51
Momentum Chapter-6

Momentum

  • Upload
    marlie

  • View
    16

  • Download
    1

Embed Size (px)

DESCRIPTION

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

Citation preview

Page 1: Momentum

Momentum

Chapter-6

Page 2: Momentum

Momentum

• Symbol is lower case p

• Momentum is a product of mass and velocity

• p = mv

Page 3: Momentum

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

Page 4: Momentum
Page 5: Momentum

82,288 kg x 0.02m/s = 1600 kgm/s

Page 6: Momentum

100kg astronaut in a 60 kg suit movingAt 10 m/s

1600 kg m/s

Page 7: Momentum

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

Page 8: Momentum

1600 kgm/s astronaut grabs a 100 kg

Sputnik, how fast do both go?

10 m/s

Page 9: Momentum

m1v1 = m2v2

1600 kgm/s = 260 kg v2

v2 = 6.2 m/s

Page 10: Momentum
Page 11: Momentum

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

Page 12: Momentum

Explosions between vehicles

Page 13: Momentum

Recoil

Page 14: Momentum

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

Page 15: Momentum

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

Page 16: 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

Page 17: Momentum

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

Page 18: Momentum

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?

Page 19: Momentum

(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

Page 20: Momentum

So we use straw bales around race tracks.

… and some soft squishy spectators.

Page 21: Momentum

(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

Page 22: Momentum

Billiards: the break

Page 23: Momentum

1-D conservation of momentum

Page 24: Momentum

Very few shots line up perfectly

Page 25: Momentum

Momentum of the constituents before and after contact is equal

Page 26: Momentum

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.

Page 27: Momentum

Conservation of Momentum in

2-D

0.1 kg ballRolls at 0.5 m/s

Cueball-1

GreenballCueball-2

60o

Page 28: Momentum

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

Page 29: Momentum

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

Page 30: Momentum

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.

Page 31: Momentum
Page 32: Momentum

Impulse in Rocket Flight

• A rocket engine provides thrust force over a short time interval

• Solid fuel rocket engines are rated in letters

Page 33: Momentum
Page 34: Momentum
Page 35: Momentum
Page 36: Momentum
Page 37: Momentum

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

Page 38: Momentum

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

Page 39: Momentum

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

Page 40: Momentum

Release of booster from second stage

Page 41: Momentum

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.

Page 42: Momentum

Angular Momentum

Page 43: Momentum
Page 44: Momentum
Page 45: Momentum

The spinning “beacon” of a neutron star can make it a “pulsar” as observed from Earth

Page 47: Momentum

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?

Page 48: Momentum

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

Page 49: Momentum

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

Page 50: Momentum
Page 51: Momentum