Resource Lesson
Linear Momentum
Printer Friendly Version
Momentum
is defined as the product of an object's mass and its velocity. Since velocity is a vector quantity and mass is a scalar quantity,
momentum's vector nature
is dependent on the vector properties of the object's velocity. If an object is moving in a positive direction, then its momentum is considered to be positive. Momentum can be represented by the variable
p
and has units of kg m/sec.
p = mv
Since momentum is a vector, all objects in a closed system can individually have momentum but the system as a whole can have a net momentum of zero. Consider, for example, the following system:
the 3 kg mass has a positive momentum of 6 kg m/sec;
the 2 kg mass has a negative momentum of 6 kg m/sec;
each mass is moving, but the total momentum of the system equals 0.
Derivations based on Newton's Laws
To understand the properties of momentum, we must first re-examine Newton's 2nd and 3rd Laws.
Newton's 2nd Law
net F = ma
net F = m (v
_{f}
- v
_{o}
) / t
(net F)t = m (v
_{f}
- v
_{o}
)
(net F) t = mv
_{f}
- mv
_{o}
(net F)t = p
_{f}
- p
_{o}
(net F)t = Δp
impulse = the change in momentum
Newton's 3rd Law
F
_{AB}
= - F
_{BA}
F
_{AB}
t = - F
_{BA}
t
m
_{B}
v
_{f}
_{B}
- m
_{B}
v
_{oB}
= - (m
_{A}
v
_{f}
_{A}
- m
_{A}
v
_{oA}
)
m
_{B}
v
_{f}
_{B}
+ m
_{A}
v
_{f}
_{A}
= m
_{A}
v
_{oA}
+ m
_{B}
v
_{oB}
Σ
p
_{f}
=
Σ
p
_{o}
The Law of Conservation of Momentum states the sum of the momenta before a collision equals the sum of the momenta after a collision
Impulse
Impulse
can be represented by the variable
J
and has units of N sec. Since the impulse an object receives equals the change in its momentum, the units for impulse and momentum must be equivalent.
N sec
kg m/sec
[kg m/sec
^{2}
] sec
kg m/sec
Note that in the equation for impulse, if the amount of momentum being changed remains constant, then the net force can be maximized by decreasing the time of impact. That is, a short jab is much more effective than a long, drawn-out swing when striking someone for maximum force. Conversely, when a large amount of momentum has to be lost doing so over a longer period of time decreases the net force applied to the object. For example, when you jump off of a high tower bending your knees when you land decreases the impact force by increasing the time of impact. Moreover, if the amount of force remains constant then the change in momentum can be maximized by increasing the time of impact. For example, in sports, coaches are always encouraging athletes to "follow through." This allows the force to act on the ball for a greater amount of time therefore increasing the time of impact and the net impulse delivered to the ball. Subsequently, the ball receives a greater change in its momentum and has a greater final velocity.
Accompanying this restatement for Newton's 2nd law are two important graphical relationships.
Conservation of Momentum
During any collision, momentum is conserved as a consequence of Newton's 3rd Law - the Law of Action-Reaction. What this means is that the total momentum before a collision is always equal to the total momentum after a collision.
Σ
p
_{o}
=
Σ
p
_{f}
There are two general categories of collisions: elastic and inelastic.
Elastic collisions
occur when objects bounce off each other AND kinetic energy is conserved during the collision. These types of collisions are more "ideal" in nature and are difficult to observe. Usually students encounter discussions of elastic collisions when working problems with collisions between objects and ideal springs as well as collisions on the subatomic level between photons and electrons. They are also one of the fundamental assumptions when deriving laws of ideal gases. In our everyday world, the majority of collisions are inelastic.
Inelastic collisions
occur when objects collide and energy is lost during the collision. That is,
Σ
KE
_{before}
>
Σ
KE
_{after}
. During
perfectly inelastic collisions
the objects stick together during the collision and leave as one single mass. The degree to which a collision is considered to be elastic or inelastic is measured by a quantity called the
coefficient of restitution, e,
which is defined as the ratio of the (relative velocities of recession) /(relative velocities of approach) for the two objects involved in the collision. When e = 1, the collision is perfectly elastic; when e = 0 is it perfectly inelastic.
e = (v
_{f2}
- v
_{f1}
) / (v
_{o1}
- v
_{o2}
)
Recoil velocities
are considered in problems involving explosions: a gun is fired and the bullet goes in one direction while the gun "recoils" in the opposite direction, or when a canon is fired, or a coiled spring is released. Usually the total momentum before the collision is zero (the system is at rest) and then the objects travel off in opposite directions with a total final momentum that must also add to zero.
Let's look at a few examples.
Suppose that a 3-kg mass moving at 5 m/sec strikes a stationary 1-kg mass whereupon they stick other. What will be the final velocity of the combined mass, v
_{c}
, after this inelastic collision?
Suppose that a 3-kg mass moving at 2 m/sec strikes a 1-kg mass moving towards it at 10 m/sec whereupon they stick together. What will be the final velocity of the combined mass, v
_{c}
, after this inelastic collision?
Suppose a 1-kg pistol containing a 10-gram bullet is resting on a table when it is accidentally discharged. If the bullet has a muzzle velocity of 150 m/sec, how fast will the pistol recoil?
How do the impulses an object receives compare when (1) it strikes a wall and sticks to it, versus (2) it rebounds elastically off of the wall?
When objects travel along diagonal paths, they have momentum in each of the x and y dimensions. Consequently momentum vectors must be resolved into their x- and y-components when working
two-dimensional collisions
.
Consider the following scenario.
A 2-kg mass traveling left at 3 m/sec along the positive x-axis and a 3-kg mass traveling upwards along the positive y-axis at 2 m/sec collide with each other. If the two masses stick together during the collision, how fast and in what direction will they leave the collision?
.
Related Documents
Lab:
Labs -
A Battering Ram
Labs -
A Photoelectric Effect Analogy
Labs -
Air Track Collisions
Labs -
Ballistic Pendulum
Labs -
Ballistic Pendulum: Muzzle Velocity
Labs -
Bouncing Steel Spheres
Labs -
Collision Pendulum: Muzzle Velocity
Labs -
Conservation of Momentum
Labs -
Conservation of Momentum in Two-Dimensions
Labs -
Impulse
Labs -
Inelastic Collision - Velocity of a Softball
Labs -
Rube Goldberg Challenge
Labs -
Spring Carts
Labs -
Video Lab: Blow Dart Collides with a Stationary Cart
Labs -
Video Lab: M&M Colliding with Pop Can
Labs -
Video Lab: Marble Collides with Ballistic Pendulum
Resource Lesson:
RL -
A Further Look at Impulse
RL -
Famous Discoveries: The Franck-Hertz Experiment
RL -
Momentum and Energy
RL -
Springs and Blocks
RL -
Symmetries in Physics
Worksheet:
APP -
Puppy Love
APP -
The Jogger
APP -
The Pool Game
APP -
The Raft
CP -
Conservation of Momentum
CP -
Momentum
CP -
Momentum and Energy
CP -
Momentum and Kinetic Energy
CP -
Momentum Practice Problems
CP -
Momentum Systems and Conservation
NT -
Ice Boat
NT -
Momentum
WS -
Advanced Properties of Freely Falling Bodies #1
WS -
Advanced Properties of Freely Falling Bodies #2
WS -
Advanced Properties of Freely Falling Bodies #3
WS -
Force vs Displacement Graphs
WS -
Practice: Momentum and Energy #1
WS -
Practice: Momentum and Energy #2
PhysicsLAB
Copyright © 1997-2015
Catharine H. Colwell
All rights reserved.
Application Programmer
Mark Acton