Integral Control via Bias Estimation
|
|
- Howard Stewart
- 5 years ago
- Views:
Transcription
1 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 with time, bt moe slowl than the othe sstem namics, then moelling the istbance as a step ma be a goo appoimation.) Let s consie as the state of a namical sstem with nknown initial conitions: ḋ = 0, 0 nknown (It is also possible to teat othe namics in this wa; I have aske o to o so in Poblems 2 an 3 of Poblem Set 3.) Sppose that we wish to foce ( t) to asmptoticall tack a constant efeence signal espite the nknown istbance. We have seen two appoaches to this poblem. In each case, we se state feeback to stabilize the sstem; this entails no loss of genealit becase we can alwas se an obseve to econstct the state. (In Poblem 1 of Poblem Set 3, o ae aske to veif that this pocee woks.) O two appoaches ae, fist, to se a constant gain pecompensato: N B ( s I A ) 1 C
2 2 If the close loop sstem is stable, then we can calclate that the esponse to a step comman (t) = 0 1(t) an step istbance (t) = 0 1(t) satisfies (t) ss, whee ss := C( A + B) 1 BN 0 + [C( A + B) 1 + ] 0 If C( A + B) 1 B is ight invetible, then setting N = [C( A + B) 1 B] # iels ss := 0 + [C( A + B) 1 + ] 0 The isavantages of this scheme ae that it cannot fo the effects of istbances an small paamete vaiations. An altenate appoach that oes accont fo istbances an paamete vaiations is to se integal contol: B ( si A ) 1 C I w I / s e We have seen in class that if the close loop sstem is stable, then the stea state esponse to a step comman an a step istbance satisfies (t) ss, whee ss := 0. Hence, pefect comman tacking an istbance ejection ae possible; moeove, the sstem is insensitive to small moelling eos. Of cose, in pactice we won't sall be able to mease the states of the plant. Hence, we mst se an obseve to estimate these states,
3 3 as epicte in the following iagam. In Poblem 1 of Poblem Set 3, o ae aske to show that this sstem is stable if the state feeback sstem in the pevios iagam is stable, an if the obseve is stable. B ( si A ) 1 C ^ Obseve I w I / s e Note that the contol inpt in this configation oes not epen eplicitl pon the comman signal. It is often possible to mease, an hence we can consie sing this measement in a feefowa contol scheme as we i in Poblem 3 of Poblem Set 2. The avantage of the eslting Two Degee of eeom (2DO) contol topolog is that it affos geate feeom in achieving esign taeoffs.
4 4 Altenatel, let s sppose fo the sake of agment that we can mease the state of the istbance. We can then consie sing this measement in a feefowa/feeback contol law = ˆ I w + G as shown below: G B ( si A ) 1 C ^ Obseve I w I / s e Pesmabl, b sing feefowa fom the istbance, we can obtain a faste esponse to the istbance than othewise. Thee is one poblem: we will geneall not be able to mease the istbance! Recall, howeve, that a step istbance ma be viewe as the otpt of a namical sstem consisting solel of integatos: ḋ = 0, 0 nknown
5 5 Since we nee to se an obseve anwa, sppose that we esign the obseve, if possible, to estimate the state of the istbance as well as that of the plant, an se a contol law = ˆ I w + G ˆ B ( si A ) 1 C G ^ ^ Obseve I w I / s e Becase a step istbance ma be viewe as an nknown bias, the obseve in the above iagam is sometimes teme an "nknown bias estimato". A simila pocee ma be se to estimate the state of othe sots of istbances. We shall now consie the poblem of esigning an obseve to estimate the istbance. Becase the concepts we nee fo this o not epen pon the se of integal contol in the above iagam, we will instea eplain the pocee base pon the simple contol scheme with constant gain pecompensato. Once we know how to esign an obseve fo the istbance, the eslt can be applie to the poblem pose above. The following iscssion is aapte fom W. J. Rgh, Linea Sstem Theo, PenticeHall, 1993
6 6 Consie the sstem epicte below: N B ( s I A ) 1 C G ^ ^ Obseve The state eqations fo this configation ae: Plant: ẋ = A + B + = C + Obseve: ˆẋ ˆ = A ˆ 0 0 ˆ + B 0 + L ŷ ŷ = [ C ] ˆˆ L 2 ( ), L = L 1 Contol: = ˆ + G ˆ + N We mst answe seveal qestions: (1) When can a stable obseve fo an w be esigne? (2) When is the close loop sstem stable? (3) Does (t) 0 as esie? We also nee to fin vales fo, L, N, an G.
7 7 Theoem: Given the sstem escibe above, efine P (s) = C( si A) 1 B an P (s) = C(sI A) 1 + Assme that an (i) ( A, B) is contollable, (ii) ( A,C) is obsevable, (iii) nomal ank P (s) = q (iv) ( A, B,C) has no zeos at s = 0 (v) (vi) (vii) ( A, ) is contollable, nomal ank P (s) = m ( A,,C, ) has no zeos at s = 0 Then an L ma be chosen to stabilize the eslting close loop sstem, an N an G ma be chosen so that the stea state esponse to a step comman (t) = 0 1(t) an a step istbance (t) = 0 1(t) satisfies (t) ss = 0. Notes: (1) If A has no eigenvales at s = 0, then conitions (iv) an (vi) ma be eplace b ank P (0) = q an ank P w (0) = m, espectivel. (2) Conition (iii) implies that thee ae at least as man contol inpts as contolle otpts, an that these otpts ae inepenent. (3) Conitions (v)(vii) essentiall inse that all the istbance states affect the stea state otpts of the sstem. These conitions will gaantee that we can constct an obseve fo the istbance states.
8 8 Poof: ist sbstitte the eqation fo ŷ into the obseve; this iels: ˆẋ ˆ = ( à L C ) ˆˆ + B 0 + L = A L 1 C L 1 ˆ L 2 C L 2 ˆ + B 0 + L 1 L 2 whee à = A 0 0, C = [ C ]. Define the estimation eo states := ˆ an := ˆ. Then the estimation eo namics ae given b: ẋ ḋ = A L1C L 1 L 2 C L 2. It follows that we can esign a stable obseve if the matices constitte an obsevable pai. Using the feeback contol ( Ã, C ) = ˆ + G ˆ + N iels the following state space esciption fo the close loop sstem: ẋ = A + B( ˆ + Gŵ + N) + w ˆẋ ˆ = A L1C L 2 C ( ) + L 1 L 1 ˆ L 2 ˆ + B 0 ˆ + G ˆ + N L C + 2 ( ) Combining these eqations iels: ẋ A B BG BN ˆẋ = L 1 C A B L 1 C + BG L 1 L 2 ˆ + BN + L 1 ˆ L 2 C L 2 C L 2 ˆ 0 L 2
9 9 = [ C 0 0 ] ˆ + ˆ As sal, it is ifficlt to etemine an close loop popeties in these cooinates. Let s instea change cooinates to. Using the fact that ḋ = ˆḋ (becase is a constant) iels (afte some algeba) that: ẋ A B B BG BN + BG ẋ = 0 A L 1 C L ḋ 0 L 2 C L = [ C 0 0 ] + It is clea fom the above eqations that (a) Thee is a sepaation pinciple: the close loop eigenvales ae the eigenvales of the state feeback, A B, pls those of the obseve fo ˆ an ˆ. It follows that if ( A, B) is contollable, an Ã, C ( ) is obsevable, then we ma alwas obtain a stable close loop sstem. (b) If the close loop sstem is stable, then the stea state esponse to a step comman (t) = 0 1(t) an a step istbance (t) = 0 1(t) appoaches a constant vale. Hence, the eivatives of the state vaiables asmptoticall appoach zeo. Setting the left han sie of the above eqation eqal to zeo ths iels that an ss = 0 ss = 0 ( ) 1 BN 0 + C( A + B) C( A + B) 1 BG ss := C A + B [ ] 0
10 Sppose that C( A + B) 1 B is ight invetible. (Right invetibilit is gaantee b assmptions (iii) an (iv).) Then setting 10 an N = [ C( A + B) 1 B] # G = N[ C( A + B) 1 + ] iels ss = 1. The onl thing that emains to be poven is that o assmptions gaantee that Ã, C ( ) is obsevable. We o this b showing that ank λi à λi A = ank 0 λi = n + m, C C whee λ is eithe eqal to an eigenvale of A, o λ = 0. Case 1: Sppose that λ 0 is an eigenvale of A. Then λi A ank 0 λi = n + m C if an onl if this mati has n + m lineal inepenent colmns. Becase λ 0, it is clea that the last m colmns ae lineal inepenent among themselves an ae also lineal inepenent fom the fist n colmns. Hence λi A ank 0 λi = n + m ank λi A C = n C if an onl if λ is an obsevable eigenvale of A.
11 11 Case 2: Consie λ = 0. The ank test eces to eqiing that ank A C = n + m This conition is implie b assmptions (ii) an (v)(vii). ### To smmaize: Choose so that A B is stable Choose L 1 an L 2 so that A 0 0 L 1 L [ 2 C ] is stable Set N = [ C( A + B) 1 B] # an G = N[ C( A + B) 1 + ] Then ( t) 0, 0, 0. It is inteesting to note that this contol scheme is also a fom of integal contol; it is jst that the integatos ae bie in the obseve. Inee, we have ˆ = L 2 ŷ ( ) o, in block iagam fom ^ L 2. ^ I / s ^
A 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 informationf(y) signal norms system gain bounded input bounded output (BIBO) stability For what G(s) and f( ) is the closed-loop system stable?
Lecte 5 Inpt otpt stabilit Cose Otline o How to make a cicle ot of the point + i, and diffeent was to sta awa fom it... Lecte -3 Lecte 4-6 Modelling and basic phenomena (lineaization, phase plane, limit
More informationMuch that has already been said about changes of variable relates to transformations between different coordinate systems.
MULTIPLE INTEGRLS I P Calculus Cooinate Sstems Much that has alea been sai about changes of vaiable elates to tansfomations between iffeent cooinate sstems. The main cooinate sstems use in the solution
More informationQuantum Mechanics I - Session 5
Quantum Mechanics I - Session 5 Apil 7, 015 1 Commuting opeatos - an example Remine: You saw in class that Â, ˆB ae commuting opeatos iff they have a complete set of commuting obsevables. In aition you
More informationNotes for the standard central, single mass metric in Kruskal coordinates
Notes fo the stana cental, single mass metic in Kuskal cooinates I. Relation to Schwazschil cooinates One oiginally elates the Kuskal cooinates to the Schwazschil cooinates in the following way: u = /2m
More informationHomework Set 3 Physics 319 Classical Mechanics
Homewok Set 3 Phsics 319 lassical Mechanics Poblem 5.13 a) To fin the equilibium position (whee thee is no foce) set the eivative of the potential to zeo U 1 R U0 R U 0 at R R b) If R is much smalle than
More informationPhysics Courseware Physics II Electric Field and Force
Physics Cousewae Physics II lectic iel an oce Coulomb s law, whee k Nm /C test Definition of electic fiel. This is a vecto. test Q lectic fiel fo a point chage. This is a vecto. Poblem.- chage of µc is
More informationPH126 Exam I Solutions
PH6 Exam I Solutions q Q Q q. Fou positively chage boies, two with chage Q an two with chage q, ae connecte by fou unstetchable stings of equal length. In the absence of extenal foces they assume the equilibium
More informationData Flow Anomaly Analysis
Pof. D. Liggesmeye, 1 Contents Data flows an ata flow anomalies State machine fo ata flow anomaly analysis Example withot loops Example with loops Data Flow Anomaly Analysis Softwae Qality Assance Softwae
More informationSession outline. Introduction to Feedback Control. The Idea of Feedback. Automatic control. Basic setting. The feedback principle
Session otline Intodction to Feedback Contol Kal-Eik Åzen, Anton Cevin Feedback and feedfowad PID Contol State-space models Tansfe fnction models Contol design sing pole placement State feedback and obseves
More informationStability of a Discrete-Time Predator-Prey System with Allee Effect
Nonlinea Analsis an Diffeential Equations, Vol. 4, 6, no. 5, 5-33 HIKARI Lt, www.m-hikai.com http://.oi.og/.988/nae.6.633 Stabilit of a Discete-Time Peato-Pe Sstem with Allee Effect Ming Zhao an Yunfei
More informationHow to Obtain Desirable Transfer Functions in MIMO Systems Under Internal Stability Using Open and Closed Loop Control
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-03-006 June, 03 Panos J. Antsaklis
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 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 informationChapter 7 Singular Value Decomposition
EE448/58 Vesion. John Stensy Chapte 7 Singla Vale Decomposition This chapte coves the singla vale decomposition (SVD) of an m n matix. This algoithm has applications in many aeas inclding nmeical analysis
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 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 informationConservation of Linear Momentum using RTT
07/03/2017 Lectue 21 Consevation of Linea Momentum using RTT Befoe mi-semeste exam, we have seen the 1. Deivation of Reynols Tanspot Theoem (RTT), 2. Application of RTT in the Consevation of Mass pinciple
More information15. SIMPLE MHD EQUILIBRIA
15. SIMPLE MHD EQUILIBRIA In this Section we will examine some simple examples of MHD equilibium configuations. These will all be in cylinical geomety. They fom the basis fo moe the complicate equilibium
More informationSimultaneous state and unknown inputs estimation with PI and PMI observers for Takagi Sugeno model with unmeasurable premise variables
Simultaneous state an unknown inputs estimation with PI an PMI obseves fo Takagi Sugeno moel with unmeasuable pemise vaiables Dalil Ichalal, Benoît Max, José Ragot an Diie Maquin Abstact In this pape,
More information556: MATHEMATICAL STATISTICS I
556: MATHEMATICAL STATISTICS I CHAPTER 5: STOCHASTIC CONVERGENCE The following efinitions ae state in tems of scala anom vaiables, but exten natually to vecto anom vaiables efine on the same obability
More informationPhysics 121 Hour Exam #5 Solution
Physics 2 Hou xam # Solution This exam consists of a five poblems on five pages. Point values ae given with each poblem. They add up to 99 points; you will get fee point to make a total of. In any given
More informationParticle Systems. University of Texas at Austin CS384G - Computer Graphics Fall 2010 Don Fussell
Paticle Systems Univesity of Texas at Austin CS384G - Compute Gaphics Fall 2010 Don Fussell Reading Requied: Witkin, Paticle System Dynamics, SIGGRAPH 97 couse notes on Physically Based Modeling. Witkin
More informationFrom Errors to Uncertainties in Basic Course in Electrical Measurements. Vladimir Haasz, Milos Sedlacek
Fom Eos to ncetainties in asic Cose in Electical Measements Vladimi Haasz, Milos Sedlacek Czech Technical nivesity in Page, Faclty of Electical Engineeing, Technicka, CZ-667 Page, Czech epblic phone:40
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 informationCSCE 478/878 Lecture 4: Experimental Design and Analysis. Stephen Scott. 3 Building a tree on the training set Introduction. Outline.
In Homewok, you ae (supposedly) Choosing a data set 2 Extacting a test set of size > 3 3 Building a tee on the taining set 4 Testing on the test set 5 Repoting the accuacy (Adapted fom Ethem Alpaydin and
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 informationSupplementary Information for On characterizing protein spatial clusters with correlation approaches
Supplementay Infomation fo On chaacteizing potein spatial clustes with coelation appoaches A. Shivananan, J. Unnikishnan, A. Raenovic Supplementay Notes Contents Deivation of expessions fo p = a t................................
More informationSPH4UI 28/02/2011. Total energy = K + U is constant! Electric Potential Mr. Burns. GMm
8//11 Electicity has Enegy SPH4I Electic Potential M. Buns To sepaate negative an positive chages fom each othe, wok must be one against the foce of attaction. Theefoe sepeate chages ae in a higheenegy
More informationFigure 1. We will begin by deriving a very general expression before returning to Equations 1 and 2 to determine the specifics.
Deivation of the Laplacian in Spheical Coodinates fom Fist Pinciples. Fist, let me state that the inspiation to do this came fom David Giffiths Intodction to Electodynamics textbook Chapte 1, Section 4.
More information2. Electrostatics. Dr. Rakhesh Singh Kshetrimayum 8/11/ Electromagnetic Field Theory by R. S. Kshetrimayum
2. Electostatics D. Rakhesh Singh Kshetimayum 1 2.1 Intoduction In this chapte, we will study how to find the electostatic fields fo vaious cases? fo symmetic known chage distibution fo un-symmetic known
More informationGeneral Relativity Homework 5
Geneal Relativity Homewok 5. In the pesence of a cosmological constant, Einstein s Equation is (a) Calculate the gavitational potential point souce with = M 3 (). R µ Rg µ + g µ =GT µ. in the Newtonian
More informationLab 10: Newton s Second Law in Rotation
Lab 10: Newton s Second Law in Rotation We can descibe the motion of objects that otate (i.e. spin on an axis, like a popelle o a doo) using the same definitions, adapted fo otational motion, that we have
More information2.3. SLIDING MODE BASED OUTER CONTROL LOOP FOR INDUCTION MOTOR DRIVES WITH FORCED DYNAMICS
2.3. SLIDING MODE BASED OUTER CONTROL LOOP FOR INDUCTION MOTOR DRIVES WITH FORCED DYNAMICS Abstact: Though the loa toque estimation, the basic FDC base IM ive contol system pesente in the last two sections
More informationLab #0. Tutorial Exercises on Work and Fields
Lab #0 Tutoial Execises on Wok and Fields This is not a typical lab, and no pe-lab o lab epot is equied. The following execises will emind you about the concept of wok (fom 1130 o anothe intoductoy mechanics
More informationA Note on Irreducible Polynomials and Identity Testing
A Note on Irrecible Polynomials an Ientity Testing Chanan Saha Department of Compter Science an Engineering Inian Institte of Technology Kanpr Abstract We show that, given a finite fiel F q an an integer
More informationPHYS 301 HOMEWORK #10 (Optional HW)
PHYS 301 HOMEWORK #10 (Optional HW) 1. Conside the Legende diffeential equation : 1 - x 2 y'' - 2xy' + m m + 1 y = 0 Make the substitution x = cos q and show the Legende equation tansfoms into d 2 y 2
More informationMath 301: The Erdős-Stone-Simonovitz Theorem and Extremal Numbers for Bipartite Graphs
Math 30: The Edős-Stone-Simonovitz Theoem and Extemal Numbes fo Bipatite Gaphs May Radcliffe The Edős-Stone-Simonovitz Theoem Recall, in class we poved Tuán s Gaph Theoem, namely Theoem Tuán s Theoem Let
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 information15 Solving the Laplace equation by Fourier method
5 Solving the Laplace equation by Fouie method I aleady intoduced two o thee dimensional heat equation, when I deived it, ecall that it taes the fom u t = α 2 u + F, (5.) whee u: [0, ) D R, D R is the
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 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 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 informationME 210 Applied Mathematics for Mechanical Engineers
Tangent and Ac Length of a Cuve The tangent to a cuve C at a point A on it is defined as the limiting position of the staight line L though A and B, as B appoaches A along the cuve as illustated in the
More informationPhysics 235 Chapter 5. Chapter 5 Gravitation
Chapte 5 Gavitation In this Chapte we will eview the popeties of the gavitational foce. The gavitational foce has been discussed in geat detail in you intoductoy physics couses, and we will pimaily focus
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 informationMath 124B February 02, 2012
Math 24B Febuay 02, 202 Vikto Gigoyan 8 Laplace s equation: popeties We have aleady encounteed Laplace s equation in the context of stationay heat conduction and wave phenomena. Recall that in two spatial
More information4. Compare the electric force holding the electron in orbit ( r = 0.53
Electostatics WS Electic Foce an Fiel. Calculate the magnitue of the foce between two 3.60-µ C point chages 9.3 cm apat.. How many electons make up a chage of 30.0 µ C? 3. Two chage ust paticles exet a
More information7.2. Coulomb s Law. The Electric Force
Coulomb s aw Recall that chaged objects attact some objects and epel othes at a distance, without making any contact with those objects Electic foce,, o the foce acting between two chaged objects, is somewhat
More informationVersion 1.0. General Certificate of Education (A-level) June Mathematics MM04. (Specification 6360) Mechanics 4. Final.
Vesion 1.0 Geneal Cetificate of Education (A-level) June 011 Mathematics MM04 (Specification 660) Mechanics 4 Final Mak Scheme Mak schemes ae pepaed by the Pincipal Examine and consideed, togethe with
More informationThat is, the acceleration of the electron is larger than the acceleration of the proton by the same factor the electron is lighter than the proton.
PHYS 55 Pactice Test Solutions Fall 8 Q: [] poton an an electon attact each othe electicall so, when elease fom est, the will acceleate towa each othe Which paticle will have a lage acceleation? (Neglect
More informationInformation Retrieval (Relevance Feedback & Query Expansion)
Infomation Retieval (Relevance Feedback & Quey Epansion) Fabio Aiolli http://www.math.unipd.it/~aiolli Dipatimento di Matematica Univesità di Padova Anno Accademico 1 Relevance feedback and quey epansion
More informationCOORDINATE TRANSFORMATIONS - THE JACOBIAN DETERMINANT
COORDINATE TRANSFORMATIONS - THE JACOBIAN DETERMINANT Link to: phsicspages home page. To leave a comment o epot an eo, please use the auilia blog. Refeence: d Inveno, Ra, Intoducing Einstein s Relativit
More information5.61 Physical Chemistry Lecture #23 page 1 MANY ELECTRON ATOMS
5.6 Physical Chemisty Lectue #3 page MAY ELECTRO ATOMS At this point, we see that quantum mechanics allows us to undestand the helium atom, at least qualitatively. What about atoms with moe than two electons,
More informationPushdown Automata (PDAs)
CHAPTER 2 Context-Fee Languages Contents Context-Fee Gammas definitions, examples, designing, ambiguity, Chomsky nomal fom Pushdown Automata definitions, examples, euivalence with context-fee gammas Non-Context-Fee
More informationONE-POINT CODES USING PLACES OF HIGHER DEGREE
ONE-POINT CODES USING PLACES OF HIGHER DEGREE GRETCHEN L. MATTHEWS AND TODD W. MICHEL DEPARTMENT OF MATHEMATICAL SCIENCES CLEMSON UNIVERSITY CLEMSON, SC 29634-0975 U.S.A. E-MAIL: GMATTHE@CLEMSON.EDU, TMICHEL@CLEMSON.EDU
More informationSpring 2001 Physics 2048 Test 3 solutions
Sping 001 Physics 048 Test 3 solutions Poblem 1. (Shot Answe: 15 points) a. 1 b. 3 c. 4* d. 9 e. 8 f. 9 *emembe that since KE = ½ mv, KE must be positive Poblem (Estimation Poblem: 15 points) Use momentum-impulse
More informationPassivity-Based Control of Saturated Induction Motors
Passivity-Base Contol of Satuate Inuction otos Levent U. Gökee, embe, IEEE, awan A. Simaan, Fellow, IEEE, an Chales W. Bice, Senio embe, IEEE Depatment of Electical Engineeing Univesity of South Caolina
More informationThis lecture. Transformations in 2D. Where are we at? Why do we need transformations?
Thi lectue Tanfomation in 2D Thoma Sheme Richa (Hao) Zhang Geomet baic Affine pace an affine tanfomation Ue of homogeneou cooinate Concatenation of tanfomation Intouction to Compute Gaphic CMT 36 Lectue
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 information3.1 Random variables
3 Chapte III Random Vaiables 3 Random vaiables A sample space S may be difficult to descibe if the elements of S ae not numbes discuss how we can use a ule by which an element s of S may be associated
More informationElectric Potential and Gauss s Law, Configuration Energy Challenge Problem Solutions
Poblem 1: Electic Potential an Gauss s Law, Configuation Enegy Challenge Poblem Solutions Consie a vey long o, aius an chage to a unifom linea chage ensity λ a) Calculate the electic fiel eveywhee outsie
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 information18.06 Problem Set 4 Solution
8.6 Poblem Set 4 Solution Total: points Section 3.5. Poblem 2: (Recommended) Find the lagest possible numbe of independent vectos among ) ) ) v = v 4 = v 5 = v 6 = v 2 = v 3 =. Solution (4 points): Since
More informationTable of contents. Statistical analysis. Measures of statistical central tendencies. Measures of variability
Table of contents Statistical analysis Meases of statistical cental tendencies Meases of vaiability Aleatoy ncetainties Epistemic ncetainties Meases of statistical dispesion o deviation The ange Mean diffeence
More informationPhysics 201 Lecture 18
Phsics 0 ectue 8 ectue 8 Goals: Define and anale toque ntoduce the coss poduct Relate otational dnamics to toque Discuss wok and wok eneg theoem with espect to otational motion Specif olling motion (cente
More informationThe Cross Product of Fuzzy Numbers and its Applications in Geology
The Coss Podct of Fzzy Nmbes and its Applications in Geology Dedicated to the 80 th Bithday of Pofesso Gyögy Bádossy Banabás Bede *, János Fodo ** * Depatment of Mechanical and System Engineeing Bdapest
More informationDYNAMIC STABILITY STUDY AND SIMULATION OF THE SYNCHRONOUS MACHINE COUPLED WITH THE NETWORK BY A LINE AND A LOAD IN PARALLEL
IJRRAS 9 (2) Novembe 20 www.apapess.com/volmes/vol9isse2/ijrras_9_2_07.p DYNAMIC STABILITY STUDY AND SIMULATION OF THE SYNCHRONOUS MACHINE COUPLED WITH THE NETWORK BY A LINE AND A LOAD IN PARALLEL Elahem
More informationSkps Media
Skps Media Skps Media Skps Media Skps Media Skps Media Skps Media Skps Media Skps Media Skps Media Skps Media Skps Media Skps Media Skps Media Skps Media Skps Media Skps Media Skps Media Skps Media Skps
More informationECE Spring Prof. David R. Jackson ECE Dept. Notes 5
ECE 634 Sping 06 Pof. David R. Jacson ECE Dept. Notes 5 TM x Sface-Wave Soltion Poblem nde consideation: x h ε, µ z A TM x sface wave is popagating in the z diection (no y vaiation). TM x Sface-Wave Soltion
More information4.[1pt] Two small spheres with charges -4 C and -9 C are held 9.5 m apart. Find the magnitude of the force between them.
. [pt] A peson scuffing he feet on a wool ug on a y ay accumulates a net chage of - 4.uC. How many ecess electons oes this peson get? Coect, compute gets:.63e+4. [pt] By how much oes he mass incease? Coect,
More informationWhen two numbers are written as the product of their prime factors, they are in factored form.
10 1 Study Guide Pages 420 425 Factos Because 3 4 12, we say that 3 and 4 ae factos of 12. In othe wods, factos ae the numbes you multiply to get a poduct. Since 2 6 12, 2 and 6 ae also factos of 12. The
More informationChapter Eight Notes N P U1C8S4-6
Chapte Eight Notes N P UC8S-6 Name Peiod Section 8.: Tigonometic Identities An identit is, b definition, an equation that is alwas tue thoughout its domain. B tue thoughout its domain, that is to sa that
More informationA Hilbert-Type Inequality with Some Parameters and the Integral in Whole Plane
Advances in Pe Mathematics,,, 84-89 doi:.436/am..39 Pblished Online Ma (htt://www.sci.og/jonal/am) A Hilbet-Te Inealit with Some Paametes the Integal in Whole Plane Abstact Zitian Xie, Zheng Zeng Deatment
More informationarxiv: v1 [math.oc] 2 Mar 2009
HOMOGENEOUS APPROXIMATION RECURSIVE OBSERVER DESIGN AND OUTPUT FEEDBACK VINCENT ANDRIEU, LAURENT PRALY, AND ALESSANDRO ASTOLFI axiv:09030298v [mathoc] 2 Ma 2009 Abstact We intouce two new tools that can
More informationCHAPTER 2 DERIVATION OF STATE EQUATIONS AND PARAMETER DETERMINATION OF AN IPM MACHINE. 2.1 Derivation of Machine Equations
1 CHAPTER DERIVATION OF STATE EQUATIONS AND PARAMETER DETERMINATION OF AN IPM MACHINE 1 Deivation of Machine Equations A moel of a phase PM machine is shown in Figue 1 Both the abc an the q axes ae shown
More informationGRAVITATION. Einstein Classes, Unit No. 102, 103, Vardhman Ring Road Plaza, Vikas Puri Extn., New Delhi -18 PG 1
Einstein Classes, Unit No. 0, 0, Vahman Ring Roa Plaza, Vikas Pui Extn., New Delhi -8 Ph. : 96905, 857, E-mail einsteinclasses00@gmail.com, PG GRAVITATION Einstein Classes, Unit No. 0, 0, Vahman Ring Roa
More informationOn the reconstruction of the coronal magnetic field from coronal Hanle / Zeeman observations
On the econstction of the coonal magnetic field fom coonal Hanle / Zeeman obsevations M. Kama & B. Inheste Max-Planck Institte fo Sola System Reseach GERMANY Linda 005 Coonal Magnetic Field Magnetic field
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 informationMAE 210B. Homework Solution #6 Winter Quarter, U 2 =r U=r 2 << 1; ) r << U : (1) The boundary conditions written in polar coordinates,
MAE B Homewok Solution #6 Winte Quate, 7 Poblem a Expecting a elocity change of oe oe a aial istance, the conition necessay fo the ow to be ominate by iscous foces oe inetial foces is O( y ) O( ) = =
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 informationEstimation of the Correlation Coefficient for a Bivariate Normal Distribution with Missing Data
Kasetsat J. (Nat. Sci. 45 : 736-74 ( Estimation of the Coelation Coefficient fo a Bivaiate Nomal Distibution with Missing Data Juthaphon Sinsomboonthong* ABSTRACT This study poposes an estimato of the
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 informationQualifying Examination Electricity and Magnetism Solutions January 12, 2006
1 Qualifying Examination Electicity and Magnetism Solutions Januay 12, 2006 PROBLEM EA. a. Fist, we conside a unit length of cylinde to find the elationship between the total chage pe unit length λ and
More informationA STRONG BOUND FOR THE NUMBER OF SOLUTIONS OF THUE EQUATIONS
Shukhat Alladustov sh.alladustov@gmail.com A STRONG BOUND FOR THE NUMBER OF SOLUTIONS OF THUE EQUATIONS Maste s thesis, Jul 05 Supeviso: Pof. Yui Bilu Leiden Univesit Univesit of Bodeau Contents Intoduction
More informationEN40: Dynamics and Vibrations. Midterm Examination Thursday March
EN40: Dynamics and Vibations Midtem Examination Thusday Mach 9 2017 School of Engineeing Bown Univesity NAME: Geneal Instuctions No collaboation of any kind is pemitted on this examination. You may bing
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 informationLecture 8 - Gauss s Law
Lectue 8 - Gauss s Law A Puzzle... Example Calculate the potential enegy, pe ion, fo an infinite 1D ionic cystal with sepaation a; that is, a ow of equally spaced chages of magnitude e and altenating sign.
More informationNonlinear Control of Heartbeat Models
Nonlinea Contol of Heatbeat Moels Witt THANOM Robet N. K. LOH Depatment of Electical an Compte Engineeing Cente fo Robotics an Avance Atomation Oaklan Univesity Rocheste Michigan 489 U. S. A. ABSTRACT
More informationLecture 16 Root Systems and Root Lattices
1.745 Intoduction to Lie Algebas Novembe 1, 010 Lectue 16 Root Systems and Root Lattices Pof. Victo Kac Scibe: Michael Cossley Recall that a oot system is a pai (V, ), whee V is a finite dimensional Euclidean
More informationGravity and isostasy
Gavity and isostasy Reading: owle p60 74 Theoy of gavity Use two of Newton s laws: ) Univesal law of gavitation: Gmm = m m Univesal gavitational constant G=6.67 x 0 - Nm /kg ) Second law of motion: = ma
More informationb) The array factor of a N-element uniform array can be written
to Eam in Antenna Theo Time: 18 Mach 010, at 8.00 13.00. Location: Polacksbacken, Skivsal You ma bing: Laboato epots, pocket calculato, English ictiona, Råe- Westegen: Beta, Noling-Östeman: Phsics Hanbook,
More informationB da = 0. Q E da = ε. E da = E dv
lectomagnetic Theo Pof Ruiz, UNC Asheville, doctophs on YouTube Chapte Notes The Maxwell quations in Diffeential Fom 1 The Maxwell quations in Diffeential Fom We will now tansfom the integal fom of the
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 informationSolutions to Problems : Chapter 19 Problems appeared on the end of chapter 19 of the Textbook
Solutions to Poblems Chapte 9 Poblems appeae on the en of chapte 9 of the Textbook 8. Pictue the Poblem Two point chages exet an electostatic foce on each othe. Stategy Solve Coulomb s law (equation 9-5)
More informationFields and Waves I Spring 2005 Homework 4. Due 8 March 2005
Homewok 4 Due 8 Mach 005. Inceasing the Beakdown Voltage: This fist question is a mini design poject. You fist step is to find a commecial cable (coaxial o two wie line) fo which you have the following
More informationx 1 b 1 Consider the midpoint x 0 = 1 2
1 chapte 2 : oot-finding def : Given a function f(), a oot is a numbe satisfying f() = 0. e : f() = 2 3 = ± 3 question : How can we find the oots of a geneal function f()? 2.1 bisection method idea : Find
More informationConjugate Gradient Methods. Michael Bader. Summer term 2012
Gadient Methods Outlines Pat I: Quadatic Foms and Steepest Descent Pat II: Gadients Pat III: Summe tem 2012 Pat I: Quadatic Foms and Steepest Descent Outlines Pat I: Quadatic Foms and Steepest Descent
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 informationThat is, the acceleration of the electron is larger than the acceleration of the proton by the same factor the electron is lighter than the proton.
PHY 8 Test Pactice Solutions Sping Q: [] A poton an an electon attact each othe electically so, when elease fom est, they will acceleate towa each othe. Which paticle will have a lage acceleation? (Neglect
More information