Distributed control of "ball on beam" system

Size: px
Start display at page:

Download "Distributed control of "ball on beam" system"

Transcription

1 XI International PhD Workshop OWD 29, 17 2 Octoer 29 Distriuted control of "all on eam" system Michał Ganois, University of Science and Technology AGH Astract This paper presents possiilities of control for unstale dynamic systems asing on "all on eam" example. First section is a short introduction. In the second section, system is presented - its structure, equations and equilirium points. Using 1st Lapunov method and Kalman matrix it is proven that the system is unstale, ut controllale. Third section shortly descries design of LQR controller for the "all on eam". In the fourth part short description of simulation framework (Matla/Simulink, TrueTime lirary) is introduced. The influence of specific parameters of Ethernet (such as throughput, proaility of losing packet, and minimal frame size) on control quality is descried. It is shown, that insufficient network parameters can destailize control loop. The last part of the paper is a proposition of control loop design using uffers. It is proven that appropriate uffers and simple oserver are sufficient to design asymptotically stale control for "all and eam" system. 1. Introduction Distriuted control systems are significant part of a modern automatic control. Its applications can e found in many kind of industries, as oil refining, power stations, automotive, and many others. In these systems, measurements and process itself are separated, and communicate via network (e.g. Ethernet, Modus or CAN) - as a result, influence of a network has to e taken into consideration. Fig. 1. "Ball on eam" system A "all on eam" is a well-known example of unstale, controllale dynamic system. Simplicity and possiility of constructing a real oject in laoratory make it one of the most popular examples in control theory. Additionally, "all and eam" can e used as a simple model of more complicated prolems related with variale moment of inertia (e.g. stailizing of airplane flight or root manipulators). 2. Control system System consists of rotating eam, and a solid all rolling on it. We assume eam s torque as an input. The structure of the system is presented on figure (1). We assume, that: all does not slide on the eam there is no dynamic friction in the system the all is perfectly round and homogeneous the all has a constant contact with the eam the eam is perfectly flat and symmetric State equations for the system descried aove are as follow (see [3] or [1]) 479

2 ẋ 1 = x 2 (1) ẋ 2 = a(x 1 x 4 2 g sin x 3 ) (2) ẋ 3 = x 4 (3) ẋ 4 = 2x 1 x 2 x 4 g x 1 cos x 3 x u x (4) where x 1 - position of the all [m] x 2 - velocity of the all [m/s] x 3 - angular position of the eam [rad] x 4 - angular velocity of the eam [rad/s] I =.1 - eam s moment of interia [k g m 2 ] I - all s moment of inertia [k g m 2 ] m =.1, R =.1 - weight [k g] and radius [m] of the all a = 1 1+ I mr 2 = I +I m System (1) can e linearized in its equilirium point (x = [,,,]). Jacoi matrix of this system takes form J (x) = where 1 2 ax 4 ga cos x 3 2ax 1 x 4 f 1 (x) f 2 (x) f 3 (x) f 4 (x) f 1 (x) = 2x 2 x 4 g cos x 3 + x (2x 1 x 2 x 4 + g x 1 cos x 3 )x 1 (x ) 2 f 2 (x) = 2x 1 x 4 x f 3 (x) = g x 1 sin x 3 x f 4 (x) = 2x 1 x 2 x In the equilirium point we have J (x s ) = 1 ga 1 g where eigenvalues of J are λ 1 = p λ 2 = p λ 3 = j p λ 4 = j p with p = 4 g 2 3 a, j 2 = 1 For positive values a,, Re(λ 1 ) > - the system is unstale. Oservaility of the system can e proven using Kalman matrix (see e.g. [4]), which takes a form ga Q = ga 1 1 (5) Because detq >, system is considered oservale. 3. Optimal control of "Ball on eam" system This section shortly presents an optimal control of the system using LQR controller, i.e. minimizing quality index given y (6) Q(u) = (x(t) Qx(t) + u(t) Ru(t))d t (6) with assumptions Q = Q, R = R, Q R > In further experiments we assume Q = I, R =.1 Solving Riccati s equation for linearized system leads us to the controller vector 48

3 Fig. 2. Trajectories for closed loop (LQR) K = [ ] (7) Trajectories of the system with aove controller are presented on figure (2) Fig. 3. Simulink model of the system 4. Distriuted control via Ethernet and its simulations Control loop for "all on eam" system via Ethernet network was simulated using MAT- LAB/Simulink environment and TrueTime lirary (see [5]). Full simulation system is presented on figure (3). The most important parts are: "Ball on eam" lock - represents model of the system, designed using equations (1) "Sensor" lock - represents a sensor, its responsiility is a conversion of measurements to digital form appropriate for Ethernet network "Controller" - represents a digital controller "Actuator" - represents actuator, which converts data received via Ethernet to input for "all on eam" system. "Network" - represents model of Ethernet network To measure a quality of control, we use an integral of squared error in finite time T = 5 J (x,t ) = 4 ( i=1 T x 2 i d t) (8) Default parameters for simulations were: throughput DR = 18 /s proaility of packet loss LP = Fig. 4. Influence of throughput minimal frame size MFS = 46 octets Influence of particular network parameters are presented on plots (4), (5), (6). It can e noticed, that throughput elow 75/s causes with worse quality of control. Destailization of the system occurs for aout 6/s. Similarly, too ig value of minimal frame size also causes with destailization (control systems should use ig amount of small packets - this is the reason why too ig minimal frame size is not appropriate for control purposes). Interesting results can also e otained when proaility of losing packet is changed - quality of control decreases rapidly for some values (plot has a shape of "stairs"). Staility is lost for aout

4 Introduce a new state variales, related with delays of the uffers Design discrete controller for otained system First of all, discrete form (as elow) of the system is needed. x(k + 1) = A d x(k) + B d u(k) (9) y(k + 1) = C d x(k) (1) Appropriate matrices can e calculated using equations Fig. 5. Influence of packet loss proaility A d = e AT (11) B d = T e AT Bd t (12) C d = C (13) As a result, for sampling time T =.1, the following matrices are otained Fig. 6. Influence of minimal frame size 5. Design of distriuted control system Typical approach to design of distriuted control systems is to design a system neglecting its distriuted character, and then analyzing the influence of the network in various aspects (as e.g. delays) [2]. In this section, some methodology using uffers will e presented, and applied to "all on eam" system. The main prolem for distriuted control systems (e.g. via Ethernet) is a variale delay introduced y network. This prolem can e solved y introducing uffers - after such introduction, system has constant delays, which are easier to handle. The main idea of presented approach is as follows: Create discrete-time model of the system Determine max delay of the network Add uffers to the system to make delays constant A d = B d = (14) (15) C d = (16) In the second step we determine network delay. Experiments have proven, that the iggest otained delay was way smaller than discretization step T =.1. Third step is adding uffers on input and output of the system. Because delays are smaller than discretization step, one-sample uffers are sufficient. System with uffers is presented on figure (7) Now we have discrete system with one-step delay on input and all outputs. For discrete systems, it is possile to treat one-step delay as a new state variale. Using this approach, we otain extended state space, defined as 482

5 Fig. 7. Control system with uffers x(k + 1) z(k + 1) where = Ad T Γ 1 (τ) = e As Bd s, Γ (τ) = T τ Γ 1 (τ) x(k) + z(k) Γ (τ) + u(k) (17) 1 T τ e A sbd s (18) Then, using equation (17),(18) (see e.g. [2]) all delays can e incorporated. A new 9-rank system is created, with matrices as presented elow A e = B d A d C d B e = 1... C e = I n n (19) (2) (21) To create optimal LQR controller, full state of the system has to e known. To otain the full state, a simple oserver is introduced, asing on the following rules: x 1 is a control one sample efore x 2 5 can e otained asing on output (i.e. the state delayed for one sample), and internal system model x 6 9 are availale directly as an output Basing on aove system, DLQR controller parameters can e calculated: Fig. 8. DLQR with state oserver K e2 = [ ] (22) As one can see on figure (8), trajectories of the system with aove controller are asymptotically stale 6. Conclusions In this paper, a method for design distriuted control via Ethernet for "all on eam" system is presented. Model of the system in a form of differential state equations is introduced. Basic properties, as instaility and controllaility of the system are proven. The influence of particular network parameters as throughput, proaility of frame loss, and minimal size of a frame are shown. A method for design control system with compensation of variale delay using uffers is proposed. The simulations show that system with such controller guarantees stailization of the system. Biliography [1] Michał Ganois. Przegląd możliwości sterowania systemem o zmiennym momencie ezwładności typu all on eam. Automatyka, Uczelniane Wydawnictwa Naukowo-Techniczne AGH, 12(2):197 21, 28. [2] Wojciech Grega. Metody i algorytmy sterowania cyfowego w układach scentralizowanych i rozproszonych. Uczelniane Wydawnictwa Naukowo- Dydaktyczne, AGH w Krakowie, 24. [3] Wojciech Mitkowski Jerzy Baranowski, Michał Ganois. Oserver design for variale moment of inertia system. Materiały konferencji Computer Methods and Systems,

6 [4] Wojciech Mitkowski. Stailizacja Systemów Dynamicznych. Wydawnictwo AGH, Kraków, [5] Martin Ohlin, Dan Henriksson, and Anton Cervin. TrueTime Reference Manual. Department of Automatic Control, Lund University, 27. Authors: M.Sc.Michał Ganois University of Science and Technology AGH al.mickiewicza Kraków ganois@agh.edu.pl This work was supported y Ministry of Science and Higher Education in Poland in the years as a research project No N N

Electricity Market Modelling Using Dynamic LQ Games

Electricity Market Modelling Using Dynamic LQ Games XII International PhD Workshop OWD 1, 3-6 October 1 Electricity Market Modelling Using Dynamic LQ Games Michał Ganobis, Institute of Automatics, AGH ( 6.11.9, prof. Wojciech Mitkowski, University of Science

More information

Math 216 Second Midterm 28 March, 2013

Math 216 Second Midterm 28 March, 2013 Math 26 Second Midterm 28 March, 23 This sample exam is provided to serve as one component of your studying for this exam in this course. Please note that it is not guaranteed to cover the material that

More information

Effect of Uniform Horizontal Magnetic Field on Thermal Instability in A Rotating Micropolar Fluid Saturating A Porous Medium

Effect of Uniform Horizontal Magnetic Field on Thermal Instability in A Rotating Micropolar Fluid Saturating A Porous Medium IOSR Journal of Mathematics (IOSR-JM) e-issn: 78-578, p-issn: 39-765X. Volume, Issue Ver. III (Jan. - Fe. 06), 5-65 www.iosrjournals.org Effect of Uniform Horizontal Magnetic Field on Thermal Instaility

More information

A Novel Ball on Beam Stabilizing Platform with Inertial Sensors Part II: Hybrid Controller Design: Partial Pole Assignment & Rapid Control Prototyping

A Novel Ball on Beam Stabilizing Platform with Inertial Sensors Part II: Hybrid Controller Design: Partial Pole Assignment & Rapid Control Prototyping Vol. 6, No., A Novel Ball on Beam Stailizing Platform with Inertial Sensors Part II: Hyrid Controller Design: Partial Pole Assignment & Rapid Control Prototyping Ali Shahaz Haider Control Systems Laoratory

More information

Section 8.5. z(t) = be ix(t). (8.5.1) Figure A pendulum. ż = ibẋe ix (8.5.2) (8.5.3) = ( bẋ 2 cos(x) bẍ sin(x)) + i( bẋ 2 sin(x) + bẍ cos(x)).

Section 8.5. z(t) = be ix(t). (8.5.1) Figure A pendulum. ż = ibẋe ix (8.5.2) (8.5.3) = ( bẋ 2 cos(x) bẍ sin(x)) + i( bẋ 2 sin(x) + bẍ cos(x)). Difference Equations to Differential Equations Section 8.5 Applications: Pendulums Mass-Spring Systems In this section we will investigate two applications of our work in Section 8.4. First, we will consider

More information

Comments on A Time Delay Controller for Systems with Uncertain Dynamics

Comments on A Time Delay Controller for Systems with Uncertain Dynamics Comments on A Time Delay Controller for Systems with Uncertain Dynamics Qing-Chang Zhong Dept. of Electrical & Electronic Engineering Imperial College of Science, Technology, and Medicine Exhiition Rd.,

More information

Chapter #6 EEE State Space Analysis and Controller Design

Chapter #6 EEE State Space Analysis and Controller Design hapter #6 EEE3-83 State Space nalsis and ontroller Design State feedack Linear Quadratic Regulator (LQR) Open and closed loop estimators Reduced Order Estimators (not assessed) racking Module Leader: Dr

More information

Modelling and Gain Scheduled Control of a Tailless Fighter

Modelling and Gain Scheduled Control of a Tailless Fighter Modelling and Gain Scheduled Control of a Tailless Fighter Nico G. M. Rademakers a, Rini kmeliawati, Roin Hill, Cees Bil c, Henk Nijmeijer a a Department of Mechanical Engineering Mathematics and Statistics

More information

CAP Plan, Activity, and Intent Recognition

CAP Plan, Activity, and Intent Recognition CAP6938-02 Plan, Activity, and Intent Recognition Lecture 10: Sequential Decision-Making Under Uncertainty (part 1) MDPs and POMDPs Instructor: Dr. Gita Sukthankar Email: gitars@eecs.ucf.edu SP2-1 Reminder

More information

PARAMETER IDENTIFICATION, MODELING, AND SIMULATION OF A CART AND PENDULUM

PARAMETER IDENTIFICATION, MODELING, AND SIMULATION OF A CART AND PENDULUM PARAMETER IDENTIFICATION, MODELING, AND SIMULATION OF A CART AND PENDULUM Erin Bender Mechanical Engineering Erin.N.Bender@Rose-Hulman.edu ABSTRACT In this paper a freely rotating pendulum suspended from

More information

FinQuiz Notes

FinQuiz Notes Reading 9 A time series is any series of data that varies over time e.g. the quarterly sales for a company during the past five years or daily returns of a security. When assumptions of the regression

More information

sc Control Systems Design Q.1, Sem.1, Ac. Yr. 2010/11

sc Control Systems Design Q.1, Sem.1, Ac. Yr. 2010/11 sc46 - Control Systems Design Q Sem Ac Yr / Mock Exam originally given November 5 9 Notes: Please be reminded that only an A4 paper with formulas may be used during the exam no other material is to be

More information

Quadratic Stability and Singular SISO Switching Systems

Quadratic Stability and Singular SISO Switching Systems 274 IEEE RANSACIONS ON AUOMAIC CONROL, VOL. 54, NO., NOVEMBER 2009 [25] V. V. Veeravalli,. Başar, and H. V. Poor, Decentralized sequential detection with a fusion center performing the sequential test,

More information

Generalized Seasonal Tapered Block Bootstrap

Generalized Seasonal Tapered Block Bootstrap Generalized Seasonal Tapered Block Bootstrap Anna E. Dudek 1, Efstathios Paparoditis 2, Dimitris N. Politis 3 Astract In this paper a new lock ootstrap method for periodic times series called Generalized

More information

On Temporal Instability of Electrically Forced Axisymmetric Jets with Variable Applied Field and Nonzero Basic State Velocity

On Temporal Instability of Electrically Forced Axisymmetric Jets with Variable Applied Field and Nonzero Basic State Velocity Availale at http://pvamu.edu/aam Appl. Appl. Math. ISSN: 19-966 Vol. 6, Issue 1 (June 11) pp. 7 (Previously, Vol. 6, Issue 11, pp. 1767 178) Applications and Applied Mathematics: An International Journal

More information

DESIGN SUPPORT FOR MOTION CONTROL SYSTEMS Application to the Philips Fast Component Mounter

DESIGN SUPPORT FOR MOTION CONTROL SYSTEMS Application to the Philips Fast Component Mounter DESIGN SUPPORT FOR MOTION CONTROL SYSTEMS Application to the Philips Fast Component Mounter Hendri J. Coelingh, Theo J.A. de Vries and Jo van Amerongen Dreel Institute for Systems Engineering, EL-RT, University

More information

1 Systems of Differential Equations

1 Systems of Differential Equations March, 20 7- Systems of Differential Equations Let U e an open suset of R n, I e an open interval in R and : I R n R n e a function from I R n to R n The equation ẋ = ft, x is called a first order ordinary

More information

Solution: (a) (b) (N) F X =0: A X =0 (N) F Y =0: A Y + B Y (54)(9.81) 36(9.81)=0

Solution: (a) (b) (N) F X =0: A X =0 (N) F Y =0: A Y + B Y (54)(9.81) 36(9.81)=0 Prolem 5.6 The masses of the person and the diving oard are 54 kg and 36 kg, respectivel. ssume that the are in equilirium. (a) Draw the free-od diagram of the diving oard. () Determine the reactions at

More information

Computers Methods for Chaos Diagnostic

Computers Methods for Chaos Diagnostic AUTOMATYKA 2011 Tom 15 Zeszyt 1 Anna Obrączka Computers Methods for Chaos Diagnostic 1. Introduction In this article some computer methods for chaos diagnostic were presented. These methods are based on

More information

The Robust H Control for Inhibition of Load on Offshore Wind Turbines Variable Pitch Control Ping JIANG1,2, SHU-zhen GUO1

The Robust H Control for Inhibition of Load on Offshore Wind Turbines Variable Pitch Control Ping JIANG1,2, SHU-zhen GUO1 3rd International Conference on Machinery, Materials and Information echnology Applications (ICMMIA 25) he Roust H Control for Inhiition of Load on Offshore Wind urines Variale Pitch Control Ping JIANG,2,

More information

Stability Domain of a Linear Differential Equation with Two Delays

Stability Domain of a Linear Differential Equation with Two Delays ELSEVIER An International Journal Availale online at www.sciencedirect.com computers &.c,..c. ~--~c,..c.. mathematics with applications Computers and Mathematics with Applications 51 (2006) 153-159 www.elsevier.com/locate/camwa

More information

Representation theory of SU(2), density operators, purification Michael Walter, University of Amsterdam

Representation theory of SU(2), density operators, purification Michael Walter, University of Amsterdam Symmetry and Quantum Information Feruary 6, 018 Representation theory of S(), density operators, purification Lecture 7 Michael Walter, niversity of Amsterdam Last week, we learned the asic concepts of

More information

ROUNDOFF ERRORS; BACKWARD STABILITY

ROUNDOFF ERRORS; BACKWARD STABILITY SECTION.5 ROUNDOFF ERRORS; BACKWARD STABILITY ROUNDOFF ERROR -- error due to the finite representation (usually in floatingpoint form) of real (and complex) numers in digital computers. FLOATING-POINT

More information

ME 323 Examination #2

ME 323 Examination #2 ME 33 Eamination # SOUTION Novemer 14, 17 ROEM NO. 1 3 points ma. The cantilever eam D of the ending stiffness is sujected to a concentrated moment M at C. The eam is also supported y a roller at. Using

More information

Travel Grouping of Evaporating Polydisperse Droplets in Oscillating Flow- Theoretical Analysis

Travel Grouping of Evaporating Polydisperse Droplets in Oscillating Flow- Theoretical Analysis Travel Grouping of Evaporating Polydisperse Droplets in Oscillating Flow- Theoretical Analysis DAVID KATOSHEVSKI Department of Biotechnology and Environmental Engineering Ben-Gurion niversity of the Negev

More information

Design Variable Concepts 19 Mar 09 Lab 7 Lecture Notes

Design Variable Concepts 19 Mar 09 Lab 7 Lecture Notes Design Variale Concepts 19 Mar 09 La 7 Lecture Notes Nomenclature W total weight (= W wing + W fuse + W pay ) reference area (wing area) wing aspect ratio c r root wing chord c t tip wing chord λ taper

More information

Buckling Behavior of Long Symmetrically Laminated Plates Subjected to Shear and Linearly Varying Axial Edge Loads

Buckling Behavior of Long Symmetrically Laminated Plates Subjected to Shear and Linearly Varying Axial Edge Loads NASA Technical Paper 3659 Buckling Behavior of Long Symmetrically Laminated Plates Sujected to Shear and Linearly Varying Axial Edge Loads Michael P. Nemeth Langley Research Center Hampton, Virginia National

More information

Investigation of a Ball Screw Feed Drive System Based on Dynamic Modeling for Motion Control

Investigation of a Ball Screw Feed Drive System Based on Dynamic Modeling for Motion Control Investigation of a Ball Screw Feed Drive System Based on Dynamic Modeling for Motion Control Yi-Cheng Huang *, Xiang-Yuan Chen Department of Mechatronics Engineering, National Changhua University of Education,

More information

Simple Examples. Let s look at a few simple examples of OI analysis.

Simple Examples. Let s look at a few simple examples of OI analysis. Simple Examples Let s look at a few simple examples of OI analysis. Example 1: Consider a scalar prolem. We have one oservation y which is located at the analysis point. We also have a ackground estimate

More information

ENGINEERING COMPUTATION Second Year Lectures. Stephen Roberts Michaelmas Term

ENGINEERING COMPUTATION Second Year Lectures. Stephen Roberts Michaelmas Term ENGINEERING COMPUTATION Second Year Lectures Stephen Roerts Michaelmas Term Engineering Computation ENGINEERING COMPUTATION Second Year Lectures Stephen Roerts Michaelmas Term The handouts are rief lecture

More information

H-infinity Optimal Distributed Control in Discrete Time

H-infinity Optimal Distributed Control in Discrete Time H-infinity Optimal Distriuted Control in Discrete Time Lidström, Carolina; Pates, Richard; Rantzer, Anders Pulished in: 2017 IEEE 56th Conference on Decision and Control, CDC 2017 DOI: 10.1109/CDC.2017.8264176

More information

An Efficient Parallel Algorithm to Solve Block Toeplitz Systems

An Efficient Parallel Algorithm to Solve Block Toeplitz Systems The Journal of Supercomputing, 32, 251 278, 2005 C 2005 Springer Science + Business Media, Inc. Manufactured in The Netherlands. An Efficient Parallel Algorithm to Solve Block Toeplitz Systems P. ALONSO

More information

Impedance Control for a Free-Floating Robot in the Grasping of a Tumbling Target with Parameter Uncertainty

Impedance Control for a Free-Floating Robot in the Grasping of a Tumbling Target with Parameter Uncertainty Impedance Control for a Free-Floating Root in the Grasping of a Tumling Target with arameter Uncertainty Satoko Aiko, Roerto ampariello and Gerd Hirzinger Institute of Rootics and Mechatronics German Aerospace

More information

Parametric optimization of a neutral system with two delays and PD-controller

Parametric optimization of a neutral system with two delays and PD-controller 10.2478/acsc-2013-0008 Archives of Control Sciences Volume 23LIX, 2013 No. 2, pages 131 143 Parametric optimization of a neutral system with two elays an PD-controller JÓZEF DUDA In this paper a parametric

More information

Sliding mode observers for sensorless control of current-fed induction motors

Sliding mode observers for sensorless control of current-fed induction motors 2 American Control Conference on O'Farrell Street, San Francisco, CA, USA une 29 - uly, 2 Sliding mode oservers for sensorless control of current-fed induction motors Daniele Bullo, Antonella Ferrara and

More information

Solving Systems of Linear Equations Symbolically

Solving Systems of Linear Equations Symbolically " Solving Systems of Linear Equations Symolically Every day of the year, thousands of airline flights crisscross the United States to connect large and small cities. Each flight follows a plan filed with

More information

#A50 INTEGERS 14 (2014) ON RATS SEQUENCES IN GENERAL BASES

#A50 INTEGERS 14 (2014) ON RATS SEQUENCES IN GENERAL BASES #A50 INTEGERS 14 (014) ON RATS SEQUENCES IN GENERAL BASES Johann Thiel Dept. of Mathematics, New York City College of Technology, Brooklyn, New York jthiel@citytech.cuny.edu Received: 6/11/13, Revised:

More information

arxiv: v1 [hep-ph] 20 Dec 2012

arxiv: v1 [hep-ph] 20 Dec 2012 Decemer 21, 2012 UMD-PP-012-027 Using Energy Peaks to Count Dark Matter Particles in Decays arxiv:1212.5230v1 [hep-ph] 20 Dec 2012 Kaustuh Agashe a, Roerto Franceschini a, Doojin Kim a, and Kyle Wardlow

More information

Technical Appendix: Imperfect information and the business cycle

Technical Appendix: Imperfect information and the business cycle Technical Appendix: Imperfect information and the usiness cycle Farice Collard Harris Dellas Frank Smets March 29 We would like to thank Marty Eichenaum, Jesper Lindé, Thomas Luik, Frank Schorfheide and

More information

Expansion formula using properties of dot product (analogous to FOIL in algebra): u v 2 u v u v u u 2u v v v u 2 2u v v 2

Expansion formula using properties of dot product (analogous to FOIL in algebra): u v 2 u v u v u u 2u v v v u 2 2u v v 2 Least squares: Mathematical theory Below we provide the "vector space" formulation, and solution, of the least squares prolem. While not strictly necessary until we ring in the machinery of matrix algera,

More information

Chaos and Dynamical Systems

Chaos and Dynamical Systems Chaos and Dynamical Systems y Megan Richards Astract: In this paper, we will discuss the notion of chaos. We will start y introducing certain mathematical concepts needed in the understanding of chaos,

More information

Luis Manuel Santana Gallego 100 Investigation and simulation of the clock skew in modern integrated circuits. Clock Skew Model

Luis Manuel Santana Gallego 100 Investigation and simulation of the clock skew in modern integrated circuits. Clock Skew Model Luis Manuel Santana Gallego 100 Appendix 3 Clock Skew Model Xiaohong Jiang and Susumu Horiguchi [JIA-01] 1. Introduction The evolution of VLSI chips toward larger die sizes and faster clock speeds makes

More information

The Capacity Region of 2-Receiver Multiple-Input Broadcast Packet Erasure Channels with Channel Output Feedback

The Capacity Region of 2-Receiver Multiple-Input Broadcast Packet Erasure Channels with Channel Output Feedback IEEE TRANSACTIONS ON INFORMATION THEORY, ONLINE PREPRINT 2014 1 The Capacity Region of 2-Receiver Multiple-Input Broadcast Packet Erasure Channels with Channel Output Feedack Chih-Chun Wang, Memer, IEEE,

More information

Modelling of Ball and Plate System Based on First Principle Model and Optimal Control

Modelling of Ball and Plate System Based on First Principle Model and Optimal Control 2017 21st International Conference on Process Control (PC) June 6 9, 2017, Štrbské Pleso, Slovakia Modelling of Ball and Plate System Based on First Principle Model and Optimal Control František Dušek,

More information

Stability of the logistic population model with generalized piecewise constant delays

Stability of the logistic population model with generalized piecewise constant delays Aruğaslan and Güzel Advances in Difference Equations (2015) 2015:173 DOI 10.1186/s13662-015-0521-8 R E S E A R C H Open Access Staility of the logistic population model with generalized piecewise constant

More information

ESC794: Special Topics: Model Predictive Control

ESC794: Special Topics: Model Predictive Control ESC794: Special Topics: Model Predictive Control Discrete-Time Systems Hanz Richter, Professor Mechanical Engineering Department Cleveland State University Discrete-Time vs. Sampled-Data Systems A continuous-time

More information

Robot Position from Wheel Odometry

Robot Position from Wheel Odometry Root Position from Wheel Odometry Christopher Marshall 26 Fe 2008 Astract This document develops equations of motion for root position as a function of the distance traveled y each wheel as a function

More information

Analysis of undamped second order systems with dynamic feedback

Analysis of undamped second order systems with dynamic feedback Control and Cybernetics vol. 33 (24) No. 4 Analysis of undamped second order systems with dynamic feedback by Wojciech Mitkowski Chair of Automatics AGH University of Science and Technology Al. Mickiewicza

More information

On the orientation of flat triaxial objects in shear flows.

On the orientation of flat triaxial objects in shear flows. On the orientation of flat triaxial ojects in shear flows. J.R. Angilella Octoer 13, 011 (LAEGO, group Transfer in Porous Media, Nancy) Goal: predict the orientation of nonspherical particles in shear

More information

The variance for partial match retrievals in k-dimensional bucket digital trees

The variance for partial match retrievals in k-dimensional bucket digital trees The variance for partial match retrievals in k-dimensional ucket digital trees Michael FUCHS Department of Applied Mathematics National Chiao Tung University January 12, 21 Astract The variance of partial

More information

THE INFLATION-RESTRICTION SEQUENCE : AN INTRODUCTION TO SPECTRAL SEQUENCES

THE INFLATION-RESTRICTION SEQUENCE : AN INTRODUCTION TO SPECTRAL SEQUENCES THE INFLATION-RESTRICTION SEQUENCE : AN INTRODUCTION TO SPECTRAL SEQUENCES TOM WESTON. Example We egin with aelian groups for every p, q and maps : + (here, as in all of homological algera, all maps are

More information

Demographic noise slows down cycles of dominance in ecological models

Demographic noise slows down cycles of dominance in ecological models J. Math. Biol manuscript No. (will e inserted y the editor) Demographic noise slows down cycles of dominance in ecological models Qian Yang Tim Rogers Jonathan H.P. Dawes Received: date / Accepted: date

More information

Supplement to: Guidelines for constructing a confidence interval for the intra-class correlation coefficient (ICC)

Supplement to: Guidelines for constructing a confidence interval for the intra-class correlation coefficient (ICC) Supplement to: Guidelines for constructing a confidence interval for the intra-class correlation coefficient (ICC) Authors: Alexei C. Ionan, Mei-Yin C. Polley, Lisa M. McShane, Kevin K. Doin Section Page

More information

Exact Free Vibration of Webs Moving Axially at High Speed

Exact Free Vibration of Webs Moving Axially at High Speed Eact Free Viration of Wes Moving Aially at High Speed S. HATAMI *, M. AZHARI, MM. SAADATPOUR, P. MEMARZADEH *Department of Engineering, Yasouj University, Yasouj Department of Civil Engineering, Isfahan

More information

ragsdale (zdr82) HW7 ditmire (58335) 1 The magnetic force is

ragsdale (zdr82) HW7 ditmire (58335) 1 The magnetic force is ragsdale (zdr8) HW7 ditmire (585) This print-out should have 8 questions. Multiple-choice questions ma continue on the net column or page find all choices efore answering. 00 0.0 points A wire carring

More information

3 Forces and pressure Answer all questions and show your working out for maximum credit Time allowed : 30 mins Total points available : 32

3 Forces and pressure Answer all questions and show your working out for maximum credit Time allowed : 30 mins Total points available : 32 1 3 Forces and pressure Answer all questions and show your working out for maximum credit Time allowed : 30 mins Total points availale : 32 Core curriculum 1 A icycle pump has its outlet sealed with a

More information

PHYS 705: Classical Mechanics. Introduction and Derivative of Moment of Inertia Tensor

PHYS 705: Classical Mechanics. Introduction and Derivative of Moment of Inertia Tensor 1 PHYS 705: Classical Mechanics Introduction and Derivative of Moment of Inertia Tensor L and N depends on the Choice of Origin Consider a particle moving in a circle with constant v. If we pick the origin

More information

Module 9: Further Numbers and Equations. Numbers and Indices. The aim of this lesson is to enable you to: work with rational and irrational numbers

Module 9: Further Numbers and Equations. Numbers and Indices. The aim of this lesson is to enable you to: work with rational and irrational numbers Module 9: Further Numers and Equations Lesson Aims The aim of this lesson is to enale you to: wor with rational and irrational numers wor with surds to rationalise the denominator when calculating interest,

More information

Rigid bodies - general theory

Rigid bodies - general theory Rigid bodies - general theory Kinetic Energy: based on FW-26 Consider a system on N particles with all their relative separations fixed: it has 3 translational and 3 rotational degrees of freedom. Motion

More information

Estimating a Finite Population Mean under Random Non-Response in Two Stage Cluster Sampling with Replacement

Estimating a Finite Population Mean under Random Non-Response in Two Stage Cluster Sampling with Replacement Open Journal of Statistics, 07, 7, 834-848 http://www.scirp.org/journal/ojs ISS Online: 6-798 ISS Print: 6-78X Estimating a Finite Population ean under Random on-response in Two Stage Cluster Sampling

More information

RATIONAL EXPECTATIONS AND THE COURNOT-THEOCHARIS PROBLEM

RATIONAL EXPECTATIONS AND THE COURNOT-THEOCHARIS PROBLEM RATIONAL EXPECTATIONS AND THE COURNOT-THEOCHARIS PROBLEM TÖNU PUU Received 18 April 006; Accepted 1 May 006 In dynamic models in economics, often rational expectations are assumed. These are meant to show

More information

Multivariable Control Configurations for Fluid Catalytic Cracking Units

Multivariable Control Configurations for Fluid Catalytic Cracking Units Multivariale Control Configurations for Fluid Catalytic Cracking Units Hector Puela, Jesus Valencia, and Jose Alvarez-Ramirez Programa de Investigacion en Matematicas Aplicadas y Computacion Instituto

More information

A NEW HYBRID TESTING PROCEDURE FOR THE LOW CYCLE FATIGUE BEHAVIOR OF STRUCTURAL ELEMENTS AND CONNECTIONS

A NEW HYBRID TESTING PROCEDURE FOR THE LOW CYCLE FATIGUE BEHAVIOR OF STRUCTURAL ELEMENTS AND CONNECTIONS SDSS Rio 010 STABILITY AND DUCTILITY OF STEEL STRUCTURES E. Batista, P. Vellasco, L. de Lima (Eds.) Rio de Janeiro, Brazil, Septemer 8-10, 010 A NEW HYBRID TESTING PROCEDURE FOR THE LOW CYCLE FATIGUE BEHAVIOR

More information

Minimum Wages, Employment and. Monopsonistic Competition

Minimum Wages, Employment and. Monopsonistic Competition Minimum Wages, Employment and Monopsonistic Competition V. Bhaskar Ted To University of Essex Bureau of Laor Statistics August 2003 Astract We set out a model of monopsonistic competition, where each employer

More information

Experimental testing and modelling of a passive mechanical steering compensator for high-performance motorcycles

Experimental testing and modelling of a passive mechanical steering compensator for high-performance motorcycles Proceedings of the European Control Conference 27 Kos, Greece, July 2-5, 27 WeC12.5 Experimental testing and modelling of a passive mechanical steering compensator for high-performance motorcycles Christakis

More information

XV International PhD Workshop OWD 2013, October Limitations Caused by Sampling and Quantization in Position Control of a Single Axis Robot

XV International PhD Workshop OWD 2013, October Limitations Caused by Sampling and Quantization in Position Control of a Single Axis Robot XV International PhD Workshop OWD 2013, 19 22 Octoer 2013 Liitations Caused y Sapling and Quantization in Position Control of a Single Axis Root Csaa Budai, Budapest University of Technology and Econoics

More information

IX. Mass Wasting Processes

IX. Mass Wasting Processes IX. Mass Wasting Processes 1. Deris Flows Flow types: Deris flow, lahar (volcanic), mud flow (few gravel, no oulders) Flowing mixture of water, clay, silt, sand, gravel, oulder, etc. Flowing is liquefied

More information

Regulating Web Tension in Tape Systems with Time-varying Radii

Regulating Web Tension in Tape Systems with Time-varying Radii Regulating Web Tension in Tape Systems with Time-varying Radii Hua Zhong and Lucy Y. Pao Abstract A tape system is time-varying as tape winds from one reel to the other. The variations in reel radii consist

More information

Characterization of the Burst Aggregation Process in Optical Burst Switching.

Characterization of the Burst Aggregation Process in Optical Burst Switching. See discussions, stats, and author profiles for this pulication at: http://www.researchgate.net/pulication/221198381 Characterization of the Burst Aggregation Process in Optical Burst Switching. CONFERENCE

More information

SU(N) representations

SU(N) representations Appendix C SU(N) representations The group SU(N) has N 2 1 generators t a which form the asis of a Lie algera defined y the commutator relations in (A.2). The group has rank N 1 so there are N 1 Casimir

More information

Final Exam April 30, 2013

Final Exam April 30, 2013 Final Exam Instructions: You have 120 minutes to complete this exam. This is a closed-book, closed-notes exam. You are allowed to use a calculator during the exam. Usage of mobile phones and other electronic

More information

Formulating structural matrices of equations of electric circuits containing dependent sources, with the use of the Maple program

Formulating structural matrices of equations of electric circuits containing dependent sources, with the use of the Maple program 1 st World Conerence on echnology and Engineering Education 2010 WIEE Kraków, Poland, 14-17 Septemer 2010 Formulating structural matrices o equations o electric circuits containing dependent sources, with

More information

Mathematical Modelling And Simulation of Quadrotor

Mathematical Modelling And Simulation of Quadrotor IOSR Journal of Electrical and Electronics Engineering (IOSR-JEEE) e-issn: 78-1676,p-ISSN: 3-3331, Volume 1, Issue 6 Ver. II (Nov. Dec. 17), PP 11-18 www.iosrjournals.org Mathematical Modelling And Simulation

More information

Self-propelled hard disks: implicit alignment and transition to collective motion

Self-propelled hard disks: implicit alignment and transition to collective motion epl draft Self-propelled hard disks: implicit alignment and transition to collective motion UMR Gulliver 783 CNRS, ESPCI ParisTech, PSL Research University, rue Vauquelin, 755 Paris, France arxiv:5.76v

More information

Fatigue Failure Analysis of a Cooling Fan Blade: A Case Study

Fatigue Failure Analysis of a Cooling Fan Blade: A Case Study Fatigue Failure Analysis of a Cooling Fan Blade: A Case Study Triloki Nath Kushwaha * NTPC Limited,Farakka,742236,india Email:-tnkushwaha@ntpc.co.in Astract Cooling tower (CT) fan lade are long in size

More information

PAPER Closed Form Expressions of Balanced Realizations of Second-Order Analog Filters

PAPER Closed Form Expressions of Balanced Realizations of Second-Order Analog Filters 565 PAPER Closed Form Expressions of Balanced Realizations of Second-Order Analog Filters Shunsuke YAMAKI a), Memer, Masahide ABE ), Senior Memer, and Masayuki KAWAMATA c), Fellow SUMMARY This paper derives

More information

Resonance Effects on Lifetime of Low Earth Orbit Satellites

Resonance Effects on Lifetime of Low Earth Orbit Satellites Resonance Effects on Lifetime of Low Earth Orit atellites Alain Lamy, Vincent Morand, Clémence Le Fèvre and Huert Fraysse CNE, 18 Avenue Edouard Belin, 31401 Toulouse Cedex 9, +3356173561, Alain.Lamy@cnes.fr

More information

Supporting Information. Dynamics of the Dissociating Uracil Anion. Following Resonant Electron Attachment

Supporting Information. Dynamics of the Dissociating Uracil Anion. Following Resonant Electron Attachment Supporting Information Dynamics of the Dissociating Uracil Anion Following Resonant Electron Attachment Y. Kawarai,, Th. Weer, Y. Azuma, C. Winstead, V. McKoy, A. Belkacem, and D.S. Slaughter, Department

More information

Dynamics Modeling and Identification of the Amigobot Robot

Dynamics Modeling and Identification of the Amigobot Robot Mechanics and Mechanical Engineering Vol. 14, No. 1 (2010) 65 79 c Technical University of Lodz Dynamics Modeling and Identification of the Amigobot Robot Tomasz Buratowski Department of Robotics and Mechatronics,

More information

arxiv:physics/ v1 [physics.plasm-ph] 19 Oct 2004

arxiv:physics/ v1 [physics.plasm-ph] 19 Oct 2004 Staility of off-axis motion for intense particle eams in periodically focusing channels J.S. Moraes a,, R. Pakter a, and F.B. Rizzato a a Instituto de Física, Universidade Federal do Rio Grande do Sul,

More information

Control Systems Design

Control Systems Design ELEC4410 Control Systems Design Lecture 14: Controllability Julio H. Braslavsky julio@ee.newcastle.edu.au School of Electrical Engineering and Computer Science Lecture 14: Controllability p.1/23 Outline

More information

Lulea University of Technology Department of Computer Science, Electrical and Space Engineering. Master Thesis. by Alexander Lebedev

Lulea University of Technology Department of Computer Science, Electrical and Space Engineering. Master Thesis. by Alexander Lebedev Julius Maximilian University of Würzurg Faculty of Mathematics and Computer Science Aerospace Information Technology Chair of Computer Science VIII Prof. Dr. Sergio Montenegro Lulea University of Technology

More information

Magnetic attitude control for satellites

Magnetic attitude control for satellites Magnetic attitude control for satellites Jan Tommy Gravdahl, Department of Engineering Cyernetics Norwegian University of Science and Technology N-7491 TRONDHEIM, Norway Astract In this paper it is proven

More information

Upper Bounds for Stern s Diatomic Sequence and Related Sequences

Upper Bounds for Stern s Diatomic Sequence and Related Sequences Upper Bounds for Stern s Diatomic Sequence and Related Sequences Colin Defant Department of Mathematics University of Florida, U.S.A. cdefant@ufl.edu Sumitted: Jun 18, 01; Accepted: Oct, 016; Pulished:

More information

Stability Analysis of Delayed 4-Channel Bilateral Teleoperation Systems

Stability Analysis of Delayed 4-Channel Bilateral Teleoperation Systems Staility Analysis of Delayed 4Channel Bilateral Teleoperation Systems Noushin Miandashti Mahdi Tavakoli, IEEE Memer Department of Electrical and Computer Engineering, University of Alerta, Edmonton, AB

More information

Determinants of generalized binary band matrices

Determinants of generalized binary band matrices Determinants of generalized inary and matrices Dmitry Efimov arxiv:17005655v1 [mathra] 18 Fe 017 Department of Mathematics, Komi Science Centre UrD RAS, Syktyvkar, Russia Astract Under inary matrices we

More information

Superluminal Hidden Communication as the Underlying Mechanism for Quantum Correlations: Constraining Models

Superluminal Hidden Communication as the Underlying Mechanism for Quantum Correlations: Constraining Models 38 Brazilian Journal of Physics, vol. 35, no. A, June, 005 Superluminal Hidden Communication as the Underlying Mechanism for Quantum Correlations: Constraining Models Valerio Scarani and Nicolas Gisin

More information

Problem 3 Solution Page 1. 1A. Assuming as outlined in the text that the orbit is circular, and relating the radial acceleration

Problem 3 Solution Page 1. 1A. Assuming as outlined in the text that the orbit is circular, and relating the radial acceleration Prolem 3 Solution Page Solution A. Assug as outlined in the text that the orit is circular, and relating the radial acceleration V GM S to the graitational field (where MS is the solar mass we otain Jupiter's

More information

ON FLATNESS OF NONLINEAR IMPLICIT SYSTEMS

ON FLATNESS OF NONLINEAR IMPLICIT SYSTEMS ON FLATNESS OF NONLINEAR IMPLICIT SYSTEMS Paulo Sergio Pereira da Silva, Simone Batista Escola Politécnica da USP Av. Luciano Gualerto trav. 03, 158 05508-900 Cidade Universitária São Paulo SP BRAZIL Escola

More information

Research Article Relative Status Determination for Spacecraft Relative Motion Based on Dual Quaternion

Research Article Relative Status Determination for Spacecraft Relative Motion Based on Dual Quaternion Mathematical Prolems in Engineering Volume 214, Article ID 62724, 7 pages http://dx.doi.org/1.1155/214/62724 Research Article Relative Status Determination for Spacecraft Relative Motion Based on Dual

More information

Stability Analysis and Stability Chart for Unsaturated Residual Soil Slope

Stability Analysis and Stability Chart for Unsaturated Residual Soil Slope American Journal of Environmental Sciences 2 (4): 154-160, 2006 ISSN 1553-345X 2006 Science Pulications Staility Analysis and Staility Chart for Unsaturated Residual Soil Slope 1 Bujang B.K. Huat, 2 Faisal

More information

A Sufficient Condition for Optimality of Digital versus Analog Relaying in a Sensor Network

A Sufficient Condition for Optimality of Digital versus Analog Relaying in a Sensor Network A Sufficient Condition for Optimality of Digital versus Analog Relaying in a Sensor Network Chandrashekhar Thejaswi PS Douglas Cochran and Junshan Zhang Department of Electrical Engineering Arizona State

More information

DESCRIPTION OF THE PROGRAM

DESCRIPTION OF THE PROGRAM 1 DESCRIPTION OF THE PROGRAM TwoDoFSim_BB VERSION 1. May 213. 2 TABLE OF CONTENTS TABLE OF CONTENTS2 1. INTRODUCTION3 1.1 ABBREVIATIONS:... ERROR! BOOKMARK NOT DEFINED. 1.2 GENERAL INFORMATION ABOUT PROGRAM...

More information

ME 230: Kinematics and Dynamics Spring 2014 Section AD. Final Exam Review: Rigid Body Dynamics Practice Problem

ME 230: Kinematics and Dynamics Spring 2014 Section AD. Final Exam Review: Rigid Body Dynamics Practice Problem ME 230: Kinematics and Dynamics Spring 2014 Section AD Final Exam Review: Rigid Body Dynamics Practice Problem 1. A rigid uniform flat disk of mass m, and radius R is moving in the plane towards a wall

More information

Rotary Inverted Pendulum

Rotary Inverted Pendulum Rotary Inverted Pendulum Eric Liu 1 Aug 2013 1 1 State Space Derivations 1.1 Electromechanical Derivation Consider the given diagram. We note that the voltage across the motor can be described by: e b

More information

SUCCESSIVE POLE SHIFTING USING SAMPLED-DATA LQ REGULATORS. Sigeru Omatu

SUCCESSIVE POLE SHIFTING USING SAMPLED-DATA LQ REGULATORS. Sigeru Omatu SUCCESSIVE POLE SHIFING USING SAMPLED-DAA LQ REGULAORS oru Fujinaka Sigeru Omatu Graduate School of Engineering, Osaka Prefecture University, 1-1 Gakuen-cho, Sakai, 599-8531 Japan Abstract: Design of sampled-data

More information

Torque/Rotational Energy Mock Exam. Instructions: (105 points) Answer the following questions. SHOW ALL OF YOUR WORK.

Torque/Rotational Energy Mock Exam. Instructions: (105 points) Answer the following questions. SHOW ALL OF YOUR WORK. AP Physics C Spring, 2017 Torque/Rotational Energy Mock Exam Name: Answer Key Mr. Leonard Instructions: (105 points) Answer the following questions. SHOW ALL OF YOUR WORK. (22 pts ) 1. Two masses are attached

More information

PADEU. The 1 : 2 resonance in the Sitnikov problem. 1 Introduction. T. Kovács 1

PADEU. The 1 : 2 resonance in the Sitnikov problem. 1 Introduction. T. Kovács 1 PADEU PADEU 7, (6) ISBN 963 463 557, ISSN 38-43 c Pulished y the Astron. Dept. of the Eötvös Univ. The : resonance in the Sitnikov prolem T. Kovács Eötvös University, Department of Astronomy, H-58 Budapest,

More information

Concentration of magnetic transitions in dilute magnetic materials

Concentration of magnetic transitions in dilute magnetic materials Journal of Physics: Conference Series OPEN ACCESS Concentration of magnetic transitions in dilute magnetic materials To cite this article: V I Beloon et al 04 J. Phys.: Conf. Ser. 490 065 Recent citations

More information

Riveted Joints and Linear Buckling in the Steel Load-bearing Structure

Riveted Joints and Linear Buckling in the Steel Load-bearing Structure American Journal of Mechanical Engineering, 017, Vol. 5, No. 6, 39-333 Availale online at http://pus.sciepu.com/ajme/5/6/0 Science and Education Pulishing DOI:10.1691/ajme-5-6-0 Riveted Joints and Linear

More information