Linear Momentum. Lecture 15. Chapter 9. Physics I Department of Physics and Applied Physics
|
|
- Gabriel Taylor
- 5 years ago
- Views:
Transcription
1 Lecture 15 Chapter 9 Physics I Linear Momentum Course website: Lecture Capture:
2 Outline Chapter 9 Momentum Conservation of momentum Impulse Collisions (Elastic & Inelastic)
3 Exam II Info Exam II Mon Nov 4, 9:00-9:50am, OH 150. Exam II covers Chapters 5-8 Same format as Exam I Prior Examples of Exam II posted Ch. 5: Using Newton s Laws, Friction, Uniform Circular motion Ch. 6: Universal Law of Gravitation, Kepler s Laws Ch. 7: Work & Energy Ch. 8: Conservation of Energy Exam Review Session Thursday 6-8pm, Ball 210
4 Linear Momentum m Linear momentum is defined as the product of an object s mass and velocity: p v mv Momentum is a VECTOR! Units of momentum: kg m s The greater the linear momentum of a body, the greater its tendency to continue in motion. n iron shot (m larger) is harder to stop than a baseball (m small) of the same velocity.
5 Force and Momentum (Newton s 2 nd law) Let s rewrite Newton s 2 nd law in terms of momentum: F ma m d v d dt (m v) dt F dp dt d p dt The rate of change of momentum is equal to the net force So, a force is required to change momentum of an object.
6 How to find an average force? This can be used to get average force from momentum change: p m i v i F t net p f mv f F So, let s rewrite N. 2 nd law for an average force: dp dt F average p t p f p i t Let s look at an example:
7 Example: finding an average force The speed of a fastball is about 40 m/s, and the speed of the ball coming off of player s bat for a home run is about 54 m/s. The ball (0.145kg) is in contact with the bat for 1ms. What is the average Force exerted by the player? x F average p f t p i m( v f ( v t i )) Pay attention to directions!!!!!!!! ( 0.145kg)[54 F average s F average 136, 300N 40] m / s in the direction of v f or x
8 ConcepTest 1 Two Boxes/Momentum Two boxes, one heavier than the other, are initially at rest on a horizontal frictionless surface. The same constant force F acts on each one for exactly 1 second. Which box has more momentum after the force acts? ) the heavier one B) the lighter one C) both the same F We know: p f av p t p f pi t In this case F and t are the same for both boxes! Both boxes will have the same final momentum. F av t p i 0 F light F heavy
9 ConcepTest 2 Two Boxes/velocity In the previous question, which box has the larger velocity after the force acts? ) the heavier one B) the lighter one C) both the same Mv h p f mv l Since M m, then v l v h
10 From Newton s 2 nd law: Conservation of Momentum dp F dt dp If Fexternal 0, then 0 thus p dt If no net external force acts on a system, its momentum is conserved. m v m v B B P initial m v m BvB P initial P final m, const v Pfinal m v ' m v m B vb m v ' m m B vb ' B v B m B vb '
11 Why is Momentum conserved? F N1 F N 2 m g m g 1 2 mg s are canceled by normal forces, so net external force is zero, and the momentum is conserved m g 1 F N 2 m g 2 The net external force is m 1 g, and the momentum is NOT conserved Isolated system is a system on which no external forces act. There are only internal forces acting between objects. this system (two balls) is isolated this system (two balls) is NOT isolated The total momentum of an isolated system of objects is conserved
12 Internal forces of an isolated system Internal forces of an isolated system. acts on B: B acts on : F F B B F B F B Forces equal and opposite (Newton s 3rd Law). F B F B During collision Thus, they all cancel each other. That s why they cannot ruin conservation of momentum. (It is not a proof)
13 Impulse During a collision, objects are deformed because of the large forces involved. How to relate those forces with a change in momentum? From Newton s 2 nd law: Integrate it: Before collision p i J F d p dt t f Fdt p dp f t i p f Force exerted on one of the balls fter collision p i Define Impulse as: J Fdt p f p i p t t f i Fdt dp J So, Impulse= area under F-vs-t curve p Impulse= change in momentum
14 Impulse/verage force The exact variation of F with time is very often not known. So, it is easier to find an average force. J the same J J F avg t t f Fdt t i p Having a certain p, a cat by bending its lags tries to increase t (impact time), so that an impact force would be reduced. F avg t p (intuitive knowledge of Physics ) How to avoid broken legs
15 Example: Tennis ball/impulse The force exerted by a tennis racket on the ball (mass 56 g) during a serve ( v i 0 )can be approximated by the F vs time plot below. What is the impulse on the ball? t f What is the speed of the serve? Force (kn) 2 0 Time (ms) 10 Fdt J p f p 0 i t i rea under force-time curve is an impulse: 2kN 2ms J rea 2( ) 4N s 2 J J p f mv f v f m 4 N s v f 71m/s kg
16 Different types of collisions Momentum is conserved in any two-body collision (since there is no net external force) Is mechanical energy conserved in these collisions? Metal balls get deformed and restored Mech. energy is conserved Elastic collision Cars get deformed and not restored. Some Mech. Energy is spent on deformation. Mech. energy is NOT conserved Inelastic collision
17 1-D Elastic Collisions
18 m v Elastic Collision Math (1D) m v B B m v m B v B Conservation of momentum Conservation of mech. energy m v m B v B m v m B v 1 B 2 m v 2 1 m 2 Bv 2 B 1 m v m 2 2 B m v m v m B v B m B v B m v 2 m v 2 m B v 2 2 B m B v B m (v v ) m B ( v B v B ) Relative velocities switch signs in the collision v v B m (v 2 v 2 ) m B ( v 2 B v 2 B ) m (v v )(v v ) m B ( v B v B )( v B v B ) ( v v ) B v v v B v B v B
19 Elastic Collision Math (1D) 1 st m v m B v B m v m B v B 1 m 2 v 2 1 m 2 Bv 2 B 1 m v m 2 B v 2 B Conservation of momentum Conservation of mechanical energy 2 nd m v m B v B m v m B v v ( v v ) B B v B Conservation of momentum Conservation of mechanical energy So, instead of the 1 st set of crazy equations, we can use the 2 nd one which is easier (both are linear)
20 Example: Ballistic Pendulum device used to measure the speed of a bullet. m v o M M+m v 1 h
21 Example: Ballistic Pendulum (cont.) For Bullet mass 10 g Block mass is 3 kg Block swings up to a height of 5 cm the speed of a bullet v o 298 m s
22 Different Ballistic Pendulum device used to measure the speed of a bullet. Bullet mass 30 g Block mass is 5 kg Spring compresses by 12 cm Spring constant k = 300 N/m Bullet velocity before collision? mv 0 (M m)v 1 v 0 M m m v 1 m 1 2 (M m)v kx2 v 1 x M k M m v o m s v m s
23 Thank you See you on Monday
Lecture 17. Conservation of Linear Momentum
Lecture 17 Chapter 11 Physics I Conservation of Linear Momentum Course website: http://faculty.uml.edu/ndriy_danylov/teaching/physicsi Department of Physics and pplied Physics IN THIS CHPTER, you will
More informationLecture 16. Conservation of Linear Momentum
Lecture 16 Chapter 11 Conservation of Linear Momentum nother conservation? I like conservations! Course website: http://faculty.uml.edu/ndriy_danylov/teaching/physicsi Department of Physics and pplied
More informationCollisions. Lecture 18. Chapter 11. Physics I. Department of Physics and Applied Physics
Lecture 18 Chater 11 Physics I Collisions Course website: htt://faculty.uml.edu/ndriy_danylov/teaching/physicsi Deartment of Physics and lied Physics IN THIS CHPTER, you will discuss collisions of two
More informationPhys101 Lectures 14, 15, 16 Momentum and Collisions
Phys101 Lectures 14, 15, 16 Momentum and Collisions Key points: Momentum and impulse Condition for conservation of momentum and why How to solve collision problems Centre of mass Ref: 9-1,2,3,4,5,6,7,8,9.
More informationChapter 9 Linear Momentum and Collisions
Chapter 9 Linear Momentum and Collisions The Center of Mass The center of mass of a system of particles is the point that moves as though (1) all of the system s mass were concentrated there and (2) all
More informationLast class, we learned Section 9-8, Momentum and Kinetic Energy in Collisions
Final Exam 8:30-11:00 am, May 8th, 2007, Tuesday 208 Kupfrian Hall (Different from the room for the previous exams) From Chapter 1 to Chapter 9 Bring your scientific calculators. Lecture notes at Last
More informationLINEAR MOMENTUM. Momentum Impulse Conservation of Momentum Inelastic Collisions Elastic Collisions Momentum In 2 Dimensions Center of Mass
LINEAR MOMENTUM Momentum Impulse Conservation of Momentum Inelastic Collisions Elastic Collisions Momentum In 2 Dimensions Center of Mass MOMENTUM Quantity of Motion Product of Mass and Velocity p = mv
More informationPRINCIPLE OF LINEAR IMPULSE AND MOMENTUM AND CONSERVATION OF LINEAR MOMENTUM FOR SYSTEMS OF PARTICLES
PRINCIPLE OF LINEAR IMPULSE AND MOMENTUM AND CONSERVATION OF LINEAR MOMENTUM FOR SYSTEMS OF PARTICLES Today s Objectives: Students will be able to: 1. Apply the principle of linear impulse and momentum
More informationChapter 9 Linear Momentum
Chapter 9 Linear Momentum 7 12/7 16/7 Units of Chapter 9 Momentum, Impulse and Collisions Momentum and Impulse Define momentum Force and rate of change of momentum; resultant force as rate of change of
More informationPhysics 2514 Lecture 26
Physics 2514 Lecture 26 P. Gutierrez Department of Physics & Astronomy University of Oklahoma Physics 2514 p. 1/12 Review We have defined the following using Newton s second law of motion ( F net = d p
More informationPhysics 111: Week 8 10 Review
Physics 111: Week 8 10 Review Bin Chen NJIT Physics Department Announcements q Common Exam #3 on Nov 19 (Next Monday) from 4:15 pm to 5:45 pm in KUPF 107 q Must bring your NJIT ID q Cell phone and electronic
More informationPRINCIPLE OF LINEAR IMPULSE AND MOMENTUM FOR A SYSTEM OF PARTICLES AND CONSERVATION OF LINEAR MOMENTUM FOR A SYSTEM OF PARTICLES
PRINCIPLE OF LINEAR IMPULSE AND MOMENTUM FOR A SYSTEM OF PARTICLES AND CONSERVATION OF LINEAR MOMENTUM FOR A SYSTEM OF PARTICLES Today s Objectives: Students will be able to: 1. Apply the principle of
More informationThink-Pair-Share. Linear Momentum (Ch 9) Linear Momentum, cont. Newton and Momentum
Linear Momentum (Ch 9) The linear momentum of a particle or an object that can be modeled as a particle of mass m moving with a velocity v is defined to be the product of the mass and velocity: p = m v
More informationMULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question.
PH105-007 Exam 2 VERSION A Name MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. 1) A 1.0-kg block and a 2.0-kg block are pressed together on a horizontal
More informationChapter 9. Linear Momentum and Collisions
Chapter 9 Linear Momentum and Collisions Momentum Analysis Models Force and acceleration are related by Newton s second law. When force and acceleration vary by time, the situation can be very complicated.
More informationChapter 15 Kinematics of a Particle: Impulse and Momentum. Lecture Notes for Section 15-2~3
Chapter 15 Kinematics of a Particle: Impulse and Momentum Lecture Notes for Section 15-2~3 PRINCIPLE OF LINEAR IMPULSE AND MOMENTUM AND CONSERVATION OF LINEAR MOMENTUM FOR SYSTEMS OF PARTICLES Today s
More informationChapter 7- Linear Momentum
Chapter 7- Linear Momentum Old assignments and midterm exams (solutions have been posted on the web) can be picked up in my office (LB-212) All marks, including assignments, have been posted on the web.
More informationCh. 2 The Laws of Motion
Ch. 2 The Laws of Motion Lesson 1 Gravity and Friction Force - A push or pull we pull on a locker handle push a soccer ball or on the computer keys Contact force - push or pull on one object by another
More informationCh 7 Impulse-Momentum Theorem, Conservation of Momentum, and Collisions
Ch 7 Impulse-Momentum Theorem, Conservation of Momentum, and Collisions Momentum and its relation to force Momentum describes an object s motion. Linear momentum is the product of an object s mass and
More informationNotes Momentum. Momentum and Impulse. - The product (multiplication) of an objects mass and velocity is called momentum.
Notes Momentum Momentum and Impulse - The product (multiplication) of an objects mass and velocity is called momentum. Momentum is the energy of motion of an object. Momentum is represented by the letter.
More informationChapter 9. Linear Momentum
Chapter 9 Linear Momentum Linear Momentum Conservation of Linear Momentum Kinetic Energy of a System Collisions Collisions in Center of Mass Reference Frame MFMcGraw-PHY 45 Chap09Ha-Momentum-Revised-10//01
More informationImpulse/Momentum And Its Conservation
Impulse/Momentum And Its Conservation Which is easier to stop? Truck, car, bowling ball, or baseball all moving at 30 mph. Baseball -it is the least massive. Baseball at 30 mph or a baseball at 90 mph.
More informationPHYSICS FORMULAS. A. B = A x B x + A y B y + A z B z = A B cos (A,B)
PHYSICS FORMULAS A = A x i + A y j Φ = tan 1 A y A x A + B = (A x +B x )i + (A y +B y )j A. B = A x B x + A y B y + A z B z = A B cos (A,B) linear motion v = v 0 + at x - x 0 = v 0 t + ½ at 2 2a(x - x
More informationPHYS 1441 Section 002 Lecture #17
PHYS 1441 Section 002 Lecture #17 Monday, April 1, 2013 Linear Momentum Linear Momentum and Impulse Linear Momentum and Forces Linear Momentum Conservation Linear Momentum Conservation in a Two - body
More informationProblem Set 9: Momentum and Collision Theory. Nov 1 Hour One: Conservation Laws: Momentum and Collision Theory. Reading: YF
MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics Physics 8.0T Fall Term 2004 Problem Set 9: Momentum and Collision Theory Available on-line October 29; Due: November 9 at 4:00 p.m. Please write
More informationCollisions. Conservation of Momentum Elastic and inelastic collisions. Serway For practice: Chapter 9, problems 10, 11, 23, 70, 75
Collisions Conservation of Momentum Elastic and inelastic collisions Serway 9.3-9.4 For practice: Chapter 9, problems 10, 11, 23, 70, 75 Momentum: p = mv Impulse (a vector) is defined as F t (for a constant
More information(k = force constant of the spring)
Lecture 10: Potential Energy, Momentum and Collisions 1 Chapter 7: Conservation of Mechanical Energy in Spring Problems The principle of conservation of Mechanical Energy can also be applied to systems
More informationChapter 9 Impulse and Momentum
Chapter 9 Impulse and Momentum Chapter Goal: To understand and apply the new concepts of impulse and momentum. Slide 9-2 Chapter 9 Preview Slide 9-3 Chapter 9 Preview Slide 9-4 Chapter 9 Preview Slide
More informationPhysics 1501 Lecture 17
Physics 50: Lecture 7 Today s Agenda Homework #6: due Friday Midterm I: Friday only Topics Chapter 9» Momentum» Introduce Collisions Physics 50: Lecture 7, Pg Newton s nd Law: Chapter 9 Linear Momentum
More informationChapter 9. Linear Momentum and Collisions
Chapter 9 Linear Momentum and Collisions Linear Momentum The linear momentum of a particle or an object that can be modeled as a particle of mass m moving with a velocity v is defined to be the product
More informationAngular Momentum Conservation of Angular Momentum
Lecture 22 Chapter 12 Physics I Angular Momentum Conservation of Angular Momentum Course website: http://faculty.uml.edu/andriy_danylov/teaching/physicsi IN THIS CHAPTER, you will continue discussing rotational
More informationImpulse and Momentum continued
Chapter 7 Impulse and Momentum continued 7.2 The Principle of Conservation of Linear Momentum External forces Forces exerted on the objects by agents external to the system. Net force changes the velocity
More informationProblem Set 9: Momentum and Collision Theory : Solutions
MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics Physics 8.0T Fall Term 2004 Problem Set 9: Momentum and Collision Theory : Solutions Problem : Impulse and Momentum The compressive force per
More informationMomentum in 1-Dimension
Momentum in 1-Dimension Level : Physics I Date : Warm-up Questions If you were in a car that was out of control and had to choose between hitting a concrete wall or a haystack to stop, which would you
More informationWhat is momentum? Inertia in Motion.
What is momentum? Inertia in Motion. p = mv From Newton s 2 nd Law: F = ma = dv d( mv) m = dt dt F = dp dt The time rate of change of the linear momentum of a particle is equal to the net force acting
More information7-6 Inelastic Collisions
7-6 Inelastic Collisions With inelastic collisions, some of the initial kinetic energy is lost to thermal or potential energy. It may also be gained during explosions, as there is the addition of chemical
More informationCEE 271: Applied Mechanics II, Dynamics Lecture 17: Ch.15, Sec.2 4
1 / 38 CEE 271: Applied Mechanics II, Dynamics Lecture 17: Ch.15, Sec.2 4 Prof. Albert S. Kim Civil and Environmental Engineering, University of Hawaii at Manoa Tuesday, October 16, 2012 2 / 38 PRINCIPLE
More information23. A force in the negative direction of an x-axis is applied for 27ms to a 0.40kg ball initially moving at 14m/s in the positive direction of the
23. A force in the negative direction of an x-axis is applied for 27ms to a 0.40kg ball initially moving at 14m/s in the positive direction of the axis. The force varies in magnitude, and the impulse has
More informationExam 3--PHYS 101--F15
Name: Exam 3--PHYS 0--F5 Multiple Choice Identify the choice that best completes the statement or answers the question.. It takes 00 m to stop a car initially moving at 25.0 m/s. The distance required
More informationVersion PREVIEW Semester 1 Review Slade (22222) 1
Version PREVIEW Semester 1 Review Slade () 1 This print-out should have 48 questions. Multiple-choice questions may continue on the next column or page find all choices before answering. Holt SF 0Rev 10A
More informationPhys 2101 Gabriela González. Single particle: = ma. net. dt = F. Several particles: P dt = M a com. F ext. If F net =0, momentum is conserved
Phys 2101 Gabriela González Single particle: Several particles: p = mv dp dt = F net = ma p +... P = p p 1 + 2 3 + d P dt = M a com = F ext If F net =0, momentum is conserved Ricardo, mass 95 kg, and Carmelita,
More informationAn astronaut of mass 80 kg pushes away from a space Both!p x
Chapter 6 Momentum Collisions Definition: Momentum Important because it is CONSERVED proof: p = m v F = m v t = p t Ft = p Since F 12 =-F 21, p 1 + p 2 = 0 p i for isolated particles never changes Vector
More informationCompare the momentum of the same object moving with different velocities. Identify examples of change in the momentum of an object.
HOLT CH 6 notes Objectives :Compare the momentum of different moving objects. Compare the momentum of the same object moving with different velocities. Identify examples of change in the momentum of an
More informationMomentum and Its Relation to Force
Linear Momentum Momentum and Its Relation to Force The linear momentum, or momentum, of an object is defined as the product of its mass and its velocity. Momentum, p, is a vector and its direction is the
More informationMomentum Energy Angular Momentum
Notes 8 Impulse and Momentum Page 1 Impulse and Momentum Newton's "Laws" require us to follow the details of a situation in order to calculate properties of the system. Is there a simpler way? CONSERVATION
More informationPhysics 231. Topic 6: Momentum and Collisions. Alex Brown October MSU Physics 231 Fall
Physics 231 Topic 6: Momentum and Collisions Alex Brown October 7 2015 MSU Physics 231 Fall 2015 1 Momentum F = m a Newton s 2nd law F = m v/ t a= v/ t F = m (v final - v inital )/ t Define p = mv p: momentum
More informationMar 20, 2013 PHYSICS I Lecture 14
95.141 Mar 20, 2013 PHYSICS I Lecture 14 Exam II Wed Mar 27 Review Session Mon Mar 25 6-8:30 pm Ball 210 Course website: faculty.uml.edu/pchowdhury/95.141/ www.masteringphysics.com Course: UML95141SPRING2013
More informationPHYSICS. Chapter 11 Lecture FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E RANDALL D. KNIGHT Pearson Education, Inc.
PHYSICS FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E Chapter 11 Lecture RANDALL D. KNIGHT Chapter 11 Impulse and Momentum IN THIS CHAPTER, you will learn to use the concepts of impulse and momentum.
More informationModule 17: Systems, Conservation of Momentum and Center of Mass
Module 17: Systems, Conservation of Momentum and Center of Mass 17.1 External and Internal Forces and the Change in Momentum of a System So far we have restricted ourselves to considering how the momentum
More information4.) A baseball that weighs 1.6 N leaves a bat with a speed of 40.0 m/s. Calculate the kinetic energy of the ball. 130 J
AP Physics-B Energy And Its Conservation Introduction: Energy is a term that most of us take for granted and use quite freely. We assume we know what we are talking about when speaking of energy. In truth,
More informationPHYS 1441 Section 002 Lecture #17
PHYS 1441 Section 002 Lecture #17 Dr. Jaehoon Linear Momentum Linear Momentum and Impulse Linear Momentum and Forces Linear Momentum Conservation Collisions Center of Mass Today s homework is homework
More informationPhysics 1A Fall 2013: Quiz 4 Version A 1. Department of Physics Physics 1A Fall Quarter 2013 Dr. Paddock. Version A
Physics 1A Fall 2013: Quiz 4 Version A 1 Department of Physics Physics 1A Fall Quarter 2013 Dr. Paddock Version A DO NOT TURN OVER THIS PAGE UNTIL INSTRUCTED TO DO SO PUT AWAY ALL BOOKS, NOTES, PHONES,
More informationCHAPTER 9 LINEAR MOMENTUM AND COLLISION
CHAPTER 9 LINEAR MOMENTUM AND COLLISION Couse Outline : Linear momentum and its conservation Impulse and Momentum Collisions in one dimension Collisions in two dimension The center of mass (CM) 9.1 Linear
More informationRecap: Energy Accounting
Recap: Energy Accounting Energy accounting enables complex systems to be studied. Total Energy = KE + PE = conserved Even the simple pendulum is not easy to study using Newton s laws of motion, as the
More informationMomentum and Its Relation to Force
Linear Momentum Momentum and Its Relation to Force Momentum is a vector symbolized by the symbol p, and is defined as: It is a vector and has units of: (kg m/s) or (Ns) The rate of change of momentum is
More informationMOMENTUM. The world is wide, and I will not waste my life in friction when it could be turned into momentum. Frances E. Willard.
MOMENTUM The world is wide, and I will not waste my life in friction when it could be turned into momentum. Frances E. Willard Honors Physics CONSERVATION OF Energy Linear Momentum Angular Momentum Electric
More informationLecture 16. Chapter 11. Energy Dissipation Linear Momentum. Physics I. Department of Physics and Applied Physics
Lecture 16 Chapter 11 Physcs I Energy Dsspaton Lnear Momentum Course webste: http://aculty.uml.edu/andry_danylov/teachng/physcsi Department o Physcs and Appled Physcs IN IN THIS CHAPTER, you wll learn
More informationBroughton High School of Wake County
Name: Section: 1 Section 1: Which picture describes Newton s Laws of Motion? 5. Newton s Law 1. Newton s Law 2. Newton s Law 6. Newton s Law 3. Newton s Law 7. Newton s Law 4. Newton s Law 8. Newton s
More informationLecture 13. Impulse and Linear Momentum. Center of Mass for a system of particles. Momentum Conservation And Collisions. Physics 105 Summer 2006
Lecture 13 Center of Mass for a system of particles 2 bodies, 1 dimension Momentum Conservation And Collisions (HR&W, Chapters 9) http://web.njit.edu/~sirenko/ 0 COM Physics 105 Summer 2006 Lecture 13
More informationChapter 9. Center of Mass and Linear Momentum
Chapter 9 Center of Mass and Linear Momentum 9.2 The Center of Mass Recall we had idealized a body by treating it as a point particle (neglecting its extent). We now start working towards a more complete
More informationPhysics 211: Lecture 14. Today s Agenda
Physics 211: Lecture 14 Today s Agenda Systems of Particles Center of mass Linear Momentum Example problems Momentum Conservation Inelastic collisions in one dimension Ballistic pendulum Physics 211: Lecture
More informationChapter 9. Collisions. Copyright 2010 Pearson Education, Inc.
Chapter 9 Linear Momentum and Collisions Linear Momentum Units of Chapter 9 Momentum and Newton s Second Law Impulse Conservation of Linear Momentum Inelastic Collisions Elastic Collisions Units of Chapter
More informationChapter 9 Linear Momentum and Collisions
Chapter 9 Linear Momentum and Collisions Units of Chapter 9 Linear Momentum Momentum and Newton s Second Law Impulse Conservation of Linear Momentum Inelastic Collisions Elastic Collisions Units of Chapter
More informationPhysics 207 Lecture 11. Lecture 11. Chapter 8: Employ rotational motion models with friction or in free fall
Goals: Lecture 11 Chapter 8: Employ rotational motion models with friction or in free fall Chapter 9: Momentum & Impulse Understand what momentum is and how it relates to forces Employ momentum conservation
More informationChapter 6 Work and Energy
Chapter 6 Work and Energy Midterm exams will be available next Thursday. Assignment 6 Textbook (Giancoli, 6 th edition), Chapter 6: Due on Thursday, November 5 1. On page 162 of Giancoli, problem 4. 2.
More informationMomentum. Physics 1425 Lecture 15. Michael Fowler, UVa
Momentum Physics 1425 Lecture 15 Michael Fowler, UVa Physics Definition of Momentum Momentum is another word (like work, energy, etc.) from everyday life that has a precise meaning when used in physics.
More informationLecture 13. Collisions. and Review of material. Pre-reading: KJF 9.5. Please take an evaluation form
Lecture 13 Collisions and Review of material Pre-reading: KJF 9.5 Please take an evaluation form COLLISIONS KJF 9.5, 10.7 Conservation of momentum Recall from our discussion of momentum (Lecture 9), that
More informationEnergy problems look like this: Momentum conservation problems. Example 8-1. Momentum is a VECTOR Example 8-2
Review Chp 7: Accounting with Mechanical Energy: the overall Bank Balance When we judge how much energy a system has, we must have two categories: Kinetic energy (K sys ), and potential energy (U sys ).
More informationChap. 8: Collisions and Momentum Conservation
Chap. 8: Collisions and Momentum Conservation 1. System in Collision and Explosion C.M. 2. Analysis of Motion of System (C.M.) Kinematics and Dynamics Conservation between Before and After a) b) Energy
More informationthe spring is compressed and x is the compression
Lecture 4 Spring problem and conservation of mechanical energy Hooke's Law The restoring force exerted by the spring is directly proportional to its displacement. The restoring force acts in a direction
More informationMomentum and Impulse
Momentum and Impulse How can we describe the change in velocities of colliding football players, or balls colliding with bats? How does a strong force applied for a very short time affect the motion? Can
More information(D) Based on Ft = m v, doubling the mass would require twice the time for same momentum change
1. A car of mass m, traveling at speed v, stops in time t when maximum braking force is applied. Assuming the braking force is independent of mass, what time would be required to stop a car of mass m traveling
More informationA. B. C. D. E. v x. ΣF x
Q4.3 The graph to the right shows the velocity of an object as a function of time. Which of the graphs below best shows the net force versus time for this object? 0 v x t ΣF x ΣF x ΣF x ΣF x ΣF x 0 t 0
More informationToday's goal: I can explain and apply concepts of work and energy (3U) to real world applicaons.
Lesson21.notebook September 17, 2013 Work and Energy A 3U Review Today's goal: I can explain and apply concepts of work and energy (3U) to real world applicaons. What is Work? How do we calculate it? Example:
More informationChapter 7. Impulse and Momentum
Chapter 7 Impulse and Momentum Chaper 6 Review: Work and Energy Forces and Displacements Effect of forces acting over a displacement Work W = (F cos)s Work changes the Kinetic Energy of a mass Kinetic
More informationOctober 24. Linear Momentum: - It is a vector which may require breaking it into components
October 24 Linear Momentum: - It is a vector which may require breaking it into components Newton s First Law: A body continues with Constant Linear Momentum unless it is acted upon by a Net External Force.
More informationEnergy in Collisions Problems AP Physics C
1. A bullet of mass m and velocity v 0 is fired toward a block of mass 4m. The block is initially at rest on a v frictionless horizontal surface. The bullet penetrates the block and emerges with a velocity
More informationAP Physics 1 Momentum and Impulse Practice Test Name
AP Physics 1 Momentum and Impulse Practice Test Name MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. 1) A rubber ball and a lump of clay have equal
More informationPhysics 141. Lecture 8.
Physics 141. Lecture 8. Conservation of energy! Changing kinetic energy into thermal energy. Frank L. H. Wolfs Department of Physics and Astronomy, University of Rochester, Lecture 08, Page 1 Outline.
More informationLecture 11. Linear Momentum and Impulse. Collisions.
Lecture 11 Linear Momentum and Impulse. Collisions. Momentum and Newton s Second Law F net = m a= m Δ v Δ t = Δ (m v ) Δ t = Δ p Δ t Linear momentum p = m v Newton s second law in terms of linear momentum:
More informationhorizontal motion? Assume that the positive direction is the direction the ball is traveling before it is hit by the opponent's racket.
Ch 8 Supplemental [ Edit ] Overview Summary View Diagnostics View Print View with Answers Ch 8 Supplemental Due: 6:59pm on Wednesday, November 16, 2016 To understand how points are awarded, read the Grading
More information(A) 0 (B) mv (C) 2mv (D) 2mv sin θ (E) 2mv cos θ
Physics 1 Lesson 8 Forces and Momentum Homework Outcomes 1. Define linear momentum. 2. Determine the total linear momentum of a system. 3. Apply the Law of Conservation of Momentum to solve problems. 4.
More information1. A train moves at a constant velocity of 90 km/h. How far will it move in 0.25 h? A. 10 km B km C. 25 km D. 45 km E. 50 km
Name: Physics I Mid Term Exam Review Multiple Choice Questions Date: Mr. Tiesler 1. A train moves at a constant velocity of 90 km/h. How far will it move in 0.25 h? A. 10 km B. 22.5 km C. 25 km D. 45 km
More informationCenter of Mass & Linear Momentum
PHYS 101 Previous Exam Problems CHAPTER 9 Center of Mass & Linear Momentum Center of mass Momentum of a particle Momentum of a system Impulse Conservation of momentum Elastic collisions Inelastic collisions
More informationNewton s Laws of Motion
Chapter 4 Newton s Second Law: in vector form Newton s Laws of Motion σ റF = m റa in component form σ F x = ma x σ F y = ma y in equilibrium and static situations a x = 0; a y = 0 Strategy for Solving
More informationWhen particle with mass m moves with velocity v, we define its Linear Momentum p as product of its mass m and its velocity v:
8. LINEAR MOMENTUM. Key words: Linear Momentum, Law of Conservation of Momentum, Collisions, Elastic Collisions, Inelastic Collisions, Completely Inelastic Collision, Impulse, Impulse Momentum Theorem.
More informationPhysics 141. Lecture 8. Outline. Course Information. Conservation of energy! Changing kinetic energy into thermal energy.
Physics 141. Lecture 8. Conservation of energy! Changing kinetic energy into thermal energy. Frank L. H. Wolfs Department of Physics and Astronomy, University of Rochester, Lecture 08, Page 1 Outline.
More informationChapter 7. Impulse and Momentum
Chapter 7 Impulse and Momentum 7.1 The Impulse-Momentum Theorem There are many situations when the force on an object is not constant. 7.1 The Impulse-Momentum Theorem DEFINITION OF IMPULSE The impulse
More informationWelcome back to Physics 211
Welcome back to Physics 211 Today s agenda: Work Power Physics 211 Fall 2012 Lecture 09-2 1 Current assignments HW#9 due this Friday at 5 pm. Short assignment SAGE (Thanks for the feedback!) I am using
More informationImpulse. Two factors influence the amount by which an object s momentum changes.
Impulse In order to change the momentum of an object, either its mass, its velocity, or both must change. If the mass remains unchanged, which is most often the case, then the velocity changes and acceleration
More information1. A tennis ball of mass m moving horizontally with speed u strikes a vertical tennis racket. The ball bounces back with a horizontal speed v.
1. A tennis ball of mass m moving horizontally with speed u strikes a vertical tennis racket. The ball bounces back with a horizontal speed v. The magnitude of the change in momentum of the ball is A.
More informationREVISING MECHANICS (LIVE) 30 JUNE 2015 Exam Questions
REVISING MECHANICS (LIVE) 30 JUNE 2015 Exam Questions Question 1 (Adapted from DBE November 2014, Question 2) Two blocks of masses 20 kg and 5 kg respectively are connected by a light inextensible string,
More informationUNIT 2G. Momentum & It s Conservation
Name: Date:_ UNIT 2G Momentum & It s Conservation Momentum & Newton s 2 nd Law of Motion Newton s 2 nd Law states When an unbalanced force acts upon a body, it accelerates that body in the direction of
More informationANSWER'SHEET' 'STAPLE'TO'FRONT'OF'EXAM'! Name:!!!CWID:!!! Lab'section'(circle'one):' 6!(W!3pm)! 8!(W!7pm)!!!
ANSWER'SHEET' 'STAPLE'TO'FRONT'OF'EXAM' Name: CWID: Lab'section'(circle'one):' 6(W3pm) 8(W7pm) Multiplechoice: 1. 2. 3. 4. 5. 6. 7. 8. 9. 10. 11. 12. 13. 14. 15. Shortanswer: 16. 17. 18. 19. 20. 5(R7pm)
More informationANSWER'SHEET' 'STAPLE'TO'FRONT'OF'EXAM'! Name:!!!CWID:!!! Lab'section'(circle'one):' 6!(W!3pm)! 8!(W!7pm)!!!
ANSWER'SHEET' 'STAPLE'TO'FRONT'OF'EXAM' Name: CWID: Lab'section'(circle'one):' 6(W3pm) 8(W7pm) Multiplechoice: 1. 2. 3. 4. 5. 6. 7. 8. 9. 10. 11. 12. 13. 14. 15. Shortanswer: 16. 17. 18. 19. 20. 5(R7pm)
More informationMomentum and Collisions
Momentum and Collisions Objectives: You Should Be Able To: Define and give examples of impulse and momentum along with appropriate units. Write and apply a relationship between impulse and momentum in
More informationConcepts in Physics. Friday, October 16th
1206 - Concepts in Physics Friday, October 16th Notes Assignment #4 due Wednesday, October 21 st in class (no later than noon) There are still assignments #1 and #2 in my office to be picked up... If you
More informationMomentum & Energy Review Checklist
Momentum & Energy Review Checklist Impulse and Momentum 3.1.1 Use equations to calculate impulse; momentum; initial speed; final speed; force; or time. An object with a mass of 5 kilograms is moving at
More informationAP Physics C Summer Homework. Questions labeled in [brackets] are required only for students who have completed AP Calculus AB
1. AP Physics C Summer Homework NAME: Questions labeled in [brackets] are required only for students who have completed AP Calculus AB 2. Fill in the radian conversion of each angle and the trigonometric
More informationPhysics 110 Homework Solutions Week #6 - Wednesday
Physics 110 Homework Solutions Week #6 - Wednesday Friday, May3, 2013 Chapter 6 Questions - none Multiple-Choice 66 C 67 D 68 B 69 C Problems 612 It s velocity as the ball hits the ground is found from
More information