Physics 101: Lecture 15, Pg 1 Physics 101: Lecture 15 Rolling Objects l Today’s lecture will cover Textbook Chapter 8.5-8.7 Exam III.

Slides:



Advertisements
Similar presentations
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 a.
Advertisements

Classical Mechanics Review 3, Units 1-16
Physics 101: Lecture 13 Rotational Kinetic Energy and Inertia
Two-Dimensional Rotational Dynamics W09D2. Young and Freedman: 1
Torque and Equilibrium
Torque Looking back Looking ahead Newton’s second law.
Physics 106: Mechanics Lecture 04
MSTC Physics Chapter 8 Sections 3 & 4.
Chapter 9 Rotational Dynamics.
Physics 203 College Physics I Fall 2012
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.
Torque Torque and golden rule of mechanics Definition of torque r F
Physics 101: Lecture 8, Pg 1 Centripetal Acceleration and Circular Motion Physics 101: Lecture 08 l Today’s lecture will cover Chapter 5 Exam II Problems.
PHY131H1S - Class 20 Today: Gravitational Torque Rotational Kinetic Energy Rolling without Slipping Equilibrium with Rotation Rotation Vectors Angular.
Physics Montwood High School R. Casao
A 40-kg mass placed 1.25 m on the opposite side of the support point balances a mass of 25 kg, placed (x) m from the support point of a uniform beam. What.
Lecture 37, Page 1 Physics 2211 Spring 2005 © 2005 Dr. Bill Holm Physics 2211: Lecture 37 l Work and Kinetic Energy l Rotational Dynamics Examples çAtwood’s.
Physics 111: Mechanics Lecture 10 Dale Gary NJIT Physics Department.
Torque and Angular Momentum
Physics 207: Lecture 17, Pg 1 Lecture 17 Goals: Chapter 12 Chapter 12  Define center of mass  Analyze rolling motion  Introduce and analyze torque 
Schedule Mechanics Lecture 14, Slide 1 Midterm 3 Friday April 24 Collisions and Rotations Units Final Exam Units 1-19 Section 001 Section 002.
Physics 2211: Lecture 38 Rolling Motion
Chapter 11 Rolling, Torque, and Angular Momentum In this chapter we will cover the following topics: -Rolling of circular objects and its relationship.
Physics 218, Lecture XX1 Physics 218 Lecture 20 Dr. David Toback.
Department of Physics and Applied Physics , F2010, Lecture 19 Physics I LECTURE 19 11/17/10.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lectures 24, 25 Hw: Chapter 15 problems and exercises.
D. Roberts PHYS 121 University of Maryland Physic² 121: Phundament°ls of Phy²ics I November 20, 2006.
Rotational Dynamics Example
Classical Mechanics Review 4: Units 1-19
Physics. Session Rotational Mechanics - 5 Session Objectives.
Physics. Session Rotational Mechanics - 6 Session Objectives.
Wed. March 9th1 PHSX213 class Class stuff –HW6W returned. –HW7. Worth 1.5 times normal assignment. Due Wed Mar. 16 th 6PM. –Practice Exam. –Projects …
Rotational KE, Angular Momentum
Physics 101: Lecture 16, Pg 1 Physics 101: Lecture 16 Angular Momentum Today’s lecture will cover Textbook Chapter Exam II.
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.
Torque Chap 8 Units: m N 2.
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.
1 7/26/04 Midterm 2 – Next Friday (7/30/04)  Material from Chapters 7-12 I will post a practice exam on Monday Announcements.
Chapter 8 Rotational Motion.
Equations for Projectile Motion
Torque Calculations with Pulleys
Rotational Motion. Angular Quantities Angular Displacement Angular Speed Angular Acceleration.
Rotational Dynamics Chapter 8 Section 3.
The center of gravity of an object is the point at which its weight can be considered to be located.
Rotational Dynamics Chapter 11.
Rotational Motion. 6-1 Angular Position, Velocity, & Acceleration.
Physics 101: Lecture 13, Pg 1 Physics 101: Lecture 13 Rotational Kinetic Energy and Rotational Inertia Exam II.
Lecture 14: Rolling Objects l Rotational Dynamics l Rolling Objects and Conservation of Energy l Examples & Problem Solving.
Today’s Concepts: a) Rolling Kinetic Energy b) Angular Acceleration
Lecture 13: Rotational Kinetic Energy and Rotational Inertia l Review: Rotational Kinematics l Rotational Kinetic Energy l Rotational Inertia l Torque.
Physics 101: Lecture 13, Pg 1 Physics 101: Lecture 13 Rotational Kinetic Energy and Inertia Exam II.
Angular Displacement, Velocity, and Acceleration Rotational Energy Moment of Inertia Torque Work, Power and Energy in Rotational Motion.
Two-Dimensional Rotational Dynamics 8.01 W09D2 Young and Freedman: 1.10 (Vector Product), , 10.4, ;
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 101: Lecture 13, Pg 1 Physics 101: Lecture 13 Rotational Kinetic Energy and Inertia l Today’s lecture will cover Textbook Section 8.1.
Rotational Dynamics The Action of Forces and Torques on Rigid Objects
Rotational Dynamics.
Two-Dimensional Rotational Dynamics 8.01 W09D2
Physics 101: Lecture 13 Rotational Kinetic Energy and Inertia
General Physics I Rotational Motion
Physics 101: Lecture 15 Rolling Objects
Physics 101: Lecture 15 Rolling Objects
Rotational Inertia & Kinetic Energy
Torque and Equilibrium
Equilibrium and Dynamics
Newton’s 2nd Law for Rotation
Presentation transcript:

Physics 101: Lecture 15, Pg 1 Physics 101: Lecture 15 Rolling Objects l Today’s lecture will cover Textbook Chapter Exam III

Physics 101: Lecture 15, Pg 2Overview l Review  K rotation = ½ I  2 è Torque = Force that causes rotation  = F r sin  è Equilibrium  F = 0  = 0 l Today   = I    nergy conservation revisited 05

Physics 101: Lecture 15, Pg 3 Linear and Angular LinearAngular Displacement x  Velocity v  Acceleration a  Inertia mI KE ½ m v2 ½ I  2 N2L F=ma  = I  Momentum p = mv L = I  Today 08

Physics 101: Lecture 15, Pg 4 Rotational Form Newton’s 2 nd Law  = I  è Torque is amount of twist provide by a force »Signs: positive = CCW è Moment of Inertial like mass. Large I means hard to start or stop from spinning. l Problems Solved Like N2L è Draw FBD è Write N2L 09

Physics 101: Lecture 15, Pg 5 The Hammer! You want to balance a hammer on the tip of your finger, which way is easier A) Head up B) Head down C) Same 15 30% 64% 6% by putting it [the head] towards you finger there is less torque due to gravity If the most mass is farther from the axis of rotation (my finger), the moment of inertia will be greater and less torque will be needed to balance it. This is mainly from personal experience. I don't have a great physics answer. But I believe that it has something to do with the distance of the mass from the finger. For some reason, a greater distance makes it easier to balance. WHY is this person balancing a hammer...shouldn't they be doing work!?!

Physics 101: Lecture 15, Pg 6 The Hammer! You want to balance a hammer on the tip of your finger, which way is easier A) Head up B) Head down C) Same  = I  m g R sin(  ) = mR 2  mg R Torque increases with R Inertia increases as R 2 g sin(  ) / R =  Angular acceleration decreases with R! So large R is easier to balance % 64% 6%

Physics 101: Lecture 15, Pg 7 Falling weight & pulley l A mass m is hung by a string that is wrapped around a pulley of radius R attached to a heavy flywheel. The moment of inertia of the pulley + flywheel is I. The string does not slip on the pulley. Starting at rest, how long does it take for the mass to fall a distance L. I m R T mg  a L 18 What method should we use to solve this problem A)Conservation of Energy (including rotational)  and then use kinematics Either would work, but since it asks for time, we will use B.

Physics 101: Lecture 15, Pg 8 Falling weight & pulley... For the hanging mass use  F = ma è mg - T = ma For the flywheel use  = I   TR sin(90) = I  Realize that a =  R l Now solve for a using the above equations. I m R T mg  a L 21

Physics 101: Lecture 15, Pg 9 Falling weight & pulley... l Using 1-D kinematics we can solve for the time required for the weight to fall a distance L: I m R T mg  a L where 23

Physics 101: Lecture 15, Pg 10 Tension….. m2 m1 T1T1 T2T2 T 1 < T 2 since T 2 – T 1 = m 2 a. It takes force to accelerate block 2. m3 F m3m3 m1m1 m2m2 T1T1 T2T2 T 2 > T 1 since RT 2 – RT 1 = I 2 . It takes force (torque) to accelerate the pulley. 09 Compare the tensions T 1 and T 2 as the blocks are accelerated to the right by the force F. A) T 1 T 2 Compare the tensions T 1 and T 2 as block 3 falls A) T 1 T 2

Physics 101: Lecture 15, Pg 11Rolling A wheel is spinning clockwise such that the speed of the outer rim is 2 m/s. What is the velocity of the top of the wheel relative to the ground? What is the velocity of the bottom of the wheel relative to the ground? 28 x y You now carry the spinning wheel to the right at 2 m/s. What is the velocity of the top of the wheel relative to the ground? A) -4 m/s B) -2 m/s C) 0 m/s D) +2m/s E) +4 m/s What is the velocity of the bottom of the wheel relative to the ground? A) -4 m/s B) -2 m/s C) 0 m/s D) +2m/s E) +4 m/s + 2 m/s -2 m/s 2 m/s

Physics 101: Lecture 15, Pg 12Rolling An object with mass M, radius R, and moment of inertia I rolls without slipping down a plane inclined at an angle  with respect to horizontal. What is its acceleration? l Consider CM motion and rotation about the CM separately when solving this problem  R I M 29

Physics 101: Lecture 15, Pg 13Rolling... l Static friction f causes rolling. It is an unknown, so we must solve for it. First consider the free body diagram of the object and use  F NET = Ma cm : In the x direction Mg sin  - f = Ma cm Now consider rotation about the CM and use  = I  realizing that  = Rf and a =  R R M  f y x 33 Mg 

Physics 101: Lecture 15, Pg 14 Rolling... We have two equations: Mg sin  - f = Ma l We can combine these to eliminate f:  A R I M For a sphere: 36

Physics 101: Lecture 15, Pg 15 Energy Conservation! l Friction causes object to roll, but if it rolls w/o slipping friction does NO work!  W = F d cos  d is zero for point in contact l No dissipated work, energy is conserved l Need to include both translation and rotation kinetic energy.  K = ½ m v 2 + ½ I  2 38

Physics 101: Lecture 15, Pg 16 Translational + Rotational KE l Consider a cylinder with radius R and mass M, rolling w/o slipping down a ramp. Determine the ratio of the translational to rotational KE. H useand 43 Translational: K T = ½ M v 2 Rotational: K R = ½ I  2 Rotational: K R = ½ (½ M R 2 )  V/R) 2 = ¼ M v 2 = ½ K T

Physics 101: Lecture 15, Pg 17 Rolling Act l Two uniform cylinders are machined out of solid aluminum. One has twice the radius of the other. è If both are placed at the top of the same ramp and released, which is moving faster at the bottom? (a) bigger one (b) smaller one (c) same 48 K i + U i = K f + U f

Physics 101: Lecture 15, Pg 18Summary  = I  l Energy is Conserved è Need to include translational and rotational

Physics 101: Lecture 15, Pg 19 Torque ACT l Which pulley will make it drop fastest? 1) Small pulley 2) Large pulley 3) Same 25 Larger R, gives larger acceleration.