EXAM 3 REVIEW: hardest problems
|
|
- Jewel Craig
- 6 years ago
- Views:
Transcription
1 PHYS 17: oern echanics Spring 011 xa 3 results: ultiple choice: 4.5/70 = 60.7% Hanwritten: XXX FINAL XA: 1. Coprehensie. About 0-5 ultiple choice questions only. If you hae Final xa conflict: 1. Notify us ieiately (before next onay, Apr 5). Inicate your exa scheule for Thursay, Friay an Saturay.. Depening on your input, the akeup exa will be scheule for Friay or Saturay. Lecture 5 ntropy ea XA 3 VIW: harest probles
2 xa 3: Harest proble, 39% A rocket is at rest (not oing) in outer space far away fro any assie objects, i.e. the external net force on the rocket is negligible. The rocket turns on its engine throwing out burning gases of rocket fuel to the left, while accelerating the right. Consier a syste consisting of the rocket, fuel an burning gases, an escribe the irection of otion of the center of ass of this syste. P net, ext 39% A) The center of ass will not oe 1% B) The center of ass will accelerate to the right at the sae rate as the rocket itself 44% C) The center of ass will accelerate to the right at rate that is saller than that of rocket 3% D) The center of ass will accelerate to the left 1% ) The answer epens on the cheical energy release uring burning What will be the elocity of the center of ass c? C = F LCTU 16 clicker question: A syste is ly at rest an consists of a an with a bottle sitting on ice (ignore friction). The an then throws the bottle away as shown. 3 xa 3: Harest proble, 39% A rocket is at rest (not oing) in outer space far away fro any assie objects, i.e. the external net force on the rocket is negligible. The rocket turns on its engine throwing out burning gases of rocket fuel to the left, while accelerating the right. Consier a syste consisting of the rocket, fuel an burning gases, an escribe the irection of otion of the center of ass of this syste. P net, ext 39% A) The center of ass will not oe 1% B) The center of ass will accelerate to the right at the sae rate as the rocket itself 44% C) The center of ass will accelerate to the right at rate that is saller than that of rocket 3% D) The center of ass will accelerate to the left 1% ) The answer epens on the cheical energy release uring burning C = F
3 xa 3: Har proble, 4% Two hockey pucks are pulle using attache weightless strings as shown using the sae force. The string in case is wrappe aroun the puck an can unwin freely. In case 1 it is attache to the center. Which puck will accelerate quicker? P C = F net, ext 4% A) They accelerate at the sae rate 46% B) Puck 1 10% C) Puck 1% D) ass of the puck is neee to answer this question 5 xa 3: Har proble, 4% A string is wrappe aroun a isk of ass = 1.6 kg an raius = Starting fro rest, you pull the string with a constant force F = 6 N along a nearly frictionless surface. At the instant when the center of the isk has oe a istance x = 0.10, a length = 0.8 of string has unwoun off the isk. 6% A) K rot = F. 13% B) K rot = F. x 1% C) K rot = F. + F. x 4% D) K rot = F. - F. x 6
4 xa 3: Har proble, 4% A sphere of ass is attache to a fixe piot by a weightless string. Initially, it oes aroun the circle of raius with spee. As it keeps circling the string is pulle into the sphere by a echanis hien within the sphere. What will be the linear spee f of the sphere when it gets two ties closer to the axle, i.e. oes aroun a circle of raius /? A) f = 4% B) f = 4 9 C) f = 10 D) f = / 1 ) f = /4 7 LA = ra F L = r p A A net LA = ra p ra = const 7 xa 3: Har proble, 55% A perfectly elastic ball of ass 100 g bounces off the arth. Which of the stateents are correct: 1) The elocity (ector) of the ball experiences larger change uring the collision than the elocity of arth A: TU B: FALS (not to scale) ) The oentu of the ball experiences larger change uring the collision than the oentu of arth A: TU B: FALS 3) The position of the center of ass of the syste ball+arth fluctuates in the process A: TU B: FALS 8
5 xa 3: Har proble, 58% A bullet of ass is fire horizontally an at a istance aboe the axis of a cyliner of ass, raius. The cyliner is ly at rest an is free to rotate surface as it hits it. The cyliner begins to rotate at an angular spee such that it copletes one coplete reolution in T after catching the bullet. Calculate the spee of the bullet prior to ipact. 1. Which funaental principle will you use? A) oentu principle B) nergy principle C) Angular oentu principle D) None of the aboe 9 xa 3: Har proble, 58% A bullet of ass is fire horizontally an at a istance aboe the axis of a cyliner of ass, raius. The cyliner is ly at rest an is free to rotate surface as it hits it. The cyliner begins to rotate at an angular spee such that it copletes one coplete reolution in T after catching the bullet. Calculate the spee of the bullet prior to ipact.. Angular oentu of which syste is consere uring collision? A) Bullet B) Cyliner LA = r C) Bullet + cyliner A Fnet =τ A D) None of the aboe Approxiation: all other interactions uring collision are negligible 10
6 xa 3: Har proble, 58% A bullet of ass is fire horizontally an at a istance aboe the axis of a cyliner of ass, raius. The cyliner is ly at rest an is free to rotate surface as it hits it. The cyliner begins to rotate at an angular spee such that it copletes one coplete reolution in T after catching the bullet. Calculate the spee of the bullet prior to ipact. Initial angular oentu in respect to center axle: A) B) C) D) L = + 0 L = + 0 L = + L = + / 11 xa 3: Har proble, 58% A bullet of ass is fire horizontally an at a istance aboe the axis of a cyliner of ass, raius. The cyliner is ly at rest an is free to rotate surface as it hits it. The cyliner begins to rotate at an angular spee such that it copletes one coplete reolution in T after catching the bullet. Calculate the spee of the bullet prior to ipact (I isk = /). L = What is the angular oentu? f = ω ω = π T L = ( + ) ω L = ω + f A) B) C) L = ω + f 1
7 xa 3: Har proble, 58% A bullet of ass is fire horizontally an at a istance aboe the axis of a cyliner of ass, raius. The cyliner is ly at rest an is free to rotate surface as it hits it. The cyliner begins to rotate at an angular spee such that it copletes one coplete reolution in T after catching the bullet. Calculate the spee of the bullet prior to ipact (I isk = /). f = ω ω = π T = ω + f π = + T Fin 13 The Boltzann istribution N=100 oscillators, q=4 quanta What is the probability to fin an ato in a soli at certain energy leel? Separate syste into objects: Object 1: 99 atos Object : 1ato Ω = ( q + N ) q! ( N 1 )! 1! Clicker: In how any ways can we istribute 4 quanta in object? A) 1 way B) 4 ways C) 4!=1**3*4=4 ways Total nuber of icrostates with n quanta in object : Ω = Ω1Ω = Ω1 Probability to fin n quanta on Object is proportional to the nuber of icrostates with (q-n) quanta in Object 1
8 The Boltzann istribution N=100 oscillators, q=4 quanta What is the probability to fin an ato in a soli at certain energy leel? The Boltzann istribution The probability of fining a icroscopic syste to be in a state with energy aboe groun state is proportional to Ω ( ) e kt For large systes! Boltzann factor Nuber of icrostates corresponing to energy See pages for eriation The Boltzann istribution e kt e -1 =0.37 Clicker: At ery high teperature it is possible to hae ore oscillators in the first excite state than in groun state. A) True B) False e -1 =0.37
9 The Boltzann istribution: hyrogen at T e kt oo teperature ~300 K: kt = 0.06 ev 10. ev kt=0.06 ev Teperature at which kt = 10. ev : T=10,000 K The Boltzann istribution easure energy on a single oscillator any ties. Nuber of easureents at energy is proportional to: e kt easure energy on each oscillator on a syste at once. Nuber of oscillators at energy is proportional to: e kt Boltzann istribution: istribution of oscillator energies in a large syste
8.012 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 informationSPH4U. Conservation of Energy. Review: Springs. More Spring Review. 1-D Variable Force Example: Spring. Page 1. For a spring we recall that F x = -kx.
-D Variable Force Exaple: Spring SPH4U Conseration of Energ For a spring we recall that F x = -kx. F(x) x x x relaxe position -kx F = - k x the ass F = - k x Reiew: Springs Hooke s Law: The force exerte
More informationOn my honor, I have neither given nor received unauthorized aid on this examination.
Instructor(s): Field/Furic PHYSICS DEPARTENT PHY 2053 Exam 1 October 5, 2011 Name (print, last first): Signature: On my honor, I hae neither gien nor receied unauthorized aid on this examination. YOUR
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 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 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 informationm A 9. The length of a simple pendulum with a period on Earth of one second is most nearly (A) 0.12 m (B) 0.25 m (C) 0.50 m (D) 1.0 m (E) 10.
P Physics Multiple Choice Practice Oscillations. ass, attache to a horizontal assless spring with spring constant, is set into siple haronic otion. Its axiu isplaceent fro its equilibriu position is. What
More informationm A 1 m mgd k m v ( C) AP Physics Multiple Choice Practice Oscillations
P Physics Multiple Choice Practice Oscillations. 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 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 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 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 information9. h = R. 10. h = 3 R
Version PREVIEW Torque Chap. 8 sizeore (13756) 1 This print-out should have 3 questions. ultiple-choice questions ay continue on the next colun or page find all choices before answering. Note in the dropped
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 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 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 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. 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 informationDepartment of Physics Preliminary Exam January 3 6, 2006
Departent of Physics Preliinary Exa January 3 6, 2006 Day 1: Classical Mechanics Tuesday, January 3, 2006 9:00 a.. 12:00 p.. Instructions: 1. Write the answer to each question on a separate sheet of paper.
More informationChapter 7 Impulse and Momentum. So far we considered only constant force/s BUT There are many situations when the force on an object is not constant
Chapter 7 Ipulse and Moentu So far we considered only constant force/s BUT There are any situations when the force on an object is not constant JUST IN TIME TEACHING E-ail or bring e your questions prior
More informationPractice Final Exam PY 205 Monday 2004 May 3
Practice Final Exa PY 05 Monday 004 May 3 Nae There are THREE forula pages. Read all probles carefully before attepting to solve the. Your work ust be legible, and the organization ust be clear. Correct
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 information2009 Academic Challenge
009 Acadeic Challenge PHYSICS TEST - REGIONAL This Test Consists of 5 Questions Physics Test Production Tea Len Stor, Eastern Illinois University Author/Tea Leader Doug Brandt, Eastern Illinois University
More informationUNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics
UNIVERSITY OF SASKATCHEWAN Departent of Physics and Engineering Physics 017 Saskatchewan High School Physics Scholarship Copetition Wednesday May 10, 017 Tie allowed: 90 inutes This copetition is based
More informationA. unchanged increased B. unchanged unchanged C. increased increased D. increased unchanged
IB PHYSICS Name: DEVIL PHYSICS Period: Date: BADDEST CLASS ON CAMPUS CHAPTER B TEST REVIEW. A rocket is fired ertically. At its highest point, it explodes. Which one of the following describes what happens
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 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 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 informationKinetics of Rigid (Planar) Bodies
Kinetics of Rigi (Planar) Boies Types of otion Rectilinear translation Curvilinear translation Rotation about a fixe point eneral planar otion Kinetics of a Syste of Particles The center of ass for a syste
More informationCommon Exam 2 Physics 111 Fall 2006 Name A
Coon Ea Physics Fall 006 Nae A Total Nuber of Points is 5 (Multiple Choice and Worout Probles). Multiple Choice Probles are Point per Question..) A toy car oving at constant speed copletes one lap around
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 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 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 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 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 informationFlipping Physics Lecture Notes: Free Response Question #1 - AP Physics Exam Solutions
2015 FRQ #1 Free Response Question #1 - AP Physics 1-2015 Exa Solutions (a) First off, we know both blocks have a force of gravity acting downward on the. et s label the F & F. We also know there is a
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 informationCHECKLIST. r r. Newton s Second Law. natural frequency ω o (rad.s -1 ) (Eq ) a03/p1/waves/waves doc 9:19 AM 29/03/05 1
PHYS12 Physics 1 FUNDAMENTALS Module 3 OSCILLATIONS & WAVES Text Physics by Hecht Chapter 1 OSCILLATIONS Sections: 1.5 1.6 Exaples: 1.6 1.7 1.8 1.9 CHECKLIST Haronic otion, periodic otion, siple haronic
More informationUNIT HOMEWORK MOMENTUM ANSWER KEY
UNIT HOMEWORK MOMENTUM ANSWER KEY MOMENTUM FORMULA & STUFF FROM THE PAST: p = v, TKE = ½v 2, d = v t 1. An ostrich with a ass of 146 kg is running to the right with a velocity of 17 /s. a. Calculate the
More 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 informationIn the session you will be divided into groups and perform four separate experiments:
Mechanics Lab (Civil Engineers) Nae (please print): Tutor (please print): Lab group: Date of lab: Experients In the session you will be divided into groups and perfor four separate experients: (1) air-track
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 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 informationToday s topic: IMPULSE AND MOMENTUM CONSERVATION
Today s topic: IMPULSE ND MOMENTUM CONSERVTION Reiew of Last Week s Lecture Elastic Potential Energy: x: displacement from equilibrium x = 0: equilibrium position Work-Energy Theorem: W tot W g W el W
More informationPhysics 201, Review 3
Physics 0, Reiew Important Notes: This reiew does not replace your own preparation efforts Exercises used in this reiew do not form a test problem pool. Please practice more with end of chapter problems.
More informationPhysics x141 Practice Final Exam
Physics x141 Practice Final Exam Name: Partial credit will be awarded. However, you must show/explain your work. A correct answer without explanatory material will not receive full credit. Clearly indicate
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 informationKinetic Molecular Theory of Ideal Gases
Lecture -3. Kinetic Molecular Theory of Ideal Gases Last Lecture. IGL is a purely epirical law - solely the consequence of experiental obserations Explains the behaior of gases oer a liited range of conditions.
More informationChapter 9. 9 Momentum. Momentum. PowerPoint Lectures for College Physics: A Strategic Approach, Second Edition Pearson Education, Inc.
Chapter 9 Momentum PowerPoint Lectures for College Physics: A Strategic Approach, Second Edition 9 Momentum Slide 9-2 Slide 9-3 1 Slide 9-4 Reading Quiz 1. Impulse is A. a force that is applied at a random
More 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 informationFinal Test for PHYS 2130 section 091 Date: 2 nd May 2007
Final Test for PHYS 2130 section 091 Date: 2 nd May 2007 Student First Name: Student Rocket ID: Student Last Name: You may use the backside of all pages. No calculators are allowed. Express all answers
More informationLINEAR MOMENTUM. Contents. (A. Savas ARAPO GLU) July 16, Introduction 2. 2 Linear Momentum 2
LINEAR MOMENTUM (A. Savas ARAPO GLU) July 16, 2017 Contents 1 Introduction 2 2 Linear Momentum 2 3 Impulse & Collisions 4 3.1 Collison of Particles................................ 5 3.2 Collison Types...................................
More informationOn my honor, I have neither given nor received unauthorized aid on this examination.
Instructor(s): iel/uric PHYSICS DEPARTENT PHY 2053 Exam 1 October 3, 2012 Name (print, last first): Signature: On my onor, I ave neiter given nor receive unautorize ai on tis examination. YOUR TEST NUBER
More informationA body of unknown mass is attached to an ideal spring with force constant 123 N/m. It is found to vibrate with a frequency of
Chapter 14 [ Edit ] Overview Suary View Diagnostics View Print View with Answers Chapter 14 Due: 11:59p on Sunday, Noveber 27, 2016 To understand how points are awarded, read the Grading Policy for this
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 informationKinetic Molecular Theory of. IGL is a purely empirical law - solely the
Lecture -3. Kinetic Molecular Theory of Ideal Gases Last Lecture. IGL is a purely epirical law - solely the consequence of experiental obserations Explains the behaior of gases oer a liited range of conditions.
More informationShow all work in answering the following questions. Partial credit may be given for problems involving calculations.
Physics 3210, Spring 2018 Final Exam Name: Signature: UID: Please read the following before continuing: Show all work in answering the following questions. Partial credit may be given for problems involving
More informationBROCK UNIVERSITY. Course: PHYS 1P21/1P91 Number of students: 234 Examination date: 5 December 2014 Number of hours: 3
Name: Student #: BROCK UNIVERSITY Page 1 of 12 Final Exam: December 2014 Number of pages: 12 (+ formula sheet) Course: PHYS 1P21/1P91 Number of students: 234 Examination date: 5 December 2014 Number of
More informationChapter 9. Momentum. PowerPoint Lectures for College Physics: A Strategic Approach, Second Edition Pearson Education, Inc.
Chapter 9 Momentum PowerPoint Lectures for College Physics: A Strategic Approach, Second Edition 9 Momentum Slide 9-2 Slide 9-3 Slide 9-4 Reading Quiz 1. Impulse is A. a force that is applied at a random
More 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 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 informationName & Surname:... No:... Class: 11 /...
METU D. F. HIGH SCHOOL 2017-2018 ACADEMIC YEAR, 1 st SEMESTER GRADE 11 / PHYSICS REVIEW FOR GENERAL EXAM-3 UNIFORMLY ACCELERATED MOTION IN TWO DIMENSIONS, ENERGY, IMPULSE & MOMENTUM & TORQUE DECEMBER 2017
More informationUNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics
UNIVERSITY OF SASKATCHEWAN Departent of Physics and Engineering Physics 05 Saskatchewan High School Physics Scholarship Copetition May, 05 Tie allowed: 90 inutes This copetition is based on the Saskatchewan
More informationPhys101 Lectures 13, 14 Momentum and Collisions
Phs0 Lectures 3, 4 Moentu and ollisions Ke points: Moentu and ipulse ondition for conservation of oentu and wh How to solve collision probles entre of ass Ref: 7-,,3,4,5,6,7,8,9,0. Page Moentu is a vector:
More informationQuestions. denotes answer available in Student Solutions Manual/Study Guide; O denotes objective question
Questions 329 Questions enotes answer aailable in tuent olutions anual/tuy Guie; O enotes objectie question 1. O Is it possible to calculate the torque acting on a rigi object without specifying an axis
More informationPhysics 221 Quiz 6 chapters 7-9, Form: A
Physics 1 Quiz 6 chapters 7-9, Form: A Name: Date: An apparatus consists of three balls each of mass M = 0.6 kg mounted on the ends of low-mass rods of length R = 0.4 m. The whole apparatus rotates clockwise
More informationProblem T1. Main sequence stars (11 points)
Proble T1. Main sequence stars 11 points Part. Lifetie of Sun points i..7 pts Since the Sun behaves as a perfectly black body it s total radiation power can be expressed fro the Stefan- Boltzann law as
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 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 informationMassachusetts Institute of Technology Quantum Mechanics I (8.04) Spring 2005 Solutions to Problem Set 4
Massachusetts Institute of Technology Quantu Mechanics I (8.04) Spring 2005 Solutions to Proble Set 4 By Kit Matan 1. X-ray production. (5 points) Calculate the short-wavelength liit for X-rays produced
More informationPhysics 207 Lecture 24
Physics 7 Lecture 4 Physics 7, Lecture 4, Nov. 7 gena: Mi-Ter 3 Review Elastic Properties of Matter, Mouli Pressure, Wor, rchiees Principle, Flui flow, Bernoulli Oscillatory otion, Linear oscillator, Penulus
More informationFALL TERM EXAM, PHYS 1211, INTRODUCTORY PHYSICS I Thursday, 11 December 2014, 6 PM to 9 PM, Field House Gym
FALL TERM EXAM, PHYS 1211, INTRODUCTORY PHYSICS I Thursday, 11 December 2014, 6 PM to 9 PM, Field House Gym NAME: STUDENT ID: INSTRUCTION 1. This exam booklet has 13 pages. Make sure none are missing 2.
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 informationCENTURION UNIVERSITY OF TECHNOLOGY & MANAGEMENT,ODISHA CUEE-2015
CENTURION UNIVERSITY OF TECHNOLOGY & MANAGEMENT,ODISHA CUEE-015 PHYSICS 1. The imensional formula of angular momentum is a) ML T - b) MLT - c) MLT -1 ) ML T -1. If A B = B A, then the angle between A an
More informationPHYSICS 2210 Fall Exam 4 Review 12/02/2015
PHYSICS 10 Fall 015 Exa 4 Review 1/0/015 (yf09-049) A thin, light wire is wrapped around the ri of a unifor disk of radius R=0.80, as shown. The disk rotates without friction about a stationary horizontal
More informationThe product of force and displacement ( in the direction of force ), during which the force is acting, is defined as work.
5 WORK, ENERGY ND POWER Page 5. Work The product of force and displaceent ( in the direction of force ), during which the force is acting, is defined as work. When N force is applied on a particle and
More informationUnit 14 Harmonic Motion. Your Comments
Today s Concepts: Periodic Motion Siple - Mass on spring Daped Forced Resonance Siple - Pendulu Unit 1, Slide 1 Your Coents Please go through the three equations for siple haronic otion and phase angle
More informationPhysics 211: Lecture 14. Today s Agenda
Physics 211: Lecture 14 Today s Agenda Systems of Particles Center of mass Linear Momentum Example problems Momentum Conservation Inelastic collisions in one dimension Ballistic pendulum Physics 211: Lecture
More informationYour Thoughts. What is the difference between elastic collision and inelastic collision?
Your Thoughts This seemed pretty easy...before we got the checkpoint questions What is the difference between elastic collision and inelastic collision? The most confusing part of the pre lecture was the
More information2.25 m. (a) Using Newton s laws of motion, explain why the student can gain an initial speed to leave the ground vertically.
NAME : F.5 ( ) MARS: /70 FORM FIVE PHYSICS TEST on MECHANICS Time Allowe: 70 minutes This test consists of two sections: Section A (structure type questions, 50 marks); Section B (multiple choice, 20 marks)
More informationFinal Exam, vers Physics Fall, 2012
1 Final Exa, - Physics 1110 - Fall, 01 NAME Signature Student ID # TA s Nae(Circle one): Clarissa Briner, Effie Fine, Mathis Habich, Ada Keith, Willia Lewis, John Papaioannou, WeisenShen, JiayiXie, Jian
More informationPhysics Circular Motion: Energy and Momentum Conservation. 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 Circular Motion: Energy and Moentu Conservation Science and Matheatics Education Research Group Supported
More informationPHYS 107 Practice Final Test Fall 2018
The actual test contains 10 ultiple choice questions and 2 probles. However, for extra exercise, this practice test includes 20 questions and 5 probles. Questions: N.B. Make sure that you justify your
More informationT = 2.34x10 6 s = 27.2days.
Sole the following probles in the space proided Use the back of the page if needed Each proble is worth 10 points You ust show your work in a logical fashion starting with the correctly applied and clearly
More information2006 Academic Challenge
2006 Academic Challenge PHYSICS TEST - REGIONAL This Test Consists of 35 Questions Physics Test Production Team Len Storm, Eastern Illinois University Author/Team Coordinator Doug Brandt, Eastern Illinois
More informationis acting on a body of mass m = 3.0 kg and changes its velocity from an initial
PHYS 101 second major Exam Term 102 (Zero Version) Q1. A 15.0-kg block is pulled over a rough, horizontal surface by a constant force of 70.0 N acting at an angle of 20.0 above the horizontal. The block
More information= T. Oscillations and Waves. Example of an Oscillating System IB 12 IB 12
Oscillation: the vibration of an object Oscillations and Waves Eaple of an Oscillating Syste A ass oscillates on a horizontal spring without friction as shown below. At each position, analyze its displaceent,
More informationConservation of Momentum. The total momentum of a closed, isolated system does not change.
Conservation of Momentum In the 17 th century, Newton and others had measured the momentum of colliding objects before and after collision, and had discovered a strange phenomenon: the total momentum of
More informationQ2. A machine carries a 4.0 kg package from an initial position of d ˆ. = (2.0 m)j at t = 0 to a final position of d ˆ ˆ
Coordinator: Dr. S. Kunwar Monday, March 25, 2019 Page: 1 Q1. An object moves in a horizontal circle at constant speed. The work done by the centripetal force is zero because: A) the centripetal force
More informationReading from Young & Freedman: For this topic, read the introduction to chapter 25 and sections 25.1 to 25.3 & 25.6.
PHY10 Electricity Topic 6 (Lectures 9 & 10) Electric Current and Resistance n this topic, we will cover: 1) Current in a conductor ) Resistivity 3) Resistance 4) Oh s Law 5) The Drude Model of conduction
More informationbefore the collision and v 1 f and v 2 f after the collision. Since conservation of the linear momentum
Lecture 7 Collisions Durin the preious lecture we stared our discussion of collisions As it was stated last tie a collision is an isolated eent in which two or ore odies (the collidin odies) exert relatiely
More informationSRI LANKAN PHYSICS OLYMPIAD MULTIPLE CHOICE TEST 30 QUESTIONS ONE HOUR AND 15 MINUTES
SRI LANKAN PHYSICS OLYMPIAD - 5 MULTIPLE CHOICE TEST QUESTIONS ONE HOUR AND 5 MINUTES INSTRUCTIONS This test contains ultiple choice questions. Your answer to each question ust be arked on the answer sheet
More information1. The diagram below shows the variation with time t of the velocity v of an object.
1. The diagram below shows the variation with time t of the velocity v of an object. The area between the line of the graph and the time-axis represents A. the average velocity of the object. B. the displacement
More informationQuiz Samples for Chapter 9 Center of Mass and Linear Momentum
Name: Department: Student ID #: Notice +2 ( 1) points per correct (incorrect) answer No penalty for an unanswered question Fill the blank ( ) with ( ) if the statement is correct (incorrect) : corrections
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 informationAP Physics C! name I CM R 2. v cm K = m
AP Physics C! name 120pt TAKE HOME TEST Chap 11 Rolling Mot., Angular Mom., Torque 3/9-14/12 Show your work on the problems Box in answers No Naked Numbers! 80pts from Chap 11 in class Questions and Problems:
More informationForce Concept Inventory
Force Concept Inventory 1. Two metal balls are the same size but one weighs twice as much as the other. The balls are dropped from the roof of a single story building at the same instant of time. The time
More information(D) Based on Ft = m v, doubling the mass would require twice the time for same momentum change
1. A car of mass m, traveling at speed v, stops in time t when maximum braking force is applied. Assuming the braking force is independent of mass, what time would be required to stop a car of mass m traveling
More informationPHYSICS 220. Lecture 15. Textbook Sections Lecture 15 Purdue University, Physics 220 1
PHYSICS 220 Lecture 15 Angular Momentum Textbook Sections 9.3 9.6 Lecture 15 Purdue University, Physics 220 1 Last Lecture Overview Torque = Force that causes rotation τ = F r sin θ Work done by torque
More informationHW 6 - Solutions Due November 20, 2017
Conteporary Physics I HW 6 HW 6 - Solutions Due Noveber 20, 2017 1. A 4 kg block is attached to a spring with a spring constant k 200N/, and is stretched an aount 0.2 [5 pts each]. (a) Sketch the potential
More informationRotation and Translation Challenge Problems Problem 1:
Rotation and Translation Challenge Problems Problem 1: A drum A of mass m and radius R is suspended from a drum B also of mass m and radius R, which is free to rotate about its axis. The suspension is
More information