Linear-Quadratic-Gaussian (LQG) Controller for Two link- robotic Manipulator Control
|
|
- Mervin Hensley
- 5 years ago
- Views:
Transcription
1 Lnear-Quadrat-Gaussan (LQG) Controller for Two lnk- robot Manpulator Control Lela Fallah Aragh, M Habbnejad Korayem, Amn Nkoobn Abstrat Ths paper presents a new method for the ontrol of Two lnk- robot manpulator systems usng Lnear-Quadrat- Gaussan (LQG), n Ths method Lnear-Quadrat-Gaussan (LQG) that s a modern state-spae tehnque for desgnng optmal dynam regulators by kalman used for the ontrol of Two lnk- robot manpulator systems The smulaton result are very promsng Index Terms Two lnk- robot manpulator systems, usng Lnear-Quadrat-Gaussan ontroller, optmal dynam regulators I INTRODUCTION In the reent years usng ntellgee ontrol suh as fuzzy ontrol, Neural Network, Neuro Fuzzy and beause that they an ontrol nonlnear systems that would be dffult or mpossble to model mathematally In the reently years In Dynam ontrol of robot have been utlzed n many researhers work n ths area Suh as Lanfang Tan et al use a neural network approah for the moton ontrol of onstraned flexble manpulators robots [], Y, et al have nvestgated the robustness and stablty of a fuzzy log ontroller appled to a robot manpulator wth unertantes suh as frton, unmodeled dynams, and external dsturbane et [], Kumbla et al have mplemented herarhal ontrol on robot manpulator usng fuzzy log [3] Bannerjee, et al have used a Fuzzy Log Controller to aheve poston ontrol of a two-lnk manpulator [4] Adams, et al [5] have used GA to optmze the membershp funtons and rule bases of a mult-stage fuzzy PID ontroller wth a fuzzy swth ror robot ontrol Brudka, et al presented an ntellgent robot ontrol system whh employs ultrason dstane measurements, And for Conseutve stages of data proessng they used to neural networks applatons [6], Adamv, et al used neural networks applaton for moble robot ontrol on predetermned trajetory of the road [7], Ya- Chen, et al used an Fuzzy neural adaptve ontroller to multple-lnk robot ontrol [8], Devendra P, et al used the proportonal plus dervatve (PD) ontrol wth the PD ontroller gan parameters optmzed va Genet Algorthm Lela Fallah Aragh, PhD Student, Eletral Eng Dept, Tehran Researh Sene Azad Unversty, Tehran, Iran (orrespondng author to provde phone: e-mal: l_falah@srbauar) M Habbnejad Korayem, Professor, Eletral Eng Dept, Tehran Unversty of sene & tehnology, (e-mal: hkorayem@ustar) Amn Nkoobn, Assstant Professor, Eletral Eng Dept, Tehran Unversty of sene & tehnology (e-mal: ankoobn@ustar) (GA) And Fuzzy Log for ontrol of Two lnk- robot [9], ZG Zhang, et al report on the desgn and stablty analyss of a smple quadruped runnng ontroller that an autonomously generate steady runnng wth good energy effeny and suppress suh dsturbanes as rregulartes of terran [0], Dongbng Gu, et al presented a new path-trakng sheme for a ar-lke moble robot based on neural predtve ontrol, they employed A mult-layer bakpropagaton neural network to model non-lnear knemats of the robot nstead of a lnear regresson estmator n order to adapt the robot to a large operatng range [], Mathew L, et al studed on the mplementaton of several Intellgent ontrol tehnques as appled to the balanng of the nverted wedge problem These nluded a bas four-nput dret fuzzy ontroller (nludng the use of the nonlnear nput term) and an adaptve fuzzy ontrol tehnque known as the FMRLC [] Lawrene J Alder, et al developed a new approah to dentfaton s That utlzes a nomnal ontroller n order to solate the dynam effets related to the unertan parameters from the other known system dynams[], John L Meyery, et al presented the results of postve poston feedbak (PPF) ontrol and lnear quadrat Gaussan (LQG) ontrol for vbraton suppresson of a flexble struture usng pezoerams [3], In ths paper Two lnk- robot manpulator systems s ontrolled, The problem statement s gven n seton II In seton III LQG ontrollers s proposed Smulaton results are gven n seton IV Fnally seton V nludes onlusons, II DYNAMIC EQUATION OF TWO LINK- ROBOTIC MANIPULATOR SYSTEMS [] In ths seton we derve the equatons of moton for an ndvdual lnk based on the dret method has been derved, e Newton-Euler Formulaton The moton of a rgd body an be deomposed nto the translatonal moton wth respet to an arbtrary pont fxed to the rgd body, and the rotatonal moton of the rgd body about that pont The dynam equatons of a rgd body an also be represented by two equatons: one desrbes the translatonal moton of the entrod (or enter of mass), whle the other desrbes the rotatonal moton about the entrod The former s Newton's
2 equaton of moton for a mass partle, and the latter s alled Euler's equaton of moton Fgure shows all the fores and moments atng on lnk III Fg : Free body dagram of lnk n moton Let be V the lnear veloty of the entrod of lnk wth referene to the base oordnate frame O-xyz, whh s an nertal referene frame The nertal fore s then gven by m V, where m s the mass of the lnk and V s the tme dervatve of V Based on D Alembert s prnple, the equaton of moton s then obtaned by addng the nertal fore to the stat balane of fores n eq( ) so that, f, + + m g m V 0 f, 0,,, n f, and f, + are the ouplng fores appled to lnk by lnks - and +, respetvely, and g s the aeleraton of gravty Addng these terms to the orgnal balane of moments we have: N, N, + ( r, r, ) f, + ( r, ) f, + I ω ω ( I ω ) 0 () Smlarly, elmnatng f 0, yelds, N, and N, + are the moment appled to lnk by lnks - and +, respetvely If we onsder two ndvdual lnks robot, Let us obtan the Newton-Euler equatons of moton for the two ndvdual lnks () IV Fg: Mass propertes of two planar robot From eq () and (), the Newton-Euler equatons for lnk are gven by: f f + m g m V (3) 0,, 0 0,, 0, 0,,, N N ( r ) f + ( r ) f I ω 0 (4) Note that all vetors are x, so that moment N -, and the other vetor produts are salar quanttes Smlarly, for lnk, f m g m V (5), + 0,,, N ( r ) f I ω 0 (6) To obtan losed-form dynam equatons, we frst elmnate the onstrant fores and separate them from the jont torques, so as to expltly nvolve the jont torques n the dynam equatons For the planar manpulator, the jont torques τ and τ are equal to the ouplng moments: N, τ (7) Substtutng eq(7) nto eq(6) :, τ ( r ) ( m V m g) I ω 0 (8) τ τ ( r0, ) mv + ( r0, ) mv + ( r0, ) mg + ( r0, ) mg I ω 0 (9) Next, we rewrtev, ω and r, usng jont dsplaements, whh are ndependent varables Note
3 that ω s the angular veloty relatve to the base oordnate frame, whle s measured relatve to lnk Then, we have, ω ω + (0) The lnear velotes an be wrtten as l sn( ) V () l os( ) V τ () { l sn( ) + l sn( + ) } l sn( + ) { l os( ) + l os( + ) } l os( + ) H + H h h + G τ (3) H + H h+ G That: H m l + I + m l + l + ll os( )) + m l I ( I H + (4) dfferene between desred and Atual responses What s then requred s to desgn a ontroller so that the plant ontroller ombnaton satsfes the spefatons The LQG ontrol s a modern state spae tehnque for desgnng optmal dynam regulators It enables a trade off n performane and ontrol effort, and takes nto aount proess and measurement nose Lnear-Quadrat-Gaussan (LQG) ontrol s a modern statespae tehnque for desgnng optmal dynam regulators, The LQG regulator onssts of an optmal state-feedbak gan and a Kalman state estmator The frst desgn step s to seek a state-feedbak law that mnmzes the ost funton of regulaton performane, whh s measured by a quadrat performane rteron wth user-spefed weghtng matres, and to defne the tradeoff between regulaton performane and ontrol effort The next desgn step s to derve a state estmator usng a Kalman flter beause the optmal state feedbak annot be mplemented wthout full state measurement Sne the Kalman flter s an optmal estmator when dealng wth Gaussan whte nose, t mnmzes the G m l + H g os( ) + mg{ l os( + ) l os( )} m l + ll os( )) + ( I h m l sn( ) (5) l G m g l os( + ) (6) asymptot ovarane of the estmaton error In the optmal feedbak ontrol, a gan matrx s sought to mnmze a spefed quadrat performane rteron J (u) expressed as the ntegral of a quadrat form n the state vetor x plus a seond quadrat form n the ontrol vetor u, e III LQG ontroller [4, 5, 6, 7] J ( u) 0 T ( x Qx + u T Ru) dt ( 7) In a typal ontrol system desgn problem, nputs are a dynam system to be ontrolled (plant), a desrpton of the types of nputs to be enountered, and spefatons Regardng aeptable values of system errors, e, the The weghtng matres Q and R are user-spefed and defne the trade-off between Regulaton performane (how fast x(t) goes to zero) and ontrol effort [6,7] The frst
4 desgn step seeks a state feedbak law u kx that To form the LQG regulator, smply onnet the Kalman flter mnmzes the ost funton J (u) The mnmzng gan and LQ optmal gan K as shown n Fgure 5-3 matrx K s obtaned by solvng an algebra Rat equaton [4] Ths gan s usually alled the LQ-optmal gan Sometmes, the proess seekng the LQ state feedbak regulator, e LQ-optmal gan matrx k, s alled Lnear Quadrat Regulator (LQR) desgn It s lear that the LQ-optmal state feedbak u kx s not mplemental wthout full state measurement However, one Fgure4 Blok dagram of LQG regulator an derve a state estmate x suh that u kx remans Ths regulator has state spae equatons: optmal for output feedbak problem Ths state estmate s generated by Kalman flter [5] as shown below: x ( A LC + Bk) x + Ly0 (9) u kx (0) In addton to LQG desgn, a Dsturbane Aommodate Control (DAC) desgn and a hybrd LQG/DAC ontrol system Fg3: Blok dagram of the Kalman estmator Mathematally, the Kalman state estmator an be expressed by: x A x+ Bu + L( y0 C x) ( 8) wth two nputs, ontrols u and measurements y 0 Determnes the Kalman gan L n onjunton wth dynam systems through an are also studed n ths hapter Hene, nne ases wll have to be dsussed, whh are three ontrol systems, the LQG, the DAC and the hybrd LQG/DAC, n onjunton wth three dfferent ontrol models, the MCC model, the SCC model and the SSCC model, respetvely I n ths paper LQG regulator has been used for two lnk- robot manpulator systems Fgure 5 shows the struture of system that used n ths system [6] Algebra Rat equaton The Kalman flter s an optmal estmator when dealng wth Gaussan whte nose Spefally, t mnmzes the asymptot ovarane of the x estmaton error x
5 IN LPF T q IN LPF T q LQG Controller NOISE Fg 7: the output of two lnk- robot manpulator systems LQG Controller NOISE Fg 5: struture of LQG regulator for Two lnk- robot manpulator systems As the frst method for losed loop ontrol of two lnk robot the LQG regulator ontroller has been used, fgure 8 shows the smulaton result IV SIMULATION RESULT In the frst the dynam model of two lnk- robot manpulator systems has been smulated usng Matlab software 007 as you see the system s unstable Fgure 6 shows the shemat of two lnk- robot manpulator systems and fgure 7 shows the smulaton result for step nput: Fg 6: shemat of the two lnk- robot manpulator systems Fg 8: the output of two lnk- robot manpulator systems usng LQG regulator,
6 V CONCLUSION Ths paper presents a new method for the ontrol of Two lnk- robot manpulator systems usng method Lnear-Quadrat- Gaussan (LQG) REFERENCES [] Lanfang Tan, Jun Wang, and Zongyuan Mao, "Constraned Moton Control of Flexble Robot Manpulators Based on Reurrent Neural Networks" IEEE TRANSACTIONS ON SYSTEMS, MAN, AND CYBERNETICS PART B: CYBERNETICS, VOL 34, NO 3, JUNE 004 [] Y, SY and Chung, M, J, 997, A Robust Fuzzy Log Controller for Robot Manpulators wth Unertantes, IEEE Transatons on Systems, Man and Cybernets, 7, No 4, pp [3] K umbla, KK and Jamshd, M, 994, Control of Robot Manpulator Usng Fuzzy Log, Proeedngs of the Thrd IEEE Conferene on Fuzzy Systems, Vol, pp [4] Bannerjee, S and Woo, PY, 993, Fuzzy Log Control of Robot Manpulator, IEEE Conferene on Control Applatons, pp [5] Adams, JM and Rattan, KS, 00, Genet Mult-Stage Fuzzy PID Controller wth Fuzzy Swth, Proeedngs of the IEEE Internatonal Conferene on Control Applatons, pp [6] Brudka, M Paut, A, " Intellgent robot ontrol usng ultrason measurements" Proeedngs of the 6th IEEE Instrumentaton and Measurement Tehnology Conferene, 999 IMTC/99 [7] Adamv, O Koval, V Turhenko, I, Predetermned movement of moble robot usng neural networks" Proeedngs of the Seond IEEE Internatonal Workshop on Intellgent Data Aquston and Advaned Computng Systems: Tehnology and Applatons, 003 [8] Petropoulaks, L, " Intellgent ontrol usng agents and fuzzy behavoural strutures" Proeedngs of the 000 IEEE Internatonal Symposum on Intellgent Control, 000 [9] Ya-Chen Hsu Guanrong Chen Malk, HA, " Fuzzy neural adaptve ontroller desgn: wth applaton to multple-lnk robot ontrol" IEEE Internatonal Conferene on Neural Networks,997, [0] Dongbng Gu and Huosheng Hu, Neural Predtve Control for a Carlke Moble Robot Internatonal Journal of Robots and Autonomous Systems, Vol 39, No -3, May, 00 [] Mathew L Moore, John T Musaho, Kevn M Passno, Genet adaptve ontrol for an nverted wedge: experments and omparatve analyses Engneerng Applatons of Artfal Intellgene 00 [] Lawrene J Alder, Stephen M Rok, Adaptve Control of a Flexble- Lnk Robot Manpulator Presented at The Ameran Control Conferene, San Fransso, CA June 993 [3] John L Meyery, Wllam B Harrngtony, Brj N Agrawal and Gangbng Song, Vbraton suppresson of a spaeraft flexble appendage usng smart materal Smart Mater Strut 7 (998) Prnted n the UK [4] Dorato, P, Abdallah, C and Cerone V, LINEAR-QUADRATIC CONTROL AN INTRODUCTION, Prente-Hall, In, New Jersey, 995 [5] Fredland, B, CONTROL SYSTEM DESIGN, AN INTRODUCTION TO STATE-SPACE METHODS MGraw-Hll Book Company, 986 [6] Toolbox, Matlab 008 [7] ASHWIN DHABALE, R N BANAVAR and M V DHEKANE, LQG ontroller desgns from redued order models for a launh vehle S adhan Vol 33, Part, February 008, pp 4 Prnted n Inda
Controller Design for Networked Control Systems in Multiple-packet Transmission with Random Delays
Appled Mehans and Materals Onlne: 03-0- ISSN: 66-748, Vols. 78-80, pp 60-604 do:0.408/www.sentf.net/amm.78-80.60 03 rans eh Publatons, Swtzerland H Controller Desgn for Networed Control Systems n Multple-paet
More informationFAULT DETECTION AND IDENTIFICATION BASED ON FULLY-DECOUPLED PARITY EQUATION
Control 4, Unversty of Bath, UK, September 4 FAUL DEECION AND IDENIFICAION BASED ON FULLY-DECOUPLED PARIY EQUAION C. W. Chan, Hua Song, and Hong-Yue Zhang he Unversty of Hong Kong, Hong Kong, Chna, Emal:
More informationAdaptive Multilayer Neural Network Control of Blood Pressure
Proeedng of st Internatonal Symposum on Instrument Sene and Tenology. ISIST 99. P4-45. 999. (ord format fle: ISIST99.do) Adaptve Multlayer eural etwork ontrol of Blood Pressure Fe Juntao, Zang bo Department
More informationParticle Swarm Optimization of Neural Controller for Tanker Ship Steering
Proeedngs of the th WSEAS Internatonal Conferene on SYSEMS, Agos Nkolaos, Crete Island, Greee, July 3-5, 007 394 Partle Swarm Optmzaton of Neural Controller for anker Shp Steerng C. K. Loo, Nkos, E. Mastoraks
More informationKey words: path synthesis, joint clearances, Lagrange s equation, Differential evaluation (DE), optimization.
Rub Mshra, T.K.Naskar, Sanb Ahara / nternatonal Journal of Engneerng Researh and Applatons (JERA) SSN: 8-96 www.era.om Vol., ssue, Januar -Februar 0, pp.9-99 Snthess of oupler urve of a Four Bar Lnkage
More informationJSM Survey Research Methods Section. Is it MAR or NMAR? Michail Sverchkov
JSM 2013 - Survey Researh Methods Seton Is t MAR or NMAR? Mhal Sverhkov Bureau of Labor Statsts 2 Massahusetts Avenue, NE, Sute 1950, Washngton, DC. 20212, Sverhkov.Mhael@bls.gov Abstrat Most methods that
More informationNMT EE 589 & UNM ME 482/582 ROBOT ENGINEERING. Dr. Stephen Bruder NMT EE 589 & UNM ME 482/582
NMT EE 589 & UNM ME 48/58 ROBOT ENGINEERING Dr. Stephen Bruder NMT EE 589 & UNM ME 48/58 7. Robot Dynamcs 7.5 The Equatons of Moton Gven that we wsh to fnd the path q(t (n jont space) whch mnmzes the energy
More information425. Calculation of stresses in the coating of a vibrating beam
45. CALCULAION OF SRESSES IN HE COAING OF A VIBRAING BEAM. 45. Calulaton of stresses n the oatng of a vbratng beam M. Ragulsks,a, V. Kravčenken,b, K. Plkauskas,, R. Maskelunas,a, L. Zubavčus,b, P. Paškevčus,d
More informationTransfer Functions. Convenient representation of a linear, dynamic model. A transfer function (TF) relates one input and one output: ( ) system
Transfer Functons Convenent representaton of a lnear, dynamc model. A transfer functon (TF) relates one nput and one output: x t X s y t system Y s The followng termnology s used: x y nput output forcng
More informationAn Application of the IMSC on a Non-linear Flexible Structure: Numerical Analysis and Experimental Validation
, July 6-8, 2011, London, U.K. An Applaton of the IMSC on a Non-lnear Flexble Struture: Numeral Analyss and Expermental Valdaton G. Caulan, F. Resta, F. Rpamont Abstrat he ndependent modal ontrol to suppress
More informationSliding Mode Control Based on Synthesis of Approximating State Feedback for Robotic Manipulator
Internatonal Journal on Eletral Engneerng and Informats - Volume 9, Number, September 07 Sldng Mode Control Based on Synthess of Approxmatng State Feedbak for Robot Manpulator Dmtr Mahayana Shool of Eletral
More informationStudy on Active Micro-vibration Isolation System with Linear Motor Actuator. Gong-yu PAN, Wen-yan GU and Dong LI
2017 2nd Internatonal Conference on Electrcal and Electroncs: echnques and Applcatons (EEA 2017) ISBN: 978-1-60595-416-5 Study on Actve Mcro-vbraton Isolaton System wth Lnear Motor Actuator Gong-yu PAN,
More informationTracking with Kalman Filter
Trackng wth Kalman Flter Scott T. Acton Vrgna Image and Vdeo Analyss (VIVA), Charles L. Brown Department of Electrcal and Computer Engneerng Department of Bomedcal Engneerng Unversty of Vrgna, Charlottesvlle,
More informationOn Adaptive Control of Simulated Moving Bed Plants. Plants Using Comsol s Simulink Interface. Speaker: Marco Fütterer
daptve Smulated Movng ed Plants Usng Comsol s Smulnk Interfae Speaker: Maro Fütterer Insttut für utomatserungstehnk Otto-von-Guerke Unverstät Unverstätsplatz, D-39106 Magdeburg Germany e-mal: maro.fuetterer@ovgu.de
More informationComplement of an Extended Fuzzy Set
Internatonal Journal of Computer pplatons (0975 8887) Complement of an Extended Fuzzy Set Trdv Jyot Neog Researh Sholar epartment of Mathemats CMJ Unversty, Shllong, Meghalaya usmanta Kumar Sut ssstant
More informationThe corresponding link function is the complementary log-log link The logistic model is comparable with the probit model if
SK300 and SK400 Lnk funtons for bnomal GLMs Autumn 08 We motvate the dsusson by the beetle eample GLMs for bnomal and multnomal data Covers the followng materal from hapters 5 and 6: Seton 5.6., 5.6.3,
More informationALGEBRAIC SCHUR COMPLEMENT APPROACH FOR A NON LINEAR 2D ADVECTION DIFFUSION EQUATION
st Annual Internatonal Interdsplnary Conferene AIIC 03 4-6 Aprl Azores Portugal - Proeedngs- ALGEBRAIC SCHUR COMPLEMENT APPROACH FOR A NON LINEAR D ADVECTION DIFFUSION EQUATION Hassan Belhad Professor
More informationCharged Particle in a Magnetic Field
Charged Partle n a Magnet Feld Mhael Fowler 1/16/08 Introduton Classall, the fore on a harged partle n eletr and magnet felds s gven b the Lorentz fore law: v B F = q E+ Ths velot-dependent fore s qute
More informationDOAEstimationforCoherentSourcesinBeamspace UsingSpatialSmoothing
DOAEstmatonorCoherentSouresneamspae UsngSpatalSmoothng YnYang,ChunruWan,ChaoSun,QngWang ShooloEletralandEletronEngneerng NanangehnologalUnverst,Sngapore,639798 InsttuteoAoustEngneerng NorthwesternPoltehnalUnverst,X
More informationLecture 23: Newton-Euler Formulation. Vaibhav Srivastava
Lecture 23: Newton-Euler Formulaton Based on Chapter 7, Spong, Hutchnson, and Vdyasagar Vabhav Srvastava Department of Electrcal & Computer Engneerng Mchgan State Unversty Aprl 10, 2017 ECE 818: Robotcs
More informationThe Chaotic Robot Prediction by Neuro Fuzzy Algorithm (2) = θ (3) = ω. Asin. A v. Mana Tarjoman, Shaghayegh Zarei
The Chaotc Robot Predcton by Neuro Fuzzy Algorthm Mana Tarjoman, Shaghayegh Zare Abstract In ths paper an applcaton of the adaptve neurofuzzy nference system has been ntroduced to predct the behavor of
More informationIterative General Dynamic Model for Serial-Link Manipulators
EEL6667: Knematcs, Dynamcs and Control of Robot Manpulators 1. Introducton Iteratve General Dynamc Model for Seral-Lnk Manpulators In ths set of notes, we are gong to develop a method for computng a general
More informationChapter 11 Angular Momentum
Chapter 11 Angular Momentum Analyss Model: Nonsolated System (Angular Momentum) Angular Momentum of a Rotatng Rgd Object Analyss Model: Isolated System (Angular Momentum) Angular Momentum of a Partcle
More informationSo far: simple (planar) geometries
Physcs 06 ecture 5 Torque and Angular Momentum as Vectors SJ 7thEd.: Chap. to 3 Rotatonal quanttes as vectors Cross product Torque epressed as a vector Angular momentum defned Angular momentum as a vector
More informationLinear Feature Engineering 11
Lnear Feature Engneerng 11 2 Least-Squares 2.1 Smple least-squares Consder the followng dataset. We have a bunch of nputs x and correspondng outputs y. The partcular values n ths dataset are x y 0.23 0.19
More informationInterval Valued Neutrosophic Soft Topological Spaces
8 Interval Valued Neutrosoph Soft Topologal njan Mukherjee Mthun Datta Florentn Smarandah Department of Mathemats Trpura Unversty Suryamannagar gartala-7990 Trpura Indamal: anjan00_m@yahooon Department
More informationRigid body simulation
Rgd bod smulaton Rgd bod smulaton Once we consder an object wth spacal etent, partcle sstem smulaton s no longer suffcent Problems Problems Unconstraned sstem rotatonal moton torques and angular momentum
More informationHomework Math 180: Introduction to GR Temple-Winter (3) Summarize the article:
Homework Math 80: Introduton to GR Temple-Wnter 208 (3) Summarze the artle: https://www.udas.edu/news/dongwthout-dark-energy/ (4) Assume only the transformaton laws for etors. Let X P = a = a α y = Y α
More informationECE 6340 Intermediate EM Waves. Fall Prof. David R. Jackson Dept. of ECE. Notes 3
C 634 Intermedate M Waves Fall 216 Prof. Davd R. akson Dept. of C Notes 3 1 Types of Current ρ v Note: The free-harge densty ρ v refers to those harge arrers (ether postve or negatve) that are free to
More informationImproving the Performance of Fading Channel Simulators Using New Parameterization Method
Internatonal Journal of Eletrons and Eletral Engneerng Vol. 4, No. 5, Otober 06 Improvng the Performane of Fadng Channel Smulators Usng New Parameterzaton Method Omar Alzoub and Moheldn Wanakh Department
More informationVoltammetry. Bulk electrolysis: relatively large electrodes (on the order of cm 2 ) Voltammetry:
Voltammetry varety of eletroanalytal methods rely on the applaton of a potental funton to an eletrode wth the measurement of the resultng urrent n the ell. In ontrast wth bul eletrolyss methods, the objetve
More informationAPPROXIMATE OPTIMAL CONTROL OF LINEAR TIME-DELAY SYSTEMS VIA HAAR WAVELETS
Journal o Engneerng Sene and ehnology Vol., No. (6) 486-498 Shool o Engneerng, aylor s Unversty APPROIAE OPIAL CONROL OF LINEAR IE-DELAY SYSES VIA HAAR WAVELES AKBAR H. BORZABADI*, SOLAYAN ASADI Shool
More informationPhysics 181. Particle Systems
Physcs 181 Partcle Systems Overvew In these notes we dscuss the varables approprate to the descrpton of systems of partcles, ther defntons, ther relatons, and ther conservatons laws. We consder a system
More informationELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM
ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM An elastc wave s a deformaton of the body that travels throughout the body n all drectons. We can examne the deformaton over a perod of tme by fxng our look
More informationFriction parameters identification and compensation of LuGre model base on genetic algorithms
Internatonal Sympoum on Computer & Informat (ISCI 015) Frton parameter dentfaton and ompenaton of LuGre model bae on genet algorthm Yuqn Wen a, Mng Chu b and Hanxu Sun Shool of Automaton, Bejng Unverty
More informationIntroduction to Molecular Spectroscopy
Chem 5.6, Fall 004 Leture #36 Page Introduton to Moleular Spetrosopy QM s essental for understandng moleular spetra and spetrosopy. In ths leture we delneate some features of NMR as an ntrodutory example
More information1 Derivation of Point-to-Plane Minimization
1 Dervaton of Pont-to-Plane Mnmzaton Consder the Chen-Medon (pont-to-plane) framework for ICP. Assume we have a collecton of ponts (p, q ) wth normals n. We want to determne the optmal rotaton and translaton
More informationPhysics 5153 Classical Mechanics. D Alembert s Principle and The Lagrangian-1
P. Guterrez Physcs 5153 Classcal Mechancs D Alembert s Prncple and The Lagrangan 1 Introducton The prncple of vrtual work provdes a method of solvng problems of statc equlbrum wthout havng to consder the
More informationPhase Transition in Collective Motion
Phase Transton n Colletve Moton Hefe Hu May 4, 2008 Abstrat There has been a hgh nterest n studyng the olletve behavor of organsms n reent years. When the densty of lvng systems s nreased, a phase transton
More informationExperimental. Nonlinear Feedback and Feedforward Control Schemes for Manipulators
~ Pradeep K. Khosla* Expermental Takeo Kanade** Department of Eletral and omputer Engneerng Lvaluaton 0 The Robots nsttute arnege Mellon Unversty Pttsburgh, Pennsylvana 52 3 Nonlnear Feedbak and Feedforward
More informationA Simple Inventory System
A Smple Inventory System Lawrence M. Leems and Stephen K. Park, Dscrete-Event Smulaton: A Frst Course, Prentce Hall, 2006 Hu Chen Computer Scence Vrgna State Unversty Petersburg, Vrgna February 8, 2017
More informationMachine Learning: and 15781, 2003 Assignment 4
ahne Learnng: 070 and 578, 003 Assgnment 4. VC Dmenson 30 onts Consder the spae of nstane X orrespondng to all ponts n the D x, plane. Gve the VC dmenson of the followng hpothess spaes. No explanaton requred.
More informationA particle in a state of uniform motion remain in that state of motion unless acted upon by external force.
The fundamental prncples of classcal mechancs were lad down by Galleo and Newton n the 16th and 17th centures. In 1686, Newton wrote the Prncpa where he gave us three laws of moton, one law of gravty,
More informationCOEFFICIENT DIAGRAM: A NOVEL TOOL IN POLYNOMIAL CONTROLLER DESIGN
Int. J. Chem. Sc.: (4), 04, 645654 ISSN 097768X www.sadgurupublcatons.com COEFFICIENT DIAGRAM: A NOVEL TOOL IN POLYNOMIAL CONTROLLER DESIGN R. GOVINDARASU a, R. PARTHIBAN a and P. K. BHABA b* a Department
More informationDr. M. Perumal Professor & Head Department of Hydrology Indian Institute of Technology Roorkee INDIA Co-authors: Dr. B. Sahoo & Dr. C.M.
Dr.. Perumal Professor & Head Department of Hdrolog Indan Insttute of Tehnolog Roorkee INDIA o-authors: Dr. B. Sahoo & Dr... Rao Dr. Dr... Perumal, Professor & & Head, Dept. Dept. of of Hdrolog, I.I.T.
More informationD DAVID PUBLISHING. 1. Introduction. Md. Rifat Hazari 1, Effat Jahan 1, Mohammad Abdul Mannan 2 and Junji Tamura 1
Journal of Mehans Engneerng and Automaton 7 (207) 50-57 do: 0.7265/259-5275/207.0.007 D DAVID PUBISHING Comparatve Analyss between Conventonal PI, Fuzzy og and Artfal Neural Network Based Speed Controllers
More informationWeek 11: Chapter 11. The Vector Product. The Vector Product Defined. The Vector Product and Torque. More About the Vector Product
The Vector Product Week 11: Chapter 11 Angular Momentum There are nstances where the product of two vectors s another vector Earler we saw where the product of two vectors was a scalar Ths was called the
More informationELEKTRYKA 2016 Zeszyt 3-4 ( )
ELEKTRYKA 206 Zeszyt 3-4 (239-240) Rok LXII Waldemar BAUER, Jerzy BARANOWSKI, Tomasz DZIWIŃSKI, Paweł PIĄTEK, Marta ZAGÓROWSKA AGH Unversty of Sene and Tehnology, Kraków OUSTALOUP PARALLEL APPROXIMATION
More informationDesign and Optimization of Fuzzy Controller for Inverse Pendulum System Using Genetic Algorithm
Desgn and Optmzaton of Fuzzy Controller for Inverse Pendulum System Usng Genetc Algorthm H. Mehraban A. Ashoor Unversty of Tehran Unversty of Tehran h.mehraban@ece.ut.ac.r a.ashoor@ece.ut.ac.r Abstract:
More informationNeuro-Adaptive Design II:
Lecture 37 Neuro-Adaptve Desgn II: A Robustfyng Tool for Any Desgn Dr. Radhakant Padh Asst. Professor Dept. of Aerospace Engneerng Indan Insttute of Scence - Bangalore Motvaton Perfect system modelng s
More informationPhysics 5153 Classical Mechanics. Principle of Virtual Work-1
P. Guterrez 1 Introducton Physcs 5153 Classcal Mechancs Prncple of Vrtual Work The frst varatonal prncple we encounter n mechancs s the prncple of vrtual work. It establshes the equlbrum condton of a mechancal
More informationAn Algorithm to Solve the Inverse Kinematics Problem of a Robotic Manipulator Based on Rotation Vectors
An Algorthm to Solve the Inverse Knematcs Problem of a Robotc Manpulator Based on Rotaton Vectors Mohamad Z. Al-az*, Mazn Z. Othman**, and Baker B. Al-Bahr* *AL-Nahran Unversty, Computer Eng. Dep., Baghdad,
More informationTheoretical Aspects of Active Skew Control
Theoretal Aspets of Atve Skew ontrol A. El Azzouz, R. van der ekken,. hner Semens Nederland NV. Industral Installatons and Power Generaton Department Harbour Transhpment Systems Prnses Beatrlaan 6, NL-595
More informationSome Results on the Counterfeit Coins Problem. Li An-Ping. Beijing , P.R.China Abstract
Some Results on the Counterfet Cons Problem L An-Png Bejng 100085, P.R.Chna apl0001@sna.om Abstrat We wll present some results on the ounterfet ons problem n the ase of mult-sets. Keywords: ombnatoral
More informationThe Synchronous 8th-Order Differential Attack on 12 Rounds of the Block Cipher HyRAL
The Synchronous 8th-Order Dfferental Attack on 12 Rounds of the Block Cpher HyRAL Yasutaka Igarash, Sej Fukushma, and Tomohro Hachno Kagoshma Unversty, Kagoshma, Japan Emal: {garash, fukushma, hachno}@eee.kagoshma-u.ac.jp
More informationConservation of Angular Momentum = "Spin"
Page 1 of 6 Conservaton of Angular Momentum = "Spn" We can assgn a drecton to the angular velocty: drecton of = drecton of axs + rght hand rule (wth rght hand, curl fngers n drecton of rotaton, thumb ponts
More information(2016) 57 (8) ISSN
Vetrsano, Massmo and Vasle, Massmlano (2016) Autonomous navgaton of a spaeraft formaton n the proxmty of an asterod. Advanes n Spae Researh, 57 (8). pp. 1783-1804. ISSN 0273-1177, http://dx.do.org/10.1016/j.asr.2015.07.024
More informationJournal of Engineering and Applied Sciences. Ultraspherical Integration Method for Solving Beam Bending Boundary Value Problem
Journal of Engneerng and Appled Senes Volue: Edton: Year: 4 Pages: 7 4 Ultraspheral Integraton Method for Solvng Bea Bendng Boundary Value Proble M El-Kady Matheats Departent Faulty of Sene Helwan UnverstyEgypt
More informationActive Control of Adaptive Optics System in a Large Segmented Mirror Telescope. M. Nagashima and B. N. Agrawal
Atve Control of Adaptve Opts System n a Large Segmented Mrror elesope M. Nagashma and B. N. Agrawal Abstrat For a large Adaptve Opts () system suh as a large Segmented Mrror elesope (SM), t s often dffult,
More informationQueueing Networks II Network Performance
Queueng Networks II Network Performance Davd Tpper Assocate Professor Graduate Telecommuncatons and Networkng Program Unversty of Pttsburgh Sldes 6 Networks of Queues Many communcaton systems must be modeled
More informationMagnitude Approximation of IIR Digital Filter using Greedy Search Method
Ranjt Kaur, Damanpreet Sngh Magntude Approxmaton of IIR Dgtal Flter usng Greedy Searh Method RANJIT KAUR, DAMANPREET SINGH Department of Eletrons & Communaton, Department of Computer Sene & Engnnerng Punjab
More informationCHAPTER 5 NUMERICAL EVALUATION OF DYNAMIC RESPONSE
CHAPTER 5 NUMERICAL EVALUATION OF DYNAMIC RESPONSE Analytcal soluton s usually not possble when exctaton vares arbtrarly wth tme or f the system s nonlnear. Such problems can be solved by numercal tmesteppng
More informationIrregular vibrations in multi-mass discrete-continuous systems torsionally deformed
(2) 4 48 Irregular vbratons n mult-mass dscrete-contnuous systems torsonally deformed Abstract In the paper rregular vbratons of dscrete-contnuous systems consstng of an arbtrary number rgd bodes connected
More informationModeling of Dynamic Systems
Modelng of Dynamc Systems Ref: Control System Engneerng Norman Nse : Chapters & 3 Chapter objectves : Revew the Laplace transform Learn how to fnd a mathematcal model, called a transfer functon Learn how
More informationPHYS 705: Classical Mechanics. Newtonian Mechanics
1 PHYS 705: Classcal Mechancs Newtonan Mechancs Quck Revew of Newtonan Mechancs Basc Descrpton: -An dealzed pont partcle or a system of pont partcles n an nertal reference frame [Rgd bodes (ch. 5 later)]
More informationPrediction of Solid Paraffin Precipitation Using Solid Phase Equation of State
Predton of old Paraffn Preptaton Usng old Phase Equaton of tate Proeedngs of European Congress of Chemal Engneerng (ECCE-6) Copenhagen, 16- eptember 7 Predton of old Paraffn Preptaton Usng old Phase Equaton
More informationNotes on Analytical Dynamics
Notes on Analytcal Dynamcs Jan Peters & Mchael Mstry October 7, 004 Newtonan Mechancs Basc Asssumptons and Newtons Laws Lonely pontmasses wth postve mass Newtons st: Constant velocty v n an nertal frame
More informationA Developed Method of Tuning PID Controllers with Fuzzy Rules for Integrating Processes
A Develope Metho of Tunng PID Controllers wth Fuzzy Rules for Integratng Proesses Janmng Zhang, Nng Wang an Shuqng Wang Abstrat The proportonal ntegral ervatve (PID) ontrollers are wely apple n nustral
More informationELG4179: Wireless Communication Fundamentals S.Loyka. Frequency-Selective and Time-Varying Channels
Frequeny-Seletve and Tme-Varyng Channels Ampltude flutuatons are not the only effet. Wreless hannel an be frequeny seletve (.e. not flat) and tmevaryng. Frequeny flat/frequeny-seletve hannels Frequeny
More informationMr.Said Anwar Shah, Dr. Noor Badshah,
Internatonal Journal of Sentf & Engneerng Researh Volume 5 Issue 5 Ma-04 56 ISS 9-558 Level Set Method for Image Segmentaton and B Feld Estmaton usng Coeffent of Varaton wth Loal Statstal Informaton Mr.Sad
More informationA Tale of Friction Basic Rollercoaster Physics. Fahrenheit Rollercoaster, Hershey, PA max height = 121 ft max speed = 58 mph
A Tale o Frcton Basc Rollercoaster Physcs Fahrenhet Rollercoaster, Hershey, PA max heght = 11 t max speed = 58 mph PLAY PLAY PLAY PLAY Rotatonal Movement Knematcs Smlar to how lnear velocty s dened, angular
More informationNote 10. Modeling and Simulation of Dynamic Systems
Lecture Notes of ME 475: Introducton to Mechatroncs Note 0 Modelng and Smulaton of Dynamc Systems Department of Mechancal Engneerng, Unversty Of Saskatchewan, 57 Campus Drve, Saskatoon, SK S7N 5A9, Canada
More informationof concretee Schlaich
Seoul Nat l Unersty Conrete Plastty Hong Sung Gul Chapter 1 Theory of Plastty 1-1 Hstory of truss model Rtter & Morsh s 45 degree truss model Franz Leonhardt - Use of truss model for detalng of renforement.
More informationParameter Estimation for Dynamic System using Unscented Kalman filter
Parameter Estmaton for Dynamc System usng Unscented Kalman flter Jhoon Seung 1,a, Amr Atya F. 2,b, Alexander G.Parlos 3,c, and Klto Chong 1,4,d* 1 Dvson of Electroncs Engneerng, Chonbuk Natonal Unversty,
More informationThe Study of Teaching-learning-based Optimization Algorithm
Advanced Scence and Technology Letters Vol. (AST 06), pp.05- http://dx.do.org/0.57/astl.06. The Study of Teachng-learnng-based Optmzaton Algorthm u Sun, Yan fu, Lele Kong, Haolang Q,, Helongang Insttute
More informationClustering. CS4780/5780 Machine Learning Fall Thorsten Joachims Cornell University
Clusterng CS4780/5780 Mahne Learnng Fall 2012 Thorsten Joahms Cornell Unversty Readng: Mannng/Raghavan/Shuetze, Chapters 16 (not 16.3) and 17 (http://nlp.stanford.edu/ir-book/) Outlne Supervsed vs. Unsupervsed
More informationSpin-rotation coupling of the angularly accelerated rigid body
Spn-rotaton couplng of the angularly accelerated rgd body Loua Hassan Elzen Basher Khartoum, Sudan. Postal code:11123 E-mal: louaelzen@gmal.com November 1, 2017 All Rghts Reserved. Abstract Ths paper s
More informationInstance-Based Learning and Clustering
Instane-Based Learnng and Clusterng R&N 04, a bt of 03 Dfferent knds of Indutve Learnng Supervsed learnng Bas dea: Learn an approxmaton for a funton y=f(x based on labelled examples { (x,y, (x,y,, (x n,y
More informationThe classical spin-rotation coupling
LOUAI H. ELZEIN 2018 All Rghts Reserved The classcal spn-rotaton couplng Loua Hassan Elzen Basher Khartoum, Sudan. Postal code:11123 louaelzen@gmal.com Abstract Ths paper s prepared to show that a rgd
More informationReport on Image warping
Report on Image warpng Xuan Ne, Dec. 20, 2004 Ths document summarzed the algorthms of our mage warpng soluton for further study, and there s a detaled descrpton about the mplementaton of these algorthms.
More informationPhysics 141. Lecture 14. Frank L. H. Wolfs Department of Physics and Astronomy, University of Rochester, Lecture 14, Page 1
Physcs 141. Lecture 14. Frank L. H. Wolfs Department of Physcs and Astronomy, Unversty of Rochester, Lecture 14, Page 1 Physcs 141. Lecture 14. Course Informaton: Lab report # 3. Exam # 2. Mult-Partcle
More informationChaos-Based Physical Layer Design for WSN Applications
Reent Advanes n Teleommunatons Crut Desgn Chaos-Based Physal Layer Desgn for WS Applatons STVA BRBR Department of letral Computer ngneerng The Unversty of Aukl Aukl, ew Zeal s.berber@aukl.a.nz SHU FG Department
More informationThe Similar Structure Method for Solving Boundary Value Problems of a Three Region Composite Bessel Equation
The Smlar Struture Method for Solvng Boundary Value Problems of a Three Regon Composte Bessel Equaton Mngmng Kong,Xaou Dong Center for Rado Admnstraton & Tehnology Development, Xhua Unversty, Chengdu 69,
More informationElectrical Circuits 2.1 INTRODUCTION CHAPTER
CHAPTE Electrcal Crcuts. INTODUCTION In ths chapter, we brefly revew the three types of basc passve electrcal elements: resstor, nductor and capactor. esstance Elements: Ohm s Law: The voltage drop across
More information3D Numerical Analysis for Impedance Calculation and High Performance Consideration of Linear Induction Motor for Rail-guided Transportation
ADVANCED ELECTROMAGNETICS SYMPOSIUM, AES 13, 19 MARCH 13, SHARJAH UNITED ARAB EMIRATES 3D Numeral Analss for Impedane Calulaton and Hgh Performane Consderaton of Lnear Induton Motor for Ral-guded Transportaton
More information6.3.7 Example with Runga Kutta 4 th order method
6.3.7 Example wth Runga Kutta 4 th order method Agan, as an example, 3 machne, 9 bus system shown n Fg. 6.4 s agan consdered. Intally, the dampng of the generators are neglected (.e. d = 0 for = 1, 2,
More informationPhysics 111: Mechanics Lecture 11
Physcs 111: Mechancs Lecture 11 Bn Chen NJIT Physcs Department Textbook Chapter 10: Dynamcs of Rotatonal Moton q 10.1 Torque q 10. Torque and Angular Acceleraton for a Rgd Body q 10.3 Rgd-Body Rotaton
More informationDepartment of Statistics University of Toronto STA305H1S / 1004 HS Design and Analysis of Experiments Term Test - Winter Solution
Department of Statstcs Unversty of Toronto STA35HS / HS Desgn and Analyss of Experments Term Test - Wnter - Soluton February, Last Name: Frst Name: Student Number: Instructons: Tme: hours. Ads: a non-programmable
More informationLie Group Formulation of Articulated Rigid Body Dynamics
Le Group Formulaton of Artculated Rgd Body Dynamcs Junggon Km 11/9/2012, Ver 1.01 Abstract It has been usual n most old-style text books for dynamcs to treat the formulas descrbng lnearor translatonal
More informationECE559VV Project Report
ECE559VV Project Report (Supplementary Notes Loc Xuan Bu I. MAX SUM-RATE SCHEDULING: THE UPLINK CASE We have seen (n the presentaton that, for downlnk (broadcast channels, the strategy maxmzng the sum-rate
More informationNON-LINEAR CONVOLUTION: A NEW APPROACH FOR THE AURALIZATION OF DISTORTING SYSTEMS
NON-LINEAR CONVOLUTION: A NEW APPROAC FOR TE AURALIZATION OF DISTORTING SYSTEMS Angelo Farna, Alberto Belln and Enrco Armellon Industral Engneerng Dept., Unversty of Parma, Va delle Scenze 8/A Parma, 00
More informationMoments of Inertia. and reminds us of the analogous equation for linear momentum p= mv, which is of the form. The kinetic energy of the body is.
Moments of Inerta Suppose a body s movng on a crcular path wth constant speed Let s consder two quanttes: the body s angular momentum L about the center of the crcle, and ts knetc energy T How are these
More informationOutline. Clustering: Similarity-Based Clustering. Supervised Learning vs. Unsupervised Learning. Clustering. Applications of Clustering
Clusterng: Smlarty-Based Clusterng CS4780/5780 Mahne Learnng Fall 2013 Thorsten Joahms Cornell Unversty Supervsed vs. Unsupervsed Learnng Herarhal Clusterng Herarhal Agglomeratve Clusterng (HAC) Non-Herarhal
More informationMEEM 3700 Mechanical Vibrations
MEEM 700 Mechancal Vbratons Mohan D. Rao Chuck Van Karsen Mechancal Engneerng-Engneerng Mechancs Mchgan echnologcal Unversty Copyrght 00 Lecture & MEEM 700 Multple Degree of Freedom Systems (ext: S.S.
More informationMMA and GCMMA two methods for nonlinear optimization
MMA and GCMMA two methods for nonlnear optmzaton Krster Svanberg Optmzaton and Systems Theory, KTH, Stockholm, Sweden. krlle@math.kth.se Ths note descrbes the algorthms used n the author s 2007 mplementatons
More informationNUMERICAL DIFFERENTIATION
NUMERICAL DIFFERENTIATION 1 Introducton Dfferentaton s a method to compute the rate at whch a dependent output y changes wth respect to the change n the ndependent nput x. Ths rate of change s called the
More informationSupporting Information
Supportng Informaton The neural network f n Eq. 1 s gven by: f x l = ReLU W atom x l + b atom, 2 where ReLU s the element-wse rectfed lnear unt, 21.e., ReLUx = max0, x, W atom R d d s the weght matrx to
More informationA SIMULATION TOOL FOR INTRODUCING ALGEBRAIC CELP (ACELP) CODING CONCEPTS IN A DSP COURSE
A SIMULATION TOOL FOR INTRODUCING ALGEBRAIC CELP (ACELP) CODING CONCEPTS IN A DSP COURSE Venkatraman Att and Andreas Spanas Department of Eletral Engneerng, MIDL TRC Arzona State Unversty, Tempe, AZ, 85287-7206,
More informationA Theorem of Mass Being Derived From Electrical Standing Waves (As Applied to Jean Louis Naudin's Test)
A Theorem of Mass Beng Derved From Eletral Standng Waves (As Appled to Jean Lous Naudn's Test) - by - Jerry E Bayles Aprl 4, 000 Ths paper formalzes a onept presented n my book, "Eletrogravtaton As A Unfed
More information