Newton s second law: dp dt. p = mv. Sergi Hildebrandt Cahill 364)

Size: px
Start display at page:

Download "Newton s second law: dp dt. p = mv. Sergi Hildebrandt Cahill 364)"

Transcription

1 Newton s second law: SF dp dt S p = mv Sergi Hildebrandt (srh@caltech.edu. Cahill 364)

2 Watch also: Video 1 Video 2

3

4 F M B µs M A 0 µ s = 0 For M A, M B and µ s, find the maximum force, F, that can be applied without sliding M B

5 The most interesting thing to learn from this problem is the action/reaction pair due to friction between body A and B and their direction (to the right in B and to the left in A). F f M B µs M A f 0 µ s = 0 f = M B a B and F f = M A a A We want to impose a A =a B =a. Summing up get: F = (M A +M B ) a. On the other hand, the static friction is at most f=µ s N B =µ s M B g. Therefore, the maximum acceleration is a=f/m B = µ s g and: F max =(M A +M B )a max = (M A +M B )µ s g

6 FP9 from the Course webpage

7

8

9

10

11

12

13 e) Not yet. Later on in the course, when we deal with angular momentum

14 Consider a flexible chain of length L and linear density l (M=lL)lying on an incline as shown in the figure. There s friction all along the incline. The chain is initially at x=x 0 and at rest. x a b 1) Find the acceleration of the chain in terms of x and any other relevant variable of the problem 2) Find the speed when x=0

15

16

17

18

19

20

21 Write it down!

22 Write it down! F = m a?

23 Write it down! F = m a? NOPE!

24 Write it down! F = d(mv)/dt!

25 F = d(mv)/dt F = v dm/dt + ma!

26 If m = constant, then F = ma

27 F = ma Who wrote this equation? Probably the most used equation in physics!

28 ?

29 1707, Basel, Switzerland 1783, Saint Petersburg, Russia Leonhard Euler 65 years after Newton published it!

30 What s the difference compared to the problem of the chain on an incline? Lifting up a chain Chain falling through a hole

31 y

32

33

34

35

36

37 y

38

39

40

41

42

43

44 DR. NO S ANTIGRAVITY MACHINE SERGI R HILDEBRANDT Figure 1 Dr. No wants to get big money from some CEO and Army Generals by selling the idea that he has discovered the secret for antigrativity. He plans to launch his Dr.No-Box1 and once it has attained a certain speeed, v 0,he llturno the engines as he pushes the button of what he claims is the antigravity engine. He will show to his audience that the spacecraft will continue to move upwards with constant velocity, despite the gravitational attraction of the Earth. After some demonstration time, he ll turn o the antigravity engine and come back to the ground, landing with some parachutes. Please, answer the following questions: a) How is it possible? b) The picture on the right hand side, shows what his fooling plan looks like: he will eject mass from the original spacecraft, after he pushes the antigravity button and during the demonstration time. The mass and speed with which the mass is ejected on both sides of the spacecraft is the same, so there is no horizontal force or motion. Find the relationship between v 0, g (the Earth s 1

45 2 SERGI R HILDEBRANDT gravitational acceleration), the initial mass of the whole system, M 0 and the time of the antigravity demonstration, t. c) How much mass should be ejected if v 0 =10m/s, t =1min?Doesitmakesenseinpractice? (Hint: assume that the minimum mass at the end has to be the mass of the enclosure of the spacecraft, plus engines, people, etc... say about 10,000 kg). d) Dr. No s engines cannot speed up Dr.No-Box1 faster than the speed of sound (he also wants to keep his tests silent ). What would be the minimum initial weight of the spacecraft be if the antigravity demonstration is a minute long?

46 DR. NO S ANTIGRAVITY MACHINE 3 1. Solutions a) Yes. Force is equal to d(m~v)/dt, sothatvelocitymaybeconstantifthemassvaries. The spacecraft can only lose mass. Therefore, dm/dt < 0andthatimpliesthatthedirectionofthe velocity has to be the contrary of that of the force. The trick may work when moving upwards, but not when descending.

47 4 SERGI R HILDEBRANDT 2. Solutions a) Yes. Force is equal to d(m~v)/dt, sothatvelocitymaybeconstantifthemassvaries. The spacecraft can only lose mass. Therefore, dm/dt < 0andthatimpliesthatthedirectionofthe velocity has to be the contrary of that of the force. The trick may work when moving upwards, but not when descending. b) F ~ = ~v 0 dm/dt, with~v 0 the velocity when Dr. No stops the engines of his spacecraft. On the other hand, W ~ = m~g (~g is pointing downwards). Consequently, i) ~v and ~g must be parallel. One can leave the sign of the direction free and check that + would imply increase of mass, and decrease. Let s choose, as explained in a) the negative sign and re-arrange W ~ = ~v 0 dm/dt: g/v 0 dt = dm/m, which is a simple di erential equation. Integrating, with the initial condition of m(t = t 0 )=m 0 : (1) m(t) =m 0 e g/v 0 t, ~v 0 = (v 0 /g)~g = v 0ˆk, where t is the time of the demonstration ( = t f t 0,ifonewishes). Itmakessensedimensionally, and ~ W = d(m~v 0 )/dt is satisfied.

48 DR. NO S ANTIGRAVITY MACHINE 5 3. Solutions a) Yes. Force is equal to d(m~v)/dt, sothatvelocitymaybeconstantifthemassvaries. The spacecraft can only lose mass. Therefore, dm/dt < 0andthatimpliesthatthedirectionofthe velocity has to be the contrary of that of the force. The trick may work when moving upwards, but not when descending. b) F ~ = ~v 0 dm/dt, with~v 0 the velocity when Dr. No stops the engines of his spacecraft. On the other hand, W ~ = m~g (~g is pointing downwards). Consequently, i) ~v and ~g must be parallel. One can leave the sign of the direction free and check that + would imply increase of mass, and decrease. Let s choose, as explained in a) the negative sign and re-arrange W ~ = ~v 0 dm/dt: g/v 0 dt = dm/m, which is a simple di erential equation. Integrating, with the initial condition of m(t = t 0 )=m 0 : (2) m(t) =m 0 e g/v 0 t, ~v 0 = (v 0 /g)~g = v 0ˆk, where t is the time of the demonstration ( = t f t 0,ifonewishes). Itmakessensedimensionally, and ~ W = d(m~v 0 )/dt is satisfied. c) The final mass will be: m F = m 0 e 58.8 = m 0!! No way in practice of having m 0.Recall m F =10, 000 kg. However: d) The speed of sound is approximately 342 m/s at sea level and at 20 C. Now, m F = m 0 e 1.72 = 0.18m 0. This sets the minimum mass of the spacecraft. Less will not provide enough mass to be ejected. If the final mass is 10,000 kg, then the minimum initial mass of Dr.No-Box1 has to be: m 0 =10, 000/0.18 = 55, 806 kg. Seems okay! Let s do it. address: srh@caltech.edu

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

Forces and Newton s Laws Reading Notes. Give an example of a force you have experienced continuously all your life. Forces and Newton s Laws Reading Notes Name: Section 4-1: Force What is force? Give an example of a force you have experienced continuously all your life. Give an example of a situation where an object

More information

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

Dynamic equilibrium: object moves with constant velocity in a straight line. = 0, a x = i Dynamic equilibrium: object moves with constant velocity in a straight line. We note that F net a s are both vector quantities, so in terms of their components, (F net ) x = i (F i ) x = 0, a x = i (a

More information

Quick Introduction to Momentum Principle. Momentum. Momentum. Basic principle not at all obvious on Earth 24/02/11

Quick Introduction to Momentum Principle. Momentum. Momentum. Basic principle not at all obvious on Earth 24/02/11 Momentum Quick Introduction to Momentum Principle We will come back to all of this - this is just a taster. The momentum principle is another way of saying Newton s Laws It is one of the three great principles

More information

Example force problems

Example force problems PH 105 / LeClair Fall 2015 Example force problems 1. An advertisement claims that a particular automobile can stop on a dime. What net force would actually be necessary to stop a 850 kg automobile traveling

More information

Yung Tae Kim (Physics PhD) Physicist and Educator Puget Sound Community School Seattle, WA

Yung Tae Kim (Physics PhD) Physicist and Educator Puget Sound Community School Seattle, WA PHYSICIST PROFILE Yung Tae Kim (Physics PhD) Physicist and Educator Puget Sound Community School Seattle, WA Why Physics? Tae, who enjoyed mathematics in high school, signed up for an honors physics class

More information

Laws of Motion. Multiple Choice Questions

Laws of Motion. Multiple Choice Questions The module presented herein is a sequel to MCQs on different units in Physics, a few viz. Rotational motion and Oscillations etc. posted earlier. The contents of the documents are intended to give the

More information

Answers without work shown will not be given any credit.

Answers without work shown will not be given any credit. MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics Physics 8.01 Fall Term 2012 Problem 1 of 4 (25 points) Exam 1 Solutions with Grading Scheme Answers without work shown will not be given any

More information

Physics 2414 Group Exercise 8. Conservation of Energy

Physics 2414 Group Exercise 8. Conservation of Energy Physics 244 Group Exercise 8 Name : OUID : Name 2: OUID 2: Name 3: OUID 3: Name 4: OUID 4: Section Number: Solutions Solutions Conservation of Energy A mass m moves from point i to point f under the action

More information

l Every object in a state of uniform motion tends to remain in that state of motion unless an

l Every object in a state of uniform motion tends to remain in that state of motion unless an Motion and Machine Unit Notes DO NOT LOSE! Name: Energy Ability to do work To cause something to change move or directions Energy cannot be created or destroyed, but transferred from one form to another.

More information

MOTION & FORCES. Observing Motion. Speed and Velocity. Distance vs. Displacement CHAPTERS 11 & 12

MOTION & FORCES. Observing Motion. Speed and Velocity. Distance vs. Displacement CHAPTERS 11 & 12 Observing Motion CHAPTERS 11 & 12 MOTION & FORCES Everything surrounding us is in motion, but it is relative to other object that remain in place. Motion is observed using a frame of reference. Motion

More information

Review: Newton s Laws

Review: Newton s Laws More force was needed to stop the rock Review: Newton s Laws F r 1 F r F r 3 F r 4 2 Newton s First Law The velocity of an object does not change unless a force acts on the object Newton s Second Law:

More information

Newton s Laws of Motion and Gravitation

Newton s Laws of Motion and Gravitation Newton s Laws of Motion and Gravitation Introduction: In Newton s first law we have discussed the equilibrium condition for a particle and seen that when the resultant force acting on the particle is zero,

More information

PYP 001 FIRST MAJOR EXAM CODE: TERM: 151 SATURDAY, OCTOBER 17, 2015 PAGE: 1

PYP 001 FIRST MAJOR EXAM CODE: TERM: 151 SATURDAY, OCTOBER 17, 2015 PAGE: 1 TERM: 151 SATURDAY, OCTOBER 17, 2015 PAGE: 1 *Read the following (20) questions and choose the right answer: 1 The figure below represents the speed-time graph for the motion of a vehicle during a 7.0-minute

More information

Forces Part 1: Newton s Laws

Forces Part 1: Newton s Laws Forces Part 1: Newton s Laws Last modified: 13/12/2017 Forces Introduction Inertia & Newton s First Law Mass & Momentum Change in Momentum & Force Newton s Second Law Example 1 Newton s Third Law Common

More information

Dynamics Review Checklist

Dynamics Review Checklist Dynamics Review Checklist Newton s Laws 2.1.1 Explain Newton s 1 st Law (the Law of Inertia) and the relationship between mass and inertia. Which of the following has the greatest amount of inertia? (a)

More information

P - f = m a x. Now, if the box is already moving, for the frictional force, we use

P - f = m a x. Now, if the box is already moving, for the frictional force, we use Chapter 5 Class Notes This week, we return to forces, and consider forces pointing in different directions. Previously, in Chapter 3, the forces were parallel, but in this chapter the forces can be pointing

More information

Marr College Science. Forces. Learning Outcomes and Summary Notes

Marr College Science. Forces. Learning Outcomes and Summary Notes Marr College Science Forces Learning Outcomes and Summary Notes Learning Intentions By the end of this unit I will be able to 1. Describe a force as a push or a pull. 2. Describe the effects of forces

More information

POGIL: Newton s First Law of Motion and Statics. Part 1: Net Force Model: Read the following carefully and study the diagrams that follow.

POGIL: Newton s First Law of Motion and Statics. Part 1: Net Force Model: Read the following carefully and study the diagrams that follow. POGIL: Newton s First Law of Motion and Statics Name Purpose: To become familiar with the forces acting on an object at rest Part 1: Net Force Model: Read the following carefully and study the diagrams

More information

Practice Test for Midterm Exam

Practice Test for Midterm Exam A.P. Physics Practice Test for Midterm Exam Kinematics 1. Which of the following statements are about uniformly accelerated motion? Select two answers. a) If an object s acceleration is constant then it

More information

Chapter 7. Preview. Objectives Tangential Speed Centripetal Acceleration Centripetal Force Describing a Rotating System. Section 1 Circular Motion

Chapter 7. Preview. Objectives Tangential Speed Centripetal Acceleration Centripetal Force Describing a Rotating System. Section 1 Circular Motion Section 1 Circular Motion Preview Objectives Tangential Speed Centripetal Acceleration Centripetal Force Describing a Rotating System Section 1 Circular Motion Objectives Solve problems involving centripetal

More information

PHYSICS 221, FALL 2009 EXAM #1 SOLUTIONS WEDNESDAY, SEPTEMBER 30, 2009

PHYSICS 221, FALL 2009 EXAM #1 SOLUTIONS WEDNESDAY, SEPTEMBER 30, 2009 PHYSICS 221, FALL 2009 EXAM #1 SOLUTIONS WEDNESDAY, SEPTEMBER 30, 2009 Note: The unit vectors in the +x, +y, and +z directions of a right-handed Cartesian coordinate system are î, ĵ, and ˆk, respectively.

More information

Phys101 Second Major-131 Zero Version Coordinator: Dr. A. A. Naqvi Sunday, November 03, 2013 Page: 1

Phys101 Second Major-131 Zero Version Coordinator: Dr. A. A. Naqvi Sunday, November 03, 2013 Page: 1 Coordinator: Dr. A. A. Naqvi Sunday, November 03, 2013 Page: 1 Q1. Two forces are acting on a 2.00 kg box. In the overhead view of Figure 1 only one force F 1 and the acceleration of the box are shown.

More information

Webreview practice test. Forces (again)

Webreview practice test. Forces (again) Please do not write on test. ID A Webreview 4.3 - practice test. Forces (again) Multiple Choice Identify the choice that best completes the statement or answers the question. 1. A 5.0-kg mass is suspended

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

Chapter 6: Systems in Motion

Chapter 6: Systems in Motion Chapter 6: Systems in Motion The celestial order and the beauty of the universe compel me to admit that there is some excellent and eternal Being, who deserves the respect and homage of men Cicero (106

More information

Solving two-body problems with Newton s Second Law. Example Static and Kinetic Friction. Section 5.1 Friction 10/15/13

Solving two-body problems with Newton s Second Law. Example Static and Kinetic Friction. Section 5.1 Friction 10/15/13 Solving two-body problems with Newton s Second Law You ll get multiple equations from the x and y directions, these equations can be solved simultaneously to find unknowns 1. Draw a separate free body

More information

Laws of Motion. A fighter aircraft is looping in a vertical plane. The minimum velocity at the highest point is (Given r = radius of the loop) a) gr b) gr c) gr d) 3gr. In non-inertial frame, the second

More information

Recall: Gravitational Potential Energy

Recall: Gravitational Potential Energy Welcome back to Physics 15 Today s agenda: Work Power Physics 15 Spring 017 Lecture 10-1 1 Recall: Gravitational Potential Energy For an object of mass m near the surface of the earth: U g = mgh h is height

More information

The Laws of Motion. Before You Read. Science Journal

The Laws of Motion. Before You Read. Science Journal The Laws of Motion Before You Read Before you read the chapter, use the What I know column to list three things you know about motion. Then list three questions you have about motion in the What I want

More information

Dynamics Review Checklist

Dynamics Review Checklist Dynamics Review Checklist Newton s Laws 2.1.1 Explain Newton s 1 st Law (the Law of Inertia) and the relationship between mass and inertia. Which of the following has the greatest amount of inertia? (a)

More information

AP Physics C 2015 Summer Assignment

AP Physics C 2015 Summer Assignment AP Physics C 2015 Summer Assignment College Board (the people in charge of AP exams) recommends students to only take AP Physics C if they have already taken a 1 st year physics course and are currently

More information

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

Chapter 4. Forces and Newton s Laws of Motion. continued Chapter 4 Forces and Newton s Laws of Motion continued Quiz 3 4.7 The Gravitational Force Newton s Law of Universal Gravitation Every particle in the universe exerts an attractive force on every other

More information

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

Main points of today s lecture: Normal force Newton s 3 d Law Frictional forces: kinetic friction: static friction Examples. Physic 231 Lecture 9 Main points of today s lecture: Normal force Newton s 3 d Law Frictional forces: kinetic friction: static friction Examples. Physic 3 Lecture 9 f N k = µ k f N s < µ s Atwood s machine Consider the Atwood

More information

3. The diagram shows two bowling balls, A and B, each having a mass of 7.00 kilograms, placed 2.00 meters apart.

3. The diagram shows two bowling balls, A and B, each having a mass of 7.00 kilograms, placed 2.00 meters apart. 1. Which statement describes the gravitational force and the electrostatic force between two charged particles? A) The gravitational force may be either attractive or repulsive, whereas the electrostatic

More information

MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question.

MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. Name MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. 1) A baseball is thrown vertically upward and feels no air resistance. As it is rising A) both

More information

= v 0 x. / t = 1.75m / s 2.25s = 0.778m / s 2 nd law taking left as positive. net. F x ! F

= v 0 x. / t = 1.75m / s 2.25s = 0.778m / s 2 nd law taking left as positive. net. F x ! F Multiple choice Problem 1 A 5.-N bos sliding on a rough horizontal floor, and the only horizontal force acting on it is friction. You observe that at one instant the bos sliding to the right at 1.75 m/s

More information

Dynamics; Newton s Laws of Motion

Dynamics; Newton s Laws of Motion Dynamics; Newton s Laws of Motion Force A force is any kind of push or pull on an object. An object at rest needs a force to get it moving; a moving object needs a force to change its velocity. The magnitude

More information

Dynamics of Systems of Particles. Hasbun, Ch 11 Thornton & Marion, Ch 9

Dynamics of Systems of Particles. Hasbun, Ch 11 Thornton & Marion, Ch 9 Dynamics of Systems of Particles Hasbun, Ch 11 Thornton & Marion, Ch 9 Center of Mass Discrete System Center of Mass R CM 1 m i r i M i v CM = RCM 1 m i v i M a CM = v CM = RCM 1 M i m i a i i Center of

More information

Physics 2211 A & B Quiz #3 Solutions Fall 2016

Physics 2211 A & B Quiz #3 Solutions Fall 2016 Physics 2211 A & B Quiz #3 Solutions Fall 2016 I. (16 points) A block of mass m 1 is connected by an ideal rope passing over an ideal pulley to a block of mass m 2. The block of mass m 1 slides up a plane

More information

Physics Exam 2 October 11, 2007

Physics Exam 2 October 11, 2007 INSTRUCTIONS: Write your NAME on the front of the blue exam booklet. The exam is closed book, and you may have only pens/pencils and a calculator (no stored equations or programs and no graphing). Show

More information

MOMENTUM, IMPULSE & MOMENTS

MOMENTUM, IMPULSE & MOMENTS the Further Mathematics network www.fmnetwork.org.uk V 07 1 3 REVISION SHEET MECHANICS 1 MOMENTUM, IMPULSE & MOMENTS The main ideas are AQA Momentum If an object of mass m has velocity v, then the momentum

More information

AP PHYSICS C Momentum Name: AP Review

AP PHYSICS C Momentum Name: AP Review AP PHYSICS C Momentum Name: AP Review Momentum How hard it is to stop a moving object. Related to both mass and velocity. For one particle p = mv For a system of multiple particles P = p i = m ivi Units:

More information

CHAPTER 2 TEST REVIEW

CHAPTER 2 TEST REVIEW IB PHYSICS Name: Period: Date: # Marks: 69 Raw Score: IB Curve: DEVIL PHYSICS BADDEST CLASS ON CAMPUS CHAPTER 2 TEST REVIEW 1. Samantha walks along a horizontal path in the direction shown. The curved

More information

PHYSICS 221, FALL 2010 EXAM #1 Solutions WEDNESDAY, SEPTEMBER 29, 2010

PHYSICS 221, FALL 2010 EXAM #1 Solutions WEDNESDAY, SEPTEMBER 29, 2010 PHYSICS 1, FALL 010 EXAM 1 Solutions WEDNESDAY, SEPTEMBER 9, 010 Note: The unit vectors in the +x, +y, and +z directions of a right-handed Cartesian coordinate system are î, ĵ, and ˆk, respectively. In

More information

Preparing for Six Flags Physics Concepts

Preparing for Six Flags Physics Concepts Preparing for Six Flags Physics Concepts uniform means constant, unchanging At a uniform speed, the distance traveled is given by Distance = speed x time At uniform velocity, the displacement is given

More information

Net Force and Acceleration

Net Force and Acceleration NEWTON'S SECOND LAW Net Force and Acceleration According to Newton: v A constant velocity is the natural state of motion To accelerate a physical system requires a force F The amount of force required

More information

MA 102 Mathematics II Lecture Feb, 2015

MA 102 Mathematics II Lecture Feb, 2015 MA 102 Mathematics II Lecture 1 20 Feb, 2015 Differential Equations An equation containing derivatives is called a differential equation. The origin of differential equations Many of the laws of nature

More information

University Physics 226N/231N Old Dominion University. More Circular Motion, then Newton s Laws

University Physics 226N/231N Old Dominion University. More Circular Motion, then Newton s Laws University Physics 226N/231N Old Dominion University More Circular Motion, then Newton s Laws Dr. Todd Satogata (ODU/Jefferson Lab) satogata@jlab.org http://www.toddsatogata.net/2016-odu Wednesday, September

More information

Chapter 4 Forces Newton s Laws of Motion

Chapter 4 Forces Newton s Laws of Motion Chapter 4 Forces Newton s Laws of Motion Forces Force A vector quantity that changes the velocity vector of an object. When you hit a baseball, the velocity of the ball changes. Can be a push or a pull

More information

Forces and Motion. Reference: Prentice Hall Physical Science: Concepts in Action Chapter 12

Forces and Motion. Reference: Prentice Hall Physical Science: Concepts in Action Chapter 12 Forces and Motion Reference: Prentice Hall Physical Science: Concepts in Action Chapter 12 What is Force? A push or pull that acts on an object Can cause a resting object to move Can accelerate a moving

More information

dt 2 x = r cos(θ) y = r sin(θ) r = x 2 + y 2 tan(θ) = y x A circle = πr 2

dt 2 x = r cos(θ) y = r sin(θ) r = x 2 + y 2 tan(θ) = y x A circle = πr 2 v = v i + at a dv dt = d2 x dt 2 A sphere = 4πr 2 x = x i + v i t + 1 2 at2 x = r cos(θ) V sphere = 4 3 πr3 v 2 = v 2 i + 2a x F = ma R = v2 sin(2θ) g y = r sin(θ) r = x 2 + y 2 tan(θ) = y x a c = v2 r

More information

Practice. Newton s 3 Laws of Motion. Recall. Forces a push or pull acting on an object; a vector quantity measured in Newtons (kg m/s²)

Practice. Newton s 3 Laws of Motion. Recall. Forces a push or pull acting on an object; a vector quantity measured in Newtons (kg m/s²) Practice A car starts from rest and travels upwards along a straight road inclined at an angle of 5 from the horizontal. The length of the road is 450 m and the mass of the car is 800 kg. The speed of

More information

PHYSICS 121 FALL Homework #3 - Solutions. Problems from Chapter 5: 3E, 7P, 11E, 15E, 34P, 45P

PHYSICS 121 FALL Homework #3 - Solutions. Problems from Chapter 5: 3E, 7P, 11E, 15E, 34P, 45P PHYSICS 121 FALL 2003 - Homework #3 - Solutions Problems from Chapter 5: 3E, 7P, 11E, 15E, 34P, 45P 3 We are only concerned with horizontal forces in this problem (gravity plays no direct role) We take

More information

One-Dimensional Motion Review IMPORTANT QUANTITIES Name Symbol Units Basic Equation Name Symbol Units Basic Equation Time t Seconds Velocity v m/s

One-Dimensional Motion Review IMPORTANT QUANTITIES Name Symbol Units Basic Equation Name Symbol Units Basic Equation Time t Seconds Velocity v m/s One-Dimensional Motion Review IMPORTANT QUANTITIES Name Symbol Units Basic Equation Name Symbol Units Basic Equation Time t Seconds Velocity v m/s v x t Position x Meters Speed v m/s v t Length l Meters

More information

Chapter 12 Study Guide

Chapter 12 Study Guide Chapter 12 Study Guide Key Concepts 12.1 12.2 12.3 12.4 A force can cause a resting object to move, or it can accelerate a moving object by changing the object s speed or direction. When the forces on

More information

Physics 12 Unit 2: Vector Dynamics

Physics 12 Unit 2: Vector Dynamics 1 Physics 12 Unit 2: Vector Dynamics In this unit you will extend your study of forces. In particular, we will examine force as a vector quantity; this will involve solving problems where forces must be

More information

Force. The cause of an acceleration or change in an object s motion. Any kind of a push or pull on an object.

Force. The cause of an acceleration or change in an object s motion. Any kind of a push or pull on an object. Force The cause of an acceleration or change in an object s motion. Any kind of a push or pull on an object. Forces do not always give rise to motion. Forces can be equal and opposite. Force is a vector

More information

Help Desk: 9:00-5:00 Monday-Thursday, 9:00-noon Friday, in the lobby of MPHY.

Help Desk: 9:00-5:00 Monday-Thursday, 9:00-noon Friday, in the lobby of MPHY. Help Desk: 9:00-5:00 Monday-Thursday, 9:00-noon Friday, in the lobby of MPHY. SI (Supplemental Instructor): Thomas Leyden (thomasleyden@tamu.edu) 7:00-8:00pm, Sunday/Tuesday/Thursday, MPHY 333 Chapter

More information

Physics 2211 ABC Quiz #3 Solutions Spring 2017

Physics 2211 ABC Quiz #3 Solutions Spring 2017 Physics 2211 ABC Quiz #3 Solutions Spring 2017 I. (16 points) A block of mass m b is suspended vertically on a ideal cord that then passes through a frictionless hole and is attached to a sphere of mass

More information

Physics 2211 A & B Quiz #4 Solutions Fall 2016

Physics 2211 A & B Quiz #4 Solutions Fall 2016 Physics 22 A & B Quiz #4 Solutions Fall 206 I. (6 points) A pendulum bob of mass M is hanging at rest from an ideal string of length L. A bullet of mass m traveling horizontally at speed v 0 strikes it

More information

Reading Quiz. Chapter 5. Physics 111, Concordia College

Reading Quiz. Chapter 5. Physics 111, Concordia College Reading Quiz Chapter 5 1. The coefficient of static friction is A. smaller than the coefficient of kinetic friction. B. equal to the coefficient of kinetic friction. C. larger than the coefficient of kinetic

More information

PH 2213 : Chapter 05 Homework Solutions

PH 2213 : Chapter 05 Homework Solutions PH 2213 : Chapter 05 Homework Solutions Problem 5.4 : The coefficient of static friction between hard rubber and normal street pavement is about 0.90. On how steep a hill (maximum angle) can you leave

More information

Physics 221, January 24

Physics 221, January 24 Key Concepts: Newton s 1 st law Newton s 2 nd law Weight Newton s 3 rd law Physics 221, January 24 Please find a seat. Keep all walkways free for safety reasons and to comply with the fire code. Matter

More information

PHYSICS 149: Lecture 5

PHYSICS 149: Lecture 5 PHYSICS 149: Lecture 5 Chapter.5 Newton s Third Law.6 Gravitational Forces.7 Contact Forces: Normal Force and Friction 1 Newton s Third Law All forces come in pairs Third law forces involve TWO OBJECTS.

More information

Newton s Laws.

Newton s Laws. Newton s Laws http://mathsforeurope.digibel.be/images Forces and Equilibrium If the net force on a body is zero, it is in equilibrium. dynamic equilibrium: moving relative to us static equilibrium: appears

More information

Physics 8 Friday, November 4, 2011

Physics 8 Friday, November 4, 2011 Physics 8 Friday, November 4, 2011 Please turn in Homework 7. I will hand out solutions once everyone is here. The handout also includes HW8 and a page or two of updates to the equation sheet needed to

More information

B C = B 2 + C 2 2BC cosθ = (5.6)(4.8)cos79 = ) The components of vectors B and C are given as follows: B x. = 6.

B C = B 2 + C 2 2BC cosθ = (5.6)(4.8)cos79 = ) The components of vectors B and C are given as follows: B x. = 6. 1) The components of vectors B and C are given as follows: B x = 6.1 C x = 9.8 B y = 5.8 C y = +4.6 The angle between vectors B and C, in degrees, is closest to: A) 162 B) 111 C) 69 D) 18 E) 80 B C = (

More information

Dynamics Review Checklist

Dynamics Review Checklist Dynamics Review Checklist Newton s Laws 2.1.1 Explain Newton s 1 st Law (the Law of Inertia) and the relationship between mass and inertia. Which of the following has the greatest amount of inertia? (a)

More information

SEMESTER REVIEW FOR FINAL EXAM

SEMESTER REVIEW FOR FINAL EXAM SEMESTER REVIEW FOR FINAL EXAM ACCELERATION When is an object s acceleration not equal to zero? What is the equation for acceleration? ANGULAR SPEED AND MOMENTUM Does an object on the outside of a spinning

More information

Example. F and W. Normal. F = 60cos 60 N = 30N. Block accelerates to the right. θ 1 F 1 F 2

Example. F and W. Normal. F = 60cos 60 N = 30N. Block accelerates to the right. θ 1 F 1 F 2 Physic 3 Lecture 7 Newton s 3 d Law: When a body exerts a force on another, the second body exerts an equal oppositely directed force on the first body. Frictional forces: kinetic friction: fk = μk N static

More information

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

Chapter 4. Forces and Newton s Laws of Motion. continued Chapter 4 Forces and Newton s Laws of Motion continued Clicker Question 4.3 A mass at rest on a ramp. How does the friction between the mass and the table know how much force will EXACTLY balance the gravity

More information

Introduction to Newton s Laws Newton s First Law. Oct 21 8:32 AM

Introduction to Newton s Laws Newton s First Law. Oct 21 8:32 AM Introduction to Newton s Laws Newton s First Law. Isaac Newton Arguably the greatest scientific genius ever. Came up with 3 Laws of Motion to explain the observations and analyses of Galileo and Johannes

More information

b) What does each letter (or symbol) stand for in this equation? c) What are the corresponding SI units? (Write: symbol $ unit).

b) What does each letter (or symbol) stand for in this equation? c) What are the corresponding SI units? (Write: symbol $ unit). First Name: Last Name: 1. a) What is Newton s Second Law in formula form? b) What does each letter (or symbol) stand for in this equation? c) What are the corresponding SI units? (Write: symbol $ unit).

More information

Review: Advanced Applications of Newton's Laws

Review: Advanced Applications of Newton's Laws Review: Advanced Applications of Newton's Laws 1. The free-body diagram of a wagon being pulled along a horizontal surface is best represented by a. A d. D b. B e. E c. C 2. The free-body diagram of a

More information

Physics B Newton s Laws AP Review Packet

Physics B Newton s Laws AP Review Packet Force A force is a push or pull on an object. Forces cause an object to accelerate To speed up To slow down To change direction Unit: Newton (SI system) Newton s First Law The Law of Inertia. A body in

More information

Making Sense of the Universe (Chapter 4) Why does the Earth go around the Sun? Part, but not all, of Chapter 4

Making Sense of the Universe (Chapter 4) Why does the Earth go around the Sun? Part, but not all, of Chapter 4 Making Sense of the Universe (Chapter 4) Why does the Earth go around the Sun? Part, but not all, of Chapter 4 Based on part of Chapter 4 This material will be useful for understanding Chapters 8 and 11

More information

PHYS 185 Final Exam December 4, 2012

PHYS 185 Final Exam December 4, 2012 PHYS 185 Final Exam December 4, 2012 Name: Answer the questions in the spaces provided on the question sheets. If you run out of room for an answer, continue on the back of the page. Please make an effort

More information

Video Analysis of a Ball on a Rotating Merry-go-round

Video Analysis of a Ball on a Rotating Merry-go-round Video Analysis of a Ball on a Rotating Merry-go-round Apparatus Tracker software (free; download from http://www.cabrillo.edu/ dbrown/tracker/) video: coriolis-merry-go-round-ball.mov from http://physics.highpoint.edu/

More information

Topic: Force PHYSICS 231

Topic: Force PHYSICS 231 Topic: Force PHYSICS 231 Current Assignments Homework Set 2 due this Thursday, Jan 27, 11 pm Reading for next week: Chapters 10.1-6,10.10,8.3 2/1/11 Physics 231 Spring 2011 2 Key Concepts: Force Free body

More information

LECTURE 11 FRICTION AND DRAG

LECTURE 11 FRICTION AND DRAG LECTURE 11 FRICTION AND DRAG 5.5 Friction Static friction Kinetic friction 5.6 Drag Terminal speed Penguins travel on ice for miles by sliding on ice, made possible by small frictional force between their

More information

Solution of HW4. and m 2

Solution of HW4. and m 2 Solution of HW4 9. REASONING AND SOLUION he magnitude of the gravitational force between any two of the particles is given by Newton's law of universal gravitation: F = Gm 1 m / r where m 1 and m are the

More information

Chapter 5. The Laws of Motion

Chapter 5. The Laws of Motion Chapter 5 The Laws of Motion The Laws of Motion The description of an object in There was no consideration of what might influence that motion. Two main factors need to be addressed to answer questions

More information

PHYSICS - CLUTCH CH 04: INTRO TO FORCES (DYNAMICS)

PHYSICS - CLUTCH CH 04: INTRO TO FORCES (DYNAMICS) !! www.clutchprep.com FORCE, APPLIED FORCE, TENSION A force is either a push or a pull. Unit = ( ) - We ll represent all forces as a We ll refer to generic forces as forces. - Usually on an object by a

More information

Distance travelled time taken and if the particle is a distance s(t) along the x-axis, then its instantaneous speed is:

Distance travelled time taken and if the particle is a distance s(t) along the x-axis, then its instantaneous speed is: Chapter 1 Kinematics 1.1 Basic ideas r(t) is the position of a particle; r = r is the distance to the origin. If r = x i + y j + z k = (x, y, z), then r = r = x 2 + y 2 + z 2. v(t) is the velocity; v =

More information

PRACTICE TEST for Midterm Exam

PRACTICE TEST for Midterm Exam South Pasadena AP Physics PRACTICE TEST for Midterm Exam FORMULAS Name Period Date / / d = vt d = v o t + ½ at 2 d = v o + v 2 t v = v o + at v 2 = v 2 o + 2ad v = v x 2 + v y 2 = tan 1 v y v v x = v cos

More information

What was Aristotle s view of motion? How did Galileo disagree with Aristotle? Which answers agrees with Aristotle s view? Eliminate the others.

What was Aristotle s view of motion? How did Galileo disagree with Aristotle? Which answers agrees with Aristotle s view? Eliminate the others. Quest Chapter 04 # Problem Hint 1 A ball rolls across the top of a billiard table and slowly comes to a stop. How would Aristotle interpret this observation? How would Galileo interpret it? 1. Galileo

More information

A PHYSICS 201 Final Exam

A PHYSICS 201 Final Exam PHYSICS 201 Final Exam Fall 2014 Last Name: First Name: Section: UIN: You have 120 minutes to complete the exam. Formulae are provided. You may NOT use any other formula sheet. You may use a calculator

More information

A N D. c h a p t e r 1 2 M O T I O N F O R C E S

A N D. c h a p t e r 1 2 M O T I O N F O R C E S F O R C E S A N D c h a p t e r 1 2 M O T I O N What is a FORCE? A FORCE is a push or pull that acts on an object. A force can cause a resting object to move OR Accelerate a moving object by: changing

More information

Physics 2211 A & B Quiz #2 Solutions Fall P sin θ = µ k P cos θ + mg

Physics 2211 A & B Quiz #2 Solutions Fall P sin θ = µ k P cos θ + mg Physics 2211 A & B Quiz #2 Solutions Fall 2016 I. (16 points) A block of mass m is sliding up a vertical wall at constant non-zero velocity v 0, due to an applied force P pushing against it at an angle

More information

Go on to the next page.

Go on to the next page. Chapter 10: The Nature of Force Force a push or a pull Force is a vector (it has direction) just like velocity and acceleration Newton the SI unit for force = kg m/s 2 Net force the combination of all

More information

SPS8. STUDENTS WILL DETERMINE RELATIONSHIPS AMONG FORCE, MASS, AND MOTION.

SPS8. STUDENTS WILL DETERMINE RELATIONSHIPS AMONG FORCE, MASS, AND MOTION. MOTION & FORCES SPS8. STUDENTS WILL DETERMINE RELATIONSHIPS AMONG FORCE, MASS, AND MOTION. A. CALCULATE VELOCITY AND ACCELERATION. B. APPLY NEWTON S THREE LAWS TO EVERYDAY SITUATIONS BY EXPLAINING THE

More information

FORCES. Chapter 2: Section 3, Chapter 3: Sections 1-3

FORCES. Chapter 2: Section 3, Chapter 3: Sections 1-3 FORCES Chapter 2: Section 3, Chapter 3: Sections 1-3 Vocab: 2.3-3.3 DEFINE THESE Force Net force Balanced force Inertia Newton s second law of motion Friction Law of gravitation Weight Newton s third law

More information

PHYSICS 231 INTRODUCTORY PHYSICS I

PHYSICS 231 INTRODUCTORY PHYSICS I PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 6 Last Lecture: Gravity Normal forces Strings, ropes and Pulleys Today: Friction Work and Kinetic Energy Potential Energy Conservation of Energy Frictional Forces

More information

AP PHYSICS 1. Energy 2016 EDITION

AP PHYSICS 1. Energy 2016 EDITION AP PHYSICS 1 Energy 2016 EDITION Copyright 2016 National Math + Initiative, Dallas, Texas. All rights reserved. Visit us online at www.nms.org. 1 Pre-Assessment Questions Consider a system which could

More information

Forces. Video Demos. Graphing HW: October 03, 2016

Forces. Video Demos. Graphing HW: October 03, 2016 Distance (m or km) : Create a story using the graph. Describe what will be happening at each point during the day (A-D). Example: Trump has a busy day. He is currently at Trump Tower in NY. A- Trump jumps

More information

UNIT XX: DYNAMICS AND NEWTON S LAWS. DYNAMICS is the branch of mechanics concerned with the forces that cause motions of bodies

UNIT XX: DYNAMICS AND NEWTON S LAWS. DYNAMICS is the branch of mechanics concerned with the forces that cause motions of bodies I. Definition of FORCE UNIT XX: DYNAMICS AND NEWTON S LAWS DYNAMICS is the branch of mechanics concerned with the forces that cause motions of bodies FORCE is a quantitative interaction between two (or

More information

IB Physics Fall Refresh Work

IB Physics Fall Refresh Work IB Physics Fall Refresh Work Odell says, "Physics is phun!" Fall 2014 38 min 25 marks Complete this packet and turn in to Mr. Odell the first day after Thanksgiving Break 1 1. Linear motion At a sports

More information

Chapter 5. The Laws of Motion

Chapter 5. The Laws of Motion Chapter 5 The Laws of Motion The Laws of Motion The description of an object in motion included its position, velocity, and acceleration. There was no consideration of what might influence that motion.

More information

Figure 5.1a, b IDENTIFY: Apply to the car. EXECUTE: gives.. EVALUATE: The force required is less than the weight of the car by the factor.

Figure 5.1a, b IDENTIFY: Apply to the car. EXECUTE: gives.. EVALUATE: The force required is less than the weight of the car by the factor. 51 IDENTIFY: for each object Apply to each weight and to the pulley SET UP: Take upward The pulley has negligible mass Let be the tension in the rope and let be the tension in the chain EXECUTE: (a) The

More information

EQUATIONS OF MOTION: RECTANGULAR COORDINATES

EQUATIONS OF MOTION: RECTANGULAR COORDINATES EQUATIONS OF MOTION: RECTANGULAR COORDINATES Today s Objectives: Students will be able to: 1. Apply Newton s second law to determine forces and accelerations for particles in rectilinear motion. In-Class

More information