DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS AP PHYSICS

Size: px
Start display at page:

Download "DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS AP PHYSICS"

Transcription

1 DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS AP PHYSICS

2 LSN 8-5: ROTATIONAL DYNAMICS; TORQUE AND ROTATIONAL INERTIA LSN 8-6: SOLVING PROBLEMS IN ROTATIONAL DYNAMICS

3 Questions From Reading Activity?

4 Big Idea(s): Interactions between systems can result in changes in those systems. Changes that occur as a result of interactions are constrained by conservation laws.

5 Enduring Understanding(s): A net torque exerted on a system by other objects or systems will change the angular momentum of the system. The angular momentum of a system is conserved.

6 Essential Knowledge(s): The angular momentum of a system may change due to interactions with other objects or systems. Alternatively, the angular momentum of a system can be found om the product of the system s rotational inertia and its angular velocity.

7 Essential Knowledge(s): The angular momentum of a system is determined by the locations and velocities of the objects that make up the system. The rotational inertia of an object or system depends upon the distribution of mass within the object or system.

8 Essential Knowledge(s): Changes in the radius of a system or in the distribution of mass within the system result in changes in the system s rotational inertia, and hence in its angular velocity and linear speed for a given angular momentum.

9 Essential Knowledge(s): Examples should include elliptical orbits in an Earth-satellite system. Mathematical expressions for the moments of inertia will be provided where needed. Students will not be expected to know the parallel axis theorem.

10 Learning Objective(s): The student is able to plan a data collection and analysis strategy to determine the change in angular momentum of a system and relate it to interactions with other objects and systems.

11 Learning Objective(s): The student is able to describe or calculate the angular momentum and rotational inertia of a system in terms of the locations and velocities of objects that make up the system. Students are expected to do qualitative reasoning with compound objects. Students are expected to do calculations with a fixed set of extended objects and point masses.

12 Introductory Video

13 Moment of Inertia Angular acceleration is proportional to the net torque applied to it Force along a moment arm is torque More force means more acceleration F m

14 Moment of Inertia Everything in life relates to Newton s Second Law F ma rf F m a tan r F mr F mr r mr mr r

15 Moment of Inertia Moment of Inertia defined: F I mr m Note that the moment of inertia is much more affected by distance than by mass. Determination of the axis of rotation (reference point) is critical!

16 Moment of Inertia Example 8-10: Find the moment of inertia for (a) and (b)

17 Moment of Inertia Example 8-10: Find the moment of inertia for (a) and (b) a. I I b. I I I 5kg.0 7kg.0 48kgm I mr mr 5kg 0.5 7kg kgm

18 Moment of Inertia Moment of Inertia defined: F mr m I mr I This is Newton s Second Law for rotation!

19 Moment of Inertia Moment of Inertia defined: F I mr m I So how do you find the moment of inertia and the torque on these objects?

20 Moment of Inertia Without calculus, finding the moment of inertia can be difficult as seen by this chart It can be determined experimentally by finding the acceleration om a known torque

21 Problem Solving Rotational Motion 1. Draw a diagram of the system.. Draw a ee-body diagram for the object of interest. 3. Identify the axis of rotation (reference point) and determine the torques (remember directions!) 4. Apply Newton s Second Law for rotation (Στ = Iα). 5. Apply Newton s Second Law for translation as needed. 6. Solve and check for reasonability.

22 Example 8-11 Determine the moment of inertia of the pulley F T m 15.0N 4.00kg 30.0rad t 3.00s / s

23 Example 8-11 Determine the moment of inertia of the pulley I I F T m 15.0N 4.00kg 30.0rad / s t 3.00s 1.10m N

24 Example 8-11 Determine the moment of inertia of the pulley I F T R m n 1.10 F T m t 15.0N 4.00kg 30.0rad / 3.00s 1.10m N s

25 Example 8-11 Determine the moment of inertia of the pulley I 3.85m n 30.0 t rad s F T m t 15.0N 4.00kg 30.0rad / 3.00s 1.10m N s

26 Example 8-11 Determine the moment of inertia of the pulley I 3.85m n 10.0 rad I s kg m F T m t 15.0N 4.00kg 30.0rad / 3.00s 1.10m N s

27 Example 8-1 Calculate the angular and linear acceleration of the pulley. w 15.0N m 1.53kg I 0.385kgm 1.10m N I mg F T F T ma R

28 Example 8-1 Calculate the angular and linear acceleration of the pulley. w 15.0N m 1.53kg I 0.385kgm 1.10m N I F R mg mg T F T ma F T ma

29 Example 8-1 Calculate the angular and linear acceleration of the pulley. w 15.0N m 1.53kg I 0.385kgm 1.10m N I I F T R mg ma mg F T ma I mgr mar R

30 Example 8-1 Calculate the angular and linear acceleration of the pulley. w 15.0N m 1.53kg I 0.385kgm 1.10m N I mgr mar a a I tan mgr R m I mgr mr R R

31 Example 8-1 Calculate the angular and linear acceleration of the pulley. mr I mgr mgr mr I mgr mr I mr mgr I N m m kg I kg m N w

32 Example 8-1 Calculate the angular and linear acceleration of the pulley. w 15.0N m 1.53kg I 0.385kgm 1.10m N mgr I mr rad / s

33 Review Video

34 Learning Objective(s): The student is able to plan a data collection and analysis strategy to determine the change in angular momentum of a system and relate it to interactions with other objects and systems.

35 Learning Objective(s): The student is able to describe or calculate the angular momentum and rotational inertia of a system in terms of the locations and velocities of objects that make up the system. Students are expected to do qualitative reasoning with compound objects. Students are expected to do calculations with a fixed set of extended objects and point masses.

36 Essential Knowledge(s): The angular momentum of a system may change due to interactions with other objects or systems. Alternatively, the angular momentum of a system can be found om the product of the system s rotational inertia and its angular velocity.

37 Essential Knowledge(s): The angular momentum of a system is determined by the locations and velocities of the objects that make up the system. The rotational inertia of an object or system depends upon the distribution of mass within the object or system.

38 Essential Knowledge(s): Changes in the radius of a system or in the distribution of mass within the system result in changes in the system s rotational inertia, and hence in its angular velocity and linear speed for a given angular momentum.

39 Essential Knowledge(s): Examples should include elliptical orbits in an Earth-satellite system. Mathematical expressions for the moments of inertia will be provided where needed. Students will not be expected to know the parallel axis theorem.

40 Enduring Understanding(s): A net torque exerted on a system by other objects or systems will change the angular momentum of the system. The angular momentum of a system is conserved.

41 Big Idea(s): Interactions between systems can result in changes in those systems. Changes that occur as a result of interactions are constrained by conservation laws.

42 QUESTIONS?

43 Homework #7-40

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS AP PHYSICS

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS AP PHYSICS DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS AP PHYSICS LSN 8-8: ANGULAR MOMENTUM AND ITS CONSERVATION Questions From Reading Activity? Big Idea(s): The interactions of an object with other objects can be

More information

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS AP PHYSICS

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS AP PHYSICS DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS AP PHYSICS LSN 8-7: ROTATIONAL KINETIC ENERGY Questions From Reading Activity? Big Idea(s): The interactions of an object with other objects can be described by

More information

GIANCOLI READING ACTIVITY Lesson 8-4

GIANCOLI READING ACTIVITY Lesson 8-4 AP PHYSICS Name: Period: Date: DEVIL PHYSICS BADDEST CLASS ON CAMPUS 1. Big Idea(s): GIANCOLI READING ACTIVITY Lesson 8-4 a. Big Idea 3: The interactions of an object with other objects can be described

More information

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS AP PHYSICS

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS AP PHYSICS DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS AP PHYSICS LSN 11-1: SIMPLE HARMONIC MOTION LSN 11-: ENERGY IN THE SIMPLE HARMONIC OSCILLATOR LSN 11-3: PERIOD AND THE SINUSOIDAL NATURE OF SHM Introductory Video:

More information

INTRO VIDEO REVIEW QUIZ

INTRO VIDEO REVIEW QUIZ DEVIL PHYSICS BADDEST CLASS ON CAMPUS PRE-DP PHYSICS INTRO VIDEO Newton's Third Law of Motion REVIEW QUIZ 1. What is force? 2. Name Newton s First Law of Motion. 3. What is inertia? 4. What is the chemistry

More information

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS AP PHYSICS

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS AP PHYSICS DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS AP PHYSICS GIANCOLI CHAPTER 5: CIRCULAR MOTION; GRAVITATION LSN 5-1: KINEMATICS OF UNIFORM CIRCULAR MOTION LSN 5-2: DYNAMICS OF UNIFORM CIRCULAR MOTION LSN 5-3:

More information

Physics 101 Lecture 11 Torque

Physics 101 Lecture 11 Torque Physics 101 Lecture 11 Torque Dr. Ali ÖVGÜN EMU Physics Department www.aovgun.com Force vs. Torque q Forces cause accelerations q What cause angular accelerations? q A door is free to rotate about an axis

More information

CHAPTER 9 ROTATIONAL DYNAMICS

CHAPTER 9 ROTATIONAL DYNAMICS CHAPTER 9 ROTATIONAL DYNAMICS PROBLEMS. REASONING The drawing shows the forces acting on the person. It also shows the lever arms for a rotational axis perpendicular to the plane of the paper at the place

More information

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS AP PHYSICS

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS AP PHYSICS DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS AP PHYSICS LSN 7-1: MOMENTUM AND ITS RELATION TO FORCE LSN 7-2: CONSERVATION OF MOMENTUM LSN 7-3: COLLISIONS AND IMPULSE Big Idea(s): The interactions of an object

More information

Chapter 8. Rotational Motion

Chapter 8. Rotational Motion Chapter 8 Rotational Motion The Action of Forces and Torques on Rigid Objects In pure translational motion, all points on an object travel on parallel paths. The most general motion is a combination of

More information

Center of Gravity Pearson Education, Inc.

Center of Gravity Pearson Education, Inc. Center of Gravity = The center of gravity position is at a place where the torque from one end of the object is balanced by the torque of the other end and therefore there is NO rotation. Fulcrum Point

More information

General Definition of Torque, final. Lever Arm. General Definition of Torque 7/29/2010. Units of Chapter 10

General Definition of Torque, final. Lever Arm. General Definition of Torque 7/29/2010. Units of Chapter 10 Units of Chapter 10 Determining Moments of Inertia Rotational Kinetic Energy Rotational Plus Translational Motion; Rolling Why Does a Rolling Sphere Slow Down? General Definition of Torque, final Taking

More information

( )( ) ( )( ) Fall 2017 PHYS 131 Week 9 Recitation: Chapter 9: 5, 10, 12, 13, 31, 34

( )( ) ( )( ) Fall 2017 PHYS 131 Week 9 Recitation: Chapter 9: 5, 10, 12, 13, 31, 34 Fall 07 PHYS 3 Chapter 9: 5, 0,, 3, 3, 34 5. ssm The drawing shows a jet engine suspended beneath the wing of an airplane. The weight W of the engine is 0 00 N and acts as shown in the drawing. In flight

More information

III. Work and Energy

III. Work and Energy Rotation I. Kinematics - Angular analogs II. III. IV. Dynamics - Torque and Rotational Inertia Work and Energy Angular Momentum - Bodies and particles V. Elliptical Orbits The student will be able to:

More information

Slide 1 / 37. Rotational Motion

Slide 1 / 37. Rotational Motion Slide 1 / 37 Rotational Motion Slide 2 / 37 Angular Quantities An angle θ can be given by: where r is the radius and l is the arc length. This gives θ in radians. There are 360 in a circle or 2π radians.

More information

Rotation. I. Kinematics - Angular analogs

Rotation. I. Kinematics - Angular analogs Rotation I. Kinematics - Angular analogs II. III. IV. Dynamics - Torque and Rotational Inertia Work and Energy Angular Momentum - Bodies and particles V. Elliptical Orbits The student will be able to:

More information

General Physics (PHY 2130)

General Physics (PHY 2130) General Physics (PHY 130) Lecture 0 Rotational dynamics equilibrium nd Newton s Law for rotational motion rolling Exam II review http://www.physics.wayne.edu/~apetrov/phy130/ Lightning Review Last lecture:

More information

AP Physics 1 Rotational Motion Practice Test

AP Physics 1 Rotational Motion Practice Test AP Physics 1 Rotational Motion Practice Test MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. 1) A spinning ice skater on extremely smooth ice is able

More information

AP PHYSICS 1 Learning Objectives Arranged Topically

AP PHYSICS 1 Learning Objectives Arranged Topically AP PHYSICS 1 Learning Objectives Arranged Topically with o Big Ideas o Enduring Understandings o Essential Knowledges o Learning Objectives o Science Practices o Correlation to Knight Textbook Chapters

More information

DEVIL PHYSICS BADDEST CLASS ON CAMPUS IB PHYSICS

DEVIL PHYSICS BADDEST CLASS ON CAMPUS IB PHYSICS DEVIL PHYSICS BADDEST CLASS ON CAMPUS IB PHYSICS OPTION B-1A: ROTATIONAL DYNAMICS Essential Idea: The basic laws of mechanics have an extension when equivalent principles are applied to rotation. Actual

More information

A) 1 gm 2 /s. B) 3 gm 2 /s. C) 6 gm 2 /s. D) 9 gm 2 /s. E) 10 gm 2 /s. A) 0.1 kg. B) 1 kg. C) 2 kg. D) 5 kg. E) 10 kg A) 2:5 B) 4:5 C) 1:1 D) 5:4

A) 1 gm 2 /s. B) 3 gm 2 /s. C) 6 gm 2 /s. D) 9 gm 2 /s. E) 10 gm 2 /s. A) 0.1 kg. B) 1 kg. C) 2 kg. D) 5 kg. E) 10 kg A) 2:5 B) 4:5 C) 1:1 D) 5:4 1. A 4 kg object moves in a circle of radius 8 m at a constant speed of 2 m/s. What is the angular momentum of the object with respect to an axis perpendicular to the circle and through its center? A)

More information

Rotational N.2 nd Law

Rotational N.2 nd Law Lecture 19 Chapter 12 Rotational N.2 nd Law Torque Newton 2 nd Law again!? That s it. He crossed the line! Course website: http://faculty.uml.edu/andriy_danylov/teaching/physicsi IN THIS CHAPTER, you will

More information

Chapter 8 continued. Rotational Dynamics

Chapter 8 continued. Rotational Dynamics Chapter 8 continued Rotational Dynamics 8.6 The Action of Forces and Torques on Rigid Objects Chapter 8 developed the concepts of angular motion. θ : angles and radian measure for angular variables ω :

More information

Flipping Physics Lecture Notes: Demonstrating Rotational Inertia (or Moment of Inertia)

Flipping Physics Lecture Notes: Demonstrating Rotational Inertia (or Moment of Inertia) Flipping Physics Lecture Notes: Demonstrating Rotational Inertia (or Moment of Inertia) Have you ever struggled to describe Rotational Inertia to your students? Even worse, have you ever struggled to understand

More information

III. Angular Momentum Conservation (Chap. 10) Rotation. We repeat Chap. 2-8 with rotatiing objects. Eqs. of motion. Energy.

III. Angular Momentum Conservation (Chap. 10) Rotation. We repeat Chap. 2-8 with rotatiing objects. Eqs. of motion. Energy. Chap. 10: Rotational Motion I. Rotational Kinematics II. Rotational Dynamics - Newton s Law for Rotation III. Angular Momentum Conservation (Chap. 10) 1 Toward Exam 3 Eqs. of motion o To study angular

More information

Rotational N.2 nd Law

Rotational N.2 nd Law Lecture 0 Chapter 1 Physics I Rotational N. nd Law Torque Course website: http://faculty.uml.edu/andriy_danylov/teaching/physicsi IN THIS CHAPTER, you will continue discussing rotational dynamics Today

More information

Chapter 9. Rotational Dynamics

Chapter 9. Rotational Dynamics Chapter 9 Rotational Dynamics In pure translational motion, all points on an object travel on parallel paths. The most general motion is a combination of translation and rotation. 1) Torque Produces angular

More information

31 ROTATIONAL KINEMATICS

31 ROTATIONAL KINEMATICS 31 ROTATIONAL KINEMATICS 1. Compare and contrast circular motion and rotation? Address the following Which involves an object and which involves a system? Does an object/system in circular motion have

More information

Circular Motion, Pt 2: Angular Dynamics. Mr. Velazquez AP/Honors Physics

Circular Motion, Pt 2: Angular Dynamics. Mr. Velazquez AP/Honors Physics Circular Motion, Pt 2: Angular Dynamics Mr. Velazquez AP/Honors Physics Formulas: Angular Kinematics (θ must be in radians): s = rθ Arc Length 360 = 2π rads = 1 rev ω = θ t = v t r Angular Velocity α av

More information

Chapter 8. Rotational Equilibrium and Rotational Dynamics. 1. Torque. 2. Torque and Equilibrium. 3. Center of Mass and Center of Gravity

Chapter 8. Rotational Equilibrium and Rotational Dynamics. 1. Torque. 2. Torque and Equilibrium. 3. Center of Mass and Center of Gravity Chapter 8 Rotational Equilibrium and Rotational Dynamics 1. Torque 2. Torque and Equilibrium 3. Center of Mass and Center of Gravity 4. Torque and angular acceleration 5. Rotational Kinetic energy 6. Angular

More information

Equilibrium. For an object to remain in equilibrium, two conditions must be met. The object must have no net force: and no net torque:

Equilibrium. For an object to remain in equilibrium, two conditions must be met. The object must have no net force: and no net torque: Equilibrium For an object to remain in equilibrium, two conditions must be met. The object must have no net force: F v = 0 and no net torque: v τ = 0 Worksheet A uniform rod with a length L and a mass

More information

= o + t = ot + ½ t 2 = o + 2

= o + t = ot + ½ t 2 = o + 2 Chapters 8-9 Rotational Kinematics and Dynamics Rotational motion Rotational motion refers to the motion of an object or system that spins about an axis. The axis of rotation is the line about which the

More information

Moment of Inertia & Newton s Laws for Translation & Rotation

Moment of Inertia & Newton s Laws for Translation & Rotation Moment of Inertia & Newton s Laws for Translation & Rotation In this training set, you will apply Newton s 2 nd Law for rotational motion: Στ = Σr i F i = Iα I is the moment of inertia of an object: I

More information

Rolling without slipping Angular Momentum Conservation of Angular Momentum. Physics 201: Lecture 19, Pg 1

Rolling without slipping Angular Momentum Conservation of Angular Momentum. Physics 201: Lecture 19, Pg 1 Physics 131: Lecture Today s Agenda Rolling without slipping Angular Momentum Conservation o Angular Momentum Physics 01: Lecture 19, Pg 1 Rolling Without Slipping Rolling is a combination o rotation and

More information

Cross Product Angular Momentum

Cross Product Angular Momentum Lecture 21 Chapter 12 Physics I Cross Product Angular Momentum Course website: http://faculty.uml.edu/andriy_danylov/teaching/physicsi IN THIS CHAPTER, you will continue discussing rotational dynamics

More information

Rotational Dynamics continued

Rotational Dynamics continued Chapter 9 Rotational Dynamics continued 9.4 Newton s Second Law for Rotational Motion About a Fixed Axis ROTATIONAL ANALOG OF NEWTON S SECOND LAW FOR A RIGID BODY ROTATING ABOUT A FIXED AXIS I = ( mr 2

More information

Physics 2A Chapter 10 - Rotational Motion Fall 2018

Physics 2A Chapter 10 - Rotational Motion Fall 2018 Physics A Chapter 10 - Rotational Motion Fall 018 These notes are five pages. A quick summary: The concepts of rotational motion are a direct mirror image of the same concepts in linear motion. Follow

More information

Video Lecture #2 Introductory Conservation of Momentum Problem using Unit Vectors

Video Lecture #2 Introductory Conservation of Momentum Problem using Unit Vectors AP Physics C Video Lecture Notes Chapter 09-10 Thank You, Emily Rencsok, for these notes. Video Lecture #1 Introduction to Momentum and Derivation of Conservation of Momentum Video Lecture #2 Introductory

More information

Review for 3 rd Midterm

Review for 3 rd Midterm Review for 3 rd Midterm Midterm is on 4/19 at 7:30pm in the same rooms as before You are allowed one double sided sheet of paper with any handwritten notes you like. The moment-of-inertia about the center-of-mass

More information

Torque rotational force which causes a change in rotational motion. This force is defined by linear force multiplied by a radius.

Torque rotational force which causes a change in rotational motion. This force is defined by linear force multiplied by a radius. Warm up A remote-controlled car's wheel accelerates at 22.4 rad/s 2. If the wheel begins with an angular speed of 10.8 rad/s, what is the wheel's angular speed after exactly three full turns? AP Physics

More information

Chapter 8 Lecture Notes

Chapter 8 Lecture Notes Chapter 8 Lecture Notes Physics 2414 - Strauss Formulas: v = l / t = r θ / t = rω a T = v / t = r ω / t =rα a C = v 2 /r = ω 2 r ω = ω 0 + αt θ = ω 0 t +(1/2)αt 2 θ = (1/2)(ω 0 +ω)t ω 2 = ω 0 2 +2αθ τ

More information

PHY 111L Activity 9 Moments of Inertia

PHY 111L Activity 9 Moments of Inertia PHY 111L Activity 9 Moments of Inertia Name: Section: ID #: Date: Lab Partners: TA initials: Objectives 1. Introduce moment of inertia for different objects 2. Understand the moment of inertia apparatus

More information

Static Equilibrium, Gravitation, Periodic Motion

Static Equilibrium, Gravitation, Periodic Motion This test covers static equilibrium, universal gravitation, and simple harmonic motion, with some problems requiring a knowledge of basic calculus. Part I. Multiple Choice 1. 60 A B 10 kg A mass of 10

More information

Name (please print): UW ID# score last first

Name (please print): UW ID# score last first Name (please print): UW ID# score last first Question I. (20 pts) Projectile motion A ball of mass 0.3 kg is thrown at an angle of 30 o above the horizontal. Ignore air resistance. It hits the ground 100

More information

Worksheet for Exploration 10.1: Constant Angular Velocity Equation

Worksheet for Exploration 10.1: Constant Angular Velocity Equation Worksheet for Exploration 10.1: Constant Angular Velocity Equation By now you have seen the equation: θ = θ 0 + ω 0 *t. Perhaps you have even derived it for yourself. But what does it really mean for the

More information

ΣF = ma Στ = Iα ½mv 2 ½Iω 2. mv Iω

ΣF = ma Στ = Iα ½mv 2 ½Iω 2. mv Iω Thur Oct 22 Assign 9 Friday Today: Torques Angular Momentum x θ v ω a α F τ m I Roll without slipping: x = r Δθ v LINEAR = r ω a LINEAR = r α ΣF = ma Στ = Iα ½mv 2 ½Iω 2 I POINT = MR 2 I HOOP = MR 2 I

More information

Physics 121, March 25, Rotational Motion and Angular Momentum. Department of Physics and Astronomy, University of Rochester

Physics 121, March 25, Rotational Motion and Angular Momentum. Department of Physics and Astronomy, University of Rochester Physics 121, March 25, 2008. Rotational Motion and Angular Momentum. Physics 121. March 25, 2008. Course Information Topics to be discussed today: Review of Rotational Motion Rolling Motion Angular Momentum

More information

Lecture 20 Chapter 12 Angular Momentum Course website:

Lecture 20 Chapter 12 Angular Momentum Course website: Lecture 20 Chapter 12 Angular Momentum Another Law? Am I in a Law school? Course website: http://faculty.uml.edu/andriy_danylov/teaching/physicsi IN THIS CHAPTER, you will continue discussing rotational

More information

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS AP PHYSICS

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS AP PHYSICS DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS AP PHYSICS LSN 7-4: CONSERVATION OF ENERGY AND MOMENTUM IN COLLISIONS LSN 7-5: ELASTIC COLLISIONS IN ONE DIMENSION LSN 7-6: INELASTIC COLLISIONS Questions From

More information

Handout 7: Torque, angular momentum, rotational kinetic energy and rolling motion. Torque and angular momentum

Handout 7: Torque, angular momentum, rotational kinetic energy and rolling motion. Torque and angular momentum Handout 7: Torque, angular momentum, rotational kinetic energy and rolling motion Torque and angular momentum In Figure, in order to turn a rod about a fixed hinge at one end, a force F is applied at a

More information

PH1104/PH114S - MECHANICS

PH1104/PH114S - MECHANICS PH04/PH4S - MECHANICS FAISAN DAY FALL 06 MULTIPLE CHOICE ANSWES. (E) the first four options are clearly wrong since v x needs to change its sign at a moment during the motion and there s no way v x could

More information

1. Which of the following is the unit for angular displacement? A. Meters B. Seconds C. Radians D. Radian per second E. Inches

1. Which of the following is the unit for angular displacement? A. Meters B. Seconds C. Radians D. Radian per second E. Inches AP Physics B Practice Questions: Rotational Motion Multiple-Choice Questions 1. Which of the following is the unit for angular displacement? A. Meters B. Seconds C. Radians D. Radian per second E. Inches

More information

GIANCOLI LESSON 6-1, WORK DONE BY A CONSTANT FORCE LESSON 6-2, WORK DONE BY A VARYING FORCE

GIANCOLI LESSON 6-1, WORK DONE BY A CONSTANT FORCE LESSON 6-2, WORK DONE BY A VARYING FORCE AP PHYSICS GIANCOLI LESSON 6-1, ORK DONE BY A CONSTANT ORCE LESSON 6-2, ORK DONE BY A VARYING ORCE Big Idea(s): The interactions of an object with other objects can be described by forces. Interactions

More information

Torque/Rotational Energy Mock Exam. Instructions: (105 points) Answer the following questions. SHOW ALL OF YOUR WORK.

Torque/Rotational Energy Mock Exam. Instructions: (105 points) Answer the following questions. SHOW ALL OF YOUR WORK. AP Physics C Spring, 2017 Torque/Rotational Energy Mock Exam Name: Answer Key Mr. Leonard Instructions: (105 points) Answer the following questions. SHOW ALL OF YOUR WORK. (22 pts ) 1. Two masses are attached

More information

Torque. Physics 6A. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB

Torque. Physics 6A. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB Physics 6A Torque is what causes angular acceleration (just like a force causes linear acceleration) Torque is what causes angular acceleration (just like a force causes linear acceleration) For a torque

More information

Physics 131: Lecture 21. Today s Agenda

Physics 131: Lecture 21. Today s Agenda Physics 131: Lecture 21 Today s Agenda Rotational dynamics Torque = I Angular Momentum Physics 201: Lecture 10, Pg 1 Newton s second law in rotation land Sum of the torques will equal the moment of inertia

More information

Physics 141. Lecture 18. Frank L. H. Wolfs Department of Physics and Astronomy, University of Rochester, Lecture 18, Page 1

Physics 141. Lecture 18. Frank L. H. Wolfs Department of Physics and Astronomy, University of Rochester, Lecture 18, Page 1 Physics 141. Lecture 18. Frank L. H. Wolfs Department of Physics and Astronomy, University of Rochester, Lecture 18, Page 1 Physics 141. Lecture 18. Course Information. Topics to be discussed today: A

More information

Please read this introductory material carefully; it covers topics you might not yet have seen in class.

Please read this introductory material carefully; it covers topics you might not yet have seen in class. b Lab Physics 211 Lab 10 Torque What You Need To Know: Please read this introductory material carefully; it covers topics you might not yet have seen in class. F (a) (b) FIGURE 1 Forces acting on an object

More information

Chapter 9-10 Test Review

Chapter 9-10 Test Review Chapter 9-10 Test Review Chapter Summary 9.2. The Second Condition for Equilibrium Explain torque and the factors on which it depends. Describe the role of torque in rotational mechanics. 10.1. Angular

More information

Rotational Motion. Rotational Motion. Rotational Motion

Rotational Motion. Rotational Motion. Rotational Motion I. Rotational Kinematics II. Rotational Dynamics (Netwton s Law for Rotation) III. Angular Momentum Conservation 1. Remember how Newton s Laws for translational motion were studied: 1. Kinematics (x =

More information

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS IB PHYSICS

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS IB PHYSICS DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS IB PHYSICS TSOKOS LSN 2-2A THE CONCEPT OF FORCE Introductory Video Introducing Sir Isaac Newton Essential Idea: Classical physics requires a force to change a

More information

Physics 101: Lecture 15 Torque, F=ma for rotation, and Equilibrium

Physics 101: Lecture 15 Torque, F=ma for rotation, and Equilibrium Physics 101: Lecture 15 Torque, F=ma for rotation, and Equilibrium Strike (Day 10) Prelectures, checkpoints, lectures continue with no change. Take-home quizzes this week. See Elaine Schulte s email. HW

More information

PHYS 111 HOMEWORK #11

PHYS 111 HOMEWORK #11 PHYS 111 HOMEWORK #11 Due date: You have a choice here. You can submit this assignment on Tuesday, December and receive a 0 % bonus, or you can submit this for normal credit on Thursday, 4 December. If

More information

GIANCOLI READING ACTIVITY Section(s) 5-1 to 5-3

GIANCOLI READING ACTIVITY Section(s) 5-1 to 5-3 AP PHYSICS Name: Period: Date: DEVIL PHYSICS BADDEST CLASS ON CAMPUS 1. Big Idea(s): GIANCOLI READING ACTIVITY Section(s) 5-1 to 5-3 a. 1: Objects and systems have properties such as mass and charge. Systems

More information

CIRCULAR MOTION AND ROTATION

CIRCULAR MOTION AND ROTATION 1. UNIFORM CIRCULAR MOTION So far we have learned a great deal about linear motion. This section addresses rotational motion. The simplest kind of rotational motion is an object moving in a perfect circle

More information

AP Physics 1- Torque, Rotational Inertia, and Angular Momentum Practice Problems FACT: The center of mass of a system of objects obeys Newton s second law- F = Ma cm. Usually the location of the center

More information

Motion in Space. MATH 311, Calculus III. J. Robert Buchanan. Fall Department of Mathematics. J. Robert Buchanan Motion in Space

Motion in Space. MATH 311, Calculus III. J. Robert Buchanan. Fall Department of Mathematics. J. Robert Buchanan Motion in Space Motion in Space MATH 311, Calculus III J. Robert Buchanan Department of Mathematics Fall 2011 Background Suppose the position vector of a moving object is given by r(t) = f (t), g(t), h(t), Background

More information

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS AP PHYSICS

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS AP PHYSICS DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS AP PHYSICS LSN 3-7: PROJECTILE MOTION IS PARABOLIC LSN 3-8: RELATIVE VELOCITY Questions From Reading Actiity? Big Idea(s): The interactions of an object with other

More information

PHY 2048 Final Exam Review DISCLAIMER - I am a student and there could potentially be errors in the solutions.

PHY 2048 Final Exam Review DISCLAIMER - I am a student and there could potentially be errors in the solutions. PHY 2048 Final Exam Review DISCLAIMER - I am a student and there could potentially be errors in the solutions. 1. A large wheel of cheese, initially at rest, accelerates at a rate of 10 rad/s^2. The radius

More information

Chapter 8 Rotational Motion and Dynamics Reading Notes

Chapter 8 Rotational Motion and Dynamics Reading Notes Name: Chapter 8 Rotational Motion and Dynamics Reading Notes Section 8-1: Angular quantities A circle can be split into pieces called degrees. There are 360 degrees in a circle. A circle can be split into

More information

Physics 4A Solutions to Chapter 10 Homework

Physics 4A Solutions to Chapter 10 Homework Physics 4A Solutions to Chapter 0 Homework Chapter 0 Questions: 4, 6, 8 Exercises & Problems 6, 3, 6, 4, 45, 5, 5, 7, 8 Answers to Questions: Q 0-4 (a) positive (b) zero (c) negative (d) negative Q 0-6

More information

Physics C: Mechanics

Physics C: Mechanics Physics C: Mechanics 2013 2014 PISCATAWAY TOWNSHIP SCHOOLS COURSE SYLLABUS Mr. Rohan Gokhale rgokhale@pway.org www.piscatawayschools.org/phs Brief Description of Course The AP Physics course is a full

More information

PHYSICS - CLUTCH 1E CH 12: TORQUE & ROTATIONAL DYNAMICS.

PHYSICS - CLUTCH 1E CH 12: TORQUE & ROTATIONAL DYNAMICS. !! www.clutchprep.com INTRO TO TORQUE TORQUE is a twist that a Force gives an object around an axis of rotation. - For example, when you push on a door, it rotates around its hinges. - When a Force acts

More information

PHYSICS - CLUTCH CH 12: TORQUE & ROTATIONAL DYNAMICS.

PHYSICS - CLUTCH CH 12: TORQUE & ROTATIONAL DYNAMICS. !! www.clutchprep.com TORQUE & ACCELERATION (ROTATIONAL DYNAMICS) When a Force causes rotation, it produces a Torque. Think of TORQUE as the equivalent of FORCE! FORCE (F) TORQUE (τ) - Causes linear acceleration

More information

Chapter 8. Rotational Equilibrium and Rotational Dynamics

Chapter 8. Rotational Equilibrium and Rotational Dynamics Chapter 8 Rotational Equilibrium and Rotational Dynamics Wrench Demo Torque Torque, τ, is the tendency of a force to rotate an object about some axis τ = Fd F is the force d is the lever arm (or moment

More information

Chapter 8. Rotational Motion

Chapter 8. Rotational Motion Chapter 8 Rotational Motion Rotational Work and Energy W = Fs = s = rθ Frθ Consider the work done in rotating a wheel with a tangential force, F, by an angle θ. τ = Fr W =τθ Rotational Work and Energy

More information

CHAPTER 8 TEST REVIEW MARKSCHEME

CHAPTER 8 TEST REVIEW MARKSCHEME AP PHYSICS Name: Period: Date: 50 Multiple Choice 45 Single Response 5 Multi-Response Free Response 3 Short Free Response 2 Long Free Response MULTIPLE CHOICE DEVIL PHYSICS BADDEST CLASS ON CAMPUS AP EXAM

More information

Dynamics of Rotational Motion

Dynamics of Rotational Motion Chapter 10 Dynamics of Rotational Motion To understand the concept of torque. To relate angular acceleration and torque. To work and power in rotational motion. To understand angular momentum. To understand

More information

Name SOLUTION Student ID Score Speed of blocks is is decreasing. Part III. [25 points] Two blocks move on a frictionless

Name SOLUTION Student ID Score Speed of blocks is is decreasing. Part III. [25 points] Two blocks move on a frictionless Name SOLUTION Student ID Score last first Speed of blocks is is decreasing. Part III. [25 points] Two blocks move on a frictionless v o incline with initial speed v o, as shown, while a hand pushes with

More information

Physics Kinematics, Projectile Motion, Free-Body Diagrams, and Rotational Motion

Physics Kinematics, Projectile Motion, Free-Body Diagrams, and Rotational Motion Physics Kinematics, Projectile Motion, Free-Body Diagrams, and Rotational Motion Kinematics and Projectile Motion Problem Solving Steps 1. Read and Re-Read the whole problem carefully before trying to

More information

Chapter 8 - Rotational Dynamics and Equilibrium REVIEW

Chapter 8 - Rotational Dynamics and Equilibrium REVIEW Pagpalain ka! (Good luck, in Filipino) Date Chapter 8 - Rotational Dynamics and Equilibrium REVIEW TRUE/FALSE. Write 'T' if the statement is true and 'F' if the statement is false. 1) When a rigid body

More information

Chapter 10: Dynamics of Rotational Motion

Chapter 10: Dynamics of Rotational Motion Chapter 10: Dynamics of Rotational Motion What causes an angular acceleration? The effectiveness of a force at causing a rotation is called torque. QuickCheck 12.5 The four forces shown have the same strength.

More information

Rotational Kinetic Energy

Rotational Kinetic Energy Lecture 17, Chapter 10: Rotational Energy and Angular Momentum 1 Rotational Kinetic Energy Consider a rigid body rotating with an angular velocity ω about an axis. Clearly every point in the rigid body

More information

1. Write the symbolic representation and one possible unit for angular velocity, angular acceleration, torque and rotational inertia.

1. Write the symbolic representation and one possible unit for angular velocity, angular acceleration, torque and rotational inertia. ROTATIONAL DYNAMICS Pre-Lab Questions Page Name: Class: Roster Number: Instructor: 1. Write the symbolic representation and one possible unit for angular velocity, angular acceleration, torque and rotational

More information

Physics 121, March 27, Angular Momentum, Torque, and Precession. Department of Physics and Astronomy, University of Rochester

Physics 121, March 27, Angular Momentum, Torque, and Precession. Department of Physics and Astronomy, University of Rochester Physics 121, March 27, 2008. Angular Momentum, Torque, and Precession. Physics 121. March 27, 2008. Course Information Quiz Topics to be discussed today: Review of Angular Momentum Conservation of Angular

More information

Lecture Outline Chapter 11. Physics, 4 th Edition James S. Walker. Copyright 2010 Pearson Education, Inc.

Lecture Outline Chapter 11. Physics, 4 th Edition James S. Walker. Copyright 2010 Pearson Education, Inc. Lecture Outline Chapter 11 Physics, 4 th Edition James S. Walker Chapter 11 Rotational Dynamics and Static Equilibrium Units of Chapter 11 Torque Torque and Angular Acceleration Zero Torque and Static

More information

Angular Momentum. Objectives CONSERVATION OF ANGULAR MOMENTUM

Angular Momentum. Objectives CONSERVATION OF ANGULAR MOMENTUM Angular Momentum CONSERVATION OF ANGULAR MOMENTUM Objectives Calculate the angular momentum vector for a moving particle Calculate the angular momentum vector for a rotating rigid object where angular

More information

Physics 131: Lecture 21. Today s Agenda

Physics 131: Lecture 21. Today s Agenda Physics 131: Lecture 1 Today s Agenda Rotational dynamics Torque = I Angular Momentum Physics 01: Lecture 10, Pg 1 Newton s second law in rotation land Sum of the torques will equal the moment of inertia

More information

Name Student ID Score Last First. I = 2mR 2 /5 around the sphere s center of mass?

Name Student ID Score Last First. I = 2mR 2 /5 around the sphere s center of mass? NOTE: ignore air resistance in all Questions. In all Questions choose the answer that is the closest!! Question I. (15 pts) Rotation 1. (5 pts) A bowling ball that has an 11 cm radius and a 7.2 kg mass

More information

Table of Contents. Pg. # Momentum & Impulse (Bozemanscience Videos) Lab 2 Determination of Rotational Inertia 1 1/11/16

Table of Contents. Pg. # Momentum & Impulse (Bozemanscience Videos) Lab 2 Determination of Rotational Inertia 1 1/11/16 Table of Contents g. # 1 1/11/16 Momentum & Impulse (Bozemanscience Videos) 2 1/13/16 Conservation of Momentum 3 1/19/16 Elastic and Inelastic Collisions 4 1/19/16 Lab 1 Momentum 5 1/26/16 Rotational tatics

More information

Physics 2210 Homework 18 Spring 2015

Physics 2210 Homework 18 Spring 2015 Physics 2210 Homework 18 Spring 2015 Charles Jui April 12, 2015 IE Sphere Incline Wording A solid sphere of uniform density starts from rest and rolls without slipping down an inclined plane with angle

More information

Chapter 9. Rotational Dynamics

Chapter 9. Rotational Dynamics Chapter 9 Rotational Dynamics In pure translational motion, all points on an object travel on parallel paths. The most general motion is a combination of translation and rotation. 1) Torque Produces angular

More information

Big Idea 4: Interactions between systems can result in changes in those systems. Essential Knowledge 4.D.1: Torque, angular velocity, angular

Big Idea 4: Interactions between systems can result in changes in those systems. Essential Knowledge 4.D.1: Torque, angular velocity, angular Unit 7: Rotational Motion (angular kinematics, dynamics, momentum & energy) Name: Big Idea 3: The interactions of an object with other objects can be described by forces. Essential Knowledge 3.F.1: Only

More information

Chapter 6, Problem 18. Agenda. Rotational Inertia. Rotational Inertia. Calculating Moment of Inertia. Example: Hoop vs.

Chapter 6, Problem 18. Agenda. Rotational Inertia. Rotational Inertia. Calculating Moment of Inertia. Example: Hoop vs. Agenda Today: Homework quiz, moment of inertia and torque Thursday: Statics problems revisited, rolling motion Reading: Start Chapter 8 in the reading Have to cancel office hours today: will have extra

More information

Fall 2007 RED Barcode Here Physics 105, sections 1 and 2 Please write your CID Colton

Fall 2007 RED Barcode Here Physics 105, sections 1 and 2 Please write your CID Colton Fall 007 RED Barcode Here Physics 105, sections 1 and Exam 3 Please write your CID Colton -3669 3 hour time limit. One 3 5 handwritten note card permitted (both sides). Calculators permitted. No books.

More information

E = K + U. p mv. p i = p f. F dt = p. J t 1. a r = v2. F c = m v2. s = rθ. a t = rα. r 2 dm i. m i r 2 i. I ring = MR 2.

E = K + U. p mv. p i = p f. F dt = p. J t 1. a r = v2. F c = m v2. s = rθ. a t = rα. r 2 dm i. m i r 2 i. I ring = MR 2. v = v i + at x = x i + v i t + 1 2 at2 E = K + U p mv p i = p f L r p = Iω τ r F = rf sin θ v 2 = v 2 i + 2a x F = ma = dp dt = U v dx dt a dv dt = d2 x dt 2 A circle = πr 2 A sphere = 4πr 2 V sphere =

More information

Lab 11: Rotational Dynamics

Lab 11: Rotational Dynamics Lab 11: Rotational Dynamics Objectives: To understand the relationship between net torque and angular acceleration. To understand the concept of the moment of inertia. To understand the concept of angular

More information

1 MR SAMPLE EXAM 3 FALL 2013

1 MR SAMPLE EXAM 3 FALL 2013 SAMPLE EXAM 3 FALL 013 1. A merry-go-round rotates from rest with an angular acceleration of 1.56 rad/s. How long does it take to rotate through the first rev? A) s B) 4 s C) 6 s D) 8 s E) 10 s. A wheel,

More information

Work and kinetic Energy

Work and kinetic Energy Work and kinetic Energy Problem 66. M=4.5kg r = 0.05m I = 0.003kgm 2 Q: What is the velocity of mass m after it dropped a distance h? (No friction) h m=0.6kg mg Work and kinetic Energy Problem 66. M=4.5kg

More information

Welcome back to Physics 211

Welcome back to Physics 211 Welcome back to Physics 211 Today s agenda: Moment of Inertia Angular momentum 13-2 1 Current assignments Prelecture due Tuesday after Thanksgiving HW#13 due next Wednesday, 11/24 Turn in written assignment

More information