Chapter 4 Dynamics: Newton s Laws of Motion
|
|
- Alan Lenard Holland
- 6 years ago
- Views:
Transcription
1 Chapter 4 Dynamics: Newton s Laws of Motion
2 Force Newton s First Law of Motion Mass Newton s Second Law of Motion Newton s Third Law of Motion Weight the Force of Gravity; and the Normal Force Applications Involving Friction, Inclines
3 Assignment 5 Textbook (Giancoli, 6 th edition). Due on Oct. 28 th On page 101 of Giancoli, problem On page 102 of Giancoli,problem On page 102 of Giancoli, problem A block is pressed against a vertical wall by a force P, as the drawing shows. This force can either push the block upward at a constant velocity or allow it to slide downward at a constant velocity. The magnitude of the force is different in the two cases, while the directional angle is the same. Kinetic friction exists between the block and the wall, and the coefficient of kinetic friction is The weight of the block is 39.0 N, and the directional angle for the force P is θ = Determine the magnitude of P when the block slides (a) up the wall and (b) down the wall.
4 Remind: Midterm Date: October 19, 1pm 2:15pm. Location: EA There are four problems. One of them will be based on problems found in assignment 5. The midterm includes everything covered until today, including friction and inclines (chapters 1 to 4). - You ARE allowed to use a calculator. An equation sheet will be provided (link at ) - Solutions of the assignments can be found on the webpage listed above. You can also find a link to old midterms from this webpage. - I will be exceptionally available for discussions, questions, etc between 14:30 and 15:00h tomorrow, and between 12:30 and 15:00h on Monday. - Dr. Ouimet will offer a review session on October 19 th (Monday) between 4:00pm-6:00pm in CL-112. Next Wednesday s tutorial session has been cancelled - Remember, your marked assignments are available for you. Feel free to come anytime to my office (LB-212) if you have failed to pick it up in classroom.
5 Tension in a Flexible Cord Problem 4-38 (textbook Suppose that you are standing on a train accelerating (horizontally) at 0.20 g. What minimum coefficient of static friction must exist between your feet and the floor if you are not to slide?
6 Problem 4.38 (textbook): A free-body diagram for you as you stand on the train is shown. You do not accelerate vertically, and so FN = mg mg r F r fr F r N µ F The maximum static frictional force is, and that must be greater than or equal s N to the force needed to accelerate you. F ma µ F ma µ mg ma µ a g = 0.20g g = 0.20 fr s N s s The static coefficient of friction must be at least 0.20 for you not to slide.
7 Friction and Inclined Planes Remember: (4.5) (4.6)
8 Friction and Inclined Planes The problem with inclined plans are no different from the problems we have dealt with so far. However, remember: 1- The normal force is ALWAYS perpendicular to the plane where the object lies on. So, on an inclined plane it is not going to be in the vertical direction. (See next slide)
9 Friction and Inclined Planes Three forces can ALWAYS be identified acting on an object moving on an inclined plane: Gravity (vertical); friend 2 Friction (along the surface); Normal (perpendicular to the surface). So, it is convenient to define your coordinate system such that the x direction coincides with the inclined line, and y in the direction perpendicular to the plane. friend 1 you You can surely have other applied forces: for instance, you (or you and a group of friends) can push or pull this object.
10 Friction and Inclined Planes Problem 4-41 (textbook A 15.0-kg box is released on a 32º incline and accelerates down the incline at 0.30 m/s 2. Find the friction force impeding its motion. What is the coefficient of kinetic friction? = 0.30 m/s 2 32 o
11 Problem 4.41 (textbook): A free-body diagram for the box is shown. Write Newton s 2 nd law for each direction: F = mg sin θ F = ma x F = F mg cosθ = ma = 0 y N Notice that the sum in the y direction is 0, since there is no motion (and hence no acceleration) in the y direction. Solve for the force of friction. fr x y F r fr F r N θ mg r y θ x mg sin θ F = ma fr x ( ) ( )( ) F = mg ma = = fr 2 o 2 sinθ 15.0 kg 9.80 m s sin m s N 73 N x Now solve for the coefficient of kinetic friction. Note that the expression for the normal force comes from the y direction force equation above. F N fr F = µ F = µ mg cos θ µ = = fr k N k k 2 o mg cosθ 15.0 kg 9.80 m s cos 32 = 0.59 ( )( )( )
12 Tension in a Flexible Cord Problem 4-65 (textbook A bicyclist of mass 65 kg (including the bicycle) can coast down a 6.0º hill at a steady speed of 6.0 Km/h because of air resistance. How much force must be applied to climb the hill at the same speed and same air resistance?
13 Problem 4.65 (textbook): Consider a free-body diagram for the cyclist coasting downhill at a constant speed. Here we call F fr the friction due to air resistance (and not sliding or static friction). Since there is no acceleration, the net force in each direction must be zero. Write Newton s 2 nd law for the x direction. F = mg sinθ F = 0 F = mg sinθ x fr fr F r fr F r N y This establishes the size of the air friction force at 6.0 km/h, and so can be used in the next part. Now consider a free-body diagram for the cyclist climbing the hill. F p is the force pushing the cyclist uphill. Again, write Newton s 2 nd law for the x direction, with a net force of 0. F = F + m g sin θ F = 0 x fr F = F + mg sin θ = 2mg sin θ P fr ( )( )( ) = = 2 o kg 9.8 m s sin N P y F r P x θ θ θ mg r θ mg r F r N F r fr x
14 Chapter 5 Circular Motion; Gravitation
15 Kinematics of Uniform Circular Motion Dynamics of Uniform Circular Motion Highway Curves, Banked and Unbanked Non-uniform Circular Motion Centrifugation Will be covered after chapter 7 (5.6) Newton s Law of Universal Gravitation (5.7) Gravity Near the Earth s Surface
16 Newton s Law of Universal Gravitation If the force of gravity is being exerted on objects on Earth, what is the origin of that force? Newton s realization was that the force must come from the Earth. He further realized that this force must be what keeps the Moon in its orbit.
17 Newton s Law of Universal Gravitation More than that: the Earth exerts a downward force on you, and you exert an upward force on the Earth. When there is such a difference in masses, the reaction force is undetectable, but for bodies more equal in mass it can be significant. Therefore, the gravitational force must be proportional to both masses.
18 Newton s Law of Universal Gravitation By observing planetary orbits, Newton also concluded that the gravitational force must decrease as the inverse of the square of the distance between the masses. Summary: The gravitational force is directly proportional to the masses and inversely proportional to the square of their distance. Or, as stated in Newton s law of universal gravitation: Every particle in the universe attracts every other particle with a force that is proportional to the products of their masses and inversely proportional to the square of the distance between them. This forces acts along the line joining the two particles.
19 Newton s Law of Universal Gravitation The magnitude of this force is given by: (4.7) Where:
20 Newton s Law of Universal Gravitation We know the relation between force and acceleration:. But what is a in? If m 2 is the object exerting a force on m 1, then the gravitational acceleration felt by object 1 can be identified as: (4.8) The opposite is also true: object 2 will feel an acceleration due to the gravitational force applied by object 1. You can then write for the force acting on m 1 force acting on m 2. and for the
21 Gravity Near the Earth s Surface An object of mass m ON the surface of the Earth will feel a force given by: Where, m E = mass of the Earth ; r E = 6.38 x 10 6 m = radius of the Earth. g has been measured and it is known to be 9.80 m/s 2. (4.9) In fact, the value of g can be considered constant at any position near the Earth s surface (this is what we have been assuming without much discussion so far). Note that knowing G, r E and g, we can calculate the mass of the Earth. From eq. 4.9: More accurate calculations lead to m E = x Kg
22 Newton s Law of Universal Gravitation Problem 5-31 (textbook): A hypothetical planet has a radius 1.5 times that of Earth, but has the same mass. What is the acceleration due to gravity near its surface? Solution: The acceleration due to gravity at any location on or above the surface of a planet is given by g = G M r planet Planet 2 where r is the distance from the center of the planet to the location in question. 2 M M 1 M m s g = G = G = G = g = = planet r Planet Earth Earth Earth 2 ( 1.5REarth ) 1.5 R Earth 4.4 m s 2
23 Newton s Law of Universal Gravitation Problem 5-34 (textbook): Calculate the effective value of g, the acceleration of gravity, at (a) 3200 m, and (b) 3200 km, above the Earth s surface. Solution: The acceleration due to gravity at any location at or above the surface of a planet is 2 given by where r is the distance from the center of the planet to the location in question. For 2 4 this problem, M = M = kg P lanet E arth (a) (b) g = G M r plan et P lanet 6 r = R Earth m = m m Earth 2 24 ( kg ) ( ) 6 ( m m ) M g = G = N m kg = 9.77 m s r r = R Earth km = m m = m Earth 2 ( ) ( kg ) 6 2 ( m ) M g = G = N m kg = 4.34 m s r
Chapter 5 Circular Motion; Gravitation
Chapter 5 Circular Motion; Gravitation Kinematics of Uniform Circular Motion Dynamics of Uniform Circular Motion Highway Curves, Banked and Unbanked Non-uniform Circular Motion Centrifugation Will be covered
More informationChapter 5 Gravitation Chapter 6 Work and Energy
Chapter 5 Gravitation Chapter 6 Work and Energy Chapter 5 (5.6) Newton s Law of Universal Gravitation (5.7) Gravity Near the Earth s Surface Chapter 6 (today) Work Done by a Constant Force Kinetic Energy,
More informationReview 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 informationForce 10/01/2010. (Weight) MIDTERM on 10/06/10 7:15 to 9:15 pm Bentley 236. (Tension)
Force 10/01/2010 = = Friction Force (Weight) (Tension), coefficient of static and kinetic friction MIDTERM on 10/06/10 7:15 to 9:15 pm Bentley 236 2008 midterm posted for practice. Help sessions Mo, Tu
More informationPHYS-2010: General Physics I Course Lecture Notes Section V
PHYS-2010: General Physics I Course Lecture Notes Section V Dr. Donald G. Luttermoser East Tennessee State University Edition 2.5 Abstract These class notes are designed for use of the instructor and students
More informationChapter 4: Newton s Second Law F = m a. F = m a (4.2)
Lecture 7: Newton s Laws and Their Applications 1 Chapter 4: Newton s Second Law F = m a First Law: The Law of Inertia An object at rest will remain at rest unless, until acted upon by an external force.
More informationForces 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 informationChapter 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 informationPOGIL: 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 informationPhysics 101 Lecture 5 Newton`s Laws
Physics 101 Lecture 5 Newton`s Laws Dr. Ali ÖVGÜN EMU Physics Department The Laws of Motion q Newton s first law q Force q Mass q Newton s second law q Newton s third law qfrictional forces q Examples
More informationCHAPTER 4 NEWTON S LAWS OF MOTION
62 CHAPTER 4 NEWTON S LAWS O MOTION CHAPTER 4 NEWTON S LAWS O MOTION 63 Up to now we have described the motion of particles using quantities like displacement, velocity and acceleration. These quantities
More informationChapter 5. The Laws of Motion
Chapter 5 The Laws of Motion Sir Isaac Newton 1642 1727 Formulated basic laws of mechanics Discovered Law of Universal Gravitation Invented form of calculus Many observations dealing with light and optics
More informationChapter 9- Static Equilibrium
Chapter 9- Static Equilibrium Changes in Office-hours The following changes will take place until the end of the semester Office-hours: - Monday, 12:00-13:00h - Wednesday, 14:00-15:00h - Friday, 13:00-14:00h
More informationFriction is always opposite to the direction of motion.
6. Forces and Motion-II Friction: The resistance between two surfaces when attempting to slide one object across the other. Friction is due to interactions at molecular level where rough edges bond together:
More informationChapter 4. Forces and Newton s Laws of Motion. continued
Chapter 4 Forces and Newton s Laws of Motion continued 4.9 Static and Kinetic Frictional Forces When an object is in contact with a surface forces can act on the objects. The component of this force acting
More informationThe Laws of Motion. Newton s first law Force Mass Newton s second law Gravitational Force Newton s third law Examples
The Laws of Motion Newton s first law Force Mass Newton s second law Gravitational Force Newton s third law Examples Gravitational Force Gravitational force is a vector Expressed by Newton s Law of Universal
More informationChapter 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 informationPhysics 201, Review 2
Physics 201, Review 2 Important Notes: v This review does not replace your own preparation efforts v The review is not meant to be complete. v Exercises used in this review do not form a test problem pool.
More informationDynamics: Forces and Newton s Laws of Motion
Lecture 7 Chapter 5 Dynamics: Forces and Newton s Laws of Motion Course website: http://faculty.uml.edu/andriy_danylov/teaching/physicsi Today we are going to discuss: Chapter 5: Force, Mass: Section 5.1
More informationDynamics: Forces and Newton s Laws of Motion
Lecture 7 Chapter 5 Physics I Dynamics: Forces and Newton s Laws of Motion Course website: http://faculty.uml.edu/andriy_danylov/teaching/physicsi Today we are going to discuss: Chapter 5: Force, Mass:
More informationWhat is a Force? Free-Body diagrams. Contact vs. At-a-Distance 11/28/2016. Forces and Newton s Laws of Motion
Forces and Newton s Laws of Motion What is a Force? In generic terms: a force is a push or a pull exerted on an object that could cause one of the following to occur: A linear acceleration of the object
More informationCircular Motion. - The velocity is tangent to the path and perpendicular to the radius of the circle
Circular Motion Level : Physics Teacher : Kim 1. Uniform Circular Motion - According to Newton s 1 st law, an object in motion will move in a straight line at a constant speed unless an unbalance force
More information1. 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
1. A sphere with a radius of 1.7 cm has a volume of: A) 2.1 10 5 m 3 B) 9.1 10 4 m 3 C) 3.6 10 3 m 3 D) 0.11 m 3 E) 21 m 3 2. A 25-N crate slides down a frictionless incline that is 25 above the horizontal.
More informationExamples Newton's Laws and Friction
Examples Newton's Laws and Friction 1. A 10.0 kg box is sitting on a table. (A) If a 49 N force is required to overcome friction and start the block moving, calculate the coefficient of static friction.
More informationChapter 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 informationChapter 8: Newton s Laws Applied to Circular Motion
Chapter 8: Newton s Laws Applied to Circular Motion Centrifugal Force is Fictitious? F actual = Centripetal Force F fictitious = Centrifugal Force Center FLEEing Centrifugal Force is Fictitious? Center
More informationPhysics 201, Review 2
Physics 01, Review Important Notes: v This review does not replace your own preparation efforts v The review is not meant to be complete. v Exercises used in this review do not form a test problem pool.
More informationdt 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= 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 informationAnnouncements. Principle of Work and Energy - Sections Engr222 Spring 2004 Chapter Test Wednesday
Announcements Test Wednesday Closed book 3 page sheet sheet (on web) Calculator Chap 12.6-10, 13.1-6 Principle of Work and Energy - Sections 14.1-3 Today s Objectives: Students will be able to: a) Calculate
More informationWelcome back to Physics 211
Welcome back to Physics 211 Today s agenda: Weight Friction Tension 07-1 1 Current assignments Thursday prelecture assignment. HW#7 due this Friday at 5 pm. 07-1 2 Summary To solve problems in mechanics,
More informationInclined Planes Worksheet Answers
Physics 12 Name: Inclined Planes Worksheet Answers 1. An 18.0 kg box is released on a 33.0 o incline and accelerates at 0.300 m/s 2. What is the coefficient of friction? m 18.0kg 33.0? a y 0 a 0.300m /
More informationb) 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 informationDynamics; 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 informationAnnouncements. There will still be a WebAssign due this Friday, the last before the midterm.
Announcements THERE WILL BE NO CLASS THIS FRIDAY, MARCH 5 (We are 1 full lecture ahead of the syllabus, so we will still have review/problem solving on March 7 and 9). There will still be a WebAssign due
More informationChapter 5 Newton s Laws of Motion. Copyright 2010 Pearson Education, Inc.
Chapter 5 Newton s Laws of Motion Force and Mass Units of Chapter 5 Newton s First Law of Motion Newton s Second Law of Motion Newton s Third Law of Motion The Vector Nature of Forces: Forces in Two Dimensions
More informationFigure 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 informationP - 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 informationLecture 7. Forces. Important note: First Exam is next Tuesday, Feb. 6, 8:15-9:45 pm (see link on Canvas for locations)
Lecture 7 Forces Important note: First Exam is next Tuesday, Feb. 6, 8:15-9:45 pm (see link on Canvas for locations) Today s Topics: Forces The gravitational force The normal force Frictional Forces Next
More informationPhysics 1100: Uniform Circular Motion & Gravity
Questions: 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 Physics 1100: Uniform Circular Motion & Gravity 1. In the diagram below, an object travels over a hill, down a valley, and around a loop the loop at constant
More informationPractice 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 informationNewton s 3 rd Law. The Nature of Force. Matthew W. Milligan
Newton s 3 rd Law The Nature of Force Forces Dynamics I. Laws of Motion: 1 & 2 - inertia, force, mass - weight II. Law 3 - interaction & nature of force - types of force: normal, friction - air resistance,
More informationWiley Plus. Final Assignment (5) Is Due Today: Before 11 pm!
Wiley Plus Final Assignment (5) Is Due Today: Before 11 pm! Final Exam Review December 9, 009 3 What about vector subtraction? Suppose you are given the vector relation A B C RULE: The resultant vector
More informationDynamic 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 informationMarch 10, P12 Inclined Planes.notebook. Physics 12. Inclined Planes. Push it Up Song
Physics 12 Inclined Planes Push it Up Song 1 Bell Work A box is pushed up a ramp at constant velocity. Draw a neatly labeled FBD showing all of the forces acting on the box. direction of motion θ F p F
More informationYear 11 Physics Tutorial 84C2 Newton s Laws of Motion
Year 11 Physics Tutorial 84C2 Newton s Laws of Motion Module Topic 8.4 Moving About 8.4.C Forces Name Date Set 1 Calculating net force 1 A trolley was moved to the right by a force applied to a cord attached
More informationEQUATIONS OF MOTION: NORMAL AND TANGENTIAL COORDINATES (Section 13.5)
EQUATIONS OF MOTION: NORMAL AND TANGENTIAL COORDINATES (Section 13.5) Today s Objectives: Students will be able to apply the equation of motion using normal and tangential coordinates. APPLICATIONS Race
More informationPhysics 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 informationThurs Sept.23. Thurs Sept. Phys .23. Why is it moving upwards after I let go? Don t forget to read over the lab write-up and be ready for the quiz.
ics Announcements day, ember 23, 2004 Ch 5: Newton s 1st and 2nd Laws Example Problems Ch 6: Intro to Friction static kinetic Help this week: Wednesday, 8-9 pm in NSC 118/119 Sunday, 6:30-8 pm in CCLIR
More informationLecture PowerPoints. Chapter 5 Physics for Scientists & Engineers, with Modern Physics, 4 th edition. Giancoli
Lecture PowerPoints Chapter 5 Physics for Scientists & Engineers, with Modern Physics, 4 th edition 2009 Pearson Education, Inc. This work is protected by United States copyright laws and is provided solely
More informationPhysics 2211 M Quiz #2 Solutions Summer 2017
Physics 2211 M Quiz #2 Solutions Summer 2017 I. (16 points) A block with mass m = 10.0 kg is on a plane inclined θ = 30.0 to the horizontal, as shown. A balloon is attached to the block to exert a constant
More informationChapter 4. Dynamics: Newton s Laws of Motion. That is, describing why objects move
Chapter 4 Dynamics: Newton s Laws of Motion That is, describing why objects move orces Newton s 1 st Law Newton s 2 nd Law Newton s 3 rd Law Examples of orces: Weight, Normal orce, Tension, riction ree-body
More informationConceptual Questions. SPH4U1 - Dynamics Problems Set 3
3 Conceptual Questions 1. A 100-kg sofa needs to be moved across a level floor. The coefficient of static friction between the sofa and the floor is 0.40. Two physics students decide to apply a force F
More informationEQUATIONS 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 informationTopic: 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 informationWiley Plus Reminder! Assignment 1
Wiley Plus Reminder! Assignment 1 6 problems from chapters and 3 Kinematics Due Monday October 5 Before 11 pm! Chapter 4: Forces and Newton s Laws Force, mass and Newton s three laws of motion Newton s
More informationChapter 4. Forces and Newton s Laws of Motion. F=ma; gravity
Chapter 4 Forces and Newton s Laws of Motion F=ma; gravity 0) Background Galileo inertia (horizontal motion) constant acceleration (vertical motion) Descartes & Huygens Conservation of momentum: mass x
More informationPS113 Chapter 4 Forces and Newton s laws of motion
PS113 Chapter 4 Forces and Newton s laws of motion 1 The concepts of force and mass A force is described as the push or pull between two objects There are two kinds of forces 1. Contact forces where two
More informationNewton s First Law and IRFs
Goals: Physics 207, Lecture 6, Sept. 22 Recognize different types of forces and know how they act on an object in a particle representation Identify forces and draw a Free Body Diagram Solve 1D and 2D
More informationPhysics 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 informationCEE 271: Applied Mechanics II, Dynamics Lecture 9: Ch.13, Sec.4-5
1 / 40 CEE 271: Applied Mechanics II, Dynamics Lecture 9: Ch.13, Sec.4-5 Prof. Albert S. Kim Civil and Environmental Engineering, University of Hawaii at Manoa 2 / 40 EQUATIONS OF MOTION:RECTANGULAR COORDINATES
More information4.1 Forces. Chapter 4 The Laws of Motion
4.1 Forces Chapter 4 he Laws of Motion 4.2 Newton s First Law it s not the nature of an object to stop, once set in motion, but rather to continue in its original state of motion. An object moves with
More informationMechanics II. Which of the following relations among the forces W, k, N, and F must be true?
Mechanics II 1. By applying a force F on a block, a person pulls a block along a rough surface at constant velocity v (see Figure below; directions, but not necessarily magnitudes, are indicated). Which
More informationThe 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
The Laws of 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 Models using Newton s Second Law Forces
More informationWS-CH-4 Motion and Force Show all your work and equations used. Isaac Newton ( )
AP PHYSICS 1 WS-CH-4 Motion and Force Show all your work and equations used. Isaac Newton (1643-1727) Isaac Newton was the greatest English mathematician of his generation. He laid the foundation for differential
More informationPhysics 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 informationMULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question.
Exam Name MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. 1) You are standing in a moving bus, facing forward, and you suddenly fall forward as the
More informationUnit 1: Equilibrium and Center of Mass
Unit 1: Equilibrium and Center of Mass FORCES What is a force? Forces are a result of the interaction between two objects. They push things, pull things, keep things together, pull things apart. It s really
More informationNewton s 3 rd Law. Book page 48-49
Newton s 3 rd Law Book page 48-49 14/9/2016 cgrahamphysics.com 2016 Newton s 2 nd Law problem Newton s second law does not always work: - does not work when applied to atoms and molecules - does not work
More informationNewton s Laws. A force is simply a push or a pull. Forces are vectors; they have both size and direction.
Newton s Laws Newton s first law: An object will stay at rest or in a state of uniform motion with constant velocity, in a straight line, unless acted upon by an external force. In other words, the bodies
More informationPhysics 8 Wednesday, October 19, Troublesome questions for HW4 (5 or more people got 0 or 1 points on them): 1, 14, 15, 16, 17, 18, 19. Yikes!
Physics 8 Wednesday, October 19, 2011 Troublesome questions for HW4 (5 or more people got 0 or 1 points on them): 1, 14, 15, 16, 17, 18, 19. Yikes! Troublesome HW4 questions 1. Two objects of inertias
More informationSolution 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 informationChapter 4 Force and Motion
Chapter 4 Force and Motion Units of Chapter 4 The Concepts of Force and Net Force Inertia and Newton s First Law of Motion Newton s Second Law of Motion Newton s Third Law of Motion More on Newton s Laws:
More informationNewton 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 informationPhysics 111 Lecture 4 Newton`s Laws
Physics 111 Lecture 4 Newton`s Laws Dr. Ali ÖVGÜN EMU Physics Department www.aovgun.com he Laws of Motion q Newton s first law q Force q Mass q Newton s second law q Newton s third law q Examples Isaac
More informationChapter 4. Dynamics: Newton s Laws of Motion
Chapter 4 Dynamics: Newton s Laws of Motion Types of Forces: An Overview In nature there are two general types of forces, fundamental and nonfundamental. Fundamental Forces -- three have been identified,
More informationChapter 4 Dynamics: Newton s Laws of Motion
Chapter 4 Dynamics: Newton s Laws of Motion Units of Chapter 4 Force Newton s First Law of Motion Mass Newton s Second Law of Motion Newton s Third Law of Motion Weight the Force of Gravity; and the Normal
More information24/06/13 Forces ( F.Robilliard) 1
R Fr F W 24/06/13 Forces ( F.Robilliard) 1 Mass: So far, in our studies of mechanics, we have considered the motion of idealised particles moving geometrically through space. Why a particular particle
More informationPH211 Chapter 4 Solutions
PH211 Chapter 4 Solutions 4.3.IDENTIFY: We know the resultant of two vectors of equal magnitude and want to find their magnitudes. They make the same angle with the vertical. Figure 4.3 SET UP: Take to
More informationWeek 4 Homework/Recitation: 9/21/2017 Chapter4: Problems 3, 5, 11, 16, 24, 38, 52, 77, 78, 98. is shown in the drawing. F 2
Week 4 Homework/Recitation: 9/1/017 Chapter4: Problems 3, 5, 11, 16, 4, 38, 5, 77, 78, 98. 3. Two horizontal forces, F 1 and F, are acting on a box, but only F 1 is shown in the drawing. F can point either
More informationForce a push or a pull exerted on some object the cause of an acceleration, or the change in an objects velocity
Chapter 4 Physics Notes Changes in Motion Force a push or a pull exerted on some object the cause of an acceleration, or the change in an objects velocity Forces cause changes in velocity Causes a stationary
More informationCircular Motion. A car is traveling around a curve at a steady 45 mph. Is the car accelerating? A. Yes B. No
Circular Motion A car is traveling around a curve at a steady 45 mph. Is the car accelerating? A. Yes B. No Circular Motion A car is traveling around a curve at a steady 45 mph. Which vector shows the
More informationPHYS 100 Midterm Exam Review Session
PHYS 100 Midterm Exam Review Session y x F net on A = m a A A v = v + a t x 0x x x = x + v + a t 1 0 0x ( ) ( ) v = v + a x x x 0x x 0 x Physics 100 Midterm Review, Slide 1 Midterm Exam TODAY (Mar 9):
More informationIntroduction 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 informationLast-night s Midterm Test. Last-night s Midterm Test. PHY131H1F - Class 10 Today, Chapter 6: Equilibrium Mass, Weight, Gravity
PHY131H1F - Class 10 Today, Chapter 6: Equilibrium Mass, Weight, Gravity Clicker Question 1 Which of the following objects described below is in dynamic equilibrium? A. A 100 kg barbell is held at rest
More informationPHYSICS 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(35+70) 35 g (m 1+m 2)a=m1g a = 35 a= =3.27 g 105
Coordinator: Dr. W. L-Basheer Monday, March 16, 2015 Page: 1 Q1. 70 N block and a 35 N block are connected by a massless inextendable string which is wrapped over a frictionless pulley as shown in Figure
More informationChapter 5 Force and Motion
Force F Chapter 5 Force and Motion is the interaction between objects is a vector causes acceleration Net force: vector sum of all the forces on an object. v v N v v v v v Ftotal Fnet = Fi = F1 + F2 +
More information1N the force that a 100g bar of chocolate exerts on your hand.
Forces: - - > cause change in motions Newton's first law = law of inertia In absence of a net external force acting upon it, a body will either remain at rest or continue in its rectilinear uniform motion.
More informationPhys101 Lecture 5 Dynamics: Newton s Laws of Motion
Phys101 Lecture 5 Dynamics: Newton s Laws of Motion Key points: Newton s second law is a vector equation Action and reaction are acting on different objects Free-Body Diagrams Ref: 4-1,2,3,4,5,6,7. Page
More informationCourse Name : Physics I Course # PHY 107. Lecture-5 : Newton s laws - Part Two
Course Name : Physics I Course # PHY 107 Lecture-5 : Newton s laws - Part Two Abu Mohammad Khan Department of Mathematics and Physics North South University https://abukhan.weebly.com Copyright: It is
More informationYou know the drill: Turn in hw Pick up graded hw Name tags up Grab white boards and markers for your group
You know the drill: Turn in hw Pick up graded hw Name tags up Grab white boards and markers for your group Missing hw from: Hamilton, Herbig, I. Singh, Midterm #1 on Tuesday, September 24th Covers: Chapter
More informationChapter 4 Dynamics: Newton s Laws of Motion
Chapter 4 Dynamics: Newton s Laws of Motion Force Newton s First Law of Motion Mass Newton s Second Law of Motion Newton s Third Law of Motion Weight the Force of Gravity; and the Normal Force Applications
More informationMULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. Diagram 1 A) B - A. B) A - B. C) A + B. D) A B.
Exam Name MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. 1) In the diagram shown, the unknown vector is 1) Diagram 1 A) B - A. B) A - B. C) A + B.
More informationQuestion 01. A. Incorrect! This is not Newton s second law.
College Physics - Problem Drill 06: Newton s Laws of Motion Question No. 1 of 10 1. Which of the options best describes the statement: Every object continues in a state of rest or uniform motion in a straight
More informationCircular Motion and Gravitation Notes 1 Centripetal Acceleration and Force
Circular Motion and Gravitation Notes 1 Centripetal Acceleration and Force This unit we will investigate the special case of kinematics and dynamics of objects in uniform circular motion. First let s consider
More informationPhys101 First Major-111 Zero Version Monday, October 17, 2011 Page: 1
Monday, October 17, 011 Page: 1 Q1. 1 b The speed-time relation of a moving particle is given by: v = at +, where v is the speed, t t + c is the time and a, b, c are constants. The dimensional formulae
More informationCircular Motion (Chapter 5)
Circular Motion (Chapter 5) So far we have focused on linear motion or motion under gravity (free-fall). Question: What happens when a ball is twirled around on a string at constant speed? Ans: Its velocity
More information12/1/2014. Chapter 5 Circular Motion; Gravitation. Contents of Chapter 5. Contents of Chapter Kinematics of Uniform Circular Motion
Lecture PowerPoints Chapter 5 Physics: Principles with Applications, 7 th edition Giancoli Chapter 5 Circular Motion; Gravitation This work is protected by United States copyright laws and is provided
More informationPhysics 111: Mechanics Lecture 5
Physics 111: Mechanics Lecture 5 Bin Chen NJIT Physics Department Forces of Friction: f q When an object is in motion on a surface or through a viscous medium, there will be a resistance to the motion.
More information