Physics 11 Chapter 4: Forces and Newton s Laws of Motion. Problem Solving

Similar documents
Chapter 5 Force and Motion

Chapter 5 Force and Motion

PHYS Summer Professor Caillault Homework Solutions. Chapter 5

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

Chapter 4: The laws of motion. Newton s first law

Chapter 4. Newton s Laws of Motion

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.

Chapter 5. Applying Newton s Laws. Newton s Laws. r r. 1 st Law: An object at rest or traveling in uniform. 2 nd Law:

The Laws of Motion ( ) N SOLUTIONS TO PROBLEMS ! F = ( 6.00) 2 + ( 15.0) 2 N = 16.2 N. Section 4.4. Newton s Second Law The Particle Under a Net Force

PS113 Chapter 5 Dynamics of Uniform Circular Motion

Easy. P4.2 Since the car is moving with constant speed and in a straight line, the. resultant force on it must be regardless of whether it is moving

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

Phys 201A. Homework 6 Solutions. F A and F r. B. According to Newton s second law, ( ) ( )2. j = ( 6.0 m / s 2 )ˆ i ( 10.4m / s 2 )ˆ j.

Physics 111 Lecture 5 Circular Motion

Sections and Chapter 10

To Feel a Force Chapter 7 Static equilibrium - torque and friction

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

Force can be exerted by direct contact between bodies: Contact Force.

Uniform Circular Motion

SAMPLE QUIZ 3 - PHYSICS For a right triangle: sin θ = a c, cos θ = b c, tan θ = a b,

to point uphill and to be equal to its maximum value, in which case f s, max = μsfn

F g. = G mm. m 1. = 7.0 kg m 2. = 5.5 kg r = 0.60 m G = N m 2 kg 2 = = N

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

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

Physics 11 Chapter 3: Vectors and Motion in Two Dimensions. Problem Solving

Physics 101 Lecture 6 Circular Motion

7.2. Coulomb s Law. The Electric Force

Physics Fall Mechanics, Thermodynamics, Waves, Fluids. Lecture 6: motion in two and three dimensions III. Slide 6-1

Phys 201A. Homework 5 Solutions

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

Centripetal Force. Lecture 11. Chapter 8. Course website:

Physics 11 Chapter 20: Electric Fields and Forces

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

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.

Physics 211: Newton s Second Law

DYNAMICS OF UNIFORM CIRCULAR MOTION

Lab #4: Newton s Second Law

Chapters 5-8. Dynamics: Applying Newton s Laws

Spring 2001 Physics 2048 Test 3 solutions

PHYSICS 1210 Exam 2 University of Wyoming 14 March ( Day!) points

Movie Review Part One due Tuesday (in class) please print

Chapter 4. Newton s Laws of Motion. Newton s Law of Motion. Sir Isaac Newton ( ) published in 1687

Physics 107 TUTORIAL ASSIGNMENT #8

Chapter 5: Uniform Circular Motion

Multiple choice questions [100 points] As shown in the figure, a mass M is hanging by three massless strings from the ceiling of a room.

( ) ( ) Review of Force. Review of Force. r = =... Example 1. What is the dot product for F r. Solution: Example 2 ( )

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.

PHYS Summer Professor Caillault Homework Solutions. Chapter 9

AP * PHYSICS B. Circular Motion, Gravity, & Orbits. Teacher Packet

15 B1 1. Figure 1. At what speed would the car have to travel for resonant oscillations to occur? Comment on your answer.

INTRODUCTION. 2. Vectors in Physics 1

Physics 181. Assignment 4

Circular Orbits. and g =

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

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

20-9 ELECTRIC FIELD LINES 20-9 ELECTRIC POTENTIAL. Answers to the Conceptual Questions. Chapter 20 Electricity 241

Objective Notes Summary

Describing Circular motion

FZX: Personal Lecture Notes from Daniel W. Koon St. Lawrence University Physics Department CHAPTER 7

Flux. Area Vector. Flux of Electric Field. Gauss s Law

Department of Physics, Korea University Page 1 of 5

Section 26 The Laws of Rotational Motion

Physics C Rotational Motion Name: ANSWER KEY_ AP Review Packet

Chap 5. Circular Motion: Gravitation

EN40: Dynamics and Vibrations. Midterm Examination Thursday March

Chapter Sixteen: Electric Charge and Electric Fields

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?

Motion in a Plane Uniform Circular Motion

1121 T Question 1

Electricity Revision ELECTRICITY REVISION KEY CONCEPTS TERMINOLOGY & DEFINITION. Physical Sciences X-Sheets

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

Ch. 4: FOC 9, 13, 16, 18. Problems 20, 24, 38, 48, 77, 83 & 115;

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

4. Two and Three Dimensional Motion

Current Balance Warm Up

Rectilinea Motion. A foce P is applied to the initially stationay cat. Detemine the velocity and displacement at time t=5 s fo each of the foce histoi

17.1 Electric Potential Energy. Equipotential Lines. PE = energy associated with an arrangement of objects that exert forces on each other

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

CHAPTER 25 ELECTRIC POTENTIAL

Physics 201 Homework 4

3.3 Centripetal Force

Motion along curved path *

Motion in Two Dimensions

Solutions to Problems : Chapter 19 Problems appeared on the end of chapter 19 of the Textbook

4.[1pt] Two small spheres with charges -4 C and -9 C are held 9.5 m apart. Find the magnitude of the force between them.

Physics 207 Lecture 5. Lecture 5

Objects usually are charged up through the transfer of electrons from one object to the other.

Recap. Centripetal acceleration: v r. a = m/s 2 (towards center of curvature)

Ch 13 Universal Gravitation

3.2 Centripetal Acceleration

Chapter 12. Kinetics of Particles: Newton s Second Law

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

PHYS 1444 Lecture #5

Easy. r p 2 f : r p 2i. r p 1i. r p 1 f. m blood g kg. P8.2 (a) The momentum is p = mv, so v = p/m and the kinetic energy is

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS IB PHYSICS

Uniform Circular Motion

Voltage ( = Electric Potential )

2 Governing Equations

QUESTION 1 [25 points]

Lab 10: Newton s Second Law in Rotation

Transcription:

Physics 11 Chapte 4: Foces and Newton s Laws of Motion Thee is nothing eithe good o bad, but thinking makes it so. William Shakespeae It s not what happens to you that detemines how fa you will go in life; it is how you handle what happens to you. Zig Zigla Reading: pages 102 125 Outline: Newton s 1 st law inetia and mass foces what is a foce? diffeent kinds of foces identifying foces Newton s 2 nd law units of foce fee-body diagams (FBDs) Newton s 3 d law Poblem Solving Definite pocedues has been devised fo identifying the foces acting on an object and then dawing a fee-body diagam. These pocedues ae given in Tactics Box 4.2 on page 111 and Tactics Box 4.3 on page 118. The list below gives a simplified vesion of these pocedues. 1. Identify the object to be consideed. It is usually the object on which the given foces act o about which a question is posed. 2. Daw a sketch of the situation that includes the object of inteest and all othe objects (opes, sufaces, ) that touch it. Identify all contact and long-ange foces that act on the object. The had pat is getting all the foces. If appopiate, don't foget to include the gavitational foce on the object, the nomal foce of a suface on the object, any fictional foces, and the foces of any stings o ods attached to the object. (Some students eoneously include foces that ae not acting on the object. Fo each foce you include you should be able to point to something in the envionment that is exeting the foce. This simple pocedue should pevent you fom eoneously including a nomal foce, fo example, when the object you ae consideing is not in contact with a suface.) 3. Daw a coodinate system and epesent the object by a dot at the oigin of the coodinate axes. 4. Daw vectos that epesent each of the identified foces. Place the tail of each foce vecto on the object, which is epesented as a dot. Be sue to label each foce vecto. 5. Daw and label the net foce vecto F net next to the fee-body diagam. Check that F net points in the same diection as the acceleation vecto a, o, if appopiate, wite F net = 0.

SUMMARY The goal of Chapte 4 has been to establish a connection between foce and motion. GENERAL PRINCIPLES Newton s Fist Law Conside an object with no foce acting on it. If it is at est, it will emain at est. If it is in motion, then it will continue to move in a staight line at a constant speed. v F 5 0 v v v v a 5 0 The fist law tells us that no cause is needed fo motion. Unifom motion is the natual state of an object. Newton s Second Law An object with mass m will undego acceleation a B = FB net m whee the net foce F B 3 + Á F B net = F B 1 + F B 2 + is the vecto sum of all the individual foces acting on the object. v v F net v a v The second law tells us that a net foce causes an object to acceleate. This is the connection between foce and motion. The acceleation points in the diection of F B net. v Newton s Thid Law Evey foce occus as one membe of an action/eaction pai of foces. The two membes of an action/eaction pai: act on two diffeent objects. point in opposite diections and ae equal in magnitude: F B on A F B A on B =-F B B on A A B Action/eaction pai A B F A on B IMPORTANT CONCEPTS Foce is a push o pull on an object. Foce is a vecto, with a magnitude and a diection. A foce equies an agent. A foce is eithe a contact foce o a long-ange foce. The SI unit of foce is the newton (N). A 1 N foce will cause a 1 kg mass to acceleate at 1 m/s 2. Net foce is the vecto sum of all the foces acting on an object. F 1 F 3 F 2 5 F net 5 F 1 1 F 2 1 F 3 Mass is the popety of an object that detemines its esistance to acceleation. If the same foce is applied to objects A and B, then the atio of thei acceleations is elated to the atio of thei masses as a A a B = m B m A The mass of objects can be detemined in tems of thei acceleations. APPLICATIONS Identifying Foces Foces ae identified by locating the points whee othe objects touch the object of inteest. These ae points whee contact foces ae exeted. In addition, objects feel a long-ange weight foce. Thust foce F thust Weight w Nomal foce n Fee-Body Diagams A fee-body diagam epesents the object as a paticle at the oigin of a coodinate system. Foce vectos ae dawn with thei tails on the paticle. The net foce vecto is dawn beside the diagam. y n w F thust F net x

Questions and Example Poblems fom Chapte 4 Question 1 Why do you lung fowad when you ca suddenly comes to a halt? Why ae you pessed backwad against the seat when you ca apidly acceleates? Question 2 A peson sits on a sloped hillside. Is it eve possible to have the static fiction foce on this peson point down the hill? Explain. Question 3 Two foces act on an object that is on a fictionless suface, as shown below. Rank these situations fom geatest acceleation to least acceleation. (Note: All vectos diected to the ight ae positive, and those to the left ae negative. Also, 0 m/s 2 > -10 m/s 2.) Geatest 1 2 3 4 Least

Poblem 1 A baseball playe is sliding into second base. Identify the foces on the baseball playe. Poblem 2 A constant foce is applied to an object, causing the object to acceleate at 8.0 m/s 2. What will the acceleation be if a) The foce is doubled? b) The object's mass is doubled? c) The foce and the object's mass ae both doubled? d) The foce is doubled and the object's mass is halved? Poblem 3 Two childen fight ove a 200 g stuffed bea. The 25 kg boy pulls to the ight with a 15 N foce and the 20 kg gil pulls to the left with a 17 N foce. Ignoe all othe foces on the bea (such as its weight). a) At this instant, can you say what the velocity of the bea is? If so, what ae the magnitude and diection of the velocity? b) At this instant, can you say what the acceleation of the bea is? If so, what ae the magnitude and diection of the acceleation?

Poblem 4 In the figues below, one foce is missing. Use the given diection of acceleation to detemine the missing foce and daw it on object. Poblem 5 Vey small foces can have temendous effects on the motion of vey small objects. Conside a single electon, with a mass of 9.1 10-31 kg, subject to a single foce equal to the weight of a penny, 2.5 10-2 N. What is the acceleation of the electon?

Poblem 6 When a 58-g tennis ball is seved, it acceleates fom est to a speed of 45 m/s. The impact with the acket gives the ball a constant acceleation ove a distance of 44 cm. What is the magnitude of the net foce acting on the ball? Poblem 7 A student daws the flawed fee-body diagam shown in the figue below to epesent the foces acting on a golf ball that is taveling upwad and to the ight a vey shot time afte being hit off the tee. Ai esistance is assumed to be elevant. Identify the eos in the diagam, then daw a coect fee-body diagam fo this situation.

Poblem 8 Fo each situation, daw a sketch of the situation, a motion diagam, and a FBD. a) An elevato, suspended by a single cable, has just left the tenth floo and is speeding up as it descends towad the gound floo. b) A heavy box is in the back of a tuck. The tuck is acceleating to the ight. Apply you analysis to the box. Poblem 9 Fo each situation, daw a sketch of the situation, a motion diagam, and a FBD. a) A ocket is being launched staight up. Ai esistance is not negligible. b) You've slammed on the bakes and you ca is skidding to a stop while going down a 20 hill.