the static friction is replaced by kinetic friction. There is a net force F net = F push f k in the direction of F push.
|
|
- Georgia Barber
- 5 years ago
- Views:
Transcription
1 the static friction is replaced by kinetic friction. There is a net force F net = F push f k in the direction of F push. Exaple of kinetic friction. Force diagra for kinetic friction. Again, we find that f k N, or Figure 42: Kinetic friction. where µ k is the coefficient of kinetic friction. f k = µ k N, (4.29) Rolling friction f r : the frictional force that appears when an object rolls on a surface. As in equations (4.28) and (4.29), we find that f r N, or f r = µ r N, (4.30) which defines the coefficient of rolling friction, µ r. Typical values for various object/surface coefficients of the various frictional forces are shown in table 1. Notice, in particular, that µ k < µ s ; i.e. the kinetic frictional force is less than the axiu static friction. 65
2 Materials µ s µ k µ r Rubber/Concrete Steel/Steel (dry) Steel/Steel (lubricated) Wood/Wood Wood/Snow Ice/Ice Table 1: Typical friction coefficients. µ r µ k : i.e. it is easier to roll an object on wheels than to slide it. Figure shows how the frictional force changes as the applied horizontal force F push on an object increases. F push = 0 : object is at rest. F push < f s ax : static frictional force increases proportionally with F push. F push = f s ax : applied force is equal to the axiu static frictional force. The object slips, and begins to accelerate. The frictional force on it is now kinetic. F push > f s ax : object is oving. Kinetic frictional force reains constant Drag Force Recall that the drag force is a resistive force acting on an object due to its otion through a fluid. e.g. objects oving through air experience a drag force due to air resistance. 32 Knight, Figure 5.13, page
3 Figure 43: Variation in frictional force with F push. 67
4 Object Drag coefficient, C D Strealined body 1.00 Sports car 0.80 Typical car 0.10 Racing cyclist 0.50 Table 2: Typical drag coefficients in air. To quantify the drag force, D, we suppose that it is in soe way proportional to the following: the speed of the object, v s. the cross-sectional area of the object, A. the density of the fluid, ρ. Fro diensional analysis (see Additional Materials 33 ), we derive the for D = C D A vs 2 ρ (4.31) for D, where C D is the drag coefficient. Therefore, D depends upon the size and shape of the object, but not on its ass, as well as on the density of the fluid. Note: in general, C D is not constant it depends upon factors such as the object s speed and shape, roughness of the object s surface and viscosity of the fluid. Soe typical values of C D for objects in air are shown in table 2. Consider the otion of a ball being thrown vertically upwards (figure ). If D = 0 (i.e. no air resistance), a s = g throughout its flight. If D 0, a s changes. 33 Derivation of the Drag Force via Diensional Analysis, ne131/ 34 Knight, Figure 5.21, page
5 Figure 44: Vertical otion of a ball. (1) Ball rises with a net force (F net ) y = W + D y = g D acting on it, so by Newton s 2nd Law, its acceleration is a s = (F net) y = g D ( = g + D ) i.e. ball decelerates, and agnitude of this acceleration is > g. (2) Fro equation (4.31), D decreases as ball s speed decreases., (4.32) (3) At the axiu height of ball, its velocity v s = 0, so that D = 0, and ball s acceleration is siply a s = a free fall = g. (4) Fro equation (4.31), D increases as ball s speed increases. (5) Net force on ball is (F net ) y = W D y = g + D. By Newton s 2nd Law, its acceleration is a s = (F net) y = g + D ( = g D ). (4.33) Equations (4.32) and (4.33) show that since D is independent of the object s ass: 69
6 Upwards otion: less-assive objects subject to larger acceleration than ore-assive objects of sae size. Downwards otion: less-assive objects subject to saller acceleration than ore-assive objects of sae size. Galileo s experient: although haer > feather, the cross section of the feather is greater then that of the haer, and so the feather experiences a greater drag. Terinal speed Fro (4.31), D varies quadratically with v s. Furtherore, in the exaple shown in figure 44, we observe that the net vertical force on a falling object is (F net ) y = g + D (4.34) i.e. the weight and drag forces act in opposite directions. If the object falls far enough, the agnitude D will increase until it becoes equal to its weight. The net force (F net ) y in equation (4.34) will thus disappear: There will be no further acceleration of the object - it will reach a constant speed, and so by equation (4.31), D will also reain constant. This constant speed, at which D = g, is called the terinal speed v ter. Once the object reaches this terinal speed, it will continue falling until it reaches the ground. Using equation (4.31) in the condition D = g, i.e. C D A v 2 ter ρ = g, 70
7 yields the expression v ter = g C D Aρ (4.35) for v ter, i.e. V ter (thus, a ore assive object has a larger terinal speed than a less assive object). Consider the speed-tie graphs for free-fall otion with and without drag (figure 45); the effect of the forer can clearly be seen. Without drag. With drag Figure 45: Speed-tie graphs for free fall including and not including the drag force due to air resistance. Note: although the above refers to objects in free fall, D can also act to slow down objects oving horizontally in the sae way as those oving vertically. e.g. an airplane reaches a axiu speed when the drag force is equal and opposite to the thrust (e.g. for a passenger jet, this axiu speed is 550 ph) Relative Motion Recall our exaple involving the aircraft containing the following observers 71
8 Man fixed to Earth observes an airplane accelerating along the runway. Stewardess standing still in aircraft. Let us change the exaple such that The aircraft now oves along the runway such that its speedoeter reads a constant speed of 20 s 1 (i.e. inertial reference frae). The stewardess walks along the aisle, towards the cockpit, with a constant speed of 2 s 1 (i.e. inertial reference frae). Fixing a reference frae to both people, what does the an and stewardess see? Man: Observes airplane oving with a constant velocity of 20 s 1. Observes stewardess oving with a constant velocity of 22 s 1. Stewardess: Observes airplane oving with a constant speed of -2 s 1. Observes an oving with a constant speed of -22 s 1. So each person disagrees on what the speed of the airplane is. Which one is correct? Each observer s co-ordinate syste is an inertial frae - so both are correct. Each of the clais to be at rest - what they are really doing is reporting the relative otion of the aircraft, i.e. relative to their own reference frae. So how do we analyse the dynaics of an object in differing inertial fraes? 72
9 Let an object have position vectors r and r in inertial reference fraes S and S, respectively. Velocity of object in S and S are v and v, respectively. Frae S oves at a constant speed V with respect to frae S. It can be easily shown (see Additional Materials 35 ) that the velocities are related by v = v + V, v = v V. (4.36) Equation (4.36) constitute the Galilean Transforations (intuitively obvious?). Thus, if we know an object s velocity in one inertial frae, we can transfor it into the velocity easured by an observer in a different inertial frae. Exaple: 36 Police are chasing a bank robber. While driving at 50 s 1, they fire a bullet to shoot out a tire of his car. The police gun shoots bullets at 300 s 1. What is the bullet s speed relative to a TV caera crew parked beside the road? Solution: confining all otion to 1-diension, let frae S be fixed to the TV crew, and frae S fixed to the police car. We therefore have the following inforation: v x = 300 s 1, V x = 50 s 1. Using the x-coponent equation of (4.36), the speed v x of the bullet in the TV crew s frae is v x = v x + V x = = 350 s The Galilean Transforations, ne131/ 36 Knight, Exaple 6.8, page
Chapter 5, Conceptual Questions
Chapter 5, Conceptual Questions 5.1. Two forces are present, tension T in the cable and gravitational force 5.. F G as seen in the figure. Four forces act on the block: the push of the spring F, sp gravitational
More informationFor a situation involving gravity near earth s surface, a = g = jg. Show. that for that case v 2 = v 0 2 g(y y 0 ).
Reading: Energy 1, 2. Key concepts: Scalar products, work, kinetic energy, work-energy theore; potential energy, total energy, conservation of echanical energy, equilibriu and turning points. 1.! In 1-D
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 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 informationNAME NUMBER SEC. PHYCS 101 SUMMER 2001/2002 FINAL EXAME:24/8/2002. PART(I) 25% PART(II) 15% PART(III)/Lab 8% ( ) 2 Q2 Q3 Total 40%
NAME NUMER SEC. PHYCS 101 SUMMER 2001/2002 FINAL EXAME:24/8/2002 PART(I) 25% PART(II) 15% PART(III)/Lab 8% ( ) 2.5 Q1 ( ) 2 Q2 Q3 Total 40% Use the followings: Magnitude of acceleration due to gravity
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 informationTactics Box 2.1 Interpreting Position-versus-Time Graphs
1D kineatic Retake Assignent Due: 4:32p on Friday, October 31, 2014 You will receive no credit for ites you coplete after the assignent is due. Grading Policy Tactics Box 2.1 Interpreting Position-versus-Tie
More informationFor more Study Material and Latest Questions related to IIT-JEE visit
or ore Study Material and Latest Questions related to IIT-JEE visit www. ICTION Introduction If we slide or try to slide a body over a surface, the otion is resisted by a bonding between the body and the
More informationy scalar component x scalar component A. 770 m 250 m file://c:\users\joe\desktop\physics 2A\PLC Assignments - F10\2a_PLC7\index.
Page 1 of 6 1. A certain string just breaks when it is under 400 N of tension. A boy uses this string to whirl a 10-kg stone in a horizontal circle of radius 10. The boy continuously increases the speed
More informationSystems of Masses. 1. Ignoring friction, calculate the acceleration of the system below and the tension in the rope. and (4.0)(9.80) 39.
Systes of Masses. Ignoring friction, calculate the acceleration of the syste below and the tension in the rope. Drawing individual free body diagras we get 4.0kg 7.0kg g 9.80 / s a?? g and g (4.0)(9.80)
More information8.1 Force Laws Hooke s Law
8.1 Force Laws There are forces that don't change appreciably fro one instant to another, which we refer to as constant in tie, and forces that don't change appreciably fro one point to another, which
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 informationChapter 6 Dynamics I: Motion Along a Line
Chapter 6 Dynamics I: Motion Along a Line Chapter Goal: To learn how to solve linear force-and-motion problems. Slide 6-2 Chapter 6 Preview Slide 6-3 Chapter 6 Preview Slide 6-4 Chapter 6 Preview Slide
More informationFriction. Objectives. Assessment. Assessment. Physics terms. Equations 5/20/14. Models for friction
Objectives Friction Calculate friction forces from equation models for static, kinetic, and rolling friction. Solve one-dimensional force problems that include friction. 1. A box with a mass of 10 kg is
More informationParticle dynamics Physics 1A, UNSW
1 Particle dynaics Physics 1A, UNSW Newton's laws: S & J: Ch 5.1 5.9, 6.1 force, ass, acceleration also weight Physclips Chapter 5 Friction - coefficients of friction Physclips Chapter 6 Hooke's Law Dynaics
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 informationPreClass Notes: Chapter 5, Sections 5.4,5.5
PreClass Notes: Chapter 5, Sections 5.4,5.5 From Essential University Physics 3 rd Edition by Richard Wolfson, Middlebury College 2016 by Pearson Education, Inc. Narration and extra little notes by Jason
More information2.003 Engineering Dynamics Problem Set 2 Solutions
.003 Engineering Dynaics Proble Set Solutions This proble set is priarily eant to give the student practice in describing otion. This is the subject of kineatics. It is strongly recoended that you study
More informationTUTORIAL 1 SIMPLE HARMONIC MOTION. Instructor: Kazumi Tolich
TUTORIAL 1 SIMPLE HARMONIC MOTION Instructor: Kazui Tolich About tutorials 2 Tutorials are conceptual exercises that should be worked on in groups. Each slide will consist of a series of questions that
More informationQ5 We know that a mass at the end of a spring when displaced will perform simple m harmonic oscillations with a period given by T = 2!
Chapter 4.1 Q1 n oscillation is any otion in which the displaceent of a particle fro a fixed point keeps changing direction and there is a periodicity in the otion i.e. the otion repeats in soe way. In
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 informationName Class Date. two objects depends on the masses of the objects.
CHAPTER 12 2 Gravity SECTION Forces KEY IDEAS As you read this section keep these questions in ind: What is free fall? How are weight and ass related? How does gravity affect the otion of objects? What
More informationUNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics
UNIVERSITY OF SASKATCHEWAN Departent of Physics and Engineering Physics Physics 115.3 MIDTERM TEST October 22, 2008 Tie: 90 inutes NAME: (Last) Please Print (Given) STUDENT NO.: LECTURE SECTION (please
More informationName Period. What force did your partner s exert on yours? Write your answer in the blank below:
Nae Period Lesson 7: Newton s Third Law and Passive Forces 7.1 Experient: Newton s 3 rd Law Forces of Interaction (a) Tea up with a partner to hook two spring scales together to perfor the next experient:
More information15 Newton s Laws #2: Kinds of Forces, Creating Free Body Diagrams
Chapter 15 ewton s Laws #2: inds of s, Creating ree Body Diagras 15 ewton s Laws #2: inds of s, Creating ree Body Diagras re is no force of otion acting on an object. Once you have the force or forces
More informationDefinition of Work, The basics
Physics 07 Lecture 16 Lecture 16 Chapter 11 (Work) v Eploy conservative and non-conservative forces v Relate force to potential energy v Use the concept of power (i.e., energy per tie) Chapter 1 v Define
More informationacceleration of 2.4 m/s. (b) Now, we have two rubber bands (force 2F) pulling two glued objects (mass 2m). Using F ma, 2.0 furlongs x 2.0 s 2 4.
5.. 5.6. Model: An object s acceleration is linearl proportional to the net force. Solve: (a) One rubber band produces a force F, two rubber bands produce a force F, and so on. Because F a and two rubber
More informationLecture #8-3 Oscillations, Simple Harmonic Motion
Lecture #8-3 Oscillations Siple Haronic Motion So far we have considered two basic types of otion: translation and rotation. But these are not the only two types of otion we can observe in every day life.
More informationma x = -bv x + F rod.
Notes on Dynaical Systes Dynaics is the study of change. The priary ingredients of a dynaical syste are its state and its rule of change (also soeties called the dynaic). Dynaical systes can be continuous
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 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 informationUniversity Physics (Prof. David Flory) Chapt_06 Saturday, October 06, 2007 Page 1
University Physics (Prof. David Flory) Chapt_06 Saturday, October 06, 2007 Page 1 Name: Date: 1. A crate resting on a rough horizontal floor is to be moved horizontally. The coefficient of static friction
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 information2. What two units of measurement are necessary for describing speed? Ans. Distance and time.
Conceptual Physics-9 th edition Answers by R. E. Treblay Ch. 3 Pg.51 Review questions. What two units of easureent are necessary for describing speed? Ans. Distance and tie. 3. What kind of speed is registered
More informationm potential kinetic forms of energy.
Spring, Chapter : A. near the surface of the earth. The forces of gravity and an ideal spring are conservative forces. With only the forces of an ideal spring and gravity acting on a ass, energy F F will
More information4.2. Visualize: Assess: Note that the climber does not touch the sides of the crevasse so there are no forces from the crevasse walls.
4.1. Solve: A force is basically a push or a pull on an object. There are five basic characteristics of forces. (i) A force has an agent that is the direct and immediate source of the push or pull. (ii)
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 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 information1 k. 1 m. m A. AP Physics Multiple Choice Practice Work-Energy
AP Physics Multiple Choice Practice Wor-Energy 1. A ass attached to a horizontal assless spring with spring constant, is set into siple haronic otion. Its axiu displaceent fro its equilibriu position 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 informationU V. r In Uniform Field the Potential Difference is V Ed
SPHI/W nit 7.8 Electric Potential Page of 5 Notes Physics Tool box Electric Potential Energy the electric potential energy stored in a syste k of two charges and is E r k Coulobs Constant is N C 9 9. E
More informationQuestion 1. [14 Marks]
6 Question 1. [14 Marks] R r T! A string is attached to the dru (radius r) of a spool (radius R) as shown in side and end views here. (A spool is device for storing string, thread etc.) A tension T is
More information2. Which of the following best describes the relationship between force and potential energy?
Work/Energy with Calculus 1. An object oves according to the function x = t 5/ where x is the distance traveled and t is the tie. Its kinetic energy is proportional to (A) t (B) t 5/ (C) t 3 (D) t 3/ (E)
More informationChapter 11 Simple Harmonic Motion
Chapter 11 Siple Haronic Motion "We are to adit no ore causes of natural things than such as are both true and sufficient to explain their appearances." Isaac Newton 11.1 Introduction to Periodic Motion
More informationPage 1. Name: Section This assignment is due at the first class in 2019 Part I Show all work!
Name: Section This assignment is due at the first class in 2019 Part I Show all work! 7164-1 - Page 1 1) A car travels at constant speed around a section of horizontal, circular track. On the diagram provided
More informationApplying Newton s Laws
Applying Newton s Laws Free Body Diagrams Draw and label the forces acting on the object. Examples of forces: weight, normal force, air resistance, friction, applied forces (like a push or pull) Velocity
More informationSection /07/2013. PHY131H1F University of Toronto Class 9 Preclass Video by Jason Harlow. Based on Knight 3 rd edition Ch. 5, pgs.
PHY131H1F University of Toronto Class 9 Preclass Video by Jason Harlow Based on Knight 3 rd edition Ch. 5, pgs. 116-133 Section 5.1 A force is a push or a pull What is a force? What is a force? A force
More informationPhysics 6A TR Section Winter 2012 Midterm
Physics 6A TR Section Winter 2012 Midterm The test consists of 19 multiple choice questions. Enter the answer to the multiple choice questions in the pink scantron sheet. Use a pencil, not a pen. There
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 informationL 2. AP Physics Free Response Practice Oscillations ANSWERS 1975B7. (a) F T2. (b) F NET(Y) = 0
AP Physics Free Response Practice Oscillations ANSWERS 1975B7. (a) 60 F 1 F g (b) F NE(Y) = 0 F1 F1 = g / cos(60) = g (c) When the string is cut it swings fro top to botto, siilar to the diagra for 1974B1
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 informationExperiment 2: Hooke s Law
COMSATS Institute of Inforation Technology, Islaabad Capus PHYS-108 Experient 2: Hooke s Law Hooke s Law is a physical principle that states that a spring stretched (extended) or copressed by soe distance
More information66 Chapter 6: FORCE AND MOTION II
Chapter 6: FORCE AND MOTION II 1 A brick slides on a horizontal surface Which of the following will increase the magnitude of the frictional force on it? A Putting a second brick on top B Decreasing the
More information= 1.49 m/s m. 2 kg. 2 kg
5.6. Visualize: Please refer to Figure Ex5.6. Solve: For the diagra on the left, three of the vectors lie along the axes of the tilted coordinate sste. Notice that the angle between the 3 N force and the
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 informationPhysics Dynamics: Forces. Science and Mathematics Education Research Group
F FA ACULTY C U L T Y OF O F EDUCATION E D U C A T I O N Departent of Curriculu and Pedagogy Physics Dynaics: Forces Science and Matheatics Education Research Group Supported by UBC Teaching and Learning
More informationAP Physics C: Mechanics Practice (Newton s Laws including friction, resistive forces, and centripetal force).
AP Physics C: Mechanics Practice (Newton s Laws including friction, resistive forces, and centripetal force). 1981M1. A block of mass m, acted on by a force of magnitude F directed horizontally to the
More informationForces and Motion in One Dimension
Nicholas J. Giordano www.cengage.com/physics/giordano Forces and Motion in One Dimension Applications of Newton s Laws We will learn how Newton s Laws apply in various situations We will begin with motion
More informationWhat changes in space as opposed to being on the Earth? How does this affect mass? Is the car is in equilibrium? Where will the forces act?
Quest Chapter 05 1 How would your mass change if you took a trip to the space station? 1. decreases; you weigh less. 2. increases; you weigh more. 3. no change in mass 2 (part 1 of 3) You are driving a
More informationAppendix- B POST-TEST QUESTION PAPER BASED ON PROGRAMMED INSTRUCTION (LINEAR PROGRAMME) OF IX STANDARD PHYSICAL SCIENCE
Appendix- B POST-TEST QUESTION PAPER BASED ON PROGRAMMED INSTRUCTION (LINEAR PROGRAMME) OF IX STANDARD PHYSICAL SCIENCE 1. To change a state of rest or to stop the motion of a body we apply a) 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 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 information1. Type your first name. * 2. Type your last name. * 3. Choose the block I teach you for science. * Mark only one oval. Block 1.
Hippenmeyer Physics Assessment 1 Your email address (khippenmeyer@ncmcs.net) will be recorded when you submit this form. Not khippenmeyer? Sign out * Required 1. Type your first name. * 2. Type your last
More informationPHYSICS. Chapter 5 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 5 Lecture RANDALL D. KNIGHT Chapter 5 Force and Motion IN THIS CHAPTER, you will learn about the connection between force and motion.
More informationChapter 5 Force and Motion
Chapter 5 Force and Motion Chapter Goal: To establish a connection between force and motion. Slide 5-2 Chapter 5 Preview Slide 5-3 Chapter 5 Preview Slide 5-4 Chapter 5 Preview Slide 5-5 Chapter 5 Preview
More informationNEWTON S LAWS OF MOTION
NAME SCHOOL INDEX NUMBER DATE NEWTON S LAWS OF MOTION 1. 1995 Q21 P1 State Newton s first law of motion (1 mark) 2. 1998 Q22 P1 A body of mass M is allowed to slide down an inclined plane. State two factors
More information3. The diagram shows two bowling balls, A and B, each having a mass of 7.00 kilograms, placed 2.00 meters apart.
1. Which statement describes the gravitational force and the electrostatic force between two charged particles? A) The gravitational force may be either attractive or repulsive, whereas the electrostatic
More informationSir Isaac Newton. Newton s Laws of Motion. Mass. First Law of Motion. Weight. Weight
Sir Isaac Newton Newton s Laws of Motion Suppleental Textbook Material Pages 300-320 Born 1642 1665 began individual studies Proved universal gravitation Invented the Calculus Reflector telescope 1672
More informationThe accelerated expansion of the universe is explained by quantum field theory.
The accelerated expansion of the universe is explained by quantu field theory. Abstract. Forulas describing interactions, in fact, use the liiting speed of inforation transfer, and not the speed of light.
More information7. Two forces are applied to a 2.0-kilogram block on a frictionless horizontal surface, as shown in the diagram below.
1. Which statement about the movement of an object with zero acceleration is true? The object must be at rest. The object must be slowing down. The object may be speeding up. The object may be in motion.
More informationLesson 24: Newton's Second Law (Motion)
Lesson 24: Newton's Second Law (Motion) To really appreciate Newton s Laws, it soeties helps to see how they build on each other. The First Law describes what will happen if there is no net force. The
More informationPHYS 101 Previous Exam Problems. Force & Motion I
PHYS 101 Previous Exam Problems CHAPTER 5 Force & Motion I Newton s Laws Vertical motion Horizontal motion Mixed forces Contact forces Inclines General problems 1. A 5.0-kg block is lowered with a downward
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 informationChapter 4. Forces and Newton s Laws of Motion
Chapter 4 Forces and Newton s Laws of Motion Chapter 4: Forces and Newton s Laws Force, mass and Newton s three laws of motion Newton s law of gravity Normal, friction and tension forces Apparent weight,
More informationLecture Presentation. Chapter 4 Forces and Newton s Laws of Motion. Chapter 4 Forces and Newton s Laws of Motion. Reading Question 4.
Chapter 4 Forces and Newton s Laws of Motion Lecture Presentation Chapter 4 Forces and Newton s Laws of Motion Chapter Goal: To establish a connection between force and motion. Slide 4-2 Chapter 4 Preview
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 informationPHYS 1114, Lecture 10, February 8 Contents:
PHYS 1114, Lecture 10, February 8 Contents: 1 Example of projectile motion: Man shooting a gun firing a bullet horizontally. 2 Example of projectile motion: Man shooting an arrow at a monkey in a tree.
More informationForce - a push or a pull A force described by its strength and by the direction in which it acts The SI unit for force is the newton (N)
Forces Force - a push or a pull A force described by its strength and by the direction in which it acts The SI unit for force is the newton (N) The direction and strength of forces can be represented by
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 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 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 informationName Class Date. What are the four fundamental forces in nature? How can forces affect the motion of an object? Why is friction sometime necessary?
CHAPTER 11 SECTION Motion 3 Motion and Force KEY IDEAS As you read this section, keep these questions in mind: What are the four fundamental forces in nature? How can forces affect the motion of an object?
More information1. A baseball player throws a ball horizontally. Which statement best describes the ball's motion after it is thrown? [Neglect the effect of
1. A baseball player throws a ball horizontally. Which statement best describes the ball's motion after it is thrown? [Neglect the effect of friction.] A) Its vertical speed remains the same, and its horizontal
More informationPhysically Based Modeling CS Notes Spring 1997 Particle Collision and Contact
Physically Based Modeling CS 15-863 Notes Spring 1997 Particle Collision and Contact 1 Collisions with Springs Suppose we wanted to ipleent a particle siulator with a floor : a solid horizontal plane which
More informationChapter 10 Atmospheric Forces & Winds
Chapter 10 Atospheric Forces & Winds Chapter overview: Atospheric Pressure o Horizontal pressure variations o Station vs sea level pressure Winds and weather aps Newton s 2 nd Law Horizontal Forces o Pressure
More informationBasic concept of dynamics 3 (Dynamics of a rigid body)
Vehicle Dynaics (Lecture 3-3) Basic concept of dynaics 3 (Dynaics of a rigid body) Oct. 1, 2015 김성수 Vehicle Dynaics Model q How to describe vehicle otion? Need Reference fraes and Coordinate systes 2 Equations
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 informationHonors Lab 4.5 Freefall, Apparent Weight, and Friction
Nae School Date Honors Lab 4.5 Freefall, Apparent Weight, and Friction Purpose To investigate the vector nature of forces To practice the use free-body diagras (FBDs) To learn to apply Newton s Second
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 informationROTATIONAL MOTION FROM TRANSLATIONAL MOTION
ROTATIONAL MOTION FROM TRANSLATIONAL MOTION Velocity Acceleration 1-D otion 3-D otion Linear oentu TO We have shown that, the translational otion of a acroscopic object is equivalent to the translational
More informationPhysics-MC Page 1 of 29 Inertia, Force and Motion 1.
Physics-MC 2006-7 Page 1 of 29 Inertia, Force and Motion 1. 3. 2. Three blocks of equal mass are placed on a smooth horizontal surface as shown in the figure above. A constant force F is applied to block
More informationAnnouncement. Grader s name: Qian Qi. Office number: Phys Office hours: Thursday 4:00-5:00pm in Room 134
Lecture 3 1 Announceent Grader s nae: Qian Qi Office nuber: Phys. 134 -ail: qiang@purdue.edu Office hours: Thursday 4:00-5:00p in Roo 134 2 Millikan s oil Drop xperient Consider an air gap capacitor which
More informationChapter 05 Test A. Name: Class: Date: Multiple Choice Identify the choice that best completes the statement or answers the question.
Class: Date: Chapter 05 Test A Multiple Choice Identify the choice that best completes the statement or answers the question. 1. The SI unit of force preferred by scientists is the: a. kilogram. b. newton.
More informationForce and Motion Easy to read Version. Junior Science
Force and Motion Easy to read Version Junior Science 1 1a The different types of motion Objects that move from one point of space to another over time are said to have motion. Examples include a tortoise
More informationTutorial Exercises: Incorporating constraints
Tutorial Exercises: Incorporating constraints 1. A siple pendulu of length l ass is suspended fro a pivot of ass M that is free to slide on a frictionless wire frae in the shape of a parabola y = ax. The
More informationPhysics 221, January 24
Key Concepts: Newton s 1 st law Newton s 2 nd law Weight Newton s 3 rd law Physics 221, January 24 Please find a seat. Keep all walkways free for safety reasons and to comply with the fire code. Matter
More informationHSC PHYSICS ONLINE B F BA. repulsion between two negatively charged objects. attraction between a negative charge and a positive charge
HSC PHYSICS ONLINE DYNAMICS TYPES O ORCES Electrostatic force (force mediated by a field - long range: action at a distance) the attractive or repulsion between two stationary charged objects. AB A B BA
More informationNB1140: Physics 1A - Classical mechanics and Thermodynamics Problem set 2 - Forces and energy Week 2: November 2016
NB1140: Physics 1A - Classical echanics and Therodynaics Proble set 2 - Forces and energy Week 2: 21-25 Noveber 2016 Proble 1. Why force is transitted uniforly through a assless string, a assless spring,
More information12/06/2010. Chapter 2 Describing Motion: Kinematics in One Dimension. 2-1 Reference Frames and Displacement. 2-1 Reference Frames and Displacement
Chapter 2 Describing Motion: Kinematics in One Dimension 2-1 Reference Frames and Displacement Any measurement of position, distance, or speed must be made with respect to a reference frame. For example,
More informationReview 3: Forces. 1. Which graph best represents the motion of an object in equilibrium? A) B) C) D)
1. Which graph best represents the motion of an object in equilibrium? A) B) C) D) 2. A rock is thrown straight up into the air. At the highest point of the rock's path, the magnitude of the net force
More information