Physics Dynamics: Springs
|
|
- Annabel Brown
- 6 years ago
- Views:
Transcription
1 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
2 Question Springs in Tite Series and Parae k s
3 Question Tite Vertica Springs I A 0.50 m spring with spring constant 100 N/m hangs from the ceiing. A 2.0 kg bock is tied to the spring. How much does the spring stretch? (Use g = 10 m/s 2 ) A. 2.0 m B m C m D m E m 0.5 m 0.5 m? 2 kg
4 Comments Soution Answer: D Justification: The 2.0 kg mass appies a 20 N force downwards on the spring (this force is caused by gravity the pu of the Earth). In order to support the 20 N downward force, the spring must appy a 20 N force upwards. Assume upwards is positive and downwards is negative. F kd S 20 N ( 100 N/m) d d 0.20 m Therefore, the spring wi stretch (etend downwards) by 0.20 m. The tota ength of the spring wi be 0.70 m, but the stretch is ony 20 cm.
5 Question Tite Vertica Springs II A spring with ength and spring constant k s hangs from the ceiing. A mass m is paced on the spring and increases the ength of the spring by. By how much wi a 2m mass stretch the spring from its origina - un-stretched state? A. The spring wi stretch by 2. B. The spring wi stretch by. C. The spring wi stretch by 0.5. m? m m
6 Comments Soution Answer: A Justification: The tension force of a spring is directy proportiona to the amount it is compressed or stretched from its rest position: F = -k. A 2m mass wi eert a downward force twice as arge as a 1m mass. Thus the spring must stretch twice as much in order to hod the 2m mass.
7 Question Tite Vertica Springs III A singe spring is stretched by when a mass m is attached. An identica spring is joined in series to the first spring. How much wi the two springs stretch when a mass m is attached? (Assume the springs have negigibe mass) m A. The spring wi stretch by 2 since each spring stretches by B. The spring wi stretch by since the spring constant remains the same C. The spring wi stretch by 0.5 since there are 2 springs hoding the mass D. There is not enough information to answer
8 Comments Soution Answer: A Justification: For springs with negigibe mass, the tension aong them has to be constant at a points. Since the tension of the spring hoding the mass is equa to mg, the tension of the other spring is aso mg. Each spring stretches by, causing a tota stretch of 2. This means that two identica springs connected in series wi stretch twice as much as one spring woud have stretched! m
9 Question Tite Vertica Springs IV Two identica springs (each with spring constant k s ) are connected in series as shown. What is the spring constant of the two springs together (k T )? (Assume the springs have negigibe mass) A. k T = 2k s B. k T = k s C. k T = 0.5k s D. Cannot be determined
10 Comments Soution Answer: C Justification: From question III, we earned that doubing the ength of a spring wi cause it to stretch twice as much. The spring becomes weaker, since a smaer force is required to stretch it by the same amount. The spring constant is therefore haved: F T F k (2 ) k T k d T F 1 F k s
11 Question Tite Vertica Springs V A singe spring is stretched by when a mass m is attached. An identica spring is joined in parae to the first spring. How much wi the two springs stretch when a mass m is attached to both springs simutaneousy? (Assume the springs have negigibe mass) A. The spring wi stretch by 2 since each spring stretches by B. The spring wi stretch by since the spring constant remains the same m C. The spring wi stretch by 0.5 since there are 2 springs hoding the mass m
12 Comments Soution Answer: C Justification: The downward force mg is now supported by 2 separate springs. Each spring must then eert an upward force mg equa to 2. Therefore, each spring wi stretch haf as much, or. 2 2 m
13 Question Tite Vertica Springs VI Two identica springs (each with spring constant k s ) are connected in parae as shown. What is the spring constant of the two springs together (k T )? (Assume the springs have negigibe mass) A. k T = 2k s B. k T = k s C. k T = 0.5k s D. Cannot be determined
14 Comments Soution Answer: A Justification: We earned from question 5 that two springs in parae wi stretch haf as much as a singe spring with the same mass attached. It requires twice as much force to stretch the two springs. The two springs are stronger and have twice the spring constant. F k d F k T T kt( ) 2 2F F 2 2k s
15 Question Tite Vertica Springs VII Which coection of springs has the argest spring constant? A. B. C. D. E. A have the same spring constant
16 Comments Soution Answer: D Justification: Spring A has 3 springs in series, so the spring constant is k s. 3 Spring B and Spring C have springs connected in parae and in series. The springs in parae stretch 0.5, and the singe spring stretches. The tota stretch is 1.5, giving a spring constant of Spring D has 3 springs in parae, so the spring constant is 3k s. For this case: F k d F k T T kt( ) 3 3F F 3 3k s 2k s 3
Mechanics 3. Elastic strings and springs
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
More informationSure Shot 2016 Electric Current By M K Ezaz
Sure Shot 06 Eectric Current B M K Ezaz. A 0 V batter of negigibe interna resistance is connected across a 00 V batter and a resistance of 38 Ω. Find the vaue of the current in circuit. () E 00 0 A: I
More informationMathematics Arithmetic Sequences
a place of mind F A C U L T Y O F E D U C A T I O N Department of Curriculum and Pedagogy Mathematics Arithmetic Sequences Science and Mathematics Education Research Group Supported by UBC Teaching and
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 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 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 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 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 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 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 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 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 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 information(Refer Slide Time: 2:34) L C V
Microwave Integrated Circuits Professor Jayanta Mukherjee Department of Eectrica Engineering Indian Intitute of Technoogy Bombay Modue 1 Lecture No 2 Refection Coefficient, SWR, Smith Chart. Heo wecome
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 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 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 informationSelf Inductance of a Solenoid with a Permanent-Magnet Core
1 Probem Sef Inductance of a Soenoid with a Permanent-Magnet Core Kirk T. McDonad Joseph Henry Laboratories, Princeton University, Princeton, NJ 08544 (March 3, 2013; updated October 19, 2018) Deduce the
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 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 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 informationMathematics Functions: Logarithms
a place of mind F A C U L T Y O F E D U C A T I O N Department of Curriculum and Pedagogy Mathematics Functions: Logarithms Science and Mathematics Education Research Group Supported by UBC Teaching and
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 informationMathematics Numbers: Absolute Value of Functions I
a place of mind F A C U L T Y O F E D U C A T I O N Department of Curriculum and Pedagogy Mathematics Numbers: Absolute Value of Functions I Science and Mathematics Education Research Group Supported by
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 informationThe Binary Space Partitioning-Tree Process Supplementary Material
The inary Space Partitioning-Tree Process Suppementary Materia Xuhui Fan in Li Scott. Sisson Schoo of omputer Science Fudan University ibin@fudan.edu.cn Schoo of Mathematics and Statistics University of
More informationSydU STAT3014 (2015) Second semester Dr. J. Chan 18
STAT3014/3914 Appied Stat.-Samping C-Stratified rand. sampe Stratified Random Samping.1 Introduction Description The popuation of size N is divided into mutuay excusive and exhaustive subpopuations caed
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 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 informationPhysics 1-D Kinematics: Relative Velocity
a place of mind F A C U L T Y O F E D U C A T I O N Department of Curriculum and Pedagogy Physics 1-D Kinematics: Relative Velocity Science and Mathematics Education Research Group Supported by UBC Teaching
More informationPhysicsAndMathsTutor.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 informationChapter 4. Moving Observer Method. 4.1 Overview. 4.2 Theory
Chapter 4 Moving Observer Method 4.1 Overview For a compete description of traffic stream modeing, one woud reuire fow, speed, and density. Obtaining these parameters simutaneousy is a difficut task if
More informationPhysics Dynamics: Forces. Science and Mathematics Education Research Group
F F CULTY C U L T Y OF O F EDUCTION E D U C T I O N Department of Curriculum and Pedagogy Physics Dynamics: Forces Science and Mathematics Education Research Group Supported by UBC Teaching and Learning
More informationPhysics Circuits: Series
FACULTY OF EDUCATION Department of Curriculum and Pedagogy Physics Circuits: Series Science and Mathematics Education Research Group Supported by UBC Teaching and Learning Enhancement Fund 2012-2013 Series
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 information(1) Class Test Solution (STRUCTURE) Answer key. 31. (d) 32. (b) 33. (b) IES MASTER. 34. (c) 35. (b) 36. (c) 37. (b) 38. (c) 39.
() ass Test Soution (STRUTUR) 7-09-07 nswer key. (b). (b). (c). (a) 5. (b) 6. (a) 7. (c) 8. (c) 9. (b) 0. (d). (c). (d). (d). (c) 5. (d) 6. (a) 7. (c) 8. (d) 9. (b) 0. (c). (a). (a). (b) (b) 5. (b) 6.
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 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 informationPhysics Circular Motion Problems. 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 Department of Curriculum and Pedagogy Physics Circular Motion Problems Science and Mathematics Education Research Group Supported by UBC Teaching
More informationF A C U L T Y O F E D U C A T I O N. Physics Electromagnetism: Induced Currents Science and Mathematics Education Research Group
F A C U L T Y O F E D U C A T I O N Department of Curriculum and Pedagogy Physics Electromagnetism: Induced Currents Science and Mathematics Education Research Group Supported by UBC Teaching and Learning
More informationEnergy Problems. 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 Department of Curriculum and Pedagogy Energy Problems Science and Mathematics Education Research Group Supported by UBC Teaching and Learning Enhancement
More informationXSAT of linear CNF formulas
XSAT of inear CN formuas Bernd R. Schuh Dr. Bernd Schuh, D-50968 Kön, Germany; bernd.schuh@netcoogne.de eywords: compexity, XSAT, exact inear formua, -reguarity, -uniformity, NPcompeteness Abstract. Open
More informationBrine Discharge Plumes on a Sloping Beach
Brine Discharge Pumes on a Soping Beach H.H. AL-BARWANI, Anton PURNAMA Department of Mathematics and Statistics, Coege of Science Sutan Qaboos Universit, PO Bo 6, A-Khod 1, Muscat, Sutanate of Oman E-mai:
More informationMultiple Beam Interference
MutipeBeamInterference.nb James C. Wyant 1 Mutipe Beam Interference 1. Airy's Formua We wi first derive Airy's formua for the case of no absorption. ü 1.1 Basic refectance and transmittance Refected ight
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 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 informationUnit 48: Structural Behaviour and Detailing for Construction. Deflection of Beams
Unit 48: Structura Behaviour and Detaiing for Construction 4.1 Introduction Defection of Beams This topic investigates the deformation of beams as the direct effect of that bending tendency, which affects
More informationTraffic data collection
Chapter 32 Traffic data coection 32.1 Overview Unike many other discipines of the engineering, the situations that are interesting to a traffic engineer cannot be reproduced in a aboratory. Even if road
More information(1) Class Test Solution (STRUCTURE) Answer key. 31. (d) 32. (b) 33. (b) IES MASTER. 34. (c) 35. (b) 36. (c) 37. (b) 38. (c) 39.
() ass Test Soution (STRUTUR) 7-08-08 nswer key. (b). (b). (c). (a) 5. (b) 6. (a) 7. (c) 8. (c) 9. (b) 0. (d). (c). (d). (d). (c) 5. (b, d) 6. ( ) 7. (c) 8. (d) 9. (b) 0. (c). (a). (a). (b) (b) 5. (b)
More informationGauss Law. 2. Gauss s Law: connects charge and field 3. Applications of Gauss s Law
Gauss Law 1. Review on 1) Couomb s Law (charge and force) 2) Eectric Fied (fied and force) 2. Gauss s Law: connects charge and fied 3. Appications of Gauss s Law Couomb s Law and Eectric Fied Couomb s
More informationEECS 117 Homework Assignment 3 Spring ω ω. ω ω. ω ω. Using the values of the inductance and capacitance, the length of 2 cm corresponds 1.5π.
EES 7 Homework Assignment Sprg 4. Suppose the resonant frequency is equa to ( -.5. The oad impedance is If, is equa to ( ( The ast equaity hods because ( -.5. Furthermore, ( Usg the vaues of the ductance
More informationChapter 4 ( ) ( ) F Fl F y = = + Solving for k. k kt. y = = + +
Chapter 4 4- For a torsion bar, k T T/ F/, and so F/k T. For a cantiever, k F/δ,δ F/k. For the assemby, k F/y, or, y F/k + δ Thus F F F y + k kt k Soving for k kkt k ns. k + kt + kt k 4- For a torsion
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 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 informationJackson 4.10 Homework Problem Solution Dr. Christopher S. Baird University of Massachusetts Lowell
Jackson 4.10 Homework Probem Soution Dr. Christopher S. Baird University of Massachusetts Lowe PROBLEM: Two concentric conducting spheres of inner and outer radii a and b, respectivey, carry charges ±.
More informationHigh Efficiency Development of a Reciprocating Compressor by Clarification of Loss Generation in Bearings
Purdue University Purdue e-pubs Internationa Compressor Engineering Conference Schoo of Mechanica Engineering 2010 High Efficiency Deveopment of a Reciprocating Compressor by Carification of Loss Generation
More informationChapter 4. Forces and Newton s Laws of Motion. continued
Chapter 4 Forces and Newton s Laws of Motion continued Quiz 3 4.7 The Gravitational Force Newton s Law of Universal Gravitation Every particle in the universe exerts an attractive force on every other
More informationLaboratory Exercise 1: Pendulum Acceleration Measurement and Prediction Laboratory Handout AME 20213: Fundamentals of Measurements and Data Analysis
Laboratory Exercise 1: Penduum Acceeration Measurement and Prediction Laboratory Handout AME 20213: Fundamentas of Measurements and Data Anaysis Prepared by: Danie Van Ness Date exercises to be performed:
More informationNotes 32 Magnetic Force and Torque
ECE 3318 Appied Eectricity and Magnetism Spring 18 Prof. David R. Jackson Dept. of ECE Notes 3 Magnetic orce and Torque 1 orce on Wire q Singe charge: = q( v ) v (derivation omitted) Wire: = d C d orce
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 information<C 2 2. λ 2 l. λ 1 l 1 < C 1
Teecommunication Network Contro and Management (EE E694) Prof. A. A. Lazar Notes for the ecture of 7/Feb/95 by Huayan Wang (this document was ast LaT E X-ed on May 9,995) Queueing Primer for Muticass Optima
More informationPhysics 1 Second Midterm Exam (AM) 2/25/2010
Physics Second Midterm Eam (AM) /5/00. (This problem is worth 40 points.) A roller coaster car of m travels around a vertical loop of radius R. There is no friction and no air resistance. At the top of
More informationCoded Caching for Files with Distinct File Sizes
Coded Caching for Fies with Distinct Fie Sizes Jinbei Zhang iaojun Lin Chih-Chun Wang inbing Wang Department of Eectronic Engineering Shanghai Jiao ong University China Schoo of Eectrica and Computer Engineering
More informationSOLUTION a. Since the applied force is equal to the person s weight, the spring constant is 670 N m ( )( )
5. ssm A person who weighs 670 N steps onto a spring scale in the bathroom, and the spring compresses by 0.79 cm. (a) What is the spring constant? (b) What is the weight of another person who compresses
More informationChapter 7 PRODUCTION FUNCTIONS. Copyright 2005 by South-Western, a division of Thomson Learning. All rights reserved.
Chapter 7 PRODUCTION FUNCTIONS Copyright 2005 by South-Western, a division of Thomson Learning. A rights reserved. 1 Production Function The firm s production function for a particuar good (q) shows the
More informationSECTION A. Question 1
SECTION A Question 1 (a) In the usua notation derive the governing differentia equation of motion in free vibration for the singe degree of freedom system shown in Figure Q1(a) by using Newton's second
More informationMerging to ordered sequences. Efficient (Parallel) Sorting. Merging (cont.)
Efficient (Paae) Soting One of the most fequent opeations pefomed by computes is oganising (soting) data The access to soted data is moe convenient/faste Thee is a constant need fo good soting agoithms
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 informationConcept of Force Challenge Problem Solutions
Concept of Force Challenge Problem Solutions Problem 1: Force Applied to Two Blocks Two blocks sitting on a frictionless table are pushed from the left by a horizontal force F, as shown below. a) Draw
More informationChemistry Atomic Theory: Model of the Atom Science and Mathematics Education Research Group
a place of mind F A C U L T Y O F E D U C A T I O N Department of Curriculum and Pedagogy Chemistry Atomic Theory: Model of the Atom Science and Mathematics Education Research Group Supported by UBC Teaching
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 informationOld Exam. Question Chapter 7 072
Old Exam. Question Chapter 7 072 Q1.Fig 1 shows a simple pendulum, consisting of a ball of mass M = 0.50 kg, attached to one end of a massless string of length L = 1.5 m. The other end is fixed. If the
More informationPhysical Science Astronomy: Eclipses
a place of mind F A C U L T Y O F E D U C A T I O N Department of Curriculum and Pedagogy Physical Science Astronomy: Eclipses Science and Mathematics Education Research Group Supported by UBC Teaching
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 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 informationSeparation of Variables and a Spherical Shell with Surface Charge
Separation of Variabes and a Spherica She with Surface Charge In cass we worked out the eectrostatic potentia due to a spherica she of radius R with a surface charge density σθ = σ cos θ. This cacuation
More informationLobontiu: System Dynamics for Engineering Students Website Chapter 3 1. z b z
Chapter W3 Mechanica Systems II Introduction This companion website chapter anayzes the foowing topics in connection to the printed-book Chapter 3: Lumped-parameter inertia fractions of basic compiant
More informationForce mediated by a field - long range: action at a distance: The attractive or repulsion between two stationary charged objects.
VISUAL PHYSICS ONLINE DYNAMICS TYPES O ORCES 1 Electrostatic force orce mediated by a field - long range: action at a distance: The attractive or repulsion between two stationary charged objects. AB A
More informationWhich expression gives the elastic energy stored in the stretched wire?
1 wire of length L and cross-sectional area is stretched a distance e by a tensile force. The Young modulus of the material of the wire is E. Which expression gives the elastic energy stored in the stretched
More informationDynamics: Forces and Newton s Laws of Motion
Lecture 7 Chapter 5 Physics I Dynamics: Forces and Newton s Laws of Motion Course website: http://faculty.uml.edu/andriy_danylov/teaching/physicsi Today we are going to discuss: Chapter 5: Force, Mass:
More informationPhysics Momentum: Collisions. 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 Deartment of Curriculum and Pedagogy Physics Momentum: Collisions Science and Mathematics Education Research Grou Suorted by UBC Teaching and Learning
More informationQuestion ( ) Solution. Approximate length of an atomic bond for solid aluminum.
Question (1450001) Approximate length of an atomic bond for solid aluminum. Spring A of stiness 10 N/m is hung vertically from a ringstand. From the lower end of this spring, a dierent spring (Spring B)
More informationChemistry Stoichiometry: Mole Ratios
a place of mind F A C U L T Y O F E D U C A T I O N Department of Curriculum and Pedagogy Chemistry Stoichiometry: Mole Ratios Science and Mathematics Education Research Group Supported by UBC Teaching
More informationPhysics Circular Motion
FACULTY OF EDUCATION Department of Curriculum and Pedagogy Physics Circular Motion Science and Mathematics Education Research Group Supported by UBC Teaching and Learning Enhancement Fund 2012-2015 Question
More informationElastic Potential Energy and Conservation of Mechanical Energy
Elastic Potential Energy and Conservation of Mechanical Energy Level : Physics I Instructor : Kim Hook s Law Springs are familiar objects that have many applications, ranging from push-button switches
More informationMathematics Numbers: Absolute Value of Functions II
a place of mind F A C U L T Y O F E D U C A T I O N Department of Curriculum and Pedagogy Mathematics Numbers: Absolute Value of Functions II Science and Mathematics Education Research Group Supported
More informationLecture 6: Moderately Large Deflection Theory of Beams
Structura Mechanics 2.8 Lecture 6 Semester Yr Lecture 6: Moderatey Large Defection Theory of Beams 6.1 Genera Formuation Compare to the cassica theory of beams with infinitesima deformation, the moderatey
More informationStochastic Complement Analysis of Multi-Server Threshold Queues. with Hysteresis. Abstract
Stochastic Compement Anaysis of Muti-Server Threshod Queues with Hysteresis John C.S. Lui The Dept. of Computer Science & Engineering The Chinese University of Hong Kong Leana Goubchik Dept. of Computer
More informationInternational Journal of Advance Engineering and Research Development
Scientific Journa of Impact Factor (SJIF): 4.4 Internationa Journa of Advance Engineering and Research Deveopment Voume 3, Issue 3, March -206 e-issn (O): 2348-4470 p-issn (P): 2348-6406 Study and comparison
More informationSession : Electrodynamic Tethers
Session : Eectrodynaic Tethers Eectrodynaic tethers are ong, thin conductive wires depoyed in space that can be used to generate power by reoving kinetic energy fro their orbita otion, or to produce thrust
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 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 informationMA 201: Partial Differential Equations Lecture - 10
MA 201: Partia Differentia Equations Lecture - 10 Separation of Variabes, One dimensiona Wave Equation Initia Boundary Vaue Probem (IBVP) Reca: A physica probem governed by a PDE may contain both boundary
More informationThe HALO-2 Supernova Detector
The HALO-2 Supernova Detector Vucano Workshop 2016 FRONTIER OBJECTS IN ASTROPHYSICS AND PARTICLE PHYSICS Carence J. Virtue Outine Science Motivation Supernovae in genera Lead-based detectors in particuar
More informationLecture 17 - The Secrets we have Swept Under the Rug
Lecture 17 - The Secrets we have Swept Under the Rug Today s ectures examines some of the uirky features of eectrostatics that we have negected up unti this point A Puzze... Let s go back to the basics
More informationDiscrete Techniques. Chapter Introduction
Chapter 3 Discrete Techniques 3. Introduction In the previous two chapters we introduced Fourier transforms of continuous functions of the periodic and non-periodic (finite energy) type, as we as various
More informationA Brief Introduction to Markov Chains and Hidden Markov Models
A Brief Introduction to Markov Chains and Hidden Markov Modes Aen B MacKenzie Notes for December 1, 3, &8, 2015 Discrete-Time Markov Chains You may reca that when we first introduced random processes,
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 informationCE601-Structura Anaysis I UNIT-IV SOPE-DEFECTION METHOD 1. What are the assumptions made in sope-defection method? (i) Between each pair of the supports the beam section is constant. (ii) The joint in
More information