How to Obtain Desirable Transfer Functions in MIMO Systems Under Internal Stability Using Open and Closed Loop Control
|
|
- Oliver French
- 5 years ago
- Views:
Transcription
1 How to Obtain Desiable ansfe Functions in MIMO Sstems Unde Intenal Stabilit Using Open and losed Loop ontol echnical Repot of the ISIS Goup at the Univesit of Note Dame ISIS June, 03 Panos J. Antsaklis and Elo Gacia Depatment of Electical Engineeing Univesit of Note Dame Note Dame, IN Intedisciplina Studies in Intelligent Sstems-echnical Repot
2 How to Obtain Desiable ansfe Functions in MIMO Sstems Unde Intenal Stabilit Using Open and losed Loop ontol Panos J. Antsaklis and Elo Gacia Abstact his pape summaizes impotant esults useful fo contolle design of multi-input multi-output sstems. he main goal is to chaacteize the stabilizing contolles that povide a desied esponse. I. INRODUION he aim of this bief pape is to use esults fom [] to show how in Multi-Input Multi-Output (MIMO) sstems, using -degees of feedom compensation and existing techniques, the attainable esponse unde intenal stabilit can be completel chaacteized. hese include the model matching poblem, the invese poblem, the diagonal and block diagonal decoupling poblems, and the static decoupling poblem among othes. he equiement fo stabilit esticts the design when the given sstem is non-minimum phase. Specificall, the compensated sstem tansfe function matix must have among its zeos all the unstable zeos of the given plant, togethe with thei associated diections. In addition, the equiement fo causalit does not allow the compensated sstem tansfe function to have elative degee lowe than the given plant s. his pape also shows constuctivel how to design feedback and feed-fowad -degees of feedom contolles that attain the desiable esponses unde intenal stabilit. In fact all such contolles will be paameticall chaacteized. It is then up to the designe to decide how much of the needed contol should be implemented via feedback compensation and how much via feedfowad compensation. his decision depends on the specifications on feedback popeties such as sensitivit to plant paamete vaiations, distubance eduction, noise attenuation etc. In man cases, the contol achitectue ma not be a full -degees of feedom achitectue but ma be esticted. Fo example it could be the ve common in pactice state feedback achitectue, state feedback with obseve, unit output feedback achitectue etc. he eect of such estictions on the attainable esponses is examined and it is shown in each case how to deive the appopiate contolles.
3 Special attention is being paid to the special case of the tansfe function of the plant P(s) being squae and non-singula and it is shown how expessions ae simplified; note that this case includes the SISO case. Examples ae used thoughout. In the following section, Section II, two basic esults ae fist pesented. he fist chaacteizes all esponses attainable using a -degees of feedom contolle unde intenal stabilit. he second esult paameticall chaacteizes all stabilizing -degees of feedom contolles, which attain the desied esponse, showing explicitl the intepla of feedfowad and feedback contol actions. Achitectues that ealize and implement the contol policies ae also shown. In Section III seveal design poblems ae discussed including the decoupling and invese poblems. he eect of seveal moe esticted common contol achitectues on the sstem esponse is discussed in Section IV. In Section V we stud the special case of the plant tansfe function matix being squae and nonsingula which includes the SISO case and deive esults fo the case when the denominato of the compensated tansfe function is given. II. DESIGN OF ONROL SYSEMS FOR DESIRED RESPONSE onside the MIMO plant with p x m tansfe function matix P = ND ( = Pu), whee N, D ae ight copime polnomial matices. (he esults in this pape ae based on [], pp ). Suppose we want to contol P so that: = u M whee, M ae pope and stable desied tansfe function matices and is an extenal input. Basic Result I. It has been shown in [] (h. 4.3 p. 67; also h. 4.4 fo pope stable factoizations) that the above and M can be ealized via a geneal -degees of feedom contolle with intenal stabilit if onl if thee exist stable ational matix X so that: N = X. M D In [], Fig. 7. p. 67, shows a wa to ealize such and M. See Fig. below whee is an feedback stabilizing contolle fo P.
4 Fig.. Fig.. Basic Result II. he geneal -degee of feedom configuation is shown in Fig., whee u = =, (see [] p. 63 Fig. 7.0 and h. 4.), with an feedback stabilizing contolle ( u = intenall stabilizes = Pu) and such that X = D ( I P) stable o = ( I P) DX = ( I PM ). Hee = = NX and u = M = DX. Feedback ontolle. all stabilizing contolles ([] h. 4. p. 64): can be an stabilizing contolle. o see the flexibilit we chaacteize [ ] [ ] =, = ( I + QP) Q, M = ( I + LN) D L, X whee Q = DL, M = DX ae pope with L, X, exists and is pope). D ( I + QP) = ( I + LN) D stable (also ( I + QP) = X, KN ( X + KD), X whee K, X stable; K is the Youla paamete. Othe expessions ma be found in [] h. 4. p.64. 3
5 III. RESPONSE. In ou case X is given (o pat of X is specified). Note that, M cannot be chosen independentl fo a solution to () to exist, but the must be in the ange of N D, o equivalentl, ank N D M = ank N = m D, full column ank. he also must be stable, which is to be expected. So, the onl significant estictions imposed (othe than popeness) ae due to the unstable zeos of P, (in N), if an. Since = NX and, X stable, must contain all unstable zeos of the plant P. ( s )( s+ ) he example 4. in [], on p. 68 whee P = ( s ) illustates all these points. It is also shown in the next section what additional estictions ae imposed if instead of a geneal - degees of feedom configuation the moe esticted unit feedback is used. ( s )( s+ ) Example. We conside P = ( s ) and wish to chaacteize all pope and stable tansfe functions (s) that can be ealized b means of some contol configuation with intenal stabilit. Let ( s) ( s ) P = = N' D' ( s+ ) ( s+ ) all such must satisf be an c MFD in RH. hen in view of [], heoem 4.4 on p. 67, ( s + ) N' = = X ' RH ( s ) heefoe, an pope with a zeo at + can be ealized via a -degees of feedom feedback contolle with intenal stabilit. Diagonal Decoupling. Hee the desied tansfe function (s) is not completel specified but is equied to be diagonal, pope and stable. hat is N ' X ' = diag( n / d ) i i whee N', X ' ae pope and stable. If P exists (see also the last section of this pape) then X N diag n d ' = ' ( i / i). If P(s) has onl stable zeos then no additional estictions ae imposed on (s). When diagonal decoupling is accomplished using moe esticted contol configuations (e.g. unit feedback) additional estictions ae imposed on X ' due to the contol achitectue (see next section). 4
6 When linea state feedback u = Fx+ G is used fo diagonal decoupling = N D G M = D D G and ' ' f, ' ' f, X ' = D G. ' f So, when P exists X D G N diag n d ' ' = f = ' ( i / i) fo a solution to exist (see Execise 4.7, 4.0, hapte 4 of []). Invese poblem. In this case (s)=i and so = I = N' X ' which gives the conditions on the stable and pope paamete hapte 4 of []). X '(see also Execise 4.7, 4.8 in Static decoupling. Hee (s) is squae, pope and stable and (s)=λ, a eal nonsingula diagonal matix, so that a step change in the fist input will onl aect the fist output at stead state. Fom = N' X ' in view of (s)=λ, a necessa and suicient condition is that P(s) does not have a zeo at the oigin (so det N '(0) 0). hen '( ) X s must satisf X '( s) ( N' ( s) ) = Λ. his is also suicient and static decoupling in this case can be achieved with just pe-compensation b a eal gain matix his can be seen fom the expession in Section II fo fom which = P () s Λ. = ( I P) D' X ' = D' X ' ( = 0) s = D s X s = P s Λ () '() '() (). IV. RESRIED ONROLLER ONFIGURAION. If the configuation in Fig. 3 ([], Fig. 7.3 p. 69) is chosen, then ' ' u =, =, R = D ' c N, N a lc factoization is RH (pope and stable). 5
7 Fig. 3 Fig. 4 hen, if =, is given one could choose ' R = N, =, ' D c ' N. = Note that R, ae stable; exists and it is stable. In tems of the pope and stable paametes X ', K ' the can be elated as R = X ', X K N = ( ', ' '), = ( X ' + K' N '). If the configuation in Fig. 4 (unit feedback) is chosen, ([], Fig. 7.5 p. 63), then i.e. = and in view of (4.58) (o 4.6) Hee (fom 4.58) u =, =, L = X ( L' = X ') o ( Q = M). 6
8 = ( I + MP) M = M( I + PM) M I I XN D X = ( + ) = ( + ) whee D ( I + MP) = ( I + XN) D stable which imposes a estiction on the allowed X (o X ). onside again the example above, if a single degee of feedom contolle must be used, the class of ealizable (s) unde intenal stabilit is esticted. In paticula, if the unit feedback configuation { I;, } again given b I in Fig. 4 is used, then all pope and stable that ae ealizable unde intenal stabilit ae whee X ' = L' RH and in addition ( s ) = N' X ' = X ' ( s + ) I + X N D = + X ( s ) ( s+ ) RH ( ' ') ' ' ( ) ( ) s+ s i.e., X ' = n / d is pope and stable and should also satisf x x s+ d + s n = s p s ( ) x ( ) x ( ) ( ) fo some polnomial p(s). his illustates the estictions imposed b the unit feedback contolle, as opposed to a -degees of feedom contolle. Notice that these additional estictions ae imposed because the given plant has unstable poles. he unit feedback case is studied in [] Poblem 7.3 p V. P EXISS. Example. Next it is shown how the expessions ae simplified when Poblem 7.3 pat (c) p In the unit feedback configuation when onl if: is stable and if is chosen so that P P exists. his is fom [] exists the closed loop sstem is intenall stable if and N ( I ) P, N 7
9 = NX, X stable, then this is the same as ( I ) + XN D stable (in Fig. 7.9 the sign is dieent). In the Single-Input Single-Output (SISO) case, fom (d) p. 643 when P and ae scala, the conditions become ( ) d = Sd and n stable. he contolle Applications of esults. is still given b the fomula ( ). = I + XN D X Suppose then that the desied stable tansfe function matix needs to have onl some desied denominato. In = ND, completel, like in decoupling, ae biefl discussed). Fom = NX, X stable implies that we can select exist whee fo example X D is given (note that in [] p. 633, poblems whee is not specified N = NN. = ND x and X X N = D, assuming that Fom the pevious discussion, fo stabilit (in unit feedback) we need = N ; othe options X, D, ( I ) + XN D stable, o D ( D + N) D stable and since D is assumed stable, the onl condition is ( D ) + N D stable and the contolle is given b onside now Fig. 4 and veif esponse = ( + ) I D N D D = ( D ( D + N) D ) D = DD ( + N) DD = DD + ( N). = P + = I P P ( ) ( ). Hee P= ND, = D( D + N) 8
10 Fig. 5. = P ( I P ) = ND D( D + N) I N D = N ( D + N) ( D + N) = ND [ ] D( D + N) D + N N as expected. Note that hee + P = D N + DN = ( D + D) N = + = ( D D) D DN P. If the configuation in Fig. 5 is chosen (see also [], Fig. 7.8 p. 63), then u =, =, I and then (4.58) p.64 whee L is esticted to satisf = ( I + LN) D L X = I + LN D XD= I + LN ( ) ( ). In the special case when P exists ( exists) X ( XD I) N X L = =. So the stabilit condition is just X must be stable. Hee, 9
11 = ( I P ) P = P( I P) ND I I LN D LND = ( ) [( + ) ] = ( ND ) (( I + LN) D ) [( I + LN ) LN = ( ND ) D ( ) I + LN D = NX X ] D as desied. Assuming P and exist, when X = stable fom pevious page, fo intenal stabilit D = ( D ) D D I N = D D [ D D ] N ( ). = D D N leal, the closed loop tansfe function with as above as expected. = P( I P) = ( ND ) I ( D D ) N N D = ( ND ) D D D = ND + D So given NX ND = = stable ( D desied) select = ( D D ) N and onl wo about popeness. Note that hee P = D N DN = ( D D) N =. VI. ONLUDING REMARKS Seveal esults fom [] on -degee of feedom contolles wee used to solve a set of poblems whee the denominato of the desied tansfe function is given. he contol design poblems whee o pats of it ae specified can be addessed in simila wa. Dieent contol configuations can also be studied; fo example, in the linea stable feedback M = DD and X = D. 0
12 REFERENES [] P. J. Antsaklis and A. N. Michel, Linea Sstems, Spinge/ Bikhause, 006.
A NEW VARIABLE STIFFNESS SPRING USING A PRESTRESSED MECHANISM
Poceedings of the ASME 2010 Intenational Design Engineeing Technical Confeences & Computes and Infomation in Engineeing Confeence IDETC/CIE 2010 August 15-18, 2010, Monteal, Quebec, Canada DETC2010-28496
More informationMultiple Experts with Binary Features
Multiple Expets with Binay Featues Ye Jin & Lingen Zhang Decembe 9, 2010 1 Intoduction Ou intuition fo the poect comes fom the pape Supevised Leaning fom Multiple Expets: Whom to tust when eveyone lies
More informationME 3600 Control Systems Frequency Domain Analysis
ME 3600 Contol Systems Fequency Domain Analysis The fequency esponse of a system is defined as the steady-state esponse of the system to a sinusoidal (hamonic) input. Fo linea systems, the esulting steady-state
More informationChapter 5 Linear Equations: Basic Theory and Practice
Chapte 5 inea Equations: Basic Theoy and actice In this chapte and the next, we ae inteested in the linea algebaic equation AX = b, (5-1) whee A is an m n matix, X is an n 1 vecto to be solved fo, and
More informationGeometry of the homogeneous and isotropic spaces
Geomety of the homogeneous and isotopic spaces H. Sonoda Septembe 2000; last evised Octobe 2009 Abstact We summaize the aspects of the geomety of the homogeneous and isotopic spaces which ae most elevant
More informationWeighted least-squares estimators of parametric functions of the regression coefficients under a general linear model
Ann Inst Stat Math (2010) 62:929 941 DOI 10.1007/s10463-008-0199-8 Weighted least-squaes estimatos of paametic functions of the egession coefficients unde a geneal linea model Yongge Tian Received: 9 Januay
More informationHua Xu 3 and Hiroaki Mukaidani 33. The University of Tsukuba, Otsuka. Hiroshima City University, 3-4-1, Ozuka-Higashi
he inea Quadatic Dynamic Game fo Discete-ime Descipto Systems Hua Xu 3 and Hioai Muaidani 33 3 Gaduate School of Systems Management he Univesity of suuba, 3-9- Otsua Bunyo-u, oyo -0, Japan xuhua@gssm.otsua.tsuuba.ac.jp
More informationAbsolute Specifications: A typical absolute specification of a lowpass filter is shown in figure 1 where:
FIR FILTER DESIGN The design of an digital filte is caied out in thee steps: ) Specification: Befoe we can design a filte we must have some specifications. These ae detemined by the application. ) Appoximations
More informationAnalytical Solutions for Confined Aquifers with non constant Pumping using Computer Algebra
Poceedings of the 006 IASME/SEAS Int. Conf. on ate Resouces, Hydaulics & Hydology, Chalkida, Geece, May -3, 006 (pp7-) Analytical Solutions fo Confined Aquifes with non constant Pumping using Compute Algeba
More informationPhysics 2B Chapter 22 Notes - Magnetic Field Spring 2018
Physics B Chapte Notes - Magnetic Field Sping 018 Magnetic Field fom a Long Staight Cuent-Caying Wie In Chapte 11 we looked at Isaac Newton s Law of Gavitation, which established that a gavitational field
More informationF-IF Logistic Growth Model, Abstract Version
F-IF Logistic Gowth Model, Abstact Vesion Alignments to Content Standads: F-IFB4 Task An impotant example of a model often used in biology o ecology to model population gowth is called the logistic gowth
More informationChapter 9 Dynamic stability analysis III Lateral motion (Lectures 33 and 34)
Pof. E.G. Tulapukaa Stability and contol Chapte 9 Dynamic stability analysis Lateal motion (Lectues 33 and 34) Keywods : Lateal dynamic stability - state vaiable fom of equations, chaacteistic equation
More informationResearch Article On Alzer and Qiu s Conjecture for Complete Elliptic Integral and Inverse Hyperbolic Tangent Function
Abstact and Applied Analysis Volume 011, Aticle ID 697547, 7 pages doi:10.1155/011/697547 Reseach Aticle On Alze and Qiu s Conjectue fo Complete Elliptic Integal and Invese Hypebolic Tangent Function Yu-Ming
More informationAuchmuty High School Mathematics Department Advanced Higher Notes Teacher Version
The Binomial Theoem Factoials Auchmuty High School Mathematics Depatment The calculations,, 6 etc. often appea in mathematics. They ae called factoials and have been given the notation n!. e.g. 6! 6!!!!!
More informationSolution to HW 3, Ma 1a Fall 2016
Solution to HW 3, Ma a Fall 206 Section 2. Execise 2: Let C be a subset of the eal numbes consisting of those eal numbes x having the popety that evey digit in the decimal expansion of x is, 3, 5, o 7.
More informationFUNDAMENTAL PROPERTIES OF LINEAR SHIP STEERING DYNAMIC MODELS
Jounal of Maine Science and Technology, Vol. 7, No. 2, pp. 79-88 (1999) 79 FUNDAMENTAL PROPERTIES OF LINEAR SHIP STEERING DYNAMIC MODELS Ching-Yaw Tzeng* and Ju-Fen Chen** Keywods: Nomoto model, Contollability
More informationLocalization of Eigenvalues in Small Specified Regions of Complex Plane by State Feedback Matrix
Jounal of Sciences, Islamic Republic of Ian (): - () Univesity of Tehan, ISSN - http://sciencesutaci Localization of Eigenvalues in Small Specified Regions of Complex Plane by State Feedback Matix H Ahsani
More informationPerturbation to Symmetries and Adiabatic Invariants of Nonholonomic Dynamical System of Relative Motion
Commun. Theo. Phys. Beijing, China) 43 25) pp. 577 581 c Intenational Academic Publishes Vol. 43, No. 4, Apil 15, 25 Petubation to Symmeties and Adiabatic Invaiants of Nonholonomic Dynamical System of
More informationCALCULUS II Vectors. Paul Dawkins
CALCULUS II Vectos Paul Dawkins Table of Contents Peface... ii Vectos... 3 Intoduction... 3 Vectos The Basics... 4 Vecto Aithmetic... 8 Dot Poduct... 13 Coss Poduct... 21 2007 Paul Dawkins i http://tutoial.math.lama.edu/tems.aspx
More informationNonlinear dynamic inversion
Nonlinea dynamic invesion Aicat don t always behave like linea systems. In some light egimes, o in some (ailue) scenaios, they behave in a nonlinea way. To contol them, you theeoe also need a nonlinea
More informationThe Substring Search Problem
The Substing Seach Poblem One algoithm which is used in a vaiety of applications is the family of substing seach algoithms. These algoithms allow a use to detemine if, given two chaacte stings, one is
More informationAPPLICATION OF MAC IN THE FREQUENCY DOMAIN
PPLICION OF MC IN HE FREQUENCY DOMIN D. Fotsch and D. J. Ewins Dynamics Section, Mechanical Engineeing Depatment Impeial College of Science, echnology and Medicine London SW7 2B, United Kingdom BSRC he
More informationCHAPTER 25 ELECTRIC POTENTIAL
CHPTE 5 ELECTIC POTENTIL Potential Diffeence and Electic Potential Conside a chaged paticle of chage in a egion of an electic field E. This filed exets an electic foce on the paticle given by F=E. When
More informationA Crash Course in (2 2) Matrices
A Cash Couse in ( ) Matices Seveal weeks woth of matix algeba in an hou (Relax, we will only stuy the simplest case, that of matices) Review topics: What is a matix (pl matices)? A matix is a ectangula
More informationFunctions Defined on Fuzzy Real Numbers According to Zadeh s Extension
Intenational Mathematical Foum, 3, 2008, no. 16, 763-776 Functions Defined on Fuzzy Real Numbes Accoding to Zadeh s Extension Oma A. AbuAaqob, Nabil T. Shawagfeh and Oma A. AbuGhneim 1 Mathematics Depatment,
More informationOLYMON. Produced by the Canadian Mathematical Society and the Department of Mathematics of the University of Toronto. Issue 9:2.
OLYMON Poduced by the Canadian Mathematical Society and the Depatment of Mathematics of the Univesity of Toonto Please send you solution to Pofesso EJ Babeau Depatment of Mathematics Univesity of Toonto
More information( ) [ ] [ ] [ ] δf φ = F φ+δφ F. xdx.
9. LAGRANGIAN OF THE ELECTROMAGNETIC FIELD In the pevious section the Lagangian and Hamiltonian of an ensemble of point paticles was developed. This appoach is based on a qt. This discete fomulation can
More informationIn many engineering and other applications, the. variable) will often depend on several other quantities (independent variables).
II PARTIAL DIFFERENTIATION FUNCTIONS OF SEVERAL VARIABLES In man engineeing and othe applications, the behaviou o a cetain quantit dependent vaiable will oten depend on seveal othe quantities independent
More informationEM Boundary Value Problems
EM Bounday Value Poblems 10/ 9 11/ By Ilekta chistidi & Lee, Seung-Hyun A. Geneal Desciption : Maxwell Equations & Loentz Foce We want to find the equations of motion of chaged paticles. The way to do
More informationA Power Method for Computing Square Roots of Complex Matrices
JOURNAL OF MATHEMATICAL ANALYSIS AND APPLICATIONS 13, 39345 1997 ARTICLE NO. AY975517 A Powe Method fo Computing Squae Roots of Complex Matices Mohammed A. Hasan Depatment of Electical Engineeing, Coloado
More informationHammerstein Model Identification Based On Instrumental Variable and Least Square Methods
Intenational Jounal of Emeging Tends & Technology in Compute Science (IJETTCS) Volume 2, Issue, Januay Febuay 23 ISSN 2278-6856 Hammestein Model Identification Based On Instumental Vaiable and Least Squae
More informationPulse Neutron Neutron (PNN) tool logging for porosity Some theoretical aspects
Pulse Neuton Neuton (PNN) tool logging fo poosity Some theoetical aspects Intoduction Pehaps the most citicism of Pulse Neuton Neuon (PNN) logging methods has been chage that PNN is to sensitive to the
More informationMODULE 5a and 5b (Stewart, Sections 12.2, 12.3) INTRO: In MATH 1114 vectors were written either as rows (a1, a2,..., an) or as columns a 1 a. ...
MODULE 5a and 5b (Stewat, Sections 2.2, 2.3) INTRO: In MATH 4 vectos wee witten eithe as ows (a, a2,..., an) o as columns a a 2... a n and the set of all such vectos of fixed length n was called the vecto
More informationworking pages for Paul Richards class notes; do not copy or circulate without permission from PGR 2004/11/3 10:50
woking pages fo Paul Richads class notes; do not copy o ciculate without pemission fom PGR 2004/11/3 10:50 CHAPTER7 Solid angle, 3D integals, Gauss s Theoem, and a Delta Function We define the solid angle,
More informationSchool of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007
School of Electical and Compute Engineeing, Conell Univesity ECE 303: Electomagnetic Fields and Waves Fall 007 Homewok 8 Due on Oct. 19, 007 by 5:00 PM Reading Assignments: i) Review the lectue notes.
More informationMechatronic system design
Mechatonic system design Mechatonic system design wb2414 2013/2014 Couse pat 5 Motion contol Pof.i. R.H.Munnig Schmidt Mechatonic System Design 1 Lectue outline: What did you lean about PID motion contol
More informationof the contestants play as Falco, and 1 6
JHMT 05 Algeba Test Solutions 4 Febuay 05. In a Supe Smash Bothes tounament, of the contestants play as Fox, 3 of the contestants play as Falco, and 6 of the contestants play as Peach. Given that thee
More informationLET a random variable x follows the two - parameter
INTERNATIONAL JOURNAL OF MATHEMATICS AND SCIENTIFIC COMPUTING ISSN: 2231-5330, VOL. 5, NO. 1, 2015 19 Shinkage Bayesian Appoach in Item - Failue Gamma Data In Pesence of Pio Point Guess Value Gyan Pakash
More information4/18/2005. Statistical Learning Theory
Statistical Leaning Theoy Statistical Leaning Theoy A model of supevised leaning consists of: a Envionment - Supplying a vecto x with a fixed but unknown pdf F x (x b Teache. It povides a desied esponse
More informationPHYS 110B - HW #7 Spring 2004, Solutions by David Pace Any referenced equations are from Griffiths Problem statements are paraphrased
PHYS 0B - HW #7 Sping 2004, Solutions by David Pace Any efeenced euations ae fom Giffiths Poblem statements ae paaphased. Poblem 0.3 fom Giffiths A point chage,, moves in a loop of adius a. At time t 0
More informationTemporal-Difference Learning
.997 Decision-Making in Lage-Scale Systems Mach 17 MIT, Sping 004 Handout #17 Lectue Note 13 1 Tempoal-Diffeence Leaning We now conside the poblem of computing an appopiate paamete, so that, given an appoximation
More informationA Relativistic Electron in a Coulomb Potential
A Relativistic Electon in a Coulomb Potential Alfed Whitehead Physics 518, Fall 009 The Poblem Solve the Diac Equation fo an electon in a Coulomb potential. Identify the conseved quantum numbes. Specify
More informationRigid Body Dynamics 2. CSE169: Computer Animation Instructor: Steve Rotenberg UCSD, Winter 2018
Rigid Body Dynamics 2 CSE169: Compute Animation nstucto: Steve Rotenbeg UCSD, Winte 2018 Coss Poduct & Hat Opeato Deivative of a Rotating Vecto Let s say that vecto is otating aound the oigin, maintaining
More informationNumerical Integration
MCEN 473/573 Chapte 0 Numeical Integation Fall, 2006 Textbook, 0.4 and 0.5 Isopaametic Fomula Numeical Integation [] e [ ] T k = h B [ D][ B] e B Jdsdt In pactice, the element stiffness is calculated numeically.
More informationradians). Figure 2.1 Figure 2.2 (a) quadrant I angle (b) quadrant II angle is in standard position Terminal side Terminal side Terminal side
. TRIGONOMETRIC FUNCTIONS OF GENERAL ANGLES In ode to etend the definitions of the si tigonometic functions to geneal angles, we shall make use of the following ideas: In a Catesian coodinate sstem, an
More informationCentral Coverage Bayes Prediction Intervals for the Generalized Pareto Distribution
Statistics Reseach Lettes Vol. Iss., Novembe Cental Coveage Bayes Pediction Intevals fo the Genealized Paeto Distibution Gyan Pakash Depatment of Community Medicine S. N. Medical College, Aga, U. P., India
More informationA scaling-up methodology for co-rotating twin-screw extruders
A scaling-up methodology fo co-otating twin-scew extudes A. Gaspa-Cunha, J. A. Covas Institute fo Polymes and Composites/I3N, Univesity of Minho, Guimaães 4800-058, Potugal Abstact. Scaling-up of co-otating
More informationChem 453/544 Fall /08/03. Exam #1 Solutions
Chem 453/544 Fall 3 /8/3 Exam # Solutions. ( points) Use the genealized compessibility diagam povided on the last page to estimate ove what ange of pessues A at oom tempeatue confoms to the ideal gas law
More information22.615, MHD Theory of Fusion Systems Prof. Freidberg Lecture 4: Toroidal Equilibrium and Radial Pressure Balance
.615, MHD Theoy of Fusion Systems Pof. Feidbeg Lectue 4: Tooidal Equilibium and Radial Pessue Balance Basic Poblem of Tooidal Equilibium 1. Radial pessue balance. Tooidal foce balance Radial Pessue Balance
More informationMATH 220: SECOND ORDER CONSTANT COEFFICIENT PDE. We consider second order constant coefficient scalar linear PDEs on R n. These have the form
MATH 220: SECOND ORDER CONSTANT COEFFICIENT PDE ANDRAS VASY We conside second ode constant coefficient scala linea PDEs on R n. These have the fom Lu = f L = a ij xi xj + b i xi + c i whee a ij b i and
More information7.2.1 Basic relations for Torsion of Circular Members
Section 7. 7. osion In this section, the geomety to be consideed is that of a long slende cicula ba and the load is one which twists the ba. Such poblems ae impotant in the analysis of twisting components,
More informationRelated Rates - the Basics
Related Rates - the Basics In this section we exploe the way we can use deivatives to find the velocity at which things ae changing ove time. Up to now we have been finding the deivative to compae the
More informationMath 451: Euclidean and Non-Euclidean Geometry MWF 3pm, Gasson 204 Homework 9 Solutions
Math 451: Euclidean and Non-Euclidean Geomety MWF 3pm, Gasson 04 Homewok 9 Solutions Execises fom Chapte 3: 3.3, 3.8, 3.15, 3.19, 3.0, 5.11, 5.1, 5.13 Execise 3.3. Suppose that C and C ae two cicles with
More informationOn the Quasi-inverse of a Non-square Matrix: An Infinite Solution
Applied Mathematical Sciences, Vol 11, 2017, no 27, 1337-1351 HIKARI Ltd, wwwm-hikaicom https://doiog/1012988/ams20177273 On the Quasi-invese of a Non-squae Matix: An Infinite Solution Ruben D Codeo J
More informationChapter Introduction to Finite Element Methods
Chapte 1.4 Intoduction to Finite Element Methods Afte eading this chapte, you should e ale to: 1. Undestand the asics of finite element methods using a one-dimensional polem. In the last fifty yeas, the
More informationChapter 3: Theory of Modular Arithmetic 38
Chapte 3: Theoy of Modula Aithmetic 38 Section D Chinese Remainde Theoem By the end of this section you will be able to pove the Chinese Remainde Theoem apply this theoem to solve simultaneous linea conguences
More informationConservative Averaging Method and its Application for One Heat Conduction Problem
Poceedings of the 4th WSEAS Int. Conf. on HEAT TRANSFER THERMAL ENGINEERING and ENVIRONMENT Elounda Geece August - 6 (pp6-) Consevative Aveaging Method and its Application fo One Heat Conduction Poblem
More informationAvailable online through ISSN
Intenational eseach Jounal of Pue Algeba -() 01 98-0 Available online though wwwjpainfo ISSN 8 907 SOE ESULTS ON THE GOUP INVESE OF BLOCK ATIX OVE IGHT OE DOAINS Hanyu Zhang* Goup of athematical Jidong
More information0606 ADDITIONAL MATHEMATICS 0606/01 Paper 1, maximum raw mark 80
UNIVERSITY OF CAMBRIDGE INTERNATIONAL EXAMINATIONS Intenational Geneal Cetificate of Seconday Education MARK SCHEME fo the Octobe/Novembe 009 question pape fo the guidance of teaches 0606 ADDITIONAL MATHEMATICS
More informationState tracking control for Takagi-Sugeno models
State tacing contol fo Taagi-Sugeno models Souad Bezzaoucha, Benoît Max,3,DidieMaquin,3 and José Ragot,3 Abstact This wo addesses the model efeence tacing contol poblem It aims to highlight the encouteed
More informationScattering in Three Dimensions
Scatteing in Thee Dimensions Scatteing expeiments ae an impotant souce of infomation about quantum systems, anging in enegy fom vey low enegy chemical eactions to the highest possible enegies at the LHC.
More informationMEASURES OF BLOCK DESIGN EFFICIENCY RECOVERING INTERBLOCK INFORMATION
MEASURES OF BLOCK DESIGN EFFICIENCY RECOVERING INTERBLOCK INFORMATION Walte T. Fedee 337 Waen Hall, Biometics Unit Conell Univesity Ithaca, NY 4853 and Tey P. Speed Division of Mathematics & Statistics,
More informationMethod for Approximating Irrational Numbers
Method fo Appoximating Iational Numbes Eic Reichwein Depatment of Physics Univesity of Califonia, Santa Cuz June 6, 0 Abstact I will put foth an algoithm fo poducing inceasingly accuate ational appoximations
More informationIntegral Control via Bias Estimation
1 Integal Contol via Bias stimation Consie the sstem ẋ = A + B +, R n, R p, R m = C +, R q whee is an nknown constant vecto. It is possible to view as a step istbance: (t) = 0 1(t). (If in fact (t) vaies
More informationMarkscheme May 2017 Calculus Higher level Paper 3
M7/5/MATHL/HP3/ENG/TZ0/SE/M Makscheme May 07 Calculus Highe level Pape 3 pages M7/5/MATHL/HP3/ENG/TZ0/SE/M This makscheme is the popety of the Intenational Baccalaueate and must not be epoduced o distibuted
More informationHomework # 3 Solution Key
PHYSICS 631: Geneal Relativity Homewok # 3 Solution Key 1. You e on you hono not to do this one by hand. I ealize you can use a compute o simply look it up. Please don t. In a flat space, the metic in
More informationSurveillance Points in High Dimensional Spaces
Société de Calcul Mathématique SA Tools fo decision help since 995 Suveillance Points in High Dimensional Spaces by Benad Beauzamy Januay 06 Abstact Let us conside any compute softwae, elying upon a lage
More informationMiskolc Mathematical Notes HU e-issn Tribonacci numbers with indices in arithmetic progression and their sums. Nurettin Irmak and Murat Alp
Miskolc Mathematical Notes HU e-issn 8- Vol. (0), No, pp. 5- DOI 0.85/MMN.0.5 Tibonacci numbes with indices in aithmetic pogession and thei sums Nuettin Imak and Muat Alp Miskolc Mathematical Notes HU
More informationRight-handed screw dislocation in an isotropic solid
Dislocation Mechanics Elastic Popeties of Isolated Dislocations Ou study of dislocations to this point has focused on thei geomety and thei ole in accommodating plastic defomation though thei motion. We
More informationMotion along curved path *
OpenStax-CNX module: m14091 1 Motion along cuved path * Sunil Kuma Singh This wok is poduced by OpenStax-CNX and licensed unde the Ceative Commons Attibution License 2.0 We all expeience motion along a
More informationTransformations in Homogeneous Coordinates
Tansfomations in Homogeneous Coodinates (Com S 4/ Notes) Yan-Bin Jia Aug 4 Complete Section Homogeneous Tansfomations A pojective tansfomation of the pojective plane is a mapping L : P P defined as u a
More informationAn Adaptive Neural-Network Model-Following Speed Control of PMSM Drives for Electric Vehicle Applications
Poceedings of the 9th WSEAS Intenational Confeence on Applied Mathematics, Istanbul, Tuey, May 27-29, 2006 (pp412-417) An Adaptive Neual-Netwo Model-Following Speed Contol of PMSM Dives fo Electic Vehicle
More informationAalborg Universitet. Load Estimation from Natural input Modal Analysis Aenlle, Manuel López; Brincker, Rune; Canteli, Alfonso Fernández
Aalbog Univesitet Load Estimation fom atual input Modal Analysis Aenlle, Manuel López; Bincke, Rune; Canteli, Alfonso Fenández Published in: Confeence Poceedings Publication date: 005 Document Vesion Publishe's
More informationESCI 342 Atmospheric Dynamics I Lesson 3 Fundamental Forces II
Reading: Matin, Section. ROTATING REFERENCE FRAMES ESCI 34 Atmospheic Dnamics I Lesson 3 Fundamental Foces II A efeence fame in which an object with zeo net foce on it does not acceleate is known as an
More informationKOEBE DOMAINS FOR THE CLASSES OF FUNCTIONS WITH RANGES INCLUDED IN GIVEN SETS
Jounal of Applied Analysis Vol. 14, No. 1 2008), pp. 43 52 KOEBE DOMAINS FOR THE CLASSES OF FUNCTIONS WITH RANGES INCLUDED IN GIVEN SETS L. KOCZAN and P. ZAPRAWA Received Mach 12, 2007 and, in evised fom,
More informationModel and Controller Order Reduction for Infinite Dimensional Systems
IT J. Eng. Sci., Vol. 4, No.,, -6 Model and Contolle Ode Reduction fo Infinite Dimensional Systems Fatmawati,*, R. Saagih,. Riyanto 3 & Y. Soehayadi Industial and Financial Mathematics Goup email: fatma47@students.itb.ac.id;
More informationDIMENSIONALITY LOSS IN MIMO COMMUNICATION SYSTEMS
DIMENSIONALITY LOSS IN MIMO COMMUNICATION SYSTEMS Segey Loya, Amma Koui School of Infomation Technology and Engineeing (SITE) Univesity of Ottawa, 6 Louis Pasteu, Ottawa, Ontaio, Canada, KN 6N5 Email:
More informationPhysics 2A Chapter 10 - Moment of Inertia Fall 2018
Physics Chapte 0 - oment of netia Fall 08 The moment of inetia of a otating object is a measue of its otational inetia in the same way that the mass of an object is a measue of its inetia fo linea motion.
More informationInteraction of Feedforward and Feedback Streams in Visual Cortex in a Firing-Rate Model of Columnar Computations. ( r)
Supplementay mateial fo Inteaction of Feedfowad and Feedback Steams in Visual Cotex in a Fiing-Rate Model of Columna Computations Tobias Bosch and Heiko Neumann Institute fo Neual Infomation Pocessing
More informationThe Strain Compatibility Equations in Polar Coordinates RAWB, Last Update 27/12/07
The Stain Compatibility Equations in Pola Coodinates RAWB Last Update 7//7 In D thee is just one compatibility equation. In D polas it is (Equ.) whee denotes the enineein shea (twice the tensoial shea)
More informationAdvanced Problems of Lateral- Directional Dynamics!
Advanced Poblems of Lateal- Diectional Dynamics! Robet Stengel, Aicaft Flight Dynamics! MAE 331, 216 Leaning Objectives 4 th -ode dynamics! Steady-state esponse to contol! Tansfe functions! Fequency esponse!
More informationQuestion 1: The dipole
Septembe, 08 Conell Univesity, Depatment of Physics PHYS 337, Advance E&M, HW #, due: 9/5/08, :5 AM Question : The dipole Conside a system as discussed in class and shown in Fig.. in Heald & Maion.. Wite
More informationOn the integration of the equations of hydrodynamics
Uebe die Integation de hydodynamischen Gleichungen J f eine u angew Math 56 (859) -0 On the integation of the equations of hydodynamics (By A Clebsch at Calsuhe) Tanslated by D H Delphenich In a pevious
More informationIntroduction to Mathematical Statistics Robert V. Hogg Joeseph McKean Allen T. Craig Seventh Edition
Intoduction to Mathematical Statistics Robet V. Hogg Joeseph McKean Allen T. Caig Seventh Edition Peason Education Limited Edinbugh Gate Halow Essex CM2 2JE England and Associated Companies thoughout the
More informationUnobserved Correlation in Ascending Auctions: Example And Extensions
Unobseved Coelation in Ascending Auctions: Example And Extensions Daniel Quint Univesity of Wisconsin Novembe 2009 Intoduction In pivate-value ascending auctions, the winning bidde s willingness to pay
More informationPsychometric Methods: Theory into Practice Larry R. Price
ERRATA Psychometic Methods: Theoy into Pactice Lay R. Pice Eos wee made in Equations 3.5a and 3.5b, Figue 3., equations and text on pages 76 80, and Table 9.1. Vesions of the elevant pages that include
More informationPROBLEM SET #1 SOLUTIONS by Robert A. DiStasio Jr.
POBLM S # SOLUIONS by obet A. DiStasio J. Q. he Bon-Oppenheime appoximation is the standad way of appoximating the gound state of a molecula system. Wite down the conditions that detemine the tonic and
More informationEasy. r p 2 f : r p 2i. r p 1i. r p 1 f. m blood g kg. P8.2 (a) The momentum is p = mv, so v = p/m and the kinetic energy is
Chapte 8 Homewok Solutions Easy P8. Assume the velocity of the blood is constant ove the 0.60 s. Then the patient s body and pallet will have a constant velocity of 6 0 5 m 3.75 0 4 m/ s 0.60 s in the
More informationPhysics 2020, Spring 2005 Lab 5 page 1 of 8. Lab 5. Magnetism
Physics 2020, Sping 2005 Lab 5 page 1 of 8 Lab 5. Magnetism PART I: INTRODUCTION TO MAGNETS This week we will begin wok with magnets and the foces that they poduce. By now you ae an expet on setting up
More informationSemicanonical basis generators of the cluster algebra of type A (1)
Semicanonical basis geneatos of the cluste algeba of type A (1 1 Andei Zelevinsky Depatment of Mathematics Notheasten Univesity, Boston, USA andei@neu.edu Submitted: Jul 7, 006; Accepted: Dec 3, 006; Published:
More informationReview: Electrostatics and Magnetostatics
Review: Electostatics and Magnetostatics In the static egime, electomagnetic quantities do not vay as a function of time. We have two main cases: ELECTROSTATICS The electic chages do not change postion
More informationHopefully Helpful Hints for Gauss s Law
Hopefully Helpful Hints fo Gauss s Law As befoe, thee ae things you need to know about Gauss s Law. In no paticula ode, they ae: a.) In the context of Gauss s Law, at a diffeential level, the electic flux
More informationMULTILAYER PERCEPTRONS
Last updated: Nov 26, 2012 MULTILAYER PERCEPTRONS Outline 2 Combining Linea Classifies Leaning Paametes Outline 3 Combining Linea Classifies Leaning Paametes Implementing Logical Relations 4 AND and OR
More informationDouble-angle & power-reduction identities. Elementary Functions. Double-angle & power-reduction identities. Double-angle & power-reduction identities
Double-angle & powe-eduction identities Pat 5, Tigonomety Lectue 5a, Double Angle and Powe Reduction Fomulas In the pevious pesentation we developed fomulas fo cos( β) and sin( β) These fomulas lead natually
More informationJournal of Inequalities in Pure and Applied Mathematics
Jounal of Inequalities in Pue and Applied Mathematics COEFFICIENT INEQUALITY FOR A FUNCTION WHOSE DERIVATIVE HAS A POSITIVE REAL PART S. ABRAMOVICH, M. KLARIČIĆ BAKULA AND S. BANIĆ Depatment of Mathematics
More informationI( x) t e. is the total mean free path in the medium, [cm] tis the total cross section in the medium, [cm ] A M
t I ( x) I e x x t Ie (1) whee: 1 t is the total mean fee path in the medium, [cm] N t t -1 tis the total coss section in the medium, [cm ] A M 3 is the density of the medium [gm/cm ] v 3 N= is the nuclea
More informationDo Managers Do Good With Other People s Money? Online Appendix
Do Manages Do Good With Othe People s Money? Online Appendix Ing-Haw Cheng Haison Hong Kelly Shue Abstact This is the Online Appendix fo Cheng, Hong and Shue 2013) containing details of the model. Datmouth
More informationMASSACHUSETTS INSTITUTE OF TECHNOLOGY Physics Department Physics 8.07: Electromagnetism II September 15, 2012 Prof. Alan Guth PROBLEM SET 2
MASSACHUSETTS INSTITUTE OF TECHNOLOGY Physics Depatment Physics 8.07: Electomagnetism II Septembe 5, 202 Pof. Alan Guth PROBLEM SET 2 DUE DATE: Monday, Septembe 24, 202. Eithe hand it in at the lectue,
More informationWhat to Expect on the Placement Exam
What to Epect on the Placement Eam Placement into: MTH o MTH 44 05 05 The ACCUPLACER placement eam is an adaptive test ceated by the College Boad Educational Testing Sevice. This document was ceated to
More informationMEASURING CHINESE RISK AVERSION
MEASURING CHINESE RISK AVERSION --Based on Insuance Data Li Diao (Cental Univesity of Finance and Economics) Hua Chen (Cental Univesity of Finance and Economics) Jingzhen Liu (Cental Univesity of Finance
More information