Determining robot s maximum dynamic load carrying capacity in point-to-point motion by applying limitation of joints torque

Similar documents
Introduction. Voice Coil Motors. Introduction - Voice Coil Velocimeter Electromechanical Systems. F = Bli

II The Z Transform. Topics to be covered. 1. Introduction. 2. The Z transform. 3. Z transforms of elementary functions

Supporting information How to concatenate the local attractors of subnetworks in the HPFP

Numbers Related to Bernoulli-Goss Numbers

e t dt e t dt = lim e t dt T (1 e T ) = 1

1.B Appendix to Chapter 1

P-Convexity Property in Musielak-Orlicz Function Space of Bohner Type

Background and Motivation: Importance of Pressure Measurements

Review: Transformations. Transformations - Viewing. Transformations - Modeling. world CAMERA OBJECT WORLD CSE 681 CSE 681 CSE 681 CSE 681

Physics 201 Lecture 2

Forms of Energy. Mass = Energy. Page 1. SPH4U: Introduction to Work. Work & Energy. Particle Physics:

PHYS 1443 Section 001 Lecture #4

An object moving with speed v around a point at distance r, has an angular velocity. m/s m

Response of MDOF systems

OP = OO' + Ut + Vn + Wb. Material We Will Cover Today. Computer Vision Lecture 3. Multi-view Geometry I. Amnon Shashua

How to Prove the Riemann Hypothesis Author: Fayez Fok Al Adeh.

4.8 Improper Integrals

ANOTHER CATEGORY OF THE STOCHASTIC DEPENDENCE FOR ECONOMETRIC MODELING OF TIME SERIES DATA

How to prove the Riemann Hypothesis

Advanced Machine Learning

( ) ( ) ( ) 0. Conservation of Energy & Poynting Theorem. From Maxwell s equations we have. M t. From above it can be shown (HW)

A L A BA M A L A W R E V IE W

Wave Phenomena Physics 15c

Chapter 2 Linear Mo on

The Mathematics of Harmonic Oscillators

PHY2053 Summer C 2013 Exam 1 Solutions

September 20 Homework Solutions

P441 Analytical Mechanics - I. Coupled Oscillators. c Alex R. Dzierba

The Characterization of Jones Polynomial. for Some Knots

Physics 2A HW #3 Solutions

Investigation of the Evolution Equations of the. Three-Body Problem with Variable Masses

Rotations.

Chapters 2 Kinematics. Position, Distance, Displacement

Physics 15 Second Hour Exam

Variants of Pegasos. December 11, 2009

Exponents and Powers

Calculus 241, section 12.2 Limits/Continuity & 12.3 Derivatives/Integrals notes by Tim Pilachowski r r r =, with a domain of real ( )

Fast Algorithm for Robust Template Matching with M-estimators

THE EXISTENCE OF SOLUTIONS FOR A CLASS OF IMPULSIVE FRACTIONAL Q-DIFFERENCE EQUATIONS

Physics 3 (PHYF144) Chap 3: The Kinetic Theory of Gases - 1

A Cell Decomposition Approach to Online Evasive Path Planning and the Video Game Ms. Pac-Man

Appendix. In the absence of default risk, the benefit of the tax shield due to debt financing by the firm is 1 C E C

6. Gas dynamics. Ideal gases Speed of infinitesimal disturbances in still gas

Interval Estimation. Consider a random variable X with a mean of X. Let X be distributed as X X

T h e C S E T I P r o j e c t

P a g e 5 1 of R e p o r t P B 4 / 0 9

Contraction Mapping Principle Approach to Differential Equations

( ) () we define the interaction representation by the unitary transformation () = ()

NUMERICAL SOLUTION OF THIN FILM EQUATION IN A CLASS OF DISCONTINUOUS FUNCTIONS

Chapter Newton-Raphson Method of Solving a Nonlinear Equation

Physics 120 Spring 2007 Exam #1 April 20, Name

DEEP UNFOLDING FOR MULTICHANNEL SOURCE SEPARATION SUPPLEMENTARY MATERIAL

1. Consider an economy of identical individuals with preferences given by the utility function

Chapter Lagrangian Interpolation

FI 3103 Quantum Physics

Chapter 10. Simple Harmonic Motion and Elasticity. Goals for Chapter 10

Stat 6863-Handout 5 Fundamentals of Interest July 2010, Maurice A. Geraghty

1. Consider a PSA initially at rest in the beginning of the left-hand end of a long ISS corridor. Assume xo = 0 on the left end of the ISS corridor.

Chapter 2. Motion along a straight line. 9/9/2015 Physics 218

From the Hamilton s Variational Principle to the Hamilton Jacobi Equation

Advanced time-series analysis (University of Lund, Economic History Department)

UNIVERSAL BOUNDS FOR EIGENVALUES OF FOURTH-ORDER WEIGHTED POLYNOMIAL OPERATOR ON DOMAINS IN COMPLEX PROJECTIVE SPACES

CH.3. COMPATIBILITY EQUATIONS. Continuum Mechanics Course (MMC) - ETSECCPB - UPC

Including the ordinary differential of distance with time as velocity makes a system of ordinary differential equations.

Week 8 Lecture 3: Problems 49, 50 Fourier analysis Courseware pp (don t look at French very confusing look in the Courseware instead)

3 Motion with constant acceleration: Linear and projectile motion

2D Motion WS. A horizontally launched projectile s initial vertical velocity is zero. Solve the following problems with this information.

f t f a f x dx By Lin McMullin f x dx= f b f a. 2

Suyash Narayan Mishra, Piyush Kumar Tripathi & Alok Agrawal

Use 10 m/s 2 for the acceleration due to gravity.

Relative controllability of nonlinear systems with delays in control

An Ising model on 2-D image

Water Hammer in Pipes

Reinforcement Learning

Motion. Part 2: Constant Acceleration. Acceleration. October Lab Physics. Ms. Levine 1. Acceleration. Acceleration. Units for Acceleration.

Jordan Journal of Physics

Average & instantaneous velocity and acceleration Motion with constant acceleration

PHYS 601 HW3 Solution

Modeling and Predicting Sequences: HMM and (may be) CRF. Amr Ahmed Feb 25

Normal Random Variable and its discriminant functions

Some Inequalities variations on a common theme Lecture I, UL 2007

Physics 101 Lecture 4 Motion in 2D and 3D

WebAssign HW Due 11:59PM Tuesday Clicker Information

Chapter Runge-Kutta 2nd Order Method for Ordinary Differential Equations

On Convergence Rate of Concave-Convex Procedure

Chapter 6 Plane Motion of Rigid Bodies

Introduction to Inertial Dynamics

φ p ( B) AR polynomial of B of order p, p Non-seasonal differencing operator = 1 B

SOLUTIONS TO CONCEPTS CHAPTER 6

Introduction. Section 9: HIGHER ORDER TWO DIMENSIONAL SHAPE FUNCTIONS

A NEW INTERPRETATION OF INTERVAL-VALUED FUZZY INTERIOR IDEALS OF ORDERED SEMIGROUPS

SUMMER KNOWHOW STUDY AND LEARNING CENTRE

In the complete model, these slopes are ANALYSIS OF VARIANCE FOR THE COMPLETE TWO-WAY MODEL. (! i+1 -! i ) + [(!") i+1,q - [(!

Macroscopic quantum effects generated by the acoustic wave in a molecular magnet

Chapter 2: Evaluative Feedback

Science & Technologies GENERAL BIRTH-DEATH PROCESS AND SOME OF THEIR EM (EXPETATION- MAXIMATION) ALGORITHM

Parameter Estimation and Hypothesis Testing of Two Negative Binomial Distribution Population with Missing Data

Homework 8: Rigid Body Dynamics Due Friday April 21, 2017

Bag for Sophia by Leonie Bateman and Deirdre Bond-Abel

UNIQUENESS THEOREMS FOR ORDINARY DIFFERENTIAL EQUATIONS WITH HÖLDER CONTINUITY

Transcription:

Globl Journl o Scenc Reserches Avlble onlne gjsr.blue-.org GJSR Journl. Vol.. - June E-ISSN: -7 Deernng robo s u ync lo crryng ccy n on-o-on oon by lyng lon o jons orue H. R. She M. Bhr A. Kl E n A. M. She - Mechnc Engneerng Deren Arkbr nversy o echnology ehrn Irn - Mech. Eng. Arkbr nversy o echnology ehrn Irn - Mech. Eng. Arkbr nversy o echnology ehrn Irn - Deren o Mechncl Engneerng Shh Bhonr nversy o Kern Kern Irn Corresonng Auhor: A. M. She Receve: My Accee: June Publshe: June A B S R A C hs rcle seeks o eerne wo-lnk robo s u ync lo crryng ccy DCC n on-o-on oon by lyng orue ls on s jons. he eho resene here s bse on oen-loo ol conrol n uses nrec roch o erve oly conons. he Ponrygn's nu rncle PMP hs been use o obn he oly conons h les o wo-on bounry vlue roble PBVP. wo ses o erenl euons n one lgebrc euon re obne whch re solve by usng BVPC con n MAAB sowre. In hs er robo s DCC n on-o-on oon hs been eerne n wo wys. In he rs cse no orue l consrn hs been consere n he Hlonn uncon or he jons; whle n he secon cse hs consrn hs been ncorore no he Hlonn uncon n ers n he euons obne by usng PMP whch cuses hs consrn o show u n he se n cose euons. In boh cses sulons hve been erore. he sulon resuls nce h when orue l consrn s consere n he Hlonn uncon he ngulr osons n velocy o robo s jons re he se bu he orue o jons re eren. Keywors: Roboc r; Mu lo crryng ccy; Ou rjecory; orue ls. GJSR Journl All rghs reserve. INRODCION he ync lo crryng ccy o robo s ene s he u lo h roboc syse cn crry rove h he oors' orues o no ecee he suron ls. DCC s one o he crer or selecon o roboc syses. Generlly wo ehos rec n nrec es or solvng he roble o DCC -. Drec eho: hs eho s bse on he screzon o syse s ync vrbles se n conrol vrbles h les o reer ozon roble. hen lner ozon ehos nonlner ozon ehos evoluonry echnues or Sochsc echnues 6 re eloye o obn he ol vlues o he reers. he vrbles y be clsse s se vrbles conrol vrbles or boh 7. he lnerzng roceure n rec eho n s convergence s chllengng ssue eseclly when nonlner ers re lrge n lucung 7 8. In hs wy he obne nswer s n roe soluon whch s recly rele o he orer o olynol uncon. Wng e l. hve solve n ol conrol roble by usng Bslne uncons o clcule he u lo o e nulor. he n e o her reserch s o screzon he jons rjecores by usng Bslne uncons n hen eernng he reers hrough nonlner ozon so s o obn locl nu whch yels he consrns. A shorcong o hs eho s h ls he soluon o -orer olynol 9.

Glob. J. Sc. Res. : - Ierve ner Progrng IP s noher rec eho by whch rjecory ozon roble becoes lner rogrng roble. he rs orulon o hs eho or clculng he u lo crre by sle robo hs been rove by Wng n Rvn. he lnerzon oeron n he IP eho n s convergence owrs he ol h re cul sks eseclly when syse hs lrge egree o reeo or conns lrge n luonry nonlner ers. Korye n Ghrblu use he IP eho o eerne he DCC o roboc r wh elsc lnks n lso wh elsc jons or on-o-on oon n lso or oon long sece rjecory. hey orule he DCC roble s n ozon roble n hen eloye he IP eho rec eho o solve he roble. In her work he bounry conons re hrly sse n here s n los % error n he nl soluon. Inrec eho: hs s noher eho or obnng he ol rjecory o he u ylo. he nrec eho whch s bse on he PMP ws nlly use o solve ol conrol robles. hs eho ws eloye o solve he robles o obnng he nu e o oon long sece rjecores. In hs eho he oly conons re erce s se o erenl euons whch long wh he gven bounry conons or PBVP. hese ses o erenl euons re solve by ens o nuercl echnues such ulle shoong eho or Gren eho GM. By solvng hs roble n ec soluon cn be oun. hrough hs roch he ol rjecores or e n reunn robos cn be clcule by conserng eren objecve uncons such s he zon o he lo crryng nzon o he oveen e n nzon o orue ec. By lyng n nrec eho whch yele PBVP Korye n Nkoobn obne wo-lnk robo s DCC n on-o-on sk 6. In hs rcle rs wo-lnk robo s DCC s eerne by lyng orue consrn on he jons s ws revously obne by Korye n Nkoobn 6. hen by revsng he eho use n Re. 6 n conserng he lcon o ync orue he roble s resolve n hen he obne resuls re core o ech oher. So he res o he er s orgnze s ollows. In Secon he hecl oelng o he roble wll be escrbe. Secon s evoe o erc oly conons n he PBVP. In Secon rs wo-lnk robo s DCC s obne usng he eho le n Re. 6 n hen hs roble s resolve by ssung ync orue o ech jon. An nlly n Secon he conclusons ro he resen work re surze. Proble orulon: he yncl oel o robo s escrbe n he grngn orulon s: D C G where s he orue vecor o he jons D s he ner r C reresens he cenrel n Corols orces n G eresses he eecs o grvy. By usng he se vecor s: In he se sce or E. s eresse s: F where F s ene s: F F F N N D Z Z D [ C G ] hus he ync euons o oon n se-sce re obne. P g e

Glob. J. Sc. Res. : - Eressng he roble o ol conrol Suosng h roer jon orue vlue ess n he sce generl cos uncon s nze s ollows: he gol s o eerne so h he J o e ev h 6 where e ev n re ene s e e v where n 7 8 W W R re he nl n nl es n s he u lo h cn be crre by he roboc syse. W reresens unor n ervble uncon. n Wv re syerc osve se-ene rces. W W n R re syerc osve ene r. n re he esre vlues or he oson n ngulr velocy o jons resecvely. he cos uncon eerne by E. 6 hrough E. 8 s nze whn he enre rjecory o he robo. In E. 6 he rs n secon ers re rele o nzon o errors o robo s oson n velocy he nl on resecvely. E. 8 s rele o nzon o jon s ngulr oson velocy n orue hroughou he enre rjecory o he robo. 9 E. 9 enes he ngulr oson n ngulr velocy o ech jon he nl n nl on. he erssble boun o ech oor cn eress s ollows: In nrec eho by nroucng cose vecor he Hlonn uncon s eresse s: F where bse on he PMP here ess non-zero cose vecor or sece oly conons us be sse. ylo or whch he ollowng Η ψ ψ Η ψ ψ P g e

Glob. J. Sc. Res. : - P g e ψ Η h H h In hese relons he sybol nces he erels o he ses coses n conrols. he obne oly conon s rele o se n whch he se vrbles n he jons orue vlues re no boune. In orer o ly consrn on he conrol vrbles we shoul conser he ollowng: Η ψ Η ψ 6 n ll or 7 In E. 6 s erssble conrol vlue. By ssung o be cose vecor he oly conons re obne s E. 8 o E.. Z N 8 ψ N ψ ψ Z N ψ 9 ψ Z δ δ δ E. 8 n E. 9 eress he reure oly conons. he cheve soluon s cne ol soluon. Snce he uer n lower orue ls hve been ene by E. he orue vlue o ech oor cn be obne ro E.. Z R Z R Z R Z R Whch n hs relon hgh n low ls o orues vlue s eerne s ollows. K K K K

Glob. J. Sc. Res. : - K Whch n E. he reer o s s sn K g s sn n n re ene. Regrng h se vecors re e nl n nl eros hus he E. kes he or o E. n bounry conons re ene s ollows. Here he E. 8 o eress hree cegores o relons. So he E. 8-9 ene syse s ync oel. Ou conons re obne by E. n bounry conons by E.s n. In orer or solvng he wo-on bounry vlue roble erve lgorh s use. By nserng E. n E. 8 9 n o erenl euon s obne. n o bounry conon s obne ro E.. So wo-on bounry vlue roble s consruce. In hs lgorh he obne error vlue ro E. 7 shoul be lower hn vore vlue o. hereore: Where n hs relon s he vore vlue n he nl e n s he clcule se vecor vlue he nl on. he relve sgncnce o oson n velocy error vlue or ech o he jons s eerne usng W v n W rces. he eree vlue o oors ccy - n + s use or eernng orble u lo. So h he lo vlue ecees he u orble lo by he robo he oor o ech jon reures lyng orue greer hn he ere l whch cuses he jons orue o ecee her ls. Sulon In hs r we el wh he sulon o lnr wo-lnk ync r wh he seccons rove n ble. Fg. shows hs robo n he horzonl lne. ble. sulon reers 6 reer vlue engh o lnks M Mss Kg Moen o ner I I.66 Kg. M. no lo see s s.6 R s Acuor sll orue s s N. 6 P g e

Glob. J. Sc. Res. : - Fgure. Schec o robo n ol h 6 s s Regrng he reerence o 6 he nl oson o he en-eecor n he Z ln n he nl oson s.7 s. Moreover he velocy o nl en eecor n he begnnng n en o he rjecory s zero. Jons oson n velocy vlues re obne ro nverse knec soluon s ollows. 6 6 6 Se vrbles o n ro E. re ene s ollows. u u Where n re he rs n secon lnk ngles n show he lnks ngle velocy. u n u show he orue o he rs n secon lnk oors. sng E. 8 our euons rele o ync euons se sce or s erce s ollows. 7 - - - C - G - - C - G - - - C - G - - C - G 8 Where j C G : I j = s rele o wo-lnk robo whch s rove n he en secon. Now by enng enly rces s w w w w r R r W ; W ; 9 An by nserng E. 8 n E. 8 rge uncon: =. ru +r u w +w w w 7 P g e

Glob. J. Sc. Res. : - Fro E. Hlonn uncon s obne s ollows. H Where n ro E. 8 n re nsere. sng E. ervng ro Hlonn uncon he euons rele o us-ses re obne s ollows. H H H H ; ; ; Now usng E. n ervng or Hlonn uncon n rooron o conrol vlues he ollowng wo relons resul. H = ru u H = ru u - r - - r - By solvng hese euons he conrol vlues re obne n he cceble rnge. - - = r - - ; u = r - u hereore ou conrol rule or E. s wren s ollows. u u u u Whch he lons o conrol vlues o ech oor s clcule s ollows. k k k k ; ; k k k k 6 Where he k j j = vlues s clcule ro oor seccons rove n ble. Deernng ou rjecory o u lo or wo-lnk nulor usng hyohess o he rcle 6 In hs r or he gven wo-lnk nulor n bounry conons n reerence 6 u o lo crryng ccy n corresonng ou rjecory re clcule. Vlues o W W n R re selece n hs wy. So h W = W = n R= g - -. For hs nulor he gven bounry conons n nene rge uncon he obne u lo s / kg. In orer o show he lgorh erornce or clculng u lo he resuls o sulon or ve eren lo vlues hve been resene n grs. In Fg. he oson o he en eecor n Z lne or eren lo vlues s shown. Fgs. n b show he jons oson wh resec o e. Also Fgs. n b vrons o ngulr velocy wh resec o e wh lo crryng vrons re shown. 8 P g e

Glob. J. Sc. Res. : - Y. = Kg = Kg = Kg =. Kg =. Kg....6.8 Fgure. En eecor rjecory n Y ln =kg - =kg. =kg =kg -. =kg =kg r =.kg =.kg r - =.kg =.kg. -....6.8 -...6.8 sec sec Fgure. ngulr oson o jon Fgure b. ngulr oson o jon 6 o r/sec - =kg =kg =kg =.kg =.kg -...6.8 -...6.8 sec sec Fgure. Angulr veloces o jons Fgure b. Angulr veloces o jons o r/sec - =kg =kg =kg =.kg =.kg In Fgs. n b he gr o he rs n secon jon orues n rooron o e or eren lo vlues hs been shown. As you cn see wh he ncrese o he lo orue vlues ncrese oo n rogress owr orue ls unl hey rech o her vlues. As cn be seen he orues hve reche suron or / kg lo n lwys re on hgh n low ls. In hs suon he lo ecees / kg necesses he orues o ecee her ls whch s no ossble n when he conon s no ullle n he roble soluon o bounry vlue hs c s subsne. he obne =. kg s he u lo crryng ccy or he nene rge uncon. he obne resul s ully conssen wh reerence 6. 9 P g e

Glob. J. Sc. Res. : - =.kg =kg N. - =kg =kg =kg =.kg N. - =.kg =kg =kg =.kg -...6.8 -...6.8 sec sec Fgure. orues o jon Fgure b. orues o jon Deernng he ou rjecory o wo-lnk nulor by lyng ync orue ssuon In Sec. he u lo n he corresonng ou rjecory were obne. In Re. 6 orue s hgh n low ls bse on uncon o robo s jons velocy E. 6 s consere. Regrng h orue s velocy vres by jons velocy n Hlonn uncon s no erve n rooron o jons velocy. Here he oreenone roble s consere by lyng jons orue ls ynclly. sng E. 6 we rrve he ollowng relon. k k k k k k k k 7 Fro he bove wo neules he ollowng our neules re obne. k k k k k k k k 8 9 hus wo new se vrbles re ene s ollows 7. 6 Where H sgnes Hevse uncon. So Hlonn uncon s obne s ollows. H 66 P g e

Glob. J. Sc. Res. : - Now usng ervon ro Hlonn uncon n rooron o se n us-se vrbles wo ses o erenl euons re obne s ollows 7. 6 - C - - G - - - C - G - - C - - G - C - G - An us-se euons by ervng ro Hlonn uncon n rooron o se vrbles s obne s ollows. H H H ; H 6 6 H ; ; H In E. he ls wo senences eue zero. hus n 6 vlues wll be e. By ervng ro Hlonn uncon n rooron o conrol orue o E. s obne s ollows. H u H u In orer o eror he corson beween he resene eho n Re. 6 n he eho oere n hs er sulon s erore or he wo-lnk robo whch lo eul o kg s lce on s en eecor. In wh ollows he resuls o sulon re resene n Fgs. 6 o 7b.. - r. Re [6] -. Re [6] hs work hs work -...6.8...6.8 sec sec Fgure 6. Corson ngulr oson o jon Fgure 6b. Corson ngulr oson o jon r -. - P g e

Glob. J. Sc. Res. : - o r/sec Re [6] hs work Re [6] - hs work -...6.8 -...6.8 sec sec Fgure 7. Corson ngulr velocy o jon Fgure 7b. Corson ngulr velocy o jon o r/sec As s even ro he bove grs he oson n velocy o boh ses re slr n grs re on ech oher. Fgs. 8 n 8b show he orues o rs n secon jon. N. 8 6 9 8 7... Re [6] hs work N. 6 - Re [6] hs work - -...6.8...6.8 sec sec Fgure 8. Corson orue o jon Fgure 8b. Corson orue o jon Frs jon orue vlue Fg. 8 n secon eho s greer hn he rs one. hs s becuse n he rs eho er he orue vlue s obne ro E. usng E.s -6 he orue vlue s le unl reches suron whle n he secon eho hgh n low ls o jons orue hve been e o Hlonn uncon s uneul consrns. In oher wors jons orues cn ncrese uner he nluence o ngulr velocy whle n he eho oere n Re. 6 hs ws no ossble. CONCSIONS In hs rcle u lo crryng ccy o wo-lnk robo hs been obne by oen chne ou conrol eho n eloyng Ponyerygen Mnu Prncle. Regrng oors lons oors orue lon consrn ws le o he roble. he reure conons o oly were obne once by Re. 6 n noher e by ync orue ssuon. In eho Re. 6 hs consrn s no e no Hlonn uncon whle usng new eho whch s eloye n hs rcle hs consrn hs been e no Hlonn uncon s n neuly n hereore s e no se n us-se euons. he obne erenl euons se long wh bounry conons ors wo-on bounry vlue euon se whch ws solve usng BVPC con o MAAB sowre. By erorng he sulon whch ws crre ou bou lnr wo-lnk robo n orer o eerne u lo crryng ccy n on- o- on oon s shown h jons oson n ngulr velocy n boh ses s he se. Aen he oon o nulor s erore n horzonl lne hereore grvy velocy s ken s zero. Iner r o wo- lnk nulor s eresse s ollows. P g e

Glob. J. Sc. Res. : - P g e cos cos D In whch I I c c c c c erl-corols orces o C cener n grvy orce o G re ene s ollows. ; G G G C C C In whch sn sn C cos cos cos g g G hus ync euons o wo- lnk robo n he horzon lne re obne. REFERENCES Bes J. 998. Survey o nuercl ehos or rjecory ozon J. o Gunce Con. Dyn. Vol. No... 9 7. Cheb ehhe HE H M n Hnch S.. Mnu cos rjecory lnnng or nusrl robos Euroen J. o Mechncs A/Sols Vol... 7 7. Dehl M Bock HG De H n Weber PB. 9. Fs Drec Mulle Shoong Algorhs or Ol Robo Conrol Fs oons n Boechncs n Robocs Vol... Jun. H M Cheb Hnch S n ehhe HE. 6. Ol oon lnner o oble nulors n generlze on-oon sk 9h IEEE In. Worksho on Avnce Moon Conrol.. -6. Hull DG. 997. Converson o ol conrol robles no reer ozon robles J. o Gunce Conrol n Dyncs Vol. No... 7-6. Krk DE. 97. Ol conrol heory An Inroucon Prence-Hll Inc. Korye MH. 9. Nkoobn Forulon n Nuercl Soluon o Robo Mnulors n Pon-o-Pon Moon wh Mu o Crryng Ccy rnscon B: Mechncl Engneerng Shr nversy o echnology Vol. 6. P.. - 9. Korye MH n Nkoobn A. 9. Mu ylo h lnnng or reunn nulor usng nrec soluon o ol conrol roble In. J. Av. Mnu. ech. Vol... 7-76. Korye MH n Ghrblu H.. Mu llowble lo o oble nulor or wo gven en ons o en-eecor In. J. o AM Vol. No... 7 7.

Glob. J. Sc. Res. : - Korye MH n Grblu H.. Anlyss o wheele oble leble nulor ync oons wh u lo crryng cces Robocs n Auonoous Syses Vol. 8 No... 6-76. uus R.. Ierve ync rogrng Auoc Vol. 9 No. 7.. -6. Mele A. 97. Recen Avnces n Gren Algorhs or Ol Conrol Probles Journl o Ozon heory n Alcons Vol. 7. 6 Dec. Ponrygn Bolnsk V Gkrelze R n Mchchenko E. 96. Mhecl heory o ol rocesses Iner-scence ublsher. Szyszkowsk W n Foouh R.. Irovng e-ol conrol neuvers o wo-lnk roboc nulors J. o Gunce Conrol n Dyncs Vol. No... 888-889. Wng n Rvn B. 988. Dync lo crryng ccy o echncl nulors-pr J. o Dync Sys. Mes. n Conrol Vol... -6. Wng CYE oszyk WK n Bobrow JE.. Pylo zon or oen chne nulor: Fnng oons or Pu 76 robo IEEE rnscons on Robocs n Auoon Vol. 7 No... 8-. n-sheng GE n -Qun CH. 6. Ol oon lnnng or nonholonoc syses usng genec lgorh wh wvele roon Ale Mhecs n Couon Vol. 8.. 76 8. P g e