Lecture 13 EXAM 2. Today s Topics: Rotational motion Moment of inertia. Tuesday March 8, :15 PM 9:45 PM

Similar documents
Lecture 13. Rotational motion Moment of inertia

Rotational Motion. Lecture 6. Chapter 4. Physics I. Course website:

Chapter 8. Accelerated Circular Motion

r cos, and y r sin with the origin of coordinate system located at

Physics 1114: Unit 5 Hand-out Homework (Answers)

PHYS 1114, Lecture 21, March 6 Contents:

- 5 - TEST 1R. This is the repeat version of TEST 1, which was held during Session.

HW 7 Help. 60 s t. (4.0 rev/s)(1 min) 240 rev 1 min Solving for the distance traveled, we ll need to convert to radians:

Chapter. s r. check whether your calculator is in all other parts of the body. When a rigid body rotates through a given angle, all

ω = θ θ o = θ θ = s r v = rω

Rotational Motion. Every quantity that we have studied with translational motion has a rotational counterpart

Chapter 7-8 Rotational Motion

Physics C Rotational Motion Name: ANSWER KEY_ AP Review Packet

Dynamics of Rotational Motion


OSCILLATIONS AND GRAVITATION

Describing Circular motion

Circular Motion. Mr. Velazquez AP/Honors Physics

PHYSICS 220. Lecture 08. Textbook Sections Lecture 8 Purdue University, Physics 220 1

Circular motion. Objectives. Physics terms. Assessment. Equations 5/22/14. Describe the accelerated motion of objects moving in circles.

Rotational Motion: Statics and Dynamics

Uniform Circular Motion

Lab #9: The Kinematics & Dynamics of. Circular Motion & Rotational Motion

Translation and Rotation Kinematics

Exam 3: Equation Summary

Experiment 09: Angular momentum

b) (5) What average force magnitude was applied by the students working together?

Sections and Chapter 10

Kinematics of rigid bodies

Lab 10: Newton s Second Law in Rotation

Phys 201A. Homework 5 Solutions

Rigid Body Dynamics 2. CSE169: Computer Animation Instructor: Steve Rotenberg UCSD, Winter 2018

Physics 111 Lecture 10. SJ 8th Ed.: Chap Torque, Energy, Rolling. Copyright R. Janow Spring basics, energy methods, 2nd law problems)

10. Force is inversely proportional to distance between the centers squared. R 4 = F 16 E 11.

3.2 Centripetal Acceleration

Answers to test yourself questions

Circular Motion & Torque Test Review. The period is the amount of time it takes for an object to travel around a circular path once.

Midterm Exam #2, Part A

The study of the motion of a body along a general curve. the unit vector normal to the curve. Clearly, these unit vectors change with time, u ˆ

Torque, Angular Momentum and Rotational Kinetic Energy

ROTATORY MOTION HORIZONTAL AND VERTICAL CIRCULAR MOTION

DYNAMICS OF UNIFORM CIRCULAR MOTION

Section 26 The Laws of Rotational Motion

Written as per the revised syllabus prescribed by the Maharashtra State Board of Secondary and Higher Secondary Education, Pune.

AP Physics 1 - Circular Motion and Gravitation Practice Test (Multiple Choice Section) Answer Section

Physics 4A Chapter 8: Dynamics II Motion in a Plane

Objective Notes Summary

Quiz 6--Work, Gravitation, Circular Motion, Torque. (60 pts available, 50 points possible)

c) (6) Assuming the tires do not skid, what coefficient of static friction between tires and pavement is needed?

MAGNETIC FIELD INTRODUCTION

Momentum is conserved if no external force

Conflict Exam Issue. Sorry, Can t do it. Please see Kevin Pitts if you have any additional questions or concerns about this. Office is 231 Loomis

Circular Motion. x-y coordinate systems. Other coordinates... PHY circular-motion - J. Hedberg

Chapter 4. Newton s Laws of Motion

INTRODUCTION. 2. Vectors in Physics 1

Unit 6 Practice Test. Which vector diagram correctly shows the change in velocity Δv of the mass during this time? (1) (1) A. Energy KE.

Kinematics in 2-D (II)

PHYS 1410, 11 Nov 2015, 12:30pm.

CIRCULAR MOTION. Particle moving in an arbitrary path. Particle moving in straight line

Chapter 5. really hard to start the object moving and then, once it starts moving, you don t have to push as hard to keep it moving.

Niraj Sir. circular motion;; SOLUTIONS TO CONCEPTS CHAPTER 7

Math Section 4.2 Radians, Arc Length, and Area of a Sector

Wheel : MC, IC, rc. Pendulum : MB, IB, LB

Name. Date. Period. Engage Examine the pictures on the left. 1. What is going on in these pictures?

Physics 201, Lecture 6

Unit 6 Practice Test. Which vector diagram correctly shows the change in velocity Δv of the mass during this time? (1) (1) A. Energy KE.

10.2 Parametric Calculus

Physics 231 Lecture 17

Chapter 5. Uniform Circular Motion. a c =v 2 /r

PS113 Chapter 5 Dynamics of Uniform Circular Motion

Understanding the Concepts

From Newton to Einstein. Mid-Term Test, 12a.m. Thur. 13 th Nov Duration: 50 minutes. There are 20 marks in Section A and 30 in Section B.

4. Two and Three Dimensional Motion

Physics 231 Lecture 21

When a mass moves because of a force, we can define several types of problem.

Exam 3: Equation Summary

Circular-Rotational Motion Mock Exam. Instructions: (92 points) Answer the following questions. SHOW ALL OF YOUR WORK.

Teachers notes. Beyond the Thrills excursions. Worksheets in this book. Completing the worksheets

Lecture 1a: Satellite Orbits

Chapter 13 Gravitation

Uniform Circular Motion

06 - ROTATIONAL MOTION Page 1 ( Answers at the end of all questions )


Chapter 5: Uniform Circular Motion

ESTIMATION MODELS USING MATHEMATICAL CONCEPTS AND NEWTON S LAWS FOR CONIC SECTION TRAJECTORIES ON EARTH S SURFACE

b) (5) What is the magnitude of the force on the 6.0-kg block due to the contact with the 12.0-kg block?

A car of mass m, traveling at constant speed, rides over the top of a circularly shaped hill as shown.

CHAPTER 5: Circular Motion; Gravitation

B. Spherical Wave Propagation

= 4 3 π( m) 3 (5480 kg m 3 ) = kg.

Physics 201 Lecture 18

Uniform Circular Motion

1121 T Question 1

Physics 111 Lecture 5 Circular Motion

e.g: If A = i 2 j + k then find A. A = Ax 2 + Ay 2 + Az 2 = ( 2) = 6

Chapter 7 Rotational Motion and the Law of Gravity

Between any two masses, there exists a mutual attractive force.

Physics 2A Chapter 10 - Moment of Inertia Fall 2018

AH Mechanics Checklist (Unit 2) AH Mechanics Checklist (Unit 2) Circular Motion

Physics 207 Lecture 5. Lecture 5

Transcription:

Lectue 13 Rotational motion Moment of inetia EXAM uesday Mach 8, 16 8:15 PM 9:45 PM oday s opics: Rotational Motion and Angula Displacement Angula Velocity and Acceleation Rotational Kinematics Angula and angential Vaiables Centipetal and angential Acceleation Rolling Moments of Inetia 1

Get Oiented Eveything we ve done so fa elates to tanslational (linea) motion. Geneal motion involves both tanslation and otation! hink about putting a mak on the edge of at tie and then olling it down the oad Let s fist deal with pue otation he angle though which the object otates is called the angula displacement. = θ θ o By convention, the angula displacement is positive if it is counteclockwise and negative if it is clockwise. SI Unit of Angula Displacement: adian (ad) Rotational Motion and Angula Displacement o a full evolution: π θ = = π ad Ac length s θ (in adians) = = Radius! π ad = 36

A otal Eclipse of the Sun he diamete of the sun is about 4 times geate than that of the moon. By coincidence, the sun is also about 4 times fathe fom the eath than is the moon. o an obseve on the eath, the angle subtended by the moon and the angle subtended by the sun is the same and explains why this can esult in a total sola eclipse. Ac length s θ (in adians) = = Radius θ (Sun) = θ (moon) Angula Velocity DEINIION O AVERAGE ANGULAR VELOCIY Angula displacement Aveage angula velocity = Elapsed time θ θo ω = = t t o SI Unit of Angula Velocity: adian pe second (ad/s) INSANANEOUS ANGULAR VELOCIY ω = lim ω = lim Look familia? Angula Acceleation DEINIION O AVERAGE ANGULAR ACCELERAION Change in angula velocity Aveage angula acceleation = Elapsed time ω ωo Δω α = = t t o SI Unit of Angula acceleation: adian pe second squaed (ad/s ) Can you hea me now???? 3

Kinematics of Rotation Example Duing the spin-dy cycle of a washing machine, the moto slows fom 95 ad/s to 3 ad/s while the tuning the dum though an angle of 4 adians. What is the magnitude of the angula acceleation of the moto? (a) 64 ad/s (b) 3 ad/s (c)1 ad/s (d) ad/s (e)1. ad/s ω = 95 ad/s ω = 3 ad/s = 4 ad α =? ω = ω + α α = ω ω = ( 3 ad/s ) 95 ad/s 4 ad = 1ad/s ( ) ( ) Note that the magnitude is 1 ad/s while the diection (-) is opposite to the angula velocity! angential Velocity and Speed We ve aleady seen that an angula displacement of θ coesponds to a tangential displacement of s fo a point a distance fom the axis of otation We have a simila elationship between angula velocity, ω, and tangential velocity, o speed v. 4

Δ ω = θ v s = = = v = ω (ω in ad/s) What about angula and tangential acceleation? v vo a = = ( ω) ( ω ) o ω ωo = ω ωo α = a = α ( α in ad/s ) Example On an amusement pak ide, passenges ae seated in a hoizontal cicle of adius 7.5 m. he seats begin fom est and ae unifomly acceleated fo 1 seconds to a maximum otational speed of 1.4 ad/s. What is the tangential acceleation of the passenges duing the fist 1 s of the ide? (a).67 m/s (b).5 m/s (c)1.4 m/s (d)7.5 m/s (e)11 m/s What is the instantaneous tangential speed of the passenges 15 s afte the acceleation begins? (a).67 m/s (b).5 m/s (c) 1.4 m/s (d) 7.5 m/s (e) 11 m/s = 7.5 m = 1s ω = ad/s ω = 1.4 ad/s a = α ω = ω + α ω 1.4 ad/s α = = =.67 ad/s 1s a = α = (7.5 m)(.67 ad/s ) a =.5 m/s v = ωt= 15s ω = ω + α ω = (.67 ad/s )(15 s) = 1ad/s v = (7.5 m)(1 ad/s) = 7.5 m/s 5

Rewiting centipetal acceleation a v ( ω) c = = = ω mv m( ω) c = = = mω Conceptual Poblem A igid body otates about a fixed axis with a constant angula acceleation. Which one of the following statements is tue concening the tangential acceleation of any point on the body? (a) he tangential acceleation is zeo m/s. (b) he tangential acceleation depends on the angula velocity. (c) he tangential acceleation is equal to the centipetal acceleation. (d) he tangential acceleation is constant in both magnitude and diection. (e) he tangential acceleation depends on the change in the angula velocity. Δω a = α = a = ω c Rolling (without slipping) Put otational and tanslational motion togethe he tangential speed of a point on the oute edge of the tie is equal to the speed of the ca ove the gound. o an object that is olling without slipping, the tanslational and otational motions ae coupled! v = ω a = α 6

Rotational Kinetic Enegy and the Moment of Inetia Imagine a mass on a sting, We can also wite the kinetic enegy as Whee I, the moment of inetia, is given by I = m 7