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The principle of conservation of linear momentum is one of the most powerful tools in mechanics. It applies to collisions, explosions, and any interaction where no external resultant force acts on the system.
When no external resultant force acts on a system, the total momentum of the system is conserved.
For two particles:
m_1 u_1 + m_2 u_2 = m_1 v_1 + m_2 v_2
This follows from Newton's Third Law: the internal forces between the particles are equal and opposite, so they produce equal and opposite impulses, and the total momentum change is zero.
| Type | Momentum | Kinetic Energy |
|---|---|---|
| Perfectly elastic | Conserved | Conserved |
| Inelastic | Conserved | Not conserved (some lost) |
| Perfectly inelastic | Conserved | Maximum loss (particles coalesce) |
A 4 kg object moving at 6 m s^(-1) collides with a 2 kg object at rest. They coalesce. Find the common velocity.
Solution:
m_1 u_1 + m_2 u_2 = (m_1 + m_2) v
4(6) + 2(0) = (4 + 2)v
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