WYSE Academic Challenge Sectional Physics 2006 Solution Set
|
|
- Aubrie Goodwin
- 5 years ago
- Views:
Transcription
1 WYSE Acadeic Challenge Sectional Physics 6 Solution Set. Correct answer: d. Using Newton s nd Law: r r F 6.N a.kg 6./s.. Correct answer: c. 6. sin θ Correct answer: b. o N 6. N Using Newton s nd Law: r r F ( )(g) (3M)(g) a ( + ) (M + 3M) A B B 3g/5 θ θ 4. Correct answer: c. W Fdcos θ ( ) (9.N)(35.)cos(8 o ) -665 J 5. Correct answer: b. Using Hook s Law twice and diiding: F F k k 34 N 48 N k k 9.4 c 6.4 c 6. Correct answer: b. 3.8 /s 3 (.5 s).5 (.5 s) s 3 (. s).5 (. s) s 3 (.5 s) (. s) V 3.8 /s.5 s. s.5 s ( ) 6 Sectional Solution Set
2 7. Correct answer: e. [ ] [ ][ ] ) [] τ [][ r F] ()(kg /s ) a. a force. F a (kg)(/s No b. a torque. No c. an electrical current. (C/s) No d. power. [ ] [ W] [ F][ d] (kg)(/s )() P [] t [] t s No e. none of the aboe. Correct answer 8. Correct answer: b. y oyt gt ot Soling the equation for t and substituting into the y equation, one obtains: y oy g o V. Thus y has a quadratic dependence upon. o 9. Correct answer: a. Joule Joule second. Watt Joule second. Correct answer: a. Using the right hand rule, position your right hand with fingers wrapped and pointing in the sae sense as the wheel is spinning. The thub then points to the right. R Ale. Correct answer: d. Using the right hand rule, one finds that the two forces produce a torque which is into the of the paper. Since torque equals the rate of change of angular oentu, the change in angular oentu is into the of the paper. Since the direction of the torque is perpendicular to the direction of the angular oentu, the agnitude of the angular oentu reains the sae. Only the direction of the angular oentu changes. The wheel is said to precess. 6 Sectional Solution Set
3 . Correct answer: c. Since the object is said to be in free flight, friction is assued to be negligible. Therefore, the only force acting on the object is graity, which is a conseratie force. Therefore, one ay use conseration of energy to sole the proble. The intial energy of the object and earth syste is 36. J J 9. J. A little later, the systes total energy is still 9. J, but now its potential energy is 54. J, so the kinetic energy of the object is 9. J 54. J 36. J. Using the forula for kinetic energy: 36. J (. kg) V. Soling for the speed, one obtains: V 8.49 /s. 3. Correct answer: e. The change in potential energy between the two eents is 54. J 36. J 8. J. Using the forula for potential energy: 8. J g Δy (. kg)(9.8 /s ) Δy. Soling, Δy Correct answer: e. Since the wires M and N are oing apart, the length after tie is related to the initial length by: (Lf Li ) L f L i + V + V. Thus, V + V. The ef is then found using: Δ(BA) BA f BA i B(A f A i ) B(WL f WL i ) BW(L f Li ) BW( V + V ε ). 5. Correct answer: d. Series cobination of 5. Ω and 5. Ω gies: (5. Ω + 5. Ω 67. Ω) 67. Ω ιn parallel wih 4. Ω gies: ( 67. )( 4. ) ( ) 6. Correct answer: a. Ω 5.Ω Using a for of Kirchhoff s Current Law, (8 A) + (-3A) + I 3 I 3-5 A ΣI ΣI, one has: entering leaing 6 Sectional Solution Set
4 7. Correct answer: d. Here one akes use of Archiede s Principle. The weight of the displaced fluid equals the buoyant force on the object. Since the object floats, the buoyant force ust equal the weight of the cylinder. The weight of the lower fluid that is displaced can be calculated as follows: (olue displaced) X (density) X (acceleration due to graity) (.5)( 6. c 3 )(. g/c 3 )(. kg / g)(9.8 /s ).94 N The weight of the top fluid that is displaced can be calculated as follows: (olue displaced) X (density) X (acceleration due to graity) (.5)( 6. c 3 )(. g/c 3 )(. kg / g)(9.8 /s ).94 N Total weight of fluid displaced weight of floating object.94 N +.94 N.588 N. 8. Correct answer: e. The nth haronic has n lobes ( waelength ( λ/ ). ). A lobe represents one half of a If L represents the length of the string, then for n lobes one has nλ L. The speed of waes on the string, the frequency of of the waes, and the waelength are related by the equation: f n λ n, where n indicates the nth haronic. The speed,, of waes on the string is independent of the haronic. That is, is constant for a gien string and string tension. Thus, using the relationship aboe to replace the waelength, L The net higher haronic would thus gie, f + n + Equating s and substituting in nubers, one has: n. L fn. n L L L L fn + fn. Or n + n n + n Cancelling L and soling for n, one obtains n Correct answer: b. Rolling without slipping can be epressed as c ω R ω R c. c/s. rad/s. c 6 Sectional Solution Set
5 . Correct answer: e. Using conseration of energy, ΔU + Δ d K gδh + ( ) f i [( 5. / s) (. / s) ] 9.9 ( 9.8 / s ) sin 4. and Δh d sin 4. ( ) ( ) f i f i d g sin 4. g sin 4.. Correct answer: c. The total east-west displaceent coponent will be d and the total north-south displaceent will be d y (. i) sin 6. + ( 3. i) sin i (. i) cos6. + ( 3. i) cos i The agnitude of the net dispalceent can be deterined by the Pythagorean theore: d (.3893 i) + ( 3. i) 3.5 i d + d y The direction is found using the inerse tangent function: d y 3. i θ tan tan 8.9 d.3893 i. Correct answer: b. total path length tie to traerse path. iles + 3. iles 3. inutes + 6. inutes.556 iles / inute 3. Correct answer: e. K 4. Correct answer: b. The acceleration is a d dt Δ Δ ( 6 /s) ( 6 /s) 4. s. s 3 /s Note that the instantaneous acceleration is equal to the aerage acceleration as this is a case of constant acceleration. 5. Correct answer: e. Ipulse Ft 6 Sectional Solution Set
6 6. Correct answer: c. y y t 3.8 s Projectile otion is constant acceleration otion. + y t + sinθ ± t or a yt y ( g) t.4 s + sin θ 4 sinθ t + ( g)( y y) gt y y + sinθ t gt (. /s) sin 3. ± (. /s) sin 3. 4( 9.8 /s )(.. ) 9.8 /s Obiously, the positie tie solution is the one that answers the question. 7. Correct answer: b. The difference (-y) has its least significant figure in the tenths place because y has its least significant figure in the tenths place. Calculating (-y)/z results in.64 which should be rounded to the tenth place, giing. as the correct answer. 8. Correct answer: d. c + 9. Correct answer: b. + (. kg)(. ) + (. kg)(. ) + ( 3. kg)( 3. ) (. kg) + (. kg) + ( 3. kg) Applying conseration of oentu, In a copletely inelastic collision, the final elocities are the sae: ( + ) g + g + g g ( 8 lb)(. /s) + ( 9 lb)( /s) ( 8 lb) + ( 9 lb) 9. /s 3. Correct answer: a. The equipotential lines are perpendicular to the electric field lines as shown. The electric field points fro higher electric potential to lower electric potential. D C B A 6 Sectional Solution Set
7 3. Correct answer: c. By the appropriate right-hand rule, the direction of the agnetic field produced by the currents can be deterined. The current toward the top of the page produces agnetic field out of the page in the quadrants containing points A and C and into the page in the quadrants containing points B and D. The current toward the left produces agnetic field out of the page in the quadrants containing points C and D and into the page in the quadrants containing points A and B. Because points A and D are all the sae distance fro the wires, the total agnetic field at points A and D is zero. The the total agnetic field at point C is greater than the agnetic field at point B because the agnetic field drops in agnitude as the distance fro the wires increases. 3. Correct answer: d. I r ( 3. kg)(.3 ) + (. kg)(.7 ).5 kg 33. Correct answer: c. τ rf sinθ 34. Correct answer: c. ( 3. kg)( 9.8 / s )(.3 ) sin 9 (. kg)( 9.8 / s )(.7 ) sin N There are one-fourth the original nuclei reaining after 6. inutes hae passed. This iplies that two half-lies hae passed in 6. inutes. Therefore, the half-life is 3. inutes. N Alternatiely, t ln t ln N ep t / t / ln N / N ( ) ln ( 6. in) ln [(. 9 )/( 8. 9 )] 3. in 35. Correct answer: c. I V + πfc ( 3. Ω) + π. V rs rs rs Z R V 6 ( Hz)( 4. F).78 A 6 Sectional Solution Set
Physics 11 HW #7 Solutions
hysics HW #7 Solutions Chapter 7: Focus On Concepts: 2, 6, 0, 3 robles: 8, 7, 2, 22, 32, 53, 56, 57 Focus On Concepts 7-2 (d) Moentu is a ector quantity that has a agnitude and a direction. The agnitudes
More informationT = 2.34x10 6 s = 27.2days.
Sole the following probles in the space proided Use the back of the page if needed Each proble is worth 10 points You ust show your work in a logical fashion starting with the correctly applied and clearly
More 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 informationPhysics with Health Science Applications Ch. 3 pg. 56
Physics with Health Science Applications Ch. 3 pg. 56 Questions 3.4 The plane is accelerating forward. The seat is connected to the plane and is accelerated forward. The back of the seat applies a forward
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 informationCHAPTER 21 MAGNETIC FORCES AND MAGNETIC FIELDS
CHAPTER 21 MAGNETIC FORCES AND MAGNETIC FIELDS PROBLEMS 5. SSM REASONING According to Equation 21.1, the agnitude of the agnetic force on a oving charge is F q 0 vb sinθ. Since the agnetic field points
More informationKey Terms Electric Potential electrical potential energy per unit charge (JC -1 )
Chapter Seenteen: Electric Potential and Electric Energy Key Ter Electric Potential electrical potential energy per unit charge (JC -1 ) Page 1 of Electrical Potential Difference between two points is
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 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 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 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 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 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 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 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 informationPhysics 218 Exam 3 Fall 2010, Sections
Physics 28 Exa 3 Fall 200, Sections 52-524 Do not fill out the inforation below until instructed to do so! Nae Signature Student ID E-ail Section # : SOUTIONS ules of the exa:. You have the full class
More informationEN40: Dynamics and Vibrations. Midterm Examination Tuesday March
EN4: Dynaics and Vibrations Midter Exaination Tuesday March 8 16 School of Engineering Brown University NAME: General Instructions No collaboration of any kind is peritted on this exaination. You ay bring
More informationPhysics 4A Solutions to Chapter 15 Homework
Physics 4A Solutions to Chapter 15 Hoework Chapter 15 Questions:, 8, 1 Exercises & Probles 6, 5, 31, 41, 59, 7, 73, 88, 90 Answers to Questions: Q 15- (a) toward -x (b) toward +x (c) between -x and 0 (d)
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 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 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 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 informationPH 221-1D Spring Oscillations. Lectures Chapter 15 (Halliday/Resnick/Walker, Fundamentals of Physics 9 th edition)
PH 1-1D Spring 013 Oscillations Lectures 35-37 Chapter 15 (Halliday/Resnick/Walker, Fundaentals of Physics 9 th edition) 1 Chapter 15 Oscillations In this chapter we will cover the following topics: Displaceent,
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 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 informationXI PHYSICS M. AFFAN KHAN LECTURER PHYSICS, AKHSS, K. https://promotephysics.wordpress.com
XI PHYSICS M. AFFAN KHAN LECTURER PHYSICS, AKHSS, K affan_414@live.co https://prootephysics.wordpress.co [MOTION] CHAPTER NO. 3 In this chapter we are going to discuss otion in one diension in which we
More informationPhysics Fall Mechanics, Thermodynamics, Waves, Fluids. Lecture 20: Rotational Motion. Slide 20-1
Physics 1501 Fall 2008 Mechanics, Thermodynamics, Waves, Fluids Lecture 20: Rotational Motion Slide 20-1 Recap: center of mass, linear momentum A composite system behaves as though its mass is concentrated
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 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 informationPHYS 154 Practice Final Test Spring 2018
The actual test contains 10 ultiple choice questions and 2 probles. However, for extra exercise and enjoyent, this practice test includes18 questions and 4 probles. Questions: N.. ake sure that you justify
More informationTransverse waves. Waves. Wave motion. Electromagnetic Spectrum EM waves are transverse.
Transerse waes Physics Enhanceent Prograe for Gifted Students The Hong Kong Acadey for Gifted Education and, HKBU Waes. Mechanical waes e.g. water waes, sound waes, seisic waes, strings in usical instruents.
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 informationPhysics 4A Winter 2016 Final Exam
Physics 4A Winter 016 Final Exa Nae: Mar, 016 Please show your work! Answers are not coplete without clear reasoning. When asked for an expression, you ust give your answer in ters of the variables given
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 informationKinematics (special case) Dynamics gravity, tension, elastic, normal, friction. Energy: kinetic, potential gravity, spring + work (friction)
Kinematics (special case) a = constant 1D motion 2D projectile Uniform circular Dynamics gravity, tension, elastic, normal, friction Motion with a = constant Newton s Laws F = m a F 12 = F 21 Time & Position
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 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 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 informationQuestion 1. [14 Marks]
6 Question 1. [14 Marks] R r T! A string is attached to the dru (radius r) of a spool (radius R) as shown in side and end views here. (A spool is device for storing string, thread etc.) A tension T is
More 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 informatione = n 1 ( ) 3 [ m 3] = n [ m 3] n
Magnetospheric Physics - Hoework Solutions, /7/4 7. Plasa definition Can a plasa be aintained at teperatures of T e K Hint: Calculate the density liit using the plasa paraeter and explain your result).
More informationIn this chapter we will start the discussion on wave phenomena. We will study the following topics:
Chapter 16 Waves I In this chapter we will start the discussion on wave phenoena. We will study the following topics: Types of waves Aplitude, phase, frequency, period, propagation speed of a wave Mechanical
More informationPhysics 41 HW Set 1 Chapter 15 Serway 7 th Edition
Physics HW Set Chapter 5 Serway 7 th Edition Conceptual Questions:, 3, 5,, 6, 9 Q53 You can take φ = π, or equally well, φ = π At t= 0, the particle is at its turning point on the negative side of equilibriu,
More informationwhich proves the motion is simple harmonic. Now A = a 2 + b 2 = =
Worked out Exaples. The potential energy function for the force between two atos in a diatoic olecules can be expressed as follows: a U(x) = b x / x6 where a and b are positive constants and x is the distance
More informationName: Partner(s): Date: Angular Momentum
Nae: Partner(s): Date: Angular Moentu 1. Purpose: In this lab, you will use the principle of conservation of angular oentu to easure the oent of inertia of various objects. Additionally, you develop a
More informationOscillations: Review (Chapter 12)
Oscillations: Review (Chapter 1) Oscillations: otions that are periodic in tie (i.e. repetitive) o Swinging object (pendulu) o Vibrating object (spring, guitar string, etc.) o Part of ediu (i.e. string,
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 information1 (40) Gravitational Systems Two heavy spherical (radius 0.05R) objects are located at fixed positions along
(40) Gravitational Systes Two heavy spherical (radius 0.05) objects are located at fixed positions along 2M 2M 0 an axis in space. The first ass is centered at r = 0 and has a ass of 2M. The second ass
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 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 informationFinal Exam. conflicts with the regular time. Two students have confirmed conflicts with me and will take the
Reiew 3 Final Exam A common final exam time is scheduled d for all sections of Phsics 31 Time: Wednesda December 14, from 8-10 pm. Location for section 00 : BPS 1410 (our regular lecture room). This information
More informationPHYS 102 Previous Exam Problems
PHYS 102 Previous Exa Probles CHAPTER 16 Waves Transverse waves on a string Power Interference of waves Standing waves Resonance on a string 1. The displaceent of a string carrying a traveling sinusoidal
More informationONLINE: MATHEMATICS EXTENSION 2 Topic 6 MECHANICS 6.6 MOTION IN A CIRCLE
ONLINE: MAHEMAICS EXENSION opic 6 MECHANICS 6.6 MOION IN A CICLE When a particle moes along a circular path (or cured path) its elocity must change een if its speed is constant, hence the particle must
More informationChapter 11 Simple Harmonic Motion
Chapter 11 Siple Haronic Motion "We are to adit no ore causes of natural things than such as are both true and sufficient to explain their appearances." Isaac Newton 11.1 Introduction to Periodic Motion
More informationPhysics 4A Solutions to Chapter 4 Homework
Physics 4A Solutions to Chapter 4 Homework Chapter 4 Questions: 4, 1, 1 Exercises & Problems: 5, 11, 3, 7, 8, 58, 67, 77, 87, 11 Answers to Questions: Q 4-4 (a) all tie (b) 1 and tie (the rocket is shot
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 informationEN40: Dynamics and Vibrations. Final Examination Monday May : 2pm-5pm
EN40: Dynaics and Vibrations Final Exaination Monday May 13 013: p-5p School of Engineering Brown University NAME: General Instructions No collaboration of any kind is peritted on this exaination. You
More informationFREE BODY DIAGRAMS! For each of the layouts, draw the f.b.d.s for the bodies in the system. (The solutions follow--try each before looking!)! 3.)!
1.)! FREE BODY DIAGRAMS! For each of the layouts, draw the f.b.d.s for the bodies in the syste. (he solutions follow--try each before looking!)! 3.)!! 1.)! 3.)! 2.)! 4.)!! 2.)! 4.)! 1.) answer 3.) answer!
More information11-2 A General Method, and Rolling without Slipping
11-2 A General Method, and Rolling without Slipping Let s begin by summarizing a general method for analyzing situations involving Newton s Second Law for Rotation, such as the situation in Exploration
More informationPhysics 4A Solutions to Chapter 10 Homework
Physics 4A Solutions to Chapter 0 Homework Chapter 0 Questions: 4, 6, 8 Exercises & Problems 6, 3, 6, 4, 45, 5, 5, 7, 8 Answers to Questions: Q 0-4 (a) positive (b) zero (c) negative (d) negative Q 0-6
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 informationThe Lagrangian Method vs. other methods (COMPARATIVE EXAMPLE)
The Lagrangian ethod vs. other ethods () This aterial written by Jozef HANC, jozef.hanc@tuke.sk Technical University, Kosice, Slovakia For Edwin Taylor s website http://www.eftaylor.co/ 6 January 003 The
More informationQ5 We know that a mass at the end of a spring when displaced will perform simple m harmonic oscillations with a period given by T = 2!
Chapter 4.1 Q1 n oscillation is any otion in which the displaceent of a particle fro a fixed point keeps changing direction and there is a periodicity in the otion i.e. the otion repeats in soe way. In
More 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 informationAxis. Axis. Axis. Hoop about. Annular cylinder (or ring) about central axis. Solid cylinder (or disk) about. central axis. central axis I = MR 2 1
Instructor(s): Matchea/Yelton PHYSICS DEPATMENT PHY 2048 Exam 2 Noember 7th, 207 Name (print, last first): Signature: On my honor, I hae neither gien nor receied unauthorized aid on this examination. YOU
More information) = slugs/ft 3. ) = lb ft/s. ) = ft/s
1. Make use of Tables 1. in the text book (See the last page in this assignent) to express the following quantities in SI units: (a) 10. in./in, (b) 4.81 slugs, (c).0 lb, (d) 7.1 ft/s, (e) 0.04 lb s/ft.
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 informationHORIZONTAL MOTION WITH RESISTANCE
DOING PHYSICS WITH MATLAB MECHANICS HORIZONTAL MOTION WITH RESISTANCE Ian Cooper School of Physics, Uniersity of Sydney ian.cooper@sydney.edu.au DOWNLOAD DIRECTORY FOR MATLAB SCRIPTS ec_fr_b. This script
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 informationSeat: PHYS 1500 (Fall 2006) Exam #2, V1. After : p y = m 1 v 1y + m 2 v 2y = 20 kg m/s + 2 kg v 2y. v 2x = 1 m/s v 2y = 9 m/s (V 1)
Seat: PHYS 1500 (Fall 006) Exa #, V1 Nae: 5 pt 1. Two object are oving horizontally with no external force on the. The 1 kg object ove to the right with a peed of 1 /. The kg object ove to the left with
More informationPart A Here, the velocity is at an angle of 45 degrees to the x-axis toward the z-axis. The velocity is then given in component form as.
Electrodynaics Chapter Andrew Robertson 32.30 Here we are given a proton oving in a agnetic eld ~ B 0:5^{ T at a speed of v :0 0 7 /s in the directions given in the gures. Part A Here, the velocity is
More informationCIRCULAR MOTION EXERCISE 1 1. d = rate of change of angle
CICULA MOTION EXECISE. d = rate of change of angle as they both complete angle in same time.. c m mg N r m N mg r Since r A r B N A N B. a Force is always perpendicular to displacement work done = 0 4.
More informationEN40: Dynamics and Vibrations. Final Examination Tuesday May 15, 2011
EN40: ynaics and Vibrations Final Exaination Tuesday May 15, 011 School of Engineering rown University NME: General Instructions No collaboration of any ind is peritted on this exaination. You ay use double
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 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 informationFeb 6, 2013 PHYSICS I Lecture 5
95.141 Feb 6, 213 PHYSICS I Lecture 5 Course website: faculty.uml.edu/pchowdhury/95.141/ www.masteringphysics.com Course: UML95141SPRING213 Lecture Capture h"p://echo36.uml.edu/chowdhury213/physics1spring.html
More informationSimple Harmonic Motion
Reading: Chapter 15 Siple Haronic Motion Siple Haronic Motion Frequency f Period T T 1. f Siple haronic otion x ( t) x cos( t ). Aplitude x Phase Angular frequency Since the otion returns to its initial
More informationChapter 11 Collision Theory
Chapter Collision Theory Introduction. Center o Mass Reerence Frame Consider two particles o masses m and m interacting ia some orce. Figure. Center o Mass o a system o two interacting particles Choose
More informationChapter 4 FORCES AND NEWTON S LAWS OF MOTION PREVIEW QUICK REFERENCE. Important Terms
Chapter 4 FORCES AND NEWTON S LAWS OF MOTION PREVIEW Dynaics is the study o the causes o otion, in particular, orces. A orce is a push or a pull. We arrange our knowledge o orces into three laws orulated
More informationME Machine Design I. FINAL EXAM. OPEN BOOK AND CLOSED NOTES. Friday, May 8th, 2009
ME 5 - Machine Design I Spring Seester 009 Nae Lab. Div. FINAL EXAM. OPEN BOOK AND LOSED NOTES. Friday, May 8th, 009 Please use the blank paper for your solutions. Write on one side of the paper only.
More informationNote: the net distance along the path is a scalar quantity its direction is not important so the average speed is also a scalar.
PHY 309 K. Solutions for the first mid-term test /13/014). Problem #1: By definition, aerage speed net distance along the path of motion time. 1) ote: the net distance along the path is a scalar quantity
More informationPH 221-2A Fall Waves - I. Lectures Chapter 16 (Halliday/Resnick/Walker, Fundamentals of Physics 9 th edition)
PH 1-A Fall 014 Waves - I Lectures 4-5 Chapter 16 (Halliday/Resnick/Walker, Fundaentals of Physics 9 th edition) 1 Chapter 16 Waves I In this chapter we will start the discussion on wave phenoena. We will
More informationLesson 6: Apparent weight, Radial acceleration (sections 4:9-5.2)
Beore we start the new material we will do another Newton s second law problem. A bloc is being pulled by a rope as shown in the picture. The coeicient o static riction is 0.7 and the coeicient o inetic
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 information2.003 Engineering Dynamics Problem Set 2 Solutions
.003 Engineering Dynaics Proble Set Solutions This proble set is priarily eant to give the student practice in describing otion. This is the subject of kineatics. It is strongly recoended that you study
More informationPractice Midterm #1 Solutions. Physics 6A
Practice Midter # Solution Phyic 6A . You drie your car at a peed of 4 k/ for hour, then low down to k/ for the next k. How far did you drie, and what wa your aerage peed? We can draw a iple diagra with
More informationFOCUS ON CONCEPTS Section 7.1 The Impulse Momentum Theorem
WEEK-6 Recitation PHYS 3 FOCUS ON CONCEPTS Section 7. The Impulse Momentum Theorem Mar, 08. Two identical cars are traeling at the same speed. One is heading due east and the other due north, as the drawing
More informationHandout 7: Torque, angular momentum, rotational kinetic energy and rolling motion. Torque and angular momentum
Handout 7: Torque, angular momentum, rotational kinetic energy and rolling motion Torque and angular momentum In Figure, in order to turn a rod about a fixed hinge at one end, a force F is applied at a
More informationP235 Midterm Examination Prof. Cline
P235 Mier Exaination Prof. Cline THIS IS A CLOSED BOOK EXAMINATION. Do all parts of all four questions. Show all steps to get full credit. 7:00-10.00p, 30 October 2009 1:(20pts) Consider a rocket fired
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 information= o + t = ot + ½ t 2 = o + 2
Chapters 8-9 Rotational Kinematics and Dynamics Rotational motion Rotational motion refers to the motion of an object or system that spins about an axis. The axis of rotation is the line about which the
More informationGENERAL PHYSICS PH 221-1D (Dr. S. Mirov) Test 4 (04/29/13) ALL QUESTIONS ARE WORTH 20 POINTS. WORK OUT FIVE PROBLEMS.
GENERAL PHYSICS PH -D (Dr. S. Mirov) Test 4 (04/9/3) STUDENT NAME: key STUDENT id #: -------------------------------------------------------------------------------------------------------------------------------------------
More informationPHYS 1443 Section 003 Lecture #22
PHYS 443 Section 003 Lecture # Monda, Nov. 4, 003. Siple Bloc-Spring Sste. Energ of the Siple Haronic Oscillator 3. Pendulu Siple Pendulu Phsical Pendulu orsion Pendulu 4. Siple Haronic Motion and Unifor
More informationPhysics 207 Lecture 18. Physics 207, Lecture 18, Nov. 3 Goals: Chapter 14
Physics 07, Lecture 18, Nov. 3 Goals: Chapter 14 Interrelate the physics and atheatics of oscillations. Draw and interpret oscillatory graphs. Learn the concepts of phase and phase constant. Understand
More informationRotation. I. Kinematics - Angular analogs
Rotation I. Kinematics - Angular analogs II. III. IV. Dynamics - Torque and Rotational Inertia Work and Energy Angular Momentum - Bodies and particles V. Elliptical Orbits The student will be able to:
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 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 information= 1.49 m/s m. 2 kg. 2 kg
5.6. Visualize: Please refer to Figure Ex5.6. Solve: For the diagra on the left, three of the vectors lie along the axes of the tilted coordinate sste. Notice that the angle between the 3 N force and the
More informationPeriodic Motion is everywhere
Lecture 19 Goals: Chapter 14 Interrelate the physics and atheatics of oscillations. Draw and interpret oscillatory graphs. Learn the concepts of phase and phase constant. Understand and use energy conservation
More informationCausality and the Kramers Kronig relations
Causality and the Kraers Kronig relations Causality describes the teporal relationship between cause and effect. A bell rings after you strike it, not before you strike it. This eans that the function
More information