linear momentum unit 5. lesson 1 : linear momentum and its conservation f 21 + f 12 = 0 (newton’s...
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Linear Momentum
Unit 5
Lesson 1 : Linear Momentum and Its Conservation
F21 + F12 = 0(Newton’s Third Law)
m1a1 + m2a2 = 0(Newton’s Second Law)
m1
dv1
dtm2
dv2
dt+ = 0
d(m1v1)
dt
d(m2v2)
dt+ = 0
(m1v1 + m2v2) = 0d
dt
sum of linear momentum is constant
p = mv (linear momentum)
Linear momentum is a vector quantity whose direction the same as the
direction of v. Its SI unit is kg . m/s.
F = ma = mdv
dt
F =d(mv)
dt
dp=
dt
The time rate of change of the linear momentum of a particle is equal to the
net force acting on the particle.
(This is the form in which Newton presented his second law.)
Conservation of Linear Momentum
Whenever two or more particles in an isolated system interact, the total momentum of the
system remains constant.
The total momentum of an isolated system at all times equals its initial momentum.
Total p before = Total p after
A 60. kg archer stands at rest on frictionless ice and fires a 0.50 kg arrow horizontally at
50. m/s.
Example 1
a) With what velocity does the archer move across the ice after firing the arrow.
b) What if the arrow were shot in a direction that makes an angle with the
horizontal ? How will this change the recoil velocity of the archer ?
Two blocks of masses M and 3M are placed on a horizontal, frictionless
surface. A light spring is attached to one of them,
and the blocks are pushed together with the spring between them. A cord initially holding the
blocks together is burned, and the 3M block moves to the right with a
speed of 2.00 m/s.
Example 2
a) What is the speed of the block of mass M ?
b) Find the original elastic potential energy in the spring if M = 0.350 kg.
A swing seat of mass M is connected to a fixed point P by a massless cord of length L. A child also of mass M sits on the
seat and begins to swing with zero velocity at a position at which the cord makes a 60o angle with the vertical as shown
in Figure I. The swing continues down until the cord is exactly vertical at which time the child jumps off in a
horizontal direction.
Example 3 : AP 1981 #2
The swing continues in the same direction until the cord makes a 45o angle with the vertical as shown in Figure II; at that point it begins to swing in the reverse direction. With what velocity relative to the ground did the child leave the swing ? (cos 45o = sin 45o = 2
2
, sin 30o = cos 60o = ½,
cos 30o = sin 60o = 3
2)
Lesson 2 : Impulse and Momentum
F =d(mv)
dt
dp=
dt
dp = F dt
Integrating F with respect to t,
p = pf – pi = F dttf
ti
Impulse (I)
F dt
tf
ti
I =
Impulse has a magnitude equal to the area under the force-time
graph.
Impulse is a vector quantity with the same direction as the direction of the change in momentum.
Because the force imparting an impulse can generally vary in time, we can express impulse as
I = Ft
Impulse – Momentum Theorem
p = pf – pi = F dttf
ti
The impulse of the force F acting on a particle equals the change in the
momentum of the particle.
I = p
In a particular crash test, a car of mass
1500 kg collides with a wall, as shown. The
initial and final velocities of the car
are vi = -15.0i m/s and vf = 2.60i m/s, respectively.
^
^
Example 1
a) If the collision lasts for 0.150 s, find the impulse caused by the collision and the average force exerted on the car.
b) What if the car did not rebound from the wall ? Suppose the final velocity of the car is zero and the time interval of the collision remains 0.150 s. Would this represent a larger or a
smaller force by the wall on the car ?
A 3.00 kg steel ball strikes a wall with a speed of 10.0 m/s at an angle of 60.0o with the
surface. It bounces off with the same speed and angle. If the ball is in contact with the wall for 0.200 s, what is the average force exerted
by the wall on the ball ?
Example 2
An estimated force-time curve for a baseball struck by a bat is shown above.
From this curve, determine
Example 3
a) the impulse delivered to the ball
b) the average force exerted on the ball
c) the peak force exerted on the ball
Lesson 3 : Collisions in One-Dimension
Elastic Collisions
The total KE (as well as total momentum) of the
system is the same before and after the collision.
Inelastic Collisions
The total KE of the system is not the same before and
after the collision (even though the momentum of the system is conserved).
KE is conserved KE is not conserved
“perfectly inelastic” “inelastic”
m1v1i + m2v2i = (m1 + m2)vf
Perfectly Inelastic Collisions
when the colliding objects stick together
Elastic Collisions
m1v1i + m2v2i = m1v1f + m2v2f
½ m1v1i2 + ½ m2v2i
2 = ½ m1v1f2 + ½ m2v2f
2
Example 1
An 1800 kg car stopped at a traffic light is struck from the rear by a 900 kg car, and the two become entangled, moving along the same path as that of
the originally moving car.
a) If the smaller car were moving at 20.0 m/s before the collision, what is the velocity of the
entangled cars after the collision ?
b) Suppose we reverse the masses of the cars – a stationary 900 kg car is struck by a moving 1800 kg car. Is the final speed the same as
before ?
The ballistic pendulum is an apparatus used to measure the speed of a fast-moving projectile, such as a bullet. A bullet of mass m1 is fired into a large block of wood of mass m2 suspended from some light wires. The bullet
embeds in the block, and the entire system swings through a height h. How can we determine the speed of
the bullet from a measurement of h ?
Example 2
A block of mass m1 = 1.60 kg initially moving to the right with a speed of 4.00 m/s on a frictionless
horizontal track collides with a spring attached to a second block of mass m2 = 2.10 kg initially moving
to the left with a speed of 2.50 m/s. The spring constant is 600 N/m.
Example 3
a) Find the velocities of the two blocks after the collision.
b) During the collision, at the instant block 1 is moving to the right with a velocity of +3.00 m/s, determine the velocity of block 2.
A 5 kg ball initially at rest at the edge of a 2 m long, 1.2 m high frictionless table, as shown
above. A hard plastic cube of mass 0.5 kg slides across the table at a speed of 26 m/s and strikes the ball, causing the ball to leave the table in the
direction in which the cube was moving.
Example 4 : AP 1995 #1
The figure below shows a graph of the force exerted on the ball by the cube as a function of time.
a) Determine the total impulse given to the ball.
b) Determine the horizontal velocity of the ball immediately after the collision.
c) Determine the following for the cube immediately after the collision.
i. Its speed
ii. Its direction of travel (right or left), if moving
d) Determine the kinetic energy dissipated in the collision.
e) Determine the distance between the two points of impact of the objects with the floor.
A 2 kg block and an 8 kg block are both attached to an ideal spring (for which k = 200 N/m) and both are initially at rest on a horizontal frictionless surface, as shown in
the diagram above.
In an initial experiment, a 100 g (0.1 kg) ball of clay is thrown at the 2 kg block. The clay is moving horizontally
with speed v when it hits and sticks to the block. The 8 kg block is held still by a removable stop. As a result, the
spring compresses a maximum distance of 0.4 m.
Example 5 : AP 1994 #1
a) Calculate the energy stored in the spring at maximum compression.
b) Calculate the speed of the clay ball and 2 kg block immediately after the clay sticks to the block but before the spring compresses significantly.
c) Calculate the initial speed v of the clay.
In a second experiment, an identical ball of clay is thrown at another identical 2 kg block, but this time the stop is
removed so that the 8 kg block is free to move.
d) State whether the maximum compression of the spring will be greater than, equal to, or less than 0.4 m.
Explain briefly.
e) State the principle or principles that can be used to calculate the velocity of the 8 kg block at the instant that the spring regains its original length. Write the appropriate equation(s) and show the numerical substitutions, but do not solve for the velocity.
Lesson 4 : Two-Dimensional Collisions
m1v1i = m1v1f cos + m2v2f cos
0 = m1v1f sin - m2v2f sin
Since this is an elastic collision, KE is also conserved.*
* If this were an inelastic collision, KE would not be conserved, and
this equation does not apply.
½ m1v1i2 = ½ m1v1f
2 + ½ m2v2f2
A 1500 kg car traveling east with a speed of 25.0 m/s
collides at an intersection with a 2500 kg van traveling north at a speed of 20.0 m/s.
Find the direction and magnitude of the velocity of
the wreckage after the collision, assuming that the vehicles undergo a perfectly
inelastic collision (that is, they stick together).
Example 1
In a game of billiards, a player wishes to sink a target ball in the corner pocket. If the angle to the corner
pocket is 35o, at what angle q is the cue ball deflected ? Assume that friction and rotational motion are
unimportant and that the collision is elastic. Also assume that all billiard balls have the same mass m.
Example 2
Lesson 5 : The Center of Mass
Center of mass (CM) is the average position of the system’s mass
Center of mass is located on the line joining the two particles and is closer to the particle
having the larger mass.
System rotates clockwise when F is applied between the less massive particle and CM.
System rotates counterclockwise when F is applied between the more massive particle and CM.
System moves in the direction of F without rotating when F is
applied at CM.
How to Locate the Center of Mass
xCM =m1x1 + m2x2
m1 + m2
Center of mass for a system of many particles
xCM =m1x1 + m2x2 + m3x3 + ……
m1 + m2 + m3 + ……
xCM =mixi
M
Y coordinates of CM
yCM =miyi
M
Z coordinates of CM
zCM =mizi
M
Using a Position Vector (r) to locate CM of a system of particles
rCM = xCM i + yCM j + zCM k^ ^ ^
Using a Position Vector (r) to locate CM of an extended object
xCM =ximi
Mlim
mi 0
(likewise for yCM and zCM)
=1
Mr dm
rCM
=1
Mx dm
xCM
Suspend the object first from points A and C.
Locating CM of an irregularly shaped object
CM is where lines AB and CD intersect
If wrench is hung freely from any point, the vertical line
through this point must pass through CM.
A baseball bat is cut at the location of its center of mass. The piece with smaller mass is
Example 1
a) the piece on the right.
b) the piece on the left.
c) both have same mass.
d) impossible to determine.
A system of three particles located as shown above. Find the center of mass of the system.
Example 2
a) Show that the center of mass of a rod of mass M and length L lies midway
between its ends, assuming the rod has a uniform mass per unit length.
Example 3
b) Suppose a rod is nonuniform such that its mass per unit length varies
linearly with x according to the expression = x, where is a constant. Find the x coordinate of the center of mass as a fraction of L.
Lesson 6 : Motion of a System of Particles
Velocity of CM
vCM =drCM
dt
Acceleration of CM
aCM =dvCM
dt
Total momentum of a system of particles
MvCM = mivi = pi = ptot
(i is the ith particle)
Newton’s Second Law for a system of particles
Fext = MaCM
total mass of system
CM of a system of particles of combined mass M moves like an equivalent particle of mass M
would move under the influence of the net external force on the system.
Suppose you tranquilize a polar bear on a smooth glacier as part of a research
effort. How might you estimate the bear’s mass using a measuring tape, a rope, and
knowledge of your own mass ?
Example 1
Example 2
Consider a system of two particles in the xy plane :
m1 = 2.00 kg is at r1 = (1.00 i + 2.00 j) m and has a velocity of (3.00 i + 0.500 j) m/s
m2 = 3.00 kg is at r2 = (-4.00 i - 3.00 j) m and has a velocity of (3.00 i – 2.00 j) m/s
^ ^
^ ^
^ ^
^ ^
a) Plot these particles on a grid or graph paper. Draw their position vectors and show their velocities.
b) Find the CM of the system and mark it on the grid.
c) Determine the velocity of the CM and also show it on the diagram.
d) What is the total linear momentum of the system ?
Example 3
A rocket is fired vertically upward. At the instant it reaches an altitude of 1000 m and a speed of 300 m/s, it explodes into three
fragments having equal mass. One fragment continues to move upward with a speed of 450 m/s following the explosion. The second fragment has a speed of 240
m/s and is moving east right after the explosion. What is the velocity of the third
fragment right after the explosion ?