Kinematics, Dynamics & Control
|
|
- Sabrina Butler
- 6 years ago
- Views:
Transcription
1 Kiematics, Dyamics & Cotol DH aametes Ais (i-) Ais i Velocity/oce Duality i- i = i- Li i- z i- i- a i- z i a i i Li i i } i c i -s i 0 a i- s i c i- c i c i- -s i- -s i- i s i s i- c i s i- c i- c i- i J J Reesetatios R Catesia Sheical Cyliical. Eule Agles Diectio Cosies Eule aametes Jacobia fo X Gie a eesetatio Basic Jacobia J ( q) q J q E J q ( ) ( ) ( ) 0 J ( ) 0 q q R
2 Basic Jacobia Jacobia a Basic Jacobia {0} liea elocity agula elocity J J 0 X E J JXR 0 ER Jw I GJ HK (6 ) J ( q) q 0 ( 6 ) ( ) Jq ( ) EX ( ) J( q) J ( ) 0 q q 0 ositio Reesetatios E( ) Catesia Cooiates (, yz, ) E ( ) I3 Cyliical Cooiates (,, z) Usig ( y z) ( cos si z) E cos si 0 ( X) si cos E Sheical Cooiates (,, ) Usig ( y z) ( cossi sisi cos ) cos si sisi cos ( X) si cos 0 si si cos cos si cos si ositio Reesetatios (iese) Catesia Cooiates (, y, z) E ( X) I E E ( ) Cyliical Cooiates (,, z) 3 cos si 0 ( X) si cos E Sheical Cooiates (,, ) cos si sisi cos cos ( X) si si cossi si cos cos 0 si
3 Rotatio Reesetatios Diectio Cosies ˆ ˆ ; E( ) ˆ 3 3 E Diectio Cosies Rotatio Eo Istataeous Agula Eo ; E E Istataeous Agula Eo esie 3 3 ˆ ˆ ˆ 33 E Eule Agles SC CC S S E ( X) C S 0 S C 0 S S 0 cos si si 0 si cos si 0 cos Eule aametes 0 3 E E
4 E Eule aametes E q : Joit Sace Dyamics M ( q): V( q, q ): Gq ( ): : M( q) q V( q, q ) G( q) Geealize Joit Cooiates Mass Mati - Kietic Eegy Mati Cetifugal a Coiolis foces Gaity foces Geealize foces D Cotol Stability Mqq () Bqqq ()[ ] Cqq ()[ ] G () ( qq ) q V / ( qq ) K K V V s ( ) q t q q q q D Cotol Stability Mqq () Bqqq ()[ ] Cqq ()[ ] G () ( qq ) q V / ( qq ) ( qq ) K K ( Vs V ) ( ) s t q q q s q with q 0 fo q 0; 0 s efomace High Gais bette istubace ejectio Gais ae limite by stuctual fleibilities time elays (actuato-sesig) samlig ate es lowest stuctual fleibility elay I lagest elay 3 HG elay KJ samligate 5 Noliea Dyamic Decoulig M( ) V(, ) G( ) M ( ) V (, ) G ( ). ( M M ) M [( V V ) ( G G )] with efect estimates. ( t) : iut of the uit-mass systems ( ) ( ) Close-loo E E E 0 () t 4
5 q q - e - e q Mq ( ) Am q q a f Bqq (, ) Cqq, Gq ( ) as Oiete Cotol Joit Sace Cotol Joit Sace Cotol Oeatioal Sace Cotol Uifie Motio & oce Cotol ( ) V Goal motio V( Goal ) J cotact motio cotact 5
6 Oeatioal Sace Dyamics M V G [ Mˆ, Vˆ, Gˆ, V( )] Goal as-oiete Equatios of Motio {0} { } 0 No-Reuat Maiulato ; m m q qq q : Oeatioal Sace Dyamics M ( ) V(, ) G( ) E-Effecto ositio a Oietatio M ( ): E-Effecto Kietic Eegy Mati V (, ): E-Effecto Cetifugal a Coiolis foces G ( ): E-Effecto Gaity foces : E-Effecto Geealize foces Joit Sace/as Sace Relatioshis Kietic Eegy K (, ) K ( q qq, ) M ( ) qmqq ( ) Usig Jqq ( ) q ( J MJ) q q M q Joit Sace/as Sace Relatioshis E-Effecto Cotol M ( ) J ) ( q) M ( q J ( q) V (, ) J ( q) V( q, q ) M ( q) h( q, q ) G ( ) J ( q) G( q) whee hqq (, ) Jqq ( ) J ( q) 6
7 assie Systems (Stability) V goal g g ( K V) ( K V) System t V ˆ goal V X K K V Coseatie oces goal 0 t Stable Asymtotic Stability a system is asymtotically stable if s 0 ; fo 0 0 s Cotol Gˆ goal K K VV goal 0 s t s Noliea Dyamic Decoulig Moel M ( ) V (, ) G ( ) Cotol Stuctue Mˆ ( ) ' Vˆ (, ) Gˆ ( ) Decoule System I ' with J efect Estimates ' I ' iut of ecoule e-effecto Goal ositio Cotol ' ' ' g Close Loo I ( ) 0 ' ' g Close Loo g g I m0 g ma D Cotol * g Velocity-Lie Cotol * g t 7
8 g * g * with V ma sat if sat sig( ) if 0 ma ajectoy acig ajectoy:,, I ' ' ' ( ) ( ) ' ' ( ) ( ) ( ) 0 o 0 ' ' with I joit sace as-oiete Cotol 0 ' ' q q q with qq q - e - e a f M ( q) J q Am q q af af Ki q Jq V (, ) q q G ( q) 8
9 Comliace I ( ) y 0 0 z ' ' set to zeo ( ) 0 y y ( y y ) 0 ' ' y z z 0 ' Comliace alog Z as Descitio as Secificatio motio foce Selectio mati ; I Uifie Motio & oce Cotol wo ecoule Subsystems * motio * foce 9
10 Natual Systems Coseatie Systems V m 0 System Ietificatio equecy iceases with stiffess a iese mass Natual equecy 0 m () t c cos( t ) t Natual Systems Dissiatie Systems ( KV) ( KV) ( ) f fictio t Viscous fictio: f fictio b m b 0 m ictio Ietificatio System Cotol m f 0 m b f f ( ) Close-Loo m ( b ) ( ) 0 ime Resose 0 m m b m t () ce cos( t) t (t) (t) t t 0
Kinematics. Redundancy. Task Redundancy. Operational Coordinates. Generalized Coordinates. m task. Manipulator. Operational point
Mapulato smatc Jot Revolute Jot Kematcs Base Lks: movg lk fed lk Ed-Effecto Jots: Revolute ( DOF) smatc ( DOF) Geealzed Coodates Opeatoal Coodates O : Opeatoal pot 5 costats 6 paametes { postos oetatos
More informationMasses and orbits of minor planets with the GAIA mission
asses ad obits of io laets with the GAIA issio Sege ouet Suevisos : F.igad D.Hestoffe PLAN Itoductio Puose of the PhD Iotace of asses The diffeet ethods to estiate these asses Descitio of close aoach Diffeet
More informationANNEXE C Modèle mathématique du robot lego NXT
ANNEXE C Modèe athéatique du oot ego NX tié de a otice NXay-GS Mode-Based Desig - Coto of sef-aacig to-heeed oot uit ith LEGO Midstos NX, Yoihisa Yaaoto. 3 NXay-GS Modeig his chapte descies atheatica ode
More informationGround Rules. PC1221 Fundamentals of Physics I. Uniform Circular Motion, cont. Uniform Circular Motion (on Horizon Plane) Lectures 11 and 12
PC11 Fudametals of Physics I Lectues 11 ad 1 Cicula Motio ad Othe Applicatios of Newto s Laws D Tay Seg Chua 1 Goud Rules Switch off you hadphoe ad page Switch off you laptop compute ad keep it No talkig
More informationAdvanced Higher Formula List
Advaced Highe Fomula List Note: o fomulae give i eam emembe eveythig! Uit Biomial Theoem Factoial! ( ) ( ) Biomial Coefficiet C!! ( )! Symmety Idetity Khayyam-Pascal Idetity Biomial Theoem ( y) C y 0 0
More informationTwo or more points can be used to describe a rigid body. This will eliminate the need to define rotational coordinates for the body!
OINTCOORDINATE FORMULATION Two or more poits ca be used to describe a rigid body. This will elimiate the eed to defie rotatioal coordiates for the body i z r i i, j r j j rimary oits: The coordiates of
More informationTHE OPERATION AND KINEMATIC ANALYSIS OF A NOVEL CAM-BASED INFINITELY VARIABLE TRANSMISSION
Poceedigs of IDETC/CIE 6 ASME 6 Iteatioal Desig Egieeig Techical Cofeeces & Comutes ad Ifomatio i Egieeig Cofeece Setembe -, 6, Philadelhia, Pesylvaia, USA DETC6-9964 THE OPERATION AND KINEMATIC ANALYSIS
More informationDipartimento di Elettronica e Informazione e Bioingegneria Robotics
Diartimeto di Elettroica e Iformaioe e Bioigegeria Robotics arm iverse kiematics @ 5 IK ad robot rogrammig amera Tool gras referece sstem o the object the had has to reach the gras referece: T gras IK
More informationTechnical Report: Bessel Filter Analysis
Sasa Mahmoodi 1 Techical Repot: Bessel Filte Aalysis 1 School of Electoics ad Compute Sciece, Buildig 1, Southampto Uivesity, Southampto, S17 1BJ, UK, Email: sm3@ecs.soto.ac.uk I this techical epot, we
More informationVIII Dynamics of Systems of Particles
VIII Dyacs of Systes of Patcles Cete of ass: Cete of ass Lea oetu of a Syste Agula oetu of a syste Ketc & Potetal Eegy of a Syste oto of Two Iteactg Bodes: The Reduced ass Collsos: o Elastc Collsos R whee:
More information12.6 Sequential LMMSE Estimation
12.6 Sequetial LMMSE Estimatio Same kid if settig as fo Sequetial LS Fied umbe of paametes (but hee they ae modeled as adom) Iceasig umbe of data samples Data Model: [ H[ θ + w[ (+1) 1 p 1 [ [[0] [] ukow
More informationProf. Dr. I. Nasser atomic and molecular physics -551 (T-112) February 20, 2012 Spin_orbit.doc. The Fine Structure of the Hydrogen Atom
Pof. D. I. Nasse atomic ad molecula physics -55 (T-) Febuay 0, 0 Spi_obit.doc The Fie Stuctue of the Hydoge Atom Whilst the pedictios of the quatum model of hydoge ae a vey good appoximatio to eality,
More informationMulti-parameter Analysis of a Rigid Body. Nonlinear Coupled Rotations around
Adv. Theo. Appl. Mech., Vol. 6, 3, o., 9-7 HIKARI Ltd, www.m-hikai.com http://dx.doi.og/.988/atam.3.378 Multi-paamete Aalysis of a Rigid Body Noliea Coupled Rotatios aoud No Itesectig Axes Based o the
More informationSimple Design Method for a Tuned Viscous Mass Damper Seismic Control System
Simle Desig Metho fo a ue Viscous Mass Dame Seismic Cotol System K. Iago ohou Uivesity, Jaa Y. Sugimua & K. Saito N Facilities Ic., Jaa N. Ioue ohou Uivesity, Jaa SUMMARY: A tue viscous mass ame (VMD)
More information1. Linearization of a nonlinear system given in the form of a system of ordinary differential equations
. Liearizatio of a oliear system give i the form of a system of ordiary differetial equatios We ow show how to determie a liear model which approximates the behavior of a time-ivariat oliear system i a
More informationROTATIONAL MOTION PR 1
Eistei Classes, Uit No.,, Vadhma Rig Road Plaza, Vikas Pui Ext., Oute Rig Road New Delhi 8, Ph. : 969, 87 PR ROTATIONAL MOTION Syllabus : Cete of mass of a two-paticles system, Cete of mass of a igid body;
More informationZ Transforms. Lesson 20 6DT. BME 333 Biomedical Signals and Systems - J.Schesser
Z rasforms Lesso 6D BME 333 Biomedical Sigals ad Systems Z rasforms A Defiitio I a sese similar to the L excet it is associated with discrete time fuctios. Let s assume we hae a cotiuous time fuctio, f
More informationModelling and Simulation of Marine Craft DYNAMICS
Modellig ad Simulatio of Maie Caft DYNAMICS Edi Omedi Seio Reseah Fellow Moile & Maie Rootis Reseah Cete Uiesity of Limeik Outlie Uiesity of Limeik Moile & Maie Rootis Reseah Cete Dyamis Rigid-Body Euatios
More informationa) The average (mean) of the two fractions is halfway between them: b) The answer is yes. Assume without loss of generality that p < r.
Solutios to MAML Olympiad Level 00. Factioated a) The aveage (mea) of the two factios is halfway betwee them: p ps+ q ps+ q + q s qs qs b) The aswe is yes. Assume without loss of geeality that p
More informationrad / sec min rev 60sec. 2* rad / sec s
EE 559, Exa 2, Spig 26, D. McCalley, 75 iute allowed. Cloed Book, Cloed Note, Calculato Peitted, No Couicatio Device. (6 pt) Coide a.5 MW, 69 v, 5 Hz, 75 p DFG wid eegy yt. he paaete o the geeato ae give
More informationADDITIONAL INTEGRAL TRANSFORMS
Chapte IX he Itegal asfom Methods IX.7 Additioal Itegal asfoms August 5 7 897 IX.7 ADDIIONAL INEGRAL RANSFORMS 6.7. Solutio of 3-D Heat Equatio i Cylidical Coodiates 6.7. Melli asfom 6.7.3 Legede asfom
More informationATOMIC STRUCTURE EXERCISE # 1
ATOMIC STRUCTURE EXERCISE #. A N A N 5 A N (5 ) 5 A 5 N. R R A /. (6) / cm 5. (6) / cm fm 5 m 5 fm. C 8. d m m A 6.75 m.59 A Fo atom.59 5. E.6 E ().6.6 e E (e + ).6.6 e E (Li + ).6 E (Be + ).6 As B 6.
More informationc( 1) c(0) c(1) Note z 1 represents a unit interval delay Figure 85 3 Transmit equalizer functional model
Relace 85.8.3.2 with the following: 85.8.3.2 Tansmitted outut wavefom The 40GBASE-CR4 and 100GBASE-CR10 tansmit function includes ogammable equalization to comensate fo the fequency-deendent loss of the
More informationKinematics, Dynamics and Motion Planning of Wheeled Mobile Manipulators
Kieatics, Daics a Motio Plaig of Wheele Mobile Maipulatos Yuiag Wu, Yueig Hu College of Autoatio Sciece a Egieeig, South Chia Uivesit of echolog, 564, GuagZhou, Chia Eail:wu_68@63.co * Abstact I this pape,
More informationChemical Kinetics CHAPTER 14. Chemistry: The Molecular Nature of Matter, 6 th edition By Jesperson, Brady, & Hyslop. CHAPTER 14 Chemical Kinetics
Chemical Kietics CHAPTER 14 Chemistry: The Molecular Nature of Matter, 6 th editio By Jesperso, Brady, & Hyslop CHAPTER 14 Chemical Kietics Learig Objectives: Factors Affectig Reactio Rate: o Cocetratio
More informationFAR FIELD SOLUTION OF SH-WAVE BY CIRCULAR INCLUSION AND LINEAR CRACK
The 4 th Wold Cofeece o Eathquake Egieeig Octobe -7, 8, Beijig, Chia FAR FIELD SOLUTION OF SH-WAVE BY CIRCULAR INCLUSION AND LINEAR CRACK HogLiag Li,GuoHui Wu, Associate Pofesso, Depatmet of Egieeig Mechaics,
More informationMinimization of the quadratic test function
Miimizatio of the quadatic test fuctio A quadatic fom is a scala quadatic fuctio of a vecto with the fom f ( ) A b c with b R A R whee A is assumed to be SPD ad c is a scala costat Note: A symmetic mati
More informationBBU Codes Overview. Outline Introduction Beam transport Equation How to solve (BBU-R, TDBBUU, bi, MATBBU etc.) Comparison of BBU codes
BBU Codes Oveview asau Sawamua ad Ryoichi Hajima JAERI Outie Itoductio Beam tasot Equatio How to sove BBU-R, DBBUU, bi, ABBU etc. Comaiso of BBU codes Itoductio ERL cuet imited by Beam Beaku asvese defect
More informationSOLUTIONS. ydy. xdx. 4. (A) Let angle between the directions of incident ray and reflected ray be θ
JEE Advace 6 Bju s lasses 6. lah + lies o. Idia s most lied Educatioal oma otact: 99 SOLUTIONS. () F L R L R. (D) ˆ ˆ.. a a a K d d a K w a d d K dj di F F d dw a a. (A) sec. t 6 t R R t R T t R T Q Q
More informationJJMIE Jordan Journal of Mechanical and Industrial Engineering
JJIE Joda Joual o echaical ad Idustial Egieeig Volume 8 Numbe 4, August 4 ISSN 995-6665 Pages 7 - Dyamic Aalysis ad Desig o Steel-Ball Gidig achies Based o No-Slip Cases Jigju Zhag *, Guoguag Li, Ruizhe
More informationModelling rheological cone-plate test conditions
ANNUAL TRANSACTIONS OF THE NORDIC RHEOLOGY SOCIETY, VOL. 16, 28 Modellig heological coe-plate test coditios Reida Bafod Schülle 1 ad Calos Salas-Bigas 2 1 Depatmet of Chemisty, Biotechology ad Food Sciece,
More information13.8 Signal Processing Examples
13.8 Sigal Pocessig Eamples E. 13.3 Time-Vaig Chael Estimatio T Mlti Path v(t) (t) Diect Path R Chael chages with time if: Relative motio betwee R, T Reflectos move/chage with time ( t) = T ht ( τ ) v(
More information2013 Checkpoints Chapter 6 CIRCULAR MOTION
013 Checkpoints Chapte 6 CIRCULAR MOTIO Question 09 In unifom cicula motion, thee is a net foce acting adially inwads. This net foce causes the elocity to change (in diection). Since the speed is constant,
More information3D WIGNER FUNCTION MODEL FOR A QUANTUM FREE ELECTRON LASER
3D WIGNER FUNCTION MODEL FOR A QUANTUM FREE ELECTRON LASER N. Piovella (,), M.Cola (), L.Vole (), A. Schiavi (3), ad R. Boifacio (,4) () INFN-MI, Mila, Italy. () Diatimeto di Fisica, Uiv. of Mila, Italy
More informationGRAVITATIONAL FORCE IN HYDROGEN ATOM
Fudametal Joual of Mode Physics Vol. 8, Issue, 015, Pages 141-145 Published olie at http://www.fdit.com/ GRAVITATIONAL FORCE IN HYDROGEN ATOM Uiesitas Pedidika Idoesia Jl DR Setyabudhi No. 9 Badug Idoesia
More informationThe Space Redundant Robotic Manipulator Chaotic Motion Dynamics Control Algorithm
Sesors & rasducers, Vol. 75, Issue 7, July 24, pp. 27-3 Sesors & rasducers 24 by IFSA Publishig, S. L. http://www.sesorsportal.com he Space Redudat Robotic Maipulator Chaotic Motio Dyamics Cotrol Algorithm
More informationTHE FERROELECTRIC PLZT TYPE CERAMICS AS A MATERIAL FOR TRANSDUCERS M. CZERWIEC, R. ZACHARIASZ, J. ILCZUK
THE FEOELECTIC PLZT TYPE CEAMICS AS A MATEIAL FO TANSDUCES M. CZEWIEC,. ZACHAIASZ, J. ILCZUK Uivesity o Silesia, Faculty o Comutes Sciece a Mateials Sciece, Deatmet o Mateial Sciece 3 Żeomskiego St, 41-
More information4. PERMUTATIONS AND COMBINATIONS Quick Review
4 ERMUTATIONS AND COMBINATIONS Quick Review A aagemet that ca be fomed by takig some o all of a fiite set of thigs (o objects) is called a emutatio A emutatio is said to be a liea emutatio if the objects
More informationDynamic Response of Linear Systems
Dyamic Respose of Liear Systems Liear System Respose Superpositio Priciple Resposes to Specific Iputs Dyamic Respose of st Order Systems Characteristic Equatio - Free Respose Stable st Order System Respose
More informationSliding Mode Controller with Sliding Perturbation Observer Based on Gain Optimization Using Genetic Algorithm
Sliig oe Cotroller with Sliig erturbatio Observer Base o Gai Optimizatio Usig Geetic lgorithm i Sug You* Departmet of echaical a Itelliget Systems Egieerig usa Natioal Uiversity Busa 69-735, orea eayks@chol.com
More informationRigid Manipulator Control
Rigid Manipulator Control The control problem consists in the design of control algorithms for the robot motors, such that the TCP motion follows a specified task in the cartesian space Two types of task
More informationANSWERS, HINTS & SOLUTIONS HALF COURSE TEST VII (Main)
AIITS-HT-VII-PM-JEE(Mai)-Sol./7 I JEE Advaced 06, FIITJEE Studets bag 6 i Top 00 AIR, 7 i Top 00 AIR, 8 i Top 00 AIR. Studets fom Log Tem lassoom/ Itegated School Pogam & Studets fom All Pogams have qualified
More informationSPIRITUALISM. forces. of Spirit, A n stiy a e d f r o m a C o m m o n rhey. n o d and H en so S ta n d p o in t. Lea d s i 1 T U A L I.S M.
~ 3 : K G V 7 G GG 2 3 9 3» < V ; j z_! V 9 7 ' ; > : ; _ < - «-] 88 _ K _ [ -] ZZ - - _ [ ) G K < ' - - ( - '! j () - -] < : : < :?! q z ; [ > # : - 2 - - j ; :!_ - ] ' z ; : j G - j j - [ _ j! { q -
More informationCRACK DETECTION IN EULER-BERNOULLI BEAMS ON ELASTIC FOUNDATION USING GENETIC ALGORITHM BASED ON DISCRETE ELEMENT TECHNIQUE
Idia J.Sci.Res.() : 48-5, 04 ISSN:50-08(Olie) ISSN : 0976-876 (Pit) CRACK DEECION IN EULER-BERNOULLI BEAMS ON ELASIC FOUNDAION USING GENEIC ALGORIHM BASED ON DISCREE ELEMEN ECHNIQUE MOJABA GHASEMI a, ALIREZA
More informationMicroscopic Momentum Balances
013 Fluids ectue 6 7 Moison CM3110 10//013 CM3110 Tanspot I Pat I: Fluid Mechanics Micoscopic Momentum Balances Pofesso Faith Moison Depatment of Chemical Engineeing Michigan Technological Uniesity 1 Micoscopic
More information732 Appendix E: Previous EEE480 Exams. Rules: One sheet permitted, calculators permitted. GWC 352,
732 Aedix E: Previous EEE0 Exams EEE0 Exam 2, Srig 2008 A.A. Rodriguez Rules: Oe 8. sheet ermitted, calculators ermitted. GWC 32, 9-372 Problem Aalysis of a Feedback System Cosider the feedback system
More informationChapter 8 Complex Numbers
Chapte 8 Complex Numbes Motivatio: The ae used i a umbe of diffeet scietific aeas icludig: sigal aalsis, quatum mechaics, elativit, fluid damics, civil egieeig, ad chaos theo (factals. 8.1 Cocepts - Defiitio
More informationAppendix A: Mathematical Formulae and Statistical Tables
Aedi A: Mathematical Formulae ad Statistical Tables Pure Mathematics Mesuratio Surface area of shere = r Area of curved surface of coe = r J slat height Trigoometry a * b & c ' bc cos A Arithmetic Series
More informationOptimization Criterion. Minimum Distance Minimum Time Minimum Acceleration Change Minimum Torque Change Minimum End Point Variance
Lecture XIV Trajectory Formatio through Otimizatio Cotets: Otimizatio Criterio Miimum istace Miimum Time Miimum Acceleratio Chage Miimum Torque Chage Miimum Ed Poit Variace Usig Motor Redudacies Efficietly
More informationThe Discrete Fourier Transform
(7) The Discete Fouie Tasfom The Discete Fouie Tasfom hat is Discete Fouie Tasfom (DFT)? (ote: It s ot DTFT discete-time Fouie tasfom) A liea tasfomatio (mati) Samples of the Fouie tasfom (DTFT) of a apeiodic
More information2012 GCE A Level H2 Maths Solution Paper Let x,
GCE A Level H Maths Solutio Pape. Let, y ad z be the cost of a ticet fo ude yeas, betwee ad 5 yeas, ad ove 5 yeas categoies espectively. 9 + y + 4z =. 7 + 5y + z = 8. + 4y + 5z = 58.5 Fo ude, ticet costs
More informationNONLOCAL THEORY OF ERINGEN
NONLOCAL THEORY OF ERINGEN Accordig to Erige (197, 1983, ), the stress field at a poit x i a elastic cotiuum ot oly depeds o the strai field at the poit (hyperelastic case) but also o strais at all other
More informationSemiconductor Optical Communication Components and Devices Lecture 15: Light Emitting Diode (LED)
Semicoducto Otical Commuicatio Comoets ad Devices Lectue 15: Light mittig Diode (LD) Pof. Utal Das Pofesso, Deatmet of lectical gieeig, Lase Techology Pogam, Idia Istitute of Techology, Kau htt://www.iitk.ac.i/ee/faculty/det_esume/utal.html
More informationChapter 7 Introduction to vectors
Introduction to ectors MC Qld-7 Chapter 7 Introduction to ectors Eercise 7A Vectors and scalars a i r + s ii r s iii s r b i r + s Same as a i ecept scaled by a factor of. ii r s Same as a ii ecept scaled
More informationLecture #25. Amplifier Types
ecture #5 Midterm # formatio ate: Moday November 3 rd oics to be covered: caacitors ad iductors 1 st -order circuits (trasiet resose) semicoductor material roerties juctios & their alicatios MOSFEs; commo-source
More informationProblem 1. Problem Engineering Dynamics Problem Set 9--Solution. Find the equation of motion for the system shown with respect to:
2.003 Egieerig Dyamics Problem Set 9--Solutio Problem 1 Fid the equatio of motio for the system show with respect to: a) Zero sprig force positio. Draw the appropriate free body diagram. b) Static equilibrium
More informationDynamic Response of Second Order Mechanical Systems with Viscous Dissipation forces
Hadout #b (pp. 4-55) Dyamic Respose o Secod Order Mechaical Systems with Viscous Dissipatio orces M X + DX + K X = F t () Periodic Forced Respose to F (t) = F o si( t) ad F (t) = M u si(t) Frequecy Respose
More informationPhysics Equations Course Comparison
Physics Equatios Couse Compaiso Ietify you couse. You may use ay of the equatios beeath a to the left of you couse. Math A A PeCalculus Calculus AB o BC A to B is OR A:B is (Cocuet) (Cocuet) B B Algeba
More informationSchool of Mechanical Engineering Purdue University. ME375 Frequency Response - 1
Case Study ME375 Frequecy Respose - Case Study SUPPORT POWER WIRE DROPPERS Electric trai derives power through a patograph, which cotacts the power wire, which is suspeded from a cateary. Durig high-speed
More informationThe study of the motion of a body along a general curve. the unit vector normal to the curve. Clearly, these unit vectors change with time, u ˆ
Section. Cuilinea Motion he study of the motion of a body along a geneal cue. We define u ˆ û the unit ecto at the body, tangential to the cue the unit ecto nomal to the cue Clealy, these unit ectos change
More informationUsing Difference Equations to Generalize Results for Periodic Nested Radicals
Usig Diffeece Equatios to Geealize Results fo Peiodic Nested Radicals Chis Lyd Uivesity of Rhode Islad, Depatmet of Mathematics South Kigsto, Rhode Islad 2 2 2 2 2 2 2 π = + + +... Vieta (593) 2 2 2 =
More informationQuantum Mechanics Lecture Notes 10 April 2007 Meg Noah
The -Patice syste: ˆ H V This is difficut to sove. y V 1 ˆ H V 1 1 1 1 ˆ = ad with 1 1 Hˆ Cete of Mass ˆ fo Patice i fee space He Reative Haitoia eative coodiate of the tota oetu Pˆ the tota oetu tota
More informationModeling of Material Damping Properties in ANSYS
Modelig of Mateial Dampig Popeties i ANSYS C. Cai, H. Zheg, M. S. Kha ad K. C. Hug Defese Systems Divisio, Istitute of High Pefomace Computig 89C Sciece Pak Dive, Sigapoe Sciece Pak I, Sigapoe 11861 Abstact
More informationDigital Integrated Circuits
Digital Itegrated Circuits YuZhuo Fu cotact:fuyuzhuo@ic.sjtu.edu.c Office locatio:417 room WeiDiaZi buildig,no 800 DogChua road,mihag Camus Itroductio Review cotet Tye Cocet 15, Comutig 10 hours Fri. 6
More informationExecutive Committee and Officers ( )
Gifted and Talented International V o l u m e 2 4, N u m b e r 2, D e c e m b e r, 2 0 0 9. G i f t e d a n d T a l e n t e d I n t e r n a t i o n a2 l 4 ( 2), D e c e m b e r, 2 0 0 9. 1 T h e W o r
More informationBy the end of this section you will be able to prove the Chinese Remainder Theorem apply this theorem to solve simultaneous linear congruences
Chapte : Theoy of Modula Aithmetic 8 Sectio D Chiese Remaide Theoem By the ed of this sectio you will be able to pove the Chiese Remaide Theoem apply this theoem to solve simultaeous liea cogueces The
More informationFinite q-identities related to well-known theorems of Euler and Gauss. Johann Cigler
Fiite -idetities elated to well-ow theoems of Eule ad Gauss Joha Cigle Faultät fü Mathemati Uivesität Wie A-9 Wie, Nodbegstaße 5 email: oha.cigle@uivie.ac.at Abstact We give geealizatios of a fiite vesio
More informationParametric Methods. Autoregressive (AR) Moving Average (MA) Autoregressive - Moving Average (ARMA) LO-2.5, P-13.3 to 13.4 (skip
Pmeti Methods Autoegessive AR) Movig Avege MA) Autoegessive - Movig Avege ARMA) LO-.5, P-3.3 to 3.4 si 3.4.3 3.4.5) / Time Seies Modes Time Seies DT Rdom Sig / Motivtio fo Time Seies Modes Re the esut
More informationAnalytical mechanics
Divisio of Mechaics Lud Uiversity Aalytical mechaics 7059 Name (write i block letters):. Id.-umber: Writte examiatio with five tasks. Please check that all tasks are icluded. A clea copy of the solutios
More informationHomework Set 3 Physics 319 Classical Mechanics
Homewok Set 3 Phsics 319 lassical Mechanics Poblem 5.13 a) To fin the equilibium position (whee thee is no foce) set the eivative of the potential to zeo U 1 R U0 R U 0 at R R b) If R is much smalle than
More informationFINITE ELEMENT ANALYSIS OF A BWR FEED WATER DISTRIBUTOR UNDER EXTREME TRANSIENT PRESSURE LOAD
FINITE ELEMENT ANALYSIS OF A BWR FEED WATER DISTRIBUTOR UNDER EXTREME TRANSIENT PRESSURE LOAD Ebehad Altstadt, Hema Ohlmeye 1, Fak Otemba 1, Fak-Pete Weiss 1. Itoductio The beak of a feed wate lie outside
More informationAnnouncements, Nov. 19 th
Aoucemets, Nov. 9 th Lecture PRS Quiz topic: results Chemical through Kietics July 9 are posted o the course website. Chec agaist Kietics LabChec agaist Kietics Lab O Fial Exam, NOT 3 Review Exam 3 ad
More informationAanumntBAasciAs. l e t e s auas trasuarbe, amtima*. pay Bna. aaeh t!iacttign. Xat as eling te Trndi'aBd^glit!
- [ - --- --- ~ - 5 4 G 4? G 8 0 0 0 7 0 - Q - - - 6 8 7 2 75 00 - [ 7-6 - - Q - ] z - 9 - G - 0 - - z / - ] G / - - 4-6 7 - z - 6 - - z - - - - - - G z / - - - G 0 Zz 4 z4 5? - - Z z 2 - - {- 9 9? Z G
More informationCrosscorrelation of m-sequences, Exponential sums and Dickson
Cosscoelatio o m-equeces, Epoetial sums ad Dicso polyomials To Helleseth Uiesity o Bege NORWAY Joit wo with Aia Johase ad Aleade Kholosha Itoductio Outlie m-sequeces Coelatio o sequeces Popeties o m-sequeces
More information2 f(x) dx = 1, 0. 2f(x 1) dx d) 1 4t t6 t. t 2 dt i)
Math PracTest Be sure to review Lab (ad all labs) There are lots of good questios o it a) State the Mea Value Theorem ad draw a graph that illustrates b) Name a importat theorem where the Mea Value Theorem
More informationMathematics Extension 2 SOLUTIONS
3 HSC Examiatio Mathematics Extesio SOLUIONS Writte by Carrotstics. Multiple Choice. B 6. D. A 7. C 3. D 8. C 4. A 9. B 5. B. A Brief Explaatios Questio Questio Basic itegral. Maipulate ad calculate as
More informationSYMMETRY ENERGY FOR NUCLEI BEYOND THE STABILITY VALLEY. V.M. Kolomietz and A.I.Sanzhur
SYMMETRY ENERGY FOR NULEI BEYOND THE STBILITY VLLEY V.M. Kolomietz ad.i.sazhu Istitute fo Nuclea Reseach, 368 Kiev, Ukaie We aly the diect vaiatioal method to deive the equatio of state fo fiite uclei
More informationDynamics of Structures
UNION Dyamis of Stutues Pat Zbigiew Wójii Jae Gosel Pojet o-fiae by Euopea Uio withi Euopea Soial Fu UNION Sigle-egee-of-feeom systems Uampe systems The euatio of motio fo a uampe sigle-egee-of-feeom system
More informationSATELLITE ORBIT ESTIMATION USING ON-LINE NEURAL NETWORKS. Mahsa-Sadat Forghani, Mohammad Farrokhi
SATELLITE ORBIT ESTIMATION USING ON-LINE NEURAL NETWORKS Mahsa-Sadat Foghai, Mohammad Faohi Depatmet of Electical Egieeig Cete of Ecellece fo Powe System Automatio ad Opeatio Ia Uivesity of Sciece ad Techology
More informationAIEEE 2004 (MATHEMATICS)
AIEEE 004 (MATHEMATICS) Impotat Istuctios: i) The test is of hous duatio. ii) The test cosists of 75 questios. iii) The maimum maks ae 5. iv) Fo each coect aswe you will get maks ad fo a wog aswe you will
More informationMultivector Functions
I: J. Math. Aal. ad Appl., ol. 24, No. 3, c Academic Pess (968) 467 473. Multivecto Fuctios David Hestees I a pevious pape [], the fudametals of diffeetial ad itegal calculus o Euclidea -space wee expessed
More informationA L A BA M A L A W R E V IE W
A L A BA M A L A W R E V IE W Volume 52 Fall 2000 Number 1 B E F O R E D I S A B I L I T Y C I V I L R I G HT S : C I V I L W A R P E N S I O N S A N D TH E P O L I T I C S O F D I S A B I L I T Y I N
More informationReference Guide & Formula Sheet for Physics
D. Hoselto & M. Pice Page of 8 #0 Heatig a Solid, Liquid o Gas #3 Compoets of a Vecto Q = m c T if V = 34 m/sec 48 the V i = 34 m/sec (cos 48 ); ad V J = 34 m/sec (si 48 ) #4 Weight = m g g = 9.8m/sec²
More informationcosets Hb cosets Hb cosets Hc
Exam, 04-05 Do a total of 30 oits (moe if you wat, of couse) Show you wok! Q: 0 oits (4 ats, oits each fo the fist two ats, 3 oits each fo the secod two ats) Q: 0 oits ( ats, oit each, max cedit 0 oits)
More informationOn the Basis Property of Eigenfunction. of the Frankl Problem with Nonlocal Parity Conditions. of the Third Kind
It.. Cotemp. Math. Scieces Vol. 9 o. 3 33-38 HIKARI Lt www.m-hikai.com http://x.oi.og/.988/ijcms..33 O the Basis Popety o Eigeuctio o the Fakl Poblem with Nolocal Paity Coitios o the Thi Ki A. Sameipou
More informationMA 1201 Engineering Mathematics MO/2017 Tutorial Sheet No. 2
BIRLA INSTITUTE OF TECHNOLOGY, MESRA, RANCHI DEPARTMENT OF MATHEMATICS MA Egieeig Matheatis MO/7 Tutoia Sheet No. Modue IV:. Defie Beta futio ad Gaa futio.. Pove that,,,. Pove that, d. Pove that. & whee
More informationx k 34 k 34. x 3
A A A A A B A =, C =. f k k x k l f f 3 = k 3 k 3 x k 34 k 34 x 3 k 3 l 3 k 34 l 34. f 4 x 4 K K = [ ] 4 K = K (K) = (K) I m m R I m m = [e, e,, e m ] R = [a, a,, a m ] R = (r ij ) r r r m R = r r m. r
More informationV V The circumflex (^) tells us this is a unit vector
Vecto Vecto have Diection and Magnitude Mike ailey mjb@c.oegontate.edu Magnitude: V V V V x y z vecto.pptx Vecto Can lo e Defined a the oitional Diffeence etween Two oint 3 Unit Vecto have a Magnitude
More informationParameter estimation of the brake disk using in a floating caliper disk brake model with respect to low frequency squeal
The 19th Cofeece of Mechaical Egieeig Netwok of Thailad 19-1 Octobe 005, Phuket, Thailad Paamete estimatio of the bake disk usig i a floatig calipe disk bake model with espect to low fequecy squeal Thia
More informationΣF = r r v. Question 213. Checkpoints Chapter 6 CIRCULAR MOTION
Unit 3 Physics 16 6. Cicula Motion Page 1 of 9 Checkpoints Chapte 6 CIRCULAR MOTION Question 13 Question 8 In unifom cicula motion, thee is a net foce acting adially inwads. This net foce causes the elocity
More informationTP A.29 Using throw to limit cue ball motion
techical proof TP A.9 Usig to limit cue ball motio supportig: The Illustrate Priciples of Pool a Billiars http://billiars.colostate.eu by Dai G. Alciatore, PhD, PE ("Dr. Dae") techical proof origially
More informationIntroduction Common Divisors. Discrete Mathematics Andrei Bulatov
Intoduction Common Divisos Discete Mathematics Andei Bulatov Discete Mathematics Common Divisos 3- Pevious Lectue Integes Division, popeties of divisibility The division algoithm Repesentation of numbes
More informationDesign Sensitivity Analysis and Optimization of Nonlinear Transient Dynamics
Desig Sesitivity Aalysis ad Otimizatio of Noliear Trasiet Dyamics 8th AIAA/USAF/NASA/ISSOMO Symosium o Multidisciliary Aalysis ad Otimizatio Nam Ho Kim ad Kyug Kook Choi Ceter for Comuter-Aided Desig The
More informationT h e C S E T I P r o j e c t
T h e P r o j e c t T H E P R O J E C T T A B L E O F C O N T E N T S A r t i c l e P a g e C o m p r e h e n s i v e A s s es s m e n t o f t h e U F O / E T I P h e n o m e n o n M a y 1 9 9 1 1 E T
More information1-D Sampling Using Nonuniform Samples and Bessel Functions
-D Saplig Usig Nouio Saples a Bessel Fuctios Nikolaos E. Myiis *, Mebe, IEEE,Electical Egiee, Ph.D. A & Chistooulos Chazas, Seio Mebe, IEEE, Poesso B A Cultual a Eucatioal Techologies Istitute, Tsiiski
More informationMinimal order perfect functional observers for singular linear systems
Miimal ode efect fuctioal obseves fo sigula liea systems Tadeusz aczoek Istitute of Cotol Idustial lectoics Wasaw Uivesity of Techology, -66 Waszawa, oszykowa 75, POLAND Abstact. A ew method fo desigig
More informationControl of Free-floating Space Robotic Manipulators base on Neural Network
IJCSI Iteatioal Joual of Compute Sciece Iue, Vol. 9, Iue 6, No, Noembe ISSN (Olie): 694-84 www.ijcsi.og 3 Cotol of Fee-floatig Space Robotic Maipulato bae o Neual Netwok ZHANG Wehui ad ZHU Yifa College
More informationME 354, MECHANICS OF MATERIALS LABORATORY MECHANICAL PROPERTIES AND PERFORMANCE OF MATERIALS: TORSION TESTING*
ME 354, MECHANICS OF MATEIALS LABOATOY MECHANICAL POPETIES AND PEFOMANCE OF MATEIALS: TOSION TESTING* MGJ/08 Feb 1999 PUPOSE The pupose of this execise is to obtai a umbe of expeimetal esults impotat fo
More informationFree Surface Hydrodynamics
Water Sciece ad Egieerig Free Surface Hydrodyamics y A part of Module : Hydraulics ad Hydrology Water Sciece ad Egieerig Dr. Shreedhar Maskey Seior Lecturer UNESCO-IHE Istitute for Water Educatio S. Maskey
More informationElectromagnetism Physics 15b
lectomagnetism Physics 15b Lectue #20 Dielectics lectic Dipoles Pucell 10.1 10.6 What We Did Last Time Plane wave solutions of Maxwell s equations = 0 sin(k ωt) B = B 0 sin(k ωt) ω = kc, 0 = B, 0 ˆk =
More information