DYNAMIC MODELING AND PATH PLANNING OF FLEXIBLE-LINK MANIPULATORS

Size: px
Start display at page:

Download "DYNAMIC MODELING AND PATH PLANNING OF FLEXIBLE-LINK MANIPULATORS"

Transcription

1 Int. J. Mech. Eng. & Rob. Res. M Nazemzadeh et al., Research Paper ISSN ol., No., Aprl IJMERR. All Rghts Reserved DYNAMIC MODELING AND PAH PLANNING OF FLEXIBLE-LINK MANIPULAORS M Nazemzadeh *, M aher and Sh Nazer *Correspondng Author: M Nazemzadeh, mn.nazemzadeh@gmal.com In ths paper, dynamc modelng and path plannng of flexble-lnk manpulators are presented. Each lnk of flexble manpulator s modeled by fnte number of elements, and the dsplacement of element s formulated based on nodal coordnates and shape functons of beam element. hen, the knetc and potental energy of the system s developed usng the dsplacement n the reference coordnate systems. hen, by employng the Lagrange prncple, the nonlnear dynamc model of the system s derved and valdated. Keywords: Flexble-lnk, Manpulator, Dynamc modelng, Fnte element method INRODUCION Flexble-lnk manpulators exhbt many advantages over ther tradtonal rgd ones: they have lght weght, ther motors are smaller, and ther producton s frugal. Because of these novel features, the applcaton of flexble manpulators are exceedngly developed durng last decades, and they have been acheved an mportant role n many felds of scence such as surgcal operaton (Kumar et al., ; and Lao et al., 8), nuclear applcaton (Jansen et al., 99; and Perrot et al., ), and aero space structures (Satoko and Kazuya, ; and Zhong, ). hus, the dynamc modelng and analyss of such system s mportant and treated by some authors: Book (999) analyzed the dynamc behavor of flexble manpulators based on recursve lagrangan method. Moreover, a Newton-Euler approach s presented n Rakhsha and Goldenberg (985) to model the dynamc of a flexble robot. Meghdar and Fahm () used an analytcal method to decouple the dynamc equatons of elastc manpulators. Furthermore, a lumped model of a planer flexble manpulator s presented n Megahed and Hamza (). Sngh (Megahed and Hamza, ) used an extended Hamlton s prncple to derve the equaton of moton of the flexble manpulator. Korayem and Rahm () and Korayem et al. ( and ) presented the dynamc Department of Mechancs, Damavand Branch, Islamc Azad Unversty, Damavand, Iran.

2 Int. J. Mech. Eng. & Rob. Res. M Nazemzadeh et al., modelng of flexble manpulator systems, based on assumed mode method. In ther method, the flexble behavor of the system s modeled va egen functons multpled by modal coordnate of the system. In ths paper, the mathematcal analyss and dynamc modelng of flexble manpulator s presented based on fnte element method. Each lnk of the system s modeled by fnte number of elements, and the dsplacement vector of each pont of the robot s formulated n the reference coordnate by means of fnte formulaton of beam element. hen, the knetc and potental energes of the system are presented, and the dynamc model of the system s derved usng Lagrange prncple. Fnally, smulaton results are presented. FINIE ELEMEN FORMULAION FOR MAHEMAICAL MODEL OF HE SYSEM o present the mathematcal and dynamc model of the flexble manpulators, the system wth m number of lnks, each lnk s dvded to n elements wth length of l. As the total dsplacement of each pont of the flexble manpulator can be presented as r. Accordng to Fgure, the reference coordnate system s shown by OXY, and the local coordnate system attached to th lnk s assumed as O XY. he parameters of the flexble manpulator are shown as follows: s j th element of th lnk, r s dsplacement vector of element, r o s dsplacement vector of th jont, represents angular dsplacement of th jont, n s number of elements of th lnk, L s length of th lnk, m s mass per length of th lnk, g s gravtatonal constant of earth, l s length of j th element of th lnk, E s elastcty modulus of th lnk, I s moment of nerta of th lnk, represents rotaton matrx between local and global coordnate system. Fgure shows a flexble-lnk manpulator. o present the total dsplacement vector of th element of the system n the global coordnate system, ths vector s assumed as a summaton of dsplacement of O, and the deflecton of the lnk n the local coordnate O X Y : r Fgure : he Flexble Manpulator r, r r, f r O ( j ) l x y...() Where y s the deflecton of element due to flexblty of system n the local coordnates. By mplementaton of fnte element method, ths dsplacement s presumed a summaton of Hermtan shape functon multpled to nodal coordnate of the element (Zenkewcz et al., 5): x,t y k( x ) uk...() k Where k shows the shape functon and u k are the nodal coordnate of the systems, and are gven as (Zenkewcz et al., 5):

3 Int. J. Mech. Eng. & Rob. Res. M Nazemzadeh et al., x x...() l ( x ) l x x ( x ) x...() l l ( x ) l x x...(5) l x x ( x )...(6) l l As the dsplacement vector of element s formulated, the knetc energy of the element s stated as follows: l r m t r. dx t x l...(7) If, the vectors z u u u u u u u u Equaton (7) can be rewrtten as: z M ( l, p) M z l r m zl r. z p and are defned, the dx...(8) Besde, the potental energy of the element s shown as, and s a summaton of gravtatonal potental energy, and elastc potental energy g e : e g...(8) he gravtatonal potental energy s gven as: g l m g...(9) r dx And the elastc energy of the system s: y l e EI ( )dx K...() x Where the stffness matrx K s presented as: K EI l 6l 6l 6l l 6l l 6l 6l 6l l 6l l...() Now, the generalzed coordnate vector s defned as q, and the total knetc and potental energy of the system can be wrtten as: as ( q,q ) m n j ( q ) m n j...() hen, the Lagrange functon s ntroduced L( q, q ), and the Lagrange prncple s developed: he prncple of Lagrange for dynamc systems s expressed as: d dt L L Q j q j q...() j Where q j represents the generalzed coordnates, Q j s the generalzed external force. hus, by mplementaton of Lagrange prncple, the nonlnear dynamc equatons of the system are summarzed as follows: q q B M q f,...() As n Equaton () s presented, the nonlnear dynamc model of the system s developed, and no lnearzaton s done. hus, the nonlnear terms affect the dynamc of the system. It must be notced that for each lnk of the flexble manpulator, the frst node s concded 5

4 Int. J. Mech. Eng. & Rob. Res. M Nazemzadeh et al., on the jont of the lnk. hus, these nodal coordnates are zero: u ( t ), u( t )...() DYNAMIC MODEL OF A SINGLE LINK MANIPULAOR For a sngle-lnk flexble manpulator, as the lnk modeled by one element, the generalzed coordnate vector of the system s q u u, where s angular dsplacement of the robot jont, u and u are the elastc deflecton and slope of the end pont of the flexble manpulator. Moreover, the rotaton matrx of the system s: hus, the dynamc equaton of the system can be derved, usng Lagrange prncple. o smulate the dynamc behavor of the system, the parameters are gven as: m = 5 kg, L = m, I = 5e-9, E = e9 pa, g = 9.8. he smulaton results are as follows: Fgure : Angular Dsplacement of Flexble Manpulator cos( ) sn( ) sn( ) cos( )...(5) And the total dsplacement of any pont of the robot s: x xcos( ) sn( ) ( L r x x sn( ) cos( ) ( L x x ) u ( L L x x ) u ( L L x ) u L x ) u L Fgure : Dsplacement Mode Shape of the Flexble Manpulator...(6) So, the knetc and potental energes of the sngle-lnk flexble manpulator are stated as: L u 7L u L u ml 78 u u Lu L uu 78 Lu 7L u...(7) g mgl 6u cos( ) Lu cos( ) 6L sn( ) EI...(8) e u Lu u Lu...(9) L CONCLUSION In ths paper, the nonlnear dynamc analyss of the flexble manpulators has been studed usng fnte element method. he total 6

5 Int. J. Mech. Eng. & Rob. Res. M Nazemzadeh et al., dsplacement vector of the system has been formulated usng Hermtan shape functon. Hence, the total dsplacement of the elastc arm n reference coordnate system has been presented, the Lagrange prncple has been used to derve the nonlnear dynamc moton of the elastc manpulator. Fnally, the proposed method has been employed to derve the dynamc equatons of a sngle-lnk manpulator, and some smulatons are done. REFERENCES. Book W J (999), Recursve Lagrangan Dynamcs of Flexble Manpulator Arms, Int. J. of Robotcs Research, ol., pp Jansen J F, Burks B L, Babcock S M, Kress R L and Hamel W R (99), Long- Reach Manpulaton for Waste Storage ank Remedaton, n ASME Dyn. Syst. Control. Dv., DSC, ol., pp Korayem M H and Rahm H N (), Nonlnear Dynamc Analyss for Elastc Robotc Arms, Fronters of Mechancal Engneerng, ol. 6, No., pp Korayem M H, Rahm H N and Nkoobn A (), Mathematcal Modelng and rajectory Plannng of Moble Manpulators wth Flexble Lnks and Jonts, Appled Mathematcal Modellng, ol. 6, No. 7, pp Korayem M H, Rahm H N, Nkoobn A and Nazemzadeh M (), Maxmum Allowable Dynamc Payload for Flexble Moble Robotc Manpulators, Latn Amercan Appled Research, ol., No., pp Kumar R, Berkelman P, Gupta P, Barnes A, Jensen P S, Whtcomb L L and aylor R (), Prelmnary Experments n Cooperatve Human/Robot Force Control for Robot Asssted Mcro-Surgcal Manpulaton, Proc. of IEEE Int. Conf. on Robotcs and Automaton, ol. 6, pp Lao H, Suzuk H, Matsumya K, Masamune K, Doh and Chba (8), Fetus-Supportng Flexble Manpulator wth Balloon-ype Stablzer for Endoscopc Intrauterne Surgery, Int. J. of Medcal Robotcs and Computer Asssted Surgery, ol., pp Megahed S M and Hamza K (), Modelng and Smulaton of Planar Flexble Lnk Manpulators wth Rgd p Connectons to Revolute Jonts, Robotca, ol., pp Meghdar A and Fahm F (), On the Frst-Order Decouplng of Dynamcal Equatons of Moton for Elastc Multbody Systems as Appled to a wo-lnk Flexble Manpulator, Multbody Systems Dynamcs, ol. 5, pp. -.. Perrot Y, Corder J J, Frconneau J P, Masonner D, Martn E and Palmer J D (), Development of a Long Reach Artculated Manpulator for IER n essel Inspecton Under acuum and emperature, Fuson Eng. Desgn, ol. 69, pp Rakhsha F and Goldenberg A A (985), Dynamc Modelng of a Sngle Lnk Flexble Robot, Proc. of the IEEE Int. Conf. on Robotcs and Automaton, pp

6 Int. J. Mech. Eng. & Rob. Res. M Nazemzadeh et al.,. Satoko A and Kazuya Y (), Adaptve Reacton Control for Space Robotc Applcatons wth Dynamc Model Uncertanty, Advanced Robotcs, ol., pp Zhong J L (), Dynamc Modelng and braton Control of a Space Flexble Manpulator Usng Pezoelectrc Actuators and Sensors, Advanced Materals Research, ol. 5, pp Zenkewcz O C, aylor R L and Zhu J Z (5), he Fnte Element Method, ts Bass and Fundamentals, Elsever Butterworth Henemann. 8

Effects of System Parameters and Controlled Torque on the Dynamics of Rigid-Flexible Robotic Manipulator

Effects of System Parameters and Controlled Torque on the Dynamics of Rigid-Flexible Robotic Manipulator Journal of Robotcs, Networkng and Artfcal Lfe, Vol. 3, No. (September 016), 116-13 Effects of System Parameters and Controlled orque on the Dynamcs of Rgd-Flexble Robotc Manpulator Sachndra Mahto Mechancal

More information

COMPOSITE BEAM WITH WEAK SHEAR CONNECTION SUBJECTED TO THERMAL LOAD

COMPOSITE 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 information

Lecture 23: Newton-Euler Formulation. Vaibhav Srivastava

Lecture 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 information

NMT 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 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 information

THE EFFECT OF TORSIONAL RIGIDITY BETWEEN ELEMENTS ON FREE VIBRATIONS OF A TELESCOPIC HYDRAULIC CYLINDER SUBJECTED TO EULER S LOAD

THE 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 information

829. An adaptive method for inertia force identification in cantilever under moving mass

829. 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 information

The Analysis of Coriolis Effect on a Robot Manipulator

The Analysis of Coriolis Effect on a Robot Manipulator Internatonal Journal of Innovatons n Engneerng and echnology (IJIE) he Analyss of Corols Effect on a Robot Manpulator Pratap P homas Assstant Professor Department of Mechancal Engneerng K G Reddy college

More information

Study on Active Micro-vibration Isolation System with Linear Motor Actuator. Gong-yu PAN, Wen-yan GU and Dong LI

Study 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 information

Physics 5153 Classical Mechanics. D Alembert s Principle and The Lagrangian-1

Physics 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 information

VIBRATION FATIGUE DESIGN METHODOLOGY OF A LARGE SCALE HEAVY DUTY ROBOT

VIBRATION FATIGUE DESIGN METHODOLOGY OF A LARGE SCALE HEAVY DUTY ROBOT ICSV14 Carns Australa 9-12 July, 2007 VIBRATION FATIGUE DESIGN METHODOLOGY OF A LARGE SCALE HEAVY DUTY ROBOT Jong Hw Seo 1, Jae Chul Hwang 1, Yong Won Cho 1, Dong Il Km 1, Hong Jae Ym 2 1 Robotcs Technology

More information

Technical Report TR05

Technical Report TR05 Techncal Report TR05 An Introducton to the Floatng Frame of Reference Formulaton for Small Deformaton n Flexble Multbody Dynamcs Antono Recuero and Dan Negrut May 11, 2016 Abstract Ths techncal report

More information

Indeterminate pin-jointed frames (trusses)

Indeterminate 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 information

A NUMERICAL COMPARISON OF LANGRANGE AND KANE S METHODS OF AN ARM SEGMENT

A 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 information

Iterative General Dynamic Model for Serial-Link Manipulators

Iterative 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 information

Vibration Reduction of a Flexible Robot Through a Stochastic Optimal Control Strategy

Vibration Reduction of a Flexible Robot Through a Stochastic Optimal Control Strategy EngOpt 28 - Internatonal Conference on Engneerng Optmzaton Ro de Janero, Brazl, - 5 June 28. Vbraton Reducton of a Flexble Robot Through a Stochastc Optmal Control Strategy Rogéro Rodrgues dos Santos,

More information

Finite Element Modelling of truss/cable structures

Finite 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 information

Mechanics Physics 151

Mechanics Physics 151 Mechancs Physcs 151 Lecture 3 Lagrange s Equatons (Goldsten Chapter 1) Hamlton s Prncple (Chapter 2) What We Dd Last Tme! Dscussed mult-partcle systems! Internal and external forces! Laws of acton and

More information

Modeling and Simulation of a Hexapod Machine Tool for the Dynamic Stability Analysis of Milling Processes. C. Henninger, P.

Modeling 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 information

Module 3: Element Properties Lecture 1: Natural Coordinates

Module 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 information

Trajectory Optimization of Flexible Mobile Manipulators Using Open-Loop Optimal Control method

Trajectory Optimization of Flexible Mobile Manipulators Using Open-Loop Optimal Control method rajectory Optmzaton o Flexble Moble Manpulators Usng Open-Loop Optmal Control method M.H. Korayem and H. Rahm Nohooj Robotc Lab, Mechancal Department, Iran Unversty o Scence and echnology hkorayem@ust.ac.r,

More information

Please initial the statement below to show that you have read it

Please initial the statement below to show that you have read it EN0: Structural nalyss Exam I Wednesday, March 2, 2005 Dvson of Engneerng rown Unversty NME: General Instructons No collaboraton of any nd s permtted on ths examnaton. You may consult your own wrtten lecture

More information

coordinates. Then, the position vectors are described by

coordinates. Then, the position vectors are described by Revewng, what we have dscussed so far: Generalzed coordnates Any number of varables (say, n) suffcent to specfy the confguraton of the system at each nstant to tme (need not be the mnmum number). In general,

More information

Advanced Mechanical Elements

Advanced 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 information

DYNAMIC ANALYSIS OF A CONSTRAINED ROTATING FLEXIBLE EXTENSIBLE LINK WITH SEMI-PERIODIC IMPACT

DYNAMIC ANALYSIS OF A CONSTRAINED ROTATING FLEXIBLE EXTENSIBLE LINK WITH SEMI-PERIODIC IMPACT 11 th Internatonal Conference on Vbraton Problems Z. Dmtrovová et al. (eds.) Lsbon, Portugal, 9-12 September 2013 DYAMIC AALYSIS OF A COSTRAIED ROTATIG FLEXIBLE EXTESIBLE LIK WITH SEMI-PERIODIC IMPACT

More information

Dynamic Load Carrying Capacity of Flexible Manipulators Using Finite Element Method and Pontryagin s Minimum Principle

Dynamic Load Carrying Capacity of Flexible Manipulators Using Finite Element Method and Pontryagin s Minimum Principle Journal o Optmzaton n Industral Engneerng 1 (13) 17-4 Dynamc Load Carryng Capacty o Flexble Manpulators Usng Fnte Element Method and Pontryagn s Mnmum Prncple Moharam H. Korayem a,*, Mostaa Nazemzadeh

More information

EML 5223 Structural Dynamics HW 10. Gun Lee(UFID )

EML 5223 Structural Dynamics HW 10. Gun Lee(UFID ) E 5 Structural Dynamcs HW Gun ee(ufid895-47) Problem 9. ubular shaft of radus r ( ) r[ + ( )/ ], thcknesst, mass per unt volume ρ and shear modulus G. t r( ). Shaft s symmetrc wth respect to /. ass moment

More information

Physics 5153 Classical Mechanics. Principle of Virtual Work-1

Physics 5153 Classical Mechanics. Principle of Virtual Work-1 P. Guterrez 1 Introducton Physcs 5153 Classcal Mechancs Prncple of Vrtual Work The frst varatonal prncple we encounter n mechancs s the prncple of vrtual work. It establshes the equlbrum condton of a mechancal

More information

ANALYSIS OF TIMOSHENKO BEAM RESTING ON NONLINEAR COMPRESSIONAL AND FRICTIONAL WINKLER FOUNDATION

ANALYSIS OF TIMOSHENKO BEAM RESTING ON NONLINEAR COMPRESSIONAL AND FRICTIONAL WINKLER FOUNDATION VOL. 6, NO., NOVEMBER ISSN 89-668 6- Asan Research Publshng Network (ARPN). All rghts reserved. ANALYSIS OF TIMOSHENKO BEAM RESTING ON NONLINEAR COMPRESSIONAL AND FRICTIONAL WINKLER FOUNDATION Adel A.

More information

Design and Analysis of Landing Gear Mechanic Structure for the Mine Rescue Carrier Robot

Design 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 information

An Algorithm to Solve the Inverse Kinematics Problem of a Robotic Manipulator Based on Rotation Vectors

An 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 information

11. Dynamics in Rotating Frames of Reference

11. Dynamics in Rotating Frames of Reference Unversty of Rhode Island DgtalCommons@URI Classcal Dynamcs Physcs Course Materals 2015 11. Dynamcs n Rotatng Frames of Reference Gerhard Müller Unversty of Rhode Island, gmuller@ur.edu Creatve Commons

More information

STATIC ANALYSIS OF TWO-LAYERED PIEZOELECTRIC BEAMS WITH IMPERFECT SHEAR CONNECTION

STATIC ANALYSIS OF TWO-LAYERED PIEZOELECTRIC BEAMS WITH IMPERFECT SHEAR CONNECTION STATIC ANALYSIS OF TWO-LERED PIEZOELECTRIC BEAMS WITH IMPERFECT SHEAR CONNECTION Ákos József Lengyel István Ecsed Assstant Lecturer Emertus Professor Insttute of Appled Mechancs Unversty of Mskolc Mskolc-Egyetemváros

More information

2D Motion of Rigid Bodies: Falling Stick Example, Work-Energy Principle

2D Motion of Rigid Bodies: Falling Stick Example, Work-Energy Principle Example: Fallng Stck 1.003J/1.053J Dynamcs and Control I, Sprng 007 Professor Thomas Peacock 3/1/007 ecture 10 D Moton of Rgd Bodes: Fallng Stck Example, Work-Energy Prncple Example: Fallng Stck Fgure

More information

Physics 181. Particle Systems

Physics 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 information

Modelling and Analysis of Planar Robotic Arm Dynamics Based on An Improved Transfer Matrix Method for Multi-body Systems

Modelling and Analysis of Planar Robotic Arm Dynamics Based on An Improved Transfer Matrix Method for Multi-body Systems he 4th FoMM World ongress, ape, awan, ctober 5-3, 5 D Number:.6567/FoMM.4H.W.S3.46 Modellng and Analyss of Planar Robotc Arm Dynamcs Based on An mproved ransfer Matrx Method for Mult-body Systems W. hen

More information

Lesson 5: Kinematics and Dynamics of Particles

Lesson 5: Kinematics and Dynamics of Particles Lesson 5: Knematcs and Dynamcs of Partcles hs set of notes descrbes the basc methodology for formulatng the knematc and knetc equatons for multbody dynamcs. In order to concentrate on the methodology and

More information

In this section is given an overview of the common elasticity models.

In 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 information

DUE: WEDS FEB 21ST 2018

DUE: WEDS FEB 21ST 2018 HOMEWORK # 1: FINITE DIFFERENCES IN ONE DIMENSION DUE: WEDS FEB 21ST 2018 1. Theory Beam bendng s a classcal engneerng analyss. The tradtonal soluton technque makes smplfyng assumptons such as a constant

More information

A particle in a state of uniform motion remain in that state of motion unless acted upon by external force.

A particle in a state of uniform motion remain in that state of motion unless acted upon by external force. The fundamental prncples of classcal mechancs were lad down by Galleo and Newton n the 16th and 17th centures. In 1686, Newton wrote the Prncpa where he gave us three laws of moton, one law of gravty,

More information

MEEM 3700 Mechanical Vibrations

MEEM 3700 Mechanical Vibrations MEEM 700 Mechancal Vbratons Mohan D. Rao Chuck Van Karsen Mechancal Engneerng-Engneerng Mechancs Mchgan echnologcal Unversty Copyrght 00 Lecture & MEEM 700 Multple Degree of Freedom Systems (ext: S.S.

More information

Analytical classical dynamics

Analytical 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 information

LAGRANGIAN MECHANICS

LAGRANGIAN MECHANICS LAGRANGIAN MECHANICS Generalzed Coordnates State of system of N partcles (Newtonan vew): PE, KE, Momentum, L calculated from m, r, ṙ Subscrpt covers: 1) partcles N 2) dmensons 2, 3, etc. PE U r = U x 1,

More information

Statistical Energy Analysis for High Frequency Acoustic Analysis with LS-DYNA

Statistical Energy Analysis for High Frequency Acoustic Analysis with LS-DYNA 14 th Internatonal Users Conference Sesson: ALE-FSI Statstcal Energy Analyss for Hgh Frequency Acoustc Analyss wth Zhe Cu 1, Yun Huang 1, Mhamed Soul 2, Tayeb Zeguar 3 1 Lvermore Software Technology Corporaton

More information

Week 9 Chapter 10 Section 1-5

Week 9 Chapter 10 Section 1-5 Week 9 Chapter 10 Secton 1-5 Rotaton Rgd Object A rgd object s one that s nondeformable The relatve locatons of all partcles makng up the object reman constant All real objects are deformable to some extent,

More information

The Two-scale Finite Element Errors Analysis for One Class of Thermoelastic Problem in Periodic Composites

The Two-scale Finite Element Errors Analysis for One Class of Thermoelastic Problem in Periodic Composites 7 Asa-Pacfc Engneerng Technology Conference (APETC 7) ISBN: 978--6595-443- The Two-scale Fnte Element Errors Analyss for One Class of Thermoelastc Problem n Perodc Compostes Xaoun Deng Mngxang Deng ABSTRACT

More information

Scroll Generation with Inductorless Chua s Circuit and Wien Bridge Oscillator

Scroll Generation with Inductorless Chua s Circuit and Wien Bridge Oscillator Latest Trends on Crcuts, Systems and Sgnals Scroll Generaton wth Inductorless Chua s Crcut and Wen Brdge Oscllator Watcharn Jantanate, Peter A. Chayasena, and Sarawut Sutorn * Abstract An nductorless Chua

More information

Automatic PID Controller Tuning for Robots with Nonlinear Friction at the Joints

Automatic PID Controller Tuning for Robots with Nonlinear Friction at the Joints Automatc PID Controller unng for Robots wth Nonlnear Frcton at the Jonts Abílo Azenha, Ph.D. Abstract hs paper descrbes an approach to automatc tunng of PID poston controllers for manpulators wth nonlnear

More information

XXI Brain Storming Day. Catania 29/10/2010. Eng. Filippo Bonaccorso

XXI Brain Storming Day. Catania 29/10/2010. Eng. Filippo Bonaccorso XXI Bran Stormng Day Catana 29/10/2010 Eng. Flppo Bonaccorso Outlne Intro Dynamc Model of Robotc Structures Dynamc Model Evaluaton Results Conclusons & Future Works RAPOLAC clusters expertse and resources

More information

Application of B-Spline to Numerical Solution of a System of Singularly Perturbed Problems

Application of B-Spline to Numerical Solution of a System of Singularly Perturbed Problems Mathematca Aeterna, Vol. 1, 011, no. 06, 405 415 Applcaton of B-Splne to Numercal Soluton of a System of Sngularly Perturbed Problems Yogesh Gupta Department of Mathematcs Unted College of Engneerng &

More information

MH Korayem, AM Shafei, M Doosthoseini, F Absalan and B Kadkhodaei. Introduction. Original Article

MH Korayem, AM Shafei, M Doosthoseini, F Absalan and B Kadkhodaei. Introduction. Original Article Orgnal Artcle Theoretcal and expermental nvestgaton of vscoelastc seral robotc manpulators wth motors at the onts usng Tmoshenko beam theory and Gbbs Appell formulaton Proc IMechE Part K: J Mult-body Dynamcs

More information

Elshaboury SM et al.; Sch. J. Phys. Math. Stat., 2015; Vol-2; Issue-2B (Mar-May); pp

Elshaboury SM et al.; Sch. J. Phys. Math. Stat., 2015; Vol-2; Issue-2B (Mar-May); pp Elshabour SM et al.; Sch. J. Phs. Math. Stat. 5; Vol-; Issue-B (Mar-Ma); pp-69-75 Scholars Journal of Phscs Mathematcs Statstcs Sch. J. Phs. Math. Stat. 5; (B):69-75 Scholars Academc Scentfc Publshers

More information

Irregular vibrations in multi-mass discrete-continuous systems torsionally deformed

Irregular vibrations in multi-mass discrete-continuous systems torsionally deformed (2) 4 48 Irregular vbratons n mult-mass dscrete-contnuous systems torsonally deformed Abstract In the paper rregular vbratons of dscrete-contnuous systems consstng of an arbtrary number rgd bodes connected

More information

MODAL ANALYSIS AND TESTING OF ROTATING MACHINES FOR PREDICTIVE MAINTENANCE: EFFECT OF GYROSCOPIC FORCES

MODAL ANALYSIS AND TESTING OF ROTATING MACHINES FOR PREDICTIVE MAINTENANCE: EFFECT OF GYROSCOPIC FORCES MODAL ANALYSIS AND TESTING OF ROTATING MACHINES FOR PREDICTIVE MAINTENANCE: EFFECT OF GYROSCOPIC FORCES A. Vansteenkste; M. Loccufer; B. Vervsch; P. De Baets; Ghent Unversty, Belgum Abstract Through the

More information

Professor Terje Haukaas University of British Columbia, Vancouver The Q4 Element

Professor Terje Haukaas University of British Columbia, Vancouver  The Q4 Element Professor Terje Haukaas Unversty of Brtsh Columba, ancouver www.nrsk.ubc.ca The Q Element Ths document consders fnte elements that carry load only n ther plane. These elements are sometmes referred to

More information

Integrals and Invariants of Euler-Lagrange Equations

Integrals and Invariants of Euler-Lagrange Equations Lecture 16 Integrals and Invarants of Euler-Lagrange Equatons ME 256 at the Indan Insttute of Scence, Bengaluru Varatonal Methods and Structural Optmzaton G. K. Ananthasuresh Professor, Mechancal Engneerng,

More information

Dimensional Synthesis of Wristed Binary Hands

Dimensional Synthesis of Wristed Binary Hands Dmensonal Synthess of Wrsted Bnary Hands Neda Hassanzadeh Department of Mechancal Engneerng, Idaho State Unversty 921 S. 8th. Ave, Pocatello, ID 83209, USA e-mal:hassneda@su.edu Alba Perez-Graca Assocate

More information

NUMERICAL RESULTS QUALITY IN DEPENDENCE ON ABAQUS PLANE STRESS ELEMENTS TYPE IN BIG DISPLACEMENTS COMPRESSION TEST

NUMERICAL RESULTS QUALITY IN DEPENDENCE ON ABAQUS PLANE STRESS ELEMENTS TYPE IN BIG DISPLACEMENTS COMPRESSION TEST Appled Computer Scence, vol. 13, no. 4, pp. 56 64 do: 10.23743/acs-2017-29 Submtted: 2017-10-30 Revsed: 2017-11-15 Accepted: 2017-12-06 Abaqus Fnte Elements, Plane Stress, Orthotropc Materal Bartosz KAWECKI

More information

Application to Plane (rigid) frame structure

Application to Plane (rigid) frame structure Advanced Computatonal echancs 18 Chapter 4 Applcaton to Plane rgd frame structure 1. Dscusson on degrees of freedom In case of truss structures, t was enough that the element force equaton provdes onl

More information

Three views of mechanics

Three views of mechanics Three vews of mechancs John Hubbard, n L. Gross s course February 1, 211 1 Introducton A mechancal system s manfold wth a Remannan metrc K : T M R called knetc energy and a functon V : M R called potental

More information

General displacement arch-cantilever element method for stress analysis of arch dam

General displacement arch-cantilever element method for stress analysis of arch dam Water Scence and Engneerng, 009, (): 3-4 do:0.388/j.ssn.674-370.009.0.004 http://kkb.hhu.edu.cn e-mal: wse@hhu.edu.cn General dsplacement arch-cantlever element method for stress analyss of arch dam Hao

More information

1 axis. F Input force for i th joint. f Force exerted on linki by linki 1at the coordinate frame ( i 1

1 axis. F Input force for i th joint. f Force exerted on linki by linki 1at the coordinate frame ( i 1 Internatonal Journal of Robotcs and Automaton (IJRA) Vol. 3, No., December, pp. ~33 ISSN: 89-856 Dynamc Behavor of a SCARA Robot by usng N-E Method for a Straght Lne and Smulaton of Moton by usng Soldworks

More information

GEO-SLOPE International Ltd, Calgary, Alberta, Canada Vibrating Beam

GEO-SLOPE International Ltd, Calgary, Alberta, Canada   Vibrating Beam GEO-SLOPE Internatonal Ltd, Calgary, Alberta, Canada www.geo-slope.com Introducton Vbratng Beam Ths example looks at the dynamc response of a cantlever beam n response to a cyclc force at the free end.

More information

Tensor Smooth Length for SPH Modelling of High Speed Impact

Tensor Smooth Length for SPH Modelling of High Speed Impact Tensor Smooth Length for SPH Modellng of Hgh Speed Impact Roman Cherepanov and Alexander Gerasmov Insttute of Appled mathematcs and mechancs, Tomsk State Unversty 634050, Lenna av. 36, Tomsk, Russa RCherepanov82@gmal.com,Ger@npmm.tsu.ru

More information

MULTIBODY DYNAMICS METHOD FOR IMMERSED TUNNEL SUBJECTED TO LONGITUDINAL SEISMIC LOADING

MULTIBODY DYNAMICS METHOD FOR IMMERSED TUNNEL SUBJECTED TO LONGITUDINAL SEISMIC LOADING th World Congress on Computatonal Mechancs (WCCM XI) 5th European Conference on Computatonal Mechancs (ECCM V) 6th European Conference on Computatonal Flud Dynamcs (ECFD VI) E. Oñate, J. Olver and A. Huerta

More information

Nonlinear Effects in Stiffness Modeling of Robotic Manipulators

Nonlinear Effects in Stiffness Modeling of Robotic Manipulators A. Pashkevch, A. Klmchk D. Chablatonlnear effect n stffness modelng of robotc manpulators, In: Proceedngs of Internatonal Conference on Computer and Automaton echnology (ICCA 29), Vence, Italy, 29, World

More information

Modeling of Dynamic Systems

Modeling 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 information

Chapter 8. Potential Energy and Conservation of Energy

Chapter 8. Potential Energy and Conservation of Energy Chapter 8 Potental Energy and Conservaton of Energy In ths chapter we wll ntroduce the followng concepts: Potental Energy Conservatve and non-conservatve forces Mechancal Energy Conservaton of Mechancal

More information

Mathematical Modeling and Nonlinear Dynamic Analysis of Flexible Manipulators using Finite Element Method

Mathematical Modeling and Nonlinear Dynamic Analysis of Flexible Manipulators using Finite Element Method Unvesa Jouna of Non-nea Mechancs (), 56-6 www.papescences.com Mathematca Modeng and Nonnea Dynamc Anayss of Fexbe Manpuatos usng Fnte Eement Method J. Jafa, M. Mzae, M. Zandbaf Depatment of Mechancs, Damavand

More information

First 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.

First 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 information

COEFFICIENT DIAGRAM: A NOVEL TOOL IN POLYNOMIAL CONTROLLER DESIGN

COEFFICIENT DIAGRAM: A NOVEL TOOL IN POLYNOMIAL CONTROLLER DESIGN Int. J. Chem. Sc.: (4), 04, 645654 ISSN 097768X www.sadgurupublcatons.com COEFFICIENT DIAGRAM: A NOVEL TOOL IN POLYNOMIAL CONTROLLER DESIGN R. GOVINDARASU a, R. PARTHIBAN a and P. K. BHABA b* a Department

More information

Lagrange Multipliers. A Somewhat Silly Example. Monday, 25 September 2013

Lagrange Multipliers. A Somewhat Silly Example. Monday, 25 September 2013 Lagrange Multplers Monday, 5 September 013 Sometmes t s convenent to use redundant coordnates, and to effect the varaton of the acton consstent wth the constrants va the method of Lagrange undetermned

More information

Computing Nonequilibrium Conformational Dynamics of Structured Nucleic Acid Assemblies

Computing Nonequilibrium Conformational Dynamics of Structured Nucleic Acid Assemblies Supportng Informaton for Computng Nonequlbrum Conformatonal Dynamcs of Structured Nuclec Acd Assembles Reza Sharf Sedeh,, Keyao Pan,, Matthew Ralph Adendorff, Oskar Hallatschek, Klaus-Jürgen Bathe,*, and

More information

Parameter Estimation for Dynamic System using Unscented Kalman filter

Parameter Estimation for Dynamic System using Unscented Kalman filter Parameter Estmaton for Dynamc System usng Unscented Kalman flter Jhoon Seung 1,a, Amr Atya F. 2,b, Alexander G.Parlos 3,c, and Klto Chong 1,4,d* 1 Dvson of Electroncs Engneerng, Chonbuk Natonal Unversty,

More information

GENERALIZED LAGRANGE D ALEMBERT PRINCIPLE. Ðorđe Ðukić

GENERALIZED LAGRANGE D ALEMBERT PRINCIPLE. Ðorđe Ðukić PUBLICATIONS DE L INSTITUT MATHÉMATIQUE Nouvelle sére, tome 91(105) (2012), 49 58 DOI: 10.2298/PIM1205049D GENERALIZED LAGRANGE D ALEMBERT PRINCIPLE Ðorđe Ðukć Abstract. The major ssues n the analyss of

More information

FORCE-DISPLACEMENT RELATIONSHIPS OF A TENSEGRITY STRUCTURE CONSIDERING BAR INTERFERENCE

FORCE-DISPLACEMENT RELATIONSHIPS OF A TENSEGRITY STRUCTURE CONSIDERING BAR INTERFERENCE U.P.B. Sc. Bull., Seres D, Vol. 78, Iss. 2, 2016 ISSN 1454-2358 FORCE-DISPLACEMENT RELATIONSHIPS OF A TENSEGRITY STRUCTURE CONSIDERING BAR INTERFERENCE Mn LIN 1, Tuanje LI 2, Zhfe JI 3, Mngku CHE 4 Tensegrty

More information

Integrals and Invariants of

Integrals and Invariants of Lecture 16 Integrals and Invarants of Euler Lagrange Equatons NPTEL Course Varatonal Methods and Structural Optmzaton G. K. Ananthasuresh Professor, Mechancal Engneerng, Indan Insttute of Scence, Banagalore

More information

ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM

ELASTIC 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 information

Analysis of Dynamic Cross Response between Spindles in a Dual Spindle Type Multi-Functional Turning Machine

Analysis of Dynamic Cross Response between Spindles in a Dual Spindle Type Multi-Functional Turning Machine Journal of Power and Energy Engneerng, 2013, 1, 20-24 http://dx.do.org/10.4236/jpee.2013.17004 Publshed Onlne December 2013 (http://www.scrp.org/journal/jpee) Analyss of Dynamc Cross Response between Spndles

More information

Translational Equations of Motion for A Body Translational equations of motion (centroidal) for a body are m r = f.

Translational Equations of Motion for A Body Translational equations of motion (centroidal) for a body are m r = f. Lesson 12: Equatons o Moton Newton s Laws Frst Law: A artcle remans at rest or contnues to move n a straght lne wth constant seed there s no orce actng on t Second Law: The acceleraton o a artcle s roortonal

More information

Identification of Instantaneous Modal Parameters of A Nonlinear Structure Via Amplitude-Dependent ARX Model

Identification of Instantaneous Modal Parameters of A Nonlinear Structure Via Amplitude-Dependent ARX Model Identfcaton of Instantaneous Modal Parameters of A Nonlnear Structure Va Ampltude-Dependent ARX Model We Chh Su(NCHC), Chung Shann Huang(NCU), Chng Yu Lu(NCU) Outlne INRODUCION MEHODOLOGY NUMERICAL VERIFICAION

More information

Frame element resists external loads or disturbances by developing internal axial forces, shear forces, and bending moments.

Frame element resists external loads or disturbances by developing internal axial forces, shear forces, and bending moments. CE7 Structural Analyss II PAAR FRAE EEET y 5 x E, A, I, Each node can translate and rotate n plane. The fnal dsplaced shape has ndependent generalzed dsplacements (.e. translatons and rotatons) noled.

More information

A Multi-Axis Force Measurement System for a Space Docking Mechanism

A 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 information

Army Ants Tunneling for Classical Simulations

Army 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 information

Dynamic analysis and vibration control of a multi-body system using MSC Adams

Dynamic analysis and vibration control of a multi-body system using MSC Adams 1505 Dynamc analyss and vbraton control of a mult-body system usng MSC Adams Abstract In ths paper, modellng and smulaton of a mult-body system for ts vbraton control usng sensors and actuators s presented.

More information

Part C Dynamics and Statics of Rigid Body. Chapter 5 Rotation of a Rigid Body About a Fixed Axis

Part C Dynamics and Statics of Rigid Body. Chapter 5 Rotation of a Rigid Body About a Fixed Axis Part C Dynamcs and Statcs of Rgd Body Chapter 5 Rotaton of a Rgd Body About a Fxed Axs 5.. Rotatonal Varables 5.. Rotaton wth Constant Angular Acceleraton 5.3. Knetc Energy of Rotaton, Rotatonal Inerta

More information

Notes on Analytical Dynamics

Notes on Analytical Dynamics Notes on Analytcal Dynamcs Jan Peters & Mchael Mstry October 7, 004 Newtonan Mechancs Basc Asssumptons and Newtons Laws Lonely pontmasses wth postve mass Newtons st: Constant velocty v n an nertal frame

More information

CHAIN DYNAMIC FORMULATIONS FOR MULTIBODY SYSTEM TRACKED VEHICLES

CHAIN DYNAMIC FORMULATIONS FOR MULTIBODY SYSTEM TRACKED VEHICLES 2012 NDIA GROUND VEHICLE SYSEMS ENGINEERING AND ECHNOLOGY SYMOSIUM MODELING &SIMULAION, ESING AND VALIDAION (MSV) MINI-SYMOSIUM AUGUS 14-16, MICHIGAN CHAIN DYNAMIC FORMULAIONS FOR MULIBODY SYSEM RACKED

More information

UNIVERSITY OF BOLTON RAK ACADEMIC CENTRE BENG(HONS) MECHANICAL ENGINEERING SEMESTER TWO EXAMINATION 2017/2018 FINITE ELEMENT AND DIFFERENCE SOLUTIONS

UNIVERSITY OF BOLTON RAK ACADEMIC CENTRE BENG(HONS) MECHANICAL ENGINEERING SEMESTER TWO EXAMINATION 2017/2018 FINITE ELEMENT AND DIFFERENCE SOLUTIONS OCD0 UNIVERSITY OF BOLTON RAK ACADEMIC CENTRE BENG(HONS) MECHANICAL ENGINEERING SEMESTER TWO EXAMINATION 07/08 FINITE ELEMENT AND DIFFERENCE SOLUTIONS MODULE NO. AME6006 Date: Wednesda 0 Ma 08 Tme: 0:00

More information

Spin-rotation coupling of the angularly accelerated rigid body

Spin-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 information

Poisson brackets and canonical transformations

Poisson brackets and canonical transformations rof O B Wrght Mechancs Notes osson brackets and canoncal transformatons osson Brackets Consder an arbtrary functon f f ( qp t) df f f f q p q p t But q p p where ( qp ) pq q df f f f p q q p t In order

More information

On an Extension of Stochastic Approximation EM Algorithm for Incomplete Data Problems. Vahid Tadayon 1

On an Extension of Stochastic Approximation EM Algorithm for Incomplete Data Problems. Vahid Tadayon 1 On an Extenson of Stochastc Approxmaton EM Algorthm for Incomplete Data Problems Vahd Tadayon Abstract: The Stochastc Approxmaton EM (SAEM algorthm, a varant stochastc approxmaton of EM, s a versatle tool

More information

The Feynman path integral

The Feynman path integral The Feynman path ntegral Aprl 3, 205 Hesenberg and Schrödnger pctures The Schrödnger wave functon places the tme dependence of a physcal system n the state, ψ, t, where the state s a vector n Hlbert space

More information

Robust Fuzzy Control for 2-DOF Manipulator System

Robust Fuzzy Control for 2-DOF Manipulator System Amercan Journal of Artfcal Intellgence 07; (): 56-6 http://wwwscencepublshnggroupcom/j/aja do: 0648/jaja07007 Robust Fuzzy Control for -DOF Manpulator System Ayman A Aly,, Aloqla A Mechancal Engneerng

More information

UIC University of Illinois at Chicago

UIC University of Illinois at Chicago DSL Dynamc Smulaton Laboratory UIC Unversty o Illnos at Chcago FINITE ELEMENT/ MULTIBODY SYSTEM ALGORITHMS FOR RAILROAD VEHICLE SYSTEM DYNAMICS Ahmed A. Shabana Department o Mechancal and Industral Engneerng

More information

Effects of Boundary Conditions on Cross-Ply Laminated Composite Beams

Effects of Boundary Conditions on Cross-Ply Laminated Composite Beams Internatonal Journal of Engneerng Research And Advanced Technology (IJERAT) DOI: http://dx.do.org/0.734/ijerat.344 E-ISSN : 454-635 Vol.3 (0) Oct -07 Effects of Boundary Condtons on Cross-Ply Lamnated

More information

A Mechanics-Based Approach for Determining Deflections of Stacked Multi-Storey Wood-Based Shear Walls

A Mechanics-Based Approach for Determining Deflections of Stacked Multi-Storey Wood-Based Shear Walls A Mechancs-Based Approach for Determnng Deflectons of Stacked Mult-Storey Wood-Based Shear Walls FPINNOVATIONS Acknowledgements Ths publcaton was developed by FPInnovatons and the Canadan Wood Councl based

More information

Lecture 8 Modal Analysis

Lecture 8 Modal Analysis Lecture 8 Modal Analyss 16.0 Release Introducton to ANSYS Mechancal 1 2015 ANSYS, Inc. February 27, 2015 Chapter Overvew In ths chapter free vbraton as well as pre-stressed vbraton analyses n Mechancal

More information

modeling of equilibrium and dynamic multi-component adsorption in a two-layered fixed bed for purification of hydrogen from methane reforming products

modeling of equilibrium and dynamic multi-component adsorption in a two-layered fixed bed for purification of hydrogen from methane reforming products modelng of equlbrum and dynamc mult-component adsorpton n a two-layered fxed bed for purfcaton of hydrogen from methane reformng products Mohammad A. Ebrahm, Mahmood R. G. Arsalan, Shohreh Fatem * Laboratory

More information

So far: simple (planar) geometries

So far: simple (planar) geometries Physcs 06 ecture 5 Torque and Angular Momentum as Vectors SJ 7thEd.: Chap. to 3 Rotatonal quanttes as vectors Cross product Torque epressed as a vector Angular momentum defned Angular momentum as a vector

More information

Lagrangian Field Theory

Lagrangian Field Theory Lagrangan Feld Theory Adam Lott PHY 391 Aprl 6, 017 1 Introducton Ths paper s a summary of Chapter of Mandl and Shaw s Quantum Feld Theory [1]. The frst thng to do s to fx the notaton. For the most part,

More information