Rotational Kinematics and Energy

Slides:



Advertisements
Similar presentations
Rotational Kinematics
Advertisements

Angular Momentum The vector angular momentum of the point mass m about the point P is given by: The position vector of the mass m relative to the point.
Rotational Motion Chapter Opener. Caption: You too can experience rapid rotation—if your stomach can take the high angular velocity and centripetal acceleration.
ConcepTest 9.1bBonnie and Klyde II Bonnie Klyde 1 ) Klyde 2) Bonnie 3) both the same 4) linear velocity is zero for both of them Bonnie sits on the outer.
Torque and Rotational Equilibrium Chapter 8. Torque Rotational equivalent of force Rotational equivalent of force Force isn’t enough to provide a rotation.
Physics: Principles with Applications, 6th edition
Chapter 10 Rotational Motion and Torque Angular Position, Velocity and Acceleration For a rigid rotating object a point P will rotate in a circle.
Rotational Kinematics
Physics 111: Mechanics Lecture 09
Rotational Motion Lecturer: Professor Stephen T. Thornton
Rotational Dynamics October 24, 2005.
Rotational Kinematics
Chapter 10 Rotational Motion
Lecture 34, Page 1 Physics 2211 Spring 2005 © 2005 Dr. Bill Holm Physics 2211: Lecture 34 l Rotational Kinematics çAnalogy with one-dimensional kinematics.
Rotational Energy. Rigid Body  Real objects have mass at points other than the center of mass.  Each point in an object can be measured from an origin.
CT1:A ladybug sits at the outer edge of a merry-go-round, and a gentleman bug sits halfway between her and the axis of rotation. The merry-go-round makes.
Ch10-1 Angular Position, Displacement, Velocity and Acceleration Rigid body: every point on the body moves through the same displacement and rotates through.
Chapter 8 Rotational Motion.
Section 8-2: Kinematic Equations Recall: 1 dimensional kinematic equations for uniform (constant) acceleration (Ch. 2). We’ve just seen analogies between.
Rotational Work and Kinetic Energy Dual Credit Physics Montwood High School R. Casao.
© 2007 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for the use of instructors in teaching their.
Rotation about a fixed axis
Chapter 10 Rotational Motion.
Chapter 11 Angular Momentum.
Chapter 9 Rotations of Rigid Bodies Up to this point when studying the motion of objects we have made the (implicit) assumption that these are “point objects”
Chapter 10 Rotational Kinematics and Energy. Units of Chapter 10 Angular Position, Velocity, and Acceleration Rotational Kinematics Connections Between.
Lecture 18 Rotational Motion
Chapter 10 Rotation of a Rigid Object about a Fixed Axis.
ROTATIONAL MOTION AND EQUILIBRIUM
Chapter 10 - Rotation Definitions: –Angular Displacement –Angular Speed and Velocity –Angular Acceleration –Relation to linear quantities Rolling Motion.
Chapter 8 Rotational Motion.
When the axis of rotation is fixed, all particles move in a circle. Because the object is rigid, they move through the same angular displacement in the.
Rotational Kinematics. Angular Position Degrees and revolutions: Angular Position θ > 0 θ < 0.
Chapter 8 Rotational Kinematics. Radians Angular Displacement  Angle through which something is rotated  Counterclockwise => positive(+) Units => radians.
© 2007 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for the use of instructors in teaching their.
Chapter 8 Rotational Motion.
Rotation of a Rigid Object about a Fixed Axis
Chapter 10 Rotational Motion.
Rotational kinematics and energetics
Physics 111: Lecture 17, Pg 1 Physics 111: Lecture 17 Today’s Agenda l Rotational Kinematics çAnalogy with one-dimensional kinematics l Kinetic energy.
Rotational Motion. 6-1 Angular Position, Velocity, & Acceleration.
Force is applied at the handle The axis of rotation is at the nut or bolt The distance away is the length of the handle. Torque direction is either clockwise.
ConcepTest 7.1aBonnie and Klyde I Bonnie Klyde Bonnie sits on the outer rim of a merry-go-round, and Klyde sits midway between the center and the rim.
4.1 Rotational kinematics 4.2 Moment of inertia 4.3 Parallel axis theorem 4.4 Angular momentum and rotational energy CHAPTER 4: ROTATIONAL MOTION.
D. Roberts PHYS 121 University of Maryland Physic² 121: Phundament°ls of Phy²ics I November 1, 2006.
Ch. 9 Rotational Kinematics
Chapter 11 Angular Momentum. The Vector Product and Torque The torque vector lies in a direction perpendicular to the plane formed by the position vector.
ConcepTest 10.1aBonnie and Klyde I Bonnie Klyde Bonnie sits on the outer rim of a merry-go-round, and Klyde sits midway between the center and the rim.
ConcepTest 8.1a Bonnie and Klyde I
Chapter 10 – Rotational Kinematics & Energy – Angular Position (θ) In linear (or translational) kinematics we looked at the position of an object.
Rotation of a Rigid Object About a Fixed Axis 10.
Rotational Motion – Part I AP Physics C. The radian  There are 2 types of pure unmixed motion:  Translational - linear motion  Rotational - motion.
ConcepTest 8.1aBonnie and Klyde I Bonnie Klyde Bonnie sits on the outer rim of a merry-go-round, and Klyde sits midway between the center and the rim.
Ying Yi PhD Chapter 8 Rotational Kinematics 1 PHYS HCC.
Today: (Ch. 8)  Rotational Motion.
Copyright © 2010 Pearson Education, Inc. Lecture Outline Chapter 10 Physics, 4 th Edition James S. Walker.
Cutnell/Johnson Physics 8th edition
Rotational Motion I AP Physics 2. The radian There are 2 types of pure unmixed motion: Translational - linear motion Rotational - motion involving a rotation.
Rotational Motion.
Chapter 8 Rotational Motion
Lecture Outline Chapter 10 Physics, 4th Edition James S. Walker
Chapter 9: Rotational Motion
Rotational Kinematics with Constant Angular Acceleration
Chapter 8 Rotational Motion
Rotational Kinematics and Energy
1. Rotational Kinematics
Chapter 8 Rotational Motion.
Lecture Outline Chapter 10 Physics, 4th Edition James S. Walker
Lecture Outline Chapter 10 Physics, 4th Edition James S. Walker
Chapter 8 Rotational Motion
Presentation transcript:

Rotational Kinematics and Energy Chapter 10 Rotational Kinematics and Energy

Units of Chapter 10 Angular Position, Velocity, and Acceleration Rotational Kinematics Connections Between Linear and Rotational Quantities Rolling Motion Rotational Kinetic Energy and the Moment of Inertia Conservation of Energy

10-1 Angular Position, Velocity, and Acceleration

10-1 Angular Position, Velocity, and Acceleration Degrees and revolutions:

10-1 Angular Position, Velocity, and Acceleration Arc length s, measured in radians:

10-1 Angular Position, Velocity, and Acceleration

10-1 Angular Position, Velocity, and Acceleration

10-1 Angular Position, Velocity, and Acceleration

10-1 Angular Position, Velocity, and Acceleration

10-2 Rotational Kinematics Analogies between linear and rotational kinematics:

Angular Velocity An object at rest begins to rotate with a constant angular acceleration. If this object has angular velocity w at time t, what was its angular velocity at the time 1/2 t? 1) 1/2 w 2) 1/4 w 3) 3/4 w 4) 2 w 5) 4 w

Angular Velocity An object at rest begins to rotate with a constant angular acceleration. If this object has angular velocity w at time t, what was its angular velocity at the time 1/2 t? 1) 1/2 w 2) 1/4 w 3) 3/4 w 4) 2 w 5) 4 w The angular velocity is w = at (starting from rest), and there is a linear dependence on time. Therefore, in half the time, the object has accelerated up to only half the speed.

Example The angular speed of a propeller on a boat increases with constant acceleration from 12 rad/s to 26 rad/s in 2.5 revolutions. What is the acceleration of the propeller? How long did the change in angular speed take?

10-3 Connections Between Linear and Rotational Quantities

Tangential Speed

10-3 Connections Between Linear and Rotational Quantities

10-3 Connections Between Linear and Rotational Quantities

10-3 Connections Between Linear and Rotational Quantities This merry-go-round has both tangential and centripetal acceleration.

Bonnie and Klyde Bonnie sits on the outer rim of a merry-go-round, and Klyde sits midway between the center and the rim. The merry-go-round makes one revolution every two seconds. Who has the larger linear (tangential) velocity? 1) Klyde 2) Bonnie 3) both the same 4) linear velocity is zero for both of them [CORRECT 5 ANSWER] w Bonnie Klyde

Bonnie and Klyde Bonnie sits on the outer rim of a merry-go-round, and Klyde sits midway between the center and the rim. The merry-go-round makes one revolution every two seconds. Who has the larger linear (tangential) velocity? 1) Klyde 2) Bonnie 3) both the same 4) linear velocity is zero for both of them Their linear speeds v will be different since v = Rw and Bonnie is located further out (larger radius R) than Klyde. w Bonnie Klyde Follow-up: Who has the larger centripetal acceleration?

10-4 Rolling Motion If a round object rolls without slipping, there is a fixed relationship between the translational and rotational speeds:

10-4 Rolling Motion We may also consider rolling motion to be a combination of pure rotational and pure translational motion:

10-5 Rotational Kinetic Energy and the Moment of Inertia For this mass,

10-5 Rotational Kinetic Energy and the Moment of Inertia We can also write the kinetic energy as Where I, the moment of inertia, is given by

10-5 Rotational Kinetic Energy and the Moment of Inertia Moments of inertia of various regular objects can be calculated:

10-6 Conservation of Energy The total kinetic energy of a rolling object is the sum of its linear and rotational kinetic energies: The second equation makes it clear that the kinetic energy of a rolling object is a multiple of the kinetic energy of translation.

10-6 ConcepTest If these two objects, of the same mass and radius, are released simultaneously, which will reach the ground first? Hoop Disc

10-6 ConcepTest If these two objects, of the same mass and radius, are released simultaneously, which will reach the ground first? Hoop Disc

Example – Real Atwood’s Machine The two masses (m1 = 5.0 kg and m2 = 3.0 kg) in the Atwood’s machine shown in the figure are released from rest, with m1 at a height of 0.75 m above the floor. When m1 hits the ground its speed is 1.8 m/s. Assuming that the pulley is a uniform disc with a radius of 12 cm, find the mass of the pulley. Assume the rope does not slip on the pulley.

Summary of Chapter 10 Describing rotational motion requires analogs to position, velocity, and acceleration Average and instantaneous angular velocity: Average and instantaneous angular acceleration:

Summary of Chapter 10 Period: Counterclockwise rotations are positive, clockwise negative Linear and angular quantities:

Summary of Chapter 10 Linear and angular equations of motion: Tangential speed: Centripetal acceleration: Tangential acceleration:

Summary of Chapter 10 Rolling motion: Kinetic energy of rotation: Moment of inertia: Kinetic energy of an object rolling without slipping: When solving problems involving conservation of energy, both the rotational and linear kinetic energy must be taken into account.