Perfect Rolling (no sliding!) Consider a disk rolling without slipping with a Uniform Acceleration. While most points both rotate and move linearly, the.

Slides:



Advertisements
Similar presentations
Rolling Motion of a Rigid Object
Advertisements

Rolling, Torque, and Angular Momentum
Rotational Inertia & Kinetic Energy
Chapter 11 Angular Momentum
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.
Comparing rotational and linear motion
MSTC Physics Chapter 8 Sections 3 & 4.
Physics 7C lecture 13 Rigid body rotation
Chapter 11 Rolling, Torque, and angular Momentum.
Using the “Clicker” If you have a clicker now, and did not do this last time, please enter your ID in your clicker. First, turn on your clicker by sliding.
Chapter 11: Rolling Motion, Torque and Angular Momentum
2008 Physics 2111 Fundamentals of Physics Chapter 11 1 Fundamentals of Physics Chapter 12 Rolling, Torque & Angular Momentum 1.Rolling 2.The Kinetic Energy.
Chapter 10 Rotational Motion and Torque Angular Position, Velocity and Acceleration For a rigid rotating object a point P will rotate in a circle.
Chapter 12: Rolling, Torque and Angular Momentum.
Rotational Kinematics
Rolling. Rotation and Translation  A rolling wheel is moving forward with kinetic energy.  The velocity is measured at the center of mass. K CM = ½.
D. Roberts PHYS 121 University of Maryland Physic² 121: Phundament°ls of Phy²ics I November 27, 2006.
Rotational Kinetic Energy. Kinetic Energy The kinetic energy of the center of mass of an object moving through a linear distance is called translational.
Physics. Session Rotational Mechanics - 5 Session Objectives.
Rotational Motion Chap NEW CONCEPT ‘Rotational force’: Torque Torque is the “twisting force” that causes rotational motion. It is equal to the.
Work Let us examine the work done by a torque applied to a system. This is a small amount of the total work done by a torque to move an object a small.
Chapter 8 Rotational Motion
Rolling. Rolling Condition – must hold for an object to roll without slipping.
Physics. Session Rotational Mechanics - 6 Session Objectives.
Rotation and angular momentum
Rolling Motion of a Rigid Object AP Physics C Mrs. Coyle.
Rolling A time exposure photo of a rolling disk shows that a point on the edge traces out a curve called a “cycloid”. As the wheel rolls to the right,
Chapter 5 Newton’s Second Law of Motion – Force and Acceleration
Rigid Body: Rotational and Translational Motion; Rolling without Slipping 8.01 W11D1 Today’s Reading Assignment Young and Freedman: 10.3.
Chapters 10, 11 Rotation and angular momentum. Rotation of a rigid body We consider rotational motion of a rigid body about a fixed axis Rigid body rotates.
Rolling, Torque, and Angular Momentum
T071 Q17. A uniform ball, of mass M = kg and radius R = 0
Physics 201: Lecture 19, Pg 1 Lecture 19 Goals: Specify rolling motion (center of mass velocity to angular velocity Compare kinetic and rotational energies.
How do you relate the angular acceleration of the object to the linear acceleration of a particular point? There are actually two perpendicular components.
1 Honors Physics 1 Class 15 Fall 2013 Rolling motion Noninertial reference frames Fictitious forces.
Rotational and Translational Motion Dynamics 8
Rotation Energy Examples Kinetic Energy ( E k ) - The ability to produce change due to an object’s motion. Linear Kinetic EnergyRotational Kinetic Energy.
Rotational kinematics and energetics
 When an extended object, like a wheel, rotates about its axis, the motion cannot be analyzed by treating the object as a particle because at any given.
Rotational and Translational Motion Dynamics 8
1 Work in Rotational Motion Find the work done by a force on the object as it rotates through an infinitesimal distance ds = r d  The radial component.
AP Physics C Montwood High School R. Casao. When a wheel moves along a straight track, the center of the wheel moves forward in pure translation. A point.
Rolling, torque, and angular momentum
Physics 101: Lecture 13, Pg 1 Physics 101: Lecture 13 Rotational Kinetic Energy and Inertia Exam II.
Rotational Inertia & Kinetic Energy AP Phys 1. Linear & Angular LinearAngular Displacementxθ Velocityv  Accelerationa  InertiamI KE½ mv 2 ½ I  2 N2F.
Rolling Motion A time exposure photo of a rolling disk shows that a point on the edge traces out a curve called a “cycloid”. As the wheel rolls to the.
Rigid Body: Rotational and Translational Motion; Rolling without Slipping 8.01 W11D1.
Constant Rotation Now that we know how to define the angular position, we can examine rotational motion. Consider the lab equipment using a view from above.
Rotational Energy Kinetic Energy ( E k ) - The ability to produce change due to an object’s motion. Linear Kinetic EnergyRotational Kinetic Energy.
Phys211C10 p1 Dynamics of Rotational Motion Torque: the rotational analogue of force Torque = force x moment arm  = Fl moment arm = perpendicular distance.
Newton’s First Law of Motion
Rotational Motion.
MOTION & FORCE.
Physics 101: Lecture 13 Rotational Kinetic Energy and Inertia
Chapter 11: Rolling Motion, Torque and Angular Momentum
Dynamics of Rotational Motion
Rotational Inertia & Kinetic Energy
PHYS 1443 – Section 003 Lecture #15
Aim: How do we explain the rolling motion of rigid bodies?
Rotational Motion AP Physics.
Equilibrium and Dynamics
Forces.
Spring 2002 Lecture #15 Dr. Jaehoon Yu Mid-term Results
Chapter 11 Angular Momentum
Forces.
Forces.
Rigid Body: Rotational and Translational Motion; Rolling without Slipping 8.01 W11D1 Today’s Reading Assignment Young and Freedman: 10.3.
Chunk 5 Application of Newton’s Laws
Rigid Body: Rotational and Translational Motion; Rolling without Slipping 8.01 W11D1 Today’s Reading Assignment Young and Freedman:
PHYS 1443 – Section 003 Lecture #15
Presentation transcript:

Perfect Rolling (no sliding!) Consider a disk rolling without slipping with a Uniform Acceleration. While most points both rotate and move linearly, the center of mass is moving linearly with a constant acceleration

Perfect Rolling (no sliding!) Rolling Condition – must hold for an object to roll without slipping. Both a point on the outside of the disk and the center of mass must move the same linear distance, with the same linear velocity and the same linear acceleration for the disk to roll without slipping! Radian measure

Perfect Rolling (no sliding!) One way to view rolling is as a combination of pure rotation and pure translation. Pure Rotation Pure Translation Rolling The point that is in contact with the ground is not in motion with respect to the ground!

Perfect Rolling (no sliding!) Rolling The point that is in contact with the ground is not in motion with respect to the ground! Since the bottom point is at rest with respect to the ground, static friction applies if any friction exists at all. Static friction does not dissipate energy. However, there usually is rolling friction caused by the deformation of the object and surface as well as the loss of pieces of the object. Rolling friction does dissipate energy.

If the disk is moving at constant speed, there is no tendency to slip at the contact point and so there is no frictional force. Both act through the axis of rotation and therefore both exert no torque!

If, however, a force acts on the disk, like when you push on a bike pedal, then there is a tendency to slide at the point of contact so a frictional force acts at that point to oppose that tendency. The force of friction does apply a torque which results in the rolling object accelerating both linearly and rotationally!

Perfect Rolling (no sliding!) Consider a rolling object smoothly accelerating down a hill. If the hill was frictionless, there would not be a force of static friction and therefore the object would slide down the hill instead of roll!

Perfect Rolling (no sliding!) Consider a rolling object smoothly accelerating down a hill.

Perfect Rolling (no sliding!) Consider a rolling object smoothly accelerating down a hill. F N and F g exert no torque since they act through the axis of rotation (cm)

A hoop and a disk with identical masses and radii roll down an incline. How do their motions compare? Perfect Rolling (no sliding!) SoSince they have the same distance to move and both start from rest,

Perfect Rolling (no sliding!) Kinetic Energy ( E k ) - The ability to produce change due to an object’s motion. Translational (Linear) Kinetic EnergyRotational Kinetic Energy

Perfect Rolling (no sliding!) Just as rolling motion can be viewed as a combination of pure rotation and pure translation, the kinetic energy of a rolling object can be viewed as a combination of pure rotational kinetic energy and pure translational kinetic energy. Pure Rotation Pure Translation

A hoop and a disk with identical masses and radii roll down an incline. How do their motions compare? Perfect Rolling (no sliding!) So More of the disk’s kinetic energy will be translational so, System = Object, Incline, Earth But