m₂v₂)/(m₁ + m₂)
- •In isolated system, v_cm is constant
Equations
[1] p = mv (momentum) [2] J = FΔt = Δp (impulse) [3] m₁v₁ᵢ + m₂v₂ᵢ = m₁v₁f + m₂v₂f (conservation of momentum) [4] (m₁ + m₂)v_f = m₁v₁ᵢ + m₂v₂ᵢ (perfectly inelastic) [5] ½m₁v₁ᵢ² + ½m₂v₂ᵢ² = ½m₁v₁f² + ½m₂v₂f² (elastic collision, KE conserved) [6] v₁f = ((m₁-m₂)/(m₁+m₂))v₁ᵢ + (2m₂/(m₁+m₂))v₂ᵢ (elastic collision formula) [7] v_cm = (m₁v₁ + m₂v₂)/(m₁ + m₂) (center of mass velocity)
Worked Examples
Example 1: Impulse
Problem: A 0.15 kg baseball moving at 40 m/s is hit by a bat and leaves at 50 m/s in the opposite direction. What impulse did the bat deliver?
Solution:
- •Define positive direction as initial ball direction
- •Initial momentum: p_i = 0.15 × 40 = 6 kg·m/s
- •Final momentum: p_f = 0.15 × (-50) = -7.5 kg·m/s
- •Impulse: J = p_f - p_i = -7.5 - 6 = -13.5 kg·m/s (or 13.5 kg·m/s toward the pitcher)
Example 2: Perfectly Inelastic Collision
Problem: A 1000 kg car moving at 20 m/s collides with a 2000 kg truck at rest. They stick together. Find the final velocity.
Solution:
- •Conservation of momentum: m₁v₁ + m₂v₂ = (m₁ + m₂)v_f
- •1000(20) + 2000(0) = (1000 + 2000)v_f
- •20000 = 3000v_f
- •v_f = 6.67 m/s
Example 3: Elastic Collision (1D)
Problem: A 2 kg ball moving at 5 m/s collides elastically with a 3 kg ball at rest. Find both final velocities.
Solution:
- •Using elastic collision formulas:
- •v₁f = ((m₁-m₂)/(m₁+m₂))v₁ᵢ = ((2-3)/(2+3)) × 5 = (-1/5) × 5 = -1 m/s
- •v₂f = (2m₁/(m₁+m₂))v₁ᵢ = (2×2/(2+3)) × 5 = (4/5) × 5 = 4 m/s
- •Check: momentum and KE should be conserved
Explanation Patterns
- •Define a coordinate system and positive direction
- •Identify the system - what objects are involved?
- •Check for external forces - if negligible, momentum is conserved
- •Determine collision type: elastic (both p and KE conserved) or inelastic (only p conserved)
- •Write conservation equations for each direction
- •For 2D problems, use vector components
- •Check your answer: total momentum before = total momentum after
Common Problem Types
- •Impulse: FΔt = Δp, finding force from momentum change
- •Inelastic collision: Objects stick together, find final velocity
- •Elastic collision: Both momentum and KE conserved
- •Recoil/explosion: Initially at rest, objects separate
- •2D collision: Use vector components, conserve p_x and p_y separately
- •Ballistic pendulum: Collision + energy conservation