Chapter 9 Centre of Mass and Linear Momentum
|
|
- Augusta Eaton
- 5 years ago
- Views:
Transcription
1 Chater 9 Centre o Mass and Linear Moentu Centre o ass o a syste o articles / objects Linear oentu Linear oentu o a syste o articles Newton s nd law or a syste o articles Conseration o oentu Elastic and Inelastic Collisions
2 Conseration o Moentu I F ext F ext That is, oentu is consered when the net external orce acting on an object is zero. This alies also to an isolated syste o two or ore objects (no external orces) that ay be in contact - the total oentu is consered. Coare Newton s irst law: t 0 then 0 elocity is constant when the net orce is zero.
3 Conseration o Moentu Two isolated asses collide. The initial total oentu is: With 0 0 While the asses are in contact, they exert equal and oosite orces on each other (Newton s third law). F F So the iulse acting on is equal in agnitude and oosite in direction to the iulse acting on
4 Thereore, (change in oentu = iulse) Ater the collision: So, the total oentu ater the collision is: That is, total oentu is consered:
5 Exale: An ice boat slides without riction horizontally across the ice. Soeone jus ertically down ro a bridge onto the boat. Does the oentu o the boat change? As the oentu o the erson is downward, not sideways, the horizontal oentu o the boat is unchanged. M o M As the ass o the boat is increased by the ass o the erson, the boat oes ore slowly, so that the oentu is unchanged. 0M M
6 Exale: A 55-kg swier is standing on a stationary 0-kg loating rat. The swier then jus o the rat horizontally with a elocity o +4.6 /s relatie to the shore. Find the recoil elocity that the rat would hae i there were no riction and resistance due to the water.
7 How ast was the bullet? Mass o bullet: = 0.0 kg Mass o block: =.50 kg The Ballistic Pendulu
8 Elastic and Inelastic Collisions Elastic collision: The total kinetic energy ater collision is equal to the total kinetic energy beore collision. Inelastic collision: The total kinetic energy is not the sae beore and ater the collision. I objects stick together ater collision, the collision is erectly inelastic no bouncing o one object ro the other. Reeber that oentu is always consered i no net orce is acting on the syste!
9 Elastic Collision Exale: A ball o ass = 0.5 kg akes a erectly elastic collision with a ball o ass = 0.8 kg. Elastic Collisions Initial oentu : Moentu ater collision: Moentu is consered : i 0 0
10 Elastic Collision Exale: A ball o ass = 0.5 kg akes a erectly elastic collision with a ball o ass = 0.8 kg. Moentu is consered : 0 Elastic Collisions 0
11 Elastic Collision Exale: A ball o ass = 0.5 kg akes a erectly elastic collision with a ball o ass = 0.8 kg. Moentu is consered : 0 Cobine with conseration o kinetic energy: 0 Elastic Collisions
12 Elastic Collision Exale: A ball o ass = 0.5 kg akes a erectly elastic collision with a ball o ass = 0.8 kg. Elastic Collisions Do soe algebra:
13 Elastic Collision Exale: A ball o ass = 0.5 kg akes a erectly elastic collision with a ball o ass = 0.8 kg. Elastic Collisions Do soe algebra: Two solutions: 0 0
14 Elastic Collision Exale: A ball o ass = 0.5 kg akes a erectly elastic collision with a ball o ass = 0.8 kg. Elastic Collisions Do soe algebra: Cobine and 0 0 0
15 Finally: Elastic Collision Exale: A ball o ass = 0.5 kg akes a erectly elastic collision with a ball o ass = 0.8 kg i, then, i Elastic Collisions
16 Elastic Collision Exale: A ball o ass = 0.5 kg akes a erectly elastic collision with a ball o ass = 0.8 kg. Elastic Collisions Finally: kg, 5 /s. 6 /s, 0. 8 kg,. 38 /s
17 Elastic Collisions Elastic Collision: In general: For any two objects with asses and colliding elastically and initially at rest!
18 Exale: An electron collides elastically with a stationary hydrogen ato. The ass o the hydrogen ato is 837 ties that o the electron. Assue that all otion, beore and ater the collision, occurs along the sae straight line. What is the ratio o the kinetic energy o the hydrogen ato ater the collision to that o the electron beore the collision?
19 The reight car on the let catches u with the one on the right and connects u with it. They trael on with the sae seed. Conseration o oentu:
20 Exale: 0 65, 000 kg, 0. 8 /s, 0 9, 000 kg. 3 /s Kinetic Energy: /s KE KE What haened to the issing energy? i J 9366 J 0 0 Missing 574 J This was an inelastic collision soe o the kinetic energy was conerted to heat and sound.
Physics Momentum: Collisions
F A C U L T Y O F E D U C A T I O N Departent o Curriculu and Pedagogy Physics Moentu: Collisions Science and Matheatics Education Research Group Supported by UBC Teaching and Learning Enhanceent Fund
More informationChapter 7. Impulse and Momentum
Chapter 7 Ipulse and Moentu 7. The Ipulse-Moentu Theore There are any situations when the force on an object is not constant. 7. The Ipulse-Moentu Theore DEFINITION OF IMPULSE The ipulse of a force is
More informationChapter 7 Impulse and Momentum. So far we considered only constant force/s BUT There are many situations when the force on an object is not constant
Chapter 7 Ipulse and Moentu So far we considered only constant force/s BUT There are any situations when the force on an object is not constant Force varies with tie 7. The Ipulse-Moentu Theore DEFINITION
More informationPage 1. t F t m v. N s kg s. J F t SPH4U. From Newton Two New Concepts Impulse & Momentum. Agenda
SPH4U Agenda Fro Newton Two New Concepts Ipulse & oentu Ipulse Collisions: you gotta consere oentu! elastic or inelastic (energy consering or not) Inelastic collisions in one diension and in two diensions
More informationChapter 7. Impulse and Momentum
Chapter 7 Ipulse and Moentu 7. The Ipulse-Moentu Theore 7. The Ipulse-Moentu Theore There are any situations when the force on an object is not constant. 7. The Ipulse-Moentu Theore DEFINITION OF IMPULSE
More informationChapter 7 Impulse and Momentum. So far we considered only constant force/s BUT There are many situations when the force on an object is not constant
Chapter 7 Ipulse and Moentu So far we considered only constant force/s BUT There are any situations when the force on an object is not constant JUST IN TIME TEACHING E-ail or bring e your questions prior
More informationMomentum, p = m v. Collisions and Work(L8) Crash! Momentum and Collisions. Conservation of Momentum. elastic collisions
Collisions and Work(L8) Crash! collisions can be ery coplicated two objects bang into each other and exert strong forces oer short tie interals fortunately, een though we usually do not know the details
More information2. REASONING According to the impulse-momentum theorem, the rocket s final momentum mv f
CHAPTER 7 IMPULSE AND MOMENTUM PROLEMS. REASONING According to the ipulse-oentu theore, the rocket s inal oentu diers ro its initial oentu by an aount equal to the ipulse ( ΣF ) o the net orce eerted on
More informationOne Dimensional Collisions
One Diensional Collisions These notes will discuss a few different cases of collisions in one diension, arying the relatie ass of the objects and considering particular cases of who s oing. Along the way,
More informationCJ57.P.003 REASONING AND SOLUTION According to the impulse-momentum theorem (see Equation 7.4), F t = mv
Solution to HW#7 CJ57.CQ.003. RASONNG AND SOLUTON a. Yes. Momentum is a ector, and the two objects hae the same momentum. This means that the direction o each object s momentum is the same. Momentum is
More informationPage 1. Physics 131: Lecture 16. Today s Agenda. Collisions. Elastic Collision
Physics 131: Lecture 16 Today s Agenda Elastic Collisions Definition Exaples Work and Energy Definition of work Exaples Physics 01: Lecture 10, Pg 1 Collisions Moentu is alost always consered during as
More informationCHAPTER 7 IMPULSE AND MOMENTUM
CHAPTER 7 IMPULSE AND MOMENTUM PROBLEMS 1. SSM REASONING The ipulse that the olleyball player applies to the ball can be ound ro the ipulse-oentu theore, Equation 7.4. Two orces act on the olleyball while
More informationToday s s topics are: Collisions and Momentum Conservation. Momentum Conservation
Today s s topics are: Collisions and P (&E) Conservation Ipulsive Force Energy Conservation How can we treat such an ipulsive force? Energy Conservation Ipulsive Force and Ipulse [Exaple] an ipulsive force
More informationMomentum, p. Crash! Collisions (L8) Momentum is conserved. Football provides many collision examples to think about!
Collisions (L8) Crash! collisions can be ery coplicated two objects bang into each other and exert strong forces oer short tie interals fortunately, een though we usually do not know the details of the
More informationCHAPTER 7 IMPULSE AND MOMENTUM
CHAPTER 7 IMPULSE AND MOMENTUM CONCEPTUAL QUESTIONS 1. REASONING AND SOLUTION The linear oentu p o an object is the product o its ass and its elocity. Since the autoobiles are identical, they hae the sae
More informationFOCUS ON CONCEPTS Section 7.1 The Impulse Momentum Theorem
WEEK-6 Recitation PHYS 3 FOCUS ON CONCEPTS Section 7. The Impulse Momentum Theorem Mar, 08. Two identical cars are traeling at the same speed. One is heading due east and the other due north, as the drawing
More informationPhysics 231 Lecture 13
Physics 3 Lecture 3 Mi Main points it o td today s lecture: Elastic collisions in one diension: ( ) v = v0 + v0 + + ( ) v = v0 + v0 + + Multiple ipulses and rocket propulsion. F Δ t = Δ v Δ v propellant
More informationWork and Energy Problems
09//00 Multiple hoice orce o strength 0N acts on an object o ass 3kg as it oes a distance o 4. I is perpendicular to the 4 displaceent, the work done is equal to: Work and Energy Probles a) 0J b) 60J c)
More informationPhysics Chapter 6. Momentum and Its Conservation
Physics Chapter 6 Moentu and Its Conservation Linear Moentu The velocity and ass of an object deterine what is needed to change its otion. Linear Moentu (ρ) is the product of ass and velocity ρ =v Unit
More informationApplied Physics I (Phys 182)
Applied Physics I (Phys 182) Dr. Joseph J. Trout E-ail: joseph.trout@drexel.edu Cell: (610)348-6495 Office: Disque 902 1 Moentu Ipulse Conservation of Moentu Explosions Inelastic Collisions Elastic Collisions
More informationPhysics 140 D100 Midterm Exam 2 Solutions 2017 Nov 10
There are 10 ultiple choice questions. Select the correct answer for each one and ark it on the bubble for on the cover sheet. Each question has only one correct answer. (2 arks each) 1. An inertial reference
More information8.012 Physics I: Classical Mechanics Fall 2008
MIT OpenCourseWare http://ocw.it.edu 8.012 Physics I: Classical Mechanics Fall 2008 For inforation about citing these aterials or our Ters of Use, isit: http://ocw.it.edu/ters. MASSACHUSETTS INSTITUTE
More informationConservation of Momentum
Conseration of Moentu We left off last with the idea that when one object () exerts an ipulse onto another (), exerts an equal and opposite ipulse onto. This happens in the case of a classic collision,
More informationPhysics 11 HW #6 Solutions
Physics HW #6 Solutions Chapter 6: Focus On Concepts:,,, Probles: 8, 4, 4, 43, 5, 54, 66, 8, 85 Focus On Concepts 6- (b) Work is positive when the orce has a coponent in the direction o the displaceent.
More informationPhysics 11 HW #7 Solutions
hysics HW #7 Solutions Chapter 7: Focus On Concepts: 2, 6, 0, 3 robles: 8, 7, 2, 22, 32, 53, 56, 57 Focus On Concepts 7-2 (d) Moentu is a ector quantity that has a agnitude and a direction. The agnitudes
More informationT = 2.34x10 6 s = 27.2days.
Sole the following probles in the space proided Use the back of the page if needed Each proble is worth 10 points You ust show your work in a logical fashion starting with the correctly applied and clearly
More informationXI PHYSICS M. AFFAN KHAN LECTURER PHYSICS, AKHSS, K. https://promotephysics.wordpress.com
XI PHYSICS M. AFFAN KHAN LECTURER PHYSICS, AKHSS, K affan_414@live.co https://prootephysics.wordpress.co [MOTION] CHAPTER NO. 3 In this chapter we are going to discuss otion in one diension in which we
More informationConservation of Linear Momentum, Collisions
Conseration of Linear Momentum, Collisions 1. 3 kg mass is moing with an initial elocity i. The mass collides with a 5 kg mass m, which is initially at rest. Find the final elocity of the masses after
More informationCHAPTER 7: Linear Momentum
CHAPTER 7: Linear Moentu Solution Guide to WebAssign Probles 7.1 [1] p v ( 0.08 kg) ( 8.4 s) 0.4 kg s 7. [] Fro Newton s second law, p Ft. For a constant ass object, p v. Equate the two expression for
More informationLecture 6. Announcements. Conservation Laws: The Most Powerful Laws of Physics. Conservation Laws Why they are so powerful
Conseration Laws: The Most Powerful Laws of Physics Potential Energy gh Moentu p = + +. Energy E = PE + KE +. Kinetic Energy / Announceents Mon., Sept. : Second Law of Therodynaics Gie out Hoework 4 Wed.,
More informationincreases. In part (b) the impulse and initial momentum are in opposite directions and the velocity decreases.
8IDENTIFY and SET U: p = K = EXECUTE: (a) 5 p = (, kg)( /s) = kg /s 5 p kg /s (b) (i) = = = 6 /s (ii) kg =, so T T SUV SUV, kg ( /s) 68 /s T SUV = T = = SUV kg EVALUATE:The SUV ust hae less speed to hae
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 informationCHAPTER 7 TEST REVIEW -- MARKSCHEME
AP PHYSICS Nae: Period: Date: Points: 53 Score: IB Curve: DEVIL PHYSICS BADDEST CLASS ON CAMPUS 50 Multiple Choice 45 Single Response 5 Multi-Response Free Response 3 Short Free Response 2 Long Free Response
More informationUNIT HOMEWORK MOMENTUM ANSWER KEY
UNIT HOMEWORK MOMENTUM ANSWER KEY MOMENTUM FORMULA & STUFF FROM THE PAST: p = v, TKE = ½v 2, d = v t 1. An ostrich with a ass of 146 kg is running to the right with a velocity of 17 /s. a. Calculate the
More informationPS113 Chapter 7. Impulse and Momentum
PS113 Chapter 7 Impulse and Momentum 1 The impulse-momentum theorem There are many situations in which the force acting on a object is not constant, but varies with time. The resulting motion can be simply
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 informationSection 1 Momentum and Impulse. Chapter 6. Preview. Objectives Linear Momentum. Houghton Mifflin Harcourt Publishing Company
Section 1 Momentum and Impulse Preview Objectives Linear Momentum Section 1 Momentum and Impulse Objectives Compare the momentum of different moving objects. Compare the momentum of the same object moving
More informationSOLUTIONS TO CONCEPTS CHAPTER 9
SOUTIONS TO CONCEPTS CHPTER 9. kg, kg, kg, x 0, x, x / y 0, y 0, y / The position of centre of ass is C. x x x y y y, ( 0) ( ) ( / ) ( 0) ( 0) ( (, 7, fro the point B. / )). et be the origin of the syste
More informationPhysics 201, Lecture 15
Physics 0, Lecture 5 Today s Topics q More on Linear Moentu And Collisions Elastic and Perfect Inelastic Collision (D) Two Diensional Elastic Collisions Exercise: Billiards Board Explosion q Multi-Particle
More informationPS 11 GeneralPhysics I for the Life Sciences
PS GeneralPhysics I for the Life Sciences W O R K N D E N E R G Y D R. E N J M I N C H N S S O C I T E P R O F E S S O R P H Y S I C S D E P R T M E N T J N U R Y 0 4 Questions and Probles for Conteplation
More informationPhys101 Lectures 13, 14 Momentum and Collisions
Phs0 Lectures 3, 4 Moentu and ollisions Ke points: Moentu and ipulse ondition for conservation of oentu and wh How to solve collision probles entre of ass Ref: 7-,,3,4,5,6,7,8,9,0. Page Moentu is a vector:
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 informationConservation of Momentum. The total momentum of a closed, isolated system does not change.
Conservation of Momentum In the 17 th century, Newton and others had measured the momentum of colliding objects before and after collision, and had discovered a strange phenomenon: the total momentum of
More informationMomentum. Momentum. Impulse. Impulse Momentum Theorem. Deriving Impulse. v a t. Momentum and Impulse. Impulse. v t
Moentu and Iule Moentu Moentu i what Newton called the quantity of otion of an object. lo called Ma in otion The unit for oentu are: = oentu = a = elocity kg Moentu Moentu i affected by a and elocity eeding
More informationbefore the collision and v 1 f and v 2 f after the collision. Since conservation of the linear momentum
Lecture 7 Collisions Durin the preious lecture we stared our discussion of collisions As it was stated last tie a collision is an isolated eent in which two or ore odies (the collidin odies) exert relatiely
More information26 Impulse and Momentum
6 Ipulse and Moentu First, a Few More Words on Work and Energy, for Coparison Purposes Iagine a gigantic air hockey table with a whole bunch of pucks of various asses, none of which experiences any friction
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 and Energy. Relativity and Astrophysics Lecture 24 Terry Herter. Energy and Momentum Conservation of energy and momentum
Momentum and Energy Relatiity and Astrohysics Lecture 4 Terry Herter Outline Newtonian Physics Energy and Momentum Conseration of energy and momentum Reading Sacetime Physics: Chater 7 Homework: (due Wed.
More informationENGINEERING COUNCIL DYNAMICS OF MECHANICAL SYSTEMS D225 TUTORIAL 2 LINEAR IMPULSE AND MOMENTUM
ENGINEERING COUNCIL DYNAMICS OF MECHANICAL SYSTEMS D5 TUTORIAL LINEAR IMPULSE AND MOMENTUM On copletion of this ttorial yo shold be able to do the following. State Newton s laws of otion. Define linear
More informationPHYSICS 2210 Fall Exam 4 Review 12/02/2015
PHYSICS 10 Fall 015 Exa 4 Review 1/0/015 (yf09-049) A thin, light wire is wrapped around the ri of a unifor disk of radius R=0.80, as shown. The disk rotates without friction about a stationary horizontal
More informationLINEAR MOMENTUM AND COLLISIONS
LINEAR MOMENTUM AND COLLISIONS Chapter 9 Units of Chapter 9 Linear Momentum Momentum and Newton s Second Law Impulse Conservation of Linear Momentum Inelastic Collisions Elastic Collisions Center of Mass
More informationA 30 o 30 o M. Homework #4. Ph 231 Introductory Physics, Sp-03 Page 1 of 4
Hoework #4. Ph 231 Introductory Physics, Sp-03 Page 1 o 4 4-1A. A particle o ass 2 kg is initially at rest at the origin x = 0. I the only orce acting on the particle is a constant 4 in the x-direction,
More informationCHAPTER 1 MOTION & MOMENTUM
CHAPTER 1 MOTION & MOMENTUM SECTION 1 WHAT IS MOTION? All atter is constantly in MOTION Motion involves a CHANGE in position. An object changes position relative to a REFERENCE POINT. DISTANCE is the total
More informationA B B A. the speed of the bat doesn t change significantly during the collision. Then the velocity of the baseball after being hit is v
CHPTER 7: Linear oentu nswers to Questions. For oentu to be consered, the syste under analysis ust be closed not hae any forces on it fro outside the syste. coasting car has air friction and road friction
More information1 A freight car of mass 20,000 kg moves along a frictionless level railroad track with a constant speed of 15 m/s. What is the momentum of the car?
Slide 1 / 26 1 freight car of mass 20,000 kg moves along a frictionless level railroad track with a constant speed of 15 m/s. What is the momentum of the car? 30,000 kg m/s 3,000 kg m/s 300,000 kg m/s
More informationDescription: Conceptual: A bullet embeds in a stationary, frictionless block: type of collision? what is conserved? v_final?
Chapter 8 [ Edit ] Overview Suary View Diagnostics View Print View with Answers Chapter 8 Due: 11:59p on Sunday, October 23, 2016 To understand how points are awarded, read the Grading Policy for this
More informationp p I p p p I p I p p
Net momentum conservation for collision on frictionless horizontal surface v1i v2i Before collision m1 F on m1 from m2 During collision for t v1f m2 F on m2 from m1 v2f +x direction After collision F F
More informationConservation of Momentum
Conservation of Momentum Law of Conservation of Momentum The sum of the momenta before a collision equal the sum of the momenta after the collision in an isolated system (=no external forces acting).
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 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 informationMomentum. February 15, Table of Contents. Momentum Defined. Momentum Defined. p =mv. SI Unit for Momentum. Momentum is a Vector Quantity.
Table of Contents Click on the topic to go to that section Moentu Ipulse-Moentu Equation The Moentu of a Syste of Objects Conservation of Moentu Types of Collisions Collisions in Two Diensions Moentu Return
More informationMomentum Practice Problems
Momentum Practice Problems PSI AP Physics C Name Multiple Choice 1. A steel ball and a piece of clay have equal mass. They are dropped from the same height on a horizontal steel platform. The ball bounces
More informationWe last left off by talking about how the area under a force vs. time curve is impulse.
Lecture 11 Ipulse and Moentu We last left off by talking about how the area under a force vs. tie curve is ipulse. Recall that for our golf ball we had a strongly peaked force curve: F F avg t You have
More information5.1 m is therefore the maximum height of the ball above the window. This is 25.1 m above the ground. (b)
.6. Model: This is a case of free fall, so the su of the kinetic and gravitational potential energy does not change as the ball rises and falls. The figure shows a ball s before-and-after pictorial representation
More informationYour Thoughts. What is the difference between elastic collision and inelastic collision?
Your Thoughts This seemed pretty easy...before we got the checkpoint questions What is the difference between elastic collision and inelastic collision? The most confusing part of the pre lecture was the
More informationAP Physics Chapter 9 QUIZ
AP Physics Chapter 9 QUIZ Name:. The graph at the right shows the force on an object of mass M as a function of time. For the time interal 0 to 4 seconds, the total change in the momentum of the object
More informationChapter 11 Collision Theory
Chapter Collision Theory Introduction. Center o Mass Reerence Frame Consider two particles o masses m and m interacting ia some orce. Figure. Center o Mass o a system o two interacting particles Choose
More informationChapter 9. 9 Momentum. Momentum. PowerPoint Lectures for College Physics: A Strategic Approach, Second Edition Pearson Education, Inc.
Chapter 9 Momentum PowerPoint Lectures for College Physics: A Strategic Approach, Second Edition 9 Momentum Slide 9-2 Slide 9-3 1 Slide 9-4 Reading Quiz 1. Impulse is A. a force that is applied at a random
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 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 informationAP Physics Momentum AP Wrapup
AP Phyic Moentu AP Wrapup There are two, and only two, equation that you get to play with: p Thi i the equation or oentu. J Ft p Thi i the equation or ipule. The equation heet ue, or oe reaon, the ybol
More informationImpulse (J) J = FΔ t Momentum Δp = mδv Impulse and Momentum j = (F)( p = ( )(v) F)(Δ ) = ( )(Δv)
Impulse (J) We create an unbalancing force to overcome the inertia of the object. the integral of force over time The unbalancing force is made up of the force we need to unbalance the object and the time
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 informationLinear Momentum and Collisions Conservation of linear momentum
Unit 4 Linear omentum and Collisions 4.. Conseration of linear momentum 4. Collisions 4.3 Impulse 4.4 Coefficient of restitution (e) 4.. Conseration of linear momentum m m u u m = u = u m Before Collision
More informationChapter 9. Momentum. PowerPoint Lectures for College Physics: A Strategic Approach, Second Edition Pearson Education, Inc.
Chapter 9 Momentum PowerPoint Lectures for College Physics: A Strategic Approach, Second Edition 9 Momentum Slide 9-2 Slide 9-3 Slide 9-4 Reading Quiz 1. Impulse is A. a force that is applied at a random
More informationName: Class: Date: p 1 = p 2. Given m = 0.15 kg v i = 5.0 m/s v f = 3.0 m/s Solution
Assessment Chapter Test A Teacher Notes and Answers Momentum and Collisions CHAPTER TEST A (GENERAL) 1. c 2. c 3. b 4. c 5. a p i = 4.0 kg m/s p f = 4.0 kg m/s p = p f p i = ( 4.0 kg m/s) 4.0 kg m/s =
More informationUNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics
UNIVERSITY OF SASKATCHEWAN Departent of Physics and Engineering Physics 017 Saskatchewan High School Physics Scholarship Copetition Wednesday May 10, 017 Tie allowed: 90 inutes This copetition is based
More informationBALLISTIC PENDULUM. EXPERIMENT: Measuring the Projectile Speed Consider a steel ball of mass
BALLISTIC PENDULUM INTRODUCTION: In this experient you will use the principles of conservation of oentu and energy to deterine the speed of a horizontally projected ball and use this speed to predict the
More informationPhysics. Impulse & Momentum
Physics Impulse & Momentum Warm up - Write down everything you know about impulse and momentum. Objectives Students will learn the definitions and equations for impulse, momentum, elastic and inelastic
More informationChapter 8. Momentum, Impulse and Collisions. 10/22/14 Physics 218
Chapter 8 Moentu, Ipulse and Collisions 0//4 Physics 8 Learning Goals n n n n n n The eaning of the oentu of a particle(syste) and how the ipulse of the net force acting on a particle causes the oentu
More informationPhysics 20 Lesson 18 Pulleys and Systems
Physics 20 Lesson 18 Pulleys and Systes I. Pulley and syste probles In this lesson we learn about dynaics probles that involve several asses that are connected and accelerating together. Using the pulley
More informationRELEASED. Go to next page. 2. The graph shows the acceleration of a car over time.
1. n object is launched across a room. How can a student determine the average horizontal velocity of the object using a meter stick and a calculator? The student can calculate the object s initial potential
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 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 informationEnergy and Momentum: The Ballistic Pendulum
Physics Departent Handout -10 Energy and Moentu: The Ballistic Pendulu The ballistic pendulu, first described in the id-eighteenth century, applies principles of echanics to the proble of easuring the
More informationPHYSICS 231 INTRODUCTORY PHYSICS I
PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 8 Last Lecture Work for nonconstant force F x Spring force F =!kx x Potential Energy of Spring PE = 1 2 kx2 Power P = "W "t P = Fv = "KE "t Chapter 6 Momentum
More informationMomentum. Conservation of Linear Momentum. Slide 1 / 140 Slide 2 / 140. Slide 3 / 140. Slide 4 / 140. Slide 6 / 140. Slide 5 / 140.
Slide 1 / 140 Slide 2 / 140 Moentu www.njctl.org Slide 3 / 140 Slide 4 / 140 Table of Contents Click on the topic to go to that section Conservation of Linear Moentu Ipulse - Moentu Equation Collisions
More informationUnit 1: Momentum & Impulse
Imulse and Change in Momentum Unit 1: Momentum & Imulse Momentum is a vector quantity. It is the roduct o a body s mass and its velocity. mv Units: kgm/s Imulse is a vector quantity. It is deined as the
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 informationWork, Energy and Momentum
Work, Energy and Moentu Work: When a body oves a distance d along straight line, while acted on by a constant force of agnitude F in the sae direction as the otion, the work done by the force is tered
More informationFREE BODY DIAGRAMS! For each of the layouts, draw the f.b.d.s for the bodies in the system. (The solutions follow--try each before looking!)! 3.)!
1.)! FREE BODY DIAGRAMS! For each of the layouts, draw the f.b.d.s for the bodies in the syste. (he solutions follow--try each before looking!)! 3.)!! 1.)! 3.)! 2.)! 4.)!! 2.)! 4.)! 1.) answer 3.) answer!
More informationMomentum. Conservation of Linear Momentum. Slide 1 / 140 Slide 2 / 140. Slide 3 / 140. Slide 4 / 140. Slide 6 / 140. Slide 5 / 140.
Slide 1 / 140 Slide 2 / 140 Moentu www.njctl.org Slide 3 / 140 Slide 4 / 140 Table of Contents Click on the topic to go to that section Conservation of Linear Moentu Ipulse - Moentu Equation Collisions
More informationThe total momentum in any closed system will remain constant.
The total momentum in any closed system will remain constant. When two or more objects collide, the collision does not change the total momentum of the two objects. Whatever momentum is lost by one object
More informationChapter 7 Lecture. Pearson Physics. Linear Momentum and Collisions. Prepared by Chris Chiaverina Pearson Education, Inc.
Chapter 7 Lecture Pearson Physics Linear Momentum and Collisions Prepared by Chris Chiaverina Chapter Contents Momentum Impulse Conservation of Momentum Collisions Momentum How can the effect of catching
More informationChapter 4 FORCES AND NEWTON S LAWS OF MOTION PREVIEW QUICK REFERENCE. Important Terms
Chapter 4 FORCES AND NEWTON S LAWS OF MOTION PREVIEW Dynaics is the study o the causes o otion, in particular, orces. A orce is a push or a pull. We arrange our knowledge o orces into three laws orulated
More informationChapter 1. Momentum. Fun and physics on screen
Chapter 1 Moentu Objectives e-learning Fun and physics on screen If you play coputer gaes (Figure 1.1) you will be failiar with the way in which characters ove about the screen. Cars accelerate and decelerate
More informationOne-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 information2009 Academic Challenge
009 Acadeic Challenge PHYSICS TEST - REGIONAL This Test Consists of 5 Questions Physics Test Production Tea Len Stor, Eastern Illinois University Author/Tea Leader Doug Brandt, Eastern Illinois University
More informationEXAM 3 REVIEW: hardest problems
PHYS 17: oern echanics Spring 011 xa 3 results: ultiple choice: 4.5/70 = 60.7% Hanwritten: XXX FINAL XA: 1. Coprehensie. About 0-5 ultiple choice questions only. If you hae Final xa conflict: 1. Notify
More informationIf there is now a constant air resistance force of 35 N, what is the new maximum height the ball attains?
A 1kg ball is launched straight up into the air with an initial speed of 64 m/s. Using only energy considerations, determine the maximum height the ball attains assuming there is no air resistance. If
More information