chapter 10 rotational motion 9-8 center of mass (cm) 9-9 center of mass and translational motion...

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Chapter 10 Rotational Motion 9-8 Center of Mass (CM) 9-9 Center of Mass and Translational Motion 10-1 Angular Quantities 10-2 Vector Nature of Angular Quantities 10-3 Constant Angular Acceleration HW#8: Due Friday, Nov 14 Chap. 9:Pb.10, Pb.25, Pb.35,Pb.50,Pb.56,Pb.64 Look at the example 9-11:Ballistic Pendulum

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Page 1: Chapter 10 Rotational Motion 9-8 Center of Mass (CM) 9-9 Center of Mass and Translational Motion 10-1 Angular Quantities 10-2 Vector Nature of Angular

Chapter 10

Rotational Motion9-8 Center of Mass (CM)9-9 Center of Mass and Translational Motion10-1 Angular Quantities10-2 Vector Nature of Angular Quantities10-3 Constant Angular Acceleration

HW#8: Due Friday, Nov 14Chap. 9:Pb.10, Pb.25, Pb.35,Pb.50,Pb.56,Pb.64

Look at the example 9-11:Ballistic Pendulum

Page 2: Chapter 10 Rotational Motion 9-8 Center of Mass (CM) 9-9 Center of Mass and Translational Motion 10-1 Angular Quantities 10-2 Vector Nature of Angular

9-8 Center of Mass (CM)

In (a), the diver’s motion is pure translation; in (b) it is translation plus rotation.

There is one point that moves in the same path a

particle would take if subjected to the same force as the diver. This point is called the center of mass (CM).

Page 3: Chapter 10 Rotational Motion 9-8 Center of Mass (CM) 9-9 Center of Mass and Translational Motion 10-1 Angular Quantities 10-2 Vector Nature of Angular

9-8 Center of Mass (CM)

The general motion of an object can be considered as the sum of the translational motion of the CM, plus rotational, vibrational, or other forms of motion about the CM.

Page 4: Chapter 10 Rotational Motion 9-8 Center of Mass (CM) 9-9 Center of Mass and Translational Motion 10-1 Angular Quantities 10-2 Vector Nature of Angular

9-8 Center of Mass (CM)

For two particles, the center of mass lies closer to the one with the most mass:

where M is the total mass.

Page 5: Chapter 10 Rotational Motion 9-8 Center of Mass (CM) 9-9 Center of Mass and Translational Motion 10-1 Angular Quantities 10-2 Vector Nature of Angular

9-8 Center of Mass (CM)

Example 9-14: CM of three guys on a raft.

Three people of roughly equal masses m on a lightweight (air-filled) banana boat sit along the x axis at positions xA = 1.0 m, xB = 5.0 m, and xC = 6.0 m, measured from the left-hand end. Find the position of the CM. Ignore the boat’s mass.

Page 6: Chapter 10 Rotational Motion 9-8 Center of Mass (CM) 9-9 Center of Mass and Translational Motion 10-1 Angular Quantities 10-2 Vector Nature of Angular

9-8 Center of Mass (CM)

Exercise 9-15: Three particles in 2-D.

Three particles, each of mass 2.50 kg, are located at the corners of a right triangle whose sides are 2.00 m and 1.50 m long, as shown. Locate the center of mass.

Page 7: Chapter 10 Rotational Motion 9-8 Center of Mass (CM) 9-9 Center of Mass and Translational Motion 10-1 Angular Quantities 10-2 Vector Nature of Angular

9-8 Center of Mass (CM)

For an extended object, we imagine making it up of tiny particles, each of tiny mass, and adding up the product of each particle’s mass with its position and dividing by the total mass. In the limit that the particles become infinitely small, this gives:

Page 8: Chapter 10 Rotational Motion 9-8 Center of Mass (CM) 9-9 Center of Mass and Translational Motion 10-1 Angular Quantities 10-2 Vector Nature of Angular

9-8 Center of Mass (CM)

Example 9-17: CM of L-shaped flat object.

Determine the CM of the uniform thin L-shaped construction brace shown.

Page 9: Chapter 10 Rotational Motion 9-8 Center of Mass (CM) 9-9 Center of Mass and Translational Motion 10-1 Angular Quantities 10-2 Vector Nature of Angular

9-8 Center of Mass (CM)

The center of gravity is the point at which the gravitational force can be considered to act. It is the same as the center of mass as long as the gravitational force does not vary among different parts of the object.

Page 10: Chapter 10 Rotational Motion 9-8 Center of Mass (CM) 9-9 Center of Mass and Translational Motion 10-1 Angular Quantities 10-2 Vector Nature of Angular

9-8 Center of Mass (CM)

The center of gravity can be found experimentally by suspending an object from different points. The CM need not be within the actual object—a doughnut’s CM is in the center of the hole.

Page 11: Chapter 10 Rotational Motion 9-8 Center of Mass (CM) 9-9 Center of Mass and Translational Motion 10-1 Angular Quantities 10-2 Vector Nature of Angular

9-9 Center of Mass and Translational Motion

The total momentum of a system of particles is equal to the product of the total mass and the velocity of the center of mass.

The sum of all the forces acting on a system is equal to the total mass of the system multiplied by the acceleration of the center of mass:

Therefore, the center of mass of a system of particles (or objects) with total mass M moves like a single particle of mass M acted upon by the same net external force.

Page 12: Chapter 10 Rotational Motion 9-8 Center of Mass (CM) 9-9 Center of Mass and Translational Motion 10-1 Angular Quantities 10-2 Vector Nature of Angular

10-1 Angular Quantities

In purely rotational motion, all points on the object move in circles around the axis of rotation (“O”). The radius of the circle is R. All points on a straight line drawn through the axis move through the same angle in the same time. The angle θ in radians is defined:

where l is the arc length.

,l

R

Page 13: Chapter 10 Rotational Motion 9-8 Center of Mass (CM) 9-9 Center of Mass and Translational Motion 10-1 Angular Quantities 10-2 Vector Nature of Angular

Example 10-1: Birds of prey—in radians.

A particular bird’s eye can just distinguish objects that subtend an angle no smaller than about 3 x 10-4 rad. (a) How many degrees is this? (b) How small an object can the bird just distinguish when flying at a height of 100 m?

10-1 Angular Quantities

Page 14: Chapter 10 Rotational Motion 9-8 Center of Mass (CM) 9-9 Center of Mass and Translational Motion 10-1 Angular Quantities 10-2 Vector Nature of Angular

Angular displacement:

The average angular velocity is defined as the total angular displacement divided by time:

The instantaneous angular velocity:

10-1 Angular Quantities

Page 15: Chapter 10 Rotational Motion 9-8 Center of Mass (CM) 9-9 Center of Mass and Translational Motion 10-1 Angular Quantities 10-2 Vector Nature of Angular

The angular acceleration is the rate at which the angular velocity changes with time:

The instantaneous acceleration:

10-1 Angular Quantities

Page 16: Chapter 10 Rotational Motion 9-8 Center of Mass (CM) 9-9 Center of Mass and Translational Motion 10-1 Angular Quantities 10-2 Vector Nature of Angular

Every point on a rotating body has an angular velocity ω and a linear velocity v.

They are related:

10-1 Angular Quantities

Page 17: Chapter 10 Rotational Motion 9-8 Center of Mass (CM) 9-9 Center of Mass and Translational Motion 10-1 Angular Quantities 10-2 Vector Nature of Angular

Questio

n• Two objects are sitting on a horizontal

table that is undergoing uniform circular motion. Assuming the objects don’t slip, which of the following statements is true?

• A) Objects 1 and 2 have the same linear velocity, v, and the same angular velocity, .

• B) Objects 1 and 2 have the same linear velocity, v, and the different angular velocities, .

• C) Objects 1 and 2 have different linear velocities, v, and the same angular velocity, .

• D) Objects 1 and 2 have different linear velocities, v, and the different angular velocities, .

1

2