The Application of Euler Lagrange Method of Optimization for Electromechanical Motion Control
|
|
- Lewis Henry
- 6 years ago
- Views:
Transcription
1 HE ANNAS OF "DUNAREA DE OS" UNIVERSIY OF GAAI FASCICE III, ISSN -454X EECROECHNICS, EECRONICS, AUOMAIC CONRO, INFORMAICS he Application o Euler agrange Metho o Optiization or Electroechanical Motion Control Ion BIVO, Cristian VASIACHE Universitatea "Dunarea e os" Galati Doneasca, 6-Galati Roania e-ail: Ion.Bivol@ugal.ro Abstract: Inustrial an non-inustrial processes such as prouction plans, robots, pups, copressors, hoe applications, transportation o people an goos etc., require soe ins o otion control. he ain unctions o electroechanical rives are to ajust these processes by controlling the torque, spee or position. he objective o this paper is to peror the control o otion while iniizing power losses, that is?ri, in process conversion o electrical energy to echanical energy. he optial control laws or our proble is in using the Euler agrange principle. We consier three types o controlle rives: torque, spee an position. Each o the has ierent control laws. By ipleentation o these controls with Borlan C++ an Matlab environent, substantial energy savings are obtaine. Keywors: Motion control, sensor less, energy saving, ac rives syste. INRODUCION he electrical rives have a wie range o practice in inustry an transportation. It is possible to istinguish three ierent requireents with regar to the ain state control: orque controlle rives Spee controlle rives Position controlle rives Depening on the application there are ierent eans or accuracy or ynaic response. With increasing accuracy the cost an coplexity rise steeply. In the classical approach, the iniization inex to be perore is the accuracy an the tie o the ynaic response. hat is, the syste coponents ust have the capability to ove in iniu tie with the best accuracy. But when the otion tie gets shorter acceleration increases by / an consequently the current an power issipation increase an otor overheats. In this paper another choice o esign objectives is use: peror a ove within tie, while iniising the otor teperature. here are ierent solutions o this proble, epening o the rive targets: torque, spee or position control.. DYNAMICS OF A MECHANICA DRIVE he equations escribing the ynaic behavior o a echanical rive with constant inertia are: his paper was recoene or publication by E. Rosu 5
2 HE ANNAS OF "DUNAREA DE OS" UNIVERSIY OF GAAI FASCICE III, ISSN -454X ε () (,, um, (,, u, α ε y y(x)? (x,y ) where is the angular velocity an a is angular coorinate. (x,y ) y (x) In orer to gain better insight the otor an loa torque, are consiere as unctions o,e an o the controls inputs u M an u to the actuators on the otor an loa sie. Hence, by neglecting the ynaics o the otor an loa, we arrive at a secon orer syste escribe by the two state equation (). - Motor ynaic /s oa ynaic Power supply Fig.. Bloc iagra or ynaics o echanical rive Figure shows a bloc iagra escribing the otion o the rive syste. We have assue that all oving parts o a rive can be cobine to or one eective inertia. However, or a ore etaile analyses o a echanical ynaic eects it ay be necessary to consier the istribution o the asses an the linage between then. he two blocs with ouble rae escribes the non linear unctions an ay contain aitional ynaic states escribe by ierential equations. 3. DESIGN SOUIONS he well nown optial regulator esign proble is to eterinate the optial control law u ( x, which can transer the syste ro its initial state to the inal state such that given perorance inex is iniize. he perorance inex is selecte to give the best trae-o between perorance an cost o control. he perorance inex that is wiely use in optial control esign is nown as the quaratic perorance inex an is base on iniu-error an iniuenergy issipation criteria. u u /s α Fig.. wo paths or transer ro (x, y ) state to (x, y ) state. Consier the syste escribe by () x &( Ax( + Bu( he quaratic perorance inex is: t (3) I ( x Qx + u Ru) t Subject to the ynaic syste equation (). In (3) Q is a positive sei-einite atrix on R is a real syetric atrix. Q is positive seieinite i all its principal inors are non-negative. he choice o the eleents o Q an R allows the relative weighting o iniviual state variable an iniviual inputs. he integrals variations ethos (the Potriagin's axiu principle or the Hailtonian etho) or the optial control low optiization give the iiculties in practical ipleentation, because either initial conitions or inal conitions are not copletely nown. In this paper, the application o agrangean etho o optiization to our proble in consiere. I we consier the unconstraint unctional: it ust in ( x) I. x (4) I g( x, y, y& ) y x x which peror the iniization o he proble's solution can be oun by eans o the Euler-agrange equation. g (5) y x y& I the target point is oving on trajectory C, the transversality conition is neee (a generalize ortogonality). x 6
3 HE ANNAS OF "DUNAREA DE OS" UNIVERSIY OF GAAI FASCICE III, ISSN -454X (6) [ ( y & g ) x + g y] g y & y& he optiisation proble or ynaic systes base on the Euler-agrange principle starts ro the general criteria: t (7) I ( x(, u(, + M ( x, t, x, t where an M are unctions eine in X U t R, respectively in X R Usually there are three types o optiisation proble: he agrange proble, when an M ; he Mayer proble when an M ; he Bolza proble when an M ; I the general state equation o the syste is: (8) x &( ( x(, u(. he unction Φ is eine as: & (9) Φ ( x x, ( x, x &, For agrange proble the unctional criteria eine as: () I ( x, + λ Φ( x, x, & where λ represents the agrange ultipliers. he Euler-agrange equation or the new unctional criteria are: () I x I u I λ I x& I u& I λ& By eans o Euler-agrange equations we can in the optial control laws, irst or echanical otion syste, an then or electrical rive syste. 4. MOION CONRO AWS WHICH MINIMISING HE MOOR EMPERAURE. he equations escribing the otions o rive with constant inertia an constant loa torque are: (3) α& & he perorance easure o energy optiisation leas to the syste is: (4) I R i. he otion torque equation is: where: (5) i ; or c otor, φ or ac otor with iel orientation 3 φ + σ where φ an φ are the lux o the achines. Fro equations (3,4), results: R (6) I 4.. Spee controlle rive In this case the proble is to oiy the state o the syste ro initial spee i to inal spee,with iniisation o energy issipation in electroechanical power conversion syste. In this conition the unctional criteria () is: (7) ( ) R + λ & + + λ I he Euler agrange equations with results ro (6) are : (8) R λ& λ& λ with initial an inal conitions: t i ; t λ Fro (7) results the optial control : & () 7
4 HE ANNAS OF "DUNAREA DE OS" UNIVERSIY OF GAAI FASCICE III, ISSN -454X where i + (9) () is the angular acceleration i ε he cost perorance inex is: () R I + [ ε ] 4.. Position controlle rive: In this case the proble is to achieve an ipose angular position a in tie with iniu cost. he perorance inex () is: () I R λ + λ ( α& ) + λ & an the Euler-agrange equations are: (3) + [ & + ] 3 R λ λ& λ λ& λ& + λ& 3 he optial control law results ro these equation by integration: (4) ( C C R where C an C are integration constants. With initial an inal conitions t +, a t - aa ; results: (5) α t t 6 α t 3 t 3 + t t t he equations (5) escribes the optial otion o the syste in tie when the ipose oveent angle is a. he evaluation o otion cost can be eectuate by eans o the relation (5): R (6) I ( ) or by echanical wor calculations: α (7) α Finally, the perorance inex (5) or position rive syste is: (8) I R 3 α + he optial control laws or spee an position rives are ierent. In the spee rive the ais is to transer the spee o the syste ro I to with inial isplaceent a. In the position rive, the ai is to transer the syste ro initial position to inally position a in tie with conition: ax. he perorance inex or position controlle rive with usual control law with constant ynaic torque or spee rive is: (9) R I + 6 α which is uch 3 greater than optial perorance inex (7). 8
5 HE ANNAS OF "DUNAREA DE OS" UNIVERSIY OF GAAI FASCICE III, ISSN -454X 6a / 4a / / / ax,5a / ax a / t t Fig. 3a Aa Fig. 3b Aa Fig. 3 orque an spee proiles or optial position control (a) an respectively sub optial control (b) I, ) C 4 C orque Controller q u q Inuction Machine i u,u q,i,i q C 3 ) i i (-) Flux Controller u I.M. i q i K, ax, α C K Fig.4 Bloc iagra o the control syste or inuction achine position rive syste 9
6 HE ANNAS OF "DUNAREA DE OS" UNIVERSIY OF GAAI FASCICE III, ISSN -454X 5. EXPERIMENA RESUS We consier the position rive syste with asynchronous achine. he ipose values or the syste are : the tie o execution, the axiu spee ax,the inal position α an the estiate loa torque. he coan syste calculate the optial trajectory or spee (C) an torque (C ), ig.4. hen the control syste in the appropriate u, u achine supply tensions coponents an q their pulsation. In igure 4 the bloc iagra o the control syste is presente. here are two PID controllers or torque an spee. he energy conversion process is nonlinear.for the copensation o the nonlinearites the unction an q are use. he pulsation are calculate in the rotor iel orientation theory anner, that is: Fig.5 Ipose values an experientals results or position spee an torque with optial velocity proile + (3) 3R pφ where φ, R are the rotor lux an rotor resistance, respectively.because the rive is not sensore with spee sensor the easure spee in (9) is replace by the calculate spee (4). he inuction otor rate paraeters use or experiental tests are : 4W,38V,5rp,5Hz. In igure 5 are represente the results or the ollowing test conitions : sec, ax 7s (3) α 46 ra, ; (3) i,9e3ws Fig.6 Ipose values an experientals results or position spee an torque with sub optial velocity proile he optial velocity proile is a parabola, which are quite well ollowe by the rive syste without spee sensor. I the velocity proile is triangular (ig.6) (33) ax 9s i 5,6e3ws; α 46ra
7 HE ANNAS OF "DUNAREA DE OS" UNIVERSIY OF GAAI FASCICE III, ISSN -454X 6. CONCUSIONS 7.REFERENCES he control o otion with iniizing power loses in process conversion o electrical energy to echanical by Euler-agrange etho o optiization is a new way in the iel o electrical rives. A sensor less control syste with PWM supply inverter or inuction otor was evelope. In this case the ipose inal position α is well reache without spee sensor. here are an iportant ierence between the cost inex in optial control case an others sub optial controls. However the ain question is the proper estiation o the loa torque..eonhar,w.,control o Electrical Drives, Springer, 996.Bolea,N.,Nasar,S.A.-Vector Control o AC Drives, CRC Press,99 3.Bivol,I.,-Moern Drives Systes, Acaeica, 999
Multivariate Methods. Matlab Example. Principal Components Analysis -- PCA
Multivariate Methos Xiaoun Qi Principal Coponents Analysis -- PCA he PCA etho generates a new set of variables, calle principal coponents Each principal coponent is a linear cobination of the original
More informationBenchmarking Power System Stabilizer Controller Performance Using Conventional Lead/Lag, Fuzzy, and Matlab PID
Bencharking Power Syste Stabilizer Controller Perforance Using Conventional Lea/Lag an Matlab PI MOHAMA HALI BILAL HANI BABA lectrical ngineering epartent University of Balaan P. O. Box ripoli LBANON ohaa.khali@balaan.eu.lb
More informationPHYSICS ADVANCED LABORATORY I UNIVERSAL GRAVITATIONAL CONSTANT Spring 2001 (additions for Spring 2005 on last page)
PHYSICS 334 - ADVANCED LABOATOY I UNIVESAL GAVITATIONAL CONSTANT Spring 001 (aitions for Spring 005 on last page) Purposes: Deterine the value of the universal gravitation constant G. Backgroun: Classical
More informationEffects of large dynamic loads on power system stability
Effects of large ynaic loas on power syste stability Author Mahu, M., Hossain, Jahangir, Pota, H. Publishe 0 Journal itle International Journal of Electrical Power & Energy Systes DOI https://oi.org/0.06/j.ijepes.0.07.05
More informationThe Simulation of an Induction Motor in Transient Behavior Taking into Account the Saturation Effect
The Siulation of an Inuction Motor in Transient Behavior Taking into Account the Saturation Effect Ileana Calofirescu "Politehnica" University of Bucharest, Bucharest, Roania, ileana.calofirescu@yahoo.co.uk
More informationPHYSICS ADVANCED LABORATORY I UNIVERSAL GRAVITATIONAL CONSTANT Spring 2001
PHYSICS 334 - ADVANCED LABOATOY I UNIVESAL GAVITATIONAL CONSTANT Spring 001 Purposes: Deterine the value of the universal gravitation constant G. Backgroun: Classical echanics topics-oents of inertia,
More informationAn active suspension with reduced complexity
An active suspension with reuce coplexity Thoas Bear Peter Pelz Institut ür Fluisystetechnik, Technische Universität Darstat, Darstat, Gerany ABSTRACT This paper introuces a new active hyro pneuatic suspension
More informationAngular movement. Torque. W = M θ [Nm] Pm = M ω [W] motor shaft. motor shaft
Meoranu Linear oeent = ass [kg] = linear isplaceent [] = linear spee [/s] a = linear acceleration [/s 2 ] r = raius [] p = pitch [] η = transission efficiency [ ] F = force [N] Force F = a [N] Angular
More informationACCUMULATION OF FLUID FLOW ENERGY BY VIBRATIONS EXCITATION IN SYSTEM WITH TWO DEGREE OF FREEDOM
ENGINEERING FOR RURAL DEVELOPMENT Jelgava, 9.-.5.8. ACCUMULATION OF FLUID FLOW ENERGY BY VIBRATION EXCITATION IN YTEM WITH TWO DEGREE OF FREEDOM Maris Eiduks, Janis Viba, Lauris tals Riga Technical University,
More informationNEURO-GENETIC INPUT-OUTPUT LINEARIZATION CONTROL OF PERMANENT MAGNET SYNCHRONOUS MOTOR
Journal of Theoretical an Applie Inforation Technology 5 th March 22. Vol. 37 No. 25-22 JATIT & LLS. All rights reserve. ISSN 992-8645 www.jatit.org E-ISSN 87-395 NERO-GENETIC INPT-OTPT LINEARIZATION CONTROL
More informationDelamination Prediction of Uni-Directional Composite Laminates using Shell Elements and a Strain Rate Dependent Micro-mechanical Material Model
14 th International LS-DYNA Users Conerence Session: Coposites Delaination Preiction o Uni-Directional Coposite Lainates using Shell Eleents an a Strain Rate Depenent Micro-echanical Material Moel Saneep
More informationSOLUTIONS for Homework #3
SOLUTIONS for Hoework #3 1. In the potential of given for there is no unboun states. Boun states have positive energies E n labele by an integer n. For each energy level E, two syetrically locate classical
More informationSummary of the Class before Exam1
uar o the lass beore Ea Builing a FEA Moel Ingreients o a FEA sotware pacage teps in builing a FEA oel Moeling consierations D pring/truss Eleents ingle D spring/truss eleent Global stiness atri; properties
More informationMaximum a Posteriori Decoding of Turbo Codes
Maxiu a Posteriori Decoing of Turbo Coes by Bernar Slar Introuction The process of turbo-coe ecoing starts with the foration of a posteriori probabilities (APPs) for each ata bit, which is followe by choosing
More informationTopic 5a Introduction to Curve Fitting & Linear Regression
/7/08 Course Instructor Dr. Rayond C. Rup Oice: A 337 Phone: (95) 747 6958 E ail: rcrup@utep.edu opic 5a Introduction to Curve Fitting & Linear Regression EE 4386/530 Coputational ethods in EE Outline
More informationModern Control Systems (ECEG-4601) Instructor: Andinet Negash. Chapter 1 Lecture 3: State Space, II
Modern Control Systes (ECEG-46) Instructor: Andinet Negash Chapter Lecture 3: State Space, II Eaples Eaple 5: control o liquid levels: in cheical plants, it is oten necessary to aintain the levels o liquids.
More informationA Robust Fully-Digital Drive for Linear Permanent Magnet Synchronous Motor
A Robust Fully-Digital Drive for Linear Peranent Magnet ynchronous Motor Michael.W. Ta* orbert. heung** *AM Assebly Autoation, Watson entre, 16 Kung Yip t., Kwai hung,.t., Hong Kong **Departent of Electrical
More informationSynchronous Reluctance Machine (SynRM) Design
Synchronous Reluctance Machine (SynRM) Design by Reza Rajabi Moghaa Master Thesis Supervisor: Dr. Frey Magnussen Exainer: Prof. Chanur Saarangani Royal Institute of Technology Departent of Electrical Engineering
More informationc h L 75 10
hapter 31 1. (a) All the energy in the circuit resies in the capacitor when it has its axiu charge. The current is then zero. f Q is the axiu charge on the capacitor, then the total energy is c c h h U
More informationFeature Extraction Techniques
Feature Extraction Techniques Unsupervised Learning II Feature Extraction Unsupervised ethods can also be used to find features which can be useful for categorization. There are unsupervised ethods that
More informationDOUBLE PENDULUM VIBRATION MOTION IN FLUID FLOW
ENGINEERING FOR RURA DEEOPMENT Jelgava,.-.5.5. DOUBE PENDUUM IBRATION MOTION IN FUID FOW Janis iba, Maris Eiuks, Martins Irbe Riga Technical University, atvia janis.viba@rtu.lv, maris.eiuks@rtu.lv, martins.irbe@rtu.lv
More informationOptimization of Flywheel Weight using Genetic Algorithm
IN: 78 7798 International Journal o cience, Engineering and Technology esearch (IJET) Volue, Issue, March 0 Optiization o Flywheel Weight using Genetic Algorith A. G. Appala Naidu*, B. T.N. Charyulu, C..C.V.aanaurthy
More informationModelling and control of hybrid renewable energy system connected to AC grid
Sai Younsi et al. / International Journal on Coputer Science an Engineering (IJCSE) Moelling an control o hybri renewable energy syste connecte to AC gri Sai Younsi Higher Institute o technological stuies
More informationNote that an that the liit li! k+? k li P!;! h (k)? ((k? )) li! i i+? i + U( i ) is just a Rieann su representation of the continuous integral h h j +
G5.65: Statistical Mechanics Notes for Lecture 5 I. THE FUNCTIONAL INTEGRAL REPRESENTATION OF THE PATH INTEGRAL A. The continuous liit In taking the liit P!, it will prove useful to ene a paraeter h P
More informationKINETOSTATIC ANALYSIS OF SIX-BAR MECHANISM USING VECTOR LOOPS AND THE VERIFICATION OF RESULTS USING WORKING MODEL 2D
International Journal of Mechanical Engineering an Technology (IJMET) Volue 8, Issue 8, ugust 017, pp. 1109 1117, rticle I: IJMET_08_08_110 vailable online at http://www.iaee.co/ijmet/issues.asp?jtype=ijmet&vtype=8&itype=8
More informationEnergy Time Dichotomy in the Optimal Control of the Electrical Drives
Proc of the 3r IAS/WSAS Int Conf on nergy, nvironment, cosystems an Sustainable Development, Agios Nikolaos, Greece, July 4-6, 7 54 nergy ime Dichotomy in the Optimal Control of the lectrical Drives CORNLIU
More informationOptimum Spacing for Agriculture Drainage Espacement optimum des drains pour la production agricole
Scientific registration n o : 56 Syposiu n o : 9 Presentation: poster Optiu Spacing for Agriculture Drainage Espaceent optiu es rains pour la prouction agricole ARROYO Victor (1), GARCIA Nahun (1), NAMUCHE
More informationDebond crack growth in fatigue along fiber in UD composite with broken fibers
Debon crack growth in atigue along iber in UD composite with broken ibers Johannes Eitzenberger an Janis arna Dept o Applie Physics an Mechanical Engineering Lulea University o Technology, Sween SE 97
More informationGuntis Orlovskis 1, Marina Konuhova 2, Karlis Ketners 3, Riga Technical University
Power an Electrical Engineering Volue 29 Coparison of Inuction Motor Transient Processes Characteristics Obtaine Experientally With Those Obtaine by Means of FORTRAN an MATLAB Softwear Guntis Orlovskis
More informationAdvances in Optimal Control of Polymerization Reactors
olyer science: research avances, practical applications an eucational aspects (A. énez-vilas; A. Solano, Es.) Avances in Optial Control o olyerization Reactors Ch. Venateswarlu B V Raju Institute o Technology,
More informationActuators & Mechanisms Actuator sizing
Course Code: MDP 454, Course Nae:, Second Seester 2014 Actuators & Mechaniss Actuator sizing Contents - Modelling of Mechanical Syste - Mechaniss and Drives The study of Mechatronics systes can be divided
More informationShahlar Gachay Askerov. Baku State University, Baku, Azerbaijan
Econoics Worl, Nov.-Dec. 2018, Vol. 6, No. 6, 450-456 oi: 10.17265/2328-7144/2018.06.004 D DAVID PUBLISHING Econophysical Applications for Econoic Progress: Monopoly an Copetition Cases Shahlar Gachay
More informationInfluence of Surface Roughness on Sliding Characteristics of Rubber Seals
TECHNICAL REPORT Influence of Surface Roughness on Sliing Characteristics of Seals K. YAMAMOTO D. OZAKI T. NAKAGAWA The influence of surface roughness on frictional vibration of a bearing seal has been
More informationDiscrete Time Linear Quadratic Optimal Control for an Electrical Servo Drive System
Discrete ime Linear Quaratic Optimal Control or an Electrical Servo Drive System CORNELIU BOAN, FLORIN OSAFI an ALEXANDRU ONEA Dept. o Automatic Control an Inustrial Inormatics Gh. Asachi echnical University
More informationVerification of Measurement System for Shearography Machine
Verification of Measureent Syste for Shearography Machine JIRAPHON SRISERTPOL 1, PAPHAKORN SOONANON 2, PREECHA CHAMPATHONG 1 AND SORADA KHAENGKARN 1 1 School of Mechanical Engineering, Institute of Engineering
More informationExperimental Determination of Mechanical Parameters in Sensorless Vector-Controlled Induction Motor Drive
Experimental Determination of Mechanical Parameters in Sensorless Vector-Controlle Inuction Motor Drive V. S. S. Pavan Kumar Hari, Avanish Tripathi 2 an G.Narayanan 3 Department of Electrical Engineering,
More informationSelf-Erecting Inverted Pendulum: Swing up and Stabilization Control
Self-Erecting Inverted Pendulu: Swing up and Stabilization Control S. McGilvray (Winner of the IEEE Life Meber ward for best paper fro the Central Canada Council for the IEEE Student Paper Contest, ) Contents
More informationA method to determine relative stroke detection efficiencies from multiplicity distributions
A ethod to deterine relative stroke detection eiciencies ro ultiplicity distributions Schulz W. and Cuins K. 2. Austrian Lightning Detection and Inoration Syste (ALDIS), Kahlenberger Str.2A, 90 Vienna,
More informationAdaptive Congestion Control in ATM Networks
Aaptive Congestion Control in ATM Networks Farza Habibipour, Mehi Galily, Masou Faris, Ali Yazian Iran Telecounication Research Center, Ministry of ICT, Tehran, IRAN habibipor@itrc.ac.ir Abstract. In this
More informationDistributed Lossy Averaging
Distribute Lossy Averaging Han-I Su Departent of Electrical Engineering Stanfor University Stanfor, CA 94305, USA Eail: hanisu@stanforeu Abbas El Gaal Departent of Electrical Engineering Stanfor University
More informationHigh-Speed Smooth Cyclical Motion of a Hydraulic Cylinder
846 1 th International Conference on Fleible Autoation and Intelligent Manufacturing 00, Dresden, Gerany High-Speed Sooth Cyclical Motion of a Hydraulic Cylinder Nebojsa I. Jaksic Departent of Industrial
More informationLecture #8-3 Oscillations, Simple Harmonic Motion
Lecture #8-3 Oscillations Siple Haronic Motion So far we have considered two basic types of otion: translation and rotation. But these are not the only two types of otion we can observe in every day life.
More informationA Comparative Study of Two Permanent Magnet Motors Structures with Interior and Exterior Rotor
Journal of Asian Electric Vehicles, Volue 8, Nuber, June A Coparative Stuy of Two Peranent Magnet Motors Structures with Interior an Exterior Rotor Mohae Chaieb, Naourez Ben Haj, Jalila Kaouthar Kaoun
More informationBlock designs and statistics
Bloc designs and statistics Notes for Math 447 May 3, 2011 The ain paraeters of a bloc design are nuber of varieties v, bloc size, nuber of blocs b. A design is built on a set of v eleents. Each eleent
More information26 Impulse and Momentum
6 Ipulse and Moentu First, a Few More Words on Work and Energy, for Coparison Purposes Iagine a gigantic air hockey table with a whole bunch of pucks of various asses, none of which experiences any friction
More information2.9 Feedback and Feedforward Control
2.9 Feedback and Feedforward Control M. F. HORDESKI (985) B. G. LIPTÁK (995) F. G. SHINSKEY (970, 2005) Feedback control is the action of oving a anipulated variable in response to a deviation or error
More informationEffects of Restitution in the Application of Crush Coefficients
970960 Eects o Restitution in the pplication o Crush Coeicients Rayon R. McHenry an rian G. McHenry McHenry Consultants, Inc. Cary, NC STRCT Eects o restitution on aage interpretations are copoune by the
More informationAn inductance lookup table application for analysis of reluctance stepper motor model
ARCHIVES OF ELECTRICAL ENGINEERING VOL. 60(), pp. 5- (0) DOI 0.478/ v07-0-000-y An inuctance lookup table application for analysis of reluctance stepper motor moel JAKUB BERNAT, JAKUB KOŁOTA, SŁAWOMIR
More informationMATHEMATICAL MODEL OF THE ENERGETIC CONSUMPTION FOR SOIL DIGGING MACHINES IN GREENHOUSES
Bulletin of the Transilvania University of Braşov Vol. 3 (5) - 00 Series II: Forestry Wood Industry Agricultural Food Engineering MATHEMATICAL MODEL OF THE ENERGETIC CONSUMPTION FOR SOIL DIGGING MACHINES
More information2.141 Modeling and Simulation of Dynamic Systems Assignment #2
2.141 Modeling and Siulation of Dynaic Systes Assignent #2 Out: Wednesday Septeber 20, 2006 Due: Wednesday October 4, 2006 Proble 1 The sketch shows a highly siplified diagra of a dry-dock used in ship
More informationPARAMETER IDENTIFICATION OF A FEED DRIVE FOR HIGH SPEED MACHINE TOOLS
PARAMEER IDENIFICAION OF A FEED DRIVE FOR HIGH SPEED MACHINE OOLS Agustín Casquero, agustincasquero@gail.co Facultad de Ingeniería, Universidad Nacional de La Papa. Calle esq. 9, General Pico (636), La
More informationTIP TRAJECTORY TRACKING OF FLEXIBLE-JOINT MANIPULATORS
TIP TRAJECTORY TRACKING OF FLEXIBLE-JOINT MANIPULATORS A Thesis Subitted to the College o Graduate Studies and Research In Partial Fulillent o the Requireents For the Degree o Doctor o Philosophy In the
More informationA QUADRATIC PROGRAMMING APPROACH TO THE MINIMUM ENERGY PROBLEM OF A MOBILE ROBOT
A QUADRAIC PROGRAMMIG APPROACH O HE MIIMUM EERGY PROBLEM OF A MOBILE ROBO Alain Segundo Potts*, José Jaie da Cruz* Reinaldo Bernardi** *Departent o elecounications Control, São Paulo University, São Paulo,
More informationSupport Vector Machine Classification of Uncertain and Imbalanced data using Robust Optimization
Recent Researches in Coputer Science Support Vector Machine Classification of Uncertain and Ibalanced data using Robust Optiization RAGHAV PAT, THEODORE B. TRAFALIS, KASH BARKER School of Industrial Engineering
More informationCHECKLIST. r r. Newton s Second Law. natural frequency ω o (rad.s -1 ) (Eq ) a03/p1/waves/waves doc 9:19 AM 29/03/05 1
PHYS12 Physics 1 FUNDAMENTALS Module 3 OSCILLATIONS & WAVES Text Physics by Hecht Chapter 1 OSCILLATIONS Sections: 1.5 1.6 Exaples: 1.6 1.7 1.8 1.9 CHECKLIST Haronic otion, periodic otion, siple haronic
More informationDYNAMIC PERFORMANCE OF RELUCTANCE SYNCHRONOUS MACHINES
Annals of the University of Craiova, Electrical Engineering series, No 33, 9; ISSN 184-485 7 TH INTERNATIONAL CONFERENCE ON ELECTROMECHANICAL AN POWER SYSTEMS October 8-9, 9 - Iaşi, Romania YNAMIC PERFORMANCE
More informationIndex Terms: Placement machines, placement head, pick-and-place, electronics assembly equipment, constant force. I. INTRODUCTION
CONSTANT FORCE LINEAR PERMANENT MAGNET ACTUATORS Johannes J.H. Paulides, Meber, Laurentiu Encica, Meber, Koen J. Meessen Student Meber, and Elena A. Loonova, Senior Meber Abstract: In applications, such
More informationDesigning a Permanent Magnet Linear Generator Multi Air-gap Structure using the Finite Element Method.
Designing a Peranent Magnet Linear Generator Multi Air-gap Structure using the Finite Eleent Method. Pierre Kenfack, Daniel Matt, and Philippe Enrici Institute of Electronics and Systes, University Montpellier,
More informationROTATIONAL MOTION FROM TRANSLATIONAL MOTION
ROTATIONAL MOTION FROM TRANSLATIONAL MOTION Velocity Acceleration 1-D otion 3-D otion Linear oentu TO We have shown that, the translational otion of a acroscopic object is equivalent to the translational
More informationCHAPTER 37. Answer to Checkpoint Questions
1010 CHAPTER 37 DIFFRACTION CHAPTER 37 Answer to Checkpoint Questions 1. (a) expan; (b) expan. (a) secon sie axiu; (b) :5 3. (a) re; (b) violet 4. iinish 5. (a) increase; (b) sae 6. (a) left; (b) less
More informationm A 1 m mgd k m v ( C) AP Physics Multiple Choice Practice Oscillations
P Physics Multiple Choice Practice Oscillations. ass, attached to a horizontal assless spring with spring constant, is set into siple haronic otion. Its axiu displaceent fro its equilibriu position is.
More informationReducing Vibration and Providing Robustness with Multi-Input Shapers
29 Aerican Control Conference Hyatt Regency Riverfront, St. Louis, MO, USA June -2, 29 WeA6.4 Reducing Vibration and Providing Robustness with Multi-Input Shapers Joshua Vaughan and Willia Singhose Abstract
More informationControl of Brushless DC Motor with Direct Torque and Indirect Flux using SVPWM Technique
Indian Journal of Science and Technology, Vol 8(2), DOI: 10.17485/ijst/2015/v8i2/71211, Septeber 2015 ISSN (Print) : 0974-6846 ISSN (Online) : 0974-5645 Control of Brushless DC Motor with Direct Torque
More informationChapter 5 Sludge treatment
Chapter 5 Sluge treatent 5.1 Sluge efinition: Sluge is ae of soli aterials separate fro the water line uring wastewater treatent. In aition to solis, sluge contains a high percent of water. 5.2 Sluge sources:
More informationm A 9. The length of a simple pendulum with a period on Earth of one second is most nearly (A) 0.12 m (B) 0.25 m (C) 0.50 m (D) 1.0 m (E) 10.
P Physics Multiple Choice Practice Oscillations. ass, attache to a horizontal assless spring with spring constant, is set into siple haronic otion. Its axiu isplaceent fro its equilibriu position is. What
More informationPage 1. Physics 131: Lecture 22. Today s Agenda. SHM and Circles. Position
Physics 3: ecture Today s genda Siple haronic otion Deinition Period and requency Position, velocity, and acceleration Period o a ass on a spring Vertical spring Energy and siple haronic otion Energy o
More informationPrecedence Effect. Beamforming
Preceence Effect Beaforing Deo of the ranssen effect Deonstrates preceence Introuction to 3D Auio capture Directivity of icrophone. Oni-irectional Avantages are that icrophones capture all soun incluing
More informationGlobal safety formats in fib Model Code 2010 for design of concrete structures
Cervenka, V: Proceeings of the 11 th International Probabilistic Workshop, Brno 2013 Global safety forats in fib Moel Coe 2010 for esign of concrete structures Vlaiir Cervenka Cervenka Consulting, Prague,
More informationUfuk Demirci* and Feza Kerestecioglu**
1 INDIRECT ADAPTIVE CONTROL OF MISSILES Ufuk Deirci* and Feza Kerestecioglu** *Turkish Navy Guided Missile Test Station, Beykoz, Istanbul, TURKEY **Departent of Electrical and Electronics Engineering,
More informationReading from Young & Freedman: For this topic, read the introduction to chapter 25 and sections 25.1 to 25.3 & 25.6.
PHY10 Electricity Topic 6 (Lectures 9 & 10) Electric Current and Resistance n this topic, we will cover: 1) Current in a conductor ) Resistivity 3) Resistance 4) Oh s Law 5) The Drude Model of conduction
More informationNUMERICAL MODELLING OF THE TYRE/ROAD CONTACT
NUMERICAL MODELLING OF THE TYRE/ROAD CONTACT PACS REFERENCE: 43.5.LJ Krister Larsson Departent of Applied Acoustics Chalers University of Technology SE-412 96 Sweden Tel: +46 ()31 772 22 Fax: +46 ()31
More informationAlgorithms for parallel processor scheduling with distinct due windows and unit-time jobs
BULLETIN OF THE POLISH ACADEMY OF SCIENCES TECHNICAL SCIENCES Vol. 57, No. 3, 2009 Algoriths for parallel processor scheduling with distinct due windows and unit-tie obs A. JANIAK 1, W.A. JANIAK 2, and
More informationCh. 6 Single Variable Control ES159/259
Ch. 6 Single Variable Control Single variable control How o we eterine the otor/actuator inut o a to coan the en effector in a eire otion? In general, the inut voltage/current oe not create intantaneou
More informationPhysics 140 D100 Midterm Exam 2 Solutions 2017 Nov 10
There are 10 ultiple choice questions. Select the correct answer for each one and ark it on the bubble for on the cover sheet. Each question has only one correct answer. (2 arks each) 1. An inertial reference
More informationSwing Up a Pendulum by Energy Control
International ournal o Engineering and Technology Volue 2 No., March, 22 Swing Up a Pendulu by Energy Control Araat Zaidan, Bashir M.Y.Nouri, Basi Alsayid, Departent o Electrical Engineering, Palestine
More informationThis is a repository copy of Analytical optimisation of electromagnetic design of a linear (tubular) switched reluctance motor.
This is a repository copy of Analytical optiisation of electroagnetic design of a linear (tubular) switched reluctance otor. White Rose Research Online URL for this paper: http://eprints.whiterose.ac.uk/907/
More informationComputer Model For Sieves Vibrations Analysis, Using an Algorithm Based on the False-Position Method
Aerican Journal of Applied Sciences 6 (): 48-56, 9 ISSN 546-939 9 Science Publications Coputer Model For Sieves Vibrations Analysis, Using an Algorith Based on the False-Position Method Dinu I. Stoicovici,
More informationOscillations: Review (Chapter 12)
Oscillations: Review (Chapter 1) Oscillations: otions that are periodic in tie (i.e. repetitive) o Swinging object (pendulu) o Vibrating object (spring, guitar string, etc.) o Part of ediu (i.e. string,
More informationSeismic Analysis of Structures by TK Dutta, Civil Department, IIT Delhi, New Delhi.
Seisic Analysis of Structures by K Dutta, Civil Departent, II Delhi, New Delhi. Module 5: Response Spectru Method of Analysis Exercise Probles : 5.8. or the stick odel of a building shear frae shown in
More informationChapter 4 FORCES AND NEWTON S LAWS OF MOTION PREVIEW QUICK REFERENCE. Important Terms
Chapter 4 FORCES AND NEWTON S LAWS OF MOTION PREVIEW Dynaics is the study o the causes o otion, in particular, orces. A orce is a push or a pull. We arrange our knowledge o orces into three laws orulated
More informationL2 IntroSurvey. EIEN20 Design of Electrical Machines, IEA, Today s goal. L2: Variety of electrical machines.
L: Variety of electrical achines Machine construction: an overview Transforer is it achine too? Today s goal ntroduction to achine construction Constructional layouts and echanical arrangeents Supply &
More informationTorsion Experiment. Encoder #3 ( 3 ) Third encoder/disk for Model 205a only. Figure 1: ECP Torsion Experiment
Torsion Experient Introduction For the Torsion lab, there are two required experients to perfor and one extra credit assignent at the end. In experient 1, the syste paraeters need to be identified so that
More informationRobust Tracking Control of Robot Manipulator Using Dissipativity Theory
Moern Applie Science July 008 Robust racking Control of Robot Manipulator Using Dissipativity heory Hongrui Wang Key Lab of Inustrial Computer Control Engineering of Hebei Province Yanshan University Qinhuangao
More informationModel Fitting. CURM Background Material, Fall 2014 Dr. Doreen De Leon
Model Fitting CURM Background Material, Fall 014 Dr. Doreen De Leon 1 Introduction Given a set of data points, we often want to fit a selected odel or type to the data (e.g., we suspect an exponential
More informationModel Based Control versus Classical Control for Parallel Robots
odel Based Control versus Classical Control for Parallel Robots Květoslav Belda Institute of Inforation heory and Autoation, Acadey of Sciences of the Czech Republic, Pod vodárensou věží 4, 82 08 Praha
More informationReduced Length Checking Sequences
Reduced Length Checing Sequences Robert M. Hierons 1 and Hasan Ural 2 1 Departent of Inforation Systes and Coputing, Brunel University, Middlesex, UB8 3PH, United Kingdo 2 School of Inforation echnology
More information1 (40) Gravitational Systems Two heavy spherical (radius 0.05R) objects are located at fixed positions along
(40) Gravitational Systes Two heavy spherical (radius 0.05) objects are located at fixed positions along 2M 2M 0 an axis in space. The first ass is centered at r = 0 and has a ass of 2M. The second ass
More informationDIRECT TORQUE CONTROL OF INDUCTION MACHINES CONSIDERING THE IRON LOSSES
DIRECT TORQUE CONTROL OF INDUCTION MACHINES CONSIDERING THE IRON LOSSES TRUC PHAM-DINH A thesis subitted in partial fulfilent of the requireents of Liverpool John Moores University for the degree of Doctor
More informationPhysics 2107 Oscillations using Springs Experiment 2
PY07 Oscillations using Springs Experient Physics 07 Oscillations using Springs Experient Prelab Read the following bacground/setup and ensure you are failiar with the concepts and theory required for
More informationExample A1: Preparation of a Calibration Standard
Suary Goal A calibration standard is prepared fro a high purity etal (cadiu) with a concentration of ca.1000 g l -1. Measureent procedure The surface of the high purity etal is cleaned to reove any etal-oxide
More information1 Identical Parallel Machines
FB3: Matheatik/Inforatik Dr. Syaantak Das Winter 2017/18 Optiizing under Uncertainty Lecture Notes 3: Scheduling to Miniize Makespan In any standard scheduling proble, we are given a set of jobs J = {j
More informationINCLUDING MODEL UNCERTAINTY IN THE MODEL PREDICTIVE CONTROL WITH OUTPUT FEEDBACK
Brazilian Journal of Cheical Engineering ISSN 004-6632 Printe in Brazil Vol. 9, No. 04, pp. 475-482, October - Deceber 2002 INCLUDING MODEL UNCERAINY IN HE MODEL PREDICIVE CONROL WIH OUPU FEEDBACK M.A.Rorigues
More informationPolygonal Designs: Existence and Construction
Polygonal Designs: Existence and Construction John Hegean Departent of Matheatics, Stanford University, Stanford, CA 9405 Jeff Langford Departent of Matheatics, Drake University, Des Moines, IA 5011 G
More informationAn Improved Particle Filter with Applications in Ballistic Target Tracking
Sensors & ransducers Vol. 72 Issue 6 June 204 pp. 96-20 Sensors & ransducers 204 by IFSA Publishing S. L. http://www.sensorsportal.co An Iproved Particle Filter with Applications in Ballistic arget racing
More informationChapter 6 1-D Continuous Groups
Chapter 6 1-D Continuous Groups Continuous groups consist of group eleents labelled by one or ore continuous variables, say a 1, a 2,, a r, where each variable has a well- defined range. This chapter explores:
More informationA 30 o 30 o M. Homework #4. Ph 231 Introductory Physics, Sp-03 Page 1 of 4
Hoework #4. Ph 231 Introductory Physics, Sp-03 Page 1 o 4 4-1A. A particle o ass 2 kg is initially at rest at the origin x = 0. I the only orce acting on the particle is a constant 4 in the x-direction,
More informationACTIVE VIBRATION CONTROL FOR STRUCTURE HAVING NON- LINEAR BEHAVIOR UNDER EARTHQUAKE EXCITATION
International onference on Earthquae Engineering and Disaster itigation, Jaarta, April 14-15, 8 ATIVE VIBRATION ONTROL FOR TRUTURE HAVING NON- LINEAR BEHAVIOR UNDER EARTHQUAE EXITATION Herlien D. etio
More informationDual porosity DRM formulation for flow and transport through fractured porous media
Boundary Eleents XXVII 407 Dual porosity DRM orulation or lo and transport through ractured porous edia T. aardzioska & V. Popov Wessex Institute o Technology, UK Abstract The ain objective o this ork
More informationIntroduction to Discrete Optimization
Prof. Friedrich Eisenbrand Martin Nieeier Due Date: March 9 9 Discussions: March 9 Introduction to Discrete Optiization Spring 9 s Exercise Consider a school district with I neighborhoods J schools and
More informationUse of PSO in Parameter Estimation of Robot Dynamics; Part One: No Need for Parameterization
Use of PSO in Paraeter Estiation of Robot Dynaics; Part One: No Need for Paraeterization Hossein Jahandideh, Mehrzad Navar Abstract Offline procedures for estiating paraeters of robot dynaics are practically
More information