PHYS 1443 – Section 001
Lecture #11
Tuesday, June 20, 2006
Dr. Jaehoon Yu
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Linear Momentum
Linear Momentum and Forces
Conservation of Momentum
Impulse and Momentum Change
Collisions
Two Dimensional Collision s
Center of Mass
Today’s homework is HW #6, due 7pm, Friday, June 23!!
Tuesday, June 20, 2006
PHYS 1443-001, Summer 2006
Dr. Jaehoon Yu
1
Announcements
• Quiz this Thursday
– Eerly in the class
– Covers Ch. 8.5 – Ch. 9
• Mid-term grade discussions tomorrow
– Bottom half of the class
Tuesday, June 20, 2006
PHYS 1443-001, Summer 2006
Dr. Jaehoon Yu
2
Linear Momentum
The principle of energy conservation can be used to solve problems
that are harder to solve just using Newton’s laws. It is used to
describe motion of an object or a system of objects.
A new concept of linear momentum can also be used to solve physical problems,
especially the problems involving collisions of objects.
Linear momentum of an object whose mass is m
and is moving at a velocity of v is defined as
What can you tell from this
definition about momentum?
What else can use see from the
definition? Do you see force?
Tuesday, June 20, 2006
1.
2.
3.
4.
p  mv
Momentum is a vector quantity.
The heavier the object the higher the momentum
The higher the velocity the higher the momentum
Its unit is kg.m/s
The change of momentum in a given time interval
r r
r
r
r
r
r
r
m  v  v0 
p
mv  mv0
v


ma   F
 m
t
t
t
t
PHYS 1443-001, Summer 2006
Dr. Jaehoon Yu
3
Linear Momentum and Forces
r dpr
 F  dt
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•
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What can we learn from this Force-momentum
relationship?
The rate of the change of particle’s momentum is the same as
the net force exerted on it.
When net force is 0, the particle’s linear momentum is
constant as a function of time.
If a particle is isolated, the particle experiences no net force.
Therefore its momentum does not change and is conserved.
Something else we can do
with this relationship. What
do you think it is?
Can you think of a
few cases like this?
Tuesday, June 20, 2006
The relationship can be used to study
the case where the mass changes as a
function of time.
r
r
d  mv  dm r
r dpr
dv
 F  dt  dt  dt v  m dt
Motion
of a meteorite
PHYS 1443-001,
Summer 2006
Dr. Jaehoon Yu
Motion of a rocket
4
Conservation of Linear Momentum in a Two
Particle System
Consider an isolated system with two particles that does not have any
external forces exerting on it. What is the impact of Newton’s 3rd Law?
If particle#1 exerts force on particle #2, there must be another force that
the particle #2 exerts on #1 as the reaction force. Both the forces are
internal forces and the net force in the entire SYSTEM is still 0.
Let say that the particle #1 has momentum
Now how would the momenta
p1 and #2 has p2 at some point of time.
of these particles look like?
r
r
dp2
F12 
dt
Using momentumforce relationship
r
r
dp1
F21 
dt
And since net force
of this system is 0
r
r
dp2 dp1
d r r
 F  F12  F21  dt  dt  dt  p2  p1 
Therefore
and
0
p2  p1  const The total linear momentum of the system is conserved!!!
Tuesday, June 20, 2006
PHYS 1443-001, Summer 2006
Dr. Jaehoon Yu
5
Linear Momentum Conservation
r
r
r
r
p1i  p2i  m1v1  m2v2
r
r
r
r
p1 f  p2 f  m1v1  m2v2
Tuesday, June 20, 2006
PHYS 1443-001, Summer 2006
Dr. Jaehoon Yu
6
More on Conservation of Linear Momentum in
a Two Particle System
From the previous slide we’ve learned that the total
momentum of the system is conserved if no external
forces are exerted on the system.
p p
2
As in the case of energy conservation, this means
that the total vector sum of all momenta in the
system is the same before and after any interaction
What does this mean?
r
r
r
r
p2i  p1i  p2 f  p1 f
Mathematically this statement can be written as
P
xi

system
P
xf
system
P
yi
system
This can be generalized into
conservation of linear momentum in
many particle systems.
Tuesday, June 20, 2006
 p1  const

P
yf
system
P
zi
system

P
zf
system
Whenever two or more particles in an
isolated system interact, the total
momentum of the system remains constant.
PHYS 1443-001, Summer 2006
Dr. Jaehoon Yu
7
Example for Linear Momentum Conservation
Estimate an astronaut’s resulting velocity after he throws his book to a
direction in the space to move to a direction.
vA
vB
From momentum conservation, we can write
pi  0  p f  mAvA  mBvB
Assuming the astronaut’s mass is 70kg, and the book’s
mass is 1kg and using linear momentum conservation
vA  
mB v B
1
 
vB
mA
70
Now if the book gained a velocity
of 20 m/s in +x-direction, the
Astronaut’s velocity is
Tuesday, June 20, 2006
vA   1  20i   0.3i
70
PHYS 1443-001, Summer 2006
Dr. Jaehoon Yu
m / s
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Impulse and Linear Momentum
Net force causes change of momentum 
Newton’s second law
By integrating the above
equation in a time interval ti to
tf, one can obtain impulse I.
So what do you
think an impulse is?

tf
ti
r dpr
F
dt
r
r r
r
dp  p f  pi  p 
r
r
dp  Fdt

tf
ti
r
r
Fdt  I
Effect of the force F acting on a particle over the time
interval t=tf-ti is equal to the change of the momentum of
the particle caused by that force. Impulse is the degree of
which an external force changes momentum.
The above statement is called the impulse-momentum theorem and is equivalent to Newton’s second law.
What are the
dimension and
unit of Impulse?
What is the
direction of an
impulse vector?
Defining a time-averaged force
Tuesday, June 20, 2006
r 1
r
F   Fi t
t i
Impulse can be rewritten
If force is constant
I  F t
I  F t
It is generally assumed that the impulse force acts on a
PHYS 1443-001, Summer 2006
short time Dr.
butJaehoon
much Yu
greater than any other forces present.
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Example 9-6
(a) Calculate the impulse experienced when a 70 kg person lands on firm ground
after jumping from a height of 3.0 m. Then estimate the average force exerted on
the person’s feet by the ground, if the landing is (b) stiff-legged and (c) with bent
legs. In the former case, assume the body moves 1.0cm during the impact, and in
the second case, when the legs are bent, about 50 cm.
We don’t know the force. How do we do this?
Obtain velocity of the person before striking the ground.
KE PE
1 2
mv  mg  y  yi   mgyi
2
Solving the above for velocity v, we obtain
v  2 gyi  2  9.8  3  7.7m / s
Then as the person strikes the ground, the
momentum becomes 0 quickly giving the impulse
I  F t  p  p f  pi  0  mv 
 70kg  7.7m / s  540 N  s
Tuesday, June 20, 2006
PHYS 1443-001, Summer 2006
Dr. Jaehoon Yu
10
Example 9 – 6 cont’d
In coming to rest, the body decelerates from 7.7m/s to 0m/s in a distance d=1.0cm=0.01m.
0  vi
7.7

 3.8m / s
2
2
0.01m
d
3
The time period the collision lasts is

2.6

10
s

t 
3.8m / s
v
I  F t  540N  s
Since the magnitude of impulse is
540
5
The average force on the feet during F  I 

2.1

10
N
3
this landing is
t 2.6 10
2
2
How large is this average force? Weight  70kg  9.8m / s  6.9 10 N
The average speed during this period is
v 
F  2.1105 N  304  6.9 102 N  304  Weight
If landed in stiff legged, the feet must sustain 300 times the body weight. The person will
likely break his leg.
d 0.50m
 0.13s

t 
3.8
m
/
s
For bent legged landing:
v
540
F
 4.1 103 N  5.9Weight
0.13
Tuesday, June 20, 2006
PHYS 1443-001, Summer 2006
Dr. Jaehoon Yu
11
Another Example for Impulse
In a crash test, an automobile of mass 1500kg collides with a wall. The initial and
final velocities of the automobile are vi= -15.0i m/s and vf=2.60i m/s. If the collision
lasts for 0.150 seconds, what would be the impulse caused by the collision and the
average force exerted on the automobile?
Let’s assume that the force involved in the collision is a lot larger than any other
forces in the system during the collision. From the problem, the initial and final
momentum of the automobile before and after the collision is
r
pi  mvi  1500   15.0 i  22500i kg  m / s
r
p f  mv f 1500   2.60 i  3900i kg  m / s
Therefore the impulse on the
automobile due to the collision is
The average force exerted on the
automobile during the collision is
Tuesday, June 20, 2006
I
 p  p f  pi 3900  22500 i kg  m / s
 26400i kg  m / s  2.64 104 i kg  m / s
p 2.64  104
F  t  0.150 i
 1.76 105 i kg  m / s 2  1.76 105 i N
PHYS 1443-001, Summer 2006
Dr. Jaehoon Yu
12
Collisions
Generalized collisions must cover not only the physical contact but also the collisions
without physical contact such as that of electromagnetic ones in a microscopic scale.
Consider a case of a collision
between a proton on a helium ion.
F
F12
t
F21
Using Newton’s
3rd
The collisions of these ions never involve
physical contact because the electromagnetic
repulsive force between these two become great
as they get closer causing a collision.
Assuming no external forces, the force
exerted on particle 1 by particle 2, F21,
changes the momentum of particle 1 by
r r
dp1  F21dt
Likewise for particle 2 by particle 1
r r
dp2  F12dt
law we obtain
dp2
r
 F12dt
So the momentum change of the system in the
collision is 0, and the momentum is conserved
Tuesday, June 20, 2006
r
  F21dt
 dp1
dp  dp1  dp2  0
psystem  p1  p2  constant
PHYS 1443-001, Summer 2006
Dr. Jaehoon Yu
13
Elastic and Inelastic Collisions
Momentum is conserved in any collisions as long as external forces are negligible.
Collisions are classified as elastic or inelastic based on whether the kinetic energy
is conserved, meaning whether it is the same before and after the collisions.
Elastic
Collision
A collision in which the total kinetic energy and momentum
are the same before and after the collision.
Inelastic
Collision
A collision in which the total kinetic energy is not the same
before and after the collision, but momentum is.
Two types of inelastic collisions:Perfectly inelastic and inelastic
Perfectly Inelastic: Two objects stick together after the collision,
moving together at a certain velocity.
Inelastic: Colliding objects do not stick together after the collision but
some kinetic energy is lost.
Note: Momentum is constant in all collisions but kinetic energy is only in elastic collisions.
Tuesday, June 20, 2006
PHYS 1443-001, Summer 2006
Dr. Jaehoon Yu
14
Elastic and Perfectly Inelastic Collisions
In perfectly Inelastic collisions, the objects stick
together after the collision, moving together.
Momentum is conserved in this collision, so the
final velocity of the stuck system is
How about elastic collisions?
m1v1i  m2v2i  (m1  m2 )v f
vf 
m1v1i  m2v2i
( m1  m2 )
m1v1i  m2v2i  m1v1 f  m2v2 f
1
1
1
1
In elastic collisions, both the
m1v12i  m2 v22i  m1v12f  m2 v22 f
2
2
2
2
momentum and the kinetic energy
m1 v12i  v12f   m2 v22i  v22 f 
are conserved. Therefore, the
final speeds in an elastic collision
m1 v1i  v1 f v1i  v1 f   m2 v2i  v2 f v2i  v2 f 
can be obtained in terms of initial From momentum
m1 v1i  v1 f   m2 v2i  v2 f 
speeds as
conservation above
 m  m2 
 2m2 
v1i  
v2i
v1 f   1
 m1  m2 
 m1  m2 
Tuesday, June 20, 2006
 2m1 
 m  m2 
v1i   1
v2i
v2 f  
 m1  m2 
 m1  m2 
PHYS 1443-001, Summer 2006
What happens when
theDr.two
masses are the same?
Jaehoon Yu
15
Example for Collisions
A car of mass 1800kg stopped at a traffic light is rear-ended by a 900kg car, and the
two become entangled. If the lighter car was moving at 20.0m/s before the collision
what is the velocity of the entangled cars after the collision?
The momenta before and after the collision are
Before collision
pi  m1v1i  m2v2i  0  m2v2i
m2
20.0m/s
m1
p f  m1v1 f  m2v2 f   m1  m2  v f
After collision
Since momentum of the system must be conserved
m2
vf
m1
vf
What can we learn from these equations
on the direction and magnitude of the
velocity before and after the collision?
Tuesday, June 20, 2006
 m1  m2  v f
pi  p f

 m2v2i
m2v2i
900  20.0i

 m1  m2  900  1800  6.67i m / s
The cars are moving in the same direction as the lighter
car’s original direction to conserve momentum.
The magnitude is inversely proportional to its own mass.
PHYS 1443-001, Summer 2006
Dr. Jaehoon Yu
16
Two dimensional Collisions
In two dimension, one needs to use components of momentum and
apply momentum conservation to solve physical problems.
m1
m1v1i  m2v2i  m1v1 f  m2v2 f
v1i
m2
q
f
x-comp.
m1v1ix  m2v2ix  m1v1 fx  m2v2 fx
y-comp.
m1v1iy  m2v2iy  m1v1 fy  m2v2 fy
Consider a system of two particle collisions and scattersin
two dimension as shown in the picture. (This is the case at
fixed target accelerator experiments.) The momentum
conservation tells us:
m1v1i  m2v2i  m1v1i
m1v1ix  m1v1 fx  m2 v2 fx  m1v1 f cos q  m2 v2 f cos f
m1v1iy  0  m1v1 fy  m2 v2 fy  m1v1 f sin q  m2 v2 f sin f
And for the elastic collisions, the
kinetic energy is conserved:
Tuesday, June 20, 2006
1
1
1
m1v 12i  m1v12f  m2 v22 f
2
2
2
PHYS 1443-001, Summer 2006
Dr. Jaehoon Yu
What do you think
we can learn from
these relationships?
17
Example for Two Dimensional Collisions
Proton #1 with a speed 3.50x105 m/s collides elastically with proton #2 initially at
rest. After the collision, proton #1 moves at an angle of 37o to the horizontal axis and
proton #2 deflects at an angle f to the same axis. Find the final speeds of the two
protons and the scattering angle of proton #2, f.
m1
v1i
m2
q
Since both the particles are protons m1=m2=mp.
Using momentum conservation, one obtains
x-comp. m p v1i  m p v1 f cos q  m p v2 f cos f
y-comp.
f
m p v1 f sin q  m p v2 f sin f  0
Canceling mp and put in all known quantities, one obtains
v1 f cos 37  v2 f cos f  3.50 105 (1)
From kinetic energy
conservation:
3.50 10 
5 2
 v v
2
1f
2
2f
Tuesday, June 20, 2006
v1 f sin 37  v2 f sin f
(2)
v1 f  2.80 105 m / s
Solving Eqs. 1-3
5
(3) equations, one gets v2 f  2.1110 m / s
f  53.0
PHYS 1443-001, Summer 2006
Dr. Jaehoon Yu
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