2. Overview
Momentum
• Center of Mass
• Impulse-Momentum Theorem
• Conservation of Momentum
Energy
• Work-Energy Theorem
• Conservation of Energy
• Elastic and Inelastic Collisions
3. Momentum
Momentum
• Momentum is defined as:
• The rate of change of momentum of an object is equal
to the net force applied to the object.
p m v=
Σ
∆
∆
F
p
t
=
4. Conservation of Momentum
Conservation of momentum states that:
the total momentum of an isolated
system of objects remains constant.
• Isolated system: no outside forces acting on
the system
• Tip: Break the momentum of each
component up into horizontal and vertical
components: these are independent of one
another!
5. Collisions and Impulse
Impulse-momentum theorem defines impulse and says
that the impulse on a system will be equal to the
change in its momentum.
F t p∆ ∆=
6. Center of Mass
The center-of-mass of a collection of particles
if given by the following equation:
• The total linear momentum of a system of particles is
equal to the total mass M of the system multiplied by
the velocity of the center of mass of the system.
• Extended systems use this formulation for Newton’s
Laws too.
x
M
m xC M i i=
1
Σ
7. Work and Energy
Work is merely a force applied on an object
over a certain distance.
Kinetic Energy is the energy of motion.
Potential Energy is the ability of an object to
start/stop motion.
• Gravity: Elastic
W F d= c o s θ
T m v=
1
2
2
U m g h= U k x=
1
2
2
8. Work-Energy Theorem
This principle states that the work done on an
object is equal to the change in kinetic energy
of an object
W T= ∆
9. Conservation of Energy
Conservative vs. Non-conservative
Forces
• Friction
Conservation of Energy: The total energy
of an isolated system cannot change.
• Shift between potential and kinetic energy.
11. Collisions
Elastic Collisions
• “Rubber” – things bounce off.
• Both energy and momentum are conserved.
Inelastic Collisions
• “Gluey” – things stick together
• Only momentum is conserved!
13. Simple Harmonic Motion
Period and Frequency
Oscillatory Motion
• Springs, Pendulums
• Conservation of Energy
• Position as a function of time
x t A t( ) c o s ( )= ω