Music. Who is the Artist? A) The Meters B) The Neville Brothers C) Trombone Shorty D) Michael Franti E) Radiators

Similar documents
Music. Who is the Artist? A) Oscar Peterson B) Kenny Barron C) Dave Brubeck D) Thelonius Monk E) Marcus Roberts

Phys101 Lecture 5 Dynamics: Newton s Laws of Motion

A Question about free-body diagrams

Lecture 6 Force and Motion. Identifying Forces Free-body Diagram Newton s Second Law

Lecture 7: More on Newton s Laws

Chapter 4 Force and Motion

Dynamics: Forces and Newton s Laws of Motion

Chapter 4: Newton s Second Law F = m a. F = m a (4.2)

Dynamics: Forces and Newton s Laws of Motion

Unit 1: Equilibrium and Center of Mass

Newton s Laws. A force is simply a push or a pull. Forces are vectors; they have both size and direction.

PHYS 100: Lecture 7. FRICTION and UNIFORM CIRCULAR MOTION. θ Mg. v R. R a. Static: Kinetic: Physics 100 Lecture 7, Slide 1

PHYS 100: Lecture 5. F F ma NEWTON S SECOND LAW. N Mg. Physics 100 Lecture 5, Slide 1

Discussion Session 6 Newton s Second & Third Laws Week 07. The Plan

Topic: Force PHYSICS 231

Physics for Scientists and Engineers. Chapter 5 Force and Motion

Physics A - PHY 2048C

Lecture 5. Dynamics. Forces: Newton s First and Second

Summary for last week: Newton s 2 nd Law + 1 st Law

CHAPTER 2. FORCE and Motion. CHAPTER s Objectives

Newton s Laws and Free-Body Diagrams General Physics I

Physics B Newton s Laws AP Review Packet

Question 1. G.M. Paily Phys 211

PHYS 100: Lecture 7. FRICTION and UNIFORM CIRCULAR MOTION. θ Mg. v R. R a. Static: Kinetic: Physics 100 Lecture 7, Slide 1

Lecture 2 - Force Analysis

Chapter 5 Force and Motion

Mass & Weight. weight a force acting on a body due to the gravitational attraction pulling that body to another. NOT constant.

Chapter 5 Newton s Laws of Motion

NEWTON S LAWS OF MOTION (EQUATION OF MOTION) (Sections )

Chapter 5 Force and Motion

Newton s Laws: Force and Motion

The Concept of Force Newton s First Law and Inertial Frames Mass Newton s Second Law The Gravitational Force and Weight Newton s Third Law Analysis

PHY2048 Physics with Calculus I

Main points of today s lecture: Normal force Newton s 3 d Law Frictional forces: kinetic friction: static friction Examples. Physic 231 Lecture 9

PHYSICS. Chapter 5 Lecture FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E RANDALL D. KNIGHT Pearson Education, Inc.

Lecture PowerPoints. Chapter 4 Physics: for Scientists & Engineers, with Modern Physics, 4th edition Giancoli

Chapter 5 Newton s Laws of Motion. Copyright 2010 Pearson Education, Inc.

PHYSICS 220 Lecture 04 Forces and Motion in 1 D Textbook Sections

4.2. Visualize: Assess: Note that the climber does not touch the sides of the crevasse so there are no forces from the crevasse walls.

Physics 101 Lecture 5 Newton`s Laws

What is a Force? Free-Body diagrams. Contact vs. At-a-Distance 11/28/2016. Forces and Newton s Laws of Motion

Chapter 5 Lecture. Pearson Physics. Newton's Laws of Motion. Prepared by Chris Chiaverina Pearson Education, Inc.

Newton s Laws Review

Lecture 6. > Forces. > Newton's Laws. > Normal Force, Weight. (Source: Serway; Giancoli) Villacorta-DLSUM-BIOPHY1-L Term01

Chapter 4. Dynamics: Newton s Laws of Motion. That is, describing why objects move

A hockey puck slides on ice at constant velocity. What is the net force acting on the puck?

1 A car moves around a circular path of a constant radius at a constant speed. Which of the following statements is true?

Forces and Newton s Laws Reading Notes. Give an example of a force you have experienced continuously all your life.

PSI AP Physics B Dynamics

Dynamic equilibrium: object moves with constant velocity in a straight line. = 0, a x = i

Unit 08 Work and Kinetic Energy. Stuff you asked about:

Dynamics Multiple Choice Homework

Newton s 3 Laws of Motion

Chapter 6. Dynamics I: Motion Along a Line

Chap. 4: Newton s Law of Motion

Concept of Force Concept Questions

PHYSICS. Chapter 5 Lecture FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E RANDALL D. KNIGHT Pearson Education, Inc.

1. A sphere with a radius of 1.7 cm has a volume of: A) m 3 B) m 3 C) m 3 D) 0.11 m 3 E) 21 m 3

Chapter 5. The Laws of Motion

Yanbu University College. General Studies Department. Phsc001 Course (111) Chapter2 (forces) Worksheet Solutions

Work. Objectives. Assessment. Assessment. Equations. Physics terms 6/3/14. Define the joule in terms of force and distance.

Physics 100: Lecture 4b Chapter 4

Chapter 3 The Laws of motion. The Laws of motion

Dynamics; Newton s Laws of Motion

Chapter 4. Forces and Newton s Laws of Motion. continued

Chapter 4: Newton's Second Law of Motion

Chapter 4: Newton's Laws of Motion

Chapter 4 Dynamics: Newton s Laws of Motion

Two Hanging Masses. ) by considering just the forces that act on it. Use Newton's 2nd law while

Chapter 5. The Laws of Motion

1 In the absence of a net force, a moving object will. slow down and eventually stop stop immediately turn right move with constant velocity turn left

PHYS 101 Previous Exam Problems. Kinetic Energy and

Unit 5 Forces I- Newton s First & Second Law

FORCE AND MOTION. Conceptual Questions F G as seen in the figure. n, and a kinetic frictional force due to the rough table surface f k

Examples Newton's Laws and Friction

Newton s First Law and IRFs

Circle the correct answer. For those questions involving calculations, working MUST be shown to receive credit.

Section /07/2013. PHY131H1F University of Toronto Class 9 Preclass Video by Jason Harlow. Based on Knight 3 rd edition Ch. 5, pgs.

= v bag. (ground) vbus (ground). (1)

Thursday February 8. Write these equations in your notes if they re not already there. You will want them for Exam 1 & the Final.

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS AP PHYSICS

PHYS 100 (from 221) Newton s Laws Week8. Exploring the Meaning of Equations

CHAPTER 4 NEWTON S LAWS OF MOTION

Unit 06 Examples. Stuff you asked about:

Chapter Four Holt Physics. Forces and the Laws of Motion

General Physics I Forces

variable Formula S or v SI variable Formula S or v SI 4. How is a Newton defined? What does a Newton equal in pounds?

Newton s 3 Laws. Explain Newton s 3 Laws of Motion. Cite observed evidence for each law of motion.

Welcome back to Physics 211

Dynamics: Newton s Laws of Motion

Forces I. Newtons Laws

Chapter 4 Dynamics: Newton s Laws of Motion

Chapter 5. Force and Motion I

Force, Friction & Gravity Notes

Physics 207 Lecture 7. Lecture 7

Dynamics: Newton s Laws of Motion

Chapter 4. Forces in One Dimension

Forces and Newton s Laws Notes

Review: Newton s Laws

Applying Newton s Laws

Transcription:

PHYS 100: Lecture 6 NEWTON S FIRST and THIRD LAWS First Law: An object subject to no external forces is at rest or moves with constant velocity if viewed from an inertial reference frame. Third law: For every action there is an equal and opposite reaction. F AonB = F BonA Physics 100 Lecture 6, Slide 1

Music Who is the Artist? A) The Meters B) The Neville Brothers C) Trombone Shorty D) Michael Franti E) Radiators Why? Didn t get to play Dr John last time Nevilles: icons of New Orleans hope you had a fun Mardi Gras! Physics 100 Lecture 6, Slide 2

THE BIG IDEAS NOTE: THE BIG IDEAS ARE ALWAYS GIVEN IN THE LAST SLIDE 1. Inertial reference frames are those frames in which Newton s Laws always are TRUE. 2. Forces always come in pairs: F AonB = F BonA Physics 100 Lecture 6, Slide 3

Newton s First Law Suppose a boy is in an elevator and the cable breaks so that the elevator is in free fall. He decides to do one last experiment and releases two balls as shown. What happens to the balls? (A) The balls fall to the floor of the elevator with acceleration = g (B) The balls fall to the floor of the elevator with acceleration > g (C) The balls fall to the floor of the elevator with acceleration < g (D) The balls remain at the same height above the floor g What is the acceleration of the floor of the elevator? What is the acceleration of the balls before release? What is the force on the balls after release? What is the acceleration of the balls after release? a elevator = g a before = g F after = m ball g a after = g After release, the balls do not move with respect to the elevator. Therefore, in the elevator frame, a ball = 0 Elevator is But, F = m ball g NOT inertial frame Therefore, in the elevator frame, F is not equal to ma!! Physics 100 Lecture 6, Slide 4

CheckPoint 2b You ask your friend to help you move. He is about to push a box across the floor when he says, due to Newtons third law the box will push on me with the same force that I push on it, so it's no use to try to push this box. What is wrong with your friend s reasoning? I. Newton s Third Law only applies when there is no acceleration. Once the box moves, the forces are not equal. II. The block can only push back a certain amount of force. Once your friend applies more than that amount of force, the box will move. (A) Both statements are TRUE (B) Both statements are FALSE (C) I is TRUE and II is FALSE (D) I is FALSE and II is TRUE I. Newton s Third Law is ALWAYS TRUE!! You can use it in ALL situations II. It s true that there is a maximum force that the box can exert on your friend. But, what would happen if your friend pushes harder than this? THE BOX WOULD BREAK! Physics 100 Lecture 6, Slide 5

CheckPoint 2b You ask your friend to help you move. He is about to push a box across the floor when he says, due to Newtons third law the box will push on me with the same force that I push on it, so it's no use to try to push this box. What is wrong with your friend s reasoning? (A) Newton's third law only when there is no acceleration. The box will only move if the amount of my friend puts on the box exceeds the amount of force the box puts on me. (B) There is no force acting on the my friend from the box. (C) The acceleration of the box is determined by the force on only on the box, not the force done by the box. (D) None of the above explain the flaw in your friend s reasoning. F me on table F table on me Physics 100 Lecture 6, Slide 6

Newton s Third Law Pairs A block of mass M rests on a frictionless floor as shown The normal force exerted by the floor on the block and the block s weight are Newton s Third Law pairs ( action-reaction forces) M (A) TRUE (B) FALSE Let s start with a freebody diagram: M N Mg Since the block is at rest, ΣF = 0 N = Mg WHY??? Both of these forces are forces exerted on the block Action-Reaction pairs are forces exerted on DIFFERENT OBJECTS Action-Reaction pairs do not appear on the same freebody diagram (what would be the point? They would always cancel!) BUT N = Mg DOES NOT MEAN THESE FORCES ARE ACTION-REACTION PAIRS!! Physics 100 Lecture 6, Slide 7

CheckPoint 1a Block A is stacked on top of Block B in an elevator that is accelerating upwards with a = +5 m/s 2 as shown. Which is greater, F BonA, the force B exerts on A or F AonB, the force A exerts on B? (A) F AonB > F BonA (B) They are the same (C) F BonA > F AonB You said: The force block a exerts on b is greater because both gravity and the force caused by the upward acceleration are pressed down on b, which is characterized only by gravity. According to Newton's first law, the forces that they exert on each other must be equal and opposite. the acceleration upwards is added to the force of B on A, while it is subtracted from the force of A on B. 70 60 50 40 30 20 10 0 Draw freebody diagrams ACTION-REACTION PAIR A M A g F BonA A B C F AonB B M B g N Physics 100 Lecture 6, Slide 8

Follow Up Block A is stacked on top of Block B in an elevator that is accelerating upwards with a = +5 m/s 2 as shown. What is F AonB, the force A exerts on B? (A) F AonB = M A g (B) F AonB = M A a (C) F AonB = M A (a+g) (D) F AonB = M A (a-g) (E) None of these : it depends on M B Draw freebody diagrams ACTION-REACTION PAIR A F AonB QUICKIE: What is magnitude of acceleration of A? (A) a (B) a+g (C) a-g (D) 0 M A g F BonA M B g B N What is net force on A? (positive = up) F BonA - M A g magnitudes: F BonA = F AonB Newton s Second Law F BonA M A g = M A a F BonA = M A (a + g) Physics 100 Lecture 6, Slide 9

CheckPoint 1b How would F AonB, the force A exerts on B, change if the acceleration is reduced to a = +2 m/s 2? (A) F AonB increases with decreasing acceleration a = +2 m/s 2 (B) F AonB stays the same with decreasing acceleration (C) F AonB decreases with decreasing acceleration You said: From the formula for Newtons Third Law, if Fb on a is decreasing then Fa on b must increase. Since the force of A on B only depends on the weight of A (ie, mass of A times acceleration due to gravity), it must not change with the accelration of the elevator. Force is equal to Mass multiplied by the acceleration so if the acceleration decreases so will the force. 60 50 40 30 (C) is correct, but most reasons given for (C) in CheckPoint were not correct!! 20 10 0 A B C Physics 100 Lecture 6, Slide 10

CheckPoint 1b How would F AonB, the force A exerts on B, change if the acceleration is reduced to a = +2 m/s 2? (A) F AonB increases with decreasing acceleration a = +2 m/s 2 (B) F AonB stays the same with decreasing acceleration (C) F AonB decreases with decreasing acceleration (C) is correct, but most reasons given for (C) in Preflight were not correct!! What is wrong with this explanation?? Force is equal to Mass multiplied by the acceleration so if the acceleration decreases so will the force. Draw freebody diagrams ACTION-REACTION PAIR A M A g F BonA F AonB B M B g N This argument works for the NET FORCE Newton s Second Law: NET FORCE = ma F AonB is NOT the NET FORCE! no help here B: NET FORCE = N M B g F AonB N-F AonB decreases A: NET FORCE = F BonA - M A g F BonA decreases Newton s Third Law F AonB decreases Physics 100 Lecture 6, Slide 11

CheckPoint 2a In Case I, Block A rests on block B which rests on the floor. In Case II, the positions are reversed. The mass of block A is twice that of block B Compare F AonB (I) to F AonB (II): (A) F AonB (I) < F AonB (II) You said: (C) F AonB (I) > F AonB (II) (B) F AonB (I) = F AonB (II) In case 1 the force block A exerts on block B would be smaller because the force is negative and in case 2 the force block A exerts on block B would be positive and therefore larger. The forces of the blocks form an action-reaction pair. They stay the same regardless of mass. In Case I Block A is exerting a force equal to its own weight on Block B while in Case II Block A is exerting a normal force equal to the weight of Block B on Block B ALSO, must understand WHY this argument is wrong! 70 60 50 40 30 20 10 0 A B C Most of the reasons given for (C) in the CheckPoint went something like this: Because A is heavier it pushes down more in I than B does in II. This is kinda OK, but I d like to make sure you understand in terms of freebody diagrams Physics 100 Lecture 6, Slide 12

Follow Up Block A rests on block B which rests on the floor. To determine F AonB, You need to draw the freebody diagrams for : (A) A only (B) B only (C) Both A and B Knowing Newton s Third Law, We need only draw the freebody diagram for A!! WHY? Newton s third law tells us the magnitudes of F AonB and F BonA are the same! M A g A F BonA Newton s Third Law F BonA = F AonB a = 0 F BonA = M Ag Why did I bother to do this freebody diagram thing here? F AonB = M A g Your intuition (a block pushes down on another block with its weight) may not work in more complicated situations.. How about 3 blocks?? Physics 100 Lecture 6, Slide 13

Follow Up Block A rests on block B which rests on block C which rests on the floor. You are told: F BonA < F BonC Which of the following statements about the masses MUST be TRUE? (A) M A < M C (B) M A > M C (C) M A > M B (D) We can say nothing about masses. A B C N To find F BonA Freebody for A A M A g F BonA To find F BonC Freebody for AandB A B (M A +M B )g F ConB Freebody for C Will introduce N! Newton s Third Law: F BonC = F ConB Newton s Third Law F BonA = M A g F ConB = (M A +M B )g = F BonC Therefore: F BonA < F BonC for any values of M A and M B!!! Physics 100 Lecture 6, Slide 14

Pushing Blocks Force F is applied to Block 1 which is in contact with Block 2 as shown. Both blocks move together to the right with acceleration a. We want to calculate F 21, the force Block 2 exerts on Block 1. First Question: Compare F 21 and F F 1 2 frictionless (A) F 21 < F (B) F 21 = F (C) F 21 > F STEP 1: Draw Freebody for Block 1 F F 21 1 m 1 g N Block 1 accelerates to the right fl F > F 21 Physics 100 Lecture 6, Slide 15

Pushing Blocks Force F is applied to Block 1 which is in contact with Block 2 as shown. Both blocks move together to the right with acceleration a. We want to calculate F 21, the force Block 2 exerts on Block 1. Second Question: What is the acceleration? F 1 2 frictionless (A) a = F/m 1 (B) a = F/m 2 (C) a = F/(m 1 +m 2 ) (D) need more info STEP 1: Draw Freebody for Blocks 1and2 F 1 2 (m 1 +m 2 )g N Newton s Second Law (Horizontal Direction) F = (m 1 + m 2 ) a a = F/(m 1 + m 2 ) Physics 100 Lecture 6, Slide 16

Pushing Blocks Force F is applied to Block 1 which is in contact with Block 2 as shown. Both blocks move together to the right with acceleration a. We want to calculate F 21, the force Block 2 exerts on Block 1. Third Question: What is F 21? (A) F 21 = 0 (B) F 21 = (m 2 -m 1 )g F 1 2 frictionless a = F/(m 1 +m 2 ) (C) F 21 = Fm 1 /(m 2 +m 1 ) (D) F 21 = Fm 2 /(m 2 +m 1 ) STEP 1: Draw Freebody for Block 1 F F 21 1 m 1 g N Newton s Second Law (Horizontal Direction) F F 21 = m 1 a a = F/(m 1 +m 2 ) F 21 = Fm 2 /(m 2 +m 1 ) NOTE: Even simpler way is to draw FBD for Block 2 to find F 12 Physics 100 Lecture 6, Slide 17

Something Similar? Two blocks connected by a string are pulled across a frictionless floor by force F What is the tension in the string connecting the blocks? (A) T = 0 (B) T = (m 2 -m 1 )g F T 1 2 frictionless (C) T = Fm 1 /(m 2 +m 1 ) (D) T= Fm 2 /(m 2 +m 1 ) STEP 1: Draw Freebody Diagrams F T T 1 2 m 1 g N 1 m 2 g N 2 a = F/(m 1 +m 2 ) Newton s Second Law (Horizontal Direction) F T = m 1 a T = m 2 a a = F/(m 1 +m 2 ) T = Fm 2 /(m 2 +m 1 ) T = Fm 2 /(m 2 +m 1 ) Physics 100 Lecture 6, Slide 18