Mechanics 3. Elastic strings and springs
|
|
- Dominick Weaver
- 6 years ago
- Views:
Transcription
1 Chapter assessment Mechanics 3 Eastic strings and springs. Two identica ight springs have natura ength m and stiffness 4 Nm -. One is suspended verticay with its upper end fixed to a ceiing and a partice of mass kg hanging in equiibrium from its ower end. (i) Cacuate the extension of the spring. [] The second spring is then attached to the partice and its other end is attached to the foor. The system is in equiibrium with the two springs in the same vertica ine. The distance between the foor and ceiing is.5 m and the extension of the upper spring is e metres. The situation is shown in the diagram beow. m.5 m e m (ii) Write down the extension of the ower spring in terms of e. [] (iii) Write down the equiibrium equation for the partice and hence cacuate e. [4] (iv) Cacuate the tensions in the springs. []. Each of two ight eastic strings, AB and BC, has moduus N. AB has natura ength.5 m and BC has natura ength.8 m. The strings are both attached at B to a partice of mass.75 kg. The ends A and C are fixed to points on a smooth horizonta tabe such that AC = m, as shown in the diagram. A m B C Initiay the partice is hed at the mid-point of AC and reeased from rest. (i) Find the tension in each string before reease and cacuate the acceeration of the partice immediatey after it is reeased. [5] MEI, 9/5/8
2 The partice is now moved to the position where it is in equiibrium. The extension in AB is e m. (ii) Cacuate e. [4] The partice is now hed at A and reeased from rest. (iii) Show that in the subsequent motion BC becomes sack. Cacuate the furthest distance of the partice from A. [6] 3. A ight eastic string AB, of natura ength.8 m and moduus 5 N, is attached at A to a ceiing which is.4 m above the foor. A sma ba of mass. kg is attached to the other end B and hangs in equiibrium. (i) Cacuate the ength of the string. [3] (ii) The ba is pued down unti it touches the foor with AB vertica and it is then reeased from rest. Cacuate the speed at which it hits the ceiing. [4] A second ight eastic string of moduus 5 N and natura ength m, where <.4, is attached to the ba at B and to the foor verticay beow A. The ba is hed at rest on the foor with AB vertica and it is then reeased. (iii) Find the range of vaues of for which the ba wi sti hit the ceiing. [8] 4. A mechanism for firing a ba in a tabe-top game is shown in the diagrams. A moving piston of mass. kg sides freey in a barre, which is fixed. A spring of natura ength.5 m and negigibe mass is fitted inside the barre so that before being primed for use the configuration is that shown in the diagram beow. You may assume that the force due to the compression of the spring may be modeed by Hooke's Law with a stiffness of Nm -.. m barre spring piston (i) Show that the energy stored in the spring is.5 J when it is in the configuration above. [] The mechanism is primed for firing by puing the piston back a distance d, in metres, where d <., as shown in the diagram beow. (ii) Show that the spring has been compressed by a distance (d +.5) m and that the work done in priming the mechanism is d( + d). [3] MEI, 9/5/8
3 The mechanism is primed with d =.8m and a ba of mass. kg is paced in contact with the piston. (iii) Cacuate the aunching speed of the ba (i.e. the speed at which the piston hits the case), if the mechanism is reeased horizontay. [3] (iv) Cacuate the aunching speed of the ba if the mechanism is fired verticay upwards. [3] Tota 5 marks Soutions to Chapter assessment. (i) Verticay: T = g Hooke s Law: T = kx g = 4x 9.8 x = =.49 4 The extension is.49 m. T g (ii) Extension = (.5 e) =.5 e (iii) Verticay: T = g + T Hooke s Law for upper spring: T = 4e Hooke s Law for ower spring: T = 4(.5 e) = 4e 4e = e 8e = 9.6 e =.745 T g + T (iv) T = 4e = = 9.8 The tension in the upper spring is 9.8 N. T = 4e = = 9. The tension in the ower spring is 9. N. MEI, 9/5/8
4 . (i) Initiay AB = m so extension =.5 λ x.5 For AB: T = = =.5 The tension in AB is N. Intiay BC = m so extension =. λ x. For BC: T = = = 5.8 The tension in BC is 5 N. Newton s nd aw: 5 =.75a a = The acceeration of the partice is ms -. (ii) In equiibrium, extension of AB is e m and extension of BC is (.7 e) m. λ x e For AB: T = = = 4e.5 λ x (.7 e) For BC: T = = = 7.5 5e.8 In equiibrium the tensions are equa, so 4e = 7.5 5e 65e = 7.5 e =.69 (3 s.f.) (iii) Initiay extension of BC is. m λ x. E.P.E. in BC = = = 8 J.8 If BC becomes sack, extension of AB wi be.7 m. λ x.7 In this case, E.P.E. in AB = = = 9.8 J..5 Since this is ess than the origina energy in the system, the partice must have kinetic energy of 8. J at this point, so BC does become sack. At furthest distance from A, K.E. =, BC is sack and so E.P.E. in AB must be equa to the origina energy in the system. λ x x E.P.E. in AB = = = x.5 x = 8 x =.949 (3 s.f.) The ength of AB is therefore.45 m (3 s.f.) MEI, 9/5/8
5 3. (i) Verticay: T =.g λ x Hooke s Law: T = 5 x.g = x = = Length of string =.36 m. T.g (ii) When ba is on foor, extension =.6 m λ x 5.6 E.P.E. stored in string = = = 8 J.8 When ba hits ceiing, G.P.E. gained = mgh = = 4.74 J and K.E. gained = mv =.v =.v By conservation of energy: E.P.E. ost = G.P.E. gained + K.E. gained 8 = v v = 5.74 (3 s.f.) Speed = 5.74 ms - (3 s.f.) MEI, 9/5/8
6 (iii) When ba hits ceiing, extension of second string =.4 λ x 5(.4 ) E.P.E. stored in second string when ba hits ceiing = = By conservation of energy: E.P.E. ost by first string = E.P.E. gained by second string + G.P.E. gained + K.E. gained If the ba hits the ceiing, the K.E. gained is greater than or equa to zero E.P.E. ost by st string E.P.E. gained by nd string G.P.E. gained 5(.4 ) (.4 ) ( ) Using the quadratic formua, roots of equation = 3.59 ± are =.6 or From the graph, the soution set of the inequaity is Since <.4, the possibe vaues of are.6 < (i) Compression of spring =.5 m E.P.E. stored = kx =.5 =.5 J. (ii) Origina compression =.5 m Further compression = d m so tota compression of spring = (.5 + d) m. Work done = increase in E.P.E. = ( d +.5).5 = d + d +.5,5 = d(d + ) MEI, 9/5/8
7 (iii) For d =.8, work done =.8(.8 + ) =.44 Work done = K.E. gained.44 =.v.44 =.v v = 3.79 (3 s.f.) Incude mass of piston as we as mass of ba (iv) Work done = K.E. gained + G.P.E. gained.44 =.v =.v v =.83 v = 3.58 (3 s.f.) MEI, 9/5/8
PhysicsAndMathsTutor.com
. Two points A and B ie on a smooth horizonta tabe with AB = a. One end of a ight eastic spring, of natura ength a and moduus of easticity mg, is attached to A. The other end of the spring is attached
More information1) For a block of mass m to slide without friction up a rise of height h, the minimum initial speed of the block must be
v m 1) For a bock of mass m to side without friction up a rise of height h, the minimum initia speed of the bock must be a ) gh b ) gh d ) gh e ) gh c ) gh P h b 3 15 ft 3) A man pus a pound crate up a
More informationPhysics Dynamics: Springs
F A C U L T Y O F E D U C A T I O N Department of Curricuum and Pedagogy Physics Dynamics: Springs Science and Mathematics Education Research Group Supported by UBC Teaching and Learning Enhancement Fund
More informationCandidate Number. General Certificate of Education Advanced Level Examination January 2012
entre Number andidate Number Surname Other Names andidate Signature Genera ertificate of Education dvanced Leve Examination January 212 Physics PHY4/1 Unit 4 Fieds and Further Mechanics Section Tuesday
More informationPREPARED BY: ER. VINEET LOOMBA (B.TECH. IIT ROORKEE)
Cass XI TARGET : JEE Main/Adv PREPARED BY: ER. VINEET LOOMBA (B.TECH. IIT ROORKEE) ALP ADVANCED LEVEL LPROBLEMS ROTATION- Topics Covered: Rigid body, moment of inertia, parae and perpendicuar axes theorems,
More informationELASTICITY PREVIOUS EAMCET QUESTIONS ENGINEERING
ELASTICITY PREVIOUS EAMCET QUESTIONS ENGINEERING. If the ratio of engths, radii and young s modui of stee and brass wires shown in the figure are a, b and c respectivey, the ratio between the increase
More informationCandidate Number. General Certificate of Education Advanced Level Examination June 2010
Centre Number Surname Candidate Number For Examiner s Use Other Names Candidate Signature Examiner s Initias Genera Certificate of Education Advanced Leve Examination June 2010 Question 1 2 Mark Physics
More informationEasticity. The strain produced in the stretched spring is ) Voume Strain ) Shearing Strain 3) Tensie Strain 4) None of the above. A body subjected to strain a number of times does not obey Hooke's aw due
More informationLecture Notes for Math 251: ODE and PDE. Lecture 34: 10.7 Wave Equation and Vibrations of an Elastic String
ecture Notes for Math 251: ODE and PDE. ecture 3: 1.7 Wave Equation and Vibrations of an Eastic String Shawn D. Ryan Spring 212 ast Time: We studied other Heat Equation probems with various other boundary
More informationMeasurement of acceleration due to gravity (g) by a compound pendulum
Measurement of acceeration due to gravity (g) by a compound penduum Aim: (i) To determine the acceeration due to gravity (g) by means of a compound penduum. (ii) To determine radius of gyration about an
More informationConvergence P H Y S I C S
+1 Test (Newton s Law of Motion) 1. Inertia is that property of a body by virtue of which the body is (a) Unabe to change by itsef the state of rest (b) Unabe to change by itsef the state of unifor otion
More informationForces of Friction. through a viscous medium, there will be a resistance to the motion. and its environment
Forces of Friction When an object is in motion on a surface or through a viscous medium, there wi be a resistance to the motion This is due to the interactions between the object and its environment This
More informationOSCILLATIONS. dt x = (1) Where = k m
OSCILLATIONS Periodic Motion. Any otion, which repeats itsef at reguar interva of tie, is caed a periodic otion. Eg: 1) Rotation of earth around sun. 2) Vibrations of a sipe penduu. 3) Rotation of eectron
More informationBIO6X/PM2. General Certificate of Education Advanced Level Examination June Unit 6X A2 Externally Marked Practical Assignment Task Sheet 2
Centre Number Surname Candidate Number For Examinerʼs Use Tota Task 2 Other Names Candidate Signature Genera Certificate of Education Advanced Leve Examination June 2012 Bioogy BIO6X/PM2 Unit 6X A2 Externay
More informationModule 22: Simple Harmonic Oscillation and Torque
Modue : Simpe Harmonic Osciation and Torque.1 Introduction We have aready used Newton s Second Law or Conservation of Energy to anayze systems ike the boc-spring system that osciate. We sha now use torque
More information1 Equations of Motion 3: Equivalent System Method
8 Mechanica Vibrations Equations of Motion : Equivaent System Method In systems in which masses are joined by rigid ins, evers, or gears and in some distributed systems, various springs, dampers, and masses
More informationProblem Set 6: Solutions
University of Aabama Department of Physics and Astronomy PH 102 / LeCair Summer II 2010 Probem Set 6: Soutions 1. A conducting rectanguar oop of mass M, resistance R, and dimensions w by fas from rest
More information3.10 Implications of Redundancy
118 IB Structures 2008-9 3.10 Impications of Redundancy An important aspect of redundant structures is that it is possibe to have interna forces within the structure, with no externa oading being appied.
More informationAPPENDIX C FLEXING OF LENGTH BARS
Fexing of ength bars 83 APPENDIX C FLEXING OF LENGTH BARS C.1 FLEXING OF A LENGTH BAR DUE TO ITS OWN WEIGHT Any object ying in a horizonta pane wi sag under its own weight uness it is infinitey stiff or
More informationWork and energy method. Exercise 1 : Beam with a couple. Exercise 1 : Non-linear loaddisplacement. Exercise 2 : Horizontally loaded frame
Work and energy method EI EI T x-axis Exercise 1 : Beam with a coupe Determine the rotation at the right support of the construction dispayed on the right, caused by the coupe T using Castigiano s nd theorem.
More informationPrevious Years Problems on System of Particles and Rotional Motion for NEET
P-8 JPME Topicwise Soved Paper- PHYSCS Previous Years Probems on Sstem of Partices and otiona Motion for NEET This Chapter Previous Years Probems on Sstem of Partices and otiona Motion for NEET is taken
More informationMP203 Statistical and Thermal Physics. Solutions to Problem Set 3
MP03 Statistica and Therma Physics Soutions to Probem Set 3 1. Consider a cyinder containing 1 mo of pure moecuar nitrogen (N, seaed off withamovabepiston,sothevoumemayvary. Thecyinderiskeptatatmospheric
More informationWork and energy. 15 m. c. Find the work done by the normal force exerted by the incline on the crate.
Work and energy 1. A 10.0-kg crate is pulled 15.0 m up along a frictionless incline as shown in the figure below. The crate starts at rest and has a final speed of 6.00 m/s. motor 15 m 5 a. Draw the free-body
More informationBohr s atomic model. 1 Ze 2 = mv2. n 2 Z
Bohr s atomic mode Another interesting success of the so-caed od quantum theory is expaining atomic spectra of hydrogen and hydrogen-ike atoms. The eectromagnetic radiation emitted by free atoms is concentrated
More informationAdd Math (4044/02) (+) x (+) 2. Find the coordinates of the points of intersection of the curve xy 2 the line 2y 1 x 0. [5]
Add Math (444/) Requirement : Answer a questions Tota mars : 7 Duration : hour 45 minutes. Sove the inequaity 5 and represent the soution set on the number ine. [4] 5 4 From the setch on number ine, we
More informationUniversity of California, Berkeley Physics 7A Spring 2009 (Yury Kolomensky) SOLUTIONS TO PRACTICE PROBLEMS FOR THE FINAL EXAM
1 University of Caifornia, Bereey Physics 7A Spring 009 (Yury Koomensy) SOLUIONS O PRACICE PROBLEMS FOR HE FINAL EXAM Maximum score: 00 points 1. (5 points) Ice in a Gass You are riding in an eevator hoding
More informationElastic Potential Energy
Elastic Potential Energy If you pull on a spring and stretch it, then you do work. That is because you are applying a force over a displacement. Your pull is the force and the amount that you stretch the
More informationGOYAL BROTHERS PRAKASHAN
Assignments in Mathematics Cass IX (Term 2) 14. STATISTICS IMPORTANT TERMS, DEFINITIONS AND RESULTS The facts or figures, which are numerica or otherwise, coected with a definite purpose are caed data.
More informationChapter 6 Work and Energy
Chapter 6 Work and Energy Midterm exams will be available next Thursday. Assignment 6 Textbook (Giancoli, 6 th edition), Chapter 6: Due on Thursday, November 5 1. On page 162 of Giancoli, problem 4. 2.
More information14 - OSCILLATIONS Page 1
14 - OSCILLATIONS Page 1 14.1 Perioic an Osciator otion Motion of a sste at reguar interva of tie on a efinite path about a efinite point is known as a perioic otion, e.g., unifor circuar otion of a partice.
More informationPHYSICS LOCUS / / d dt. ( vi) mass, m moment of inertia, I. ( ix) linear momentum, p Angular momentum, l p mv l I
6 n terms of moment of inertia, equation (7.8) can be written as The vector form of the above equation is...(7.9 a)...(7.9 b) The anguar acceeration produced is aong the direction of appied externa torque.
More informationPotential and Kinetic Energy
Potential and Kinetic Energy 1 of 31 Boardworks Ltd 2016 Potential and Kinetic Energy 2 of 31 Boardworks Ltd 2016 What is a system? 3 of 31 Boardworks Ltd 2016 A system is an object or a group of objects.
More informationm k F = "kx T = 2# L T = 2# Notes on Ch. 11 Equations: F = "kx The force (F, measured in Newtons) produced by a spring is equal to the L g T = 2#
Name: Physics Chapter 11 Study Guide ----------------------------------------------------------------------------------------------------- Useful Information: F = "kx T = 2# L T = 2# m v = f$ PE g k e
More informationChemical Kinetics Part 2
Integrated Rate Laws Chemica Kinetics Part 2 The rate aw we have discussed thus far is the differentia rate aw. Let us consider the very simpe reaction: a A à products The differentia rate reates the rate
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@ive.com https://promotephysics.wordpress.com [TORQUE, ANGULAR MOMENTUM & EQUILIBRIUM] CHAPTER NO. 5 Okay here we are going to discuss Rotationa
More informationChapter 2 Physics in Action Sample Problem 1 A weightlifter uses a force of 325 N to lift a set of weights 2.00 m off the ground. How much work did th
Chapter Physics in Action Sample Problem 1 A weightlifter uses a force of 35 N to lift a set of weights.00 m off the ground. How much work did the weightlifter do? Strategy: You can use the following equation
More informationFind the value of λ. (Total 9 marks)
1. A particle of mass 0.5 kg is attached to one end of a light elastic spring of natural length 0.9 m and modulus of elasticity λ newtons. The other end of the spring is attached to a fixed point O 3 on
More informationDemonstration of Ohm s Law Electromotive force (EMF), internal resistance and potential difference Power and Energy Applications of Ohm s Law
Lesson 4 Demonstration of Ohm s Law Eectromotive force (EMF), interna resistance and potentia difference Power and Energy Appications of Ohm s Law esistors in Series and Parae Ces in series and Parae Kirchhoff
More informationTechnical Data for Profiles. Groove position, external dimensions and modular dimensions
Technica Data for Profies Extruded Profie Symbo A Mg Si 0.5 F 25 Materia number.206.72 Status: artificiay aged Mechanica vaues (appy ony in pressing direction) Tensie strength Rm min. 245 N/mm 2 Yied point
More informationTerm Test AER301F. Dynamics. 5 November The value of each question is indicated in the table opposite.
U N I V E R S I T Y O F T O R O N T O Facuty of Appied Science and Engineering Term Test AER31F Dynamics 5 November 212 Student Name: Last Name First Names Student Number: Instructions: 1. Attempt a questions.
More informationKinetic and Potential Energy Old Exam Qs
Kinetic and Potential Energy Old Exam Qs Q. A firework rocket is fired vertically into the air and explodes at its highest point. What are the changes to the total kinetic energy of the rocket and the
More informationMECHANICAL ENGINEERING
1 SSC-JE SFF SELECION COMMISSION MECHNICL ENGINEERING SUDY MERIL Cassroom Posta Correspondence est-series16 Rights Reserved www.sscje.com C O N E N 1. SIMPLE SRESSES ND SRINS 3-3. PRINCIPL SRESS ND SRIN
More informationChapter 5 Oscillatory Motion
Chapter 5 Oscillatory Motion Simple Harmonic Motion An object moves with simple harmonic motion whenever its acceleration is proportional to its displacement from some equilibrium position and is oppositely
More informationAAPT UNITED STATES PHYSICS TEAM AIP 2012 DO NOT DISTRIBUTE THIS PAGE
2012 Semifina Exam 1 AAPT UNITED STATES PHYSICS TEAM AIP 2012 Semifina Exam DO NOT DISTRIBUTE THIS PAGE Important Instructions for the Exam Supervisor This examination consists of two parts. Part A has
More information(Specifications A and B)
Centre Number Surname Candidate Number For Examiner s Use Other Names Candidate Signature Examiner s Initias Genera Certificate of Education Advanced Subsidiary Examination June 2011 Question 1 2 Mark
More informationSTRUCTURE AND PROPERTIES OF LIQUIDS
STUCTUE AND POPETIES O LIQUIDS. Surface tension a) phenomenon The surface of a iquid behaves ike a stretched eastic membrane (proof pond skater, sma drops spheres Expanation: r range of attraction r nm,
More informationAP Physics C - Mechanics
Slide 1 / 84 Slide 2 / 84 P Physics C - Mechanics Energy Problem Solving Techniques 2015-12-03 www.njctl.org Table of Contents Slide 3 / 84 Introduction Gravitational Potential Energy Problem Solving GPE,
More informationPhysics 111. Thursday, Dec. 9, 3-5pm and 7-9pm. Announcements. Tuesday, December 7, Stress Strain. For the rest of the semester
ics day, ember 7, 004 Ch 17: Kinetic Theory Stress Strain Ch 18: 1st Law of Thermodynamics nd Law of Thermodynamics or the rest of the semester Thursday,. 9, 3-5pm and 7-9pm Monday,. 13, 004 10:30 am 1:30
More informationEnergy Problem Solving Techniques.
1 Energy Problem Solving Techniques www.njctl.org 2 Table of Contents Introduction Gravitational Potential Energy Problem Solving GPE, KE and EPE Problem Solving Conservation of Energy Problem Solving
More information14-6 The Equation of Continuity
14-6 The Equation of Continuity 14-6 The Equation of Continuity Motion of rea fuids is compicated and poory understood (e.g., turbuence) We discuss motion of an idea fuid 1. Steady fow: Laminar fow, the
More informationG481 Mark Scheme January Question Expected Answers Marks Additional Guidance 1 (a) Correct lines from:
G48 Mark Scheme January 00 G48 Mechanics (a) Correct lines from: B Note: marks for all correct joule (J) to N m mark for two correct watt (W) to J s - 0 marks for none or one correct newton (N) to kg m
More information- 1 -APPH_MidTerm. Mid - Term Exam. Part 1: Write your answers to all multiple choice questions in this space. A B C D E A B C D E
Name - 1 -APPH_MidTerm AP Physics Date Mid - Term Exam Part 1: Write your answers to all multiple choice questions in this space. 1) 2) 3) 10) 11) 19) 20) 4) 12) 21) 5) 13) 22) 6) 7) 14) 15) 23) 24) 8)
More informationUnit WorkBook 4 Level 4 ENG U8 Mechanical Principles 2018 UniCourse Ltd. All Rights Reserved. Sample
2018 UniCourse Ltd. A Rights Reserved. Pearson BTEC Levels 4 Higher Nationals in Engineering (RQF) Unit 8: Mechanical Principles Unit Workbook 4 in a series of 4 for this unit Learning Outcome 4 Translational
More informationChemical Kinetics Part 2. Chapter 16
Chemica Kinetics Part 2 Chapter 16 Integrated Rate Laws The rate aw we have discussed thus far is the differentia rate aw. Let us consider the very simpe reaction: a A à products The differentia rate reates
More informationHonor Physics Final Exam Review. What is the difference between series, parallel, and combination circuits?
Name Period Date Honor Physics Final Exam Review Circuits You should be able to: Calculate the total (net) resistance of a circuit. Calculate current in individual resistors and the total circuit current.
More informationLab: Energy-Rubber Band Cannon C O N C E P T U A L P H Y S I C S : U N I T 4
Name Date Period Objectives: Lab: Energy-Rubber Band Cannon C O N C E P T U A L P H Y S I C S : U N I T 4 1) Find the energy stored within the rubber band cannon for various displacements. 2) Find the
More information12.2. Maxima and Minima. Introduction. Prerequisites. Learning Outcomes
Maima and Minima 1. Introduction In this Section we anayse curves in the oca neighbourhood of a stationary point and, from this anaysis, deduce necessary conditions satisfied by oca maima and oca minima.
More informationPhysics lab Hooke s Law and Pendulums
Name: Date: Physics lab Hooke s Law and Pendulums Part A: Hooke s Law Introduction Hooke s Law explains the relationship between the force exerted on a spring, the stretch of the string, and the spring
More informationELASTIC STRINGS & SPRINGS
ELASTIC STRINGS & SPRINGS Question 1 (**) A particle of mass m is attached to one end of a light elastic string of natural length l and modulus of elasticity 25 8 mg. The other end of the string is attached
More informationMultiple-Choice questions
AP Physics I Work and Energy Multiple-Choice questions 1. A force F is at an angle θ above the horizontal and is used to pull a heavy suitcase of weight mg a distance d along a level floor at constant
More informationCHAPTER 4 STRESS AND STRAIN
CHPTER STRESS ND STRIN EXERCISE, Page 95. If a oid tone i dropped into the ea and come to ret at a depth of 5000 m beow the urface of the ea, what wi be the tre in the tone? Take the denity of eawater
More informationO -x 0. 4 kg. 12 cm. 3 kg
Anwer, Key { Homework 9 { Rubin H andau 1 Thi print-out houd have 18 quetion. Check that it i compete before eaving the printer. Ao, mutipe-choice quetion may continue on the net coumn or page: nd a choice
More informationMechanics 3. Dimensions and Units
Chapter Assessment Mechanics 3 Dimensions and Units. An attempt is made to model the force of air resistance against a bullet as it flies through the air. It is suggested that the resistance, R, is proportional
More informationExperimental Investigation and Numerical Analysis of New Multi-Ribbed Slab Structure
Experimenta Investigation and Numerica Anaysis of New Muti-Ribbed Sab Structure Jie TIAN Xi an University of Technoogy, China Wei HUANG Xi an University of Architecture & Technoogy, China Junong LU Xi
More informationUniversity of Alabama Department of Physics and Astronomy. PH 105 LeClair Summer Problem Set 11
University of Aabaa Departent of Physics and Astronoy PH 05 LeCair Suer 0 Instructions: Probe Set. Answer a questions beow. A questions have equa weight.. Due Fri June 0 at the start of ecture, or eectronicay
More informationParallel-Axis Theorem
Parae-Axis Theorem In the previous exampes, the axis of rotation coincided with the axis of symmetry of the object For an arbitrary axis, the paraeaxis theorem often simpifies cacuations The theorem states
More informationAQA Maths M2. Topic Questions from Papers. Energy, Work and Power. Answers
AQA Maths M Topic Questions from Papers Energy, Work and Power Answers PhysicsAndMathsTutor.com 4(a) P (30 4) 4 590 W AG Finding force Correct answer from P Fv (b)(i) F 00 9.8sin5 + 30v Finding force.
More informationWork and Energy Definition of work Examples. Definition of Mechanical Energy. Conservation of Mechanical Energy, Pg 1
Work and Energy Definition of work Examples Work and Energy Today s Agenda Definition of Mechanical Energy Conservation of Mechanical Energy Conservative forces Conservation of Mechanical Energy, Pg 1
More informationWORK, POWER & ENERGY
WORK, POWER & ENERGY Work An applied force acting over a displacement. The force being applied must be parallel to the displacement for work to be occurring. Work Force displacement Units: Newton meter
More informationMark Scheme (Results) January Pearson Edexcel International Advanced Level. Mechanics 3 (WME03/01)
Mark Scheme (Resuts) January 04 Pearson Edexce Internationa Advanced Leve Mechanics 3 (WME03/0) Edexce and BTEC Quaifications Edexce and BTEC quaifications are awarded by Pearson, the UK s argest awarding
More informationQuantum Mechanical Models of Vibration and Rotation of Molecules Chapter 18
Quantum Mechanica Modes of Vibration and Rotation of Moecues Chapter 18 Moecuar Energy Transationa Vibrationa Rotationa Eectronic Moecuar Motions Vibrations of Moecues: Mode approximates moecues to atoms
More informationAnother Method to get a Sine Wave. X = A cos θ V = Acc =
LAST NAME FIRST NAME DATE PER CJ Wave Assignment 10.3 Energy & Simple Harmonic Motion Conceptual Questions 3, 4, 6, 7, 9 page 313 6, 7, 33, 34 page 314-316 Tracing the movement of the mass on the end of
More informationLesson 8: Work and Energy
Name Period Lesson 8: Work and Energy 8.1 Experiment: What is Kinetic Energy? (a) Set up the cart, meter stick, pulley, hanging mass, and tape as you did in Lesson 5.1. You will examine the distance and
More informationWork and Energy Experiments
Work and Energy Experiments Experiment 16 When a juggler tosses a bean ball straight upward, the ball slows down until it reaches the top of its path and then speeds up on its way back down. In terms of
More informationc 2007 Society for Industrial and Applied Mathematics
SIAM REVIEW Vo. 49,No. 1,pp. 111 1 c 7 Society for Industria and Appied Mathematics Domino Waves C. J. Efthimiou M. D. Johnson Abstract. Motivated by a proposa of Daykin [Probem 71-19*, SIAM Rev., 13 (1971),
More informationWork done by multiple forces. WEST VIRGINIA UNIVERSITY Physics
Work done by multiple forces Work done by multiple forces no normal work tractor work friction work total work = W T +W f = +10 kj no weight work Work-Energy: Finding the Speed total work = W T +W f =
More informationSolution Set Seven. 1 Goldstein Components of Torque Along Principal Axes Components of Torque Along Cartesian Axes...
: Soution Set Seven Northwestern University, Cassica Mechanics Cassica Mechanics, Third Ed.- Godstein November 8, 25 Contents Godstein 5.8. 2. Components of Torque Aong Principa Axes.......................
More informationA. B. C. D. E. v x. ΣF x
Q4.3 The graph to the right shows the velocity of an object as a function of time. Which of the graphs below best shows the net force versus time for this object? 0 v x t ΣF x ΣF x ΣF x ΣF x ΣF x 0 t 0
More informationCABLE SUPPORTED STRUCTURES
CABLE SUPPORTED STRUCTURES STATIC AND DYNAMIC ANALYSIS OF CABLES 3/22/2005 Prof. dr Stanko Brcic 1 Cabe Supported Structures Suspension bridges Cabe-Stayed Bridges Masts Roof structures etc 3/22/2005 Prof.
More informationPage 2. What is the main purpose of the steel core? To force more current into the outer sheath.
Q1.The overhead cables used to transmit electrical power by the National Grid usually consist of a central core of steel cables surrounded by a sheath of cables of low resistivity material, such as aluminium.
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 informationTHE THREE POINT STEINER PROBLEM ON THE FLAT TORUS: THE MINIMAL LUNE CASE
THE THREE POINT STEINER PROBLEM ON THE FLAT TORUS: THE MINIMAL LUNE CASE KATIE L. MAY AND MELISSA A. MITCHELL Abstract. We show how to identify the minima path network connecting three fixed points on
More information1. Measurements and error calculus
EV 1 Measurements and error cacuus 11 Introduction The goa of this aboratory course is to introduce the notions of carrying out an experiment, acquiring and writing up the data, and finay anayzing the
More informationPhysics 2414 Group Exercise 8. Conservation of Energy
Physics 244 Group Exercise 8 Name : OUID : Name 2: OUID 2: Name 3: OUID 3: Name 4: OUID 4: Section Number: Solutions Solutions Conservation of Energy A mass m moves from point i to point f under the action
More informationSEMINAR 2. PENDULUMS. V = mgl cos θ. (2) L = T V = 1 2 ml2 θ2 + mgl cos θ, (3) d dt ml2 θ2 + mgl sin θ = 0, (4) θ + g l
Probem 7. Simpe Penduum SEMINAR. PENDULUMS A simpe penduum means a mass m suspended by a string weightess rigid rod of ength so that it can swing in a pane. The y-axis is directed down, x-axis is directed
More informationthe spring is compressed and x is the compression
Lecture 4 Spring problem and conservation of mechanical energy Hooke's Law The restoring force exerted by the spring is directly proportional to its displacement. The restoring force acts in a direction
More information( ) = ( ) W net = ΔKE = KE f KE i W F. F d x. KE = 1 2 mv2. Note: Work is the dot product of F and d. Work-Kinetic Energy Theorem
Work-Kinetic Energy Theorem KE = 1 2 mv2 W F change in the kinetic energy of an object F d x net work done on the particle ( ) = ( ) W net = ΔKE = KE f KE i Note: Work is the dot product of F and d W g
More informationPhysics. Chapter 7 Energy
Physics Chapter 7 Energy Work How long does a force act? Last week, we meant time as in impulse (Ft) This week, we will take how long to mean distance Force x distance (Fd) is what we call WORK W = Fd
More information4. What is the equation for the Work-Kinetic Energy theorem and what does it mean?
Bell Ringer: 1. What is a force? 2. What is Newton s 2 nd Law? 3. What is work? 4. What is the equation for the Work-Kinetic Energy theorem and what does it mean? Notes 6.1: Work done by a Spring Force
More informationCrystallisation of a supercooled spherical nodule in a flow
EUROTHERM 69 Heat and Mass Transfer in Soid-Liquid Phase hange Processes June 25-27, 2003, Bistra caste, Ljubjana, Sovenia Eds.: B. Sarer, D. Gobin rystaisation of a supercooed spherica nodue in a fow
More informationPhysicsAndMathsTutor.com
M Dynmics - Dmped nd forced hrmonic motion. A P α B A ight estic spring hs ntur ength nd moduus of esticity mg. One end of the spring is ttched to point A on pne tht is incined to the horizont t n nge
More informationFourier series. Part - A
Fourier series Part - A 1.Define Dirichet s conditions Ans: A function defined in c x c + can be expanded as an infinite trigonometric series of the form a + a n cos nx n 1 + b n sin nx, provided i) f
More informationSTABILITY OF A PARAMETRICALLY EXCITED DAMPED INVERTED PENDULUM 1. INTRODUCTION
Journa of Sound and Vibration (996) 98(5), 643 65 STABILITY OF A PARAMETRICALLY EXCITED DAMPED INVERTED PENDULUM G. ERDOS AND T. SINGH Department of Mechanica and Aerospace Engineering, SUNY at Buffao,
More informationMechanics 2. Revision Notes
Mechanics 2 Revision Notes October 2016 2 M2 OCTOER 2016 SD Mechanics 2 1 Kinematics 3 Constant acceleration in a vertical plane... 3 Variable acceleration... 5 Using vectors... 6 2 Centres of mass 7 Centre
More informationSimple Harmonic Motion
3/5/07 Simple Harmonic Motion 0. The Ideal Spring and Simple Harmonic Motion HOOKE S AW: RESTORING FORCE OF AN IDEA SPRING The restoring force on an ideal spring is F x k x spring constant Units: N/m 3/5/07
More informationVersion 2.2 NE03 - Faraday's Law of Induction
Definition Version. Laboratory Manua Department of Physics he University of Hong Kong Aims o demonstrate various properties of Faraday s Law such as: 1. Verify the aw.. Demonstrate the ighty damped osciation
More information<This Sheet Intentionally Left Blank For Double-Sided Printing>
21 22 Transformation Of Mechanical Energy Introduction and Theory One of the most powerful laws in physics is the Law of Conservation of
More informationNATIONAL SENIOR CERTIFICATE GRADE 12 PHYSICAL SCIENCES: CHEMISTRY (P2) COMMON TEST JUNE 2014
Physica Science/P2 1 June 2014 Common Test MARKS: 100 TIME: 2 hours NATIONAL SENIOR CERTIFICATE GRADE 12 PHYSICAL SCIENCES: CHEMISTRY (P2) COMMON TEST JUNE 2014 This question paper consists of 10 pages
More informationLecture 9. Stability of Elastic Structures. Lecture 10. Advanced Topic in Column Buckling
Lecture 9 Stabiity of Eastic Structures Lecture 1 Advanced Topic in Coumn Bucking robem 9-1: A camped-free coumn is oaded at its tip by a oad. The issue here is to find the itica bucking oad. a) Suggest
More informationChapter 13. Simple Harmonic Motion
Chapter 13 Simple Harmonic Motion Hooke s Law F s = - k x F s is the spring force k is the spring constant It is a measure of the stiffness of the spring A large k indicates a stiff spring and a small
More information