Physics 151: Lecture 22, Pg 1 Physics 151: Lecture 22 Today’s Agenda l Topics çEnergy and RotationsCh. 10.8 çIntro to Rolling MotionCh. 11.

Slides:



Advertisements
Similar presentations
Classical Mechanics Review 3, Units 1-16
Advertisements

Chapter 8: Dynamics II: Motion in a Plane
Rotational Equilibrium and Rotational Dynamics
Review Problems From Chapter 10&11. 1) At t=0, a disk has an angular velocity of 360 rev/min, and constant angular acceleration of rad/s**2. How.
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.
Warm-up: Centripetal Acceleration Practice
Rotational Dynamics Lecturer: Professor Stephen T. Thornton
MSTC Physics Chapter 8 Sections 3 & 4.
Physics 111: Lecture 19, Pg 1 Physics 111: Lecture 19 Today’s Agenda l Review l Many body dynamics l Weight and massive pulley l Rolling and sliding examples.
Physics 7C lecture 13 Rigid body rotation
Physics 101: Lecture 15, Pg 1 Physics 101: Lecture 15 Rolling Objects l Today’s lecture will cover Textbook Chapter Exam III.
Physics 111: Mechanics Lecture 10 Dale Gary NJIT Physics Department.
Physics 201: Lecture 18, Pg 1 Lecture 18 Goals: Define and analyze torque Introduce the cross product Relate rotational dynamics to torque Discuss work.
Chapter 11: Rolling Motion, Torque and Angular Momentum
Rotational Kinematics
Physics 207: Lecture 17, Pg 1 Lecture 17 Goals: Chapter 12 Chapter 12  Define center of mass  Analyze rolling motion  Introduce and analyze torque 
Physics 151: Lecture 23, Pg 1 Physics 151: Lecture 23 Today’s Agenda l Topics çMore on Rolling Motion çCh Angular MomentumCh
Chapter 11 Rolling, Torque, and Angular Momentum In this chapter we will cover the following topics: -Rolling of circular objects and its relationship.
Physics 2 Chapter 10 problems Prepared by Vince Zaccone
Physics 151: Lecture 20, Pg 1 Physics 151: Lecture 20 Today’s Agenda l Topics (Chapter 10) : çRotational KinematicsCh çRotational Energy Ch
Physics 106: Mechanics Lecture 02
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lectures 24, 25 Hw: Chapter 15 problems and exercises.
Halliday/Resnick/Walker Fundamentals of Physics
Physics 151: Lecture 21, Pg 1 Physics 151: Lecture 21 Today’s Agenda l Topics çMoments of InertiaCh çTorqueCh. 10.6, 10.7.
Classical Mechanics Review 4: Units 1-19
Physics. Session Rotational Mechanics - 5 Session Objectives.
Halliday/Resnick/Walker Fundamentals of Physics 8th edition
Chapter 8 Rotational Motion
AP Physics C I.E Circular Motion and Rotation. Centripetal force and centripetal acceleration.
Physics 1501: Lecture 20, Pg 1 Physics 1501: Lecture 20 Today’s Agenda l Announcements çHW#7: due Oct. 21 l Midterm 1: average ~ 45 % … l Topics çMoments.
Chapter 11 Angular Momentum.
Chapter 8: Torque and Angular Momentum
Q10. Rotational Motion.
Rotational Dynamics Just as the description of rotary motion is analogous to translational motion, the causes of angular motion are analogous to the causes.
Chapter 10 - Rotation Definitions: –Angular Displacement –Angular Speed and Velocity –Angular Acceleration –Relation to linear quantities Rolling Motion.
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.
Chapter 8 Rotational Motion.
Physics 207: Lecture 14, Pg 1 Physics 207, Lecture 14, Oct. 23 Agenda: Chapter 10, Finish, Chapter 11, Just Start Assignment: For Wednesday reread Chapter.
Rotation of Rigid Bodies
Rotational and Translational Motion Dynamics 8
2008 Physics 2111 Fundamentals of Physics Chapter 10 1 Fundamentals of Physics Chapter 10 Rotation 1.Translation & Rotation 2.Rotational Variables Angular.
Work, Power and Energy in Rotational Motion AP Physics C Mrs. Coyle.
Rotational Motion. Angular Quantities Angular Displacement Angular Speed Angular Acceleration.
Physics 1501: Lecture 22, Pg 1 Physics 1501: Lecture 22 Today’s Agenda l Announcements çHW#8: due Oct. 28 l Honors’ students çsee me Wednesday at 2:30.
Rotational Motion. 6-1 Angular Position, Velocity, & Acceleration.
Rotational and Translational Motion Dynamics 8
Physics 207: Lecture 16, Pg 1 Lecture 16Goals: Chapter 12 Chapter 12  Extend the particle model to rigid-bodies  Understand the equilibrium of an extended.
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.
Exam is Wednesday at 7:00 pm Remember extra office hours
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.
Physics 207: Lecture 15, Pg 1 Physics 207, Lecture 15, Oct. 25 Agenda: Chapter 11, Finish, Chapter 12, Just Start Assignment: For Monday read Chapter.
Wednesday, Nov. 10, 2004PHYS , Fall 2004 Dr. Jaehoon Yu 1 1.Moment of Inertia 2.Parallel Axis Theorem 3.Torque and Angular Acceleration 4.Rotational.
Angular Displacement, Velocity, and Acceleration Rotational Energy Moment of Inertia Torque Work, Power and Energy in Rotational Motion.
Physics 1501: Lecture 21, Pg 1 Physics 1501: Lecture 21 Today’s Agenda l Announcements çHW#8: due Oct. 28 l Honors’ students çsee me after class l Midterm.
Short Version : 10. Rotational Motion Angular Velocity & Acceleration (Instantaneous) angular velocity Average angular velocity  = angular displacement.
Physics. Session Rotational Mechanics -7 Session Objectives.
Lecture 18: Angular Acceleration & Angular Momentum.
Rotational Inertia & Kinetic Energy AP Phys 1. Linear & Angular LinearAngular Displacementxθ Velocityv  Accelerationa  InertiamI KE½ mv 2 ½ I  2 N2F.
Physics 1D03 - Lecture 351 Review. Physics 1D03 - Lecture 352 Topics to study basic kinematics forces & free-body diagrams circular motion center of mass.
Rotation RETEACH. Main Topics to be Covered Circular Motion  Remember, uniform circular motion- constant velocity Conical Pendulum A ball of mass m.
Classical Mechanics Review 4: Units 1-22
Chapter 11: Rolling Motion, Torque and Angular Momentum
Rotational Inertia & Kinetic Energy
Rotational Motion AP Physics.
Physics 207, Lecture 17, Nov. 1 Work/Energy Theorem, Energy Transfer
Lecture 17 Goals: Chapter 12
CH10 Recitation.
Presentation transcript:

Physics 151: Lecture 22, Pg 1 Physics 151: Lecture 22 Today’s Agenda l Topics çEnergy and RotationsCh çIntro to Rolling MotionCh. 11

Physics 151: Lecture 22, Pg 2 Lecture 22, ACT 1 A campus bird spots a member of an opposing football team (maybe qb) in an amusement park. The football player is on a ride where he goes around at angular velocity  at distance R from the center. The bird flies in a horizontal circle above him. Will a dropping the bird releases while flying directly above the person’s head hit him? a. Yes, because it falls straight down. b. Yes, because it maintains the acceleration of the bird as it falls. c. No, because it falls straight down and will land behind the person. d. Yes, because it mainatins the angular velocity of the bird as it falls. e. No, because it maintains the tangential velocity the bird had at the instant it started falling.

Physics 151: Lecture 22, Pg 3 Example: l You throw a Frisbee of mass m and radius r so that it is spinning about a horizontal axis perpendicular to the plane of the Frisbee. Ignoring air resistance, the torque exerted by gravity is : a. 0. b. mgr. c. 2mgr. d. a function of the angular velocity. e. small at first, then increasing as the Frisbee loses the torque given it by your hand. See text: 10.1

Physics 151: Lecture 22, Pg 4 Example: Rotating Road l A uniform rod of length L=0.5m and mass m=1 kg is free to rotate on a frictionless pin passing through one end as in the Figure. The rod is released from rest in the horizontal position. What is a) angular speed when it reaches the lowest point ? b) initial angular acceleration ? c) initial linear acceleration of its free end ? See example See text: 10.8 L m  = 7.67 rad/s a)  = 30 rad/s 2 b) c) a = 15 m/s 2

Physics 151: Lecture 22, Pg 5 Example 2 l A rope is wrapped around the circumference of a solid disk (R=0.2m) of mass M=10kg and an object of mass m=10 kg is attached to the end of the rope 10m above the ground, as shown in the figure.  M m h =10 m T a)How long will it take for the object to hit the ground ? a)What will be the velocity of the object when it hits the ground ? a)What is the tension on the cord ? 1.7 s 11m/s 32 N

Physics 151: Lecture 22, Pg 6 Connection with CM motion l If an object of mass M is moving at velocity V CM without rotating then its kinetic energy is Recall text 9.6, systems of particles, CM l But what if the object is both moving and rotating? If an object of moment of inertia I CM is rotating in place about its center of mass at angular velocity  then its kinetic energy is animation

Physics 151: Lecture 22, Pg 7 Connection with CM motion... l So for a solid object which rotates about its center of mass and whose CM is moving:  V CM

Physics 151: Lecture 22, Pg 8 Example Problem l Last winter break, one of my students was bored and decided to make up a new game to play in January on the frozen lakes. The idea was to throw a yoyo on to the ice while holding one end of the string. At this point the yoyo is lying flat a distance D away from the bank and still has a length of string L wrapped around the circular part. The idea is to pull the string hard enough so that it gets back on the bank before the string completely unwinds and let loose the yoyo. You want to know the relationship between the amount of string still unwound and the distance to the bank. You note that the yoyo has a mass M, forms a disk of radius R, and you can pull a string with a maximum force F. See text: 11.1

Physics 151: Lecture 22, Pg 9 Example Problem 1. We need to solve for the minimum length of string wrapped around the yoyo when it lies on the ice a distance D from the shore. l For the center of mass, we will use Newton’s Second Law and the constant acceleration kinematics equations. l For the rotational motion, we will use the rotational version of Newton’s Second Law and the constant angular acceleration kinematics equations. Top view See text: 11.1 F MA  R D

Physics 151: Lecture 22, Pg 10 Rolling Motion l Now consider a cylinder rolling at a constant speed. V CM CM The cylinder is rotating about CM and its CM is moving at constant speed (v CM ). Thus its total kinetic energy is given by : animation

Physics 151: Lecture 22, Pg 11 Rolling Motion l Consider again a cylinder rolling at a constant speed. V CM P Q CM  At any instant the cylinder is rotating about point P. Its kinetic energy is given by its rotational energy about that point. K TOT = 1/2 I P  2

Physics 151: Lecture 22, Pg 12 Rolling Motion We can find I P using the parallel axis theorem V CM P Q CM  I P = I CM + MR 2 K TOT = 1/2 (I CM + MR 2 )  2 K TOT = 1/2 I CM  2 + 1/2 M (R 2  2 ) = 1/2 I CM  2 + 1/2 M v CM 2 !

Physics 151: Lecture 22, Pg 13 Example : Rolling Motion l A cylinder is about to roll down an inclined plane. What is its speed at the bottom of the plane ? M  h M v ? Cylinder has radius R M M M M M

Physics 151: Lecture 22, Pg 14 Lecture 22, ACT 4a Rolling Motion l A race !! Two cylinders are rolled down a ramp. They have the same radius but different masses, M 1 > M 2. Which wins the race to the bottom ? A) Cylinder 1 B) Cylinder 2 C) It will be a tie M1  h M? M2

Physics 151: Lecture 22, Pg 15 Lecture 22, ACT 4b Rolling Motion l A race !! Two cylinders are rolled down a ramp. They have the same moment of inertia but different radius, R 1 > R 2. Which wins the race to the bottom ? A) Cylinder 1 B) Cylinder 2 C) It will be a tie R1  h M? R2 animation

Physics 151: Lecture 22, Pg 16 Lecture 22, ACT 4c Rolling Motion l A race !! A cylinder and a hoop are rolled down a ramp. They have the same mass and the same radius. Which wins the race to the bottom ? A) Cylinder B) Hoop C) It will be a tie M1  h M? M2 animation

Physics 151: Lecture 22, Pg 17 Remember our roller coaster. Perhaps now we can get the ball to go around the circle without anyone dying. Note: Radius of loop = R Radius of ball = r

Physics 151: Lecture 22, Pg 18 How high do we have to start the ball ? 1 2 -> The rolling motion added an extra 2/10 R to the height) h h = 2.7 R = (2R + 1/2R) + 2/10 R

Physics 151: Lecture 22, Pg 19 Example: l A mass m = 4.0 kg is connected, as shown, by a light cord to a mass M = 6.0 kg, which slides on a smooth horizontal surface. The pulley rotates about a frictionless axle and has a radius R = 0.12 m and a moment of inertia I = kg m 2. The cord does not slip on the pulley. What is the magnitude of the acceleration of m? a. 2.4 m/s 2 b. 2.8 m/s 2 c.3.2 m/s 2 d. 4.2 m/s 2 e. 1.7 m/s 2 See text: 10.1

Physics 151: Lecture 22, Pg 20 Recap of today’s lecture l Chapter 10, çWork/Energy of Rotational Motion l For next time: Read Chapter 11