Pre-AP/IB Physics. 1. The total amount of momentum in a closed, isolated system a. is constantly increasing b. is constantly decreasing
|
|
- Julius Potter
- 5 years ago
- Views:
Transcription
1 Nae: Pre-AP/IB Physs Reew: Work, Energy, & Moentu Please Note soe addtonal noraton n robles 5,6, & & Objetes/oabulary: Use the work energy theore to sole robles. Understand the onet o oste and negate work Use law o onseraton o energy to sole robles. Dene oentu and ulse and use the ulse-oentu theore Use law o onseraton o oentu to sole robles. Understand the derene between elast and nelast ollsons. Multle Choe Identy the letter o the hoe that best oletes the stateentor answers the queston. 1. he total aount o oentu n a losed, solated syste a. s onstantly nreasng b. s onstantly dereasng. s onsered d. s radal. A hange n the knet energy durng a ollson eans that. a. the ollson s nelast b. the ollson s elast. onseraton o oentu s not true d. none o these 3. When a net ore not equal to zero ats on a body. a. the eloty o the body s onstant b. the body s aeleratng. the oentu o the body s zero d. the oentu s nreasng 4. he sallest hange n oentu wll be rodued by. a. a large ore oer a short te b. a sall ore oer a short te. a sall ore oer a long te d. a large ore oer a long te 5. I an objet wth a eloty o 40 /s has the sae oentu as that o a 10 kg ass hang a eloty o 0 /s, the ass o the objet s. a. 10 kg. 5 kg b. 8 kg d. 1 kg 6. Iulse an be reresented by. a. hange n eloty dded by te b. ore tes te ore s aled. ass tes eloty d. none o the aboe 7. When a bat hts a baseball, the ore exerted by the bat on the ball s that exerted by the ball on the bat.. less than 8. When a bat hts a baseball, the hange n oentu o the ball s that o the bat.. less than
2 Nae: Pre-AP/IB Physs 9. When a bat hts a baseball, the hange n eloty o the ball s that o the bat.. less than 10. What s the oon orula or work? a. W Fd(sn θ) b. W Fd. W Fd d. W F d 11. A 1.00 x 10 3 kg sorts ar aelerates ro rest to 5.0 /s n 7.50 s. What s the aerage ower outut o the autooble engne? a. 0.8 kw kw b kw d. 5.4 kw 1. A worker ushes a wheelbarrow wth a horzontal ore o 50.0 N oer a leel dstane o 5.0. I a rtonal ore o 43 N ats on the wheelbarrow n a dreton ooste to that o the worker, what net work s done on the wheelbarrow? a. 50 J b. 0J. 35 J d J 13. A lght attendant ulls a 50.0 N lght bag a dstane o 50.0 along a leel arort loor at a onstant seed. A 30.0 N ore s exerted on the bag at an angle o 50.0 aboe the horzontal. How uh work s done on the lght bag? a J b J. 480 J d J 14. Whh o the ollowng energy ors s n a enl allng ro a desk? a. knet energy b. non-ehanal energy. gratatonal otental energy d. elast otental energy and knet energy 15. Whh o the ollowng energy ors s assoated wth an objet n oton? a. otental energy. non-ehanal energy b. elast otental energy d. knet energy 16. Whh o the ollowng energy ors s assoated wth an objet due to ts oston relate to Earth? a. otental energy. gratatonal otental energy b. elast otental energy d. knet energy 17. Whh o the ollowng araeters does not exress how resstant a srng s to beng oressed or strethed? a. oresson dstane b. relaxed length. srng onstant d. strethng dstane 18. A 40.0 N rate s ulled u a 5.0 nlned lane at a onstant eloty. I the lane s nlned at an angle o 37 o to the horzontal and there s a onstant ore o rton o 10.0 N between the rate and the surae, what s the net gan n otental energy by the rate? a. 90 J b. 10 J. 10 J d. 10 J
3 Nae: Pre-AP/IB Physs 19. A 5.00 x 10 N rate s at the to o a 5.00 ra, whh s nlned at 0.0 wth the horzontal. What s ts otental energy? (g 9.81 /s.) a. 855 J. 815 J b. 350 J d J 0. Why doesn t the rnle o ehanal energy onseraton hold n stuatons when rtonal ores are resent? a. Knet energy s not sly onerted to a or o otental energy. b. Potental energy s sly onerted to a or o gratatonal energy.. Cheal energy s not sly onerted to eletral energy. d. Knet energy s sly onerted to a or o gratatonal energy. 1. A ole aulter lears Wth what eloty does the aulter strke the at n the landng area? (Dsregard ar resstane. g 9.81 /s.) a..70 /s /s b /s d. 1.6 /s. A 15.0 kg rate, ntally at rest, sldes down a ra.0 long and nlned at an angle o 0.0 o wth the horzontal. Usng the work knet energy theore and dsregardng rton, nd the eloty o the rate at the botto o the ra. (g 9.81 /s.) a. 6.1 /s b. 3.7 /s. 9.7 /s d. 8.3 /s 3. A hld rdng a byle has a total ass o 40.0 kg. he hld aroahes the to o a hll that s 10.0 hgh and long at 5.0 /s. I the ore o rton between the byle and the hll s 0.0 N, what s the hld s eloty at the botto o the hll? (Dsregard ar resstane. g 9.81 /s.) a. 5.0 /s b /s. 11 /s d. She stos beore the botto. 4. What s the aerage ower suled by a 60.0 kg seretary runnng u a lght o stars rsng ertally 4.0 n 4. s? a. 380 W. 610 W b. 560 W d. 670 W Short Answer An exlanaton n olete sentenes ust be gen to reee redt. hs ay nlude orula, and substtutons nto the orulas. 5. In the ollowng sentene, s the eeryday or the sent eanng o work ntended? A oah does work on the bleahers by ong the nto lae beore the basketball gae. Yes, W Fd 6. Is onseraton o ehanal energy lkely to hold n the ollowng stuaton? A skateboard rolls aross a sewer grate. No, soe knet energy wll be lost due to rton 7. Is onseraton o ehanal energy lkely to hold n ths stuaton? An e skater gldes aross reshly ade e. Yes, we assue e s rtonless whh we do. 8. What ours when a ahne does work on an objet? It hanges the aount o energy the objet has
4 Nae: Pre-AP/IB Physs Free Resonse All work ust be shown to reee redt. hs nludes gens, orulas, and substtutons nto the orulas. 1. A sker wth a ass o 88 kg hts a ra o snow at 16 /s and beoes arborne. At the hghest ont o lght, the sker s 3.7 aboe the ground. What s the sker s gratatonal otental energy at ths ont? PE gh J. A ar wth a ass o 1500 kg hts a arked 18 wheeler wth a ass o 10,000 kg and stks to t. I the ar s ong at 0 /s, how ast s the 18 wheeler-ar syste ong ater the ollson? / s 0 ( ) 3. I the two ehles had ontnued traelng at 4.0 /s. How ast was the ar ong at the oent o at? / s 0 ( ) 4. he.0 kg head o an axe s ong at a eloty o 5.0 /s when t strkes a log and enetrates 0.0 nto the log. a. What was the ulse arted on the axe? ( 0 5.0) N s F t.0 10 b. What s the aerage ore exerted on the log? a x s F a N. How uh work was done on the axe blade, assue the aeleraton o the blade s unor? W Fd J 1 1 Alternate: W KE 1 0 (.0)(5) 5J 5. wo arts, one o ass M and the other o ass 3M, ollde head-on elastally. I ass 3M s ong wth a eloty V beore the ollson and at V aterward, what was the ntal eloty o ass M t s eloty was V aterwards? P 3 3V - 3V -3V P -V - V thereore M eloty ust be -V 6. What was the hange n oentu o art M n #5 M equals 10 kg and V equals /s?
5 Nae: Pre-AP/IB Physs -60 kg/s 7. A roket s shot u and reahes a seed o 50 /s just beore t exlodes nto two dental ees. Pee A goes o at 45 o to ertal and 40 /s, what are the x and y oonents o ee B s oentu n ters o M (ass)? x y osθ sn θ (40) os(45) 8.3 (40)sn(45) 8.3
Collisions Short, Sharp Shocks
16-8 Satterng R 1b n, b 19-1 Collson Colatons L1 Collsons 1 R 1 9 d, 15, 11 Derent Reerene Fraes, 111 ranslatonal ngular Moentu Quz 1 R 11a; HW1: r s 13*, 1, 3, 39 Collsons Short, Shar Shoks Sak! F Whh
More informationHow does the momentum before an elastic and an inelastic collision compare to the momentum after the collision?
Experent 9 Conseraton o Lnear Moentu - Collsons In ths experent you wll be ntroduced to the denton o lnear oentu. You wll learn the derence between an elastc and an nelastc collson. You wll explore how
More informationPhysic 231 Lecture 14
Physc 3 Lecture 4 Man ponts o last lecture: Ipulses: orces that last only a short te Moentu p Ipulse-Moentu theore F t p ( ) Ipulse-Moentu theore ptot, p, p, p, p, ptot, Moentu and external orces F p ext
More informationCollisions! Short, Sharp Shocks
d b n, b d,, -4 Introducng Collsons Quz 9 L9 Mult-artcle Systes 6-8 Scatterng 9- Collson Colcatons L Collsons 5, Derent Reerence Fraes ranslatonal ngular Moentu Quz RE a RE b RE c EP9 RE a; HW: Pr s 3*,,
More informationChapter 8. Momentum Impulse and Collisions. Analysis of motion: 2 key ideas. Newton s laws of motion. Conservation of Energy
Chapter 8 Moentu Ipulse and Collsons Analyss o oton: key deas Newton s laws o oton Conseraton o Energy Newton s Laws st Law: An object at rest or traelng n unor oton wll rean at rest or traelng n unor
More informationtotal If no external forces act, the total linear momentum of the system is conserved. This occurs in collisions and explosions.
Lesson 0: Collsons, Rotatonal netc Energy, Torque, Center o Graty (Sectons 7.8 Last te we used ewton s second law to deelop the pulse-oentu theore. In words, the theore states that the change n lnear oentu
More informationLecture 09 Systems of Particles and Conservation of Linear Momentum
Lecture 09 Systes o Partcles and Conseraton o Lnear oentu 9. Lnear oentu and Its Conseraton 9. Isolated Syste lnear oentu: P F dp dt d( dt d dt a solated syste F ext 0 dp dp F, F dt dt dp dp d F F 0, 0
More informationp p +... = p j + p Conservation Laws in Physics q Physical states, process, and state quantities: Physics 201, Lecture 14 Today s Topics
Physcs 0, Lecture 4 Conseraton Laws n Physcs q Physcal states, process, and state quanttes: Today s Topcs Partcle Syste n state Process Partcle Syste n state q Lnear Moentu And Collsons (Chapter 9.-9.4)
More informationMomentum and Collisions. Rosendo Physics 12-B
Moentu and Collsons Rosendo Physcs -B Conseraton o Energy Moentu Ipulse Conseraton o Moentu -D Collsons -D Collsons The Center o Mass Lnear Moentu and Collsons February 7, 08 Conseraton o Energy D E =
More informationChapter 9 Centre of Mass and Linear Momentum
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
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 informationName: PHYS 110 Dr. McGovern Spring 2018 Exam 1. Multiple Choice: Circle the answer that best evaluates the statement or completes the statement.
Name: PHYS 110 Dr. McGoern Sprng 018 Exam 1 Multple Choce: Crcle the answer that best ealuates the statement or completes the statement. #1 - I the acceleraton o an object s negate, the object must be
More informationTIME OF COMPLETION NAME SOLUTION DEPARTMENT OF NATURAL SCIENCES. PHYS 2211, Exam 2 Section 1 Version 1 October 18, 2013 Total Weight: 100 points
TIME OF COMPLETION NAME SOLUTION DEPARTMENT OF NATURAL SCIENCES PHYS, Exam Secton Verson October 8, 03 Total Weght: 00 ponts. Check your examnaton or completeness pror to startng. There are a total o nne
More informationPhysics 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 4: Linear Momentum and Collisions
Chater 4: Lear oetu ad Collsos 4.. The Ceter o ass, Newto s Secod Law or a Syste o artcles 4.. Lear oetu ad Its Coserato 4.3. Collso ad Iulse 4.4. oetu ad Ketc Eergy Collsos 4.. The Ceter o ass. Newto
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 informationPage 1. Clicker Question 9: Physics 131: Lecture 15. Today s Agenda. Clicker Question 9: Energy. Energy is Conserved.
Physcs 3: Lecture 5 Today s Agenda Intro to Conseraton o Energy Intro to some derent knds o energy Knetc Potental Denton o Mechancal Energy Conseraton o Mechancal Energy Conserate orces Examples Pendulum
More informationChapter 8. Momentum, Impulse and Collisions (continued) 10/22/2014 Physics 218
Chater 8 Moentu, Iulse and Collsons (contnued 0//04 Physcs 8 Learnng Goals The eanng of the oentu of a artcle(syste and how the ulse of the net force actng on a artcle causes the oentu to change. The condtons
More informationPhysics 2A Chapter 3 HW Solutions
Phscs A Chapter 3 HW Solutons Chapter 3 Conceptual Queston: 4, 6, 8, Problems: 5,, 8, 7, 3, 44, 46, 69, 70, 73 Q3.4. Reason: (a) C = A+ B onl A and B are n the same drecton. Sze does not matter. (b) C
More informationLinear Momentum and Collisions
Lnear Momentum and Collsons Chater 9 Lnear Momentum [kg m/s] x y mv x mv y Newton s nd Law n terms o momentum: Imulse I - [kg m/s] I t t Fdt I = area under curve bounded by t axs Imulse-Momentum Theorem
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. 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 information5/24/2007 Collisions ( F.Robilliard) 1
5/4/007 Collsons ( F.Robllard) 1 Interactons: In our earler studes o orce and work, we saw, that both these quanttes arse n the context o an nteracton between two bodes. We wll now look ore closely at
More informationPhysics 3A: Linear Momentum. Physics 3A: Linear Momentum. Physics 3A: Linear Momentum. Physics 3A: Linear Momentum
Recall that there was ore to oton than just spee A ore coplete escrpton of oton s the concept of lnear oentu: p v (8.) Beng a prouct of a scalar () an a vector (v), oentu s a vector: p v p y v y p z v
More informationPhysics 207, Lecture 13, Oct. 15. Energy
Physcs 07 Lecture 3 Physcs 07, Lecture 3, Oct. 5 Goals: Chapter 0 Understand the relatonshp between moton and energy Dene Potental Energy n a Hooke s Law sprng Deelop and explot conseraton o energy prncple
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 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 information(T > w) F R = T - w. Going up. T - w = ma
ANSES Suspended Acceleratng-Objects A resultant orce causes a syste to accelerate. he drecton o the acceleraton s n the drecton o the resultant orce. As llustrated belo, hen suspended objects accelerate,
More information10/2/2003 PHY Lecture 9 1
Announceents. Exa wll be returned at the end of class. Please rework the exa, to help soldfy your knowledge of ths ateral. (Up to 0 extra cre ponts granted for reworked exa turn n old exa, correctons on
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 informationMomentum. Momentum. Impulse. Momentum and Collisions
Momentum Momentum and Collsons From Newton s laws: orce must be present to change an object s elocty (speed and/or drecton) Wsh to consder eects o collsons and correspondng change n elocty Gol ball ntally
More informationSlide. King Saud University College of Science Physics & Astronomy Dept. PHYS 103 (GENERAL PHYSICS) CHAPTER 5: MOTION IN 1-D (PART 2) LECTURE NO.
Slde Kng Saud Unersty College of Scence Physcs & Astronomy Dept. PHYS 103 (GENERAL PHYSICS) CHAPTER 5: MOTION IN 1-D (PART ) LECTURE NO. 6 THIS PRESENTATION HAS BEEN PREPARED BY: DR. NASSR S. ALZAYED Lecture
More informationGAUTENG DEPARTMENT OF EDUCATION SENIOR SECONDARY INTERVENTION PROGRAMME PHYSICAL SCIENCES GRADE 12 SESSION 1 (LEARNER NOTES)
PHYSICAL SCIENCES GRADE 1 SESSION 1 (LEARNER NOTES) TOPIC 1: MECHANICS PROJECTILE MOTION Learner Note: Always draw a dagram of the stuaton and enter all the numercal alues onto your dagram. Remember to
More informationPHYS 1443 Section 004 Lecture #12 Thursday, Oct. 2, 2014
PHYS 1443 Secton 004 Lecture #1 Thursday, Oct., 014 Work-Knetc Energy Theorem Work under rcton Potental Energy and the Conservatve Force Gravtatonal Potental Energy Elastc Potental Energy Conservaton o
More informationRecitation: Energy, Phys Energies. 1.2 Three stones. 1. Energy. 1. An acorn falling from an oak tree onto the sidewalk.
Rectaton: Energy, Phys 207. Energy. Energes. An acorn fallng from an oak tree onto the sdewalk. The acorn ntal has gravtatonal potental energy. As t falls, t converts ths energy to knetc. When t hts the
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 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 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 informationPHYS 1441 Section 002 Lecture #16
PHYS 1441 Secton 00 Lecture #16 Monday, Mar. 4, 008 Potental Energy Conservatve and Non-conservatve Forces Conservaton o Mechancal Energy Power Today s homework s homework #8, due 9pm, Monday, Mar. 31!!
More informationPHYS 1441 Section 002 Lecture #15
PHYS 1441 Secton 00 Lecture #15 Monday, March 18, 013 Work wth rcton Potental Energy Gravtatonal Potental Energy Elastc Potental Energy Mechancal Energy Conservaton Announcements Mdterm comprehensve exam
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 informationi-clicker i-clicker A B C a r Work & Kinetic Energy
ork & c Energ eew of Preou Lecture New polc for workhop You are epected to prnt, read, and thnk about the workhop ateral pror to cong to cla. (Th part of the polc not new!) There wll be a prelab queton
More informationAP Physics Enosburg Falls High School Mr. Bushey. Week 6: Work, Energy, Power
AP Physcs Enosburg Falls Hgh School Mr. Bushey ee 6: or, Energy, Power Homewor! Read Gancol Chapter 6.1 6.10 AND/OR Read Saxon Lessons 1, 16, 9, 48! Read Topc Summary Handout! Answer Gancol p.174 Problems
More informationPhysics 4C. Chapter 19: Conceptual Questions: 6, 8, 10 Problems: 3, 13, 24, 31, 35, 48, 53, 63, 65, 78, 87
Physcs 4C Solutons to Chater 9 HW Chater 9: Concetual Questons: 6, 8, 0 Problems:,, 4,,, 48,, 6, 6, 78, 87 Queston 9-6 (a) 0 (b) 0 (c) negate (d) oste Queston 9-8 (a) 0 (b) 0 (c) negate (d) oste Queston
More informationLesson 27 Conservation of Energy
Physics 0 Lesson 7 Conservation o nergy In this lesson we will learn about one o the ost powerul tools or solving physics probles utilizing the Law o Conservation o nergy. I. Law o Conservation o nergy
More information2/24/2014. The point mass. Impulse for a single collision The impulse of a force is a vector. The Center of Mass. System of particles
/4/04 Chapte 7 Lnea oentu Lnea oentu of a Sngle Patcle Lnea oentu: p υ It s a easue of the patcle s oton It s a vecto, sla to the veloct p υ p υ p υ z z p It also depends on the ass of the object, sla
More information1.3 Hence, calculate a formula for the force required to break the bond (i.e. the maximum value of F)
EN40: Dynacs and Vbratons Hoework 4: Work, Energy and Lnear Moentu Due Frday March 6 th School of Engneerng Brown Unversty 1. The Rydberg potental s a sple odel of atoc nteractons. It specfes the potental
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 204A FINAL EXAM Chapters 1-14 Spring 2006
Nae: Solve the following probles in the space provided Use the back of the page if needed Each proble is worth 0 points You ust show your work in a logical fashion starting with the correctly applied physical
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 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 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 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 informationPhysics for Scientists and Engineers. Chapter 10 Energy
Physcs or Scentsts and Engneers Chapter 0 Energy Sprng, 008 Ho Jung Pak Introducton to Energy Energy s one o the ost portant concepts n scence although t s not easly dened Eery physcal process that occurs
More informationSpring Force and Power
Lecture 13 Chapter 9 Sprng Force and Power Yeah, energy s better than orces. What s net? Course webste: http://aculty.uml.edu/andry_danylov/teachng/physcsi IN THIS CHAPTER, you wll learn how to solve problems
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 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 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 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 informationChapter 28 Special Relativity
Galilean Relatiity Chapter 8 Speial Relatiity A passenger in an airplane throws a ball straight up. It appears to oe in a ertial path. The law of graity and equations of otion under unifor aeleration are
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 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 informationFrom Newton s 2 nd Law: v v. The time rate of change of the linear momentum of a particle is equal to the net force acting on the particle.
From Newton s 2 nd Law: F ma d dm ( ) m dt dt F d dt The tme rate of change of the lnear momentum of a artcle s equal to the net force actng on the artcle. Conseraton of Momentum +x The toy rocket n dee
More informationChapter 07: Kinetic Energy and Work
Chapter 07: Knetc Energy and Work Conservaton o Energy s one o Nature s undamental laws that s not volated. Energy can take on derent orms n a gven system. Ths chapter we wll dscuss work and knetc energy.
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 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 informationPhysics 231. Topic 8: Rotational Motion. Alex Brown October MSU Physics 231 Fall
Physcs 231 Topc 8: Rotatonal Moton Alex Brown October 21-26 2015 MSU Physcs 231 Fall 2015 1 MSU Physcs 231 Fall 2015 2 MSU Physcs 231 Fall 2015 3 Key Concepts: Rotatonal Moton Rotatonal Kneatcs Equatons
More informationCHAPTER 10 ROTATIONAL MOTION
CHAPTER 0 ROTATONAL MOTON 0. ANGULAR VELOCTY Consder argd body rotates about a fxed axs through pont O n x-y plane as shown. Any partcle at pont P n ths rgd body rotates n a crcle of radus r about O. The
More informationConservation of Energy
Lecture 3 Chapter 8 Physcs I 0.3.03 Conservaton o Energy Course webste: http://aculty.uml.edu/andry_danylov/teachng/physcsi Lecture Capture: http://echo360.uml.edu/danylov03/physcsall.html 95.4, Fall 03,
More informationChapter 8: Potential Energy and The Conservation of Total Energy
Chapter 8: Potental Energy and The Conservaton o Total Energy Work and knetc energy are energes o moton. K K K mv r v v F dr Potental energy s an energy that depends on locaton. -Dmenson F x d U( x) dx
More informationPHYS 1101 Practice problem set 5, Chapter 18: 4, 9, 15, 23, 27, 32, 40, 43, 55, 56, 59 1 = = = Nk T Nk T Nk T B 1 B 2 B 1
PHYS 0 Practice roble set, Chater 8: 4, 9,,, 7,, 40, 4,, 6, 9 8.4. Sole: (a he ean free ath of a olecule in a gas at teerature, olue V, and ressure is λ 00 n. We also know that λ λ V 4 π ( N V r Although,
More informationPhysics 101 Lecture 9 Linear Momentum and Collisions
Physcs 0 Lecture 9 Lnear Momentum and Collsons Dr. Al ÖVGÜN EMU Physcs Department www.aogun.com Lnear Momentum and Collsons q q q q q q q Conseraton o Energy Momentum Impulse Conseraton o Momentum -D Collsons
More informationLinear Momentum. Center of Mass.
Lecture 16 Chapter 9 Physcs I 11.06.2013 Lnear oentu. Center of ass. Course webste: http://faculty.ul.edu/ndry_danylov/teachng/physcsi Lecture Capture: http://echo360.ul.edu/danylov2013/physcs1fall.htl
More informationPhysics 120 Final Examination
Physics 120 Final Exaination 12 August, 1998 Nae Tie: 3 hours Signature Calculator and one forula sheet allowed Student nuber Show coplete solutions to questions 3 to 8. This exaination has 8 questions.
More informationChapter 10: Collisions
PHYS 172: odern echanics Sring 2010 EXA 2 Please check your ultile choice art a.s.a.. (on CHIP). The aer eas will be discarded in one week fro now. Lecture 18 Collisions Read 10.1 10.7 PHYS 172: odern
More informationMotion in One Dimension
Moton n One Dmenson Speed ds tan ce traeled Aerage Speed tme of trael Mr. Wolf dres hs car on a long trp to a physcs store. Gen the dstance and tme data for hs trp, plot a graph of hs dstance ersus tme.
More informationYou will analyze the motion of the block at different moments using the law of conservation of energy.
Physcs 00A Homework 7 Chapter 8 Where s the Energy? In ths problem, we wll consder the ollowng stuaton as depcted n the dagram: A block o mass m sldes at a speed v along a horzontal smooth table. It next
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 informationCh04 Work, Energy and Power What is work in physics?
Eunl Won Dept o Physcs, Korea Unversty 1 Ch04 Work, Energy and Power What s work n physcs? Eunl Won Dept o Physcs, Korea Unversty Eunl Won Dept o Physcs, Korea Unversty 3 Work W F d W Fd cosφ W Fd ο cos
More informationENGINEERING OF NUCLEAR REACTORS. Due November 17, 2006 by 12:00 pm
.3 ENINEEIN OF NUCEA EACOS ue Noveer 7, 006 y :00 AKE HOME QUIZ (SOUION Prole (60% Hydraul Analyss o te Eereny Core Sray Syste n a BW e nuern o te relevant loatons wtn te syste s sown n Fure elow. 3 e
More informationPhysics 2210 Fall smartphysics 20 Conservation of Angular Momentum 21 Simple Harmonic Motion 11/23/2015
Physics 2210 Fall 2015 sartphysics 20 Conservation of Angular Moentu 21 Siple Haronic Motion 11/23/2015 Exa 4: sartphysics units 14-20 Midter Exa 2: Day: Fri Dec. 04, 2015 Tie: regular class tie Section
More informationProblem While being compressed, A) What is the work done on it by gravity? B) What is the work done on it by the spring force?
Problem 07-50 A 0.25 kg block s dropped on a relaed sprng that has a sprng constant o k 250.0 N/m (2.5 N/cm). The block becomes attached to the sprng and compresses t 0.12 m beore momentarl stoppng. Whle
More informationModeling motion with VPython Every program that models the motion of physical objects has two main parts:
1 Modelng moton wth VPython Eery program that models the moton o physcal objects has two man parts: 1. Beore the loop: The rst part o the program tells the computer to: a. Create numercal alues or constants
More informationPeriod & Frequency. Work and Energy. Methods of Energy Transfer: Energy. Work-KE Theorem 3/4/16. Ranking: Which has the greatest kinetic energy?
Perod & Frequency Perod (T): Tme to complete one ull rotaton Frequency (): Number o rotatons completed per second. = 1/T, T = 1/ v = πr/t Work and Energy Work: W = F!d (pcks out parallel components) F
More informationPhysics 40 HW #4 Chapter 4 Key NEATNESS COUNTS! Solve but do not turn in the following problems from Chapter 4 Knight
Physcs 40 HW #4 Chapter 4 Key NEATNESS COUNTS! Solve but do not turn n the ollowng problems rom Chapter 4 Knght Conceptual Questons: 8, 0, ; 4.8. Anta s approachng ball and movng away rom where ball was
More informationEMU Physics Department.
Physcs 0 Lecture 9 Lnear Momentum and Collsons Assst. Pro. Dr. Al ÖVGÜN EMU Physcs Department www.aogun.com Lnear Momentum q Conseraton o Energy q Momentum q Impulse q Conseraton o Momentum q -D Collsons
More informationPhysics 123. Exam #1. October 11, 2006
hyscs Exa # October, 006 roble /0 roble /0 roble /0 roble 4 /0 roble 5 /0 roble 6 /0 roble 7 /0 roble 8 /0 roble 9 /0 roble 0 /0 Total /00 Free-Response robles: lease show all work n order to receve partal
More informationPhysics 231. Topic 8: Rotational Motion. Alex Brown October MSU Physics 231 Fall
Physcs 231 Topc 8: Rotatonal Moton Alex Brown October 21-26 2015 MSU Physcs 231 Fall 2015 1 MSU Physcs 231 Fall 2015 2 MSU Physcs 231 Fall 2015 3 Key Concepts: Rotatonal Moton Rotatonal Kneatcs Equatons
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 informationThe Impact of the Earth s Movement through the Space on Measuring the Velocity of Light
Journal of Appled Matheatcs and Physcs, 6, 4, 68-78 Publshed Onlne June 6 n ScRes http://wwwscrporg/journal/jap http://dxdoorg/436/jap646 The Ipact of the Earth s Moeent through the Space on Measurng the
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. Physics 131: Lecture 14. Today s Agenda. Things that stay the same. Impulse and Momentum Non-constant forces
Physcs 131: Lecture 14 Today s Agenda Imulse and Momentum Non-constant forces Imulse-momentum momentum thm Conservaton of Lnear momentum Eternal/Internal forces Eamles Physcs 201: Lecture 1, Pg 1 Physcs
More informationPhysics 2B Chapter 17 Notes - Calorimetry Spring 2018
Physs 2B Chapter 17 Notes - Calormetry Sprng 2018 hermal Energy and Heat Heat Capaty and Spe Heat Capaty Phase Change and Latent Heat Rules or Calormetry Problems hermal Energy and Heat Calormetry lterally
More informationLecture 16. Chapter 11. Energy Dissipation Linear Momentum. Physics I. Department of Physics and Applied Physics
Lecture 16 Chapter 11 Physcs I Energy Dsspaton Lnear Momentum Course webste: http://aculty.uml.edu/andry_danylov/teachng/physcsi Department o Physcs and Appled Physcs IN IN THIS CHAPTER, you wll learn
More information5/09/06 PHYSICS 213 Exam #1 NAME FEYNMAN Please write down your name also on the back side of the last page
5/09/06 PHYSICS 13 Exa #1 NAME FEYNMAN Please write down your nae also on the back side of the last page 1 he figure shows a horizontal planks of length =50 c, and ass M= 1 Kg, pivoted at one end. he planks
More informationPhysics 105: Mechanics Lecture 13
Physcs 05: Mechancs Lecture 3 Wenda Cao NJIT Physcs Department Momentum and Momentum Conseraton Momentum Impulse Conseraton o Momentum Collsons Lnear Momentum A new undamental quantty, lke orce, energy
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 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 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 information