On the Error Modeling of a Novel Mobile Hybrid Parallel Robot
|
|
- Joel Lambert
- 6 years ago
- Views:
Transcription
1 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. Box 2, FIN-8 Lappeenranta, Fnlan ongbo.wang@lut.f, huapeng.wu@lut.f, hekk.hanroos@lut.f Abstract hs paper presents a metho for the knematc analss an error moelng of a newl evelope hbr reunant robot IWR (Intersector Welng Robot), whch possesses ten egrees of freeom (DOF) where -DOF n parallel an atonal -DOF n seral. In ths artcle, the problem of knematc moelng an error moelng of the propose IWR robot are scusse. Base on the vector arthmetc metho, the knematc moel an the senstvt moel of the en-effector subject to the structure parameters s erve an analze. he relatons between the pose (poston an orentaton) accurac an manufacturng tolerances, actuaton errors, an connecton errors are formulate. Smulaton s performe to examne the valt an effectveness of the evolutonar algorthm for the applcaton. Kewors accurac, error moelng, parallel robot, knematc analss I. INRODUCION Accurac s an utmost mportant conseraton factor when esgn a robot, whatever t s a seral robot or parallel robot. It s beleve that parallel robot have some favorable avantages, such as hgher spees an acceleratons, compact structure, an mprove accurac because the jont errors are not accumulate lke n ts counterpart. On the other han, seral robots have some avantages lke larger workspace, hgher extert an goo maneuverablt but exhbt low stffness an poor postonng accurac because of ther seral structures. o take avantage both of ther merts, n ths paper, a reunant hbr robot whch possesses both seral an parallel lnks wll be ntrouce, the seral part of the machne s use to prove bg work volume, whle parallel lnks brng hgh loang capabltes an stffness to the whole structure [], thus a promsng compromse of best ses of parallel knematcs an seral robots mght be acheve. In the paper, base on the fferentaton algorthm metho, the error moel of the propose robot wll be formulate. In the past ecaes, there are a number of publcatons concernng the seral robots an parallel robots respectvel. For the Hexapo, Wang an Masor [2] nvestgate how manufacturng an assembl errors affect the accurac of a Hexapo b moelng the legs as seral knematc chans usng the D-H conventon. Ropponen an Ara [] presente an error moel base on fferentaton of the knematcs. For the seral robot, Vetschegger an Ch-haur Wu [] evelope a lnear error moel to etermne the Cartesan poston an orentaton (2) Department of Mechancal Engneerng SLM, Chongqng Unverst Shapngba, Chongqng,, PR. Chna accurac of a robot manpulator wth respect to the statstcal strbutons of the knematcs parameters. However, ver few publcatons ealng wth hbr robot have been foun,.-w Zhao an K.-C Fan [] llustrate a seral-parallel tpe machne tool an evaluate ts accurac base on the lnkage knematc analss an the fferental vector metho. he paper s organze nto four man sectons. he frst secton serves as ntroucton. he secon secton revews the knematc analss an error moelng of the propose robot. Smulaton results are presente n the thr secton, an conclusons are rawn n the fourth secton. II. KINEMAIC ANALYSIS AND ERROR MODELING he knematcs of the propose hbr robot as shown n Fg. can be ve nto two parts, the seral part an the parallel one,.e., the carrage an Hexapo. o smplf ts analss, the two parts wll be frst carre out respectvel, an then combne them together to obtan the fnal solutons. Fgure. D moel of IWR A. error moelng of the carrage Base on the conventon of Denavt-Hartenberg coornate sstem, the prncple of the -DOF carrage mechansm s establshe n Fg.2, whch proves four egrees of freeom at the en-effector, nclung two translatonal movements an two rotatonal movements /8 /$2. 28 IEEE RAM 28
2 p = a sθ a sθ cθ () 2 p = + a cθ + a cθ cθ () z he nverse knematc moel can be obtane as θ = sn p a a x () = p acθ acθ cθ (7) z = p asθ a sθ cθ (8) 2 Fgure 2. Coornate sstem of carrage Usng the coornate sstems establshe n Fg. 2, the corresponng lnk parameters are gven n able. Substtutng the D-H lnk parameters nto (), we can obtan the D-H homogeneous transformaton matrces A, A, 2 A an A. 2 ABLE I. ont D-H PARAMEERS OF CARRIAGE α a θ π /2 a 2 π /2 2 π /2 π /2 a θ π /2 a θ cθ cα sθ sα sθ a cθ sθ cα cθ sα cθ a sθ A = () sα cα where cθ enotes cosθ, an sθ enotes snθ. he resultng homogeneous transformaton matrx can be obtane b multplng the matrces of A, A, 2 A an A. 2 A = A A A A sθ cθ a + + asθ sθ cθ cθ sθ sθ a sθ a sθ cθ = cθcθ sθ cθsθ + acθ + acθcθ Base on (2), the forwar knematcs can be wrtten as follows (2) p = a + + a sθ () x For the accurac of the carrage, t epens on the accurac of the four-lnk parameters of each jont []. If there are errors n the mensonal relatonshps between two consecutve jont an, there wll be a fferental change A between the two jont coornates. herefore, the correct relatonshp between the two successve jont coornates wll be wrtten as A = A + A (9) c where A s the homogeneous matrx whch have the nomnal lnk parameters that can express the relatonshp between the jont coornates an, an A s the fferental change ue to errors n the lnk parameters. It can be approxmate as a lnear functon of four knematcs errors b alor s seres: A A A A A a () = θ α θ a α where θ,, a, an α are small errors n the knematc parameters an the partal ervatves are evaluate wth the nomnal geometrcal lnk parameters. From (), takng the partal ervatve wth respect to θ,, a, an α respectvel, we can obtan A θ sθ cθ cα cθ s α a sθ cθ sθ cα sθ s α acθ =, an A A A,, can be solve n the same wa. a α Let A = A δ A, an A D D D D () δ = θ + + a + α θ a α
3 where D, D, D, D can be solve as follows: a α θ cα sα cα ac α A Dθ = ( A ) =, an θ sα asα D, D, D can be got n the same wa (2) a α Expanng () nto matrx form we can obtan an = [ θ a α ], acoban matrx. G s the entfcaton B. Knematc analss an error moelng of Hexapo Fg. shows a schematc agram of hexapo parallel mechansm, for the purpose of analss, two Cartesan coornate sstems, frames O (X, Y, Z ) an O (X, Y, Z ) are attache to the base plate an the en-effector, respectvel. Sx varable lmbs are connecte wth the base plate b Unversal jonts an the task platform b Sphercal jonts. cα θ sα θ a cα θ α ac α θ + sα δ A = () sα θ α asα θ + cα he above expresson gves the fferental translaton an rotaton vectors for an tpe of jont as functons of the four D- H knematc errors. Smlarl, for the propose four egree-of-freeom carrage, the correct poston an orentaton of the task pont p wth respect to the base frame ue to the knematc errors can be expresse as c = + = + = A A A ( A A ) () Expanng (), an gnorng secon an hgher-orer fferental errors, then the relaton between the fferental change n carrage an the change n lnk parameters can be erve as, ([ ] [ ] ) = A = δa A δa = A δ A A () where δ A s the frst orer error matrx transformaton n the fxe base frame. Followng Paul [7], such a fferental operator has the followng form δθz δθ δ x δθz δθ x δ δ = δθ δθx δ z () If let δ X = δ δ δ δθ δθ δθ R x z x z enote the postonal an the orentaton errors of the carrage, then from () an (), t can also be rewrtten as: ( ) δ X = x = G (7) = = where x = [ δ x δ δ z δθ x δθ δθ z ] Fgure. Normnal moel of the Hexapo parallel mechansm For the esgne knematcs parameters, the followng vector-loop equaton represents the knematcs of the th lmb of the manpulator AB = P + R b a (ι=,2,,,, ) (8) where P enotes the poston vector of the task frame {} wth respect to the base frame {}, an R s the Z-Y-X Euler transformaton matrx expressng the orentaton of the frame {} relatve to the frame {}, cα cβ cα sβsγ sα cγ cα sβcγ + sα sγ sα cβ sα sβsγ cαcλ sαsβcγ cα sγ R = + (9) sβ cβsγ cβcγ an the a, b represent the poston vectors of U-jonts A an S-jonts B n the coornate frames {} an {} respectvel. Let l be the unt vector n the recton of AB, an l represents the magntue of the leg vector AB. Dfferentatng both ses of (8) wll el δll + lδl = δ P + δ R b + R δ b δ a (=,2,..., ) (2)
4 Let R b = s, an multpl both ses of (2) wth the unt recton vector l, snce l l =, l δ l = we can obtan: δl = l δ P + l δ Ω s + l R δ b l δ a ( ) = l δ P + s l Ω + l R δ b l δ a δ P δ a l ( s l ) l l R δ Ω δ b = + (2) Equaton (2) can be rewrtten as δl = δx + δp (22) 2 where [ l, l, l, l, l, l ] δl = δ δ δ δ δ δ R (2) 2 an 2 ( l l R ) l ( s l ) (2) l ( s l ) = R = R ( l l R ) (2) P = a b R ι=,2,..., (2) δ δ δ Snce R s a square matrx, an no sngular ponts exst nse the workspace [], s nvertble. herefore, (22) can be wrtten as: = 2 δx δl δp (27) he frst term on the rght se represents the errors nuce b actuators an the secon one s the poston errors from the passve jonts A an B. C. Knematc analss an error moelng of the hbr manpulator he schematc agram of the reunant hbr manpulator s shown n Fg., whch s a combnaton of carrage an Hexapo manpulator mentone above. he base plate frame {} of Hexapo s conce wth the en task frame of the carrage. he global base frame {} s locate at the left ral. Fgure. Schematc agram of IWR Accorng to the geometr, a vector-loop equaton can be erve as P = P + R P = P + R ( l l + a R b ) = P + R l l + R a R b (28) where P s the poston vector of the task frame {} (or eneffector) wth respect to the fxe base frame {}, an R s the rotaton matrx of the frame {} wth respect to frame {}. Dfferentatng both ses of (28) an multplng unt recton vector l els ( r δ P δ ) = P ( r ) + ( l ) Ω Ω (29) l b l l a l R l l δ δ δ a l R l δl l R l R δ b + + where r b = R b, r a = R a where Equaton (29) can be rewrtten as δx = δx + δ L + δp () ( r l ) = l ( rb l) l b R ()
5 l l R l l = l ( ra l ) + ( l R l l ) ( ra ) + ( l ) R (2) l R l = R l R l ( l R l R ) = R ( l R l R ) () () Fgure. Poston error of carrage n X, Y, an Z Snce R s a square matrx, an no sngular ponts exst nse the workspace, s nvertble. herefore, () can be rewrtten as: δx = δx + δl + δp () where δ X = δ P δ Ω R enote the fnal output pose errors, an the frst term on the rght s the errors cause b the carrage, the secon an thr one represent the errors nuce b the Hexapo machensm. III. SIMULAIONS RESULS In orer to evaluate the fnal output errors cause b the error sources, a smulaton example was performe usng the followng nomnal parameters. a = 28 mm, b = mm, a = 9 mm, a2 =, a = 22 mma, = mm ; = mm, = Moreover, to estmate the accurac of the erve error moel, we assume a certan knematcs errors occurre n the carrage an Hexapo δl =. mm, δp =.mm α = θ =. ; a = =.mm he range of the actuator nput values are gven n below, whch wll be generate b the ranom functon n Matlab. he output poston errors an orentaton errors of the carrage, Hexapo an the whole robot n X, Y an Z recton for the ranom generate poses are shown n Fgure,, 7, 8,9, respectvel. Fgure an Fgure 2 llustrate the comparson of the absolute poston an orentaton error of carrage, Hexapo an the whole robot. Fgure. Orentaton error of carrage n X, Y, an Z Fgure 7. Poston error of Hexapo n X, Y, an Z Fgure 8. Orentaton error of Hexapo n X, Y, an Z < < 8 mm, < < mm, < θ < 8, 2 < θ < 9, < α <, < β <, < γ <.
6 fnal output errors are not smpl the superposton of the carrage an Hexapo. Comparng the absolute poston an orentaton errors of the carrage, Hexapo an IWR, we can see that the carrage error s the most mportant error sources to the fnal output errors, whch causes about 8% of the whole errors. he fnal poston errors are not greater than mm, whch can be reuce to satsf the accurac requrement b means of some calbraton methos n next step. Fgure 9. Poston error of IWR n X, Y, an Z Fgure. Orentaton error of IWR n X, Y, an Z IV. CONCLUSIONS In ths paper, a hbr reunant robot use for both machnng an assemblng of Vacuum Vessel of IER s ntrouce. An error moel erve for the propose robot has the ablt to account for the statc sources of errors. Due to the reunant freeom of the robot, frst we ve t nto seral part an parallel part, an then formulate the error moel respectvel, fnall combne them together to get the fnal error moel. he error moel has been smulate n Matlab an the results show that about 8% amount of errors n the eneffector s cause b seral lnk mechansm,.e. carrage. In practce, to obtan esre accurac of robot, these errors have to be reuce b further parameter entfcaton methos. In the followng work, efforts wll be focuse on the parameter entfcaton usng some optmzaton metho to obtan esrable output errors. ACKNOWLEDGEMENS hs work, supporte b the European communtes uner the contract of assocaton between EURAOM an Fnnsh ekes, was carre out wthn the framework of the European Fuson evelopment Agreement. Authors from SLM n Chna are grateful to the IMVE n Fnlan for the use of ts research facltes an successful collaboraton an Chna Scholarshp Councl for the partal fnancal support. REFERENCES Fgure. Comparson of the absolute poston error of carrage, Hexapo an IWR [] Huapeng Wu, Hekk Hanroos, Pekka Pess, uha Klkk, Lawrence ones, Development an control towars a parallel water hraulc wel/cut for machnng processes n IER vacuum vessel. Int.. fuson Engneerng an Desgn, Vol. 7-79, pp. 2-, 2. [2]. Wang an O. Masor, On the accurac of a Hexapo part I he effect of manufacturng tolerances. IEEE Conf. on Robotcs an Automaton, pp. -2, 99 [].Ropponen..Ara, Accurac Analss of a Mofe Hexapo Manpulator. IEEE Conf. on Robotcs an Automaton, pp. 2-2, 99 [] W.K. Vetschegger, Ch-Haur Wu, Robot analss base on knematcs. IEEE. Robotcs an Automaton, Vol. RA-2,NO., pp. 7-79, september, 98 [] Lung-Wen sa, Robot Analss- the Mechancs of Seral an Parallel Manpulators. Wle & Sons, New York, 2. [].-W Zhao, K.-C Fan,.-H Chang an Z. L, Error analss of a seralparallel tpe machne tool, Int Av Manuf echnol, Vol. 9, pp. 7-79, 22 [7] R.P.Paul, Robot Manpulators:Mathematcs, Programmng, an Control, he MI Press, Cambrge, MA, 982. Fgure 2. Comparson of the absolute orentaton error of carrage, Hexapo an IWR From these Fgures t can be seen that the errors along Z axs are nfluence sgnfcantl than that of X, Y axes, an the
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 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 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 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 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 informationT f. Geometry. R f. R i. Homogeneous transformation. y x. P f. f 000. Homogeneous transformation matrix. R (A): Orientation P : Position
Homogeneous transformaton Geometr T f R f R T f Homogeneous transformaton matr Unverst of Genova T f Phlppe Martnet = R f 000 P f 1 R (A): Orentaton P : Poston 123 Modelng and Control of Manpulator robots
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 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 informationNMT EE 589 & UNM ME 482/582 ROBOT ENGINEERING. Dr. Stephen Bruder NMT EE 589 & UNM ME 482/582
NMT EE 589 & UNM ME 482/582 ROBOT ENGINEERING Dr. Stephen Bruder NMT EE 589 & UNM ME 482/582 4. Moton Knematcs 4.2 Angular Velocty Knematcs Summary From the last lecture we concluded that: If the jonts
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 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 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 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 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 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 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 informationAccuracy Analysis of General Parallel Manipulators with Joint Clearance
007 IEEE Internatonal Conference on Robotcs and Automaton Roma, Italy, 10-14 Aprl 007 WeC6. Accuracy Analyss of General Parallel Manpulators wth Jont Clearance Jan Meng, ongjun Zhang, Tnghua Zhang, Hong
More informationIn this section is given an overview of the common elasticity models.
Secton 4.1 4.1 Elastc Solds In ths secton s gven an overvew of the common elastcty models. 4.1.1 The Lnear Elastc Sold The classcal Lnear Elastc model, or Hooean model, has the followng lnear relatonshp
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 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 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 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 informationA New Concept of Modular Parallel Mechanism for Machining Applications
Submtted to ICRA A New Concept of Modular arallel Mechansm for Machnng Applcatons Damen Chablat and hlppe Wenger Insttut de Recherche en Communcatons et Cybernétque de Nantes, rue de la Noë, 44 Nantes,
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 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 informationMAE140 - Linear Circuits - Winter 16 Midterm, February 5
Instructons ME140 - Lnear Crcuts - Wnter 16 Mdterm, February 5 () Ths exam s open book. You may use whatever wrtten materals you choose, ncludng your class notes and textbook. You may use a hand calculator
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 informationThe Optimal Design of Three Degree-of-Freedom Parallel Mechanisms for Machining Applications
Submtted to ICAR D. Chablat h. Wenger F. Majou he Optmal Desgn of hree Degree-of-Freedom arallel Mechansms for Machnng Applcatons Damen Chablat - hlppe Wenger Félx Majou Insttut de Recherche en Communcatons
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 informationHuman Placement for Maximum Dexterity
Human Placement for Maxmum Dexterty Karm Abdel-Malek and We u Department of Mechancal Engneerng The Unversty of Iowa Iowa Cty, IA 52242 Tel. (319) 335-5676 amalek@engneerng.uowa.edu wyu@engneerng.uowa.edu
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 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 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 informationDARWIN-OP HUMANOID ROBOT KINEMATICS. Robert L. Williams II, Ph.D., Mechanical Engineering, Ohio University, Athens, Ohio, USA
Proceedngs of the ASME 1 Internatonal Desgn Engneerng Techncal onferences & omputers and Informaton n Engneerng onference IDET/IE 1 August 1-15, 1, hcago, IL, USA DET1-765 DARWIN-OP HUMANOID ROBOT KINEMATIS
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 informationMAE140 - Linear Circuits - Winter 16 Final, March 16, 2016
ME140 - Lnear rcuts - Wnter 16 Fnal, March 16, 2016 Instructons () The exam s open book. You may use your class notes and textbook. You may use a hand calculator wth no communcaton capabltes. () You have
More informationLectures - Week 4 Matrix norms, Conditioning, Vector Spaces, Linear Independence, Spanning sets and Basis, Null space and Range of a Matrix
Lectures - Week 4 Matrx norms, Condtonng, Vector Spaces, Lnear Independence, Spannng sets and Bass, Null space and Range of a Matrx Matrx Norms Now we turn to assocatng a number to each matrx. We could
More informationMechanics Physics 151
Mechancs Physcs 5 Lecture 3 Contnuous Systems an Fels (Chapter 3) Where Are We Now? We ve fnshe all the essentals Fnal wll cover Lectures through Last two lectures: Classcal Fel Theory Start wth wave equatons
More informationSection 8.3 Polar Form of Complex Numbers
80 Chapter 8 Secton 8 Polar Form of Complex Numbers From prevous classes, you may have encountered magnary numbers the square roots of negatve numbers and, more generally, complex numbers whch are the
More informationp(z) = 1 a e z/a 1(z 0) yi a i x (1/a) exp y i a i x a i=1 n i=1 (y i a i x) inf 1 (y Ax) inf Ax y (1 ν) y if A (1 ν) = 0 otherwise
Dustn Lennon Math 582 Convex Optmzaton Problems from Boy, Chapter 7 Problem 7.1 Solve the MLE problem when the nose s exponentally strbute wth ensty p(z = 1 a e z/a 1(z 0 The MLE s gven by the followng:
More informationNumerical Solutions of a Generalized Nth Order Boundary Value Problems Using Power Series Approximation Method
Appled Mathematcs, 6, 7, 5-4 Publshed Onlne Jul 6 n ScRes. http://www.scrp.org/journal/am http://.do.org/.436/am.6.77 umercal Solutons of a Generalzed th Order Boundar Value Problems Usng Power Seres Approxmaton
More informationA MULTIDIMENSIONAL ANALOGUE OF THE RADEMACHER-GAUSSIAN TAIL COMPARISON
A MULTIDIMENSIONAL ANALOGUE OF THE RADEMACHER-GAUSSIAN TAIL COMPARISON PIOTR NAYAR AND TOMASZ TKOCZ Abstract We prove a menson-free tal comparson between the Euclean norms of sums of nepenent ranom vectors
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 informationResearch on Time-history Input Methodology of Seismic Analysis
Transactons, SRT 19, Toronto, August 2007 Research on Tme-hstory Input ethoology of Sesmc Analyss Jang Nabn, ao Qng an Zhang Yxong State Key Laboratory of Reactor System Desgn Technology, Nuclear Power
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 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 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 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 informationA MULTIDIMENSIONAL ANALOGUE OF THE RADEMACHER-GAUSSIAN TAIL COMPARISON
A MULTIDIMENSIONAL ANALOGUE OF THE RADEMACHER-GAUSSIAN TAIL COMPARISON PIOTR NAYAR AND TOMASZ TKOCZ Abstract We prove a menson-free tal comparson between the Euclean norms of sums of nepenent ranom vectors
More informationNon-linear Canonical Correlation Analysis Using a RBF Network
ESANN' proceedngs - European Smposum on Artfcal Neural Networks Bruges (Belgum), 4-6 Aprl, d-sde publ., ISBN -97--, pp. 57-5 Non-lnear Canoncal Correlaton Analss Usng a RBF Network Sukhbnder Kumar, Elane
More informationMAE140 - Linear Circuits - Fall 13 Midterm, October 31
Instructons ME140 - Lnear Crcuts - Fall 13 Mdterm, October 31 () Ths exam s open book. You may use whatever wrtten materals you choose, ncludng your class notes and textbook. You may use a hand calculator
More information1 Matrix representations of canonical matrices
1 Matrx representatons of canoncal matrces 2-d rotaton around the orgn: ( ) cos θ sn θ R 0 = sn θ cos θ 3-d rotaton around the x-axs: R x = 1 0 0 0 cos θ sn θ 0 sn θ cos θ 3-d rotaton around the y-axs:
More informationLecture 3. Ax x i a i. i i
18.409 The Behavor of Algorthms n Practce 2/14/2 Lecturer: Dan Spelman Lecture 3 Scrbe: Arvnd Sankar 1 Largest sngular value In order to bound the condton number, we need an upper bound on the largest
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 informationClassical Mechanics Symmetry and Conservation Laws
Classcal Mechancs Symmetry an Conservaton Laws Dpan Kumar Ghosh UM-DAE Centre for Excellence n Basc Scences Kalna, Mumba 400085 September 7, 2016 1 Concept of Symmetry If the property of a system oes not
More informationInvestigation of the Relationship between Diesel Fuel Properties and Emissions from Engines with Fuzzy Linear Regression
www.esc.org Internatonal Journal of Energ Scence (IJES) Volume 3 Issue 2, Aprl 2013 Investgaton of the Relatonshp between Desel Fuel Propertes and Emssons from Engnes wth Fuzz Lnear Regresson Yuanwang
More informationInner Product. Euclidean Space. Orthonormal Basis. Orthogonal
Inner Product Defnton 1 () A Eucldean space s a fnte-dmensonal vector space over the reals R, wth an nner product,. Defnton 2 (Inner Product) An nner product, on a real vector space X s a symmetrc, blnear,
More informationDevelopment of a Novel 3-DoF Purely Translational Parallel Mechanism
27 IEEE Internatonal Conference on Robotcs and Automaton Roma Ital 1-14 Aprl 27 Development of a Novel -DoF Purel Translatonal Parallel Mechansm Yunjang Lou Jangang L Jnbo Sh and Zeang L Abstract In vew
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 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 informationALTERNATIVE METHODS FOR RELIABILITY-BASED ROBUST DESIGN OPTIMIZATION INCLUDING DIMENSION REDUCTION METHOD
Proceengs of IDETC/CIE 00 ASME 00 Internatonal Desgn Engneerng Techncal Conferences & Computers an Informaton n Engneerng Conference September 0-, 00, Phlaelpha, Pennsylvana, USA DETC00/DAC-997 ALTERATIVE
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 informationDEMO #8 - GAUSSIAN ELIMINATION USING MATHEMATICA. 1. Matrices in Mathematica
demo8.nb 1 DEMO #8 - GAUSSIAN ELIMINATION USING MATHEMATICA Obectves: - defne matrces n Mathematca - format the output of matrces - appl lnear algebra to solve a real problem - Use Mathematca to perform
More informationApplication of Linear Model Predictive Control and Input-Output Linearization to Constrained Control of 3D Cable Robots
Moern Mechancal Engneerng, 2011, 1, 69-76 o:10.4236/mme.2011.12009 Publshe Onlne November 2011 (http://www.scrp.org/journal/mme) Applcaton of Lnear Moel Prectve Control an Input-Output Lnearzaton to Constrane
More informationNumerical Solution of Ordinary Differential Equations
Numercal Methods (CENG 00) CHAPTER-VI Numercal Soluton of Ordnar Dfferental Equatons 6 Introducton Dfferental equatons are equatons composed of an unknown functon and ts dervatves The followng are examples
More informationPlacement of Robot Manipulators to Maximize Dexterity
Placement of Robot Manpulators to Maxmze Dexterty Karm Abdel-Malek and We u Department of Mechancal Engneerng he Unversty of Iowa Iowa Cty, IA 54 el. (39) 335-5676 amalek@engneerng.uowa.edu Placement of
More informationOne Dimensional Axial Deformations
One Dmensonal al Deformatons In ths secton, a specfc smple geometr s consdered, that of a long and thn straght component loaded n such a wa that t deforms n the aal drecton onl. The -as s taken as the
More informationDifference Equations
Dfference Equatons c Jan Vrbk 1 Bascs Suppose a sequence of numbers, say a 0,a 1,a,a 3,... s defned by a certan general relatonshp between, say, three consecutve values of the sequence, e.g. a + +3a +1
More informationLecture Notes on Linear Regression
Lecture Notes on Lnear Regresson Feng L fl@sdueducn Shandong Unversty, Chna Lnear Regresson Problem In regresson problem, we am at predct a contnuous target value gven an nput feature vector We assume
More informationRobot Modeling and Kinematics Errata R. Manseur. List of errors and typos reported as of 4/1/2007:
Robot Modelng and Knematcs Errata R. Manseur. Lst of errors and typos reported as of 4//7:. Fle CF4.wrl mentoned on page 45 s not on the CD. Fle ZYZ_Sm.wrl mentoned on page 67 s not on the CD. 3. Pg. 43.
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 informationQuantum Mechanics I - Session 4
Quantum Mechancs I - Sesson 4 Aprl 3, 05 Contents Operators Change of Bass 4 3 Egenvectors and Egenvalues 5 3. Denton....................................... 5 3. Rotaton n D....................................
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 informationLECTURE 9 CANONICAL CORRELATION ANALYSIS
LECURE 9 CANONICAL CORRELAION ANALYSIS Introducton he concept of canoncal correlaton arses when we want to quantfy the assocatons between two sets of varables. For example, suppose that the frst set of
More informationFormulas for the Determinant
page 224 224 CHAPTER 3 Determnants e t te t e 2t 38 A = e t 2te t e 2t e t te t 2e 2t 39 If 123 A = 345, 456 compute the matrx product A adj(a) What can you conclude about det(a)? For Problems 40 43, use
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 informationVisualization of 2D Data By Rational Quadratic Functions
7659 Englan UK Journal of Informaton an Computng cence Vol. No. 007 pp. 7-6 Vsualzaton of D Data By Ratonal Quaratc Functons Malk Zawwar Hussan + Nausheen Ayub Msbah Irsha Department of Mathematcs Unversty
More informationChapter 24 Work and Energy
Chapter 4 or an Energ 4 or an Energ You have one qute a bt of problem solvng usng energ concepts. ac n chapter we efne energ as a transferable phscal quantt that an obect can be sa to have an we sa that
More informationCHAPTER-5 INFORMATION MEASURE OF FUZZY MATRIX AND FUZZY BINARY RELATION
CAPTER- INFORMATION MEASURE OF FUZZY MATRI AN FUZZY BINARY RELATION Introducton The basc concept of the fuzz matr theor s ver smple and can be appled to socal and natural stuatons A branch of fuzz matr
More informationInductance Calculation for Conductors of Arbitrary Shape
CRYO/02/028 Aprl 5, 2002 Inductance Calculaton for Conductors of Arbtrary Shape L. Bottura Dstrbuton: Internal Summary In ths note we descrbe a method for the numercal calculaton of nductances among conductors
More informationCHARACTERISTICS OF COMPLEX SEPARATION SCHEMES AND AN ERROR OF SEPARATION PRODUCTS OUTPUT DETERMINATION
Górnctwo Geonżynera Rok 0 Zeszyt / 006 Igor Konstantnovch Mladetskj * Petr Ivanovch Plov * Ekaterna Nkolaevna Kobets * Tasya Igorevna Markova * CHARACTERISTICS OF COMPLEX SEPARATION SCHEMES AND AN ERROR
More informationCHAPTER 4 MAX-MIN AVERAGE COMPOSITION METHOD FOR DECISION MAKING USING INTUITIONISTIC FUZZY SETS
56 CHAPER 4 MAX-MIN AVERAGE COMPOSIION MEHOD FOR DECISION MAKING USING INUIIONISIC FUZZY SES 4.1 INRODUCION Intutonstc fuzz max-mn average composton method s proposed to construct the decson makng for
More informationImportant Instructions to the Examiners:
Summer 0 Examnaton Subject & Code: asc Maths (70) Model Answer Page No: / Important Instructons to the Examners: ) The Answers should be examned by key words and not as word-to-word as gven n the model
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 informationTopological Sensitivity Analysis for Three-dimensional Linear Elasticity Problem
6 th Worl Congress on Structural an Multscplnary Optmzaton Ro e Janero, 30 May - 03 June 2005, Brazl Topologcal Senstvty Analyss for Three-mensonal Lnear Elastcty Problem A.A. Novotny 1, R.A. Fejóo 1,
More informationNew Method for Solving Poisson Equation. on Irregular Domains
Appled Mathematcal Scences Vol. 6 01 no. 8 369 380 New Method for Solvng Posson Equaton on Irregular Domans J. Izadan and N. Karamooz Department of Mathematcs Facult of Scences Mashhad BranchIslamc Azad
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 informationCalculation of Coherent Synchrotron Radiation in General Particle Tracer
Calculaton of Coherent Synchrotron Raaton n General Partcle Tracer T. Myajma, Ivan V. Bazarov KEK-PF, Cornell Unversty 9 July, 008 CSR n GPT D CSR wake calculaton n GPT usng D. Sagan s formula. General
More informationPARALLEL MECHANISMS WITH VARIABLE COMPLIANCE
PRLLEL MECHNISMS WIH VRIBLE COMPLINCE By HYUN KWON JUNG DISSERION PRESENED O HE GRDUE SCHOOL OF HE UNIVERSIY OF FLORID IN PRIL FULFILLMEN OF HE REQUIREMENS FOR HE DEGREE OF DOCOR OF PHILOSOPHY UNIVERSIY
More informationUncertainty in measurements of power and energy on power networks
Uncertanty n measurements of power and energy on power networks E. Manov, N. Kolev Department of Measurement and Instrumentaton, Techncal Unversty Sofa, bul. Klment Ohrdsk No8, bl., 000 Sofa, Bulgara Tel./fax:
More informationA NUMERICAL COMPARISON OF LANGRANGE AND KANE S METHODS OF AN ARM SEGMENT
Internatonal Conference Mathematcal and Computatonal ology 0 Internatonal Journal of Modern Physcs: Conference Seres Vol. 9 0 68 75 World Scentfc Publshng Company DOI: 0.4/S009450059 A NUMERICAL COMPARISON
More informationThe Asymptotic Distributions of the Absolute Maximum of the Generalized Wiener Random Field
Internatonal Journal of Apple Engneerng esearch ISSN 973-456 Volume, Number 8 (7) pp. 79-799 esearch Ina Publcatons. http://www.rpublcaton.com The Asmptotc Dstrbutons of the Absolute Maxmum of the Generalze
More informationEN40: Dynamics and Vibrations. Homework 7: Rigid Body Kinematics
N40: ynamcs and Vbratons Homewor 7: Rgd Body Knematcs School of ngneerng Brown Unversty 1. In the fgure below, bar AB rotates counterclocwse at 4 rad/s. What are the angular veloctes of bars BC and C?.
More informationChapter 5. Solution of System of Linear Equations. Module No. 6. Solution of Inconsistent and Ill Conditioned Systems
Numercal Analyss by Dr. Anta Pal Assstant Professor Department of Mathematcs Natonal Insttute of Technology Durgapur Durgapur-713209 emal: anta.bue@gmal.com 1 . Chapter 5 Soluton of System of Lnear Equatons
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 informationSolutions to Practice Problems
Phys A Solutons to Practce Probles hapter Inucton an Maxwell s uatons (a) At t s, the ef has a agntue of t ag t Wb s t Wb s Wb s t Wb s V t 5 (a) Table - gves the resstvty of copper Thus, L A 8 9 5 (b)
More information1 Derivation of Point-to-Plane Minimization
1 Dervaton of Pont-to-Plane Mnmzaton Consder the Chen-Medon (pont-to-plane) framework for ICP. Assume we have a collecton of ponts (p, q ) wth normals n. We want to determne the optmal rotaton and translaton
More informationSCALARS AND VECTORS All physical quantities in engineering mechanics are measured using either scalars or vectors.
SCALARS AND ECTORS All phscal uanttes n engneerng mechancs are measured usng ether scalars or vectors. Scalar. A scalar s an postve or negatve phscal uantt that can be completel specfed b ts magntude.
More informationChapter 2 Transformations and Expectations. , and define f
Revew for the prevous lecture Defnton: support set of a ranom varable, the monotone functon; Theorem: How to obtan a cf, pf (or pmf) of functons of a ranom varable; Eamples: several eamples Chapter Transformatons
More informationErrors for Linear Systems
Errors for Lnear Systems When we solve a lnear system Ax b we often do not know A and b exactly, but have only approxmatons  and ˆb avalable. Then the best thng we can do s to solve ˆx ˆb exactly whch
More information