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Ch 9 Linear Momentum and Collisions 9.1 Linear Momentum and Its Conservation Linear – traveling along a path p = mv single particle dp/dt = d(mv)/dt = mdv/dt = ma F net =dp/dt If F net =0, p=0
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Ch 9 Linear Momentum and Collisions 9.1 Linear Momentum and Its Conservation Linear – traveling along a path p = mv single particle dp/dt = d(mv)/dt =

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Page 1: Ch 9 Linear Momentum and Collisions 9.1 Linear Momentum and Its Conservation Linear – traveling along a path p = mv single particle dp/dt = d(mv)/dt =

Ch 9 Linear Momentum and Collisions9.1 Linear Momentum and Its Conservation

Linear – traveling along a path p = mv single particle dp/dt = d(mv)/dt = mdv/dt = ma

Fnet =dp/dt If Fnet =0, p=0

Page 2: Ch 9 Linear Momentum and Collisions 9.1 Linear Momentum and Its Conservation Linear – traveling along a path p = mv single particle dp/dt = d(mv)/dt =

CT1: Two carts of identical inertial mass are put back-to-back on a track. Cart A has a spring loaded piston; cart B is entirely passive. When the piston is released, it pushes against cart B, and

A. A is put in motion but B remains at rest.B. both carts are set into motion, with A gaining more speed than B.C. both carts gain equal speed but in opposite directions.D. both carts are set into motion, with B gaining more speed than A.E. B is put in motion but A remains at rest.

Page 3: Ch 9 Linear Momentum and Collisions 9.1 Linear Momentum and Its Conservation Linear – traveling along a path p = mv single particle dp/dt = d(mv)/dt =

CT2: Two carts are put back-to-back on a track. Cart A has twice the mass of cart B. Cart A has a spring loaded piston; cart B is entirely passive. When the piston is released, it pushes against cart B, and

A. A is put in motion but B remains at rest.B. both carts are set into motion, with A gaining more speed than B.C. both carts gain equal speed but in opposite directions.D. both carts are set into motion, with B gaining more speed than A.E. B is put in motion but A remains at rest.

Page 4: Ch 9 Linear Momentum and Collisions 9.1 Linear Momentum and Its Conservation Linear – traveling along a path p = mv single particle dp/dt = d(mv)/dt =

Internal Forces as Third Law Pairs

Page 5: Ch 9 Linear Momentum and Collisions 9.1 Linear Momentum and Its Conservation Linear – traveling along a path p = mv single particle dp/dt = d(mv)/dt =

External forces and Momentum Conservation

System of Particles (i = 1 to N)

Fneti = dpi/dt ptot = pi

Fneti = Fext + Fint = dpi/dt = dptot/dt

Internal forces occur in third law pairs

so their sum adds to zero.

Fext = dptot/dt

If Fext = 0, then ptot = 0 and

(ptot is conserved)

Page 6: Ch 9 Linear Momentum and Collisions 9.1 Linear Momentum and Its Conservation Linear – traveling along a path p = mv single particle dp/dt = d(mv)/dt =

ptot = pi

Fext = dptot/dt

If Fext = 0, then ptot = 0

P9.4 (p.260)

Page 7: Ch 9 Linear Momentum and Collisions 9.1 Linear Momentum and Its Conservation Linear – traveling along a path p = mv single particle dp/dt = d(mv)/dt =

The Average Force During a Collision

Page 8: Ch 9 Linear Momentum and Collisions 9.1 Linear Momentum and Its Conservation Linear – traveling along a path p = mv single particle dp/dt = d(mv)/dt =

Ch9 Linear Momentum and Collisions9.2 Impulse and Momentum I = Impulse (a vector) I = Area under F vs. t curve

I = Favt = (ptot/t)t = ptot

Page 9: Ch 9 Linear Momentum and Collisions 9.1 Linear Momentum and Its Conservation Linear – traveling along a path p = mv single particle dp/dt = d(mv)/dt =

P9.9 (p.261)

Page 10: Ch 9 Linear Momentum and Collisions 9.1 Linear Momentum and Its Conservation Linear – traveling along a path p = mv single particle dp/dt = d(mv)/dt =

PHYS201F07 Exam2Average 62 Lo 9.5 Hi 100

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Page 11: Ch 9 Linear Momentum and Collisions 9.1 Linear Momentum and Its Conservation Linear – traveling along a path p = mv single particle dp/dt = d(mv)/dt =

PHYS201F07 TotalAverage 68 Lo 23 Hi 98

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Page 12: Ch 9 Linear Momentum and Collisions 9.1 Linear Momentum and Its Conservation Linear – traveling along a path p = mv single particle dp/dt = d(mv)/dt =

CT3: A ball is dropped onto the floor below. Which of the following statements is true while the ball falls (neglect air resistance)? Consider the system as just the ball.

A. Momentum is conserved for the ball, but energy is not.

B. Energy is conserved for the ball, but momentum is not.

C. Both energy and momentum are conserved for the ball.

D. Neither energy nor momentum is conserved for the ball.

Page 13: Ch 9 Linear Momentum and Collisions 9.1 Linear Momentum and Its Conservation Linear – traveling along a path p = mv single particle dp/dt = d(mv)/dt =

A. abc

B. acb

C. bca

D. bac

E. cba

F. cab

Rank greatest to least

Concept Question 4

Page 14: Ch 9 Linear Momentum and Collisions 9.1 Linear Momentum and Its Conservation Linear – traveling along a path p = mv single particle dp/dt = d(mv)/dt =

CT6: Two carts are put back-to-back on a track. Cart A has a spring-loaded piston; cart B, which has twice the inertial mass of cart A, is entirely passive. When the piston is released, it pushes against cart B, and the carts move apart. How do the magnitudes of the final momenta and kinetic energies compare?

A. pA > pB; kA > kB

B. pA > pB; kA = kB

C. pA > pB; kA < kB

D. pA = pB; kA > kB

E. pA = pB; kA = kB

F. pA = pB; kA < kB

G. pA < pB; kA > kB

H. pA < pB; kA = kB

I. pA < pB; kA < kB

Page 15: Ch 9 Linear Momentum and Collisions 9.1 Linear Momentum and Its Conservation Linear – traveling along a path p = mv single particle dp/dt = d(mv)/dt =

CT5: Two identical looking balls are dropped from the same height (demonstration). Which of the following statements is true throughout the whole process (neglect air resistance)?

A. Momentum is conserved for each of the balls, but energy is not.

B. Energy is conserved for each of the balls, but momentum is not.

C. Neither energy nor momentum is conserved for either ball.

D. Energy and momentum are conserved for both balls. E. Momentum is conserved for one ball, but not the

other. Energy isn’t conserved for either ball. F. Momentum is conserved for one ball, but not the

other. Energy is conserved for both balls. G. Energy is conserved for one ball, but not the other.

Momentum is conserved for both balls. H. Energy is conserved for one ball, but not the other.

Momentum isn’t conserved for either ball.

Page 16: Ch 9 Linear Momentum and Collisions 9.1 Linear Momentum and Its Conservation Linear – traveling along a path p = mv single particle dp/dt = d(mv)/dt =

Ch 9 Linear Momentum and Collisions9.3 Collisions in One Dimension

A. Inelastic CollisionsMomentum is conserved, but energy isn’t. Totally inelastic collision when objects stick together. P9.15 (p.261) P9.16 (p.261)

B. Elastic CollisionsMomentum and energy are both conserved. P9.19 (p.262)

Page 17: Ch 9 Linear Momentum and Collisions 9.1 Linear Momentum and Its Conservation Linear – traveling along a path p = mv single particle dp/dt = d(mv)/dt =

CT7: A golf ball is fired at a bowling ball initially at rest and sticks to it. Compared to the bowling ball, the golf ball after the collision has

A. more momentum but less kinetic energy.B. more momentum and more kinetic energy.C. less momentum and less kinetic energy.D. less momentum but more kinetic energy.E. none of the above

Page 18: Ch 9 Linear Momentum and Collisions 9.1 Linear Momentum and Its Conservation Linear – traveling along a path p = mv single particle dp/dt = d(mv)/dt =

CT8: A golf ball is fired at a bowling ball initially at rest and bounces back elastically. Compared to the bowling ball, the golf ball after the collision has

A. more momentum but less kinetic energy.B. more momentum and more kinetic energy.C. less momentum and less kinetic energy.D. less momentum but more kinetic energy.E. none of the above

Page 19: Ch 9 Linear Momentum and Collisions 9.1 Linear Momentum and Its Conservation Linear – traveling along a path p = mv single particle dp/dt = d(mv)/dt =

Ch 9 Linear Momentum and Collisions9.4 Collisions in Two Dimensions

A. Inelastic CollisionsMomentum is conserved, but energy isn’t. Totally inelastic collision when objects stick together. P9.28 (p.262)B. Elastic CollisionsMomentum and energy are both conserved.

Page 20: Ch 9 Linear Momentum and Collisions 9.1 Linear Momentum and Its Conservation Linear – traveling along a path p = mv single particle dp/dt = d(mv)/dt =

The Center of Mass of Two Objects

Page 21: Ch 9 Linear Momentum and Collisions 9.1 Linear Momentum and Its Conservation Linear – traveling along a path p = mv single particle dp/dt = d(mv)/dt =

Ch 9 Linear Momentum and Collisions9.4 Collisions in Two Dimensions

For several masses

xcm = mixi/M where M = mi

ycm = miyi/M zcm = mizi/M

rcm = miri/M

The mi/M are the weighting factors.

Page 22: Ch 9 Linear Momentum and Collisions 9.1 Linear Momentum and Its Conservation Linear – traveling along a path p = mv single particle dp/dt = d(mv)/dt =

Ch 9 Linear Momentum and Collisions9.4 Collisions in Two Dimensions

vcm = drcm/dt = (midri/dt)/M = mivi/M

Mvcm = mivi = ptot

acm = dvcm/dt = (midvi/dt)/M = miai/M

Macm = Fext + Fint = Fext

Fext = Macm = dptot/dt

If Fext = 0, then ptotal = 0 and ptotal is

conserved.

Page 23: Ch 9 Linear Momentum and Collisions 9.1 Linear Momentum and Its Conservation Linear – traveling along a path p = mv single particle dp/dt = d(mv)/dt =

Consider a system of two particles in the xy plane: m1 = 2.00 kg is at

the location i + 2j m and has a velocity of 3i +0.5j m/s; m2 = 3.00 kg

is at -4i - 3j m and has velocity 3i – 2j m/s. (a) Plot these particles on

a grid or graph paper. Draw their position vectors and show their

velocities. (b) Find the position of the center of mass of the system

and mark it on the grid. (c) Determine the velocity of the center of

mass and also show it on the diagram. (d) What is the total linear

momentum of the system?

Page 24: Ch 9 Linear Momentum and Collisions 9.1 Linear Momentum and Its Conservation Linear – traveling along a path p = mv single particle dp/dt = d(mv)/dt =

P9.57 (p.266)

Find v0