v = rω a tan = rα a rad = rω 2 rotation about a moving axis every motion of of a rigid body can...

40

Upload: melinda-marsh

Post on 14-Jan-2016

216 views

Category:

Documents


2 download

TRANSCRIPT

Page 1: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the
Page 2: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the
Page 3: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the
Page 4: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the

v = rω

atan = rα

arad = rω2

22tan radaaa

Page 5: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the

Rotation about a Moving Axis

• Every motion of of a rigid body can be represented

as a combination of motion of the center of mass (translation) and rotation about an axis through the center of mass

• The total kinetic energy can always be represented as the sum of a part associated with motion of the center of mass (treated as a point) plus a part asociated with rotation about an axis through the center of mass

Page 6: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the

Total Kinetic Energy

Ktotal = (1/2)Mvcm2 + (1/2)Icmω2

Page 7: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the

CHAPTER 10DYNAMICS OF ROTATIONAL MOTION

Page 8: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the
Page 9: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the
Page 10: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the
Page 11: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the
Page 12: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the

A plumbing problem

Page 13: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the
Page 14: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the
Page 15: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the
Page 16: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the
Page 17: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the
Page 18: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the

Torque on a pulley

Page 19: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the

Unwinding a winch

Page 20: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the

Rotation about a moving axis

Page 21: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the
Page 22: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the
Page 23: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the
Page 24: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the

Conservation of angular momentum

When the sum of the torques of all external

forces acting on a system is zero, then

THE TOTAL ANGULAR MOMENTUMIS CONSTANT (CONSERVED)

Page 25: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the

The professor as figure skater? •It seems that danger to the instructor is proportional to interest in any given demonstration.

Page 26: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the
Page 27: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the

Internal forces cannot change

the total momentum of a

system.

Page 28: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the
Page 29: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the
Page 30: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the

Balancing on a teeter-totter – Figure 10.25• The

heavier child must sit closer to balance the torque from the smaller child.

•Refer to example 10.11 on page 314.

Page 31: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the

Balanced forces during exercise

Page 32: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the
Page 33: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the
Page 34: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the

A gyroscope in the laboratory

Page 35: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the

A 1.31-kg bowling trophy is held at arm’s length, a distance of 0.505 m from the shoulder joint. What torque does the trophy exert about the shoulder if the arm is (a) horizontal, or (b) at an angle of 20° below the horizontal?

Page 36: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the

A school yard teeter-totter with a total length of 5.2 m and a mass of 36 kg is pivoted at its center. A 18 kg child sits on one end of the teeter-totter.

(a)Where should a parent push vertically

downward with a force of 210 N in order to hold the teeter-totter level?

(b)Where should the parent push with a force of 310 N?

(c)How would your answer to parts (a) and (b) change if the mass of teeter-totter were doubled?

Page 37: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the

Ch 9 Problem 39

The flywheel of a gasoline engine is required to give up 500 J of kinetic energy while its angular velocity decreases from 650 rev/min to 520 rev/min. What moment of inertia is required?

Page 38: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the

Ch 9 Problem 49

A size-5 soccer ball of diameter 22.6 cm and mass 426 g rolls up a hill without slipping, reaching a maximum height of 5.00 m above the base of the hill. We can model this ball as a thin-walled hollow sphere.

(a) At what rate was it rotating at the base of the hill?

(b) How much rotational kinetic energy did it then have?

Page 39: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the

Ch 9. Problem 51

A solid uniform cylinder and a solid uniform sphere, each with the same mass and diameter, approach a hill rolling with a forward speed of 6.50 m/s. Both of them roll up the hill without slipping.

(a) Find the maximum height that each of the centers will reach. (b) Why do they reach different heights? Didn’t both of them have the same speed at the bottom of the hill? (c) Would your answer to part (a) be different if these two objects (1) did not have the same masses or (2) did not have the same diameter? What makes you say this?

Page 40: v = rω a tan = rα a rad = rω 2 Rotation about a Moving Axis Every motion of of a rigid body can be represented as a combination of motion of the

Ch 10 Problem 27

A certain drawbridge can be modeled as a uniform 15,000 N bar, 12.0 m long, pivoted about its lower end. When this bridge is raised to an angle of 60.0 degrees above the horizontal, the cable holding it suddenly breaks, allowing the bridge to fall. At the instant after the cable breaks,

(a) what is this torque on the bridge about the pivot

and (b) at what rate is its angular momentum

changing?