Slide03 Historical Overview Haykin Chapter 3 (Chap 1, 3, 3rd Ed): Single-Layer Perceptrons Multiple Faces of a Single Neuron Part I: Adaptive Filter

Size: px
Start display at page:

Download "Slide03 Historical Overview Haykin Chapter 3 (Chap 1, 3, 3rd Ed): Single-Layer Perceptrons Multiple Faces of a Single Neuron Part I: Adaptive Filter"

Transcription

1 Slide3 Haykin Chaper 3 (Chap, 3, 3rd Ed): Single-Layer Perceprons CPSC Insrucor: Yoonsuck Choe Hisorical Overview McCulloch and Pis (943): neural neworks as compuing machines. Hebb (949): posulaed he firs rule for self-organizing learning. Rosenbla (958): percepron as a firs model of supervised learning. Widrow and Hoff (96): adapive filers using leas-mean-square (LMS) algorihm (dela rule). 2 Muliple Faces of a Single Neuron Wha a single neuron does can be viewed from differen perspecives: Adapive filer: as in signal processing Classifier: as in percepron The wo aspecs will be reviewed, in he above order. Par I: Adapive Filer 3 4

2 Adapive Filering Problem Consider an unknown dynamical sysem, ha akes m inpus and generaes one oupu. Behavior of he sysem described as is inpu/oupu pair: T : {x(i), d(i); i =, 2,..., n,...} where x(i) = [x (i), x 2 (i),..., x m (i)] T is he inpu and d(i) he desired response (or arge signal). Inpu vecor can be eiher a spaial snapsho or a emporal sequence uniformly spaced in ime. There are wo imporan processes in adapive filering: Filering process: generaion of oupu based on he inpu: y(i) = x T (i)w(i). Adapaive process: auomaic adjusmen of weighs o reduce error: e(i) = d(i) y(i). 5 Unconsrained Opimizaion Techniques How can we adjus w(i) o gradually minimize e(i)? Noe ha e(i) = d(i) y(i) = d(i) x T (i)w(i). Since d(i) and x(i) are fixed, only he change in w(i) can change e(i). In oher words, we wan o minimize he cos funcion E(w) wih respec o he weigh vecor w: Find he opimal soluion w. The necessary condiion for opimaliy is E(w ) =, where he gradien operaor is defined as [ ] T =,,... w w 2 w m Wih his, we ge E(w ) = [ E w, 6 ] E E T,.... w 2 w m Seepes Descen We wan he ieraive updae algorihm o have he following propery: E(w(n )) < E(w(n)). Define he gradien vecor E(w) as g. The ieraive weigh updae rule hen becomes: w(n ) = w(n) ηg(n) where η is a small learning-rae parameer. So we can say, w(n) = w(n ) w(n) = ηg(n) Seepes Descen (con d) We now check if E(w(n )) < E(w(n)). Using firs-order Taylor expansion of E( ) near w(n), E(w(n )) E(w(n)) g T (n) w(n) and w(n) = ηg(n), we ge E(w(n )) E(w(n)) ηg T (n)g(n) So, i is indeed (for small η): = E(w(n)) η g(n) 2. }{{} Posiive! E(w(n )) < E(w(n)). 7 Taylor series: f(x) = f(a) f (a)(x a) f (a)(xa) 2 2!... 8

3 Seepes Descen: Example Seepes Descen: Anoher Example x*xy*y y 7 Gradien of x*xy*y Convergence o opimal w is very slow x Small η: overdamped, smooh rajecory Large η: underdamped, jagged rajecory η oo large: algorihm becomes unsable 9 For f(x) = f(x, y) = x 2 y 2, [ ] f(x, y) = f x, f T y = [2x, 2y] T. Noe ha () he gradien vecors are poining upward, away from he origin, (2) lengh of he vecors are shorer near he origin. If you follow f(x, y), you will end up a he origin. We can see ha he gradien vecors are perpendicular o he level curves. * The vecor lenghs were scaled down by a facor of o avoid cluer. Newon s Mehod Newon s mehod is an exension of seepes descen, where he second-order erm in he Taylor series expansion is used. I is generally faser and shows a less erraic meandering compared o he seepes descen mehod. There are cerain condiions o be me hough, such as he Hessian marix 2 E(w) being posiive definie (for an arbiarry x, x T Hx > ). Gauss-Newon Mehod Applicable for cos-funcions expressed as sum of error squares: E(w) = 2 n e i (w) 2, i= where e i (w) is he error in he i-h rial, wih he weigh w. Recalling he Taylor series f(x) = f(a) f (a)(x a)..., we can express e i (w) evaluaed near e i (w k ) as [ ] T ei e i (w) = e i (w k ) (w w k ). w w=w k In marix noaion, we ge: e(w) = e(w k ) J e (w k )(w w k ). * We will use a slighly differen noaion han he exbook, for clariy. 2

4 Gauss-Newon Mehod (con d) Quick Example: Jacobian Marix J e (w) is he Jacobian marix, where each row is he gradien of e i (w): J e (w) = e w e w 2... e 2 w e 2 w 2... e wn e 2 wn : : : : : : en w en w 2... en wn = ( e (w)) T ( e 2 (w)) T : : ( e n (w)) T Given e(x, y) = e (x, y) e 2 (x, y) = The Jacobian of e(x, y) becomes J e (x, y) = [ e (x,y) x e 2 (x,y) x e (x,y) y e 2 (x,y) y x 2 y 2 cos(x) sin(y) ] = [ 2x sin(x), 2y cos(y) ]. We can hen evaluae J e (w k ) by plugging in acual values of w k ino he Jabobian marix above. For (x, y) = (.5π, π), we ge [ π J e (.5π, π) = sin(.5π) 2π cos(π) ] = [ π 2π ]. 3 4 Gauss-Newon Mehod (con d) Linear Leas-Square Filer Again, saring wih e(w) = e(w k ) J e (w k )(w w k ), Given m inpu and oupu funcion y(i) = φ(x T i w i) where φ(x) = x, i.e., i is linear, and a se of raining samples {x i, d i } n i=, we can define he error vecor for an arbirary weigh w as wha we wan is o se w so ha he error approaches. Tha is, we wan o minimize he norm of e(w): e(w) 2 = e(w k ) 2 2e(w k ) T J e (w k )(w w k ) e(w) = d [x, x 2,..., x n ] T w. where d = [d, d 2,..., d n ] T. Seing X = [x, x 2,..., x n ] T, we ge: e(w) = d Xw. (w w k ) T J T e (w k)j e (w k )(w w k ). Differeniaing he above wr w and seing he resul o, we ge Differeniaing he above wr w, we ge e(w) = X T. So, he Jacobian becomes J e (w) = ( e(w)) T = X. Plugging his in o he Gauss-Newon equaion, we finally ge: J T e (w k)e(w k )J T e (w k)j e (w k )(ww k ) =, from which we ge w = w k (J T e (w k)j e (w k )) J T e (w k)e(w k ). * J T e (w k)j e (w k ) needs o be nonsingular (inverse is needed). 5 w = w k (X T X) X T (d Xw k ) = w k (X T X) X T d (X T X) X T Xw k }{{} = (X T X) X T d. 6 This is Iw k = w k.

5 Poins worh noing: Linear Leas-Square Filer (con d) X does no need o be a square marix! We ge w = (X T X) X T d off he ba parly because he oupu is linear (oherwise, he formula would be more complex). The Jacobian of he error funcion only depends on he inpu, and is invarian wr he weigh w. The facor (X T X) X T (le s call i X ) is like an inverse. Muliply X o boh sides of d = Xw Linear Leas-Square Filer: Example See src/pseudoinv.m. X = ceil(rand(4,2)*), wrue = rand(2,)*, d=x*wrue, w = inv(x *X)*X *d X = wrue = d = hen we ge: w = X d = X X w. }{{} =I 7 w = Leas-Mean-Square Algorihm Cos funcion is based on insananeous values. E(w) = 2 e2 (w) Differeniaing he above wr w, we ge E(w) w Pluggin in e(w) = d x T w, e(w) w e(w) = e(w) w. E(w) = x, and hence w = xe(w). Using his in he seepes descen rule, we ge he LMS algorihm: ŵ n = ŵ n ηx n e n. Noe ha his weigh updae is done wih only one (x i, d i ) pair! 9 Leas-Mean-Square Algorihm: Evaluaion LMS algorihm behaves like a low-pass filer. LMS algorihm is simple, model-independen, and hus robus. LMS does no follow he direcion of seepes descen: Insead, i follows i sochasically (sochasic gradien descen). Slow convergence is an issue. LMS is sensiive o he inpu correlaion marix s condiion number (raio beween larges vs. smalles eigenvalue of he correl. marix). LMS can be shown o converge if he learning rae has he following propery: < η < 2 λ max where λ max is he larges eigenvalue of he correl. marix. 2

6 Improving Convergence in LMS Search-Then-Converge in LMS The main problem arises because of he fixed η. One soluion: Use a ime-varying learning rae: η(n) = c/n, as in sochasic opimizaion heory. A beer alernaive: use a hybrid mehod called search-hen-converge. η(n) = η (n/τ) When n < τ, performance is similar o sandard LMS. When n > τ, i behaves like sochasic opimizaion. η(n) = η n vs. η(n) = η (n/τ) 2 22 The Percepron Model Par II: Percepron Percepron uses a non-linear neuron model (McCulloch-Pis model). v = m if v > w i x i b, y = φ(v) = if v i= Goal: classify inpu vecors ino wo classes

7 Boolean Logic Gaes wih Percepron Unis Wha Perceprons Can Represen =.5 = W2= =.5 =.5 AND = W2= OR = NOT Russel & Norvig w w Oupu = Slope = W Perceprons can represen basic boolean funcions. Oupu=fs Thus, a nework of percepron unis can compue any Boolean funcion. Wha abou XOR or EQUIV? Perceprons can only represen linearly separable funcions. Oupu of he percepron: W I W I >, hen oupu is W I W I, hen oupu is Geomeric Inerpreaion w w Oupu=fs Oupu = Slope = W w w = The Role of he Bias = Slope = W Rearranging W I W I >, hen oupu is, we ge (if W > ) I > W W I W, where poins above he line, he oupu is, and for hose below he line. Compare wih y = W x. W 27 W Wihou he bias ( = ), learning is limied o adjusmen of he slope of he separaing line passing hrough he origin. Three example lines wih differen weighs are shown. 28

8 Limiaion of Perceprons w w Oupu=fs Oupu = Slope = W x Generalizing o n-dimensions z (x,y,z) n = [a b c] T (x,y,z ) y x y z a b c d hp://mahworld.wolfram.com/plane.hml Only funcions where he poins and poins are clearly linearly separable can be represened by perceprons. The geomeric inerpreaion is generalizable o funcions of n argumens, i.e. percepron wih n inpus plus one hreshold (or bias) uni. 29 n = (a, b, c), x = (x, y, z), x = (x, y, z ). Equaion of a plane: n ( x x ) = In shor, ax by cz d =, where a, b, c can serve as he weigh, and d = n x as he bias. For n-d inpu space, he decision boundary becomes a (n )-D hyperplane (-D less han he inpu space). 3 Linear Separabiliy Linear Separabiliy (con d) Linearlyseparable No Linearlyseparable No Linearlyseparable For funcions ha ake ineger or real values as argumens and oupu eiher or. Lef: linearly separable (i.e., can draw a sraigh line beween he classes). Righ: no linearly separable (i.e., perceprons canno represen such a funcion) AND OR XOR Perceprons canno represen XOR! Minsky and Paper (969)? 3 32

9 XOR in Deail Perceprons: A Differen Perspecive # I I XOR 2 w w Oupu = Slope = W x i w 3 4 Oupu=fs θ d W I W I >, hen oupu is : 2 W > W > 3 W > W > 4 W W W W 2 < W W < (from 2, 3, and 4), bu (from ), a conradicion. 33 w T x > b hen, oupu is w T x = w x cos θ > b hen, oupu is x cos θ > b w So, if d = x cos θ in he figure above is greaer han hen, oupu is b, hen oupu =. w Adjusing w changes he il of he decision boundary, and adjusing he bias b (and w ) moves he decision boundary closer or away from he origin. 34 Percepron Learning Rule Percepron Learning Rule (con d) Given a linearly separable se of inpus ha can belong o class C or C 2, The goal of percepron learning is o have w T x > for all inpu in class C w T x for all inpu in class C 2 If all inpus are correcly classified wih he curren weighs w(n), For misclassified inpus (η(n) is he learning rae): w(n ) = w(n) η(n)x(n) if w T x > and x C 2. w(n ) = w(n) η(n)x(n) if w T x and x C. Or, simply x(n ) = w(n) η(n)e(n)x(n), where e(n) = d(n) y(n) (he error). w(n) T x >, for all inpu in class C, and w(n) T x, for all inpu in class C 2, hen w(n ) = w(n) (no change). Oherwise, adjus he weighs

10 Learning in Percepron: Anoher Look Percepron Convergence Theorem x xw w x wx wx w Given a se of linearly separable inpus, Wihou loss of generaliy, assume η =, w() =. Assume he firs n examples C are all misclassified. Then, using w(n ) = w(n) x(n), we ge w(n ) = x() x(2)... x(n). () When a posiive example (C ) is misclassified, w(n ) = w(n) η(n)x(n). When a negaive example (C 2 ) is misclassified, w(n ) = w(n) η(n)x(n). Noe he il in he weigh vecor, and observe how i would change he decision boundary. 37 Since he inpu se is linearly separable, here is a leas on soluion w such ha w T x(n) > for all inpus in C. Define α = min x(n) C w T x(n) >. Muliply boh sides in eq. wih w, we ge: w T w(n) = wt x()wt x(2)...wt x(n). (2) From he wo seps above, we ge: w T w(n ) > nα (3) 38 Percepron Convergence Theorem (con d) Percepron Convergence Theorem (con d) Using Cauchy-Schwarz inequaliy ] w 2 w(n ) 2 [w T 2 w(n ) From he above and w T w(n ) > nα, So, finally, we ge w 2 w(n ) 2 n 2 α 2 w(n ) 2 n2 α 2 w 2 }{{} Firs main resul 39 (4) Taking he Euclidean norm of w(k ) = w(k) x(k), w(k ) 2 = w(k) 2 2w T (k)x(k) x(k) 2 Since all n inpus in C are misclassified, w T (k)x(k) for k =, 2,..., n, w(k ) 2 w(k) 2 x(k) 2 = 2w T (k)x(k), w(k ) 2 w(k) 2 x(k) 2 w(k ) 2 w(k) 2 x(k) 2 Summing up he inequaliies for all k =, 2,..., n, and w() =, we ge w(k ) 2 n x(k) 2 nβ, (5) k= where β = max x (k) C x(k) 2. 4

11 Percepron Convergence Theorem (con d) From eq. 4 and eq. 5, n 2 α 2 w 2 w(n ) 2 nβ Here, α is a consan, depending on he fixed inpu se and he fixed soluion w (so, w is also a consan), and β is also a consan since i depends only on he fixed inpu se. In his case, if n grows o a large value, he above inequaliy will becomes invalid (n is a posiive ineger). Fixed-Incremen Convergence Theorem Le he subses of raining vecors C and C 2 be linearly separable. Le he inpus presened o percepron originae from hese wo subses. The percepron converges afer some n ieraions, in he sense ha w(n ) = w(n ) = w(n 2) =... is a soluion vecor for n n max. Thus, n canno grow beyond a cerain n max, where n 2 max α2 w 2 = n maxβ n max = β w 2 α 2, and when n = n max, all inpus will be correcly classified 4 42 Summary Adapive filer using he LMS algorihm and perceprons are closely relaed (he learning rule is almos idenical). LMS and perceprons are differen, however, since one uses linear acivaion and he oher hard limiers. LMS is used in coninuous learning, while perceprons are rained for only a finie number of seps. Single-neuron or single-layer has severe limis: How can muliple layers help? 43 44

12 XOR wih Mulilayer Perceprons XOR AND Noe: he bias unis are no shown in he nework on he righ, bu hey are needed. Only hree percepron unis are needed o implemen XOR. However, you need wo layers o achieve his. 45

The Rosenblatt s LMS algorithm for Perceptron (1958) is built around a linear neuron (a neuron with a linear

The Rosenblatt s LMS algorithm for Perceptron (1958) is built around a linear neuron (a neuron with a linear In The name of God Lecure4: Percepron and AALIE r. Majid MjidGhoshunih Inroducion The Rosenbla s LMS algorihm for Percepron 958 is buil around a linear neuron a neuron ih a linear acivaion funcion. Hoever,

More information

Course Notes for EE227C (Spring 2018): Convex Optimization and Approximation

Course Notes for EE227C (Spring 2018): Convex Optimization and Approximation Course Noes for EE7C Spring 018: Convex Opimizaion and Approximaion Insrucor: Moriz Hard Email: hard+ee7c@berkeley.edu Graduae Insrucor: Max Simchowiz Email: msimchow+ee7c@berkeley.edu Ocober 15, 018 3

More information

t is a basis for the solution space to this system, then the matrix having these solutions as columns, t x 1 t, x 2 t,... x n t x 2 t...

t is a basis for the solution space to this system, then the matrix having these solutions as columns, t x 1 t, x 2 t,... x n t x 2 t... Mah 228- Fri Mar 24 5.6 Marix exponenials and linear sysems: The analogy beween firs order sysems of linear differenial equaions (Chaper 5) and scalar linear differenial equaions (Chaper ) is much sronger

More information

15. Vector Valued Functions

15. Vector Valued Functions 1. Vecor Valued Funcions Up o his poin, we have presened vecors wih consan componens, for example, 1, and,,4. However, we can allow he componens of a vecor o be funcions of a common variable. For example,

More information

2.7. Some common engineering functions. Introduction. Prerequisites. Learning Outcomes

2.7. Some common engineering functions. Introduction. Prerequisites. Learning Outcomes Some common engineering funcions 2.7 Inroducion This secion provides a caalogue of some common funcions ofen used in Science and Engineering. These include polynomials, raional funcions, he modulus funcion

More information

Section 3.5 Nonhomogeneous Equations; Method of Undetermined Coefficients

Section 3.5 Nonhomogeneous Equations; Method of Undetermined Coefficients Secion 3.5 Nonhomogeneous Equaions; Mehod of Undeermined Coefficiens Key Terms/Ideas: Linear Differenial operaor Nonlinear operaor Second order homogeneous DE Second order nonhomogeneous DE Soluion o homogeneous

More information

Lecture 9: September 25

Lecture 9: September 25 0-725: Opimizaion Fall 202 Lecure 9: Sepember 25 Lecurer: Geoff Gordon/Ryan Tibshirani Scribes: Xuezhi Wang, Subhodeep Moira, Abhimanu Kumar Noe: LaTeX emplae couresy of UC Berkeley EECS dep. Disclaimer:

More information

Lecture 2-1 Kinematics in One Dimension Displacement, Velocity and Acceleration Everything in the world is moving. Nothing stays still.

Lecture 2-1 Kinematics in One Dimension Displacement, Velocity and Acceleration Everything in the world is moving. Nothing stays still. Lecure - Kinemaics in One Dimension Displacemen, Velociy and Acceleraion Everyhing in he world is moving. Nohing says sill. Moion occurs a all scales of he universe, saring from he moion of elecrons in

More information

1 1 + x 2 dx. tan 1 (2) = ] ] x 3. Solution: Recall that the given integral is improper because. x 3. 1 x 3. dx = lim dx.

1 1 + x 2 dx. tan 1 (2) = ] ] x 3. Solution: Recall that the given integral is improper because. x 3. 1 x 3. dx = lim dx. . Use Simpson s rule wih n 4 o esimae an () +. Soluion: Since we are using 4 seps, 4 Thus we have [ ( ) f() + 4f + f() + 4f 3 [ + 4 4 6 5 + + 4 4 3 + ] 5 [ + 6 6 5 + + 6 3 + ]. 5. Our funcion is f() +.

More information

Math Week 14 April 16-20: sections first order systems of linear differential equations; 7.4 mass-spring systems.

Math Week 14 April 16-20: sections first order systems of linear differential equations; 7.4 mass-spring systems. Mah 2250-004 Week 4 April 6-20 secions 7.-7.3 firs order sysems of linear differenial equaions; 7.4 mass-spring sysems. Mon Apr 6 7.-7.2 Sysems of differenial equaions (7.), and he vecor Calculus we need

More information

CHAPTER 10 VALIDATION OF TEST WITH ARTIFICAL NEURAL NETWORK

CHAPTER 10 VALIDATION OF TEST WITH ARTIFICAL NEURAL NETWORK 175 CHAPTER 10 VALIDATION OF TEST WITH ARTIFICAL NEURAL NETWORK 10.1 INTRODUCTION Amongs he research work performed, he bes resuls of experimenal work are validaed wih Arificial Neural Nework. From he

More information

INTRODUCTION TO MACHINE LEARNING 3RD EDITION

INTRODUCTION TO MACHINE LEARNING 3RD EDITION ETHEM ALPAYDIN The MIT Press, 2014 Lecure Slides for INTRODUCTION TO MACHINE LEARNING 3RD EDITION alpaydin@boun.edu.r hp://www.cmpe.boun.edu.r/~ehem/i2ml3e CHAPTER 2: SUPERVISED LEARNING Learning a Class

More information

Dimitri Solomatine. D.P. Solomatine. Data-driven modelling (part 2). 2

Dimitri Solomatine. D.P. Solomatine. Data-driven modelling (part 2). 2 Daa-driven modelling. Par. Daa-driven Arificial di Neural modelling. Newors Par Dimiri Solomaine Arificial neural newors D.P. Solomaine. Daa-driven modelling par. 1 Arificial neural newors ANN: main pes

More information

23.2. Representing Periodic Functions by Fourier Series. Introduction. Prerequisites. Learning Outcomes

23.2. Representing Periodic Functions by Fourier Series. Introduction. Prerequisites. Learning Outcomes Represening Periodic Funcions by Fourier Series 3. Inroducion In his Secion we show how a periodic funcion can be expressed as a series of sines and cosines. We begin by obaining some sandard inegrals

More information

1 Review of Zero-Sum Games

1 Review of Zero-Sum Games COS 5: heoreical Machine Learning Lecurer: Rob Schapire Lecure #23 Scribe: Eugene Brevdo April 30, 2008 Review of Zero-Sum Games Las ime we inroduced a mahemaical model for wo player zero-sum games. Any

More information

MATH 5720: Gradient Methods Hung Phan, UMass Lowell October 4, 2018

MATH 5720: Gradient Methods Hung Phan, UMass Lowell October 4, 2018 MATH 5720: Gradien Mehods Hung Phan, UMass Lowell Ocober 4, 208 Descen Direcion Mehods Consider he problem min { f(x) x R n}. The general descen direcions mehod is x k+ = x k + k d k where x k is he curren

More information

Chapter 6. Systems of First Order Linear Differential Equations

Chapter 6. Systems of First Order Linear Differential Equations Chaper 6 Sysems of Firs Order Linear Differenial Equaions We will only discuss firs order sysems However higher order sysems may be made ino firs order sysems by a rick shown below We will have a sligh

More information

Two Coupled Oscillators / Normal Modes

Two Coupled Oscillators / Normal Modes Lecure 3 Phys 3750 Two Coupled Oscillaors / Normal Modes Overview and Moivaion: Today we ake a small, bu significan, sep owards wave moion. We will no ye observe waves, bu his sep is imporan in is own

More information

KINEMATICS IN ONE DIMENSION

KINEMATICS IN ONE DIMENSION KINEMATICS IN ONE DIMENSION PREVIEW Kinemaics is he sudy of how hings move how far (disance and displacemen), how fas (speed and velociy), and how fas ha how fas changes (acceleraion). We say ha an objec

More information

Chapter 3 Boundary Value Problem

Chapter 3 Boundary Value Problem Chaper 3 Boundary Value Problem A boundary value problem (BVP) is a problem, ypically an ODE or a PDE, which has values assigned on he physical boundary of he domain in which he problem is specified. Le

More information

Let us start with a two dimensional case. We consider a vector ( x,

Let us start with a two dimensional case. We consider a vector ( x, Roaion marices We consider now roaion marices in wo and hree dimensions. We sar wih wo dimensions since wo dimensions are easier han hree o undersand, and one dimension is a lile oo simple. However, our

More information

Ground Rules. PC1221 Fundamentals of Physics I. Kinematics. Position. Lectures 3 and 4 Motion in One Dimension. A/Prof Tay Seng Chuan

Ground Rules. PC1221 Fundamentals of Physics I. Kinematics. Position. Lectures 3 and 4 Motion in One Dimension. A/Prof Tay Seng Chuan Ground Rules PC11 Fundamenals of Physics I Lecures 3 and 4 Moion in One Dimension A/Prof Tay Seng Chuan 1 Swich off your handphone and pager Swich off your lapop compuer and keep i No alking while lecure

More information

Lecture 20: Riccati Equations and Least Squares Feedback Control

Lecture 20: Riccati Equations and Least Squares Feedback Control 34-5 LINEAR SYSTEMS Lecure : Riccai Equaions and Leas Squares Feedback Conrol 5.6.4 Sae Feedback via Riccai Equaions A recursive approach in generaing he marix-valued funcion W ( ) equaion for i for he

More information

Vehicle Arrival Models : Headway

Vehicle Arrival Models : Headway Chaper 12 Vehicle Arrival Models : Headway 12.1 Inroducion Modelling arrival of vehicle a secion of road is an imporan sep in raffic flow modelling. I has imporan applicaion in raffic flow simulaion where

More information

CHAPTER 12 DIRECT CURRENT CIRCUITS

CHAPTER 12 DIRECT CURRENT CIRCUITS CHAPTER 12 DIRECT CURRENT CIUITS DIRECT CURRENT CIUITS 257 12.1 RESISTORS IN SERIES AND IN PARALLEL When wo resisors are conneced ogeher as shown in Figure 12.1 we said ha hey are conneced in series. As

More information

Learning a Class from Examples. Training set X. Class C 1. Class C of a family car. Output: Input representation: x 1 : price, x 2 : engine power

Learning a Class from Examples. Training set X. Class C 1. Class C of a family car. Output: Input representation: x 1 : price, x 2 : engine power Alpaydin Chaper, Michell Chaper 7 Alpaydin slides are in urquoise. Ehem Alpaydin, copyrigh: The MIT Press, 010. alpaydin@boun.edu.r hp://www.cmpe.boun.edu.r/ ehem/imle All oher slides are based on Michell.

More information

Article from. Predictive Analytics and Futurism. July 2016 Issue 13

Article from. Predictive Analytics and Futurism. July 2016 Issue 13 Aricle from Predicive Analyics and Fuurism July 6 Issue An Inroducion o Incremenal Learning By Qiang Wu and Dave Snell Machine learning provides useful ools for predicive analyics The ypical machine learning

More information

Ensamble methods: Boosting

Ensamble methods: Boosting Lecure 21 Ensamble mehods: Boosing Milos Hauskrech milos@cs.pi.edu 5329 Senno Square Schedule Final exam: April 18: 1:00-2:15pm, in-class Term projecs April 23 & April 25: a 1:00-2:30pm in CS seminar room

More information

Neural Networks. Understanding the Brain

Neural Networks. Understanding the Brain Neural Neworks Threshold unis Neural Neworks Gradien descen Mulilayer neworks Backpropagaion Hidden layer represenaions Example: Face Recogniion Advanced opics And, more Neworks of processing unis (neurons)

More information

Ensamble methods: Bagging and Boosting

Ensamble methods: Bagging and Boosting Lecure 21 Ensamble mehods: Bagging and Boosing Milos Hauskrech milos@cs.pi.edu 5329 Senno Square Ensemble mehods Mixure of expers Muliple base models (classifiers, regressors), each covers a differen par

More information

PENALIZED LEAST SQUARES AND PENALIZED LIKELIHOOD

PENALIZED LEAST SQUARES AND PENALIZED LIKELIHOOD PENALIZED LEAST SQUARES AND PENALIZED LIKELIHOOD HAN XIAO 1. Penalized Leas Squares Lasso solves he following opimizaion problem, ˆβ lasso = arg max β R p+1 1 N y i β 0 N x ij β j β j (1.1) for some 0.

More information

SOLUTIONS TO ECE 3084

SOLUTIONS TO ECE 3084 SOLUTIONS TO ECE 384 PROBLEM 2.. For each sysem below, specify wheher or no i is: (i) memoryless; (ii) causal; (iii) inverible; (iv) linear; (v) ime invarian; Explain your reasoning. If he propery is no

More information

Learning a Class from Examples. Training set X. Class C 1. Class C of a family car. Output: Input representation: x 1 : price, x 2 : engine power

Learning a Class from Examples. Training set X. Class C 1. Class C of a family car. Output: Input representation: x 1 : price, x 2 : engine power Alpaydin Chaper, Michell Chaper 7 Alpaydin slides are in urquoise. Ehem Alpaydin, copyrigh: The MIT Press, 010. alpaydin@boun.edu.r hp://www.cmpe.boun.edu.r/ ehem/imle All oher slides are based on Michell.

More information

3.1.3 INTRODUCTION TO DYNAMIC OPTIMIZATION: DISCRETE TIME PROBLEMS. A. The Hamiltonian and First-Order Conditions in a Finite Time Horizon

3.1.3 INTRODUCTION TO DYNAMIC OPTIMIZATION: DISCRETE TIME PROBLEMS. A. The Hamiltonian and First-Order Conditions in a Finite Time Horizon 3..3 INRODUCION O DYNAMIC OPIMIZAION: DISCREE IME PROBLEMS A. he Hamilonian and Firs-Order Condiions in a Finie ime Horizon Define a new funcion, he Hamilonian funcion, H. H he change in he oal value of

More information

EECE 301 Signals & Systems Prof. Mark Fowler

EECE 301 Signals & Systems Prof. Mark Fowler EECE 31 Signals & Sysems Prof. Mark Fowler Noe Se #1 C-T Sysems: Convoluion Represenaion Reading Assignmen: Secion 2.6 of Kamen and Heck 1/11 Course Flow Diagram The arrows here show concepual flow beween

More information

GMM - Generalized Method of Moments

GMM - Generalized Method of Moments GMM - Generalized Mehod of Momens Conens GMM esimaion, shor inroducion 2 GMM inuiion: Maching momens 2 3 General overview of GMM esimaion. 3 3. Weighing marix...........................................

More information

Matlab and Python programming: how to get started

Matlab and Python programming: how to get started Malab and Pyhon programming: how o ge sared Equipping readers he skills o wrie programs o explore complex sysems and discover ineresing paerns from big daa is one of he main goals of his book. In his chaper,

More information

Final Spring 2007

Final Spring 2007 .615 Final Spring 7 Overview The purpose of he final exam is o calculae he MHD β limi in a high-bea oroidal okamak agains he dangerous n = 1 exernal ballooning-kink mode. Effecively, his corresponds o

More information

6.003 Homework #9 Solutions

6.003 Homework #9 Solutions 6.00 Homework #9 Soluions Problems. Fourier varieies a. Deermine he Fourier series coefficiens of he following signal, which is periodic in 0. x () 0 0 a 0 5 a k sin πk 5 sin πk 5 πk for k 0 a k 0 πk j

More information

Then. 1 The eigenvalues of A are inside R = n i=1 R i. 2 Union of any k circles not intersecting the other (n k)

Then. 1 The eigenvalues of A are inside R = n i=1 R i. 2 Union of any k circles not intersecting the other (n k) Ger sgorin Circle Chaper 9 Approimaing Eigenvalues Per-Olof Persson persson@berkeley.edu Deparmen of Mahemaics Universiy of California, Berkeley Mah 128B Numerical Analysis (Ger sgorin Circle) Le A be

More information

Some Basic Information about M-S-D Systems

Some Basic Information about M-S-D Systems Some Basic Informaion abou M-S-D Sysems 1 Inroducion We wan o give some summary of he facs concerning unforced (homogeneous) and forced (non-homogeneous) models for linear oscillaors governed by second-order,

More information

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle Chaper 2 Newonian Mechanics Single Paricle In his Chaper we will review wha Newon s laws of mechanics ell us abou he moion of a single paricle. Newon s laws are only valid in suiable reference frames,

More information

Simulation-Solving Dynamic Models ABE 5646 Week 2, Spring 2010

Simulation-Solving Dynamic Models ABE 5646 Week 2, Spring 2010 Simulaion-Solving Dynamic Models ABE 5646 Week 2, Spring 2010 Week Descripion Reading Maerial 2 Compuer Simulaion of Dynamic Models Finie Difference, coninuous saes, discree ime Simple Mehods Euler Trapezoid

More information

L07. KALMAN FILTERING FOR NON-LINEAR SYSTEMS. NA568 Mobile Robotics: Methods & Algorithms

L07. KALMAN FILTERING FOR NON-LINEAR SYSTEMS. NA568 Mobile Robotics: Methods & Algorithms L07. KALMAN FILTERING FOR NON-LINEAR SYSTEMS NA568 Mobile Roboics: Mehods & Algorihms Today s Topic Quick review on (Linear) Kalman Filer Kalman Filering for Non-Linear Sysems Exended Kalman Filer (EKF)

More information

Notes on online convex optimization

Notes on online convex optimization Noes on online convex opimizaion Karl Sraos Online convex opimizaion (OCO) is a principled framework for online learning: OnlineConvexOpimizaion Inpu: convex se S, number of seps T For =, 2,..., T : Selec

More information

Hamilton- J acobi Equation: Explicit Formulas In this lecture we try to apply the method of characteristics to the Hamilton-Jacobi equation: u t

Hamilton- J acobi Equation: Explicit Formulas In this lecture we try to apply the method of characteristics to the Hamilton-Jacobi equation: u t M ah 5 2 7 Fall 2 0 0 9 L ecure 1 0 O c. 7, 2 0 0 9 Hamilon- J acobi Equaion: Explici Formulas In his lecure we ry o apply he mehod of characerisics o he Hamilon-Jacobi equaion: u + H D u, x = 0 in R n

More information

6.003 Homework #9 Solutions

6.003 Homework #9 Solutions 6.003 Homework #9 Soluions Problems. Fourier varieies a. Deermine he Fourier series coefficiens of he following signal, which is periodic in 0. x () 0 3 0 a 0 5 a k a k 0 πk j3 e 0 e j πk 0 jπk πk e 0

More information

A Dynamic Model of Economic Fluctuations

A Dynamic Model of Economic Fluctuations CHAPTER 15 A Dynamic Model of Economic Flucuaions Modified for ECON 2204 by Bob Murphy 2016 Worh Publishers, all righs reserved IN THIS CHAPTER, OU WILL LEARN: how o incorporae dynamics ino he AD-AS model

More information

Lie Derivatives operator vector field flow push back Lie derivative of

Lie Derivatives operator vector field flow push back Lie derivative of Lie Derivaives The Lie derivaive is a mehod of compuing he direcional derivaive of a vecor field wih respec o anoher vecor field We already know how o make sense of a direcional derivaive of real valued

More information

Echocardiography Project and Finite Fourier Series

Echocardiography Project and Finite Fourier Series Echocardiography Projec and Finie Fourier Series 1 U M An echocardiagram is a plo of how a porion of he hear moves as he funcion of ime over he one or more hearbea cycles If he hearbea repeas iself every

More information

Online Convex Optimization Example And Follow-The-Leader

Online Convex Optimization Example And Follow-The-Leader CSE599s, Spring 2014, Online Learning Lecure 2-04/03/2014 Online Convex Opimizaion Example And Follow-The-Leader Lecurer: Brendan McMahan Scribe: Sephen Joe Jonany 1 Review of Online Convex Opimizaion

More information

Traveling Waves. Chapter Introduction

Traveling Waves. Chapter Introduction Chaper 4 Traveling Waves 4.1 Inroducion To dae, we have considered oscillaions, i.e., periodic, ofen harmonic, variaions of a physical characerisic of a sysem. The sysem a one ime is indisinguishable from

More information

EE363 homework 1 solutions

EE363 homework 1 solutions EE363 Prof. S. Boyd EE363 homework 1 soluions 1. LQR for a riple accumulaor. We consider he sysem x +1 = Ax + Bu, y = Cx, wih 1 1 A = 1 1, B =, C = [ 1 ]. 1 1 This sysem has ransfer funcion H(z) = (z 1)

More information

Chapter 2. First Order Scalar Equations

Chapter 2. First Order Scalar Equations Chaper. Firs Order Scalar Equaions We sar our sudy of differenial equaions in he same way he pioneers in his field did. We show paricular echniques o solve paricular ypes of firs order differenial equaions.

More information

Math 10B: Mock Mid II. April 13, 2016

Math 10B: Mock Mid II. April 13, 2016 Name: Soluions Mah 10B: Mock Mid II April 13, 016 1. ( poins) Sae, wih jusificaion, wheher he following saemens are rue or false. (a) If a 3 3 marix A saisfies A 3 A = 0, hen i canno be inverible. True.

More information

CSE/NB 528 Lecture 14: From Supervised to Reinforcement Learning (Chapter 9) R. Rao, 528: Lecture 14

CSE/NB 528 Lecture 14: From Supervised to Reinforcement Learning (Chapter 9) R. Rao, 528: Lecture 14 CSE/NB 58 Lecure 14: From Supervised o Reinforcemen Learning Chaper 9 1 Recall from las ime: Sigmoid Neworks Oupu v T g w u g wiui w Inpu nodes u = u 1 u u 3 T i Sigmoid oupu funcion: 1 g a 1 a e 1 ga

More information

CHAPTER 2 Signals And Spectra

CHAPTER 2 Signals And Spectra CHAPER Signals And Specra Properies of Signals and Noise In communicaion sysems he received waveform is usually caegorized ino he desired par conaining he informaion, and he undesired par. he desired par

More information

A Primal-Dual Type Algorithm with the O(1/t) Convergence Rate for Large Scale Constrained Convex Programs

A Primal-Dual Type Algorithm with the O(1/t) Convergence Rate for Large Scale Constrained Convex Programs PROC. IEEE CONFERENCE ON DECISION AND CONTROL, 06 A Primal-Dual Type Algorihm wih he O(/) Convergence Rae for Large Scale Consrained Convex Programs Hao Yu and Michael J. Neely Absrac This paper considers

More information

Finish reading Chapter 2 of Spivak, rereading earlier sections as necessary. handout and fill in some missing details!

Finish reading Chapter 2 of Spivak, rereading earlier sections as necessary. handout and fill in some missing details! MAT 257, Handou 6: Ocober 7-2, 20. I. Assignmen. Finish reading Chaper 2 of Spiva, rereading earlier secions as necessary. handou and fill in some missing deails! II. Higher derivaives. Also, read his

More information

10. State Space Methods

10. State Space Methods . Sae Space Mehods. Inroducion Sae space modelling was briefly inroduced in chaper. Here more coverage is provided of sae space mehods before some of heir uses in conrol sysem design are covered in he

More information

6.003 Homework #8 Solutions

6.003 Homework #8 Solutions 6.003 Homework #8 Soluions Problems. Fourier Series Deermine he Fourier series coefficiens a k for x () shown below. x ()= x ( + 0) 0 a 0 = 0 a k = e /0 sin(/0) for k 0 a k = π x()e k d = 0 0 π e 0 k d

More information

Guest Lectures for Dr. MacFarlane s EE3350 Part Deux

Guest Lectures for Dr. MacFarlane s EE3350 Part Deux Gues Lecures for Dr. MacFarlane s EE3350 Par Deux Michael Plane Mon., 08-30-2010 Wrie name in corner. Poin ou his is a review, so I will go faser. Remind hem o go lisen o online lecure abou geing an A

More information

556: MATHEMATICAL STATISTICS I

556: MATHEMATICAL STATISTICS I 556: MATHEMATICAL STATISTICS I INEQUALITIES 5.1 Concenraion and Tail Probabiliy Inequaliies Lemma (CHEBYCHEV S LEMMA) c > 0, If X is a random variable, hen for non-negaive funcion h, and P X [h(x) c] E

More information

Deep Learning: Theory, Techniques & Applications - Recurrent Neural Networks -

Deep Learning: Theory, Techniques & Applications - Recurrent Neural Networks - Deep Learning: Theory, Techniques & Applicaions - Recurren Neural Neworks - Prof. Maeo Maeucci maeo.maeucci@polimi.i Deparmen of Elecronics, Informaion and Bioengineering Arificial Inelligence and Roboics

More information

THE 2-BODY PROBLEM. FIGURE 1. A pair of ellipses sharing a common focus. (c,b) c+a ROBERT J. VANDERBEI

THE 2-BODY PROBLEM. FIGURE 1. A pair of ellipses sharing a common focus. (c,b) c+a ROBERT J. VANDERBEI THE 2-BODY PROBLEM ROBERT J. VANDERBEI ABSTRACT. In his shor noe, we show ha a pair of ellipses wih a common focus is a soluion o he 2-body problem. INTRODUCTION. Solving he 2-body problem from scrach

More information

T L. t=1. Proof of Lemma 1. Using the marginal cost accounting in Equation(4) and standard arguments. t )+Π RB. t )+K 1(Q RB

T L. t=1. Proof of Lemma 1. Using the marginal cost accounting in Equation(4) and standard arguments. t )+Π RB. t )+K 1(Q RB Elecronic Companion EC.1. Proofs of Technical Lemmas and Theorems LEMMA 1. Le C(RB) be he oal cos incurred by he RB policy. Then we have, T L E[C(RB)] 3 E[Z RB ]. (EC.1) Proof of Lemma 1. Using he marginal

More information

Particle Swarm Optimization

Particle Swarm Optimization Paricle Swarm Opimizaion Speaker: Jeng-Shyang Pan Deparmen of Elecronic Engineering, Kaohsiung Universiy of Applied Science, Taiwan Email: jspan@cc.kuas.edu.w 7/26/2004 ppso 1 Wha is he Paricle Swarm Opimizaion

More information

!!"#"$%&#'()!"#&'(*%)+,&',-)./0)1-*23)

!!#$%&#'()!#&'(*%)+,&',-)./0)1-*23) "#"$%&#'()"#&'(*%)+,&',-)./)1-*) #$%&'()*+,&',-.%,/)*+,-&1*#$)()5*6$+$%*,7&*-'-&1*(,-&*6&,7.$%$+*&%'(*8$&',-,%'-&1*(,-&*6&,79*(&,%: ;..,*&1$&$.$%&'()*1$$.,'&',-9*(&,%)?%*,('&5

More information

Math 2142 Exam 1 Review Problems. x 2 + f (0) 3! for the 3rd Taylor polynomial at x = 0. To calculate the various quantities:

Math 2142 Exam 1 Review Problems. x 2 + f (0) 3! for the 3rd Taylor polynomial at x = 0. To calculate the various quantities: Mah 4 Eam Review Problems Problem. Calculae he 3rd Taylor polynomial for arcsin a =. Soluion. Le f() = arcsin. For his problem, we use he formula f() + f () + f ()! + f () 3! for he 3rd Taylor polynomial

More information

Inventory Analysis and Management. Multi-Period Stochastic Models: Optimality of (s, S) Policy for K-Convex Objective Functions

Inventory Analysis and Management. Multi-Period Stochastic Models: Optimality of (s, S) Policy for K-Convex Objective Functions Muli-Period Sochasic Models: Opimali of (s, S) Polic for -Convex Objecive Funcions Consider a seing similar o he N-sage newsvendor problem excep ha now here is a fixed re-ordering cos (> 0) for each (re-)order.

More information

IMPLICIT AND INVERSE FUNCTION THEOREMS PAUL SCHRIMPF 1 OCTOBER 25, 2013

IMPLICIT AND INVERSE FUNCTION THEOREMS PAUL SCHRIMPF 1 OCTOBER 25, 2013 IMPLICI AND INVERSE FUNCION HEOREMS PAUL SCHRIMPF 1 OCOBER 25, 213 UNIVERSIY OF BRIISH COLUMBIA ECONOMICS 526 We have exensively sudied how o solve sysems of linear equaions. We know how o check wheher

More information

Supplement for Stochastic Convex Optimization: Faster Local Growth Implies Faster Global Convergence

Supplement for Stochastic Convex Optimization: Faster Local Growth Implies Faster Global Convergence Supplemen for Sochasic Convex Opimizaion: Faser Local Growh Implies Faser Global Convergence Yi Xu Qihang Lin ianbao Yang Proof of heorem heorem Suppose Assumpion holds and F (w) obeys he LGC (6) Given

More information

Georey E. Hinton. University oftoronto. Technical Report CRG-TR February 22, Abstract

Georey E. Hinton. University oftoronto.   Technical Report CRG-TR February 22, Abstract Parameer Esimaion for Linear Dynamical Sysems Zoubin Ghahramani Georey E. Hinon Deparmen of Compuer Science Universiy oftorono 6 King's College Road Torono, Canada M5S A4 Email: zoubin@cs.orono.edu Technical

More information

Solutions from Chapter 9.1 and 9.2

Solutions from Chapter 9.1 and 9.2 Soluions from Chaper 9 and 92 Secion 9 Problem # This basically boils down o an exercise in he chain rule from calculus We are looking for soluions of he form: u( x) = f( k x c) where k x R 3 and k is

More information

Robust estimation based on the first- and third-moment restrictions of the power transformation model

Robust estimation based on the first- and third-moment restrictions of the power transformation model h Inernaional Congress on Modelling and Simulaion, Adelaide, Ausralia, 6 December 3 www.mssanz.org.au/modsim3 Robus esimaion based on he firs- and hird-momen resricions of he power ransformaion Nawaa,

More information

1 Solutions to selected problems

1 Solutions to selected problems 1 Soluions o seleced problems 1. Le A B R n. Show ha in A in B bu in general bd A bd B. Soluion. Le x in A. Then here is ɛ > 0 such ha B ɛ (x) A B. This shows x in B. If A = [0, 1] and B = [0, 2], hen

More information

Online Appendix to Solution Methods for Models with Rare Disasters

Online Appendix to Solution Methods for Models with Rare Disasters Online Appendix o Soluion Mehods for Models wih Rare Disasers Jesús Fernández-Villaverde and Oren Levinal In his Online Appendix, we presen he Euler condiions of he model, we develop he pricing Calvo block,

More information

Mathcad Lecture #8 In-class Worksheet Curve Fitting and Interpolation

Mathcad Lecture #8 In-class Worksheet Curve Fitting and Interpolation Mahcad Lecure #8 In-class Workshee Curve Fiing and Inerpolaion A he end of his lecure, you will be able o: explain he difference beween curve fiing and inerpolaion decide wheher curve fiing or inerpolaion

More information

EXERCISES FOR SECTION 1.5

EXERCISES FOR SECTION 1.5 1.5 Exisence and Uniqueness of Soluions 43 20. 1 v c 21. 1 v c 1 2 4 6 8 10 1 2 2 4 6 8 10 Graph of approximae soluion obained using Euler s mehod wih = 0.1. Graph of approximae soluion obained using Euler

More information

Class Meeting # 10: Introduction to the Wave Equation

Class Meeting # 10: Introduction to the Wave Equation MATH 8.5 COURSE NOTES - CLASS MEETING # 0 8.5 Inroducion o PDEs, Fall 0 Professor: Jared Speck Class Meeing # 0: Inroducion o he Wave Equaion. Wha is he wave equaion? The sandard wave equaion for a funcion

More information

Multi-scale 2D acoustic full waveform inversion with high frequency impulsive source

Multi-scale 2D acoustic full waveform inversion with high frequency impulsive source Muli-scale D acousic full waveform inversion wih high frequency impulsive source Vladimir N Zubov*, Universiy of Calgary, Calgary AB vzubov@ucalgaryca and Michael P Lamoureux, Universiy of Calgary, Calgary

More information

Econ107 Applied Econometrics Topic 7: Multicollinearity (Studenmund, Chapter 8)

Econ107 Applied Econometrics Topic 7: Multicollinearity (Studenmund, Chapter 8) I. Definiions and Problems A. Perfec Mulicollineariy Econ7 Applied Economerics Topic 7: Mulicollineariy (Sudenmund, Chaper 8) Definiion: Perfec mulicollineariy exiss in a following K-variable regression

More information

Appendix to Online l 1 -Dictionary Learning with Application to Novel Document Detection

Appendix to Online l 1 -Dictionary Learning with Application to Novel Document Detection Appendix o Online l -Dicionary Learning wih Applicaion o Novel Documen Deecion Shiva Prasad Kasiviswanahan Huahua Wang Arindam Banerjee Prem Melville A Background abou ADMM In his secion, we give a brief

More information

Concourse Math Spring 2012 Worked Examples: Matrix Methods for Solving Systems of 1st Order Linear Differential Equations

Concourse Math Spring 2012 Worked Examples: Matrix Methods for Solving Systems of 1st Order Linear Differential Equations Concourse Mah 80 Spring 0 Worked Examples: Marix Mehods for Solving Sysems of s Order Linear Differenial Equaions The Main Idea: Given a sysem of s order linear differenial equaions d x d Ax wih iniial

More information

Diebold, Chapter 7. Francis X. Diebold, Elements of Forecasting, 4th Edition (Mason, Ohio: Cengage Learning, 2006). Chapter 7. Characterizing Cycles

Diebold, Chapter 7. Francis X. Diebold, Elements of Forecasting, 4th Edition (Mason, Ohio: Cengage Learning, 2006). Chapter 7. Characterizing Cycles Diebold, Chaper 7 Francis X. Diebold, Elemens of Forecasing, 4h Ediion (Mason, Ohio: Cengage Learning, 006). Chaper 7. Characerizing Cycles Afer compleing his reading you should be able o: Define covariance

More information

Solutions Problem Set 3 Macro II (14.452)

Solutions Problem Set 3 Macro II (14.452) Soluions Problem Se 3 Macro II (14.452) Francisco A. Gallego 04/27/2005 1 Q heory of invesmen in coninuous ime and no uncerainy Consider he in nie horizon model of a rm facing adjusmen coss o invesmen.

More information

Lecture Notes 2. The Hilbert Space Approach to Time Series

Lecture Notes 2. The Hilbert Space Approach to Time Series Time Series Seven N. Durlauf Universiy of Wisconsin. Basic ideas Lecure Noes. The Hilber Space Approach o Time Series The Hilber space framework provides a very powerful language for discussing he relaionship

More information

HOMEWORK # 2: MATH 211, SPRING Note: This is the last solution set where I will describe the MATLAB I used to make my pictures.

HOMEWORK # 2: MATH 211, SPRING Note: This is the last solution set where I will describe the MATLAB I used to make my pictures. HOMEWORK # 2: MATH 2, SPRING 25 TJ HITCHMAN Noe: This is he las soluion se where I will describe he MATLAB I used o make my picures.. Exercises from he ex.. Chaper 2.. Problem 6. We are o show ha y() =

More information

5. Stochastic processes (1)

5. Stochastic processes (1) Lec05.pp S-38.45 - Inroducion o Teleraffic Theory Spring 2005 Conens Basic conceps Poisson process 2 Sochasic processes () Consider some quaniy in a eleraffic (or any) sysem I ypically evolves in ime randomly

More information

= ( ) ) or a system of differential equations with continuous parametrization (T = R

= ( ) ) or a system of differential equations with continuous parametrization (T = R XIII. DIFFERENCE AND DIFFERENTIAL EQUATIONS Ofen funcions, or a sysem of funcion, are paramerized in erms of some variable, usually denoed as and inerpreed as ime. The variable is wrien as a funcion of

More information

CE 395 Special Topics in Machine Learning

CE 395 Special Topics in Machine Learning CE 395 Special Topics in Machine Learning Assoc. Prof. Dr. Yuriy Mishchenko Fall 2017 DIGITAL FILTERS AND FILTERING Why filers? Digial filering is he workhorse of digial signal processing Filering is a

More information

( ) a system of differential equations with continuous parametrization ( T = R + These look like, respectively:

( ) a system of differential equations with continuous parametrization ( T = R + These look like, respectively: XIII. DIFFERENCE AND DIFFERENTIAL EQUATIONS Ofen funcions, or a sysem of funcion, are paramerized in erms of some variable, usually denoed as and inerpreed as ime. The variable is wrien as a funcion of

More information

PMR5406 Redes Neurais e Lógica Fuzzy Aula 3 Single Layer Percetron

PMR5406 Redes Neurais e Lógica Fuzzy Aula 3 Single Layer Percetron PMR5406 Redes Neurais e Aula 3 Single Layer Percetron Baseado em: Neural Networks, Simon Haykin, Prentice-Hall, 2 nd edition Slides do curso por Elena Marchiori, Vrije Unviersity Architecture We consider

More information

WEEK-3 Recitation PHYS 131. of the projectile s velocity remains constant throughout the motion, since the acceleration a x

WEEK-3 Recitation PHYS 131. of the projectile s velocity remains constant throughout the motion, since the acceleration a x WEEK-3 Reciaion PHYS 131 Ch. 3: FOC 1, 3, 4, 6, 14. Problems 9, 37, 41 & 71 and Ch. 4: FOC 1, 3, 5, 8. Problems 3, 5 & 16. Feb 8, 018 Ch. 3: FOC 1, 3, 4, 6, 14. 1. (a) The horizonal componen of he projecile

More information

Physics 180A Fall 2008 Test points. Provide the best answer to the following questions and problems. Watch your sig figs.

Physics 180A Fall 2008 Test points. Provide the best answer to the following questions and problems. Watch your sig figs. Physics 180A Fall 2008 Tes 1-120 poins Name Provide he bes answer o he following quesions and problems. Wach your sig figs. 1) The number of meaningful digis in a number is called he number of. When numbers

More information

Explaining Total Factor Productivity. Ulrich Kohli University of Geneva December 2015

Explaining Total Factor Productivity. Ulrich Kohli University of Geneva December 2015 Explaining Toal Facor Produciviy Ulrich Kohli Universiy of Geneva December 2015 Needed: A Theory of Toal Facor Produciviy Edward C. Presco (1998) 2 1. Inroducion Toal Facor Produciviy (TFP) has become

More information

IB Physics Kinematics Worksheet

IB Physics Kinematics Worksheet IB Physics Kinemaics Workshee Wrie full soluions and noes for muliple choice answers. Do no use a calculaor for muliple choice answers. 1. Which of he following is a correc definiion of average acceleraion?

More information

Announcements: Warm-up Exercise:

Announcements: Warm-up Exercise: Fri Apr 13 7.1 Sysems of differenial equaions - o model muli-componen sysems via comparmenal analysis hp//en.wikipedia.org/wiki/muli-comparmen_model Announcemens Warm-up Exercise Here's a relaively simple

More information

EE 315 Notes. Gürdal Arslan CLASS 1. (Sections ) What is a signal?

EE 315 Notes. Gürdal Arslan CLASS 1. (Sections ) What is a signal? EE 35 Noes Gürdal Arslan CLASS (Secions.-.2) Wha is a signal? In his class, a signal is some funcion of ime and i represens how some physical quaniy changes over some window of ime. Examples: velociy of

More information