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Momentum. Chapter-6. Momentum. Symbol is lower case p Momentum is a product of mass and velocity p = mv. Units. p = mv, so the units are: p = (kg)(m/s) kgm because velocity is a vector smomentum is a vector quantity Or, N-s. 82,288 kg x 0.02m/s = 1600 kgm/s. - PowerPoint PPT Presentation
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Momentum
Chapter-6
Momentum
• Symbol is lower case p
• Momentum is a product of mass and velocity
• p = mv
Units
• p = mv, so the units are:
• p = (kg)(m/s)
kgm because velocity is a vectors momentum is a vector quantity
Or, N-s
82,288 kg x 0.02m/s = 1600 kgm/s
100kg astronaut in a 60 kg suit movingAt 10 m/s
1600 kg m/s
Conservation of momentum
• Momentum of a system is conserved:
• Before and after objects join• Before and after an explosion• Newton’s Third Law applies
• FB on A = - FA on B
1600 kgm/s astronaut grabs a 100 kg
Sputnik, how fast do both go?
10 m/s
m1v1 = m2v2
1600 kgm/s = 260 kg v2
v2 = 6.2 m/s
In a collision, the total momentum before doesn’t change:2500 N-s + 800 N-s = 3300 N-s
1500 N-s + 1800 N-s = 3300 N-s
Explosions between vehicles
Recoil
Let’s say it’s a 5 kg rifle and
a 10 g bullet fired at 1000m/s
• m1v1 = m2v2
• (0.01 kg)(1000m/s) = 5kg v2
• 10 kgm/s = 5kg v2
• 2m/s = v2 of course you usually put your shoulder there
Converting to Newton-S
• A Newton is a kgm/s2
• A Newton-second is a (kgm/s2)(s) = kgm/s
• So Newton-seconds are equivalent to units of momentum
Deriving Impulse Theorem from Newton’s
2nd Law• F = ma = m v/t
• F t = m v
• So, the average force over the time interval is equal to the change in momentum
• F t = p2 - p1
So it’s the same rifle on your shoulder, &
the recoil lasts 0.01s
• mv = Ft
• 10 kgm/s = F(s
• F = 1000N That kind of hurts
Hitting the wall at the Indianapolis Speedway
The average force you feel depends on rate of change in momentum
Lets say you’re going 100km/hr, How fast do you decelerate to0 km/hr as the front of your car crumples on the concrete? What force is felt by the 100kg driver?
(100 km/h)(1000 m/km)(1 h/3600 s) = 27.8 m/s
Let’s say the hood is one meter long d = 1/2vt t = 0.072 s
The impulse is F t = m vF (0.0726 s) = (100 kg) (27.8 m/s - 0 m/s)
F = 38,600 NThis is fatal
So we use straw bales around race tracks.
… and some soft squishy spectators.
(100 km/h)(1000 m/km)(1 h/3600 s) = 27.8 m/s
Let’s say the straw makes the car stop in 10m, d = 1/2vt t = 0.72 s
The impulse is F t = m vF (0.72 s) = (100 kg) (27.8 m/s - 0 m/s)
F = 3,860 N
3860 N / 980 N = about 4g (4x gravity)
this is likely survivable
Billiards: the break
1-D conservation of momentum
Very few shots line up perfectly
Momentum of the constituents before and after contact is equal
A stationary ball (red 3-ball) hit with a cue-ball.
They share momentum after collision.
Forward or back spin can affect the trajectory of the cue ball.
Little to no spin is transferred to the targetball.
Conservation of Momentum in
2-D
0.1 kg ballRolls at 0.5 m/s
Cueball-1
GreenballCueball-2
60o
Conservation of Momentum in
2-D
Cue ball starts with a momentum p=(0.1 kg)(0.5 m/s)= 0.05 kgm/s
After collision (time 2):
pcb2 = (sin)(pcb1) pgb = (cos)(pcb1) pcb2 = (sin 60o))(0.05kgm/s) pgb = (cos 60o))(0.05kgm/s)pcb2 = 0.0433 kgm/s pgb = 0.025 kgm/s
vcb2 = 0. 433 m/s vgb = 0. 25 m/s
Cueball-1
GreenballCueball-2
60o
Conservation of Momentum in
2-D
0.1 kg ballRolls at 0.5 m/s
Cueball-1
GreenballCueball-2
60o
0.25 m/s
0.433 m/s
So, I looked this over…
• No this is right…it seems counterintuitive but it checks
• Momentum is conserved here because these are in different directions, their vector sum is the same as the original input momentum
• And, if you check the sum total kinetic energy of the system KE = 1/2 mv2, that too is conserved.
Impulse in Rocket Flight
• A rocket engine provides thrust force over a short time interval
• Solid fuel rocket engines are rated in letters
So let’s say I use an A8-3 engine on a 45
gram rocket• F∆t = m∆v• 2.5 N-s = (.045kg) ∆v• ∆v = 55.6 m/s
• How much acceleration?
• F=ma• 8N = (.045 kg) a• a = 177.8 m/s2 -9.81 m/s2
• a = 168 m/s2
How far up does it get before it coasts and then in total before
*?• There are 2 phases to the flight• v2 = vo
2 + 2a(d-do)• (55.6 m/s)2 = 02 + 2(168m/s 2)(d-do)
• d = 9.2 m (under acceleration)
• Then its simple ballistic flight for 3 s
• d = do + vot + 1/2at2
• d = 9.2m + (55.6m/s)(3s) + 1/2(-9.8m/s2)(3s)2
• d = 131.9 m total height attained
Multiple stage rockets drop excess mass during the flight.
What about calculating theHeight attained by a rocket that has multiple stages?
These have three phases,Initial acceleration at mr+b
With the the thrust of the initial engine C-6-0, no coasting time
Then an acceleration and coast phase for the rocket mass without booster mr
Release of booster from second stage
So, currently under construction in my laboratory is this kit:
We will mass and launch this on Friday,weather permitting
We will calculate the booster, upper stage, and parachute deployment heights of this Two-stage rocket.
We must mass the rocket parts and record the Specs of the Engines used
We must have several students sight and record angles and horizontal observation Distances. Then share the data Monday.
Angular Momentum
The spinning “beacon” of a neutron star can make it a “pulsar” as observed from Earth
http://www.jb.man.ac.uk/~pulsar/Education/Sounds/sounds.html
Radiotelescopes
So, lets say I have a massive star, 10x the massof our sun. It runs out ofhydrogen fuel collapses andexplodes most of its mass into space in a supernova.
The core of the star has a Mass 1.5 x that of our sun.3 x 1030kg. Its initial radiusis 7x108 m it collapses to 2x104 m as the matter is compressed into neutrons.
What is the velocity of the surfaceof the neutron star?
Rotation speed of a star
v = 2πr T
v = 2π( 7 x 108m) 30d x 24h/d x 3600s/h
Sunspots rotate in 30 d
v = 1700 m/s
Conservation of angular momentum () = mvr
m1v1r1 = m2v2r2
(3 x 1030 kg) (1700m/s) (7 x 108m) = (3 x 1030 kg) v2 (2 x 104m)
6 x 107 m/s = v2If the speed of light is 3 x 108 m/s its about 20% of light speed
v = 2πr T6 x 107 m/s = 2π (2 x 104m) TT = 0.002 sec…. http://www.jb.man.ac.uk/~pulsar/Education/Sounds/crab.au