Robust Output Tracking Control of a Surface Vessel
|
|
- Cassandra Foster
- 5 years ago
- Views:
Transcription
1 8 American Control Conference Westin Seattle Hotel, Seattle, Whington, USA June -3, 8 WeA6. Robust Output Tracking Control of a Surface Vessel DongBinLee,EnverTatlicioglu,Timothy C.Burg,DarrenM.Dawson Abstract Inthispaper,trackingcontrolofathreeegreeof-freeom marine vessel is examine. The primary motivation forthisworkisthe compensationneee forthe ae ms common to surface vessels, resulting in an ymmetric inertia matrix. Two control schemes are consiere: a fullstate feeback controller an an output feeback controller. Numerical simulation results are shown to emonstrate the valiityofthesepropose controllers. I. Introuction Research into the control of marine surface vessels coul be loosely categorize maneuvering [,], ynamic positioning [3,4], tracking (incluing path following or way-point tracking) [6,8], an more recently formation control [5]. From a control perspective, the properties of the ynamic moel of the surface vessel are of great importance. Specifically, the symmetry an the positive efiniteness of the inertia matrix are an important sumption often use in control evelopment. The inertia matrix of a vessel is commonly efine to be equal to the sum of the rigi-boy inertia matrix an the ae ms. The rigi-boy inertia matrix is strictly a symmetric matrix. The ae ms terms result from hyroynamic forces an moments ue to motion of the vessel boy an from the interaction with the fluis an waves. In surface vessel control, the ae ms matrix can eily become ymmetric, especially for higher relative velocity. This ymmetry in the ae ms terms will result in an ymmetric inertia matrix in the ship moel, which may cause system instability or a failure in meeting the control objectives if ignore. As the founation of this work, previous closely relate work is escribe. In [], Skjetne et al. consiere maneuvering control of three egree-of-freeom(3 DOF) marine vessel an presente experiment results for the Cybership II. In [6], Do an Pan presente a global tracking controller of an uneractuate vessel where the system matrices are positive efinite but nonzero o-iagonal terms an Do in [7] propose robust an aaptive output feeback controllers for positioning of a surfacevesselsumethesystemmatricestobepositive efinite at low spee. In [8], Behal et al. utilize a ThisworkhbeensupporteinpartbyaDOEContract,a HonaCorporationGrant. D.Lee,T.C.Burg,D.M.DawsonarewiththeDep tof Electrical an Computer Engineering, Clemson University, Clemson,SC9634,USA. lee@clemson.eu,tburg@clemson.eu ( corresponingauthor),arren.awson@ces.clemson.eu.e.tatliciogluwdep tofelectrical&computerengineering,clemson University.Heisnow with thedep tofelectricalan Electronics Engineering, Izmir Institute of Technology, Urla, Izmir 3543, Turkey. enver@envertatlicioglu.com high-gain observer in the esign to control uneractuate surface vessels with nonintegrable ynamic moels where the inertia matrix w iagonal. However, a few researchers have aresse the ymmetry of the inertia matrix. For example, Skjetne et al. in[] evelope the Coriolis-centripetal an amping moel of the ship for the ymmetric ae ms matrix, but the ms-relate parameters were use in the symmetric form at the experiment, which may be violate at higher operating spees. Inthispaper,wefocusontrackingcontrolofa3DOF surface vessel. The ynamic moel of the ship is sume to be uncertain an the ae ms terms are consiere to be ymmetric which results in an ymmetric inertia matrix. To aress this problem, the ynamic moel of the ship is moifie to have a symmetric an positiveefinite inertia matrix. The novelty of this moification is the multiplication of the system ynamic moel in [] with an upper triangular matrix which results in amoelwithymmetricinertiamatrix.afterthis moification, the resulting ynamic moel becomes a special ce of the multi-input multi-output system that wconsierein[](seeequationin[] ).Next,the robust full-state feeback (FSFB) an output feeback (OFB) control strategies in [], which were esigne for general cls of multi-input multi-output nonlinear systems, are tailore to fit this ynamic surface vessel moel. The paper is organize follows: Section II presents aynamicanakinematicmoelofthe3dofsurface vessel. The error system evelopment an the control strategies are provie in Section III. The numerical simulation results are shown in Section IV followe by conclusions in Section V. II. SystemMoel In this section, the system moel an relevant properties are iscusse. The ynamic an kinematic moels of a 3 DOF surface vessel expresse in the boy-fixe frame,b,aregiven[, ] M +C+D = () ẋ = R () where the vector ẋ(t)r 3 represents the position an orientation rate in which x =[x p,y p,] > enotes the The robust control evelopment in [9] is similar to [] with aminormoification in the matrix ecomposition (see Lemma in both [9]an []).In thatsense,throughoutthispaperwe will referto [9],however,thereaerisalso referre to [] /8/$5. 8 AACC. 544
2 linear position (x p,y p )alongthex-anthey-axes an the yaw angle (). The vectors v r (t), (t)=[u, v, ] >,an (t)r 3 enotetherelativevelocitybetween the fluis an vessel an the velocity an acceleration of the rigi-boy ship, respectively. M(),C(, r ), D(, r )R 3x3 representtheinertiamatrix,centripetal an Coriolis force, an hyroynamic amping terms, respectively. In the subsequent control evelopment, M( ),C( ),and( ) are sume to be uncertain an continuously ierentiable up to their secon time erivatives.in(),(t)r 3 representsthecontrolinput vector which h the following form =[,, 3 ] > (3) where (t) an (t)r are the translational forces inthex-any-irections,respectivelyan 3 (t)r is the moment about the Z-axis. The matrix, R() SO(3),enotes the rotation matrix, containing the yaw angle, about the Z-axis.Thecoorinateframeofthe surface vessel is presente in Figure, where B is the boy-fixe reference frame of the vessel an a fixe inertial frame, approximate by the earth-fixe frame (North-Et-Down convention), is enote by I.The To facilitate the subsequent control evelopment, the ynamic moel in () will now be moifie to obtain a symmetric inertia matrix. There will exist an upper iagonalmatrix,t( )R 3x3,suchthatthemultiplication oft( )anm( )resultsinymmetric,positiveefinite matrix, enote by M s ( )R 3x3. After multiplying () with T( ), the following expression is obtaine M s =T(C+D)+T. (5) To further moify the ynamic moel, the time erivativeof()isobtaineinthefollowing form =R > ẍr > ṘR > ẋ (6) wherethepropertyoftherotationmatrixthatr - ()= R > ()wutilize.substituting(6)into(5)yiels M s R > ẍ= h i M s S 3 ( )T(C+D) R > ẋ+t (7) where the time erivative of the orientation matrix, enotebyṙ(),ankew-symmetricmatrixs 3( ) R 3x3 canbecalculatefollows Ṙ()=RS( ),S 3 ( )=. (8) Afterpremultiplying(7)withR(),thefollowingmoel is obtaine M()ẍ= C(x,ẋ,, r )ẋ+rt (9) where M()an C(x,ẋ,, r )R 3x3 areefine M,RM s R > () h i C=R M s S 3 ( )T(C+D) R >. () Fig.. Diagram ofasurfacevessel states are meure from the center point (CP) of the ship frame expresse in B an x g enotes the istance between the center point an the center of gravity(cg) oftheship. Theinertiamatrix,M( ),oftheshipisefine[] M,M RB +M A (4) wherem RB ( )R 3x3 representstherigi-boysymmetricinertiaanm A ( )R 3x3 accountsfortheymmetric ae ms. Since M A ( ) is ymmetric the inertia matrixofthesurfacevessel,m( ),isalsoanymmetric matrix. It shoul be note that the form of (9) w motivate bytheynamicmoelin[9],[]anhence,solvingthe same control problem. Property Thematrix : M()ispositiveefinite, symmetric, an satisfies the following inequalities kk T M kk,r 3 () where, R are positive bouning constants. III. Control Development A. Full-State Feeback Control The subsequent evelopment is be on the sumptionthatallthestatesofthevesselaremeurable. 545
3 ) Error System Development : The tracking error for position an orientation, enote by e (t)r 3,isefine e,x x (3) where x (t) R 3 is the esire trajectory. For the subsequent stability analysis, the esire trajectory an its first an secon time erivatives are sume to be boune (i.e., x (t), ẋ (t), an ẍ (t) L ). To facilitate the subsequent error system evelopment, a filtereerror,enoteby e (t)r 3,isefine e,ė +e. (4) Inorertosimplifytheerrorsystemantofacilitatethe stability analysis, a filtere tracking error is introuce r,e +e. (5) Theynamicsofr(t)canbeobtainefollows ṙ=ẍ ẍ+ė (6) where the secon time erivatives of(3) an(4) were utilize. After premultiplying (6) with M(),wecan obtain the following expression Mṙ= Mẍ CẋRT+Mė (7) where (9) w utilize. The expression in (7) can be rearrangeafteraingansubtractingtheterms. Mr (t),e (t),anr(t)totheright-han sie Mṙ=NR. Mre R(TI 3 ) (8) wheretheauxiliarysignaln( )R 3 isefineby N, Mẍ Cẋ+Mė +. Mr+e. (9) To facilitate the control evelopment, the open-loop error ynamics can be obtaine from(8) Mṙ=Ñ+N. Mre R () wherethesignals(t), (t)r areefine +,R(TI 3 ), () wherethethircomponentof(ti 3 )iszero(anexample of T( ) isshowninthesimulationsection)ann ( ), Ñ( )R 3 areefinefollows N,N x=x, ẋ=ẋ, ẍ=ẍ, Ñ,NN () where the esire trajectory an its first two time erivativesaresumetobebouneanhencen ( ) an Ṅ( )areboune signals. Remark: The term Ñ( ) in () is upper boune Ñ N (kzk)kzk (3) where N ( )isagloballyinvertible,non-ecreingfunction an the auxiliary error vector z(t)r 9 is efine z(t)=[e >,e >,r > ] >. ) Control Input : Beontheopen-looperrorynamicsin()anthe resultin[9], thecontrol input(t)isesigne,r > (K+I 3 )r+r >ˆf (4) where KR 3x3 is a constant positive efinite iagonal gain matrix an ˆf(t)R 3 is a feeforwar component that is introuce to compensate for N (t) an (t). After substituting (4) into (), the following closeloop error system can be obtaine Mṙ=+. Mre (K+I 3 )r (5) where (t) an (t) R 3 are auxiliary functions efine follows,ñ,,n ˆf. (6) Notethatsince ˆf( )isusetocompensateforfunctions of the esire trajectory it is known that ˆf( ) L apriori. Remark: The controller propose in (4) is an application of the previous theoretical evelopment in [9] where the propose control yiels a semi-global, uniformly, an ultimately boune (sguub) tracking result. Thus, the reaer is referre to [9] for a etaile stability analysis. Remark3: The term ˆf( ) in (4) an (35) is not irectly specifie here but in practice it can be implemente in other ways incluing a neural network. B. Output Feeback Control The following evelopment is be on the sumption that the position an the orientation of the ship, x(t), is the only state that is meurable. ) Observer Design : To facilitate the subsequent control evelopment, the auxiliaryerrorvector,enotebyz(t)r 6,isreefine z(t)=[e >,r > ] > (7) where e (t) an r(t) are error signals efine in (3) an (5), respectively. The following expression can be obtaine for the ynamics of z(t) ż=[(re ) >, ṙ > ] > (8) where(3) an(4) were utilize. An estimate of the unmeurable, z(t) in (7), is introuce follows ẑ, ê >,ˆr > > (9) where ê (t),ˆr(t) R 3 are high-gain observers that are introuce to estimate the error signals e (t) an r(t), respectively []. The time erivative of (9) can be obtaine. ẑ, ". ê.ˆr # ˆrê + = (e ê ) (e ê ). (3) 546
4 To facilitate the subsequent analysis, the following observer errors, enote by (t) an (t) R 3, are introuce = (e ê ), =rˆr. (3) Theynamicsfortheobservererrorscanbeobtaine follows = ( + ), = +ṙ (3) where(3) an(3) were utilize. After combining(3), the following simplifie expression can be obtaine.=a o+g (33) where (t),[ >, > ] > R 6 an the signals g(t)r 6 an A o R 6x6 areefinefollows I A o = 3 I 3,g=. (34) I 3 O 3 ṙ ) Control Input : Similarto(4)antheresultin[9],theoutputfeeback controller for ṙ(t) in(34) is esigne follows,r > sat{(k+i 3 )ˆr}+R >ˆf (35) where sat{ } R 3 represents the vector saturation function an ˆf(t) R 3 isthefeeforwarterm(see Remark 3). Substituting this control input into () yiels the following close-loop error system Mṙ=+. Mre sat{(k+i 3 )ˆr} (36) where( )an ( )wereintroucein(6). Remark 4: Since the output feeback controller esigne in (35) is a special ce of the evelopment in [9], a semi-global, uniformly, an ultimately boune (sguub) tracking result can be inferre. IV. Numerical Simulation Results Two numerical simulations were performe to show the valiity of the propose controllers. The rigi-boy inertia matrix incluing the ae ms terms are of the following form[] M = m+x u n a n n c n b (37) where n a,n b,n c, an n are auxiliary terms that are efine follows n a = my v,n b =I z Nṙ n c = mx g N v,n =mx g Yṙ. From(37),itcanbeseenthattheaemsmatrix,enotebyM A ( ),hnonzeroo-iagonalhyroynamic amping terms (usually refere to hyroynamic erivatives). In [], Yṙ an N v were set equal to zero which resulte in a symmetric inertia matrix. It is clear that if the values of Yṙ an N v are ierent, then the resulting matrix is ymmetric. For the simulation, the following values were chosen for these parameters Yṙ=.,N v =., (38) which prouce an ymmetric inertia matrix. Be on the inertia matrix in (37), the following T( ) matrix is efine to moify the system ynamic moel T = n a n b (39) + n c n a n + n an c n c n + n an b whereisanon-zeroauxiliarytermefine = mi z +mnṙ+y v I z Y v Nṙ+(mx g ) mx g N v mx g Yṙ+YṙN v. The Coriolis-centripetal term C( ) in () isefine by combining the rigi-boy matrix C RB () R 3x3 an corresponingaemsc A (, r )R 3x3 C(, r )= c c (4) c c wherec ( r )=mu+(x u u r )anc (, r )=m(x g + v)+(y v v r +.5(Yṙ+N v ) ). The amping matrix D( ) in () is efine by combining the linear matrix term D L ()R 3x3 an nonlinear matrix D NL (, r )R 3x3 D(, r )= (4) where ( r )=X u +(X u u u r X uuu u r), (, r )=Y v +(Y v v u r Y rv ), 33 (, r )= N r +(Y v v u r Y r v ), 3 (, r )=Y r + (Y v r u r Y r v ), an 3 (, r )=N v + (N v v v r N rv ). The saturator which limts the signals to upper an lower w use by ± for the control input both FSFB an OFB controllers. The other system parameters were obtaine from the experimental resultsin[].theesirepositionanyawtrajectory are specifie below sin(.t) x (t)= (m), cos(.t) (t)=.t(ra), an the vessel w consiere to be initially at rest in the following configuration x() = [.,, - 8 ]>. The surface vessel w specifie to have the relative velocity, v r =[3,,] > where the relative velocity is sume to have the constant surge spee, 3[m/s], about the X-axis. A. Full-State Feeback(FSFB) Control For the FSFB controller simulation, the constant control parameter w chosen K = iag 5 5 ª. In Figure, tracking the esire trajectory of the surface vessel in XY-plane is emonstrate. In Figure 3, the position an yaw angle 547
5 Desire Actual Position x Error in Boy fixe Frame Y Position y Error in Boy fixe Frame Yaw (ψ) Angle Error 5 X Fig.. Trackingemonstration inthexy-plane(fsfb) of the ship are presente along with their corresponing esire trajectories. The error signal e (t) is presente in Figure 4. From Figure 4, it is clear that the surface vessel tracke the esire trajectory. The control input (t)isshowninfigure5. Position Tracking along x axis actual esire Position Tracking along y axis Orientation Tracking along yaw irection Fig. 4. Tracking Errors in Position (x p,y p)anyawangle() (FSFB) [N] Translational Force Input u Translational Force Input u Rotational Torque Input u Fig.5. ForcesanTorqueInput(FSFB) Fig.3. Trackingemonstration (FSFB) B. Output Feeback(OFB) Control For the OFB controller, the constant control parameter w chosen K =iag 4 4 ª an the following control parameters were use =, =, an =.. In Figure 6, the position an the esire trajectory of the surface vessel in XY-plane is emonstrate. Figure 7 shows the position an yaw angle of the ship along with their corresponing esire trajectories. Figure 8 isplays the small, boune trackingerrorsignals.infigure9,thecontrolinput(t) is presente. V. Conclusion The control problem of surface vessels with ymmetric inertia matrices w aresse. The significance of this work w the moification of the inertia matrix by pre-multiplying with an upper triangular matrix to obtain a symmetric form. Then, a full-state feeback an an output feeback controller were esigne. Numerical simulation results were shown to emonstrate the propose control strategies. References 548
6 Desire Actual Position x Error Position y Error Y Yaw (ψ) Angle Error 5 X Fig.6. Trackingemonstration in thexy-plane(ofb) Position Tracking along x axis actual esire Position Tracking along y axis Orientation Tracking along yaw irection Fig.8. Tracking Errorsin Position an Yaw Angle (OFB) [N] 5 Translational Force Input u Translational Force Input u Rotational Torque Input u Fig.7. Trackingemonstration (OFB) Fig.9. ForcesanTorqueInput(OFB) []T.I.Fossen,MarineControlSystems:Guiance,Navigation, an Control of Ships, Rigs an Unerwater Vehicles, Tronheim:MarineCyberneticsAS,Norway,ste.. [] R.Skjetne,O.N.Smogeli,anT.I.Fossen, ANonlinearShip ManoeuveringMoel:Ientificationanaaptivecontrolwith experiments for a moel ship, Moeling, Ientification an Control,Vol5,No.,pp.3-7,4. [3] T. D. Nguyen, A. J. Sørensen, an S. T. Quek, Design of Hybri Controller for Dynamic Positioning from Calm to ExtremeSeaConitions,Automatica,Vol.43,No.5,pp ,May7. [4] E. A. Tannuri an H.M. Morishita, Experimental an numerical evaluation of a typical ynamic positioning system, Applie Ocean Research Vol. 8, No., pp , April 6. [5] F.Fahimi, NonlinearMoelPreictiveFormationControlfor GroupsofAutonomousSurfaceVessels,InternationalJournal ofcontrol,vol.8,issue8,pp.48-59,august7. [6] K. D. Do an J. Pan, Global tracking control of uneractuate ships with nonzero o-iagonal terms in their system matrices,automatica,vol.4,pp.87-95,5. [7] K. D. Do, Global Robust an Aaptive Output Feeback Dynamic Positioning of Surface Ships, IEEE International Conference on Robotics an Automation, Rome, Italy, pp ,April7. [8]A.Behal,D.M.Dawson,W.E.Dixon,anY.Fang, Tracking an Regulation Control of an Uneractuate Surface Vessel with NonintegrableDynamics,IEEE TransactionsonAutomaticControl,Vol.47,No.3,pp.495-5,March. [9]X.Zhang,A.Behal,D.M.Dawson,anB.Xian, Output Feeback Control for a Cls of Uncertain MIMO Nonlinear SystemswithNon-SymmetricInputGainMatrix,Proc.44th IEEEConferenceonDecisionanControl,antheEuropean ControlConference,Seville,Spain,pp ,Dec.5. []J.Chen,A.Behal,D.M.Dawson,anX.Zhang, Robust an Aaptive Output Feeback Control Strategies for a Cls of Uncertain MIMO Nonlinear Systems, Technical Report, CRB, Clemson University, April 6, Available: [] A. N. Atsi an H. K. Khalil, A Separtion Principle for the Stabilization of a Cls of Nonlinear Systems, IEEE TransactionsonAutomaticControl,Vol.44,No.9,pp ,Sept
Optimal Variable-Structure Control Tracking of Spacecraft Maneuvers
Optimal Variable-Structure Control racking of Spacecraft Maneuvers John L. Crassiis 1 Srinivas R. Vaali F. Lanis Markley 3 Introuction In recent years, much effort has been evote to the close-loop esign
More informationVIRTUAL STRUCTURE BASED SPACECRAFT FORMATION CONTROL WITH FORMATION FEEDBACK
AIAA Guiance, Navigation, an Control Conference an Exhibit 5-8 August, Monterey, California AIAA -9 VIRTUAL STRUCTURE BASED SPACECRAT ORMATION CONTROL WITH ORMATION EEDBACK Wei Ren Ranal W. Bear Department
More informationRobust Tracking Control of Robot Manipulator Using Dissipativity Theory
Moern Applie Science July 008 Robust racking Control of Robot Manipulator Using Dissipativity heory Hongrui Wang Key Lab of Inustrial Computer Control Engineering of Hebei Province Yanshan University Qinhuangao
More informationExponential Tracking Control of Nonlinear Systems with Actuator Nonlinearity
Preprints of the 9th Worl Congress The International Feeration of Automatic Control Cape Town, South Africa. August -9, Exponential Tracking Control of Nonlinear Systems with Actuator Nonlinearity Zhengqiang
More informationNested Saturation with Guaranteed Real Poles 1
Neste Saturation with Guarantee Real Poles Eric N Johnson 2 an Suresh K Kannan 3 School of Aerospace Engineering Georgia Institute of Technology, Atlanta, GA 3332 Abstract The global stabilization of asymptotically
More informationTRAJECTORY TRACKING FOR FULLY ACTUATED MECHANICAL SYSTEMS
TRAJECTORY TRACKING FOR FULLY ACTUATED MECHANICAL SYSTEMS Francesco Bullo Richar M. Murray Control an Dynamical Systems California Institute of Technology Pasaena, CA 91125 Fax : + 1-818-796-8914 email
More informationExperimental Robustness Study of a Second-Order Sliding Mode Controller
Experimental Robustness Stuy of a Secon-Orer Sliing Moe Controller Anré Blom, Bram e Jager Einhoven University of Technology Department of Mechanical Engineering P.O. Box 513, 5600 MB Einhoven, The Netherlans
More informationNumerical Integrator. Graphics
1 Introuction CS229 Dynamics Hanout The question of the week is how owe write a ynamic simulator for particles, rigi boies, or an articulate character such as a human figure?" In their SIGGRPH course notes,
More informationCriteria for Global Stability of Coupled Systems with Application to Robust Output Feedback Design for Active Surge Control
Criteria for Global Stability of Couple Systems with Application to Robust Output Feeback Design for Active Surge Control Shiriaev, Anton; Johansson, Rolf; Robertsson, Aners; Freiovich, Leoni 9 Link to
More informationInterpolated Rigid-Body Motions and Robotics
Interpolate Rigi-Boy Motions an Robotics J.M. Selig Faculty of Business, Computing an Info. Management. Lonon South Bank University, Lonon SE AA, U.K. seligjm@lsbu.ac.uk Yaunquing Wu Dept. Mechanical Engineering.
More informationAutomatica. Composite adaptive control for Euler Lagrange systems with additive disturbances
Automatica 46 (21) 14 147 Contents lists available at ScienceDirect Automatica journal homepage: www.elsevier.com/locate/automatica Brief paper Composite aaptive control for Euler Lagrange systems with
More informationLaplacian Cooperative Attitude Control of Multiple Rigid Bodies
Laplacian Cooperative Attitue Control of Multiple Rigi Boies Dimos V. Dimarogonas, Panagiotis Tsiotras an Kostas J. Kyriakopoulos Abstract Motivate by the fact that linear controllers can stabilize the
More informationAdaptive Gain-Scheduled H Control of Linear Parameter-Varying Systems with Time-Delayed Elements
Aaptive Gain-Scheule H Control of Linear Parameter-Varying Systems with ime-delaye Elements Yoshihiko Miyasato he Institute of Statistical Mathematics 4-6-7 Minami-Azabu, Minato-ku, okyo 6-8569, Japan
More informationNonlinear Adaptive Ship Course Tracking Control Based on Backstepping and Nussbaum Gain
Nonlinear Aaptive Ship Course Tracking Control Base on Backstepping an Nussbaum Gain Jialu Du, Chen Guo Abstract A nonlinear aaptive controller combining aaptive Backstepping algorithm with Nussbaum gain
More informationGyroscopic matrices of the right beams and the discs
Titre : Matrice gyroscopique es poutres roites et es i[...] Date : 15/07/2014 Page : 1/16 Gyroscopic matrices of the right beams an the iscs Summary: This ocument presents the formulation of the matrices
More informationNeural Network Controller for Robotic Manipulator
MMAE54 Robotics- Class Project Paper Neural Network Controller for Robotic Manipulator Kai Qian Department of Biomeical Engineering, Illinois Institute of echnology, Chicago, IL 666 USA. Introuction Artificial
More informationIN the recent past, the use of vertical take-off and landing
IEEE TRANSACTIONS ON ROBOTICS, VOL. 27, NO. 1, FEBRUARY 2011 129 Aaptive Position Tracking of VTOL UAVs Anrew Roberts, Stuent Member, IEEE, an Abelhami Tayebi, Senior Member, IEEE Abstract An aaptive position-tracking
More informationDynamic Load Carrying Capacity of Spatial Cable Suspended Robot: Sliding Mode Control Approach
Int J Avance Design an Manufacturing echnology, Vol. 5/ No. 3/ June - 212 73 Dynamic Loa Carrying Capacity of Spatial Cable Suspene Robot: Sliing Moe Control Approach M. H. Korayem Department of Mechanical
More informationVisual Servoing for Underactuated VTOL UAVs : a Linear, Homography-Based Framework
Visual Servoing for Uneractuate VTOL UAVs : a Linear, Homography-Base Framework Henry e Plinval, Pascal Morin, Philippe Mouyon, Tarek Hamel H. e Plinval an P. Mouyon are with ONERA-The French Aerospace
More informationSome Remarks on the Boundedness and Convergence Properties of Smooth Sliding Mode Controllers
International Journal of Automation an Computing 6(2, May 2009, 154-158 DOI: 10.1007/s11633-009-0154-z Some Remarks on the Bouneness an Convergence Properties of Smooth Sliing Moe Controllers Wallace Moreira
More information739. Design of adaptive sliding mode control for spherical robot based on MR fluid actuator
739. Design of aaptive sliing moe control for spherical robot base on MR flui actuator M. Yue,, B. Y. Liu School of Automotive Engineering, Dalian University of echnology 604, Dalian, Liaoning province,
More informationTotal Energy Shaping of a Class of Underactuated Port-Hamiltonian Systems using a New Set of Closed-Loop Potential Shape Variables*
51st IEEE Conference on Decision an Control December 1-13 212. Maui Hawaii USA Total Energy Shaping of a Class of Uneractuate Port-Hamiltonian Systems using a New Set of Close-Loop Potential Shape Variables*
More informationRobust Adaptive Control for a Class of Systems with Deadzone Nonlinearity
Intelligent Control an Automation, 5, 6, -9 Publishe Online February 5 in SciRes. http://www.scirp.org/journal/ica http://x.oi.org/.436/ica.5.6 Robust Aaptive Control for a Class of Systems with Deazone
More informationVISUAL SERVOING WITH ORIENTATION LIMITS OF A X4-FLYER
VISUAL SERVOING WITH ORIENTATION LIMITS OF A X4-FLYER Najib Metni,Tarek Hamel,Isabelle Fantoni Laboratoire Central es Ponts et Chaussées, LCPC-Paris France, najib.metni@lcpc.fr Cemif-Sc FRE-CNRS 2494,
More informationIndirect Adaptive Fuzzy and Impulsive Control of Nonlinear Systems
International Journal of Automation an Computing 7(4), November 200, 484-49 DOI: 0007/s633-00-053-7 Inirect Aaptive Fuzzy an Impulsive Control of Nonlinear Systems Hai-Bo Jiang School of Mathematics, Yancheng
More informationDead Zone Model Based Adaptive Backstepping Control for a Class of Uncertain Saturated Systems
Milano (Italy) August - September, 11 Dea Zone Moel Base Aaptive Backstepping Control for a Class of Uncertain Saturate Systems Seyye Hossein Mousavi Alireza Khayatian School of Electrical an Computer
More informationShort Intro to Coordinate Transformation
Short Intro to Coorinate Transformation 1 A Vector A vector can basically be seen as an arrow in space pointing in a specific irection with a specific length. The following problem arises: How o we represent
More informationClemson University College of Engineering and Science Control and Robotics (CRB) Technical Report
Clemson University College of Engineering an Science Control an Robotics (CRB) Technical Report Number: CU/CRB/9/1/4/#1 Title: A Moular Controller for a Class of Uncertain MIMO Nonlinear Systems with Non-Symmetric
More informationFree rotation of a rigid body 1 D. E. Soper 2 University of Oregon Physics 611, Theoretical Mechanics 5 November 2012
Free rotation of a rigi boy 1 D. E. Soper 2 University of Oregon Physics 611, Theoretical Mechanics 5 November 2012 1 Introuction In this section, we escribe the motion of a rigi boy that is free to rotate
More information'HVLJQ &RQVLGHUDWLRQ LQ 0DWHULDO 6HOHFWLRQ 'HVLJQ 6HQVLWLYLW\,1752'8&7,21
Large amping in a structural material may be either esirable or unesirable, epening on the engineering application at han. For example, amping is a esirable property to the esigner concerne with limiting
More informationClemson University College of Engineering and Science Control and Robotics (CRB) Technical Report
Clemson University College of Engineering an Science Control an Robotics (CRB) Technical Report Number: CU/CRB/3/9/07/# Title: Aaptive Visual Servo Regulation Control for Camera-in-Han Configuration with
More informationChaos, Solitons and Fractals
Chaos, Solitons an Fractals xxx (00) xxx xxx Contents lists available at ScienceDirect Chaos, Solitons an Fractals journal homepage: www.elsevier.com/locate/chaos Impulsive stability of chaotic systems
More informationIEEE TRANSACTIONS ON AUTOMATIC CONTROL, VOL. XX, NO. XX, MONTH YEAR 1
IEEE TRANSACTIONS ON AUTOMATIC CONTROL, VOL. XX, NO. XX, MONTH YEAR 1 Non-linear complementary filters on the special orthogonal group Robert Mahony, Member, IEEE, Tarek Hamel, Member, IEEE, an Jean-Michel
More informationNOTES ON EULER-BOOLE SUMMATION (1) f (l 1) (n) f (l 1) (m) + ( 1)k 1 k! B k (y) f (k) (y) dy,
NOTES ON EULER-BOOLE SUMMATION JONATHAN M BORWEIN, NEIL J CALKIN, AND DANTE MANNA Abstract We stuy a connection between Euler-MacLaurin Summation an Boole Summation suggeste in an AMM note from 196, which
More information19 Eigenvalues, Eigenvectors, Ordinary Differential Equations, and Control
19 Eigenvalues, Eigenvectors, Orinary Differential Equations, an Control This section introuces eigenvalues an eigenvectors of a matrix, an iscusses the role of the eigenvalues in etermining the behavior
More informationOptimal LQR Control of Structures using Linear Modal Model
Optimal LQR Control of Structures using Linear Moal Moel I. Halperin,2, G. Agranovich an Y. Ribakov 2 Department of Electrical an Electronics Engineering 2 Department of Civil Engineering Faculty of Engineering,
More information12.5. Differentiation of vectors. Introduction. Prerequisites. Learning Outcomes
Differentiation of vectors 12.5 Introuction The area known as vector calculus is use to moel mathematically a vast range of engineering phenomena incluing electrostatics, electromagnetic fiels, air flow
More informationOn Using Unstable Electrohydraulic Valves for Control
Kailash Krishnaswamy Perry Y. Li Department of Mechanical Engineering, University of Minnesota, 111 Church St. SE, Minneapolis, MN 55455 e-mail: kk,pli @me.umn.eu On Using Unstable Electrohyraulic Valves
More informationContinuous observer design for nonlinear systems with sampled and delayed output measurements
Preprints of th9th Worl Congress The International Feeration of Automatic Control Continuous observer esign for nonlinear systems with sample an elaye output measurements Daoyuan Zhang Yanjun Shen Xiaohua
More informationarxiv: v1 [math.oc] 25 Nov 2017
Constraine Geometric Attitue Control on SO(3) Shankar Kulumani* an Taeyoung Lee November 8, 017 arxiv:17199v1 [math.oc] 5 Nov 017 Abstract This paper presents a new geometric aaptive control system with
More informationTime-of-Arrival Estimation in Non-Line-Of-Sight Environments
2 Conference on Information Sciences an Systems, The Johns Hopkins University, March 2, 2 Time-of-Arrival Estimation in Non-Line-Of-Sight Environments Sinan Gezici, Hisashi Kobayashi an H. Vincent Poor
More informationThis section outlines the methodology used to calculate the wave load and wave wind load values.
COMPUTERS AND STRUCTURES, INC., JUNE 2014 AUTOMATIC WAVE LOADS TECHNICAL NOTE CALCULATION O WAVE LOAD VALUES This section outlines the methoology use to calculate the wave loa an wave win loa values. Overview
More informationChapter 2 Lagrangian Modeling
Chapter 2 Lagrangian Moeling The basic laws of physics are use to moel every system whether it is electrical, mechanical, hyraulic, or any other energy omain. In mechanics, Newton s laws of motion provie
More informationOptimal CDMA Signatures: A Finite-Step Approach
Optimal CDMA Signatures: A Finite-Step Approach Joel A. Tropp Inst. for Comp. Engr. an Sci. (ICES) 1 University Station C000 Austin, TX 7871 jtropp@ices.utexas.eu Inerjit. S. Dhillon Dept. of Comp. Sci.
More informationRECENTLY, vertical take-off and landing (VTOL) unmanned
IEEE/CAA JOURNAL OF AUTOMATICA SINICA VOL. NO. JANUARY 5 65 Trajectory Tracking of Vertical Take-off an Laning Unmanne Aerial Vehicles Base on Disturbance Rejection Control Lu Wang an Jianbo Su Abstract
More informationBilateral Teleoperation of Multiple Cooperative Robots over Delayed Communication Networks: Application
Proceeings of the 5 IEEE International Conference on Robotics an Automation Barcelona, Spain, April 5 Bilateral Teleoperation of Multiple Cooperative Robots over Delaye Communication Networks: Application
More informationAdaptive Optimal Path Following for High Wind Flights
Milano (Italy) August - September, 11 Aaptive Optimal Path Following for High Win Flights Ashwini Ratnoo P.B. Sujit Mangal Kothari Postoctoral Fellow, Department of Aerospace Engineering, Technion-Israel
More informationNonlinear Tracking Control of Underactuated Surface Vessel
American Control Conference June -. Portland OR USA FrB. Nonlinear Tracking Control of Underactuated Surface Vessel Wenjie Dong and Yi Guo Abstract We consider in this paper the tracking control problem
More informationJUST THE MATHS UNIT NUMBER DIFFERENTIATION 2 (Rates of change) A.J.Hobson
JUST THE MATHS UNIT NUMBER 10.2 DIFFERENTIATION 2 (Rates of change) by A.J.Hobson 10.2.1 Introuction 10.2.2 Average rates of change 10.2.3 Instantaneous rates of change 10.2.4 Derivatives 10.2.5 Exercises
More informationStability-Guaranteed Impedance Control of Hydraulic Robotic Manipulators
Tampere University o Technology Stability-Guarantee Impeance Control o Hyraulic Robotic Manipulators Citation Koivumäki, J., & Mattila, J. (217). Stability-Guarantee Impeance Control o Hyraulic Robotic
More informationDistributed Force/Position Consensus Tracking of Networked Robotic Manipulators
180 IEEE/CAA JOURNAL OF AUTOMATICA SINICA, VOL. 1, NO. 2, APRIL 2014 Distribute Force/Position Consensus Tracking of Networke Robotic Manipulators Lijiao Wang Bin Meng Abstract In this paper, we aress
More informationTRACKING CONTROL OF MULTIPLE MOBILE ROBOTS: A CASE STUDY OF INTER-ROBOT COLLISION-FREE PROBLEM
265 Asian Journal of Control, Vol. 4, No. 3, pp. 265-273, September 22 TRACKING CONTROL OF MULTIPLE MOBILE ROBOTS: A CASE STUDY OF INTER-ROBOT COLLISION-FREE PROBLEM Jurachart Jongusuk an Tsutomu Mita
More informationInvariant Extended Kalman Filter: Theory and application to a velocity-aided estimation problem
Invariant Extene Kalman Filter: Theory an application to a velocity-aie estimation problem S. Bonnabel (Mines ParisTech) Joint work with P. Martin (Mines ParisTech) E. Salaun (Georgia Institute of Technology)
More informationA new approach to explicit MPC using self-optimizing control
28 American Control Conference Westin Seattle Hotel, Seattle, Washington, USA June -3, 28 WeA3.2 A new approach to explicit MPC using self-optimizing control Henrik Manum, Sriharakumar Narasimhan an Sigur
More informationShared Control Between Adaptive Autopilots and Human Operators for Anomaly Mitigation
Share Control Between Aaptive Autopilots an Human Operators for Anomaly Mitigation Benjamin T. Thomsen Anuraha M. Annaswamy Eugene Lavretsky Massachusetts Institute of Technology, Cambrige, MA 02139 The
More informationVectors in two dimensions
Vectors in two imensions Until now, we have been working in one imension only The main reason for this is to become familiar with the main physical ieas like Newton s secon law, without the aitional complication
More informationThe canonical controllers and regular interconnection
Systems & Control Letters ( www.elsevier.com/locate/sysconle The canonical controllers an regular interconnection A.A. Julius a,, J.C. Willems b, M.N. Belur c, H.L. Trentelman a Department of Applie Mathematics,
More informationAttitude Control System Design of UAV Guo Li1, a, Xiaoliang Lv2, b, Yongqing Zeng3, c
4th National Conference on Electrical, Electronics an Computer Engineering (NCEECE 205) Attitue Control ystem Design of UAV Guo Li, a, Xiaoliang Lv2, b, Yongqing eng3, c Automation chool, University of
More informationDesign A Robust Power System Stabilizer on SMIB Using Lyapunov Theory
Design A Robust Power System Stabilizer on SMIB Using Lyapunov Theory Yin Li, Stuent Member, IEEE, Lingling Fan, Senior Member, IEEE Abstract This paper proposes a robust power system stabilizer (PSS)
More informationRobust Forward Algorithms via PAC-Bayes and Laplace Distributions. ω Q. Pr (y(ω x) < 0) = Pr A k
A Proof of Lemma 2 B Proof of Lemma 3 Proof: Since the support of LL istributions is R, two such istributions are equivalent absolutely continuous with respect to each other an the ivergence is well-efine
More informationSeparation Principle for a Class of Nonlinear Feedback Systems Augmented with Observers
Proceeings of the 17th Worl Congress The International Feeration of Automatic Control Separation Principle for a Class of Nonlinear Feeback Systems Augmente with Observers A. Shiriaev, R. Johansson A.
More informationFORMATION INPUT-TO-STATE STABILITY. Herbert G. Tanner and George J. Pappas
Copyright 2002 IFAC 5th Triennial Worl Congress, Barcelona, Spain FORMATION INPUT-TO-STATE STABILITY Herbert G. Tanner an George J. Pappas Department of Electrical Engineering University of Pennsylvania
More informationPractical implementation of Differential Flatness concept for quadrotor trajectory control
Practical implementation of Differential Flatness concept for quarotor trajectory control Abhishek Manjunath 1 an Parwiner Singh Mehrok 2 Abstract This report ocuments how the concept of Differential Flatness
More informationAdaptive Robust Control: A Piecewise Lyapunov Function Approach
Aaptive Robust Control: A Piecewise Lyapunov Function Approach Jianming Lian, Jianghai Hu an Stanislaw H. Żak Abstract The problem of output tracking control for a class of multi-input multi-output uncertain
More informationPROPORTIONAL DERIVATIVE (PD) CONTROL ON THE EUCLIDEAN GROUP F. BULLO AND R. M. MURRAY. Division of Engineering and Applied Science
PROPORTIONAL DERIVATIVE (PD) CONTROL ON THE EUCLIDEAN GROUP F. BULLO AND R. M. MURRAY Division of Engineering an Applie Science California Institute of Technology Pasaena, CA 95 CDS Technical Report 95-
More informationEuler equations for multiple integrals
Euler equations for multiple integrals January 22, 2013 Contents 1 Reminer of multivariable calculus 2 1.1 Vector ifferentiation......................... 2 1.2 Matrix ifferentiation........................
More informationTime-Optimal Motion Control of Piezoelectric Actuator: STM Application
Time-Optimal Motion Control of Piezoelectric Actuator: STM Application Yongai Xu, Peter H. Mecl Abstract This paper exaes the problem of time-optimal motion control in the context of Scanning Tunneling
More informationChapter 6: Energy-Momentum Tensors
49 Chapter 6: Energy-Momentum Tensors This chapter outlines the general theory of energy an momentum conservation in terms of energy-momentum tensors, then applies these ieas to the case of Bohm's moel.
More informationDynamics of the synchronous machine
ELEC0047 - Power system ynamics, control an stability Dynamics of the synchronous machine Thierry Van Cutsem t.vancutsem@ulg.ac.be www.montefiore.ulg.ac.be/~vct These slies follow those presente in course
More informationOn the Feedback Linearization of Robots with Variable Joint Stiffness
8 IEEE International Conference on Robotics an Automation Pasaena, CA, USA, May 19-3, 8 On the Feeback Linearization of Robots with Variable Joint Stiffness G. Palli an C. Melchiorri Dipartimento i Elettronica,
More informationSwitching Time Optimization in Discretized Hybrid Dynamical Systems
Switching Time Optimization in Discretize Hybri Dynamical Systems Kathrin Flaßkamp, To Murphey, an Sina Ober-Blöbaum Abstract Switching time optimization (STO) arises in systems that have a finite set
More informationMath 342 Partial Differential Equations «Viktor Grigoryan
Math 342 Partial Differential Equations «Viktor Grigoryan 6 Wave equation: solution In this lecture we will solve the wave equation on the entire real line x R. This correspons to a string of infinite
More informationDesign of an Industrial Distributed Controller Near Spatial Domain Boundaries
Design of an Inustrial Distribute Controller Near Spatial Domain Bounaries Stevo Mijanovic, Greg E. Stewart, Guy A. Dumont, an Michael S. Davies ABSTRACT This paper proposes moifications to an inustrial
More informationFeedback-Linearizing Control for Velocity and Attitude Tracking of an ROV with Thruster Dynamics Containing Input Dead Zones
Feeback-Linearizing Control for Velocity an Attitue Tracking of an ROV with Thruster Dynamics Containing Input Dea Zones Joran Boehm 1, Eric Berkenpas 2, Charles Shepar 3, an Derek A. Paley 4 Abstract
More informationVariation-based Linearization of Nonlinear Systems Evolving on SO(3) and S 2
Variation-base Linearization of Nonlinear Systems Evolving on SO(3) an S 2 Guofan Wu an Koushil Sreenath Abstract In this paper, we propose a variation-base metho to linearize the nonlinear ynamics of
More informationensembles When working with density operators, we can use this connection to define a generalized Bloch vector: v x Tr x, v y Tr y
Ph195a lecture notes, 1/3/01 Density operators for spin- 1 ensembles So far in our iscussion of spin- 1 systems, we have restricte our attention to the case of pure states an Hamiltonian evolution. Toay
More informationAdaptive Congestion Control in ATM Networks
Aaptive Congestion Control in ATM Networks Farza Habibipour, Mehi Galily, Masou Faris, Ali Yazian Iran Telecounication Research Center, Ministry of ICT, Tehran, IRAN habibipor@itrc.ac.ir Abstract. In this
More informationNON-SMOOTH DYNAMICS USING DIFFERENTIAL-ALGEBRAIC EQUATIONS PERSPECTIVE: MODELING AND NUMERICAL SOLUTIONS. A Thesis PRIYANKA GOTIKA
NON-SMOOTH DYNAMICS USING DIFFERENTIAL-ALGEBRAIC EQUATIONS PERSPECTIVE: MODELING AND NUMERICAL SOLUTIONS A Thesis by PRIYANKA GOTIKA Submitte to the Office of Grauate Stuies of Texas A&M University in
More informationConservation Laws. Chapter Conservation of Energy
20 Chapter 3 Conservation Laws In orer to check the physical consistency of the above set of equations governing Maxwell-Lorentz electroynamics [(2.10) an (2.12) or (1.65) an (1.68)], we examine the action
More informationA global Implicit Function Theorem without initial point and its applications to control of non-affine systems of high dimensions
J. Math. Anal. Appl. 313 (2006) 251 261 www.elsevier.com/locate/jmaa A global Implicit Function Theorem without initial point an its applications to control of non-affine systems of high imensions Weinian
More informationUniversity of Bristol - Explore Bristol Research. Peer reviewed version. Link to published version (if available): /CONTROL.2016.
Yang, R., Yang, C., Chen, M., & Na, J. (16). RBFNN base aaptive control of uncertain robot manipulators in iscrete time. In 16 UKACC 11th International Conference on Control (CONTROL 16): Proceeings of
More informationPhysics 251 Results for Matrix Exponentials Spring 2017
Physics 25 Results for Matrix Exponentials Spring 27. Properties of the Matrix Exponential Let A be a real or complex n n matrix. The exponential of A is efine via its Taylor series, e A A n = I + n!,
More informationSTABILITY CONTROL FOR SIX-WHEEL DRIVE ARTICULATED VEHICLE BASED ON DIRECT YAW MOMENT CONTROL METHOD
STABILITY CONTROL FOR SIX-WHEEL DRIVE ARTICULATED VEHICLE BASED ON DIRECT YAW MOMENT CONTROL METHOD 1 YITING KANG, 2 WENMING ZHANG 1 Doctoral Caniate, School of Mechanical Engineering, University of Science
More informationTEMPORAL AND TIME-FREQUENCY CORRELATION-BASED BLIND SOURCE SEPARATION METHODS. Yannick DEVILLE
TEMPORAL AND TIME-FREQUENCY CORRELATION-BASED BLIND SOURCE SEPARATION METHODS Yannick DEVILLE Université Paul Sabatier Laboratoire Acoustique, Métrologie, Instrumentation Bât. 3RB2, 8 Route e Narbonne,
More informationImplicit Lyapunov control of closed quantum systems
Joint 48th IEEE Conference on Decision an Control an 28th Chinese Control Conference Shanghai, P.R. China, December 16-18, 29 ThAIn1.4 Implicit Lyapunov control of close quantum systems Shouwei Zhao, Hai
More informationSemi passive walking of a 7 DOF biped robot ABSTRACT 1 INTRODUCTION
Semi passive walking of a 7 DOF bipe robot N.Khraief & N.K.M Siri khraief@lrv.uvsq.fr, nkms@free.fr Laboratoire e Robotique e Versailles Université e Versailles Saint Quentin en Yvelines 0, Avenue e l
More informationTHE VAN KAMPEN EXPANSION FOR LINKED DUFFING LINEAR OSCILLATORS EXCITED BY COLORED NOISE
Journal of Soun an Vibration (1996) 191(3), 397 414 THE VAN KAMPEN EXPANSION FOR LINKED DUFFING LINEAR OSCILLATORS EXCITED BY COLORED NOISE E. M. WEINSTEIN Galaxy Scientific Corporation, 2500 English Creek
More information6 General properties of an autonomous system of two first order ODE
6 General properties of an autonomous system of two first orer ODE Here we embark on stuying the autonomous system of two first orer ifferential equations of the form ẋ 1 = f 1 (, x 2 ), ẋ 2 = f 2 (, x
More informationTOTAL ENERGY SHAPING CONTROL OF MECHANICAL SYSTEMS: SIMPLIFYING THE MATCHING EQUATIONS VIA COORDINATE CHANGES
TOTAL ENERGY SHAPING CONTROL OF MECHANICAL SYSTEMS: SIMPLIFYING THE MATCHING EQUATIONS VIA COORDINATE CHANGES Giuseppe Viola,1 Romeo Ortega,2 Ravi Banavar Jose Angel Acosta,3 Alessanro Astolfi, Dipartimento
More informationSliding mode approach to congestion control in connection-oriented communication networks
JOURNAL OF APPLIED COMPUTER SCIENCE Vol. xx. No xx (200x), pp. xx-xx Sliing moe approach to congestion control in connection-oriente communication networks Anrzej Bartoszewicz, Justyna Żuk Technical University
More informationStable and compact finite difference schemes
Center for Turbulence Research Annual Research Briefs 2006 2 Stable an compact finite ifference schemes By K. Mattsson, M. Svär AND M. Shoeybi. Motivation an objectives Compact secon erivatives have long
More informationDamage identification based on incomplete modal data and constrained nonlinear multivariable function
Journal of Physics: Conference Series PAPER OPEN ACCESS Damage ientification base on incomplete moal ata an constraine nonlinear multivariable function To cite this article: S S Kourehli 215 J. Phys.:
More informationLecture 2 Lagrangian formulation of classical mechanics Mechanics
Lecture Lagrangian formulation of classical mechanics 70.00 Mechanics Principle of stationary action MATH-GA To specify a motion uniquely in classical mechanics, it suffices to give, at some time t 0,
More informationAll s Well That Ends Well: Supplementary Proofs
All s Well That Ens Well: Guarantee Resolution of Simultaneous Rigi Boy Impact 1:1 All s Well That Ens Well: Supplementary Proofs This ocument complements the paper All s Well That Ens Well: Guarantee
More informationConnections Between Duality in Control Theory and
Connections Between Duality in Control heory an Convex Optimization V. Balakrishnan 1 an L. Vanenberghe 2 Abstract Several important problems in control theory can be reformulate as convex optimization
More informationRobust Observer-Based Control of an Aluminum Strip Processing Line
IEEE TRANSACTIONS ON INDUSTRY APPLICATIONS, VOL. 36, NO. 3, MAY/UNE 2 865 Robust Observer-Base Control of an Aluminum Strip Processing Line Prabhakar R. Pagilla, Member, IEEE, Eugene O. King, Member, IEEE,
More informationMultirate Feedforward Control with State Trajectory Generation based on Time Axis Reversal for Plant with Continuous Time Unstable Zeros
Multirate Feeforwar Control with State Trajectory Generation base on Time Axis Reversal for with Continuous Time Unstable Zeros Wataru Ohnishi, Hiroshi Fujimoto Abstract with unstable zeros is known as
More informationRobustness of the Moore-Greitzer Compressor Model s Surge Subsystem with New Dynamic Output Feedback Controllers
Preprints of the 19th Worl Congress The International Feeration of Automatic Control Cape Town, South Africa. August 4-9, 14 Robustness of the Moore-Greiter Compressor Moel s Surge Subsystem with New Dynamic
More informationLecture 27: Generalized Coordinates and Lagrange s Equations of Motion
Lecture 27: Generalize Coorinates an Lagrange s Equations of Motion Calculating T an V in terms of generalize coorinates. Example: Penulum attache to a movable support 6 Cartesian Coorinates: (X, Y, Z)
More informationDynamic Constraint-based Optimal Shape Trajectory Planner for Shape-Accelerated Underactuated Balancing Systems
Dynamic Constraint-base Optimal Shape Trajectory Planner for Shape-Accelerate Uneractuate Balancing Systems Umashankar Nagarajan The Robotics Institute Carnegie Mellon University Pittsburgh, PA 53 Email:
More information