Application of Linear Model Predictive Control and Input-Output Linearization to Constrained Control of 3D Cable Robots
|
|
- Jordan Parks
- 5 years ago
- Views:
Transcription
1 Moern Mechancal Engneerng, 2011, 1, o: /mme Publshe Onlne November 2011 ( Applcaton of Lnear Moel Prectve Control an Input-Output Lnearzaton to Constrane Control of 3D Cable Robots Abstract Al Ghasem Member of Young Researchers Club, Scence an Research Branch, Islamc Aza Unversty, ehran, Iran E-mal: Receve September 3, 2011; revse October 13, 2011; accepte October 25, 2011 Cable robots are structurally the same as parallel robots but wth the basc fference that cables can only pull the platform an cannot push t. hs feature makes control of cable robots a lot more challengng compare to parallel robots. hs paper ntrouces a controller for cable robots uner force constrant. he controller s base on nput-output lnearzaton an lnear moel prectve control. Performance of nput-output lnearzng (IOL) controllers suffers ue to constrants on nput an output varables. hs problem s successfully tackle by augmentng IOL controllers wth lnear moel prectve controller (LMPC). he effecttveness of the propose metho s llustrate by numercal smulaton. Keywors: Cable Robots, Input-Output Lnearzaton, Lnear Moel Prectve Control 1. Introucton After a moton smulator wth parallel knematc chans was ntrouce n 1965 by D. Stewart [1], parallel manpulators receve more an more attenton because of ther hgh stffness, hgh spee, hgh accuracy, compact an hgh carryng capablty [2]. hey have been use wely n the fels of moton smulators, force/torque sensors, complance evces, mecal evces an machne tools [3,4]. A parallel robot s mae up of an en-effector, wth n egrees of freeom, an a fxe base lnke together by at least two nepenent knematc chans [5]. Actuaton takes place through m smple actuators. Parallel robots rawbacks are ther relatvely small workspace an knematcs complexty. Cable robots are a class of parallel robots n whch the lnks are replace by cables. hey are relatvely smple n form, wth multple cables attache to a moble platform or an en-effector. Cable robots posses a number of esrable characterstcs, nclung: 1) statonary heavy components an few movng parts, resultng n low nertal propertes an hgh payloa-to-weght ratos; 2) ncomparable moton range, much hgher than that obtane by conventonal seral or parallel robots; 3) cables have neglgble nerta an are sutable for hgh acceleraton applcatons; 4) transportablty an ease of sassembly/- reassembly; 5) reconfgurablty by smply relocatng the motors an upatng the control system accorngly; an, 6) economcal constructon an mantenance ue to few movng parts an relatvely smple components [6,7]. Consequently, cable robots are exceptonally well sute for many applcatons such as hanlng of heavy materals, nspecton an repar n shpyars an arplane hangars, hgh-spee manpulaton, raply eployable rescue robots, cleanup of saster areas, an access to remote locatons an nteracton wth hazarous envronments [6-12]. For these applcatons conventonal seral or parallel robots are mpractcal ue to ther lmte workspace. However, cables have the unque property they cannot prove compresson force on an en-effector. Some research has been prevously conucte to guarantee postve tenson n the cables whle the en-effector s movng. he ea of reunancy was utlze n cable system control [13,14]. hs paper ntrouces a controller for cable robots uner force constrant. By conserng, lnear moel prectve covers fferent constrant such as nput constrants. he goal s to apply the lnear moel prectve control to the nput-output lnearze system to account for the constrants. A varety of nonlnear control esgn strategy has been propose n the past two ecaes. Input-output lnearzaton (IOL) an nonlnear moel base control are the most wely stue esgn technques n nonlnear control. he
2 70 A. GHASEMI central ea of the nput output lnearzaton approach s to algebracally transform the nonlnear system nto lnear one an apply a sutable lnear control esgn technque [15,16]. LMPC s prmarly evelope for process control. herefore ts applcaton n robot control has less been reporte. he ncpent nterest n the applcatons of MPC ates back to the late 1970s. In 1978, Rchalet et al. [17], presente the Moel Prectve Heurstc Control (MPHC) metho n whch an mpulse response moel was use to prect the effect at the output of the future control actons. Lnear moel prectve control refers to a class of control algorthms that compute a manpulate varable profle by utlzng a lnear process moel to optmze a lnear or quaratc open-loop performance objectve subject to lnear constrants over a future tme horzon. he frst move of ths open loop optmal manpulate varable profle s then mplemente. hs proceure s repeate at each control nterval wth the process measurements use to upate the optmzaton problem. Durng 1980s, MPC quckly became popular partcularly n chemcal process nustry ue to the smplcty of the algorthm an to the use of the mpulse or step response moel, whch s preferre, as beng more ntutve an requrng no prevous nformaton for ts entfcaton [18]. A cable-suspene robot s actuate by servo motors that control the tensons n the cables. A major savantage of cable robots s that each cable can only exert tenson. hs constrant leas to performance eteroraton an even nstablty, f not properly accounte for n the control esgn proceure. Due to ths feature, well known results n robotcs for trajectory plannng an control are not rectly applcable to them. Several approaches nclung a lyapunov base controller wth varable gans an a feeback lnearzng controller wth varable gans [19], feeback lnearzaton together wth metho of reference sgnal management [20], lyapunov base slng controller wth metho of sgnal management [21] have been suggeste to satsfy the postve tenson n the cables whle the platform s movng. In ths paper a lnear moel prectve control s apple to lnearze moel. Moel prectve control, a computer control algorthm that utlzes an explct moel to prect the future response of a system s an effectve tool for hanlng constrane control problems. cable connecton n the platform frame. herefore, = a R b c s the vector representng the length of each cable an l s the recton of tenson force along each cable, where c s the poston vector of mass center of platform parameterze. R s the rotaton matrx between the two frames, the base an the movng, Fgure System Dynamcs he nerta of each lnk of cable robots s neglgble compare to that of the platform because the so-calle lnk s just a cable or wre. herefore, the ynamcs of the lnks can be gnore whch wll sgnfcantly smplfy the ynamc moel of the manpulator. One can erve the Newton-Euler equatons of moton of the manpulator wth respect to the center of mass on the platform as follows [10] F mamc f mg ( n s number of cables) M I I n ext 1 ext n 1 Rb f l I I where m an I are the mass an nerta tensor of the platform nclung any attache payloa; g s the gravty acceleraton vector; an f ext an τ ext are external force an moment vectors apple to the platform. c an α are the lnear an angular acceleraton vectors of the platform; an f are the force vector an force value of the th cable. Equaton (1) can be rewrtten nto a compact form as: M x Cx D Ju (2) where mi M,, f D C 033 I 033 I ext mg ext (1) 2. Knematcs Moelng of the Cable Robots he knematc notaton of a spatal cable-rven manpulator s presente n Fgure 1, where P an B are two attachng ponts of the th cable to the platform an the base, respectvely. a represents the poston vector of B n the base frame an b shows the poston vector of the Fgure 1. General knematcs of a cable robot.
3 A. GHASEMI 71 l1 ln J, J jacopan matrx Rb1l1 Rbnln f1 u f n I 3*3 s a 3*3 entty matrx an 0 I I z 0 z I I 0 y I I I x y x Equaton (2) can be wrtten nto a steay state form as: where y I x X F Gu y E X h X x x 06* n X, F, G 1 1 x M Cx D M J wth constrants 0 u u max 4. Input-Output Lnearzaton he ffculty of the trackng control esgn can be reuce f we can fn a rect an smple relaton between the system output y an the control nput u. Inee, ths ea consttutes the ntutve bass for the so-calle nput -output lnearzaton approach to nonlnear control esgn. hs artcle s ame to use the LMPC whch covers fferent constrants such as nput constrants. Because of LMPC s usually use for lnear screte systems. In the begnnng we wll lnearze the ynamcs equatons base on n Input-Output Lnearzaton. o generate a rect relatonshp between the output y an the nput u, Dfferentate the output y wth respect to tme t n Equaton (3), we have y L h X L h u t F gj j j1 where L F h (X) an L gj h (X) are the Le ervatves of h (X) wth respect to F(X) an g j (X), respectvely. If L gj h (X) = 0, y = L F h (X) then the r th ervatve of y can be represent n the followng form. n r r r1 F gj F j j1 In ths way, we can wrte all plant s nput-output equatons as n y L h X L L h u t (3) r1 r r 1 11 r11 y 1 LF h L 1 g L 1 F h1 Lg L h n F 1 u r q r q rq1 rq1 yq LF hq Lg L h 1 F qlg L h n F q where q an r are the number of egree of freeom of the robot an the relatve orer of the plant, respectvely. Equaton (4) can be represente n the followng compact form: v P Wu Now u can be obtane as: u W W W vp where 1 W s the pseuo nverse of W. 1 W W WW For a cable robotc system, t can be easly shown that the system has no zero ynamcs. herefore, the ecouplng matrx W s full rank an the control law s well X efne an a sutable change of coornates X y y y y yq y q where yel s a close- n the normal form [15]. loop system y xr 2 1,,q r1 rq n A Bv y H 5. Lnear Moel Prectve Control he basc structure of MPC to mplement s shown n Fgure 2 A moel s use to prect the future plant outputs, base on past an current values an on propose future control actons. hese actons are calculate by optmzer takng nto account the cost functon as well as constrants. he optmzer s another funamental part of the strategy as t proves the control acton. each component of ths structure s escrbe n more etal In the followng of ths artcle. Fgure 2. Basc structure of MPC. (4)
4 72 A. GHASEMI he goal s to apply the lnear moel prectve control to the nput-output lnearze system to account for the constrants. Snce the lnear moel prectve s more naturally formulate n screte tme, the lnear subsystem n (5) s scretze wth a samplng pero to yel k1 A kb vk (6) yk H k where A,B an H are obtane rectly from the contnuous-tme matrces [22]. Also, the state-epenent relaton between u(k) an v( k) s obtane as r vk L h r F X k LGLFhX k uk hs mappng can be rewrtten n the followng form v k PX k W X k u k 5.1. Constrant Mappng When lnear moel prectve control s apple to the system, t s necessary to map the constrants from the orgnal nput space to lnearze system. By conserng v s a new nput to be etermne, o obtan constrants on the new nput, he nput constrant mappng s performe usng nput output lnearzaton law an the current state measurement x(k). he transforme constrants can be etermne on each samplng pero by solvng the followng optmzaton problem: mn mn k vmn k j k P X k j max ukjk W X k j k u k j k 0 j N 1 uk ( jk ) u u k j j u max vmax k j k P X k j k W X k j k u k j k 0 j N 1 (7) where Z (k + j k) s the precte value of the system state (Z) at tme k + j base on the nformaton avalable at tme k. Note that the varable X (k + j k) cannot be calculate prove that the nput sequence s calculate, whch s not possble untl the constrants are specfe. herefore, at the begnnng (k = 0), the nput constrant over the entre control horzon can be presente by: v k j k v k k mn mn j1,, N1 max v k j k v k k max j1,, N1 hen, we use nputs calculate at last samplng tme to etermne future constrants at the current samplng tme. (8) herefore, Equaton (7) wll be change nto Equaton (9). mn max mn uk ( jk ) 1 max 1 uk ( jk ) max v k j k P X k j k W X k j k1 ] u k j k 0 jn1 v k j k P X k j k W X k j k1 u k j k 0 jn1 umn u k j j u (9) Now Equaton (9) can be solve to obtan v mn (k+ j k) an v max (k + j k). If W(,j) s postve, the control u(j) must be the smallest value for v mn an the largest value for v max an f W(,j) s negatve, then t must be the largest value for v mn an the smallest value for v max Lnear Moel Prectve Control Desgn he goal s to apply LMPC to the lnearze system to account for these constrants. Now the moel (6) s use n the nfnte horzon lnear moel prectve strategy propose by Muske an Rawlngs [23]. herefore, the openloop optmal control problem that the nput control foun by mnmzng the nfnte horzon crteron, can be expresse as V( kk ) j1 k j k H QH k j k mn ( ) ( ) vk j k vk j 1 k R vk j k vk j 1 k v k j k v S v k j k v (10) where ξ an v are target values for ξ an v, respectvely, an Q,S, an R, are postve sem efnte matrces. In orer to obtan value v(k + j k) t s necessary to mnmze the functonal of Equaton (10) to o ths value of the precte output are calculate as functon of pas values of nputs an outputs an future control sgnals obtan an expresson whose mnmzaton leas to the looke for values. he ecson vector s efne as V(k k) = [v(k k) v( k+1 k) v(k+n-1 k)], where N s the control horzon. All future moves beyon the control horzon are set equal to the target value v. As scusse n [23], the matrx A s unstable an n orer for the lnear moel prectve problem to have a feasble soluton t s necessary to mpose the equalty constrant ξ(k + N k) = ξ. o obtan a fnte set of ecson varables, nputs beyon the control horzon are set equal to the esre value: v(k + j k) = v, j N. herefore, the nfnte horzon lnear
5 A. GHASEMI 73 moel prectve problem Equaton (10) can be wrtten as a fnte horzon problem. V( kk ) vk N kv 1 mn 1 N 1 k j k H QH k j k j1 vk j k vk j 1 k 1 S v kn k v v k jk v S v k jk v R v k j k v k j k (11) hs optmzaton problem must be solve subjecte to the followng constrants: k N k (12) v k j k v k j k v k j k mn mn N 1 N 2 EE A B A B B N K N A HQH A 0 he soluton of Equaton (13) belongs to the regular system. o fn the solutons of the trackng one, that of the regular system shoul be shfte nto the orgn of the system to the steay state escrbe by ξ, an v. he esre values must le wthn the feasble regon efne by nput constrants for lnear moel prectve control an mnmze the control effort (Equaton (15)). Straghtforwar algebrac manpulaton of quaratc subject to : objectve functon of the corresponng regular system presente n Equaton (11) results n the followng stan- I A B 0 U ar quaratc program form: H 0 y mn V HHV 2V GG kffvk 1 (13) 0 DD U C Vkk where S B KN 1 A 0 GG, FF B K0 A 0 Equaton (13) shoul be solve subjecte to the followng constrants: DDV CC N (14) EE V A k where by conserng vmax k k I vmax k N 1 k 6* N DD, CC, I 6* N vmn k k vmn kn 1 k 2 mn ( 0 U 0m2m Imm U U U v m m Im m U U Qs 2 m*2m (15) U an Qs are esre value of the nput an a postve efnte matrx, respectvely. herefore control law s the summaton of the answers of Equaton (13) an Equaton (15) whch can be shown n the followng form. ( W X k k v k kp( X k k u k W X k k v k k P X k k (16) Fgure 3 shows schematc of the propose structure control. Fgure 3. Schematc of control structure. N 1 B K N1B R2S B AKN2 B S B A K0 B N 2 B KN 2 AB S B KN 2 B R 2S B A K0 B HH N1 N2 B K0 A B B K0 A B B K0 B R2S
6 74 A. GHASEMI 6. Smulaton In ths secton, smulaton results of applyng moel prectve control on a 3D cable robot wll be presente. able 1. shows the mensons of the cable robot. We conser a efnte movement of the platform from X 0 = [ 0.1, 0.1,1.5,0.002,.001, 0.001] to X = [0.2sn(t), 0.4 sn(t), t t 3,0,0,0], on a esre trajectory shown n otte lnes by Fgures 4(a) to 4(f), for poston/orentaton of the platform. Also, we conser the parameters of the moel precttve controller as: the control horzon N = 25, S, Q, an R of Equaqon (10), R = I, Q = I, S = 0.01I, an Q s of Equaton (15), Q s = I. Snce the controller nees platform s poston/orenttaton, at frst, we must solve forwar knematcs of the robot. hs has been carre out by the authors usng neural network algorthm [24]. Fgure 4 shows the moel prectve controller wth nput-out lnearzng worke qute well an a trajectory trackng are one. Fgure 5 shows the sx tensons n the cables vs. tme. As t can be seen, all of them reman postve urng the moton. able 1. Dmensons of the cable robot. Poston vector X(m) Y(m) Z(m) Poston vector x(m) y(m) z(m) a b a b a b a b a b a b 6 (a) (b) (c) () (e) Fgure 4. Plots of esre an actual poston an orentaton of the platform, (a)-(c) poston n X-Y-Z rectons, respectvely, ()-(f) orentaton aroun X-Y-Z recton, respectvely. (f)
7 A. GHASEMI 75 (a) (b) (c) () (e) (f) Fgure 5. Plots of tenson trajectores. 7. Conclusons In ths paper, a lnear moel prectve controller together wth an nput-output lnearzng control strategy for a constrane robotc system, a 3D cable robot, was evelope an evaluate. he control system s comprse of: 1) an nput-output lnearzng controller that accounts for cable robot nonlneartes; 2) a constrant mappng scheme that transforms the actual nput constrants nto nput constrants on the feeback lnearze system; an 3) a lnear moel prectve controller that proves explct compensaton for nput constrants. he smulaton re- of the propose metho. It sults showe the effectveness s worth nothng that ths approach can be extene for the reunant cable robots. 8. References [1] D. Stewart, A Platform wth Sx Degrees of Freeom, Proceengs of the Insttuton of Mechancal Engneer, Vol. 180, No. 15, 1965, pp o: /pime_proc_1965_180_029_02 [2] J. -P. Merlet, Parallel Robots, Sol Mechancs an Its Applcatons, Kluwer, Norwell, [3] J. -P. Merlet, Stll a Long Way to Go on the Roa for Parallel Mechansms, A Keynote Speech at Desgn Engneerng echncal Conferences, Montreal, 29 September-2 October [4] J. -P. Merlet, Parallel Robots, Open Problems, INRIA Sopha-Antpols, France. [5] L. -W. sa, Robot Analyss, he Mechancs of Seral an Parallel Manpulators, Wley, New York, [6] P. Bosscher, A.. Rechel an I. Ebert-Uphoff, Wrench- Feasble Workspace Generaton for Cablerven Robots, Journal of Intellgent an Robotc Systems, Vol. 22, No. 4, 2006, pp [7] A.. Rechel an I. Ebert-Uphoff, Force-Feasble Workspace Analyss for Unerconstrane Pontmass Cable Robots, Proceengs of IEEE Internatonal Conference on Robotcs an Automaton, New Orleans, 26 Aprl-1 May 2004, pp [8] S. Kawamura, W. Choe, S. anaka an S. R. Panan, Development of an Ultrahgh Spee FALCON Usng Wre Drve System, In Proceengs of the 1995 IEEE Internatonal Conference on Robotcs an Automaton, May 2003, pp [9] P. Lafourcae, M. Llbre an C. Reboulet, Desgn of a Par-
8 76 A. GHASEMI [10] X. Dao, O. Ma an R. Paz, Stuy of 6-DOF Cable Robots for Potental Applcaton of HIL Mcrogravty Con- tact-dynamcs Smulaton, In Proceengs of the AIAA Moelng an Smulaton echnologes Conference an Exhbt, Keystone, August 2006, pp [11] P. Gallna, G. Rosat an A. Ross, 3-D.O.F. Wre Drven Planar Haptc Interface, Journal of Intellgent an Robotc Systems,Vol. 32, No. 1, 2001, pp o: /a: [12] J. Albus, R. Bostelman an N. Dagalaks, he NIS Robocrane, Journal of Robotc Systems, Vol. 10, No. 5, 1993, pp o: /rob [13] Y. Q. Zheng, Workspace Analyss of a Sx DOF Wre- Drven Parallel Manpulator, Proceengs of the WORK- SHOP on Funamental Issues an Future Research Derecton for Parallel Mechansms an Manpulators, Quebec, 3-4 October 2002, pp [14] W. J. Shang, D. Cannon an J. Gorman, Dynamc Analyss of the Cable Array Robotc Crane, Proceengs of the IEEE Internatonal Conference on Robotcs an Automaton, Detrot, May 1999, pp [15] J. J. Slotne an W. Lepng, Apple Nonlnear Control, Prentce Hall, Englewoo Clffs, [16] H. Khall, Nonlnear Systems, 3r Eton, Prentce-Hall, Upper Sale Rver, [17] J. Rchalet, A. Raault, J. L. estu an J. Papon, Moel allel Wre-Drven Manpulator for Wn unnels, In Proceengs of the Workshop on Funa mental Issues an Future Research Drectons for Parallel Mechansms an Manpulators, Quebec, 3-4 October 2002, pp Prectve Heurstc Control: A pplcaton to Inustry Processes, Automatca, Vol. 14. No. 2, 1978, pp o: / (78) [18] C. E. Garca, D. M. Prett an Morar, Moel Prectve Control: heory an Practce a Survey, Automatca, Vol. 25, No , pp o: / (89) [19] A. B. Alp an A. K. Agrawal, Cable Suspene Robots: Desgn, Plannng an Control, Internatonal Conference on Robotcs Robotcs & Automaton, Washngton, DC, 9-13 May 2002, pp [20] S. R. Oh an A. K. Agrawal, Controller Desgn for a Non-reunant Cable Robot Uner Input Constrant, ASME Internatonal Mechancal Engneerng Congress & Exposton, November 2003, Washngton, DC. [21] S. R. Oh an A. K. Agrawal, A Control Lyapunov Approach for Feeback Control of Cable-Suspene Robots, IEEE Internatonal Conference on Robotcs an Automaton, Aprl 2007, pp [22] F. Frankln, J. Powell an L. Workman Dgtal Control of Dynamc Systems 2n Eton, Ason Wesley, Boston, 1994, pp [23] K. R. Muske an J. B. Rawlngs, Moel prectve control wth lnear moels, AIChE Journal, Vol. 39, No. 2, 1993, pp o: /ac [24] A. Ghasem, M. Eghtesa an M. Far Neural Network Soluton for Forwar Knematcs Problem of Cable Robot, Journal of Intellgent an Robotc Systems, Vol. 60, No. 2, 2010, pp o: /s z
ENGI9496 Lecture Notes Multiport Models in Mechanics
ENGI9496 Moellng an Smulaton of Dynamc Systems Mechancs an Mechansms ENGI9496 Lecture Notes Multport Moels n Mechancs (New text Secton 4..3; Secton 9.1 generalzes to 3D moton) Defntons Generalze coornates
More informationNew Liu Estimators for the Poisson Regression Model: Method and Application
New Lu Estmators for the Posson Regresson Moel: Metho an Applcaton By Krstofer Månsson B. M. Golam Kbra, Pär Sölaner an Ghaz Shukur,3 Department of Economcs, Fnance an Statstcs, Jönköpng Unversty Jönköpng,
More informationAdvanced Mechanical Elements
May 3, 08 Advanced Mechancal Elements (Lecture 7) Knematc analyss and moton control of underactuated mechansms wth elastc elements - Moton control of underactuated mechansms constraned by elastc elements
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 informationModule 3 LOSSY IMAGE COMPRESSION SYSTEMS. Version 2 ECE IIT, Kharagpur
Module 3 LOSSY IMAGE COMPRESSION SYSTEMS Verson ECE IIT, Kharagpur Lesson 6 Theory of Quantzaton Verson ECE IIT, Kharagpur Instructonal Objectves At the end of ths lesson, the students should be able to:
More informationHigh-Order Hamilton s Principle and the Hamilton s Principle of High-Order Lagrangian Function
Commun. Theor. Phys. Bejng, Chna 49 008 pp. 97 30 c Chnese Physcal Socety Vol. 49, No., February 15, 008 Hgh-Orer Hamlton s Prncple an the Hamlton s Prncple of Hgh-Orer Lagrangan Functon ZHAO Hong-Xa an
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 informationAnalytical classical dynamics
Analytcal classcal ynamcs by Youun Hu Insttute of plasma physcs, Chnese Acaemy of Scences Emal: yhu@pp.cas.cn Abstract These notes were ntally wrtten when I rea tzpatrck s book[] an were later revse to
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 informationDynamic Modeling of a Synchronous Generator Using T-S Fuzzy Approach
e-issn : 0975-0 Hee-Jn Lee / Internatonal Journal of Engneerng an echnology (IJE) Dynamc oelng of a Synchronous Generator Usng -S Fuzzy Approach Hee-Jn Lee Department of Electronc Engneerng Kumoh Natonal
More informationFinite Element Modelling of truss/cable structures
Pet Schreurs Endhoven Unversty of echnology Department of Mechancal Engneerng Materals echnology November 3, 214 Fnte Element Modellng of truss/cable structures 1 Fnte Element Analyss of prestressed structures
More informationENTROPIC QUESTIONING
ENTROPIC QUESTIONING NACHUM. Introucton Goal. Pck the queston that contrbutes most to fnng a sutable prouct. Iea. Use an nformaton-theoretc measure. Bascs. Entropy (a non-negatve real number) measures
More informationCHAPTER 4 HYDROTHERMAL COORDINATION OF UNITS CONSIDERING PROHIBITED OPERATING ZONES A HYBRID PSO(C)-SA-EP-TPSO APPROACH
77 CHAPTER 4 HYDROTHERMAL COORDINATION OF UNITS CONSIDERING PROHIBITED OPERATING ZONES A HYBRID PSO(C)-SA-EP-TPSO APPROACH 4.1 INTRODUCTION HTC consttutes the complete formulaton of the hyrothermal electrc
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 informationOn the Error Modeling of a Novel Mobile Hybrid Parallel Robot
On the Error Moelng of a Novel Moble Hbr Parallel Robot Yongbo Wang (,2), Huapeng Wu (), Hekk Hanroos (), Bngku Chen (2) () Department of Mechancal Engneerng IMVE, Lappeenranta Unverst of echnolog P.O.
More informationChapter 7: Conservation of Energy
Lecture 7: Conservaton o nergy Chapter 7: Conservaton o nergy Introucton I the quantty o a subject oes not change wth tme, t means that the quantty s conserve. The quantty o that subject remans constant
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 informationYukawa Potential and the Propagator Term
PHY304 Partcle Physcs 4 Dr C N Booth Yukawa Potental an the Propagator Term Conser the electrostatc potental about a charge pont partcle Ths s gven by φ = 0, e whch has the soluton φ = Ths escrbes the
More informationUnderactuated Control and Distribution of Multi-Agent Systems in Stratified Flow Environments
49th IEEE Conference on Decson an Control December 15-17, 1 Hlton Atlanta Hotel, Atlanta, GA, USA Uneractuate Control an Dstrbuton of Mult-Agent Systems n Stratfe Flow Envronments Robert H Krohn an Thomas
More informationActive Vibration Control Based on a 3-DOF Dual Compliant Parallel Robot Using LQR Algorithm
The 009 IEEE/RSJ Internatonal Conference on Intellgent Robots an Systems October -5, 009 St. Lous, USA Actve Vbraton Control Base on a 3-DOF Dual Complant Parallel Robot Usng LQR Algorthm Yuan Yun an Yangmn
More informationWHY NOT USE THE ENTROPY METHOD FOR WEIGHT ESTIMATION?
ISAHP 001, Berne, Swtzerlan, August -4, 001 WHY NOT USE THE ENTROPY METHOD FOR WEIGHT ESTIMATION? Masaak SHINOHARA, Chkako MIYAKE an Kekch Ohsawa Department of Mathematcal Informaton Engneerng College
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 informationREAL TIME OPTIMIZATION OF a FCC REACTOR USING LSM DYNAMIC IDENTIFIED MODELS IN LLT PREDICTIVE CONTROL ALGORITHM
REAL TIME OTIMIZATION OF a FCC REACTOR USING LSM DYNAMIC IDENTIFIED MODELS IN LLT REDICTIVE CONTROL ALGORITHM Durask, R. G.; Fernandes,. R. B.; Trerweler, J. O. Secch; A. R. federal unversty of Ro Grande
More informationLarge-Scale Data-Dependent Kernel Approximation Appendix
Large-Scale Data-Depenent Kernel Approxmaton Appenx Ths appenx presents the atonal etal an proofs assocate wth the man paper [1]. 1 Introucton Let k : R p R p R be a postve efnte translaton nvarant functon
More informationArmy Ants Tunneling for Classical Simulations
Electronc Supplementary Materal (ESI) for Chemcal Scence. Ths journal s The Royal Socety of Chemstry 2014 electronc supplementary nformaton (ESI) for Chemcal Scence Army Ants Tunnelng for Classcal Smulatons
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 informationSIMPLIFIED MODEL-BASED OPTIMAL CONTROL OF VAV AIR- CONDITIONING SYSTEM
Nnth Internatonal IBPSA Conference Montréal, Canaa August 5-8, 2005 SIMPLIFIED MODEL-BASED OPTIMAL CONTROL OF VAV AIR- CONDITIONING SYSTEM Nabl Nassf, Stanslaw Kajl, an Robert Sabourn École e technologe
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 informationOn Liu Estimators for the Logit Regression Model
CESIS Electronc Workng Paper Seres Paper No. 59 On Lu Estmators for the Logt Regresson Moel Krstofer Månsson B. M. Golam Kbra October 011 The Royal Insttute of technology Centre of Excellence for Scence
More informationDesign and Analysis of Landing Gear Mechanic Structure for the Mine Rescue Carrier Robot
Sensors & Transducers 214 by IFSA Publshng, S. L. http://www.sensorsportal.com Desgn and Analyss of Landng Gear Mechanc Structure for the Mne Rescue Carrer Robot We Juan, Wu Ja-Long X an Unversty of Scence
More informationKinematics of Fluid Motion
Knematcs of Flu Moton R. Shankar Subramanan Department of Chemcal an Bomolecular Engneerng Clarkson Unversty Knematcs s the stuy of moton wthout ealng wth the forces that affect moton. The scusson here
More informationPHZ 6607 Lecture Notes
NOTE PHZ 6607 Lecture Notes 1. Lecture 2 1.1. Defntons Books: ( Tensor Analyss on Manfols ( The mathematcal theory of black holes ( Carroll (v Schutz Vector: ( In an N-Dmensonal space, a vector s efne
More informationprinceton univ. F 17 cos 521: Advanced Algorithm Design Lecture 7: LP Duality Lecturer: Matt Weinberg
prnceton unv. F 17 cos 521: Advanced Algorthm Desgn Lecture 7: LP Dualty Lecturer: Matt Wenberg Scrbe: LP Dualty s an extremely useful tool for analyzng structural propertes of lnear programs. Whle there
More informationConvexity preserving interpolation by splines of arbitrary degree
Computer Scence Journal of Moldova, vol.18, no.1(52), 2010 Convexty preservng nterpolaton by splnes of arbtrary degree Igor Verlan Abstract In the present paper an algorthm of C 2 nterpolaton of dscrete
More informationThe Noether theorem. Elisabet Edvardsson. Analytical mechanics - FYGB08 January, 2016
The Noether theorem Elsabet Evarsson Analytcal mechancs - FYGB08 January, 2016 1 1 Introucton The Noether theorem concerns the connecton between a certan kn of symmetres an conservaton laws n physcs. It
More informationχ x B E (c) Figure 2.1.1: (a) a material particle in a body, (b) a place in space, (c) a configuration of the body
Secton.. Moton.. The Materal Body and Moton hyscal materals n the real world are modeled usng an abstract mathematcal entty called a body. Ths body conssts of an nfnte number of materal partcles. Shown
More informationIndeterminate pin-jointed frames (trusses)
Indetermnate pn-jonted frames (trusses) Calculaton of member forces usng force method I. Statcal determnacy. The degree of freedom of any truss can be derved as: w= k d a =, where k s the number of all
More informationENGN 40 Dynamics and Vibrations Homework # 7 Due: Friday, April 15
NGN 40 ynamcs and Vbratons Homework # 7 ue: Frday, Aprl 15 1. Consder a concal hostng drum used n the mnng ndustry to host a mass up/down. A cable of dameter d has the mass connected at one end and s wound/unwound
More information4DVAR, according to the name, is a four-dimensional variational method.
4D-Varatonal Data Assmlaton (4D-Var) 4DVAR, accordng to the name, s a four-dmensonal varatonal method. 4D-Var s actually a drect generalzaton of 3D-Var to handle observatons that are dstrbuted n tme. The
More informationOn a one-parameter family of Riordan arrays and the weight distribution of MDS codes
On a one-parameter famly of Roran arrays an the weght strbuton of MDS coes Paul Barry School of Scence Waterfor Insttute of Technology Irelan pbarry@wte Patrck Ftzpatrck Department of Mathematcs Unversty
More informationIntroduction. - The Second Lyapunov Method. - The First Lyapunov Method
Stablty Analyss A. Khak Sedgh Control Systems Group Faculty of Electrcal and Computer Engneerng K. N. Toos Unversty of Technology February 2009 1 Introducton Stablty s the most promnent characterstc of
More informationRobust Dynamic Programming for Discounted Infinite-Horizon Markov Decision Processes with Uncertain Stationary Transition Matrice
roceengs of the 2007 IEEE Symposum on Approxmate Dynamc rogrammng an Renforcement Learnng (ADRL 2007) Robust Dynamc rogrammng for Dscounte Infnte-Horzon Markov Decson rocesses wth Uncertan Statonary Transton
More informationOn the Coordinated Control of Multiple HVDC Links: Modal Analysis Approach
R. Erksson an V. Knazkns / GMSARN nternatonal Journal 2 (2008) 15-20 On the Coornate Control of Multple HVDC Lnks: Moal Analyss Approach Robert Erksson an Valerjs Knazkns Abstract There are several possbltes
More informationField and Wave Electromagnetic. Chapter.4
Fel an Wave Electromagnetc Chapter.4 Soluton of electrostatc Problems Posson s s an Laplace s Equatons D = ρ E = E = V D = ε E : Two funamental equatons for electrostatc problem Where, V s scalar electrc
More informationModule 3: Element Properties Lecture 1: Natural Coordinates
Module 3: Element Propertes Lecture : Natural Coordnates Natural coordnate system s bascally a local coordnate system whch allows the specfcaton of a pont wthn the element by a set of dmensonless numbers
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 informationYong Joon Ryang. 1. Introduction Consider the multicommodity transportation problem with convex quadratic cost function. 1 2 (x x0 ) T Q(x x 0 )
Kangweon-Kyungk Math. Jour. 4 1996), No. 1, pp. 7 16 AN ITERATIVE ROW-ACTION METHOD FOR MULTICOMMODITY TRANSPORTATION PROBLEMS Yong Joon Ryang Abstract. The optmzaton problems wth quadratc constrants often
More informationFirst Law: A body at rest remains at rest, a body in motion continues to move at constant velocity, unless acted upon by an external force.
Secton 1. Dynamcs (Newton s Laws of Moton) Two approaches: 1) Gven all the forces actng on a body, predct the subsequent (changes n) moton. 2) Gven the (changes n) moton of a body, nfer what forces act
More information829. An adaptive method for inertia force identification in cantilever under moving mass
89. An adaptve method for nerta force dentfcaton n cantlever under movng mass Qang Chen 1, Mnzhuo Wang, Hao Yan 3, Haonan Ye 4, Guola Yang 5 1,, 3, 4 Department of Control and System Engneerng, Nanng Unversty,
More informationCOMPOSITE BEAM WITH WEAK SHEAR CONNECTION SUBJECTED TO THERMAL LOAD
COMPOSITE BEAM WITH WEAK SHEAR CONNECTION SUBJECTED TO THERMAL LOAD Ákos Jósef Lengyel, István Ecsed Assstant Lecturer, Professor of Mechancs, Insttute of Appled Mechancs, Unversty of Mskolc, Mskolc-Egyetemváros,
More informationNeuro-Adaptive Design - I:
Lecture 36 Neuro-Adaptve Desgn - I: A Robustfyng ool for Dynamc Inverson Desgn Dr. Radhakant Padh Asst. Professor Dept. of Aerospace Engneerng Indan Insttute of Scence - Bangalore Motvaton Perfect system
More informationThe equation of motion of a dynamical system is given by a set of differential equations. That is (1)
Dynamcal Systems Many engneerng and natural systems are dynamcal systems. For example a pendulum s a dynamcal system. State l The state of the dynamcal system specfes t condtons. For a pendulum n the absence
More informationApplication of Gravitational Search Algorithm for Optimal Reactive Power Dispatch Problem
Applcaton of Gravtatonal Search Algorthm for Optmal Reactve Power Dspatch Problem Serhat Duman Department of Electrcal Eucaton, Techncal Eucaton Faculty, Duzce Unversty, Duzce, 8620 TURKEY serhatuman@uzce.eu.tr
More informationSolutions to exam in SF1811 Optimization, Jan 14, 2015
Solutons to exam n SF8 Optmzaton, Jan 4, 25 3 3 O------O -4 \ / \ / The network: \/ where all lnks go from left to rght. /\ / \ / \ 6 O------O -5 2 4.(a) Let x = ( x 3, x 4, x 23, x 24 ) T, where the varable
More informationMEV442 Introduction to Robotics Module 2. Dr. Santhakumar Mohan Assistant Professor Mechanical Engineering National Institute of Technology Calicut
MEV442 Introducton to Robotcs Module 2 Dr. Santhakumar Mohan Assstant Professor Mechancal Engneerng Natonal Insttute of Technology Calcut Jacobans: Veloctes and statc forces Introducton Notaton for tme-varyng
More informationEEE 241: Linear Systems
EEE : Lnear Systems Summary #: Backpropagaton BACKPROPAGATION The perceptron rule as well as the Wdrow Hoff learnng were desgned to tran sngle layer networks. They suffer from the same dsadvantage: they
More informationA Multi-Axis Force Measurement System for a Space Docking Mechanism
3rd Internatonal Conference on Materal, Mechancal and Manufacturng Engneerng (IC3ME 215) A Mult-Axs orce Measurement System for a Space Dockng Mechansm Gangfeng Lu a*, Changle L b and Zenghu Xe c Buldng
More informationStructure and Drive Paul A. Jensen Copyright July 20, 2003
Structure and Drve Paul A. Jensen Copyrght July 20, 2003 A system s made up of several operatons wth flow passng between them. The structure of the system descrbes the flow paths from nputs to outputs.
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 informationChapter 12. Ordinary Differential Equation Boundary Value (BV) Problems
Chapter. Ordnar Dfferental Equaton Boundar Value (BV) Problems In ths chapter we wll learn how to solve ODE boundar value problem. BV ODE s usuall gven wth x beng the ndependent space varable. p( x) q(
More information1 Convex Optimization
Convex Optmzaton We wll consder convex optmzaton problems. Namely, mnmzaton problems where the objectve s convex (we assume no constrants for now). Such problems often arse n machne learnng. For example,
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 informationNumerical Heat and Mass Transfer
Master degree n Mechancal Engneerng Numercal Heat and Mass Transfer 06-Fnte-Dfference Method (One-dmensonal, steady state heat conducton) Fausto Arpno f.arpno@uncas.t Introducton Why we use models and
More informationTime dependent weight functions for the Trajectory Piecewise-Linear approach?
Tme epenent weght functons for the Trajectory Pecewse-Lnear approach? Juan Pablo Amorocho an Heke Faßbener Abstract Moel orer reucton (MOR) has become an ubqutous technque n the smulaton of large-scale
More informationWeek3, Chapter 4. Position and Displacement. Motion in Two Dimensions. Instantaneous Velocity. Average Velocity
Week3, Chapter 4 Moton n Two Dmensons Lecture Quz A partcle confned to moton along the x axs moves wth constant acceleraton from x =.0 m to x = 8.0 m durng a 1-s tme nterval. The velocty of the partcle
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 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 informationPassive Bilateral Teleoperation with Constant Time Delays
Proceengs of the 6 IEEE Internatonal Conference on Robotcs an Automaton Orlano, Flora - May 6 Passve Blateral eleoperaton wth Constant me Delays Dongjun Lee an Mark W Spong Coornate Scence Laboratory Unversty
More informationCSci 6974 and ECSE 6966 Math. Tech. for Vision, Graphics and Robotics Lecture 21, April 17, 2006 Estimating A Plane Homography
CSc 6974 and ECSE 6966 Math. Tech. for Vson, Graphcs and Robotcs Lecture 21, Aprl 17, 2006 Estmatng A Plane Homography Overvew We contnue wth a dscusson of the major ssues, usng estmaton of plane projectve
More informationRobust Model Predictive Control
Robust Model Predctve Control Formulatons of robust control [1] he robust control problem concerns to the control of plants that are only approxmately nown. Usually, t s assumed that the plant les n a
More informationCubic Trigonometric B-Spline Applied to Linear Two-Point Boundary Value Problems of Order Two
World Academy of Scence Engneerng and echnology Internatonal Journal of Mathematcal and omputatonal Scences Vol: No:0 00 ubc rgonometrc B-Splne Appled to Lnear wo-pont Boundary Value Problems of Order
More informationOptimization Techniques for Natural Resources
Optmzaton Technques for Natural Resources SEFS 540 / ESRM 490 B Lecture 1 (3/27/2017) About the Instructor Teachng: nspre stuents to be curous but crtcal learners who can thnk for themselves an nurture
More informationAppendix for Causal Interaction in Factorial Experiments: Application to Conjoint Analysis
A Appendx for Causal Interacton n Factoral Experments: Applcaton to Conjont Analyss Mathematcal Appendx: Proofs of Theorems A. Lemmas Below, we descrbe all the lemmas, whch are used to prove the man theorems
More information( ) = : a torque vector composed of shoulder torque and elbow torque, corresponding to
Supplementary Materal for Hwan EJ, Donchn O, Smth MA, Shamehr R (3 A Gan-Fel Encon of Lmb Poston an Velocty n the Internal Moel of Arm Dynamcs. PLOS Boloy, :9-. Learnn of ynamcs usn bass elements he nternal
More informationLossy Compression. Compromise accuracy of reconstruction for increased compression.
Lossy Compresson Compromse accuracy of reconstructon for ncreased compresson. The reconstructon s usually vsbly ndstngushable from the orgnal mage. Typcally, one can get up to 0:1 compresson wth almost
More informationTHE EFFECT OF TORSIONAL RIGIDITY BETWEEN ELEMENTS ON FREE VIBRATIONS OF A TELESCOPIC HYDRAULIC CYLINDER SUBJECTED TO EULER S LOAD
Journal of Appled Mathematcs and Computatonal Mechancs 7, 6(3), 7- www.amcm.pcz.pl p-issn 99-9965 DOI:.75/jamcm.7.3. e-issn 353-588 THE EFFECT OF TORSIONAL RIGIDITY BETWEEN ELEMENTS ON FREE VIBRATIONS
More informationNon-negative Matrices and Distributed Control
Non-negatve Matrces an Dstrbute Control Yln Mo July 2, 2015 We moel a network compose of m agents as a graph G = {V, E}. V = {1, 2,..., m} s the set of vertces representng the agents. E V V s the set of
More informationU.C. Berkeley CS294: Beyond Worst-Case Analysis Luca Trevisan September 5, 2017
U.C. Berkeley CS94: Beyond Worst-Case Analyss Handout 4s Luca Trevsan September 5, 07 Summary of Lecture 4 In whch we ntroduce semdefnte programmng and apply t to Max Cut. Semdefnte Programmng Recall that
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 informationPhys 331: Ch 7,.2 Unconstrained Lagrange s Equations 1
Phys 33: Ch 7 Unconstrane agrange s Equatons Fr0/9 Mon / We /3 hurs /4 7-3 agrange s wth Constrane 74-5 Proof an Eaples 76-8 Generalze Varables & Classcal Haltonan (ecoen 79 f you ve ha Phys 33) HW7 ast
More informationGlobal Sensitivity. Tuesday 20 th February, 2018
Global Senstvty Tuesday 2 th February, 28 ) Local Senstvty Most senstvty analyses [] are based on local estmates of senstvty, typcally by expandng the response n a Taylor seres about some specfc values
More informationA Hybrid Variational Iteration Method for Blasius Equation
Avalable at http://pvamu.edu/aam Appl. Appl. Math. ISSN: 1932-9466 Vol. 10, Issue 1 (June 2015), pp. 223-229 Applcatons and Appled Mathematcs: An Internatonal Journal (AAM) A Hybrd Varatonal Iteraton Method
More informationPHYS 705: Classical Mechanics. Calculus of Variations II
1 PHYS 705: Classcal Mechancs Calculus of Varatons II 2 Calculus of Varatons: Generalzaton (no constrant yet) Suppose now that F depends on several dependent varables : We need to fnd such that has a statonary
More informationKernel Methods and SVMs Extension
Kernel Methods and SVMs Extenson The purpose of ths document s to revew materal covered n Machne Learnng 1 Supervsed Learnng regardng support vector machnes (SVMs). Ths document also provdes a general
More informationAppendix B: Resampling Algorithms
407 Appendx B: Resamplng Algorthms A common problem of all partcle flters s the degeneracy of weghts, whch conssts of the unbounded ncrease of the varance of the mportance weghts ω [ ] of the partcles
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 informationModeling and Simulation of a Hexapod Machine Tool for the Dynamic Stability Analysis of Milling Processes. C. Henninger, P.
Smpack User Meetng 27 Modelng and Smulaton of a Heapod Machne Tool for the Dynamc Stablty Analyss of Mllng Processes C. Hennnger, P. Eberhard Insttute of Engneerng project funded by the DFG wthn the framework
More informationTime-Varying Systems and Computations Lecture 6
Tme-Varyng Systems and Computatons Lecture 6 Klaus Depold 14. Januar 2014 The Kalman Flter The Kalman estmaton flter attempts to estmate the actual state of an unknown dscrete dynamcal system, gven nosy
More informationPLANAR TRANSLATIONAL CABLE-DIRECT-DRIVEN ROBOTS
PLANA TANSLATIONAL CABLE-DIECT-DIVEN OBOTS obert L. Wllams II Oho Unversty Athens, Oho Paolo Gallna 2 Unversty of Treste Treste, Italy Jgar Vada 3 Oho Unversty Athens, Oho Journal of obotc Systems Vol.
More informationHigh resolution entropy stable scheme for shallow water equations
Internatonal Symposum on Computers & Informatcs (ISCI 05) Hgh resoluton entropy stable scheme for shallow water equatons Xaohan Cheng,a, Yufeng Ne,b, Department of Appled Mathematcs, Northwestern Polytechncal
More informationAmiri s Supply Chain Model. System Engineering b Department of Mathematics and Statistics c Odette School of Business
Amr s Supply Chan Model by S. Ashtab a,, R.J. Caron b E. Selvarajah c a Department of Industral Manufacturng System Engneerng b Department of Mathematcs Statstcs c Odette School of Busness Unversty of
More informationDistributed Exponential Formation Control of Multiple Wheeled Mobile Robots
Proceedngs of the Internatonal Conference of Control, Dynamc Systems, and Robotcs Ottawa, Ontaro, Canada, May 15-16 214 Paper No. 46 Dstrbuted Exponental Formaton Control of Multple Wheeled Moble Robots
More informationDesign of Optimum Controllers for Gas Turbine Engines
Desgn of Optmum Controllers for Gas Turbne Engnes Junxa Mu 1, Dav Rees 1, Cer Evans 1 an Neophytos Chras 1 School of Electroncs, Unversty of Glamorgan Pontypr, CF37 1DL, Wales, UK Phone: +44() 1443 4859
More informationMathematical Preparations
1 Introducton Mathematcal Preparatons The theory of relatvty was developed to explan experments whch studed the propagaton of electromagnetc radaton n movng coordnate systems. Wthn expermental error the
More informationAppendix B. The Finite Difference Scheme
140 APPENDIXES Appendx B. The Fnte Dfference Scheme In ths appendx we present numercal technques whch are used to approxmate solutons of system 3.1 3.3. A comprehensve treatment of theoretcal and mplementaton
More informationModule 1 : The equation of continuity. Lecture 1: Equation of Continuity
1 Module 1 : The equaton of contnuty Lecture 1: Equaton of Contnuty 2 Advanced Heat and Mass Transfer: Modules 1. THE EQUATION OF CONTINUITY : Lectures 1-6 () () () (v) (v) Overall Mass Balance Momentum
More informationA Particle Swarm approach for the Design of Variable Structure Stabilizer for a Nonlinear Model of SMIB System
A Partcle Swarm approach for the Desgn of Varable Structure Stablzer for a Nonlnear Moel of SMIB System NAI A AL-MUSABI**, ZAKARIYA M AL-HAMOUZ*, HUSSAIN N AL-DUWAISH* ** The Petroleum Insttute, Electrcal
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 informationParametric fractional imputation for missing data analysis. Jae Kwang Kim Survey Working Group Seminar March 29, 2010
Parametrc fractonal mputaton for mssng data analyss Jae Kwang Km Survey Workng Group Semnar March 29, 2010 1 Outlne Introducton Proposed method Fractonal mputaton Approxmaton Varance estmaton Multple mputaton
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 information