Equation 2: The Impulse-Momentum Theorem
The second equation we can generate from our definition of momentum comes from
our equations for impulse. Recall that:
J = mvf - mvo
Substituting our expression for momentum, we find that:
This equation is known as the Impulse-Momentum Theorem. Stated verbally, an
impulse given to a particle causes a change in momentum of that particle.
Keeping this equation in mind, momentum is conceptually quite similar to
kinetic energy. Both quantities are
defined based on concepts dealing with force: kinetic energy is defined by work,
and momentum is defined by impulse. Just as a net work causes a change in
kinetic energy, a net impulse causes a change momentum. In addition, both are
related to velocity in some way. In fact, combining the two equations
K =
mv2 and
p = mv we can see that:
K =  |
|
This simple equation can be quite convenient for relating the two different
concepts.
This section, dealing exclusively with the momentum of a single particle, might
seem out of place after a section on systems of particles. However, when we
combine the definition of momentum with our knowledge of systems of particles,
we can generate a powerful conservation law: the conservation of
momentum.