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Chapter 8

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Chapter 8. Rotational Motion. q. Rotational Motion. Angular Distance ( q ) Replaces distance for rotational motion Measured in Degrees Radians Revolutions. Radian Measure. r. r. 1 rad. r. 1 rad = 57.3 degrees 2 p rad in one circle. Windows Calculator. w. Rotational Motion. - PowerPoint PPT Presentation
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Chapter 8 Chapter 8 Rotational Motion Rotational Motion
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Page 1: Chapter 8

Chapter 8Chapter 8

Rotational MotionRotational Motion

Page 2: Chapter 8

Rotational MotionRotational Motion

Angular Distance ()o Replaces distance for rotational motiono Measured in

Degrees

Radians

Revolutions

Page 3: Chapter 8

Radian MeasureRadian Measure

r

r r

1 rad

1 rad = 57.3 degrees

2 rad in one circle

Page 4: Chapter 8

Windows CalculatorWindows Calculator

Page 5: Chapter 8

Rotational MotionRotational Motion

Speed of Rotation () = Angle covered/Time required

o = to Note similarity to v = x/t

o Measured in degrees/second radians/second revolutions/second

Page 6: Chapter 8

Rotational MotionRotational Motion

Angular Acceleration - Measures how angular velocity is changing () = /t Note similarity to a = v/to Measured in …

degrees/s2

radians/s2

revolutions/s2

Page 7: Chapter 8

Rotational InertiaRotational Inertia

Property of an object that resists changes in rotation• For linear motion mass was a measure of

inertia

• For rotational motion Moment of Inertia (I) is the measure of rotational Inertia

Page 8: Chapter 8

Moments of InertiaMoments of Inertia

Depends on …

o Mass of the Object

o Axis of Rotation

o Distribution of Mass in the Object

Page 9: Chapter 8

Moments of InertiaMoments of Inertia

Standard Shapes

Page 10: Chapter 8

Moment of InertiaMoment of Inertia

Inertia Bars Ring and Disk on Incline Metronome People walking Weighted Stick - Bare Stick

Page 11: Chapter 8

TorqueTorque

Product of Force and Lever Armo Torque = Force X Lever Arm

Examples:o Balanceo See-Sawo Wrench

Page 12: Chapter 8

W1d1 = W2d2

Page 13: Chapter 8

Sample Torque ProblemSample Torque Problem

(0.5 kg)(9.8 m/s(0.5 kg)(9.8 m/s22)(0.1 m) = (0.2 kg)(9.8 m/s)(0.1 m) = (0.2 kg)(9.8 m/s22)d)d

m 0.25 d

m) (0.1 kg 0.2kg 0.5

d

Page 14: Chapter 8

Line of Action

Lever Arm

F

Page 15: Chapter 8

Torque ExamplesTorque Examples

Page 16: Chapter 8

TorqueTorque

Just as unbalanced forces produce acceleration, unbalanced torques produce angular acceleration.

Compare:

F = ma = I

Page 17: Chapter 8

Center of MassCenter of Mass

Average position of the mass of an object

o Newton showed that all of the mass of the object acts as if it is located here.

o Find cm of Texas/USA

Page 18: Chapter 8

Finding the Center of MassFinding the Center of Mass

weight

Line of actionPivot point

Lever armTorque

No Torque

Page 19: Chapter 8

High JumperHigh Jumper

Page 20: Chapter 8

StabilityStability

In order to balance forces and torques, the center of mass must always be along the vertical line through the base of support.

Demo• Coke bottle• Chair pick-up

Page 21: Chapter 8

StabilityStability

Base of Support

Page 22: Chapter 8

StabilityStability

Which object is most stable?

Page 23: Chapter 8

Centripetal ForceCentripetal Force

Any force that causes an object to move in a circle.

Examples:• Carousel• Water in a bucket• Moon and Earth• Coin and hanger• Spin cycle

Page 24: Chapter 8

Centripetal forceCentripetal force

F = mac

= mv2/r

= mr2

Page 25: Chapter 8

Centrifugal forceCentrifugal force

Fictitious center fleeing forceo Felt by object in an accelerated reference

frame Examples:

o Car on a circular patho Can on a string

Page 26: Chapter 8

Space Habitat(simulated gravity)

r

Page 27: Chapter 8

Space Habitat(simulated gravity)

“Down” is away from the center The amount of “gravity” depends on

how far from the center you are.

Page 28: Chapter 8

Angular MomentumAngular Momentum

L = (rotational inertia) X (angular velocity)

L = I

Compare to linear momentum:

p = mv

Page 29: Chapter 8

Linear Momentum and ForceLinear Momentum and ForceAngular Momentum and TorqueAngular Momentum and Torque

Linear F =p/to Impulse p = F t

Rotational = L/ to Rotational Impulse L = t

Page 30: Chapter 8

Conservation of MomentumConservation of Momentum

Linearo If F = 0, then p is constant.

Angularo If = 0, then L is constant.

Page 31: Chapter 8

Conservation of Conservation of Angular MomentumAngular Momentum

Ice Skater Throwing a football Rifling Helicopters Precession

Page 32: Chapter 8

RiflingRifling

Page 33: Chapter 8

Football PhysicsFootball Physics

L

Page 34: Chapter 8

Helicopter PhysicsHelicopter Physics

Rotation of Rotor

Body Rotation

Tail rotor used to produce thrust in opposite direction

of body rotation

Page 35: Chapter 8

PrecessionPrecession

Page 36: Chapter 8

Age of AquariusAge of Aquarius

Page 37: Chapter 8

Linear - Rotational ConnectionsLinear - Rotational Connections

Linear Rotational x (m) (rad)

v (m/s) (rad/s)

a (m/s2) (rad/s2)

m (kg) I (kg·m2)F (N) (N·m)

p (N·s) L (N·m·s)


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