1. State-Space Linear Systems 2. Block Diagrams 3. Exercises
|
|
- Tabitha Townsend
- 5 years ago
- Views:
Transcription
1 LECTURE 1 State-Space Linear Sstems This lectre introdces state-space linear sstems, which are the main focs of this book. Contents 1. State-Space Linear Sstems 2. Block Diagrams 3. Exercises 1.1 State-Space Linear Sstems A continos-time state-space linear sstem is defined b the followingtwo eqations: ẋ(t) A(t)x(t) B(t)(t), x R n, R k, (1.1a) (t) C(t)x(t) D(t)(t), R m. (1.1b) Notation. Afnction of time (either continos t [0, ) or discrete t N)is called a signal. Notation 1. We write P to mean that is one of the otpts that corresponds to, the (optional) label P specifies the sstem nder consideration. The signals :[0, ) R k, x :[0, ) R n, :[0, ) R m, are called the inpt, state, and otpt of the sstem. The first-order differential eqation (1.1a) is called the state eqation and (1.1b) is called the otpt eqation. The eqations (1.1) express an inpt-otpt relationship between theinpt signal ( ) and the otpt signal ( ). For a given inpt ( ), we need to solve the state eqation to determine the state x( ) and then replace it in the otpt eqation to obtain the otpt ( ). Attention! Forthesameinpt( ), different choices of the initial condition x(0) on the state eqation will reslt in different state trajectories x( ). Conseqentl, one inpt( ) generall corresponds to several possible otpts ( ).
2 6 LECTURE Terminolog and Notation When the inpt signal takes scalar vales (k 1) the sstem is called single-inpt (SI), otherwise it is called mltiple-inpt (MI). When the otpt signal takes scalar vales (m 1) the sstem is called single-otpt (SO), otherwise it is called mltipleotpt (MO). When there is no state eqation (n 0) and we have simpl (t) D(t)(t), R k, R m, Note. The rationale behind this terminolog is explained in Lectre 3. the sstem is called memorless. When all the matrices A(t), B(t), C(t), D(t) areconstant t 0, the sstem (1.1) is called a Linear Time-Invariant (LTI) sstem. In the general case, (1.1) is called a Linear Time-Varing (LTV) sstem to emphasize that time invariance is not being assmed. For example, Lectre 3 discsses implse responses of LTV sstems and transfer fnctions of LTI sstems. This terminolog indicates that the implse response concept applies to both LTV and LTI sstems, bt the transfer fnction concept is meaningfl onl for LTI sstems. To keep formlas short, in the following we abbreviate (1.1) to ẋ A(t)x B(t), C(t)x D(t), x R n, R k, R m (CLTV) MATLAB R Hint 1. ss(a,b,c,d) creates the continos-time LTI state-space sstem (CLTI). p. 7 and in the time-invariant case, we frther shorten this to ẋ Ax B, Cx D, x R n, R k, R m. (CLTI) Since these eqations appear in the text nmeros times, we se the special tags (CLTV) and (CLTI) to identif them Discrete-Time Case A discrete-time state-space linear sstem isdefined bthe followingtwo eqations: x(t 1) A(t)x(t) B(t)(t), x R n, R k, (1.2a) (t) C(t)x(t) D(t)(t), R m. (1.2b) Attention. One inpt generall corresponds to several otpts, becase one ma consider several initial conditions for the state eqation. All the terminolog introdced for continos-time sstems also applies to discrete time, except that now the domain of the signals is N : {0, 1, 2,...}, instead of the interval [0, ). In discrete-time sstems the state eqation is a difference eqation, instead of a first-order differential eqation. However, the relationship between inpt and otpt is analogos. For a given inpt ( ), we need to solve the state (difference)
3 STATE-SPACE LINEAR SYSTEMS 7 Note. Since this eqation appears in the text nmeros times, we se the special tag (DLTI) to identif it. The tag (DLTV) is sed to identif the time-varing case in (1.2). eqation to determine the state x( ) and then replace it in the otpt eqation to obtain the otpt ( ). To keep formlas short to, in the seqel we abbreviate the time-invariant case of (1.2) x Ax B, Cx D, x R n, R k, R m. (DLTI) State-Space Sstems in MATLAB R MATLAB R has several commands to create and maniplate LTI sstems. The following basic command is sed to create an LTI sstem. Note. Initial conditions to LTI state-space MATLAB R sstems are specified at simlation time. MATLAB R Hint 1 (ss). The command ss_ssss(a,b,c,d) assigns to ss_ss a continos-time LTI state-space MATLAB R sstem of the form ẋ Ax B, Cx D. Optionall, one can specif the names of the inpts, otpts, and state to be sed in sbseqent plots as follows: ss_ssss(a,b,c,d,... InptName, { inpt1, inpt2,...},... OtptName,{ otpt1, otpt2,...},... StateName, { state1, state2,...}); The nmber of elements in the bracketed lists mst match the nmber of inpts, otpts, and state variables. For discrete-time sstems, one shold instead se the command ss_ssss(a,b,c,d,ts), where Ts is the sampling time, or -1 if one does not want to specif it. Note. It is common practice to denote the inpt and otpt signals of a sstem b and, respectivel. However, when dealing with interconnections, one mst se different smbols for each signal, so this convention is abandoned. 1.2 Block Diagrams It is convenient to represent sstems b block diagrams as in Figre 1.1. These diagrams generall serve as compact representations for complex eqations. The two-port block in Figre 1.1(a) represents a sstem with inpt ( )andotpt ( ), where the directions of the arrows specif which is which. Althogh not explicitl represented in the diagram, one mst keep in mind the existence of the state, which affects the otpt throgh the initial condition Interconnections Interconnections of block diagrams are especiall sefl to highlight special strctres in state-space eqations. To nderstand what is meant b this, assme that the
4 8 LECTURE 1 P 1 1 P P 2 2 (a) Single block (b) Parallel z z P 1 P 2 P 1 (c) Cascade (d) Negative feedback Figre 1.1. Block diagrams. blocks P 1 and P 2 that appear in Figre 1.1 are the two LTI sstems P 1 : ẋ 1 A 1 x 1 B 1 1, 1 C 1 x 1 D 1 1, x R n 1, R k 1, 1 R m 1, P 2 : ẋ 2 A 2 B 2 2, 2 C 2 D 2 2, x R n 2, R k 2, 2 R m 2. The general procedre to obtain the state-space for an interconnection consists of stacking the states of the individal sbsstems in a tall vector x and compting ẋ sing the state and otpt eqations of the individal blocks. The otpt eqation is also obtained from the otpt eqations of the sbsstems. In Figre 1.1(b) we have 1 2 and 1 2, which corresponds to a parallel interconnection. This figre represents the LTI sstem [ [ [ [ẋ1 A1 0 x1 B1, [ [ x C ẋ 2 0 A 2 B 1 C 1 2 (D 2 x 1 D 2 ), 2 Notation. Given a vector (or matrix) x,we denote its transpose b x. with state x : [x 1 x 2 R n 1n 2. The parallel interconnection is responsible for the block-diagonal strctre in the matrix [ A A 2. A block-diagonal strctre in this matrix indicates that the state-space sstem can be decomposed as the parallel of two state-space sstems with smaller states. In Figre 1.1(c) we have 1, 2,andz 1 2, which corresponds to a cascade interconnection. This figre represents the LTI sstem [ [ [ [ẋ1 A1 0 x1 B1, [ [ x D ẋ 2 B 2 C 1 A 2 B 2 D 2 C 1 C 1 2 D 1 D 1, 2 with state x : [x 1 x 2 R n 1n 2. The cascade interconnection is responsible for the block-trianglar strctre in the matrix [ A 1 0 B 2 C 1 A 2 and, in fact, a block-trianglar strctre in this matrix indicates that the state-space sstem can be decomposed as a cascade of two state-space sstems with smaller states.
5 STATE-SPACE LINEAR SYSTEMS 9 z z P 3 P 4 (a) ẋ x, x (b) LTI sstem in (1.4) Figre 1.2. Block diagram representation sstems. Note. Howtoarriveat eqation (1.3)? Hint: Start with the otpt eqation, note that C 1 x 1 D 1 ( ), and solve for. MATLAB R Hint 2. To avoid ill-posed feedback interconnections, MATLAB R warns abot algebraic loops when one attempts to close feedback loops arond sstems like P 1 with nonzero D 1 matrices (even when I D 1 is invertible). In Figre 1.1(d) we have 1 1 and 1, which corresponds to a negativefeedback interconnection. This figre represents the following LTI sstem ẋ 1 (A 1 B 1 (I D 1 ) 1 C 1 )x 1 B 1 (I (I D 1 ) 1 D 1 ), (I D 1 ) 1 C 1 x 1 (I D 1 ) 1 D 1, (1.3a) (1.3b) with state x 1 R n 1. Sometimes feedback interconnections are ill-posed. In this example, this wold happen if the matrix I D 1 were singlar. The basic interconnections in Figre 1.1 can be combined to form arbitraril complex diagrams. The general procedre to obtain the final state-space sstem remains the same: Stack the states of all sbsstems in a tall vector x and compte ẋ sing the state and otpt eqations of the individal blocks Sstem Decomposition MATLAB R Hint 3. This tpe of decomposition is especiall sefl to bild sstems in Simlink R. Note. The pper trianglar form in (1.4) gives awa that this cold be decomposable as a cascade. Note. In general, this tpe of decomposition is not niqe, since there ma be man was to represent a sstem as the interconnection of simpler sstems. Block diagrams are also sefl to represent complex sstems as the interconnection of simple blocks. This can be seen throgh the following two examples: 1. The LTI sstem ẋ x, x can be viewed as a feedback connection in Figre 1.2(a), where the integrator sstem maps each inpt z to the soltions of 2. Consider the LTI sstem [ẋ1 ẋ 2 [ Writing these eqations as [ x1 ẏ z. [ 1, 5 [ 1 0 [ x 1. (1.4) ẋ 2 3 5, 2 (1.5)
6 10 LECTURE 1 and ẋ 1 x 1 z, x 1, (1.6) where z :, weconcldethat(1.4)canbeviewedastheblockdiagram in Figre 1.2(b), where P 3 corresponds to the LTI sstem (1.5) with inpt and otpt 2 and P 4 corresponds to the LTI sstems (1.6) with inpt z and otpt Sstem Interconnections with MATLAB R Attention! Note the different order in which ss1 and ss2 appear in the two forms of this command. MATLAB R Hint 4 (series) The command ssseries(ss1,ss2) or, alternativel, ssss2*ss1 creates a sstem ss from the cascade connection of the sstem ss1 whose otpt is connected to the inpt of ss2. For MIMO sstems, one can se ssseries(ss1,ss2,otpts1, inpts2), whereotpts1 and inpts2 are vectors that specif the otpts of ss1 andinptsofss2, respectivel, that shold be connected. These two vectors shold have the same size and contain integer indexes starting at 1. MATLAB R Hint 5 (parallel) The command ssparallel(ss1,ss2) or, alternativel, ssss1ss2 creates a sstem ss from the parallel connection of the sstems ss1 and ss2. For MIMO sstems, one can se ssparallel(ss1,ss2,inpts1, inpts2,otpts1,otpts2),whereinpts1 and inpts2 specif which inpts shold be connected and otpts1 and otpts2 specif which otpts shold be added. All for vectors shold contain integer indexes starting at 1. MATLAB R Hint 6 (append) The command ssappend(ss1,ss2,...,ssn) creates a sstem ss whose inpts are the nion of the inpts of all the sstems ss1, ss2,...,ssn and whose otpts are the nion of the otpts of all the same sstems. The dnamics are maintained decopled. MATLAB R Hint 7 (feedback) The command ssfeedback(ss1,ss2) creates a sstem ss from the negative feedback interconnection of the sstem ss1 in the forward loop, with the sstem ss2 in the backward loop. A positive feedback interconnection can be obtained sing ssfeedback(ss1,ss2,1). For MIMO sstems, one can se ssfeedback(ss1,ss2,feedinpts, feedotpts,sign), where feedinpts specif which inpts of the forwardloop sstem ss1 receive feedback from ss2, feedotpts specif which otpts of the forward-loop sstem ss1 are feedback to ss2, and sign { 1, 1} specifies whether a negative or positive feedback configration shold be sed. More details can be obtained b sing help feedback.
7 1.3 Exercises Copright, Princeton Universit Press. No part of this book ma be STATE-SPACE LINEAR SYSTEMS (Block diagram decomposition). Consider a sstem P 1 that maps each inpt to the soltions of [ẋ1 ẋ 2 [ [ x1 [ 4, [ 1 3 [ x 1. 1 Represent this sstem in terms of a block diagram consisting onl of integrator sstems, represented b the smbol,thatmaptheirinpt( ) R to the soltion ( ) R of ẏ ; smmation blocks, represented b the smbol, that map their inpt vector ( ) R k to the scalar otpt (t) k i1 i(t), t 0; and gain memorless sstems, represented b the smbol g, thatmaptheirinpt ( ) R to the otpt (t) g(t) R, t 0 for some g R.
Linear System Theory (Fall 2011): Homework 1. Solutions
Linear System Theory (Fall 20): Homework Soltions De Sep. 29, 20 Exercise (C.T. Chen: Ex.3-8). Consider a linear system with inpt and otpt y. Three experiments are performed on this system sing the inpts
More informationControl Systems
6.5 Control Systems Last Time: Introdction Motivation Corse Overview Project Math. Descriptions of Systems ~ Review Classification of Systems Linear Systems LTI Systems The notion of state and state variables
More informationINPUT-OUTPUT APPROACH NUMERICAL EXAMPLES
INPUT-OUTPUT APPROACH NUMERICAL EXAMPLES EXERCISE s consider the linear dnamical sstem of order 2 with transfer fnction with Determine the gain 2 (H) of the inpt-otpt operator H associated with this sstem.
More informationChapter 3 MATHEMATICAL MODELING OF DYNAMIC SYSTEMS
Chapter 3 MATHEMATICAL MODELING OF DYNAMIC SYSTEMS 3. System Modeling Mathematical Modeling In designing control systems we mst be able to model engineered system dynamics. The model of a dynamic system
More informationState Space Models Basic Concepts
Chapter 2 State Space Models Basic Concepts Related reading in Bay: Chapter Section Sbsection 1 (Models of Linear Systems) 1.1 1.1.1 1.1.2 1.1.3 1.1.5 1.2 1.2.1 1.2.2 1.3 In this Chapter we provide some
More informationSolving a System of Equations
Solving a System of Eqations Objectives Understand how to solve a system of eqations with: - Gass Elimination Method - LU Decomposition Method - Gass-Seidel Method - Jacobi Method A system of linear algebraic
More informationChapter 2 Difficulties associated with corners
Chapter Difficlties associated with corners This chapter is aimed at resolving the problems revealed in Chapter, which are cased b corners and/or discontinos bondar conditions. The first section introdces
More informationLecture 6 : Linear Fractional Transformations (LFTs) Dr.-Ing. Sudchai Boonto
Lectre 6 : (LFTs) Dr-Ing Sdchai Boonto Department of Control System and Instrmentation Engineering King Mongkts Unniversity of Technology Thonbri Thailand Feedback Strctre d i d r e y z K G g n The standard
More informationThe Linear Quadratic Regulator
10 The Linear Qadratic Reglator 10.1 Problem formlation This chapter concerns optimal control of dynamical systems. Most of this development concerns linear models with a particlarly simple notion of optimality.
More information10.4 Solving Equations in Quadratic Form, Equations Reducible to Quadratics
. Solving Eqations in Qadratic Form, Eqations Redcible to Qadratics Now that we can solve all qadratic eqations we want to solve eqations that are not eactl qadratic bt can either be made to look qadratic
More informationGeometric Image Manipulation. Lecture #4 Wednesday, January 24, 2018
Geometric Image Maniplation Lectre 4 Wednesda, Janar 4, 08 Programming Assignment Image Maniplation: Contet To start with the obvios, an image is a D arra of piels Piel locations represent points on the
More informationControl Using Logic & Switching: Part III Supervisory Control
Control Using Logic & Switching: Part III Spervisor Control Ttorial for the 40th CDC João P. Hespanha Universit of Sothern California Universit of California at Santa Barbara Otline Spervisor control overview
More informationNonlinear predictive control of dynamic systems represented by Wiener Hammerstein models
Nonlinear Dn (26) 86:93 24 DOI.7/s7-6-2957- ORIGINAL PAPER Nonlinear predictive control of dnamic sstems represented b Wiener Hammerstein models Maciej Ławrńcz Received: 7 December 25 / Accepted: 2 Jl
More informationSimplified Identification Scheme for Structures on a Flexible Base
Simplified Identification Scheme for Strctres on a Flexible Base L.M. Star California State University, Long Beach G. Mylonais University of Patras, Greece J.P. Stewart University of California, Los Angeles
More informationFuzzy Control of a Nonlinear Deterministic System for Different Operating Points
International Jornal of Electrical & Compter Sciences IJECS-IJE Vol: No: 9 Fzz Control of a Nonlinear Deterministic Sstem for Different Operating Points Gonca Ozmen Koca, Cafer Bal, Firat Universit, Technical
More informationChapter 1: Differential Form of Basic Equations
MEG 74 Energ and Variational Methods in Mechanics I Brendan J. O Toole, Ph.D. Associate Professor of Mechanical Engineering Howard R. Hghes College of Engineering Universit of Nevada Las Vegas TBE B- (7)
More informationFEA Solution Procedure
EA Soltion Procedre (demonstrated with a -D bar element problem) EA Procedre for Static Analysis. Prepare the E model a. discretize (mesh) the strctre b. prescribe loads c. prescribe spports. Perform calclations
More informationLecture 17 Errors in Matlab s Turbulence PSD and Shaping Filter Expressions
Lectre 7 Errors in Matlab s Trblence PSD and Shaping Filter Expressions b Peter J Sherman /7/7 [prepared for AERE 355 class] In this brief note we will show that the trblence power spectral densities (psds)
More informationClassify by number of ports and examine the possible structures that result. Using only one-port elements, no more than two elements can be assembled.
Jnction elements in network models. Classify by nmber of ports and examine the possible strctres that reslt. Using only one-port elements, no more than two elements can be assembled. Combining two two-ports
More informationAssignment Fall 2014
Assignment 5.086 Fall 04 De: Wednesday, 0 December at 5 PM. Upload yor soltion to corse website as a zip file YOURNAME_ASSIGNMENT_5 which incldes the script for each qestion as well as all Matlab fnctions
More information1 The space of linear transformations from R n to R m :
Math 540 Spring 20 Notes #4 Higher deriaties, Taylor s theorem The space of linear transformations from R n to R m We hae discssed linear transformations mapping R n to R m We can add sch linear transformations
More informationFRTN10 Exercise 12. Synthesis by Convex Optimization
FRTN Exercise 2. 2. We want to design a controller C for the stable SISO process P as shown in Figre 2. sing the Yola parametrization and convex optimization. To do this, the control loop mst first be
More informationControl Systems Design
ELEC4410 Control Systems Design Lectre 16: Controllability and Observability Canonical Decompositions Jlio H. Braslavsky jlio@ee.newcastle.ed.a School of Electrical Engineering and Compter Science Lectre
More informationPartial Differential Equations with Applications
Universit of Leeds MATH 33 Partial Differential Eqations with Applications Eamples to spplement Chapter on First Order PDEs Eample (Simple linear eqation, k + = 0, (, 0) = ϕ(), k a constant.) The characteristic
More informationGradient Projection Anti-windup Scheme on Constrained Planar LTI Systems. Justin Teo and Jonathan P. How
1 Gradient Projection Anti-windp Scheme on Constrained Planar LTI Systems Jstin Teo and Jonathan P. How Technical Report ACL1 1 Aerospace Controls Laboratory Department of Aeronatics and Astronatics Massachsetts
More informationLINEAR COMBINATIONS AND SUBSPACES
CS131 Part II, Linear Algebra and Matrices CS131 Mathematics for Compter Scientists II Note 5 LINEAR COMBINATIONS AND SUBSPACES Linear combinations. In R 2 the vector (5, 3) can be written in the form
More informationElements of Coordinate System Transformations
B Elements of Coordinate System Transformations Coordinate system transformation is a powerfl tool for solving many geometrical and kinematic problems that pertain to the design of gear ctting tools and
More informationOn the circuit complexity of the standard and the Karatsuba methods of multiplying integers
On the circit complexity of the standard and the Karatsba methods of mltiplying integers arxiv:1602.02362v1 [cs.ds] 7 Feb 2016 Igor S. Sergeev The goal of the present paper is to obtain accrate estimates
More informationMath 263 Assignment #3 Solutions. 1. A function z = f(x, y) is called harmonic if it satisfies Laplace s equation:
Math 263 Assignment #3 Soltions 1. A fnction z f(x, ) is called harmonic if it satisfies Laplace s eqation: 2 + 2 z 2 0 Determine whether or not the following are harmonic. (a) z x 2 + 2. We se the one-variable
More informationModel Predictive Control Lecture VIa: Impulse Response Models
Moel Preictive Control Lectre VIa: Implse Response Moels Niet S. Kaisare Department of Chemical Engineering Inian Institte of Technolog Maras Ingreients of Moel Preictive Control Dnamic Moel Ftre preictions
More informationComplex Variables. For ECON 397 Macroeconometrics Steve Cunningham
Comple Variables For ECON 397 Macroeconometrics Steve Cnningham Open Disks or Neighborhoods Deinition. The set o all points which satis the ineqalit
More informationSareban: Evaluation of Three Common Algorithms for Structure Active Control
Engineering, Technology & Applied Science Research Vol. 7, No. 3, 2017, 1638-1646 1638 Evalation of Three Common Algorithms for Strctre Active Control Mohammad Sareban Department of Civil Engineering Shahrood
More informationImage and Multidimensional Signal Processing
Image and Mltidimensional Signal Processing Professor William Hoff Dept of Electrical Engineering &Compter Science http://inside.mines.ed/~whoff/ Forier Transform Part : D discrete transforms 2 Overview
More informationSystem identification of buildings equipped with closed-loop control devices
System identification of bildings eqipped with closed-loop control devices Akira Mita a, Masako Kamibayashi b a Keio University, 3-14-1 Hiyoshi, Kohok-k, Yokohama 223-8522, Japan b East Japan Railway Company
More informationMEG 741 Energy and Variational Methods in Mechanics I
MEG 74 Energ and Variational Methods in Mechanics I Brendan J. O Toole, Ph.D. Associate Professor of Mechanical Engineering Howard R. Hghes College of Engineering Universit of Nevada Las Vegas TBE B- (7)
More informationA Single Species in One Spatial Dimension
Lectre 6 A Single Species in One Spatial Dimension Reading: Material similar to that in this section of the corse appears in Sections 1. and 13.5 of James D. Mrray (), Mathematical Biology I: An introction,
More informationBLOOM S TAXONOMY. Following Bloom s Taxonomy to Assess Students
BLOOM S TAXONOMY Topic Following Bloom s Taonomy to Assess Stdents Smmary A handot for stdents to eplain Bloom s taonomy that is sed for item writing and test constrction to test stdents to see if they
More informationIntrodction Finite elds play an increasingly important role in modern digital commnication systems. Typical areas of applications are cryptographic sc
A New Architectre for a Parallel Finite Field Mltiplier with Low Complexity Based on Composite Fields Christof Paar y IEEE Transactions on Compters, Jly 996, vol 45, no 7, pp 856-86 Abstract In this paper
More informationSTEP Support Programme. STEP III Hyperbolic Functions: Solutions
STEP Spport Programme STEP III Hyperbolic Fnctions: Soltions Start by sing the sbstittion t cosh x. This gives: sinh x cosh a cosh x cosh a sinh x t sinh x dt t dt t + ln t ln t + ln cosh a ln ln cosh
More information1 Differential Equations for Solid Mechanics
1 Differential Eqations for Solid Mechanics Simple problems involving homogeneos stress states have been considered so far, wherein the stress is the same throghot the component nder std. An eception to
More informationMultivariable Ripple-Free Deadbeat Control
Scholarly Jornal of Mathematics and Compter Science Vol. (), pp. 9-9, October Available online at http:// www.scholarly-jornals.com/sjmcs ISS 76-8947 Scholarly-Jornals Fll Length Research aper Mltivariable
More informationNonlinear parametric optimization using cylindrical algebraic decomposition
Proceedings of the 44th IEEE Conference on Decision and Control, and the Eropean Control Conference 2005 Seville, Spain, December 12-15, 2005 TC08.5 Nonlinear parametric optimization sing cylindrical algebraic
More informationLinear and Nonlinear Model Predictive Control of Quadruple Tank Process
Linear and Nonlinear Model Predictive Control of Qadrple Tank Process P.Srinivasarao Research scholar Dr.M.G.R.University Chennai, India P.Sbbaiah, PhD. Prof of Dhanalaxmi college of Engineering Thambaram
More informationAMS 212B Perturbation Methods Lecture 05 Copyright by Hongyun Wang, UCSC
AMS B Pertrbation Methods Lectre 5 Copright b Hongn Wang, UCSC Recap: we discssed bondar laer of ODE Oter epansion Inner epansion Matching: ) Prandtl s matching ) Matching b an intermediate variable (Skip
More informationLecture Notes On THEORY OF COMPUTATION MODULE - 2 UNIT - 2
BIJU PATNAIK UNIVERSITY OF TECHNOLOGY, ODISHA Lectre Notes On THEORY OF COMPUTATION MODULE - 2 UNIT - 2 Prepared by, Dr. Sbhend Kmar Rath, BPUT, Odisha. Tring Machine- Miscellany UNIT 2 TURING MACHINE
More informationFormal Methods for Deriving Element Equations
Formal Methods for Deriving Element Eqations And the importance of Shape Fnctions Formal Methods In previos lectres we obtained a bar element s stiffness eqations sing the Direct Method to obtain eact
More informationIII. Demonstration of a seismometer response with amplitude and phase responses at:
GG5330, Spring semester 006 Assignment #1, Seismometry and Grond Motions De 30 Janary 006. 1. Calibration Of A Seismometer Using Java: A really nifty se of Java is now available for demonstrating the seismic
More informationReduction of over-determined systems of differential equations
Redction of oer-determined systems of differential eqations Maim Zaytse 1) 1, ) and Vyachesla Akkerman 1) Nclear Safety Institte, Rssian Academy of Sciences, Moscow, 115191 Rssia ) Department of Mechanical
More informationNonparametric Identification and Robust H Controller Synthesis for a Rotational/Translational Actuator
Proceedings of the 6 IEEE International Conference on Control Applications Mnich, Germany, October 4-6, 6 WeB16 Nonparametric Identification and Robst H Controller Synthesis for a Rotational/Translational
More informationDISPLACEMENT ANALYSIS OF SUBMARINE SLOPES USING ENHANCED NEWMARK METHOD
DISPLACEMENT ANALYSIS OF SUBMARINE SLOPES USING ENHANCED NEWMARK METHOD N. ZANGENEH and R. POPESCU Faclt of Engineering & Applied Science, Memorial Universit, St. John s, Newfondland, Canada A1B 3X5 Abstract
More informationNEURAL CONTROLLERS FOR NONLINEAR SYSTEMS IN MATLAB
NEURAL CONTROLLERS FOR NONLINEAR SYSTEMS IN MATLAB S.Kajan Institte of Control and Indstrial Informatics, Faclt of Electrical Engineering and Information Technolog, Slovak Universit of Technolog in Bratislava,
More informationThe Dual of the Maximum Likelihood Method
Department of Agricltral and Resorce Economics University of California, Davis The Dal of the Maximm Likelihood Method by Qirino Paris Working Paper No. 12-002 2012 Copyright @ 2012 by Qirino Paris All
More informationModelling, Simulation and Control of Quadruple Tank Process
Modelling, Simlation and Control of Qadrple Tan Process Seran Özan, Tolgay Kara and Mehmet rıcı,, Electrical and electronics Engineering Department, Gaziantep Uniersity, Gaziantep, Trey bstract Simple
More informationBayes and Naïve Bayes Classifiers CS434
Bayes and Naïve Bayes Classifiers CS434 In this lectre 1. Review some basic probability concepts 2. Introdce a sefl probabilistic rle - Bayes rle 3. Introdce the learning algorithm based on Bayes rle (ths
More informationDepartment of Industrial Engineering Statistical Quality Control presented by Dr. Eng. Abed Schokry
Department of Indstrial Engineering Statistical Qality Control presented by Dr. Eng. Abed Schokry Department of Indstrial Engineering Statistical Qality Control C and U Chart presented by Dr. Eng. Abed
More informationPrimary dependent variable is fluid velocity vector V = V ( r ); where r is the position vector
Chapter 4: Flids Kinematics 4. Velocit and Description Methods Primar dependent ariable is flid elocit ector V V ( r ); where r is the position ector If V is known then pressre and forces can be determined
More informationThe Oscillatory Stable Regime of Nonlinear Systems, with two time constants
6th WSES International Conference on CIRCUITS SYSTEMS ELECTRONICSCONTROL & SIGNL PROCESSING Cairo Egpt Dec 9-3 7 5 The Oscillator Stable Regime of Nonlinear Sstems with two time constants NUŢU VSILE *
More informationAdvanced topics in Finite Element Method 3D truss structures. Jerzy Podgórski
Advanced topics in Finite Element Method 3D trss strctres Jerzy Podgórski Introdction Althogh 3D trss strctres have been arond for a long time, they have been sed very rarely ntil now. They are difficlt
More informationEstimating models of inverse systems
Estimating models of inverse systems Ylva Jng and Martin Enqvist Linköping University Post Print N.B.: When citing this work, cite the original article. Original Pblication: Ylva Jng and Martin Enqvist,
More informationDiscontinuous Fluctuation Distribution for Time-Dependent Problems
Discontinos Flctation Distribtion for Time-Dependent Problems Matthew Hbbard School of Compting, University of Leeds, Leeds, LS2 9JT, UK meh@comp.leeds.ac.k Introdction For some years now, the flctation
More informationSafe Manual Control of the Furuta Pendulum
Safe Manal Control of the Frta Pendlm Johan Åkesson, Karl Johan Åström Department of Atomatic Control, Lnd Institte of Technology (LTH) Box 8, Lnd, Sweden PSfrag {jakesson,kja}@control.lth.se replacements
More informationMean Value Formulae for Laplace and Heat Equation
Mean Vale Formlae for Laplace and Heat Eqation Abhinav Parihar December 7, 03 Abstract Here I discss a method to constrct the mean vale theorem for the heat eqation. To constrct sch a formla ab initio,
More informationFOUNTAIN codes [3], [4] provide an efficient solution
Inactivation Decoding of LT and Raptor Codes: Analysis and Code Design Francisco Lázaro, Stdent Member, IEEE, Gianligi Liva, Senior Member, IEEE, Gerhard Bach, Fellow, IEEE arxiv:176.5814v1 [cs.it 19 Jn
More informationOptimal Control of a Heterogeneous Two Server System with Consideration for Power and Performance
Optimal Control of a Heterogeneos Two Server System with Consideration for Power and Performance by Jiazheng Li A thesis presented to the University of Waterloo in flfilment of the thesis reqirement for
More informationBOND-GRAPH BASED CONTROLLER DESIGN OF A TWO-INPUT TWO-OUTPUT FOUR-TANK SYSTEM
BOND-GAPH BASED CONTOLLE DESIGN OF A TWO-INPUT TWO-OUTPUT FOU-TANK SYSTEM Nacsse, Matías A. (a) and Jnco, Sergio J. (b) LAC, Laboratorio de Atomatización y Control, Departamento de Control, Facltad de
More informationModelling by Differential Equations from Properties of Phenomenon to its Investigation
Modelling by Differential Eqations from Properties of Phenomenon to its Investigation V. Kleiza and O. Prvinis Kanas University of Technology, Lithania Abstract The Panevezys camps of Kanas University
More informationMaterial. Lecture 8 Backlash and Quantization. Linear and Angular Backlash. Example: Parallel Kinematic Robot. Backlash.
Lectre 8 Backlash and Qantization Material Toda s Goal: To know models and compensation methods for backlash Lectre slides Be able to analze the effect of qantization errors Note: We are sing analsis methods
More informationWe automate the bivariate change-of-variables technique for bivariate continuous random variables with
INFORMS Jornal on Compting Vol. 4, No., Winter 0, pp. 9 ISSN 09-9856 (print) ISSN 56-558 (online) http://dx.doi.org/0.87/ijoc.046 0 INFORMS Atomating Biariate Transformations Jeff X. Yang, John H. Drew,
More informationCS 450: COMPUTER GRAPHICS VECTORS SPRING 2016 DR. MICHAEL J. REALE
CS 45: COMPUTER GRPHICS VECTORS SPRING 216 DR. MICHEL J. RELE INTRODUCTION In graphics, we are going to represent objects and shapes in some form or other. First, thogh, we need to figre ot how to represent
More informationReflections on a mismatched transmission line Reflections.doc (4/1/00) Introduction The transmission line equations are given by
Reflections on a mismatched transmission line Reflections.doc (4/1/00) Introdction The transmission line eqations are given by, I z, t V z t l z t I z, t V z, t c z t (1) (2) Where, c is the per-nit-length
More informationPrototype Angle Domain Repetitive Control - Affine Parameterization Approach
Prototpe Angle Domain Repetitive Control - Affine Parameterization Approach Perr Y. Li Professor Department of Mechanical Engineering Universit of Minnesota Minneapolis, Minnesota 55455 U.S.A. Email: lixxx99@mn.ed
More informationIncompressible Viscoelastic Flow of a Generalised Oldroyed-B Fluid through Porous Medium between Two Infinite Parallel Plates in a Rotating System
International Jornal of Compter Applications (97 8887) Volme 79 No., October Incompressible Viscoelastic Flow of a Generalised Oldroed-B Flid throgh Poros Medim between Two Infinite Parallel Plates in
More informationAlternative single-step type genomic prediction equations
63rd Annal Meeting of the EAAP Bratislava, Slovakia, Agst 7-3, Alternative single-step tpe genomic prediction eqations N. engler,. Niewhof,3, K. Konstantinov,3, M. oddard 3,4 ULg - emblox Agro-Bio ech,
More informationSetting The K Value And Polarization Mode Of The Delta Undulator
LCLS-TN-4- Setting The Vale And Polarization Mode Of The Delta Undlator Zachary Wolf, Heinz-Dieter Nhn SLAC September 4, 04 Abstract This note provides the details for setting the longitdinal positions
More informationConcept of Stress at a Point
Washkeic College of Engineering Section : STRONG FORMULATION Concept of Stress at a Point Consider a point ithin an arbitraril loaded deformable bod Define Normal Stress Shear Stress lim A Fn A lim A FS
More informationA Survey of the Implementation of Numerical Schemes for Linear Advection Equation
Advances in Pre Mathematics, 4, 4, 467-479 Pblished Online Agst 4 in SciRes. http://www.scirp.org/jornal/apm http://dx.doi.org/.436/apm.4.485 A Srvey of the Implementation of Nmerical Schemes for Linear
More informationStability analysis of two predator-one stage-structured prey model incorporating a prey refuge
IOSR Jornal of Mathematics (IOSR-JM) e-issn: 78-578 p-issn: 39-765X. Volme Isse 3 Ver. II (Ma - Jn. 5) PP -5 www.iosrjornals.org Stabilit analsis of two predator-one stage-strctred pre model incorporating
More informationLecture Notes: Finite Element Analysis, J.E. Akin, Rice University
9. TRUSS ANALYSIS... 1 9.1 PLANAR TRUSS... 1 9. SPACE TRUSS... 11 9.3 SUMMARY... 1 9.4 EXERCISES... 15 9. Trss analysis 9.1 Planar trss: The differential eqation for the eqilibrim of an elastic bar (above)
More informationThe Real Stabilizability Radius of the Multi-Link Inverted Pendulum
Proceedings of the 26 American Control Conference Minneapolis, Minnesota, USA, Jne 14-16, 26 WeC123 The Real Stabilizability Radis of the Mlti-Link Inerted Pendlm Simon Lam and Edward J Daison Abstract
More informationA Radial Basis Function Method for Solving PDE Constrained Optimization Problems
Report no. /6 A Radial Basis Fnction Method for Solving PDE Constrained Optimization Problems John W. Pearson In this article, we appl the theor of meshfree methods to the problem of PDE constrained optimization.
More informationEssentials of optimal control theory in ECON 4140
Essentials of optimal control theory in ECON 4140 Things yo need to know (and a detail yo need not care abot). A few words abot dynamic optimization in general. Dynamic optimization can be thoght of as
More informationDecentralized Control with Moving-Horizon Linear Switched Systems: Synthesis and Testbed Implementation
17 American Control Conference Sheraton Seattle Hotel May 4 6, 17, Seattle, USA Decentralized Control with Moving-Horizon Linear Switched Systems: Synthesis and Testbed Implementation Joao P Jansch-Porto
More informationGen Hebb Learn PPaplinski Generalized Hebbian Learning and its pplication in Dimensionality Redction Illstrative Example ndrew P Paplinski Department
Faclty of Compting and Information Technology Department of Digital Systems Technical Report 9-2 Generalized Hebbian Learning and its pplication in Dimensionality Redction Illstrative Example ndrew P Paplinski
More informationChap 4. State-Space Solutions and
Chap 4. State-Space Solutions and Realizations Outlines 1. Introduction 2. Solution of LTI State Equation 3. Equivalent State Equations 4. Realizations 5. Solution of Linear Time-Varying (LTV) Equations
More information1 Undiscounted Problem (Deterministic)
Lectre 9: Linear Qadratic Control Problems 1 Undisconted Problem (Deterministic) Choose ( t ) 0 to Minimize (x trx t + tq t ) t=0 sbject to x t+1 = Ax t + B t, x 0 given. x t is an n-vector state, t a
More informationMove Blocking Strategies in Receding Horizon Control
Move Blocking Strategies in Receding Horizon Control Raphael Cagienard, Pascal Grieder, Eric C. Kerrigan and Manfred Morari Abstract In order to deal with the comptational brden of optimal control, it
More informationPulses on a Struck String
8.03 at ESG Spplemental Notes Plses on a Strck String These notes investigate specific eamples of transverse motion on a stretched string in cases where the string is at some time ndisplaced, bt with a
More informationOutline. Model Predictive Control Short Course Introduction. The model predictive control framework. The power of abstraction
Model Predictive Control Short Corse Introdction James B. Rawlings Michael J. Risbeck Nishith R. Patel Department of Chemical and Biological Engineering Copright c 7 b James B. Rawlings Milwakee, WI Agst
More information1. LQR formulation 2. Selection of weighting matrices 3. Matlab implementation. Regulator Problem mm3,4. u=-kx
MM8.. LQR Reglator 1. LQR formlation 2. Selection of weighting matrices 3. Matlab implementation Reading Material: DC: p.364-382, 400-403, Matlab fnctions: lqr, lqry, dlqr, lqrd, care, dare 3/26/2008 Introdction
More informationSecond-Order Wave Equation
Second-Order Wave Eqation A. Salih Department of Aerospace Engineering Indian Institte of Space Science and Technology, Thirvananthapram 3 December 016 1 Introdction The classical wave eqation is a second-order
More informationNonlocal Symmetries and Interaction Solutions for Potential Kadomtsev Petviashvili Equation
Commn. Theor. Phs. 65 (16) 31 36 Vol. 65, No. 3, March 1, 16 Nonlocal Smmetries and Interaction Soltions for Potential Kadomtsev Petviashvili Eqation Bo Ren ( ), Jn Y ( ), and Xi-Zhong Li ( ) Institte
More informationMAT389 Fall 2016, Problem Set 6
MAT389 Fall 016, Problem Set 6 Trigonometric and hperbolic fnctions 6.1 Show that e iz = cos z + i sin z for eer comple nmber z. Hint: start from the right-hand side and work or wa towards the left-hand
More informationACTUATION AND SIMULATION OF A MINISYSTEM WITH FLEXURE HINGES
The 4th International Conference Comptational Mechanics and Virtal Engineering COMEC 2011 20-22 OCTOBER 2011, Brasov, Romania ACTUATION AND SIMULATION OF A MINISYSTEM WITH FLEXURE HINGES D. NOVEANU 1,
More informationChange of Variables. (f T) JT. f = U
Change of Variables 4-5-8 The change of ariables formla for mltiple integrals is like -sbstittion for single-ariable integrals. I ll gie the general change of ariables formla first, and consider specific
More informationNonsingular Formation Control of Cooperative Mobile Robots via Feedback Linearization
Nonsinglar Formation Control of Cooperative Mobile Robots via Feedback Linearization Erf Yang, Dongbing G, and Hosheng H Department of Compter Science University of Essex Wivenhoe Park, Colchester CO4
More informationStudy on the impulsive pressure of tank oscillating by force towards multiple degrees of freedom
EPJ Web of Conferences 80, 0034 (08) EFM 07 Stdy on the implsive pressre of tank oscillating by force towards mltiple degrees of freedom Shigeyki Hibi,* The ational Defense Academy, Department of Mechanical
More informationDIGITAL LINEAR QUADRATIC SMITH PREDICTOR
DIGITAL LINEAR QUADRATIC SMITH PREDICTOR Vladimír Bobál,, Marek Kbalčík, Petr Dostál, and Stanislav Talaš Tomas Bata Universit in Zlín Centre of Polmer Sstems, Universit Institte Department of Process
More informationUNCERTAINTY FOCUSED STRENGTH ANALYSIS MODEL
8th International DAAAM Baltic Conference "INDUSTRIAL ENGINEERING - 19-1 April 01, Tallinn, Estonia UNCERTAINTY FOCUSED STRENGTH ANALYSIS MODEL Põdra, P. & Laaneots, R. Abstract: Strength analysis is a
More informationM 21 M 22 1 S. . x. x u B D A C
Robstness Assessment of Flight Controllers for a Civil Aircraft sing,analysis. G.H.N. Looye ;2, S. Bennani 2, A. Varga, D. Moormann, G. Grbel Detsches Zentrm fr Lft- nd Ramfahrt (DLR) Institt fr Robotik
More informationRESGen: Renewable Energy Scenario Generation Platform
1 RESGen: Renewable Energy Scenario Generation Platform Emil B. Iversen, Pierre Pinson, Senior Member, IEEE, and Igor Ardin Abstract Space-time scenarios of renewable power generation are increasingly
More information