Simulation Hybrid Fuzzy Control of SCARA Robot

Size: px
Start display at page:

Download "Simulation Hybrid Fuzzy Control of SCARA Robot"

Transcription

1 3rd WSEAS Internationa Conference on APPLIED and THEORETICAL MECHANICS, Spain, Decemer 4-6, Simuation Hyrid Fuzzy Contro of SCARA Root MARIUS-CONSTANTIN POPESCU, ILIE BORCOŞI, ONISIFOR OLARU, LUMINIŢA POPESCU, FLORIN GROFU Department of Eectromechanics University of Craiova str. A. I. Cuza nr.3, Craiova Department of Automatics and Informatics University of C-tin Brancusi str. Geneva nr.3, Tg-Jiu, Gorj ROMANIA Astract: - This paper presents the simuation of a Hyrid Fuzzy Controer suitae for industria appications. The deveoped Hyrid Fuzzy Controer consists of a weighted comination of the Direct Fuzzy Controer and Indirect Fuzzy Controer and a graduay activated supervisory controer. The unique feature of the Hyrid Fuzzy Controer is that no mathematica modes of the pant are required and the proposed controer is ae to adaptivey estimate the ound functions on-ine, which are required for the determination of the supervisory controer. The supervisor controer in the sense that a signas are ounded guarantees goa staiity of the cosed-oop system. The approach of rapid prototyping is empoyed to impement the Hyrid Fuzzy Controer so as to contro a Seectivey Compiance Assemy Root Arm. Simuink, an interactive graphica software for simuating dynamic systems, is used to mode, simuate and anayse the dynamic system. Key-Words: - SCARA Root, Simuink, Hyrid Fuzzy Controer Introduction The non-inear dynamics governing root motion presents a chaenging contro proem in the fied of contro engineering. As the manipuators are usuay used to perform high-precision tasks, root controers are required to contro the motion of a root effectivey and accuratey. However, as the manipuator is a mutivariae non-inear couping dynamic system with uncertainties, it is difficut to otain an accurate mathematica mode so that cassica or modern contro aws can e appied. To accommodate system uncertainties and variations, earning or adaptive techniques must e incorporated. Whie conventiona controers cannot effectivey contro the motion of a root due to compications of these noninear effects, fuzzy ogic, however, coud offer a promising approach to circumvent the deficiency. This is ecause in contrast with conventiona controers, fuzzy ogic aows one to formuate the contro proem of a pant in terms of inguistic rues drawn from the ehaviour of a 'human operator' instead of an agorithm synthesised from a rigorous mathematica mode of the pant. In this paper, a Hyrid Fuzzy Controer (HFC) suitae for rea-time industria appications is designed, deveoped and simuation. The HFC is made up of two on-ine adaptive fuzzy controers, namey Direct Fuzzy Controer (DFC) and Indirect Fuzzy Controer (IFC) with adaptive aws that can guarantee goa staiity of the cosed-oop system. In IFC, the dynamics of the root manipuator are estimated onine and the controer is chosen assuming that the estimated dynamics represents the true dynamics of the system. In AFC, the parameters of the controer are adjusted directy in order to reduce some norm of the output error etween the pant and the reference mode. The HFC is ae to compensate for environmenta variations such as payoad mass and disturance torque during the operation process. It is found to e superior to conventiona adaptive controers primariy ecause oundaries of uncertainties are eing adaptivey estimated. However, one major drawack of the HFC is that it requires massive computing resources and speeds crucia for its impementation. Therefore, the main chaenge for rea-time execution of this controer is to minimise the amount of processing that need to e performed y the controer efore the next input data arrives. The approach of rapid prototyping is

2 3rd WSEAS Internationa Conference on APPLIED and THEORETICAL MECHANICS, Spain, Decemer 4-6, empoyed to impement the HFC so as to contro a Seectivey Compiance Assemy Root Arm (SCARA) Root in rea time. Simuink, interactive graphica software for simuating dynamic systems, is used to mode, simuate and anayse the dynamic system. 2 Proem Formuation 2.. Background on the SCARA root Each of the four axes provides a different motion and contriutes to one degree of freedom of the root (see Fig. ). The asic SCARA geometry is reaised y arranging two revoute joints (T and T2 axes) and one prismatic joint (Z-axis) in such a way that a axes of motion are parae. The acronym SCARA characterises the mechanica features of a structure offering high stiffness to vertica oads and compiance to horizonta oads. Motion contro is impemented ony for axes Z, T and T2 in this work, which are designated as Joint, 2 and 3 respectivey The root dynamic mode The dynamic equations of a rigid ody root are a is generay expressed in the form of [, [4: M(θ )θ +C(, θ θ )θ +G(θ )+F Vθ +F C =τ, where M(θ ) is the n n inertia matrix of the manipuator, C(, θ θ ) is the n n vector of centrifuga and Coriois terms, G(θ ) is an n vector of gravity terms, F V is the n vector of viscous friction terms, F C is the n vector of couom terms and τ is the n vector of the input torque (generated y the joint motor). Each eement of M(θ ) and G(θ ) is a compicated function which depends on θ, anguar positions of a joints of the manipuator. Simiary, each eement of C(, θ θ ) is a compicated function of oth θ and θ. The movement of the end-effector in a desired trajectory, at a particuar veocity, thus requires a compex set of torque functions to e appied to the actuating system of the root at each joint. The dynamic mode of the SCARA root arm has een deveoped in [2, [3, with most of its parameters determined and verified through experiments. Based on this known mathematica mode of the root, simuation anaysis and design of the HFC were carried out using MATLAB simuation toos. set of highy non-inear couped differentia equations. The dynamics (of a nth joint root arm) 2.3. Motion contro A two-joint contro structure is used in this work

3 3rd WSEAS Internationa Conference on APPLIED and THEORETICAL MECHANICS, Spain, Decemer 4-6, where the motion of the T-axis and T2-axis wi e controed simutaneousy. In this scheme, the Z-axis wi not e controed since the earier work is ased on a two-joint controer. The dynamics of the two joints can e represented y a mutipe-input mutipe-output (MIMO) system. The degree of difficuty wi increase with the numer of joints moving together. 3 Proem Soution 3.. Hyrid fuzzy controer The proposed contro agorithm is given y [5: ( α) τ D τ S τ = ατ + +, () where τ is the contro torque contriuted y the IFC, τ D is the contro torque contriuted y the DFC, τ S is the supervisory controer and α is a weighting factor. If fuzzy contro rues are more important and reiae than fuzzy descriptions, choose α to e sma; otherwise, choose α to e arge. The resuting certainty equivaent controer is: = τ ( θ / Φ) [ F( θ, θ / Φ) + θ + K E K E I G M V +, )+ G( θ ) ( θ / Φ) P, (2) θ = F( θ θ τ D, (3) where ( θ τ D / Φ) F, ( θ,θ G and ( θ / Φ) assume the foowing form: f ( x) = M = i= M y n n = i= e e 2 xi xi σ i 2 xi xi σ i, (4) where f ( x) is the fuzzy ogic system with Gaussian memership function, centre average defuzzifier and product-inference rue, and y, xi and σ i are adjustae parameters. Now adding and sutracting G(θ ) τ to Eq. (3) and after some manipuations, we otain the cosed-oop error equation due to the DFC which is given as: E =-K V Ė -K E p +G(θ ) [ τ ( θ / Φ ) τ D. (5) The cosed-oop error dynamics due to the IFC ecomes: E =-K v Ė -K E +[ ( ) p θ,θ / Φ [ ( θ / Φ) F -F(, θ θ ) + G -G(θ ) τ I. (6) Since the overa controer of Eq. () consists of a weighted comination of DFC and IFC, the respective weighted errors ecome: (-α ) E =-(-α )K v Ė -(-α )K p E + (-α )G[ τ ( θ / Φ) τ D (7) and α E =-α K v Ė -α K p E+α [ F( θ,θ - F(, θ θ ) + α [ ( θ / Φ) G -G(θ ) τ I. (8) The overa error governing the cosed-oop system is given y the sum of Eqs. (7) and (8), i.e. E Fθ,θ / Φ - F(, θ θ ) + =-K V Ė -K p E +α [ ( ) α [ ( θ / Φ) τ +(-α )G(θ )[ τ ( θ / Φ) G I τ D. (9) The overa error dynamics in the state-space form is: Ẋ =AX+α B I [( ( θ,θ G( θ ) I F -F(, θ θ )) + ( ( θ / Φ ) τ +(- α )B D [ τ ( θ / Φ) where X=( e e, e,, ) A= B I = 2 and p, v e n p2 G - τ D =AX+BU, () T, B D = 2 v2 2 22, B=[B I B D, = G(θ )=M - (θ ) α[ F( θ, θ / Φ) F( θ, θ) + α[ G( θ / Φ) G( θ) τ I U=, ( α) [ τ τ ( θ / Φ) D with K p and K v chosen such that A is a stae matrix,

4 3rd WSEAS Internationa Conference on APPLIED and THEORETICAL MECHANICS, Spain, Decemer 4-6, there exists a unique 2n 2n positive definite symmetric matrix, P which satisfies the Lyapunov equation: A T P + PA=-Q, () process continues y using Simuink and toooxes to deveop the agorithm as we as anayse the resuts. where Q is an aritrary 2n 2n positive definite matrix. Let the Lyapunov function candidate e: V e = 2 X T PX. (2) Differentiating Eq. (2) with respect to time and using Eqs. () and () eads to: V e = 2 T Ẋ +α X T PB I [( ( θ,θ - G( θ ) I PX+ 2 X T P Ẋ =- 2 X T QX F -F(, θ θ ))+( ( θ / Φ ) τ +(- α )X T PB D [ τ ( θ / Φ) G (3) τ D. In order for the system to e ounded, we require V e to e ounded which means that V e < whenever V e is greater than a constant V specified y the designer. However, from Eq. (3), we see that it is difficut to design τ D ( θ / Φ) and τ I ( θ / Φ) such that the ast two terms of Eq. (3) are ess than zero. We can sove this proem y appending another contro term τ S ( θ) which is caed supervisory contro aw. The fina contro aw ecomes: τ θ / Φ = ατ θ / Φ + α τ θ / Φ τ θ (4) ( ) ( ) ( ) ( ) ( ) F I D + S 3.2. Simuation mode of HFC The simuation program for the HFC is written in Simuink to faciitate Rapid Prototyping, a process that aows one to conceptuaize soutions using ock diagram modeing environment and predict the system performance prior to aying out hardware, writing any production software, or committing to a fixed design [8. Fig. 2 shows the rapid prototyping process in greater detais. The contro system mode and dynamics of the SCARA root are created in Simuink. The first step in the design is to deveop the SCARA root mode prior to agorithm deveopment. Fig. 2 Rapid prototyping process If the resuts are not satisfactory, we iterate the modeing/anaysis process unti satisfactory resuts are otained. Fig. 3 shows a Simuink diagram for simuating the HFC system for controing Joint 2 (T-axis) and Joint 3 (T2-axis) of the SCARA root. This prototype is modeed cosey ased on the SCARA root mode and the HFC agorithm. The input variaes to the HFC are position error and ink veocity of T and T2 axis. The output variae is used to contro the SCARA root. Once a simuation mode, which is ae to mode the root with sufficient accuracy, has een deveoped, the rapid prototyping

5 3rd WSEAS Internationa Conference on APPLIED and THEORETICAL MECHANICS, Spain, Decemer 4-6, Fig. 3. Contro system mode in Simuink 3.3. Simuation resuts To evauate the performance of our HFC, a series of simuation runs were performed. The joint trajectory responses were potted against time. Overshoots are kept stricty to zero and errors of ess than % recorded for a 2 joints. a) a) ) Fig. 4. Position trajectory of joint 2, a; Position error of joint 2,. ) Fig. 5. Position trajectory of joint 3, a; Position error of joint 3,. Fig. 4a shows the position tracking trajectories and the corresponding position tracking errors for joint 2 using the HFC with α set to.95 i.e., there are joint contriutions from the DFC and the IFC, with the IFC having 95% of the tota contriution. Fig. 5a depicts those of joint 3. Desired position trajectories are indicated in dashed ines and actua trajectories after incorporating the HFC are indicated in soid ines. Figs. 4 and 5 show the position errors of joint 2 and joint 3 respectivey. Both resuts show that overshoots are kept stricty to zero and errors of ess than % recorded for oth joints. The HFC software consists of primariy 2 modues: () The main contro modue, and (2) The GUI for signa monitoring and parameters tuning. Modue () is written in Simuink whereas Modue (2) is deveoped using Contro-Desk [, [6. The overa Simuink mode for the HFC is shown in Fig. 6.

6 3rd WSEAS Internationa Conference on APPLIED and THEORETICAL MECHANICS, Spain, Decemer 4-6, 27 8 Fig. 6. Overa Simuink graphica modes for the HFC 4 Concusion Once encouraging system performances are achieved, the Hyrid Adaptive Fuzzy Controer is impemented in rea-time through Rea-Time Workshop (RTW). The performance of the Hyrid Fuzzy Controer was found to e superior and it matches favouray the simuation resuts. A HFC suitae for rea-time industria appications has een successfuy designed, deveoped and simuation in this work. The approach of rapid prototyping process was adopted to shorten the deveopment time, thus reducing the cost of deveopment. The amount of time saved is sustantia especiay when no reuiding of codes is invoved. The performance of the HFC was found to e superior and it matches favoray the simuation resuts. With the promising resuts eing accompished, the authors are confident that the proposed HFC wi e very usefu in many other rea-time industria appications [7. References: [ Adekarim A., Terra Z., Impémentation d'un système de communication FM par 'utiisation du DSP TMS32VC542, Editeur Ecoe Nationae Poytechnique, 25 [2 Nianzu Zhang, Experimenta Research on Root Contro, M.Eng. thesis, Singapore, Nanyang Technoogica University, 996. [3 Meng Joo Er ', Moo Teng Lim, Hui Song Lim, Rea-time hyrid adaptive fuzzy contro of a SCARA root, Microprocessors and Microsystems 25, 2. [4 Onisifor O., Ampificatoare integrate in echipamente de automatizare, Editura Universitaria Craiova, 23. [5 Popescu M.C., Estimarea şi identificarea proceseor, Editura Sitech, Craiova, 26. [6 Popescu M.C, Utiisation des ordinateurs, Editura Universitaria, Craiova, 24. [7 Texas Instruments TMS32C54. [8 *** User Guide Mata for Simuink

Adaptive Fuzzy Sliding Control for a Three-Link Passive Robotic Manipulator

Adaptive Fuzzy Sliding Control for a Three-Link Passive Robotic Manipulator Adaptive Fuzzy Siding Contro for a hree-link Passive Robotic anipuator Abstract An adaptive fuzzy siding contro (AFSC scheme is proposed to contro a passive robotic manipuator. he motivation for the design

More information

CFD MODELLING OF DIRECT CONTACT STEAM INJECTION

CFD MODELLING OF DIRECT CONTACT STEAM INJECTION Fifth Internationa Conference on CFD in the Process Industries CSIRO, Meourne, Austraia 13-15 Decemer 006 CFD MODELLING OF DIRECT CONTACT STEAM INJECTION Curtis MARSH 1 and Denis WITHERS 1 CFD Design &

More information

The influence of temperature of photovoltaic modules on performance of solar power plant

The influence of temperature of photovoltaic modules on performance of solar power plant IOSR Journa of Engineering (IOSRJEN) ISSN (e): 2250-3021, ISSN (p): 2278-8719 Vo. 05, Issue 04 (Apri. 2015), V1 PP 09-15 www.iosrjen.org The infuence of temperature of photovotaic modues on performance

More information

THE DIRECT KINEMATICS OF REDUNDANT PARALLEL ROBOT FOR PREDICTIVE CONTROL

THE DIRECT KINEMATICS OF REDUNDANT PARALLEL ROBOT FOR PREDICTIVE CONTROL HE DIREC KINEMAICS OF REDUNDAN PARALLEL ROBO FOR PREDICIVE CONROL BELDA KVĚOSLAV, BÖHM JOSEF, VALÁŠEK MICHAEL Department of Adaptive Systems, Institute of Information heory and Automation, Academy of Sciences

More information

Implemental Formulation of Newton Dynamics for Free Insect Flight

Implemental Formulation of Newton Dynamics for Free Insect Flight Impementa Formuation of Neton Dynamics for Free Insect Fight Sheng Xu Department of Mathematics, Southern Methodist University, Daas, TX 75275-156, USA Astract A free-fying insect fies and maneuvers y

More information

Numerical simulation of javelin best throwing angle based on biomechanical model

Numerical simulation of javelin best throwing angle based on biomechanical model ISSN : 0974-7435 Voume 8 Issue 8 Numerica simuation of javein best throwing ange based on biomechanica mode Xia Zeng*, Xiongwei Zuo Department of Physica Education, Changsha Medica University, Changsha

More information

A Brief Introduction to Markov Chains and Hidden Markov Models

A Brief Introduction to Markov Chains and Hidden Markov Models A Brief Introduction to Markov Chains and Hidden Markov Modes Aen B MacKenzie Notes for December 1, 3, &8, 2015 Discrete-Time Markov Chains You may reca that when we first introduced random processes,

More information

First-Order Corrections to Gutzwiller s Trace Formula for Systems with Discrete Symmetries

First-Order Corrections to Gutzwiller s Trace Formula for Systems with Discrete Symmetries c 26 Noninear Phenomena in Compex Systems First-Order Corrections to Gutzwier s Trace Formua for Systems with Discrete Symmetries Hoger Cartarius, Jörg Main, and Günter Wunner Institut für Theoretische

More information

9. EXERCISES ON THE FINITE-ELEMENT METHOD

9. EXERCISES ON THE FINITE-ELEMENT METHOD 9. EXERCISES O THE FIITE-ELEMET METHOD Exercise Thickness: t=; Pane strain proem (ν 0): Surface oad Voume oad; 4 p f ( x, ) ( x ) 0 E D 0 0 0 ( ) 4 p F( xy, ) Interna constrain: rigid rod etween D and

More information

Modelling and simulation of a feed drive using the transmission line modelling technique

Modelling and simulation of a feed drive using the transmission line modelling technique Transactions on Engineering Sciences vo 44, 2003 WT Press, www.witpress.com, SSN 1743-3533 Modeing and simuation of a feed drive using the transmission ine modeing technique V.Y. Moreno-Castaneda, C. Pisaru,

More information

THE OUT-OF-PLANE BEHAVIOUR OF SPREAD-TOW FABRICS

THE OUT-OF-PLANE BEHAVIOUR OF SPREAD-TOW FABRICS ECCM6-6 TH EUROPEAN CONFERENCE ON COMPOSITE MATERIALS, Sevie, Spain, -6 June 04 THE OUT-OF-PLANE BEHAVIOUR OF SPREAD-TOW FABRICS M. Wysocki a,b*, M. Szpieg a, P. Heström a and F. Ohsson c a Swerea SICOMP

More information

An Algorithm for Pruning Redundant Modules in Min-Max Modular Network

An Algorithm for Pruning Redundant Modules in Min-Max Modular Network An Agorithm for Pruning Redundant Modues in Min-Max Moduar Network Hui-Cheng Lian and Bao-Liang Lu Department of Computer Science and Engineering, Shanghai Jiao Tong University 1954 Hua Shan Rd., Shanghai

More information

8 Digifl'.11 Cth:uits and devices

8 Digifl'.11 Cth:uits and devices 8 Digif'. Cth:uits and devices 8. Introduction In anaog eectronics, votage is a continuous variabe. This is usefu because most physica quantities we encounter are continuous: sound eves, ight intensity,

More information

Steepest Descent Adaptation of Min-Max Fuzzy If-Then Rules 1

Steepest Descent Adaptation of Min-Max Fuzzy If-Then Rules 1 Steepest Descent Adaptation of Min-Max Fuzzy If-Then Rues 1 R.J. Marks II, S. Oh, P. Arabshahi Λ, T.P. Caude, J.J. Choi, B.G. Song Λ Λ Dept. of Eectrica Engineering Boeing Computer Services University

More information

Nonlinear Gaussian Filtering via Radial Basis Function Approximation

Nonlinear Gaussian Filtering via Radial Basis Function Approximation 51st IEEE Conference on Decision and Contro December 10-13 01 Maui Hawaii USA Noninear Gaussian Fitering via Radia Basis Function Approximation Huazhen Fang Jia Wang and Raymond A de Caafon Abstract This

More information

Physics 505 Fall 2007 Homework Assignment #5 Solutions. Textbook problems: Ch. 3: 3.13, 3.17, 3.26, 3.27

Physics 505 Fall 2007 Homework Assignment #5 Solutions. Textbook problems: Ch. 3: 3.13, 3.17, 3.26, 3.27 Physics 55 Fa 7 Homework Assignment #5 Soutions Textook proems: Ch. 3: 3.3, 3.7, 3.6, 3.7 3.3 Sove for the potentia in Proem 3., using the appropriate Green function otained in the text, and verify that

More information

Lobontiu: System Dynamics for Engineering Students Website Chapter 3 1. z b z

Lobontiu: System Dynamics for Engineering Students Website Chapter 3 1. z b z Chapter W3 Mechanica Systems II Introduction This companion website chapter anayzes the foowing topics in connection to the printed-book Chapter 3: Lumped-parameter inertia fractions of basic compiant

More information

CS229 Lecture notes. Andrew Ng

CS229 Lecture notes. Andrew Ng CS229 Lecture notes Andrew Ng Part IX The EM agorithm In the previous set of notes, we taked about the EM agorithm as appied to fitting a mixture of Gaussians. In this set of notes, we give a broader view

More information

Combining reaction kinetics to the multi-phase Gibbs energy calculation

Combining reaction kinetics to the multi-phase Gibbs energy calculation 7 th European Symposium on Computer Aided Process Engineering ESCAPE7 V. Pesu and P.S. Agachi (Editors) 2007 Esevier B.V. A rights reserved. Combining reaction inetics to the muti-phase Gibbs energy cacuation

More information

OSCILLATIONS OF PARTIALLY FILLED TANKER TRUCK AT ITS BRAKING

OSCILLATIONS OF PARTIALLY FILLED TANKER TRUCK AT ITS BRAKING ENGINEERING FOR RURAL DEVELOPMENT Jegava, 5.-7.05.06. OSCILLATIONS OF PARTIALLY FILLED TANKER TRUCK AT ITS BRAKING Aexandr Shimanovsky Bearusian State University of Transport tm.esut@gmai.com Astract.

More information

UI FORMULATION FOR CABLE STATE OF EXISTING CABLE-STAYED BRIDGE

UI FORMULATION FOR CABLE STATE OF EXISTING CABLE-STAYED BRIDGE UI FORMULATION FOR CABLE STATE OF EXISTING CABLE-STAYED BRIDGE Juan Huang, Ronghui Wang and Tao Tang Coege of Traffic and Communications, South China University of Technoogy, Guangzhou, Guangdong 51641,

More information

On a geometrical approach in contact mechanics

On a geometrical approach in contact mechanics Institut für Mechanik On a geometrica approach in contact mechanics Aexander Konyukhov, Kar Schweizerhof Universität Karsruhe, Institut für Mechanik Institut für Mechanik Kaiserstr. 12, Geb. 20.30 76128

More information

Introduction. Figure 1 W8LC Line Array, box and horn element. Highlighted section modelled.

Introduction. Figure 1 W8LC Line Array, box and horn element. Highlighted section modelled. imuation of the acoustic fied produced by cavities using the Boundary Eement Rayeigh Integra Method () and its appication to a horn oudspeaer. tephen Kirup East Lancashire Institute, Due treet, Bacburn,

More information

IMA Preprint Series # 2323

IMA Preprint Series # 2323 A MATRIX FORMULATION OF THE NEWTON DYNAMICS FOR THE FREE FLIGHT OF AN INSECT By Sheng Xu IMA Preprint Series # 2323 ( June 21 ) INSTITUTE FOR MATHEMATICS AND ITS APPLICATIONS UNIVERSITY OF MINNESOTA 4

More information

Research on liquid sloshing performance in vane type tank under microgravity

Research on liquid sloshing performance in vane type tank under microgravity IOP Conference Series: Materias Science and Engineering PAPER OPEN ACCESS Research on iquid soshing performance in vane type tan under microgravity Reated content - Numerica simuation of fuid fow in the

More information

Statistical Learning Theory: A Primer

Statistical Learning Theory: A Primer Internationa Journa of Computer Vision 38(), 9 3, 2000 c 2000 uwer Academic Pubishers. Manufactured in The Netherands. Statistica Learning Theory: A Primer THEODOROS EVGENIOU, MASSIMILIANO PONTIL AND TOMASO

More information

Spring Gravity Compensation Using the Noncircular Pulley and Cable For the Less-Spring Design

Spring Gravity Compensation Using the Noncircular Pulley and Cable For the Less-Spring Design The 14th IFToMM Word Congress, Taipei, Taiwan, October 25-30, 2015 DOI Number: 10.6567/IFToMM.14TH.WC.PS3.010 Spring Gravity Compensation Using the Noncircuar Puey and Cabe For the Less-Spring Design M.C.

More information

Indirect Optimal Control of Dynamical Systems

Indirect Optimal Control of Dynamical Systems Computationa Mathematics and Mathematica Physics, Vo. 44, No. 3, 24, pp. 48 439. Transated from Zhurna Vychisite noi Matematiki i Matematicheskoi Fiziki, Vo. 44, No. 3, 24, pp. 444 466. Origina Russian

More information

Tracking Control of Multiple Mobile Robots

Tracking Control of Multiple Mobile Robots Proceedings of the 2001 IEEE Internationa Conference on Robotics & Automation Seou, Korea May 21-26, 2001 Tracking Contro of Mutipe Mobie Robots A Case Study of Inter-Robot Coision-Free Probem Jurachart

More information

Bayesian Unscented Kalman Filter for State Estimation of Nonlinear and Non-Gaussian Systems

Bayesian Unscented Kalman Filter for State Estimation of Nonlinear and Non-Gaussian Systems Bayesian Unscented Kaman Fiter for State Estimation of Noninear and Non-aussian Systems Zhong Liu, Shing-Chow Chan, Ho-Chun Wu and iafei Wu Department of Eectrica and Eectronic Engineering, he University

More information

PHYSICS LOCUS / / d dt. ( vi) mass, m moment of inertia, I. ( ix) linear momentum, p Angular momentum, l p mv l I

PHYSICS LOCUS / / d dt. ( vi) mass, m moment of inertia, I. ( ix) linear momentum, p Angular momentum, l p mv l I 6 n terms of moment of inertia, equation (7.8) can be written as The vector form of the above equation is...(7.9 a)...(7.9 b) The anguar acceeration produced is aong the direction of appied externa torque.

More information

Identification of macro and micro parameters in solidification model

Identification of macro and micro parameters in solidification model BULLETIN OF THE POLISH ACADEMY OF SCIENCES TECHNICAL SCIENCES Vo. 55, No. 1, 27 Identification of macro and micro parameters in soidification mode B. MOCHNACKI 1 and E. MAJCHRZAK 2,1 1 Czestochowa University

More information

BP neural network-based sports performance prediction model applied research

BP neural network-based sports performance prediction model applied research Avaiabe onine www.jocpr.com Journa of Chemica and Pharmaceutica Research, 204, 6(7:93-936 Research Artice ISSN : 0975-7384 CODEN(USA : JCPRC5 BP neura networ-based sports performance prediction mode appied

More information

Simplified analysis of EXAFS data and determination of bond lengths

Simplified analysis of EXAFS data and determination of bond lengths Indian Journa of Pure & Appied Physics Vo. 49, January 0, pp. 5-9 Simpified anaysis of EXAFS data and determination of bond engths A Mishra, N Parsai & B D Shrivastava * Schoo of Physics, Devi Ahiya University,

More information

Extraction of Astrophysical Cross Sections in the Trojan-Horse Method

Extraction of Astrophysical Cross Sections in the Trojan-Horse Method Few-Body Systems 29, 75±93 (2000) Extraction of Astrophysica Cross Sections in the Trojan-Horse Method S. Type and H. H. Woter Sektion Physik, Universitat Munchen, Am Couomwa 1, D-85748 Garching, Germany

More information

XI PHYSICS. M. Affan Khan LECTURER PHYSICS, AKHSS, K. https://promotephysics.wordpress.com

XI PHYSICS. M. Affan Khan LECTURER PHYSICS, AKHSS, K. https://promotephysics.wordpress.com XI PHYSICS M. Affan Khan LECTURER PHYSICS, AKHSS, K affan_414@ive.com https://promotephysics.wordpress.com [TORQUE, ANGULAR MOMENTUM & EQUILIBRIUM] CHAPTER NO. 5 Okay here we are going to discuss Rotationa

More information

Conditions for Saddle-Point Equilibria in Output-Feedback MPC with MHE

Conditions for Saddle-Point Equilibria in Output-Feedback MPC with MHE Conditions for Sadde-Point Equiibria in Output-Feedback MPC with MHE David A. Copp and João P. Hespanha Abstract A new method for soving output-feedback mode predictive contro (MPC) and moving horizon

More information

NEW DEVELOPMENT OF OPTIMAL COMPUTING BUDGET ALLOCATION FOR DISCRETE EVENT SIMULATION

NEW DEVELOPMENT OF OPTIMAL COMPUTING BUDGET ALLOCATION FOR DISCRETE EVENT SIMULATION NEW DEVELOPMENT OF OPTIMAL COMPUTING BUDGET ALLOCATION FOR DISCRETE EVENT SIMULATION Hsiao-Chang Chen Dept. of Systems Engineering University of Pennsyvania Phiadephia, PA 904-635, U.S.A. Chun-Hung Chen

More information

Data Mining Technology for Failure Prognostic of Avionics

Data Mining Technology for Failure Prognostic of Avionics IEEE Transactions on Aerospace and Eectronic Systems. Voume 38, #, pp.388-403, 00. Data Mining Technoogy for Faiure Prognostic of Avionics V.A. Skormin, Binghamton University, Binghamton, NY, 1390, USA

More information

Non-linear robust control for inverted-pendulum 2D walking

Non-linear robust control for inverted-pendulum 2D walking Non-inear robust contro for inverted-penduum 2D waking Matthew Key and Andy Ruina 2 Abstract We present an approach to high-eve contro for bipeda waking exempified with a 2D point-mass inextensibeegs inverted-penduum

More information

Lecture 6: Moderately Large Deflection Theory of Beams

Lecture 6: Moderately Large Deflection Theory of Beams Structura Mechanics 2.8 Lecture 6 Semester Yr Lecture 6: Moderatey Large Defection Theory of Beams 6.1 Genera Formuation Compare to the cassica theory of beams with infinitesima deformation, the moderatey

More information

Model Predictive Control of Interconnected Linear and Nonlinear Processes

Model Predictive Control of Interconnected Linear and Nonlinear Processes Ind. Eng. Chem. Res. 2002, 41, 801-816 801 Mode Predictive Contro of Interconnected Linear and Noninear Processes Guang-Yan Zhu and Michae A. Henson* Department of Chemica Engineering, Louisiana State

More information

Multilayer Kerceptron

Multilayer Kerceptron Mutiayer Kerceptron Zotán Szabó, András Lőrincz Department of Information Systems, Facuty of Informatics Eötvös Loránd University Pázmány Péter sétány 1/C H-1117, Budapest, Hungary e-mai: szzoi@csetehu,

More information

Path planning with PH G2 splines in R2

Path planning with PH G2 splines in R2 Path panning with PH G2 spines in R2 Laurent Gajny, Richard Béarée, Eric Nyiri, Oivier Gibaru To cite this version: Laurent Gajny, Richard Béarée, Eric Nyiri, Oivier Gibaru. Path panning with PH G2 spines

More information

A. Distribution of the test statistic

A. Distribution of the test statistic A. Distribution of the test statistic In the sequentia test, we first compute the test statistic from a mini-batch of size m. If a decision cannot be made with this statistic, we keep increasing the mini-batch

More information

Numerical Simulation for Optimizing Temperature Gradients during Single Crystal Casting Process

Numerical Simulation for Optimizing Temperature Gradients during Single Crystal Casting Process ISIJ Internationa Vo 54 (2014) No 2 pp 254 258 Numerica Simuation for Optimizing Temperature Gradients during Singe Crysta Casting Process Aeksandr Aeksandrovich INOZEMTSEV 1) Aeksandra Sergeevna DUBROVSKAYA

More information

Systems & Control Letters. State and output feedback boundary control for a coupled PDE ODE system

Systems & Control Letters. State and output feedback boundary control for a coupled PDE ODE system Systems & Contro Letters 6 () 54 545 Contents ists avaiabe at ScienceDirect Systems & Contro Letters journa homepage: wwweseviercom/ocate/syscone State output feedback boundary contro for a couped PDE

More information

Explicit overall risk minimization transductive bound

Explicit overall risk minimization transductive bound 1 Expicit overa risk minimization transductive bound Sergio Decherchi, Paoo Gastado, Sandro Ridea, Rodofo Zunino Dept. of Biophysica and Eectronic Engineering (DIBE), Genoa University Via Opera Pia 11a,

More information

Asynchronous Control for Coupled Markov Decision Systems

Asynchronous Control for Coupled Markov Decision Systems INFORMATION THEORY WORKSHOP (ITW) 22 Asynchronous Contro for Couped Marov Decision Systems Michae J. Neey University of Southern Caifornia Abstract This paper considers optima contro for a coection of

More information

SE-514 (OPTIMAL CONTROL) OPTIMAL CONTROL FOR SINGLE AND DOUBLE INVERTED PENDULUM. DONE BY: Fatai Olalekan ( Ayman Abdallah (973610)

SE-514 (OPTIMAL CONTROL) OPTIMAL CONTROL FOR SINGLE AND DOUBLE INVERTED PENDULUM. DONE BY: Fatai Olalekan ( Ayman Abdallah (973610) SE-54 (OPTIAL CONTROL OPTIAL CONTROL FOR SINGLE AND DOUBLE INVERTED PENDULU DONE BY: Fatai Oaekan (363 Ayman Abdaah (9736 PREPARED FOR: Dr. Sami E-Ferik Tabe of contents Abstract... 3 Introduction... 3

More information

12.2. Maxima and Minima. Introduction. Prerequisites. Learning Outcomes

12.2. Maxima and Minima. Introduction. Prerequisites. Learning Outcomes Maima and Minima 1. Introduction In this Section we anayse curves in the oca neighbourhood of a stationary point and, from this anaysis, deduce necessary conditions satisfied by oca maima and oca minima.

More information

On some problems of synthesis of spatial five-bar hinged mechanisms with two degrees of freedom

On some problems of synthesis of spatial five-bar hinged mechanisms with two degrees of freedom Internationa Journa of Mechanica Engineering and Appications 014 (6): 104-110 Puished onine ecemer 18, 014 (http://www.sciencepuishinggroup.com/j/ijmea) doi: 10.11648/j.ijmea.014006.14 ISSN: 330-03X (Print)

More information

DISTRIBUTION OF TEMPERATURE IN A SPATIALLY ONE- DIMENSIONAL OBJECT AS A RESULT OF THE ACTIVE POINT SOURCE

DISTRIBUTION OF TEMPERATURE IN A SPATIALLY ONE- DIMENSIONAL OBJECT AS A RESULT OF THE ACTIVE POINT SOURCE DISTRIBUTION OF TEMPERATURE IN A SPATIALLY ONE- DIMENSIONAL OBJECT AS A RESULT OF THE ACTIVE POINT SOURCE Yury Iyushin and Anton Mokeev Saint-Petersburg Mining University, Vasiievsky Isand, 1 st ine, Saint-Petersburg,

More information

c 2007 Society for Industrial and Applied Mathematics

c 2007 Society for Industrial and Applied Mathematics SIAM REVIEW Vo. 49,No. 1,pp. 111 1 c 7 Society for Industria and Appied Mathematics Domino Waves C. J. Efthimiou M. D. Johnson Abstract. Motivated by a proposa of Daykin [Probem 71-19*, SIAM Rev., 13 (1971),

More information

Independent Joint Control

Independent Joint Control ME135 ADANCED OBOICS Independent oint Contro ee-hwan yu Schoo of Mechanica Engineering Introduction to Contro Contro: deterining the tie hitory of joint input to do a coanded otion Contro ethod are depend

More information

T.C. Banwell, S. Galli. {bct, Telcordia Technologies, Inc., 445 South Street, Morristown, NJ 07960, USA

T.C. Banwell, S. Galli. {bct, Telcordia Technologies, Inc., 445 South Street, Morristown, NJ 07960, USA ON THE SYMMETRY OF THE POWER INE CHANNE T.C. Banwe, S. Gai {bct, sgai}@research.tecordia.com Tecordia Technoogies, Inc., 445 South Street, Morristown, NJ 07960, USA Abstract The indoor power ine network

More information

Worst Case Analysis of the Analog Circuits

Worst Case Analysis of the Analog Circuits Proceedings of the 11th WSEAS Internationa Conference on CIRCUITS, Agios Nikoaos, Crete Isand, Greece, Juy 3-5, 7 9 Worst Case Anaysis of the Anaog Circuits ELENA NICULESCU*, DORINA-MIOARA PURCARU* and

More information

A Statistical Framework for Real-time Event Detection in Power Systems

A Statistical Framework for Real-time Event Detection in Power Systems 1 A Statistica Framework for Rea-time Event Detection in Power Systems Noan Uhrich, Tim Christman, Phiip Swisher, and Xichen Jiang Abstract A quickest change detection (QCD) agorithm is appied to the probem

More information

STABILITY OF A PARAMETRICALLY EXCITED DAMPED INVERTED PENDULUM 1. INTRODUCTION

STABILITY OF A PARAMETRICALLY EXCITED DAMPED INVERTED PENDULUM 1. INTRODUCTION Journa of Sound and Vibration (996) 98(5), 643 65 STABILITY OF A PARAMETRICALLY EXCITED DAMPED INVERTED PENDULUM G. ERDOS AND T. SINGH Department of Mechanica and Aerospace Engineering, SUNY at Buffao,

More information

APPENDIX C FLEXING OF LENGTH BARS

APPENDIX C FLEXING OF LENGTH BARS Fexing of ength bars 83 APPENDIX C FLEXING OF LENGTH BARS C.1 FLEXING OF A LENGTH BAR DUE TO ITS OWN WEIGHT Any object ying in a horizonta pane wi sag under its own weight uness it is infinitey stiff or

More information

Scalable Spectrum Allocation for Large Networks Based on Sparse Optimization

Scalable Spectrum Allocation for Large Networks Based on Sparse Optimization Scaabe Spectrum ocation for Large Networks ased on Sparse Optimization innan Zhuang Modem R&D Lab Samsung Semiconductor, Inc. San Diego, C Dongning Guo, Ermin Wei, and Michae L. Honig Department of Eectrica

More information

Optimization Based Bidding Strategies in the Deregulated Market

Optimization Based Bidding Strategies in the Deregulated Market Optimization ased idding Strategies in the Dereguated arket Daoyuan Zhang Ascend Communications, nc 866 North ain Street, Waingford, C 0649 Abstract With the dereguation of eectric power systems, market

More information

A proposed nonparametric mixture density estimation using B-spline functions

A proposed nonparametric mixture density estimation using B-spline functions A proposed nonparametric mixture density estimation using B-spine functions Atizez Hadrich a,b, Mourad Zribi a, Afif Masmoudi b a Laboratoire d Informatique Signa et Image de a Côte d Opae (LISIC-EA 4491),

More information

1 Equations of Motion 3: Equivalent System Method

1 Equations of Motion 3: Equivalent System Method 8 Mechanica Vibrations Equations of Motion : Equivaent System Method In systems in which masses are joined by rigid ins, evers, or gears and in some distributed systems, various springs, dampers, and masses

More information

Vibrations of beams with a variable cross-section fixed on rotational rigid disks

Vibrations of beams with a variable cross-section fixed on rotational rigid disks 1(13) 39 57 Vibrations of beams with a variabe cross-section fixed on rotationa rigid disks Abstract The work is focused on the probem of vibrating beams with a variabe cross-section fixed on a rotationa

More information

Symbolic models for nonlinear control systems using approximate bisimulation

Symbolic models for nonlinear control systems using approximate bisimulation Symboic modes for noninear contro systems using approximate bisimuation Giordano Poa, Antoine Girard and Pauo Tabuada Abstract Contro systems are usuay modeed by differentia equations describing how physica

More information

Modal analysis of a multi-blade system undergoing rotational motion

Modal analysis of a multi-blade system undergoing rotational motion Journa of Mechanica Science and Technoogy 3 (9) 5~58 Journa of Mechanica Science and Technoogy www.springerin.com/content/738-494x DOI.7/s6-9-43-3 Moda anaysis of a muti-bade system undergoing rotationa

More information

Disturbance decoupling by measurement feedback

Disturbance decoupling by measurement feedback Preprints of the 19th Word Congress The Internationa Federation of Automatic Contro Disturbance decouping by measurement feedback Arvo Kadmäe, Üe Kotta Institute of Cybernetics at TUT, Akadeemia tee 21,

More information

In this context, system identification is an important component

In this context, system identification is an important component 211 th IEEE Conference on Decision and Contro and European Contro Conference (CDC-ECC) Orando, FL, USA, December 12-1, 211 An improved strategy for NeuroMuscuar Bockade contro with parameter uncertainty

More information

Proceedings of Meetings on Acoustics

Proceedings of Meetings on Acoustics Proceedings of Meetings on Acoustics Voume 19, 213 http://acousticasociety.org/ ICA 213 Montrea Montrea, Canada 2-7 June 213 Underwater Acoustics Session 1pUW: Seabed Scattering: Measurements and Mechanisms

More information

arxiv: v1 [math.ca] 6 Mar 2017

arxiv: v1 [math.ca] 6 Mar 2017 Indefinite Integras of Spherica Besse Functions MIT-CTP/487 arxiv:703.0648v [math.ca] 6 Mar 07 Joyon K. Boomfied,, Stephen H. P. Face,, and Zander Moss, Center for Theoretica Physics, Laboratory for Nucear

More information

DIGITAL FILTER DESIGN OF IIR FILTERS USING REAL VALUED GENETIC ALGORITHM

DIGITAL FILTER DESIGN OF IIR FILTERS USING REAL VALUED GENETIC ALGORITHM DIGITAL FILTER DESIGN OF IIR FILTERS USING REAL VALUED GENETIC ALGORITHM MIKAEL NILSSON, MATTIAS DAHL AND INGVAR CLAESSON Bekinge Institute of Technoogy Department of Teecommunications and Signa Processing

More information

A Solution to the 4-bit Parity Problem with a Single Quaternary Neuron

A Solution to the 4-bit Parity Problem with a Single Quaternary Neuron Neura Information Processing - Letters and Reviews Vo. 5, No. 2, November 2004 LETTER A Soution to the 4-bit Parity Probem with a Singe Quaternary Neuron Tohru Nitta Nationa Institute of Advanced Industria

More information

FORECASTING TELECOMMUNICATIONS DATA WITH AUTOREGRESSIVE INTEGRATED MOVING AVERAGE MODELS

FORECASTING TELECOMMUNICATIONS DATA WITH AUTOREGRESSIVE INTEGRATED MOVING AVERAGE MODELS FORECASTING TEECOMMUNICATIONS DATA WITH AUTOREGRESSIVE INTEGRATED MOVING AVERAGE MODES Niesh Subhash naawade a, Mrs. Meenakshi Pawar b a SVERI's Coege of Engineering, Pandharpur. nieshsubhash15@gmai.com

More information

Torsion and shear stresses due to shear centre eccentricity in SCIA Engineer Delft University of Technology. Marijn Drillenburg

Torsion and shear stresses due to shear centre eccentricity in SCIA Engineer Delft University of Technology. Marijn Drillenburg Torsion and shear stresses due to shear centre eccentricity in SCIA Engineer Deft University of Technoogy Marijn Drienburg October 2017 Contents 1 Introduction 2 1.1 Hand Cacuation....................................

More information

Distributed average consensus: Beyond the realm of linearity

Distributed average consensus: Beyond the realm of linearity Distributed average consensus: Beyond the ream of inearity Usman A. Khan, Soummya Kar, and José M. F. Moura Department of Eectrica and Computer Engineering Carnegie Meon University 5 Forbes Ave, Pittsburgh,

More information

Two Kinds of Parabolic Equation algorithms in the Computational Electromagnetics

Two Kinds of Parabolic Equation algorithms in the Computational Electromagnetics Avaiabe onine at www.sciencedirect.com Procedia Engineering 9 (0) 45 49 0 Internationa Workshop on Information and Eectronics Engineering (IWIEE) Two Kinds of Paraboic Equation agorithms in the Computationa

More information

Modeling Friction Phenomena in Flexible Multibody Dynamics

Modeling Friction Phenomena in Flexible Multibody Dynamics Modeing Friction Phenomena in Fexibe Mutibody Dynamics Oivier A. Bauchau and Changuan Ju Danie Guggenheim Schoo of Aerospace Engineering, Georgia Institute of Technoogy, 270 Ferst Dr., Atanta, GA 30332,

More information

arxiv:nlin/ v2 [nlin.cd] 30 Jan 2006

arxiv:nlin/ v2 [nlin.cd] 30 Jan 2006 expansions in semicassica theories for systems with smooth potentias and discrete symmetries Hoger Cartarius, Jörg Main, and Günter Wunner arxiv:nin/0510051v [nin.cd] 30 Jan 006 1. Institut für Theoretische

More information

Physics 235 Chapter 8. Chapter 8 Central-Force Motion

Physics 235 Chapter 8. Chapter 8 Central-Force Motion Physics 35 Chapter 8 Chapter 8 Centra-Force Motion In this Chapter we wi use the theory we have discussed in Chapter 6 and 7 and appy it to very important probems in physics, in which we study the motion

More information

Distribution Systems Voltage Profile Improvement with Series FACTS Devices Using Line Flow-Based Equations

Distribution Systems Voltage Profile Improvement with Series FACTS Devices Using Line Flow-Based Equations 16th NATIONAL POWER SYSTEMS CONFERENCE, 15th-17th DECEMBER, 010 386 Distribution Systems otage Profie Improvement with Series FACTS Devices Using Line Fow-Based Equations K. enkateswararao, P. K. Agarwa

More information

LECTURE 10. The world of pendula

LECTURE 10. The world of pendula LECTURE 0 The word of pendua For the next few ectures we are going to ook at the word of the pane penduum (Figure 0.). In a previous probem set we showed that we coud use the Euer- Lagrange method to derive

More information

TIME-VARYING LINEAR OBSERVER FOR TORQUE BALANCING ON A DI ENGINE

TIME-VARYING LINEAR OBSERVER FOR TORQUE BALANCING ON A DI ENGINE TIME-VARYING LINEAR OBSERVER FOR TORQUE BALANCING ON A DI ENGINE Jonathan Chauvin Gie Corde Phiippe Mouin Miche Castagné Nicoas Petit Pierre Rouchon Centre Automatique et Systèmes, Écoe des Mines de Paris,

More information

In-plane shear stiffness of bare steel deck through shell finite element models. G. Bian, B.W. Schafer. June 2017

In-plane shear stiffness of bare steel deck through shell finite element models. G. Bian, B.W. Schafer. June 2017 In-pane shear stiffness of bare stee deck through she finite eement modes G. Bian, B.W. Schafer June 7 COLD-FORMED STEEL RESEARCH CONSORTIUM REPORT SERIES CFSRC R-7- SDII Stee Diaphragm Innovation Initiative

More information

A unified framework for design and analysis of networked and quantized control systems

A unified framework for design and analysis of networked and quantized control systems 1 A unified framework for design and anaysis of networked and quantized contro systems Dragan ešić and Danie Liberzon Abstract We generaize and unify a range of recent resuts in quantized contro systems

More information

Radar/ESM Tracking of Constant Velocity Target : Comparison of Batch (MLE) and EKF Performance

Radar/ESM Tracking of Constant Velocity Target : Comparison of Batch (MLE) and EKF Performance adar/ racing of Constant Veocity arget : Comparison of Batch (LE) and EKF Performance I. Leibowicz homson-csf Deteis/IISA La cef de Saint-Pierre 1 Bd Jean ouin 7885 Eancourt Cede France Isabee.Leibowicz

More information

Numerical solution of one dimensional contaminant transport equation with variable coefficient (temporal) by using Haar wavelet

Numerical solution of one dimensional contaminant transport equation with variable coefficient (temporal) by using Haar wavelet Goba Journa of Pure and Appied Mathematics. ISSN 973-1768 Voume 1, Number (16), pp. 183-19 Research India Pubications http://www.ripubication.com Numerica soution of one dimensiona contaminant transport

More information

Design and System Modeling of a Tri-Axial Microaccelerometer Using Piezoelectric Thin Films

Design and System Modeling of a Tri-Axial Microaccelerometer Using Piezoelectric Thin Films Ferroeectrics, 85:, 69 74, 009 Reprints avaiae directy fro the puisher DOI:.80/00509090888764 URL: http://dx.doi.org/.80/00509090888764 69 Jyh-Cheng Yu et a. 009 Tayor & Francis ISSN: 005-09 print / 56-5

More information

A simple reliability block diagram method for safety integrity verification

A simple reliability block diagram method for safety integrity verification Reiabiity Engineering and System Safety 92 (2007) 1267 1273 www.esevier.com/ocate/ress A simpe reiabiity bock diagram method for safety integrity verification Haitao Guo, Xianhui Yang epartment of Automation,

More information

FEMAG: A High Performance Parallel Finite Element Toolbox for Electromagnetic Computations

FEMAG: A High Performance Parallel Finite Element Toolbox for Electromagnetic Computations Internationa Journa of Energy and Power Engineering 2016; 5(1-1): 57-64 Pubished onine November 28, 2015 (http://www.sciencepubishinggroup.com/j/ijepe) doi: 10.11648/j.ijepe.s.2016050101.19 ISSN: 2326-957X

More information

Unconditional security of differential phase shift quantum key distribution

Unconditional security of differential phase shift quantum key distribution Unconditiona security of differentia phase shift quantum key distribution Kai Wen, Yoshihisa Yamamoto Ginzton Lab and Dept of Eectrica Engineering Stanford University Basic idea of DPS-QKD Protoco. Aice

More information

2-loop additive mass renormalization with clover fermions and Symanzik improved gluons

2-loop additive mass renormalization with clover fermions and Symanzik improved gluons 2-oop additive mass renormaization with cover fermions and Symanzik improved guons Apostoos Skouroupathis Department of Physics, University of Cyprus, Nicosia, CY-1678, Cyprus E-mai: php4as01@ucy.ac.cy

More information

DYNAMIC MODELLING OF A TWO-LINK FLEXIBLE MANIPULATOR MOHAMAD HAFIS IZRAN BIN ISHAK UNIVERSITI TEKNOLOGI MALAYSIA

DYNAMIC MODELLING OF A TWO-LINK FLEXIBLE MANIPULATOR MOHAMAD HAFIS IZRAN BIN ISHAK UNIVERSITI TEKNOLOGI MALAYSIA DYNAIC ODELLING OF A TWO-LINK FLEXIBLE ANIPULATOR OHAAD HAFIS IZRAN BIN ISHAK UNIVERSITI TEKNOLOGI ALAYSIA DYNAIC ODELLING OF A TWO-LINK FLEXIBLE ANIPULATOR OHAAD HAFIS IZRAN B ISHAK A proect report submitted

More information

On the Development of a Walking Rehabilitation Device with a Large Workspace

On the Development of a Walking Rehabilitation Device with a Large Workspace 2011 IEEE Internationa Conference on Rehabiitation Robotics Rehab Week Zurich, ETH Zurich Science City, Switzerand, June 29 - Juy 1, 2011 On the Deveopment of a Waking Rehabiitation Device with a Large

More information

International Journal of Advance Engineering and Research Development

International Journal of Advance Engineering and Research Development Scientific Journa of Impact Factor (SJIF): 4.4 Internationa Journa of Advance Engineering and Research Deveopment Voume 3, Issue 3, March -206 e-issn (O): 2348-4470 p-issn (P): 2348-6406 Study and comparison

More information

D. Prémel, J.M. Decitre and G. Pichenot. CEA, LIST, F Gif-sur-Yvette, France

D. Prémel, J.M. Decitre and G. Pichenot. CEA, LIST, F Gif-sur-Yvette, France SIMULATION OF EDDY CURRENT INSPECTION INCLUDING MAGNETIC FIELD SENSOR SUCH AS A GIANT MAGNETO-RESISTANCE OVER PLANAR STRATIFIED MEDIA COMPONENTS WITH EMBEDDED FLAWS D. Préme, J.M. Decitre and G. Pichenot

More information

The Third Group of Spacial Distribution of Magnetic Leakage Field Yielded by A Rectangular Slot on The Workpiece Surface

The Third Group of Spacial Distribution of Magnetic Leakage Field Yielded by A Rectangular Slot on The Workpiece Surface 7th Word Conference on Nondestructive Testing, 5-8 Oct 8, Shanghai, China The Third Group of Spacia Distriution of Magnetic Leakage Fied Yieded y A Rectanguar Sot on The Workpiece Surface Astract Wei-Chang

More information

Solution Set Seven. 1 Goldstein Components of Torque Along Principal Axes Components of Torque Along Cartesian Axes...

Solution Set Seven. 1 Goldstein Components of Torque Along Principal Axes Components of Torque Along Cartesian Axes... : Soution Set Seven Northwestern University, Cassica Mechanics Cassica Mechanics, Third Ed.- Godstein November 8, 25 Contents Godstein 5.8. 2. Components of Torque Aong Principa Axes.......................

More information

The EM Algorithm applied to determining new limit points of Mahler measures

The EM Algorithm applied to determining new limit points of Mahler measures Contro and Cybernetics vo. 39 (2010) No. 4 The EM Agorithm appied to determining new imit points of Maher measures by Souad E Otmani, Georges Rhin and Jean-Marc Sac-Épée Université Pau Veraine-Metz, LMAM,

More information

ASummaryofGaussianProcesses Coryn A.L. Bailer-Jones

ASummaryofGaussianProcesses Coryn A.L. Bailer-Jones ASummaryofGaussianProcesses Coryn A.L. Baier-Jones Cavendish Laboratory University of Cambridge caj@mrao.cam.ac.uk Introduction A genera prediction probem can be posed as foows. We consider that the variabe

More information