Lecture 08 Conservation of Energy

Size: px
Start display at page:

Download "Lecture 08 Conservation of Energy"

Transcription

1 Lecture 8 Conservation o Enery 8. The Nonisolated System: Conservation o Enery wor, mechanical waves, heat (drivin by a temperature dierence), matter transer (convection), electrical transmission (by means o electric currents), electromanetic radiation (photons) Conservation o Enery Equation: K U E W Q T T int MW MT T ET T ER What is the enery o a visible photon? (ev =? Joule) We can neither create nor destroy enery enery is always conserved. wor-inetic enery valid only when the object can be modeled as a particle i a rictional orce ests, how to express the wor with it? What s the dierence between inetic riction and resistive orce? I no external wor applied to the system, the loss o inetic enery will transer to wor done by the inetic riction orce. i K x dx I external orce est, the system may ain enery rom the external wor and loss enery to the inetic riction orce. K W x vi v vi dx v W = Fdx We said in previous section that no enery can be created or destroyed. the wor done by the inetic riction orce o? -> Internal Enery Where does E system K Eint E int d Nonisolated system dx isolated system The result o a riction orce is to transer inetic enery into internal enery.

2 Frictional orce -> Resistive orce -> Dra orce?? Example: A car travelin at a speed v slides a distance d to a halt ater its brae loc. Assumin that the car s initial speed is instead v at the moment the braes loc, estimate the distance it slides. 4d Example: A bloc o mass.6 is attached to a horizontal sprint that has a orce constant o. X 3 N/m. rom rest. The sprin is compressed. cm and is then released Calculate the speed o the bloc as it passes throuh the equilibrium position i a constant riction orce o 4. N retards its motion rom the moment it is released. W V x d 8. The Isolated System the wor done by the ravitational orce: W m zy yi zˆ myi my ˆ, y yi v yi y transorm to mechanical enery o the object W K my i my notice the minus sin W U wor is only intermediate substitutable quantity to express the enery transer W K -> K U inetic enery and potential enery o an object U in the system Deine Mechanical Enery: E, Emech K U mech I K U -> K K U U -> Ki U i K U i i -> i myi my system -> conservation o mechanical enery or an isolated

3 This result is called the principle o conservation o mechanical enery. (Now you can see where conservative orces ot their name.) We can write this principle in one more orm, as E K U mech Example: A child o mass m is released rom rest at the top o a water slide, at heiht h = 8.5 m above the bottom o the slide. Assumin that the slide is rictionless because o the water on it, ind the child's speed at the bottom o the slide. v h m/s Example: Ball in Free Fall m h y Example: The Pendulum ml B ml cos A Example: Two blocs are connected by a massless cord that passes over two rictionless pulleys, as in Fiure. One end o the cord is attached to an object o mass m=3. that is a distance R=.m rom the pulley on the let. The other end o the cord is connected to a bloc o mass m=6 restin on a table. From what anle must the 3. mass be released in order to just lit the 6. bloc o the table? Enery conservation: R( v cos ), mh, v Force balance: m m m, R 3

4 m m m ( cos ), 3m m cos m Elastic Potential Enery, U W x F x Fapp dx x E mech U K x, i the enery is conserved in the isolated system, E mech U K -> i x i x Example: A bead slides without riction around a loopthe-loop. The bead is released rom a heiht h = 3.5R. (a) What is its speed at point A? (b) How lare is the normal orce on it i its mass is 5.? Hint: (a) Transer potential enery to inetic enery, (b) calculate the centripetal orce that the wall exerted on the particle, the orce that the particle exert on the wall may need to subtract the ravitational term (a) v 3R (b) m normal orce is rom the plane in downward direction See AF68 & AF86. Gravitational potential enery: W x F x dx U U U U x y yi m F x dx y mdy m yi dy y y my y my yi i 4

5 elastic potential enery: U U x F x xdx xdx xdx x x x x i x The total enery E o a system can chane only by amounts o enery that are transerred to or rom the system. The Wor-Enery Theorem (compared with the wor-inetic enery theorem) W E E E mech mech K U E th E int isolated system -> W E 8.3 Situations Involvin Kinetic Friction 8.4 Chanes in Mechanical Enery or Nonconservative Forces No Friction Involved: W Emech K U Friction Involved:. Consider the inetic enery only: K d. Consider the mechanical enery: E K U d Derived rom the orce law: F ma, v v ad, Fd d By doin experiment, we ound that the bloc and the portion o the loor alon which it slides become warmer as the bloc slides E d th W Fd E E th Example: A ood shipper pushes a wood crate o cabbae heads (total mass m = 4 5

6 ) across a concrete loor with a constant horizontal orce F o manitude 4 N. In a straiht-line displacement o manitude d =.5 m, the speed o the crate decreases rom v =.6 m/s to v =. m/s. (a) How much wor is done by orce F, and on what system does it do the wor? W 4.5 J (b) What is the increase Eth in the thermal enery o the crate and loor? E th W K J J Example: A child o mass m rides on an irreularly curved slide o heiht h =. m. The child starts at rest on the top. (a) Determine his speed at the bottom, assumin no riction is present. v h (b) I a orce o inetic riction acts on the child, how much mechanical enery does the system lose? Assume that v = 3. m/s and m =.. E mh mech mh.3. 3J Example: Two blocs are connected by a liht strin. The bloc o mass m is connected to a sprin o orce constant. The system is released rom rest when the sprin is unstreched. I the bloc o mass m alls a distance o h beore comin to rest, calculate the coeicient o inetic riction between the bloc o mass m and the surace. Hint: Potential enery is provided to stretch the sprin and to the loss o inetic riction. Overdamped system? mh h m h 6

7 Example: A. pacae o tamale slides alon a loor with speed v = 4. m/s. It then runs into and compresses a sprin, until the pacae momentarily stops. Its path to the initially relaxed sprin is rictionless, but as it compresses the sprin, a inetic rictional orce rom the loor, o manitude 5 N, acts on it. The sprin constant is, N/m. By what distance d is the sprin compressed when the pacae stops? 5 d 5 d 6, 5d 5d 6, 5 d Systems With Chemical Enery Example: You are drivin a - asoline-powered car at a constant speed o m/h (7.8 m/s) up a -percent rade. (a) I the eiciency is 5 percent, what is the rate at which the chemical enery o the car-earth-atmosphere system chanes? tan %. t E chem h.5 m mvsin ~ mv tan t de 9.8 chem W dt.5 Mass and Enery In 95, Albert Einstein published his special theory o relativity, a result o which is the amous equation E mc. A particle or system o mass m has rest enery mc. The enery is intrinsic to the particle. Enery in atomic and nuclear physics are usually expressed in units o electron volts (ev). A convenient unit or the masses o atomic particles is ev/c. Particle Symbol Rest Enery (MeV) Electron e -.5 Positron e +.5 Proton p Neutron n

8 Deuteron d Triton t 88.4 Helium-4 (alpha particle) 4 He The increase in mass with an increase in enery o 4 J is E 4 7 m c 3 Nuclear Enery Example: A typical nuclear usion reaction is written H+ 3 H-> 4 He+n. enery is released in this usion reaction? ~ 7. MeV How much Newtonian Mechanics and Relativity K v c E v c mc v K E : rest mass enery c E Newtonian mechanics is valid o the speed o the particle is much less than the speed o liht. Quantization o Enery 34 Plan s constant: h 6.66 J s The quantized enery o an oscillator: E n n h round state enery E En h h The quantized enery o a photon: electromanetic radiation. E photon h, is the requency o the For macroscopic bound system, the oscillation requencies or a sprin system are about to Hz. I, the spacin between allowed levels is 33 h ~ 6 J. The enery o a macroscopic system is in the order o J. The enery level spacin is too small to be observable. Example: For a diatomic molecule, a typical requency o vibration is 4, and a typical enery o -9 J. The spacin between allowed levels is then E 6 E ev.6 n En h 6 J, ~

9 Since the enery o molecule is in the order o ev, the enery spacin is not neliible. At let is a hydroen spectral tube excited by a 5 volt transormer. The three prominent hydroen lines are shown at the riht o the imae throuh a 6 lines/mm diraction ratin. An appromate classiication o spectral colors: Violet (38-435nm) Blue(435-5 nm) Cyan (5-5 nm) Green (5-565 nm) Yellow ( nm) Orane (59-65 nm) Red (65-74 nm) 8.5 Power de P dt P dw dt d dt F r F v 3 _ Watt _ J / s _ m / s _ hp 746 _W _ Wh 5 _ W _ h _ W 36 _ s 3.6 _ J 9

P6.5 (a) static friction. v r. = r ( 30.0 cm )( 980 cm s ) P6.15 Let the tension at the lowest point be T.

P6.5 (a) static friction. v r. = r ( 30.0 cm )( 980 cm s ) P6.15 Let the tension at the lowest point be T. Q65 The speed chanes The tanential orce component causes tanential acceleration Q69 I would not accept that statement or two reasons First, to be beyond the pull o raity, one would hae to be ininitely

More information

Work Up an Incline. Work = Force x Distance. Push up: 1500J. What is the PE at the top? mg = 500N. An incline is a simple machine!

Work Up an Incline. Work = Force x Distance. Push up: 1500J. What is the PE at the top? mg = 500N. An incline is a simple machine! Quick Question Work Up an Incline The block o ice weighs 500 Newtons. How much work does it take to push it up the incline compared to liting it straight up? Ignore riction. Work Up an Incline Work = Force

More information

There are two types of forces: conservative (gravity, spring force) nonconservative (friction)

There are two types of forces: conservative (gravity, spring force) nonconservative (friction) Chapter 8: Conservation o Energy There are two types o orces: conservative (gravity, spring orce) nonconservative (riction) Conservative Forces Conservative Force the work done by the orce on an object

More information

Chapter 07: Kinetic Energy and Work

Chapter 07: Kinetic Energy and Work Chapter 07: Kinetic Energy and Work Like other undamental concepts, energy is harder to deine in words than in equations. It is closely linked to the concept o orce. Conservation o Energy is one o Nature

More information

Ground Rules. PC1221 Fundamentals of Physics I. Introduction to Energy. Energy Approach to Problems. Lectures 13 and 14. Energy and Energy Transfer

Ground Rules. PC1221 Fundamentals of Physics I. Introduction to Energy. Energy Approach to Problems. Lectures 13 and 14. Energy and Energy Transfer PC1221 Fundamentals o Physics I Lectures 13 and 14 Energy and Energy Transer Dr Tay Seng Chuan 1 Ground Rules Switch o your handphone and pager Switch o your laptop computer and keep it No talking while

More information

Ground Rules. PC1221 Fundamentals of Physics I. Introduction to Energy. Energy Approach to Problems. Lectures 13 and 14. Energy and Energy Transfer

Ground Rules. PC1221 Fundamentals of Physics I. Introduction to Energy. Energy Approach to Problems. Lectures 13 and 14. Energy and Energy Transfer PC11 Fundamentals o Physics I Lectures 13 and 14 Energy and Energy Transer A/Pro Tay Seng Chuan 1 Ground Rules Switch o your handphone and pager Switch o your laptop computer and keep it No talking while

More information

Exam 2A Solution. 1. A baseball is thrown vertically upward and feels no air resistance. As it is rising

Exam 2A Solution. 1. A baseball is thrown vertically upward and feels no air resistance. As it is rising Exam 2A Solution 1. A baseball is thrown vertically upward and feels no air resistance. As it is risin Solution: Possible answers: A) both its momentum and its mechanical enery are conserved - incorrect.

More information

Chapter 8. Conservation of Energy

Chapter 8. Conservation of Energy Chapter 8 Conservation of Energy Energy Review Kinetic Energy Associated with movement of members of a system Potential Energy Determined by the configuration of the system Gravitational and Elastic Potential

More information

Conservation of Mechanical Energy 8.01

Conservation of Mechanical Energy 8.01 Conservation o Mechanical Energy 8.01 Non-Conservative Forces Work done on the object by the orce depends on the path taken by the object Example: riction on an object moving on a level surace F riction

More information

Ground Rules. PC1221 Fundamentals of Physics I. Lectures 13 and 14. Energy and Energy Transfer. Dr Tay Seng Chuan

Ground Rules. PC1221 Fundamentals of Physics I. Lectures 13 and 14. Energy and Energy Transfer. Dr Tay Seng Chuan PC1221 Fundamentals o Physics I Lectures 13 and 14 Energy and Energy Transer Dr Tay Seng Chuan 1 Ground Rules Switch o your handphone and pager Switch o your laptop computer and keep it No talking while

More information

g L Simple Pendulum, cont Simple Pendulum Period of Simple Pendulum Equations of Motion for SHM: 4/8/16 k m

g L Simple Pendulum, cont Simple Pendulum Period of Simple Pendulum Equations of Motion for SHM: 4/8/16 k m Simple Pendulum The simple pendulum is another example of simple harmonic motion The force is the component of the weiht tanent to the path of motion F t = - m sin θ Simple Pendulum, cont In eneral, the

More information

Physics 111. Lecture 18 (Walker: 8.3-4) Energy Conservation I March 11, Conservation of Mechanical Energy

Physics 111. Lecture 18 (Walker: 8.3-4) Energy Conservation I March 11, Conservation of Mechanical Energy Physics 111 Lecture 18 (Walker: 8.3-4) Energy Conservation I March 11, 2009 Lecture 18 1/24 Conservation o Mechanical Energy Deinition o mechanical energy: (8-6) I the only work done in going rom the initial

More information

Slide. King Saud University College of Science Physics & Astronomy Dept.

Slide. King Saud University College of Science Physics & Astronomy Dept. Slide King Saud University College of Science Physics & Astronomy Dept. PHYS 103 (GENERAL PHYSICS) CHAPTER 7: ENERGY AND ENERGY TRANSFER LECTURE NO. 11 THIS PRESENTATION HAS BEEN PREPARED BY: DR. NASSR

More information

Newton's laws of motion

Newton's laws of motion Episode No - 5 Date: 03-04-2017 Faculty: Sunil Deshpande Newton's laws of motion * A plank with a box on it at one end is slowly raised about the other end. As the anle with the horizontal slowly reaches

More information

Get the frictional force from the normal force. Use dynamics to get the normal force.

Get the frictional force from the normal force. Use dynamics to get the normal force. . L F n µ k L =00 t µ k = 0.60 = 0 o = 050 lb F n +y +x x = sin y = cos = µf n Is the initial elocity o the car reater than 30 mph? Approach: Use conseration o enery. System: car Initial time: beore you

More information

WORK, ENERGY & POWER Work scalar W = F S Cosθ Unit of work in SI system Work done by a constant force

WORK, ENERGY & POWER Work scalar W = F S Cosθ Unit of work in SI system Work done by a constant force WORK, ENERGY & POWER Work Let a force be applied on a body so that the body gets displaced. Then work is said to be done. So work is said to be done if the point of application of force gets displaced.

More information

SECTION A Torque and Statics

SECTION A Torque and Statics AP Physics C Multiple Choice Practice Rotation SECTON A Torque and Statics 1. A square piece o plywood on a horizontal tabletop is subjected to the two horizontal orces shown above. Where should a third

More information

Physics 121k Exam 3 7 Dec 2012

Physics 121k Exam 3 7 Dec 2012 Answer each question and show your work. A correct answer with no supportin reasonin may receive no credit. Unless directed otherwise, please use =10.0 m/s 2. Name: 1. (15 points) An 5.0 k block, initially

More information

Experiment 3 The Simple Pendulum

Experiment 3 The Simple Pendulum PHY191 Fall003 Experiment 3: The Simple Pendulum 10/7/004 Pae 1 Suested Readin for this lab Experiment 3 The Simple Pendulum Read Taylor chapter 5. (You can skip section 5.6.IV if you aren't comfortable

More information

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

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

More information

The negative root tells how high the mass will rebound if it is instantly glued to the spring. We want

The negative root tells how high the mass will rebound if it is instantly glued to the spring. We want 8.38 (a) The mass moves down distance.0 m + x. Choose y = 0 at its lower point. K i + U gi + U si + E = K f + U gf + U sf 0 + mgy i + 0 + 0 = 0 + 0 + kx (.50 kg)9.80 m/s (.0 m + x) = (30 N/m) x 0 = (60

More information

PHYS 124 Section A01 Final Examination Autumn 2006

PHYS 124 Section A01 Final Examination Autumn 2006 PHYS 14 Section A1 Final Examination Autumn 6 Name : S Student ID Number : Instructor : Marc de Montiny Time : Monday, December 18, 6 9: 11: AM Room : Tory Lecture (Turtle) TL-B Instructions : This booklet

More information

Fs (30.0 N)(50.0 m) The magnitude of the force that the shopper exerts is f 48.0 N cos 29.0 cos 29.0 b. The work done by the pushing force F is

Fs (30.0 N)(50.0 m) The magnitude of the force that the shopper exerts is f 48.0 N cos 29.0 cos 29.0 b. The work done by the pushing force F is Chapter 6: Problems 5, 6, 8, 38, 43, 49 & 53 5. ssm Suppose in Figure 6. that +1.1 1 3 J o work is done by the orce F (magnitude 3. N) in moving the suitcase a distance o 5. m. At what angle θ is the orce

More information

(C) 7 s. (C) 13 s. (C) 10 m

(C) 7 s. (C) 13 s. (C) 10 m NAME: Ms. Dwarka, Principal Period: #: WC Bryant HS Ms. Simonds, AP Science Base your answers to questions 1 throuh 3 on the position versus time raph below which shows the motion of a particle on a straiht

More information

1- A force F = ( 6ˆ i 2ˆ j )N acts on a particle that undergoes a displacement

1- A force F = ( 6ˆ i 2ˆ j )N acts on a particle that undergoes a displacement 1- A force F = ( 6ˆ i 2ˆ j )N acts on a particle that undergoes a displacement r = ( 3ˆ i + ˆ j )m. Find (a) the work done by the force on the particle and (b) the angle between F and r. 2- The force acting

More information

(A) (B) (C) (D) None of these

(A) (B) (C) (D) None of these Exercise OBJECTIVE PROBLEMS. Action and reaction (A) act on two different objects (C) have opposite directions. Which fiure represents the correct F.B.D. of rod of mass m as shown in fiure : (B) have equal

More information

Physics 231 Lecture 9

Physics 231 Lecture 9 Physics 31 Lecture 9 Mi Main points o today s lecture: Potential energy: ΔPE = PE PE = mg ( y ) 0 y 0 Conservation o energy E = KE + PE = KE 0 + PE 0 Reading Quiz 3. I you raise an object to a greater

More information

Chapter 8 Conservation of Energy and Potential Energy

Chapter 8 Conservation of Energy and Potential Energy Chapter 8 Conservation o Energy and Potential Energy So ar we have analyzed the motion o point-like bodies under the action o orces using Newton s Laws o Motion. We shall now use the Principle o Conservation

More information

Physics Test VI Chapter 7 Impulse and Momentum

Physics Test VI Chapter 7 Impulse and Momentum Physics Test VI Chapter 7 Impulse and Momentum Name: Date: Period: Honor Pledge On my honor as a student I have neither given nor received aid on this test Sign Below HW Grade: Test Grade / Mr. Stark Loudoun

More information

Power: Sources of Energy

Power: Sources of Energy Chapter 5 Energy Power: Sources of Energy Tidal Power SF Bay Tidal Power Project Main Ideas (Encyclopedia of Physics) Energy is an abstract quantity that an object is said to possess. It is not something

More information

Potential energy and conservation of energy

Potential energy and conservation of energy Chapter 8 Potential energy and conservation of energy Copyright 8.1_2 Potential Energy and Work Potential energy U is energy that can be associated with the configuration (arrangement) of a system of objects

More information

Lecture 6.1 Work and Energy During previous lectures we have considered many examples, which can be solved using Newtonian approach, in particular,

Lecture 6.1 Work and Energy During previous lectures we have considered many examples, which can be solved using Newtonian approach, in particular, Lecture 6. Work and Energy During previous lectures we have considered many examples, which can be solved using Newtonian approach, in particular, Newton's second law. However, this is not always the most

More information

f 1. (8.1.1) This means that SI unit for frequency is going to be s 1 also known as Hertz d1hz

f 1. (8.1.1) This means that SI unit for frequency is going to be s 1 also known as Hertz d1hz ecture 8-1 Oscillations 1. Oscillations Simple Harmonic Motion So far we have considered two basic types of motion: translational motion and rotational motion. But these are not the only types of motion

More information

General Physics I Work & Energy

General Physics I Work & Energy General Physics I Work & Energy Forms of Energy Kinetic: Energy of motion. A car on the highway has kinetic energy. We have to remove this energy to stop it. The brakes of a car get HOT! This is an example

More information

Chapters 5-6. Dynamics: Forces and Newton s Laws of Motion. Applications

Chapters 5-6. Dynamics: Forces and Newton s Laws of Motion. Applications Chapters 5-6 Dynamics: orces and Newton s Laws of Motion. Applications That is, describing why objects move orces Newton s 1 st Law Newton s 2 nd Law Newton s 3 rd Law Examples of orces: Weight, Normal,

More information

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

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

Energy present in a variety of forms. Energy can be transformed form one form to another Energy is conserved (isolated system) ENERGY

Energy present in a variety of forms. Energy can be transformed form one form to another Energy is conserved (isolated system) ENERGY ENERGY Energy present in a variety of forms Mechanical energy Chemical energy Nuclear energy Electromagnetic energy Energy can be transformed form one form to another Energy is conserved (isolated system)

More information

Common Exam 3, Friday, April 13, :30 9:45 A.M. at KUPF 205 Chaps. 6, 7, 8. HW #8 and HW #9: Due tomorrow, April 6 th (Fri)

Common Exam 3, Friday, April 13, :30 9:45 A.M. at KUPF 205 Chaps. 6, 7, 8. HW #8 and HW #9: Due tomorrow, April 6 th (Fri) Common Exam 3, Friday, April 13, 2007 8:30 9:45 A.M. at KUPF 205 Chaps. 6, 7, 8 Bring calculators (Arrive by 8:15) HW #8 and HW #9: Due tomorrow, April 6 th (Fri) Today. Chapter 8 Hints for HW #9 Quiz

More information

Chapter 8. Potential Energy & Conservation of Energy

Chapter 8. Potential Energy & Conservation of Energy Chapter 8 Potential Energy & Conservation of Energy 8.1 Potential Energy Technically, potential energy is energy that can be associated with the configuration (arrangement) of a system of objects that

More information

Ch 8 Conservation of Energy

Ch 8 Conservation of Energy Ch 8 Conservation of Energy Cons. of Energy It has been determined, through experimentation, that the total mechanical energy of a system remains constant in any isolated system of objects that interact

More information

Solutions to Physics: Principles with Applications, 5/E, Giancoli Chapter 6

Solutions to Physics: Principles with Applications, 5/E, Giancoli Chapter 6 CHAPTER 6 1. Because there is no acceleration, the contact orce must have the same magnitude as the weight. The displacement in the direction o this orce is the vertical displacement. Thus, W = F Æy =

More information

(A) 10 m (B) 20 m (C) 25 m (D) 30 m (E) 40 m

(A) 10 m (B) 20 m (C) 25 m (D) 30 m (E) 40 m Work/nergy 1. student throws a ball upward where the initial potential energy is 0. t a height of 15 meters the ball has a potential energy of 60 joules and is moving upward with a kinetic energy of 40

More information

Phys101 Lectures 9 and 10 Conservation of Mechanical Energy

Phys101 Lectures 9 and 10 Conservation of Mechanical Energy Phys101 Lectures 9 and 10 Conservation of Mechanical Energy Key points: Conservative and Nonconservative Forces Potential Energy Generalized work-energy principle Mechanical Energy and Its Conservation

More information

Chapter 14 Oscillations. Copyright 2009 Pearson Education, Inc.

Chapter 14 Oscillations. Copyright 2009 Pearson Education, Inc. Chapter 14 Oscillations 14-1 Oscillations of a Spring If an object vibrates or oscillates back and forth over the same path, each cycle taking the same amount of time, the motion is called periodic. The

More information

If you have a conflict, you should have already requested and received permission from Prof. Shapiro to take the make-up exam.

If you have a conflict, you should have already requested and received permission from Prof. Shapiro to take the make-up exam. Reminder: Exam this Sunday Nov. 9. Chapters 5. 5.4, 3.4,.0, 6, 7. Time: 6:0 7:30 PM Look up locations online. Bring calculator and formula sheet. If you have a conflict, you should have already requested

More information

Physics 11 HW #6 Solutions

Physics 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 information

NEWTONS LAWS OF MOTION AND FRICTIONS STRAIGHT LINES

NEWTONS LAWS OF MOTION AND FRICTIONS STRAIGHT LINES EWTOS LAWS O OTIO AD RICTIOS STRAIGHT LIES ITRODUCTIO In this chapter, we shall study the motion o bodies along with the causes o their motion assuming that mass is constant. In addition, we are going

More information

Physics 101 Lecture 12 Equilibrium and Angular Momentum

Physics 101 Lecture 12 Equilibrium and Angular Momentum Physics 101 Lecture 1 Equilibrium and Angular Momentum Ali ÖVGÜN EMU Physics Department www.aovgun.com Static Equilibrium q Equilibrium and static equilibrium q Static equilibrium conditions n Net external

More information

Physics 40 Chapter 8 Homework Q: 12, 13 P: 3, 4, 7, 15, 19, 24, 32, 34, 39, 54, 55, 58, 59, 62, 64

Physics 40 Chapter 8 Homework Q: 12, 13 P: 3, 4, 7, 15, 19, 24, 32, 34, 39, 54, 55, 58, 59, 62, 64 Physics 40 Chapter 8 Homework Q:, 3 P: 3, 4, 7, 5, 9, 4, 3, 34, 39, 54, 55, 58, 59, 6, 64 Conceptual Questions *Q8. We hae (/)m = μ k mgd so d = /μ k g. The quantity /μ k controls the skidding distance.

More information

OSCILLATIONS

OSCILLATIONS OSCIAIONS Important Points:. Simple Harmonic Motion: a) he acceleration is directly proportional to the displacement of the body from the fixed point and it is always directed towards the fixed point in

More information

Chapter 6 Energy and Oscillations

Chapter 6 Energy and Oscillations Chapter 6 Energy and Oscillations Conservation of Energy In this chapter we will discuss one of the most important and fundamental principles in the universe. Energy is conserved. This means that in any

More information

Chapter 14 Oscillations

Chapter 14 Oscillations Chapter 14 Oscillations If an object vibrates or oscillates back and forth over the same path, each cycle taking the same amount of time, the motion is called periodic. The mass and spring system is a

More information

Chapter 11 Vibrations and Waves

Chapter 11 Vibrations and Waves Chapter 11 Vibrations and Waves If an object vibrates or oscillates back and forth over the same path, each cycle taking the same amount of time, the motion is called periodic. The mass and spring system

More information

Phys101 Lectures 9 and 10 Conservation of Mechanical Energy

Phys101 Lectures 9 and 10 Conservation of Mechanical Energy Phys101 Lectures 9 and 10 Conservation of Mechanical Energy Key points: Conservative and Nonconservative Forces Potential Energy Generalized work-energy principle Mechanical Energy and Its Conservation

More information

Chapters 10 & 11: Energy

Chapters 10 & 11: Energy Chapters 10 & 11: Energy Power: Sources of Energy Tidal Power SF Bay Tidal Power Project Main Ideas (Encyclopedia of Physics) Energy is an abstract quantity that an object is said to possess. It is not

More information

AAPT UNITED STATES PHYSICS TEAM AIP 2009

AAPT UNITED STATES PHYSICS TEAM AIP 2009 2009 F = ma Exam 1 AAPT UNITED STATES PHYSICS TEAM AIP 2009 2009 F = ma Contest 25 QUESTIONS - 75 MINUTES INSTRUCTIONS DO NOT OPEN THIS TEST UNTI YOU ARE TOD TO BEGIN Use = 10 N/k throuhout this contest.

More information

Physics 231 Lecture 12

Physics 231 Lecture 12 Physics 31 Lecture 1 Work energy theorem W Potential energy o gravity: ΔPE total = = PE KE PE KE 0 mg Conservation o energy ( y ) 0 y 0 E = KE + PE = KE 0 + PE 0 Potential energy o a spring = PE = 1 kx

More information

TFY4102 Exam Fall 2015

TFY4102 Exam Fall 2015 FY40 Eam Fall 05 Short answer (4 points each) ) Bernoulli's equation relating luid low and pressure is based on a) conservation o momentum b) conservation o energy c) conservation o mass along the low

More information

GRADE 12 JUNE 2017 PHYSICAL SCIENCES P1

GRADE 12 JUNE 2017 PHYSICAL SCIENCES P1 NATIONAL SENIOR CERTIFICATE GRADE 1 JUNE 017 PHYSICAL SCIENCES P1 MARKS: 150 TIME: 3 hours *JPHSCE1* This question paper consists o 1 pages, including a page data sheet. PHYSICAL SCIENCES P1 (EC/JUNE 017)

More information

Practice Final C. 1. The diagram below shows a worker using a rope to pull a cart.

Practice Final C. 1. The diagram below shows a worker using a rope to pull a cart. 1. The diagram below shows a worker using a rope to pull a cart. 6. The graph below represents the relationship between gravitational force and mass for objects near the surface of Earth. The worker s

More information

for any object. Note that we use letter, m g, meaning gravitational

for any object. Note that we use letter, m g, meaning gravitational Lecture 4. orces, Newton's Second Law Last time we have started our discussion of Newtonian Mechanics and formulated Newton s laws. Today we shall closely look at the statement of the second law and consider

More information

PhysicsAndMathsTutor.com

PhysicsAndMathsTutor.com . A particle of mass m is projected vertically upwards, at time t =, with speed. The particle is mv subject to air resistance of manitude, where v is the speed of the particle at time t and is a positive

More information

A. B. C. D. E. v x. ΣF x

A. 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 information

Oscillations. Phys101 Lectures 28, 29. Key points: Simple Harmonic Motion (SHM) SHM Related to Uniform Circular Motion The Simple Pendulum

Oscillations. Phys101 Lectures 28, 29. Key points: Simple Harmonic Motion (SHM) SHM Related to Uniform Circular Motion The Simple Pendulum Phys101 Lectures 8, 9 Oscillations Key points: Simple Harmonic Motion (SHM) SHM Related to Uniform Circular Motion The Simple Pendulum Ref: 11-1,,3,4. Page 1 Oscillations of a Spring If an object oscillates

More information

Unit 4 Work, Power & Conservation of Energy Workbook

Unit 4 Work, Power & Conservation of Energy Workbook Name: Per: AP Physics C Semester 1 - Mechanics Unit 4 Work, Power & Conservation of Energy Workbook Unit 4 - Work, Power, & Conservation of Energy Supplements to Text Readings from Fundamentals of Physics

More information

11. (7 points: Choose up to 3 answers) What is the tension,!, in the string? a.! = 0.10 N b.! = 0.21 N c.! = 0.29 N d.! = N e.! = 0.

11. (7 points: Choose up to 3 answers) What is the tension,!, in the string? a.! = 0.10 N b.! = 0.21 N c.! = 0.29 N d.! = N e.! = 0. A harmonic wave propagates horizontally along a taut string of length! = 8.0 m and mass! = 0.23 kg. The vertical displacement of the string along its length is given by!!,! = 0.1!m cos 1.5!!! +!0.8!!,

More information

Chapter 8. Potential Energy

Chapter 8. Potential Energy Chapter 8 Potential Energy CHAPTER OUTLINE 8. Potential Energy of a System 8.2 The Isolated System Conservation of Mechanical Energy 8.3 Conservative and Nonconservative Forces 8.4 Changes in Mechanical

More information

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

MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. PH 105 Exam 2 VERSION A Name MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. 1) Is it possible for a system to have negative potential energy? A)

More information

1. If the mass of a simple pendulum is doubled but its length remains constant, its period is multiplied by a factor of

1. If the mass of a simple pendulum is doubled but its length remains constant, its period is multiplied by a factor of 1. If the mass of a simple pendulum is doubled but its length remains constant, its period is multiplied by a factor of 1 1 (A) 2 (B) 2 (C) 1 (D) 2 (E) 2 2. A railroad flatcar of mass 2,000 kilograms rolls

More information

Old Exam. Question Chapter 7 072

Old Exam. Question Chapter 7 072 Old Exam. Question Chapter 7 072 Q1.Fig 1 shows a simple pendulum, consisting of a ball of mass M = 0.50 kg, attached to one end of a massless string of length L = 1.5 m. The other end is fixed. If the

More information

Chapter 8. Potential Energy and Conservation of Energy

Chapter 8. Potential Energy and Conservation of Energy Chapter 8 Potential Energy and Conservation of Energy 8.2 Conservative and non-conservative forces A system consists of two or more particles. A configuration of the system is just a specification of the

More information

v( t) g 2 v 0 sin θ ( ) ( ) g t ( ) = 0

v( t) g 2 v 0 sin θ ( ) ( ) g t ( ) = 0 PROJECTILE MOTION Velocity We seek to explore the velocity of the projectile, includin its final value as it hits the round, or a taret above the round. The anle made by the velocity vector with the local

More information

2007 Problem Topic Comment 1 Kinematics Position-time equation Kinematics 7 2 Kinematics Velocity-time graph Dynamics 6 3 Kinematics Average velocity

2007 Problem Topic Comment 1 Kinematics Position-time equation Kinematics 7 2 Kinematics Velocity-time graph Dynamics 6 3 Kinematics Average velocity 2007 Problem Topic Comment 1 Kinematics Position-time equation Kinematics 7 2 Kinematics Velocity-time graph Dynamics 6 3 Kinematics Average velocity Energy 7 4 Kinematics Free fall Collisions 3 5 Dynamics

More information

Lecture 9: Kinetic Energy and Work 1

Lecture 9: Kinetic Energy and Work 1 Lecture 9: Kinetic Energy and Work 1 CHAPTER 6: Work and Kinetic Energy The concept of WORK has a very precise definition in physics. Work is a physical quantity produced when a Force moves an object through

More information

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

MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. PH 105 Exam 2 VERSION B Name MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. 1) A boy throws a rock with an initial velocity of 2.15 m/s at 30.0 above

More information

Fundamentals Physics

Fundamentals Physics Fundamentals Physics Tenth Edition Halliday Chapter 8 Potential Energy and Conservation of Energy 8-1 Potential Energy (1 of 15) Learning Objectives 8.01 Distinguish a conservative force force from a nonconservative

More information

Ground Rules. PC1221 Fundamentals of Physics I. Position and Displacement. Average Velocity. Lectures 7 and 8 Motion in Two Dimensions

Ground Rules. PC1221 Fundamentals of Physics I. Position and Displacement. Average Velocity. Lectures 7 and 8 Motion in Two Dimensions PC11 Fundamentals of Physics I Lectures 7 and 8 Motion in Two Dimensions Dr Tay Sen Chuan 1 Ground Rules Switch off your handphone and paer Switch off your laptop computer and keep it No talkin while lecture

More information

Chapters 10 & 11: Energy

Chapters 10 & 11: Energy Chapters 10 & 11: Energy Power: Sources of Energy Tidal Power SF Bay Tidal Power Project Main Ideas (Encyclopedia of Physics) Energy is an abstract quantity that an object is said to possess. It is not

More information

( ) = ( ) W net = ΔKE = KE f KE i W F. F d x. KE = 1 2 mv2. Note: Work is the dot product of F and d. Work-Kinetic Energy Theorem

( ) = ( ) W net = ΔKE = KE f KE i W F. F d x. KE = 1 2 mv2. Note: Work is the dot product of F and d. Work-Kinetic Energy Theorem Work-Kinetic Energy Theorem KE = 1 2 mv2 W F change in the kinetic energy of an object F d x net work done on the particle ( ) = ( ) W net = ΔKE = KE f KE i Note: Work is the dot product of F and d W g

More information

Unit 7: Energy Notes

Unit 7: Energy Notes Unit 7: Energy Notes Energy is a conserved, substance-like quantity with the capability to produce change. Energy is conserved, neither created nor destroyed. = (Law of conservation of energy) Εnergy is

More information

P = dw dt. P = F net. = W Δt. Conservative Force: P ave. Net work done by a conservative force on an object moving around every closed path is zero

P = dw dt. P = F net. = W Δt. Conservative Force: P ave. Net work done by a conservative force on an object moving around every closed path is zero Power Forces Conservative Force: P ave = W Δt P = dw dt P = F net v Net work done by a conservative force on an object moving around every closed path is zero Non-conservative Force: Net work done by a

More information

1999 AAPT PHYSICS OLYMPIAD

1999 AAPT PHYSICS OLYMPIAD 1999 AAPT PHYSICS OLYMPIAD Entia non multiplicanda sunt praeter necessitatem 1999 MULTIPLE CHOICE SCREENING TEST 30 QUESTIONS - 40 MINUTES INSTRUCTIONS DO NOT OPEN THIS TEST UNTIL YOU ARE TOLD TO BEGIN

More information

UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics

UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics UNIVRSITY OF SASKATCHWAN Department of Physics and nineerin Physics Physics 115.3 MIDTRM TST Alternative Sittin October 009 Time: 90 minutes NAM: (Last) Please Print (Given) STUDNT NO.: LCTUR SCTION (please

More information

Work Done by a Constant Force

Work Done by a Constant Force Work and Energy Work Done by a Constant Force In physics, work is described by what is accomplished when a force acts on an object, and the object moves through a distance. The work done by a constant

More information

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

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

More information

Circular_Gravitation_P1 [22 marks]

Circular_Gravitation_P1 [22 marks] Circular_Gravitation_P1 [ marks] 1. An object of mass m at the end of a strin of lenth r moves in a vertical circle at a constant anular speed ω. What is the tension in the strin when the object is at

More information

PHYSICS 113: Contemporary Physics Final Exam Solution Key (2016)

PHYSICS 113: Contemporary Physics Final Exam Solution Key (2016) PHYSICS 113: Contemporary Physics Final Exam Solution Key (2016) 1. [25 points] (5 points each) Short Answers (a) The central reaction that governs the weak nuclear reactions of the sun reduces to: 4 p

More information

University of Alabama Department of Physics and Astronomy. PH 125 / LeClair Fall Exam III Solution

University of Alabama Department of Physics and Astronomy. PH 125 / LeClair Fall Exam III Solution University of Alabama Department of Physics and Astronomy PH 5 / LeClair Fall 07 Exam III Solution. A child throws a ball with an initial speed of 8.00 m/s at an anle of 40.0 above the horizontal. The

More information

P8.14. m 1 > m 2. m 1 gh = 1 ( 2 m 1 + m 2 )v 2 + m 2 gh. 2( m 1. v = m 1 + m 2. 2 m 2v 2 Δh determined from. m 2 g Δh = 1 2 m 2v 2.

P8.14. m 1 > m 2. m 1 gh = 1 ( 2 m 1 + m 2 )v 2 + m 2 gh. 2( m 1. v = m 1 + m 2. 2 m 2v 2 Δh determined from. m 2 g Δh = 1 2 m 2v 2. . Two objects are connected by a light string passing over a light frictionless pulley as in Figure P8.3. The object of mass m is released from rest at height h. Using the principle of conservation of

More information

= y(x, t) =A cos (!t + kx)

= y(x, t) =A cos (!t + kx) A harmonic wave propagates horizontally along a taut string of length L = 8.0 m and mass M = 0.23 kg. The vertical displacement of the string along its length is given by y(x, t) = 0. m cos(.5 t + 0.8

More information

Review D: Potential Energy and the Conservation of Mechanical Energy

Review D: Potential Energy and the Conservation of Mechanical Energy MSSCHUSETTS INSTITUTE OF TECHNOLOGY Department o Physics 8. Spring 4 Review D: Potential Energy and the Conservation o Mechanical Energy D.1 Conservative and Non-conservative Force... D.1.1 Introduction...

More information

Potential energy functions used in Chapter 7

Potential energy functions used in Chapter 7 Potential energy functions used in Chapter 7 CHAPTER 7 CONSERVATION OF ENERGY Conservation of mechanical energy Conservation of total energy of a system Examples Origin of friction Gravitational potential

More information

Old Exams Questions Ch. 8 T072 Q2.: Q5. Q7.

Old Exams Questions Ch. 8 T072 Q2.: Q5. Q7. Old Exams Questions Ch. 8 T072 Q2.: A ball slides without friction around a loop-the-loop (see Fig 2). A ball is released, from rest, at a height h from the left side of the loop of radius R. What is the

More information

Conservative vs. Non-conservative forces Gravitational Potential Energy. Conservation of Mechanical energy

Conservative vs. Non-conservative forces Gravitational Potential Energy. Conservation of Mechanical energy Next topic Conservative vs. Non-conservative forces Gravitational Potential Energy Mechanical Energy Conservation of Mechanical energy Work done by non-conservative forces and changes in mechanical energy

More information

Work and energy. 15 m. c. Find the work done by the normal force exerted by the incline on the crate.

Work and energy. 15 m. c. Find the work done by the normal force exerted by the incline on the crate. Work and energy 1. A 10.0-kg crate is pulled 15.0 m up along a frictionless incline as shown in the figure below. The crate starts at rest and has a final speed of 6.00 m/s. motor 15 m 5 a. Draw the free-body

More information

Simple Harmonic Motion Test Tuesday 11/7

Simple Harmonic Motion Test Tuesday 11/7 Simple Harmonic Motion Test Tuesday 11/7 Chapter 11 Vibrations and Waves 1 If an object vibrates or oscillates back and forth over the same path, each cycle taking the same amount of time, the motion is

More information

Chapter 14 Oscillations. Copyright 2009 Pearson Education, Inc.

Chapter 14 Oscillations. Copyright 2009 Pearson Education, Inc. Chapter 14 Oscillations Oscillations of a Spring Simple Harmonic Motion Energy in the Simple Harmonic Oscillator Simple Harmonic Motion Related to Uniform Circular Motion The Simple Pendulum The Physical

More information

Chapter 5 Oscillatory Motion

Chapter 5 Oscillatory Motion Chapter 5 Oscillatory Motion Simple Harmonic Motion An object moves with simple harmonic motion whenever its acceleration is proportional to its displacement from some equilibrium position and is oppositely

More information

Chapter 15. Oscillatory Motion

Chapter 15. Oscillatory Motion Chapter 15 Oscillatory Motion Part 2 Oscillations and Mechanical Waves Periodic motion is the repeating motion of an object in which it continues to return to a given position after a fixed time interval.

More information

Chapter 07: Kinetic Energy and Work

Chapter 07: Kinetic Energy and Work Chapter 07: Kinetic Energy and Work Conservation of Energy is one of Nature s fundamental laws that is not violated. Energy can take on different forms in a given system. This chapter we will discuss work

More information