Chapter 8 Rotational Motion Rotational Motion n Angular

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Chapter 8 Rotational Motion

Chapter 8 Rotational Motion

Rotational Motion n Angular Distance (q) o Replaces distance for rotational motion o Measured

Rotational Motion n Angular Distance (q) o Replaces distance for rotational motion o Measured in n Degrees n Radians n Revolutions q

Radian Measure r r 1 rad = 57. 3 degrees 2 p rad in

Radian Measure r r 1 rad = 57. 3 degrees 2 p rad in one circle

Windows Calculator

Windows Calculator

Rotational Motion n Speed of Rotation (w) o w = Angle covered/Time required o

Rotational Motion n Speed of Rotation (w) o w = Angle covered/Time required o o = Dq/Dt Note similarity to v = Dx/Dt o Measured in degrees/second n radians/second n revolutions/second n w

Rotational Motion v Angular Acceleration - Measures how angular velocity is changing (a) o

Rotational Motion v Angular Acceleration - Measures how angular velocity is changing (a) o a = Dw/Dt Note similarity to a = Dv/Dt o Measured in … degrees/s 2 n radians/s 2 n revolutions/s 2 n

Rotational Inertia n Property of an object that resists changes in rotation • For

Rotational Inertia n 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

Moments of Inertia n Depends on … o Mass of the Object o Axis

Moments of Inertia n Depends on … o Mass of the Object o Axis of Rotation o Distribution of Mass in the Object

Moments of Inertia Standard Shapes

Moments of Inertia Standard Shapes

Moment of Inertia Bars v Ring and Disk on Incline v Metronome v People

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

Torque n Product of Force and Lever Arm o Torque = Force X Lever

Torque n Product of Force and Lever Arm o Torque = Force X Lever Arm n Examples: o Balance o See-Saw o Wrench

W 1 d 1 = W 2 d 2

W 1 d 1 = W 2 d 2

Sample Torque Problem (0. 5 kg)(9. 8 m/s 2)(0. 1 m) = (0. 2

Sample Torque Problem (0. 5 kg)(9. 8 m/s 2)(0. 1 m) = (0. 2 kg)(9. 8 m/s 2)d

F Line of Action Lever Arm

F Line of Action Lever Arm

Torque Examples

Torque Examples

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

Torque n n Just as unbalanced forces produce acceleration, unbalanced torques produce angular acceleration. Compare: SF = ma St = Ia

Center of Mass n Average position of the mass of an object o Newton

Center of Mass n 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

Finding the Center of Mass Line of action Pivot point Lever arm Torque weight

Finding the Center of Mass Line of action Pivot point Lever arm Torque weight No Torque

High Jumper

High Jumper

Stability n n In order to balance forces and torques, the center of mass

Stability n n 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

Stability Base of Support

Stability Base of Support

Stability n Which object is most stable?

Stability n Which object is most stable?

Centripetal Force n n Any force that causes an object to move in a

Centripetal Force n n 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

Centripetal force F = mac 2 = mv /r 2 = mrw

Centripetal force F = mac 2 = mv /r 2 = mrw

Centrifugal force n Fictitious center fleeing force o Felt by object in an accelerated

Centrifugal force n Fictitious center fleeing force o Felt by object in an accelerated reference frame n Examples: o Car on a circular path o Can on a string

Space Habitat (simulated gravity) w r

Space Habitat (simulated gravity) w r

Space Habitat (simulated gravity) n n “Down” is away from the center The amount

Space Habitat (simulated gravity) n n “Down” is away from the center The amount of “gravity” depends on how far from the center you are.

Angular Momentum L = (rotational inertia) X (angular velocity) L = Iw Compare to

Angular Momentum L = (rotational inertia) X (angular velocity) L = Iw Compare to linear momentum: p = mv

Linear Momentum and Force Angular Momentum and Torque n Linear o Impulse n Rotational

Linear Momentum and Force Angular Momentum and Torque n Linear o Impulse n Rotational o Rotational Impulse SF = Dp/Dt Dp = SF Dt St = DL/ Dt DL = St Dt

Conservation of Momentum n Linear o If SF = 0, then p is constant.

Conservation of Momentum n Linear o If SF = 0, then p is constant. n Angular o If St = 0, then L is constant.

Conservation of Angular Momentum n n n Ice Skater Throwing a football Rifling Helicopters

Conservation of Angular Momentum n n n Ice Skater Throwing a football Rifling Helicopters Precession

Rifling

Rifling

Football Physics L

Football Physics L

Helicopter Physics Rotation of Rotor Body Rotation Tail rotor used to produce thrust in

Helicopter Physics Rotation of Rotor Body Rotation Tail rotor used to produce thrust in opposite direction of body rotation

Precession

Precession

Age of Aquarius

Age of Aquarius

Linear - Rotational Connections Linear x (m) Rotational q (rad) v (m/s) w (rad/s)

Linear - Rotational Connections Linear x (m) Rotational q (rad) v (m/s) w (rad/s) a (m/s 2) a (rad/s 2) m (kg) F (N) I (kg·m 2) t (N·m) p (N·s) L (N·m·s)