1.1. Example: Polynomial Curve Fitting 4 1. INTRODUCTION

Size: px
Start display at page:

Download "1.1. Example: Polynomial Curve Fitting 4 1. INTRODUCTION"

Transcription

1 4. INTRODUCTION Figure.2 Plo of a raining daa se of N = poins, shown as blue circles, each comprising an observaion of he inpu variable along wih he corresponding arge variable. The green curve shows he funcion sin(2π) used o generae he daa. Our goal is o predic he value of for some new value of, wihou knowledge of he green curve. deailed reamen lies beyond he scope of his book. Alhough each of hese asks needs is own ools and echniques, many of he key ideas ha underpin hem are common o all such problems. One of he main goals of his chaper is o inroduce, in a relaively informal way, several of he mos imporan of hese conceps and o illusrae hem using simple eamples. Laer in he book we shall see hese same ideas re-emerge in he cone of more sophisicaed models ha are applicable o real-world paern recogniion applicaions. This chaper also provides a self-conained inroducion o hree imporan ools ha will be used hroughou he book, namely probabiliy heory, decision heory, and informaion heory. Alhough hese migh sound like dauning opics, hey are in fac sraighforward, and a clear undersanding of hem is essenial if machine learning echniques are o be used o bes effec in pracical applicaions... Eample: Polynomial Curve Fiing We begin by inroducing a simple regression problem, which we shall use as a running eample hroughou his chaper o moivae a number of key conceps. Suppose we observe a real-valued inpu variable and we wish o use his observaion o predic he value of a real-valued arge variable. For he presen purposes, i is insrucive o consider an arificial eample using synheically generaed daa because we hen know he precise process ha generaed he daa for comparison agains any learned model. The daa for his eample is generaed from he funcion sin(2π) wih random noise included in he arge values, as described in deail in Appendi A. Now suppose ha we are given a raining se comprising N observaions of, wrien (,..., N ) T, ogeher wih corresponding observaions of he values of, denoed (,..., N ) T. Figure.2 shows a plo of a raining se comprising N = daa poins. The inpu daa se in Figure.2 was generaed by choosing values of n, for n =,...,N, spaced uniformly in range [, ], and he arge daa se was obained by firs compuing he corresponding values of he funcion

2 .. Eample: Polynomial Curve Fiing 5 sin(2π) and hen adding a small level of random noise having a Gaussian disribuion (he Gaussian disribuion is discussed in Secion.2.4) o each such poin in order o obain he corresponding value n. By generaing daa in his way, we are capuring a propery of many real daa ses, namely ha hey possess an underlying regulariy, which we wish o learn, bu ha individual observaions are corruped by random noise. This noise migh arise from inrinsically sochasic (i.e. random) processes such as radioacive decay bu more ypically is due o here being sources of variabiliy ha are hemselves unobserved. Our goal is o eploi his raining se in order o make predicions of he value of he arge variable for some new value of he inpu variable. As we shall see laer, his involves implicily rying o discover he underlying funcion sin(2π). This is inrinsically a difficul problem as we have o generalize from a finie daa se. Furhermore he observed daa are corruped wih noise, and so for a given here is uncerainy as o he appropriae value for. Probabiliy heory, discussed in Secion.2, provides a framework for epressing such uncerainy in a precise and quaniaive manner, and decision heory, discussed in Secion.5, allows us o eploi his probabilisic represenaion in order o make predicions ha are opimal according o appropriae crieria. For he momen, however, we shall proceed raher informally and consider a simple approach based on curve fiing. In paricular, we shall fi he daa using a polynomial funcion of he form y(, w) =w + w + w w M M = M w j j (.) where M is he order of he polynomial, and j denoes raised o he power of j. The polynomial coefficiens w,...,w M are collecively denoed by he vecor w. Noe ha, alhough he polynomial funcion y(, w) is a nonlinear funcion of, i is a linear funcion of he coefficiens w. Funcions, such as he polynomial, which are linear in he unknown parameers have imporan properies and are called linear models and will be discussed eensively in Chapers 3 and 4. The values of he coefficiens will be deermined by fiing he polynomial o he raining daa. This can be done by minimizing an error funcion ha measures he misfi beween he funcion y(, w), for any given value of w, and he raining se daa poins. One simple choice of error funcion, which is widely used, is given by he sum of he squares of he errors beween he predicions y( n, w) for each daa poin n and he corresponding arge values n, so ha we minimize E(w) = 2 j= N {y( n, w) n } 2 (.2) n= where he facor of /2 is included for laer convenience. We shall discuss he moivaion for his choice of error funcion laer in his chaper. For he momen we simply noe ha i is a nonnegaive quaniy ha would be zero if, and only if, he

3 6. INTRODUCTION Figure.3 The error funcion (.2) corresponds o (one half of) he sum of he squares of he displacemens (shown by he verical green bars) of each daa poin from he funcion y(, w). n y( n, w) n funcion y(, w) were o pass eacly hrough each raining daa poin. The geomerical inerpreaion of he sum-of-squares error funcion is illusraed in Figure.3. Eercise. We can solve he curve fiing problem by choosing he value of w for which E(w) is as small as possible. Because he error funcion is a quadraic funcion of he coefficiens w, is derivaives wih respec o he coefficiens will be linear in he elemens of w, and so he minimizaion of he error funcion has a unique soluion, denoed by w, which can be found in closed form. The resuling polynomial is given by he funcion y(, w ). There remains he problem of choosing he order M of he polynomial, and as we shall see his will urn ou o be an eample of an imporan concep called model comparison or model selecion. In Figure.4, we show four eamples of he resuls of fiing polynomials having orders M =,, 3, and9 o he daa se shown in Figure.2. We noice ha he consan (M = ) and firs order (M = ) polynomials give raher poor fis o he daa and consequenly raher poor represenaions of he funcion sin(2π). The hird order (M =3) polynomial seems o give he bes fi o he funcion sin(2π) of he eamples shown in Figure.4. When we go o a much higher order polynomial (M =9), we obain an ecellen fi o he raining daa. In fac, he polynomial passes eacly hrough each daa poin and E(w )=. However, he fied curve oscillaes wildly and gives a very poor represenaion of he funcion sin(2π). This laer behaviour is known as over-fiing. As we have noed earlier, he goal is o achieve good generalizaion by making accurae predicions for new daa. We can obain some quaniaive insigh ino he dependence of he generalizaion performance on M by considering a separae es se comprising daa poins generaed using eacly he same procedure used o generae he raining se poins bu wih new choices for he random noise values included in he arge values. For each choice of M, we can hen evaluae he residual value of E(w ) given by (.2) for he raining daa, and we can also evaluae E(w ) for he es daa se. I is someimes more convenien o use he roo-mean-square

4 .. Eample: Polynomial Curve Fiing 7 M = M = M =3 M =9 Figure.4 Figure.2. Plos of polynomials having various orders M, shown as red curves, fied o he daa se shown in (RMS) error defined by E RMS = 2E(w )/N (.3) in which he division by N allows us o compare differen sizes of daa ses on an equal fooing, and he square roo ensures ha E RMS is measured on he same scale (and in he same unis) as he arge variable. Graphs of he raining and es se RMS errors are shown, for various values of M, in Figure.5. The es se error is a measure of how well we are doing in predicing he values of for new daa observaions of. We noe from Figure.5 ha small values of M give relaively large values of he es se error, and his can be aribued o he fac ha he corresponding polynomials are raher infleible and are incapable of capuring he oscillaions in he funcion sin(2π). Values of M in he range 3 M 8 give small values for he es se error, and hese also give reasonable represenaions of he generaing funcion sin(2π), as can be seen, for he case of M =3, from Figure.4.

5 8. INTRODUCTION Figure.5 Graphs of he roo-mean-square error, defined by (.3), evaluaed on he raining se and on an independen es se for various values of M. Training Tes ERMS.5 3 M 6 9 For M =9, he raining se error goes o zero, as we migh epec because his polynomial conains degrees of freedom corresponding o he coefficiens w,...,w 9, and so can be uned eacly o he daa poins in he raining se. However, he es se error has become very large and, as we saw in Figure.4, he corresponding funcion y(, w ) ehibis wild oscillaions. This may seem paradoical because a polynomial of given order conains all lower order polynomials as special cases. The M =9polynomial is herefore capable of generaing resuls a leas as good as he M =3polynomial. Furhermore, we migh suppose ha he bes predicor of new daa would be he funcion sin(2π) from which he daa was generaed (and we shall see laer ha his is indeed he case). We know ha a power series epansion of he funcion sin(2π) conains erms of all orders, so we migh epec ha resuls should improve monoonically as we increase M. We can gain some insigh ino he problem by eamining he values of he coefficiens w obained from polynomials of various order, as shown in Table.. We see ha, as M increases, he magniude of he coefficiens ypically ges larger. In paricular for he M =9polynomial, he coefficiens have become finely uned o he daa by developing large posiive and negaive values so ha he correspond- Table. Table of he coefficiens w for polynomials of various order. Observe how he ypical magniude of he coefficiens increases dramaically as he order of he polynomial increases. M = M = M =6 M =9 w w w w w w w w w w

6 .. Eample: Polynomial Curve Fiing 9 N = 5 N = Figure.6 Plos of he soluions obained by minimizing he sum-of-squares error funcion using he M =9 polynomial for N =5daa poins (lef plo) and N = daa poins (righ plo). We see ha increasing he size of he daa se reduces he over-fiing problem. Secion 3.4 ing polynomial funcion maches each of he daa poins eacly, bu beween daa poins (paricularly near he ends of he range) he funcion ehibis he large oscillaions observed in Figure.4. Inuiively, wha is happening is ha he more fleible polynomials wih larger values of M are becoming increasingly uned o he random noise on he arge values. I is also ineresing o eamine he behaviour of a given model as he size of he daa se is varied, as shown in Figure.6. We see ha, for a given model compleiy, he over-fiing problem become less severe as he size of he daa se increases. Anoher way o say his is ha he larger he daa se, he more comple (in oher words more fleible) he model ha we can afford o fi o he daa. One rough heurisic ha is someimes advocaed is ha he number of daa poins should be no less han some muliple (say 5 or ) of he number of adapive parameers in he model. However, as we shall see in Chaper 3, he number of parameers is no necessarily he mos appropriae measure of model compleiy. Also, here is somehing raher unsaisfying abou having o limi he number of parameers in a model according o he size of he available raining se. I would seem more reasonable o choose he compleiy of he model according o he compleiy of he problem being solved. We shall see ha he leas squares approach o finding he model parameers represens a specific case of maimum likelihood (discussed in Secion.2.5), and ha he over-fiing problem can be undersood as a general propery of maimum likelihood. By adoping a Bayesian approach, he over-fiing problem can be avoided. We shall see ha here is no difficuly from a Bayesian perspecive in employing models for which he number of parameers grealy eceeds he number of daa poins. Indeed, in a Bayesian model he effecive number of parameers adaps auomaically o he size of he daa se. For he momen, however, i is insrucive o coninue wih he curren approach and o consider how in pracice we can apply i o daa ses of limied size where we

7 . INTRODUCTION ln λ = 8 ln λ = Figure.7 Plos of M =9polynomials fied o he daa se shown in Figure.2 using he regularized error funcion (.4) for wo values of he regularizaion parameer λ corresponding o ln λ = 8 and ln λ =. The case of no regularizer, i.e., λ =, corresponding o ln λ =, is shown a he boom righ of Figure.4. Eercise.2 may wish o use relaively comple and fleible models. One echnique ha is ofen used o conrol he over-fiing phenomenon in such cases is ha of regularizaion, which involves adding a penaly erm o he error funcion (.2) in order o discourage he coefficiens from reaching large values. The simples such penaly erm akes he form of a sum of squares of all of he coefficiens, leading o a modified error funcion of he form Ẽ(w) = N {y( n, w) n } 2 + λ 2 2 w 2 (.4) n= where w 2 w T w = w 2 + w wm 2, and he coefficien λ governs he relaive imporance of he regularizaion erm compared wih he sum-of-squares error erm. Noe ha ofen he coefficien w is omied from he regularizer because is inclusion causes he resuls o depend on he choice of origin for he arge variable (Hasie e al., 2), or i may be included bu wih is own regularizaion coefficien (we shall discuss his opic in more deail in Secion 5.5.). Again, he error funcion in (.4) can be minimized eacly in closed form. Techniques such as his are known in he saisics lieraure as shrinkage mehods because hey reduce he value of he coefficiens. The paricular case of a quadraic regularizer is called ridge regression (Hoerl and Kennard, 97). In he cone of neural neworks, his approach is known as weigh decay. Figure.7 shows he resuls of fiing he polynomial of order M =9o he same daa se as before bu now using he regularized error funcion given by (.4). We see ha, for a value of ln λ = 8, he over-fiing has been suppressed and we now obain a much closer represenaion of he underlying funcion sin(2π). If, however, we use oo large a value for λ hen we again obain a poor fi, as shown in Figure.7 for ln λ =. The corresponding coefficiens from he fied polynomials are given in Table.2, showing ha regularizaion has he desired effec of reducing

8 .. Eample: Polynomial Curve Fiing Table.2 Table of he coefficiens w for M = 9 polynomials wih various values for he regularizaion parameer λ. Noe ha ln λ = corresponds o a model wih no regularizaion, i.e., o he graph a he boom righ in Figure.4. We see ha, as he value of λ increases, he ypical magniude of he coefficiens ges smaller. ln λ = ln λ = 8 ln λ = w w w w w w w w w w Secion.3 he magniude of he coefficiens. The impac of he regularizaion erm on he generalizaion error can be seen by ploing he value of he RMS error (.3) for boh raining and es ses agains ln λ, as shown in Figure.8. We see ha in effec λ now conrols he effecive compleiy of he model and hence deermines he degree of over-fiing. The issue of model compleiy is an imporan one and will be discussed a lengh in Secion.3. Here we simply noe ha, if we were rying o solve a pracical applicaion using his approach of minimizing an error funcion, we would have o find a way o deermine a suiable value for he model compleiy. The resuls above sugges a simple way of achieving his, namely by aking he available daa and pariioning i ino a raining se, used o deermine he coefficiens w, and a separae validaion se, also called a hold-ou se, used o opimize he model compleiy (eiher M or λ). In many cases, however, his will prove o be oo waseful of valuable raining daa, and we have o seek more sophisicaed approaches. So far our discussion of polynomial curve fiing has appealed largely o inuiion. We now seek a more principled approach o solving problems in paern recogniion by urning o a discussion of probabiliy heory. As well as providing he foundaion for nearly all of he subsequen developmens in his book, i will also Figure.8 Graph of he roo-mean-square error (.3) versus ln λ for he M =9 polynomial. Training Tes ERMS ln λ 25 2

9 2. INTRODUCTION give us some imporan insighs ino he conceps we have inroduced in he cone of polynomial curve fiing and will allow us o eend hese o more comple siuaions..2. Probabiliy Theory A key concep in he field of paern recogniion is ha of uncerainy. I arises boh hrough noise on measuremens, as well as hrough he finie size of daa ses. Probabiliy heory provides a consisen framework for he quanificaion and manipulaion of uncerainy and forms one of he cenral foundaions for paern recogniion. When combined wih decision heory, discussed in Secion.5, i allows us o make opimal predicions given all he informaion available o us, even hough ha informaion may be incomplee or ambiguous. We will inroduce he basic conceps of probabiliy heory by considering a simple eample. Imagine we have wo boes, one red and one blue, and in he red bo we have 2 apples and 6 oranges, and in he blue bo we have 3 apples and orange. This is illusraed in Figure.9. Now suppose we randomly pick one of he boes and from ha bo we randomly selec an iem of frui, and having observed which sor of frui i is we replace i in he bo from which i came. We could imagine repeaing his process many imes. Le us suppose ha in so doing we pick he red bo 4% of he ime and we pick he blue bo 6% of he ime, and ha when we remove an iem of frui from a bo we are equally likely o selec any of he pieces of frui in he bo. In his eample, he ideniy of he bo ha will be chosen is a random variable, which we shall denoe by B. This random variable can ake one of wo possible values, namely r (corresponding o he red bo) or b (corresponding o he blue bo). Similarly, he ideniy of he frui is also a random variable and will be denoed by F. I can ake eiher of he values a (for apple) or o (for orange). To begin wih, we shall define he probabiliy of an even o be he fracion of imes ha even occurs ou of he oal number of rials, in he limi ha he oal number of rials goes o infiniy. Thus he probabiliy of selecing he red bo is 4/ Figure.9 We use a simple eample of wo coloured boes each conaining frui (apples shown in green and oranges shown in orange) o inroduce he basic ideas of probabiliy.

2 1. INTRODUCTION. Figure 1.1. Examples of hand-written digits taken from US zip codes.

2 1. INTRODUCTION. Figure 1.1. Examples of hand-written digits taken from US zip codes. Inroducion The problem of searching for paerns in daa is a fundamenal one and has a long and successful hisory. For insance, he eensive asronomical observaions of Tycho Brahe in he 6 h cenury allowed Johannes

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

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

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

ACE 562 Fall Lecture 5: The Simple Linear Regression Model: Sampling Properties of the Least Squares Estimators. by Professor Scott H.

ACE 562 Fall Lecture 5: The Simple Linear Regression Model: Sampling Properties of the Least Squares Estimators. by Professor Scott H. ACE 56 Fall 005 Lecure 5: he Simple Linear Regression Model: Sampling Properies of he Leas Squares Esimaors by Professor Sco H. Irwin Required Reading: Griffihs, Hill and Judge. "Inference in he Simple

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

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

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

Lecture 33: November 29

Lecture 33: November 29 36-705: Inermediae Saisics Fall 2017 Lecurer: Siva Balakrishnan Lecure 33: November 29 Today we will coninue discussing he boosrap, and hen ry o undersand why i works in a simple case. In he las lecure

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

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

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

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

Chapter 4. Truncation Errors

Chapter 4. Truncation Errors Chaper 4. Truncaion Errors and he Taylor Series Truncaion Errors and he Taylor Series Non-elemenary funcions such as rigonomeric, eponenial, and ohers are epressed in an approimae fashion using Taylor

More information

STATE-SPACE MODELLING. A mass balance across the tank gives:

STATE-SPACE MODELLING. A mass balance across the tank gives: B. Lennox and N.F. Thornhill, 9, Sae Space Modelling, IChemE Process Managemen and Conrol Subjec Group Newsleer STE-SPACE MODELLING Inroducion: Over he pas decade or so here has been an ever increasing

More information

On Measuring Pro-Poor Growth. 1. On Various Ways of Measuring Pro-Poor Growth: A Short Review of the Literature

On Measuring Pro-Poor Growth. 1. On Various Ways of Measuring Pro-Poor Growth: A Short Review of the Literature On Measuring Pro-Poor Growh 1. On Various Ways of Measuring Pro-Poor Growh: A Shor eview of he Lieraure During he pas en years or so here have been various suggesions concerning he way one should check

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

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

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

Zürich. ETH Master Course: L Autonomous Mobile Robots Localization II

Zürich. ETH Master Course: L Autonomous Mobile Robots Localization II Roland Siegwar Margaria Chli Paul Furgale Marco Huer Marin Rufli Davide Scaramuzza ETH Maser Course: 151-0854-00L Auonomous Mobile Robos Localizaion II ACT and SEE For all do, (predicion updae / ACT),

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

d 1 = c 1 b 2 - b 1 c 2 d 2 = c 1 b 3 - b 1 c 3

d 1 = c 1 b 2 - b 1 c 2 d 2 = c 1 b 3 - b 1 c 3 and d = c b - b c c d = c b - b c c This process is coninued unil he nh row has been compleed. The complee array of coefficiens is riangular. Noe ha in developing he array an enire row may be divided or

More information

ES.1803 Topic 22 Notes Jeremy Orloff

ES.1803 Topic 22 Notes Jeremy Orloff ES.83 Topic Noes Jeremy Orloff Fourier series inroducion: coninued. Goals. Be able o compue he Fourier coefficiens of even or odd periodic funcion using he simplified formulas.. Be able o wrie and graph

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

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

4.1 Other Interpretations of Ridge Regression

4.1 Other Interpretations of Ridge Regression CHAPTER 4 FURTHER RIDGE THEORY 4. Oher Inerpreaions of Ridge Regression In his secion we will presen hree inerpreaions for he use of ridge regression. The firs one is analogous o Hoerl and Kennard reasoning

More information

This document was generated at 1:04 PM, 09/10/13 Copyright 2013 Richard T. Woodward. 4. End points and transversality conditions AGEC

This document was generated at 1:04 PM, 09/10/13 Copyright 2013 Richard T. Woodward. 4. End points and transversality conditions AGEC his documen was generaed a 1:4 PM, 9/1/13 Copyrigh 213 Richard. Woodward 4. End poins and ransversaliy condiions AGEC 637-213 F z d Recall from Lecure 3 ha a ypical opimal conrol problem is o maimize (,,

More information

23.5. Half-Range Series. Introduction. Prerequisites. Learning Outcomes

23.5. Half-Range Series. Introduction. Prerequisites. Learning Outcomes Half-Range Series 2.5 Inroducion In his Secion we address he following problem: Can we find a Fourier series expansion of a funcion defined over a finie inerval? Of course we recognise ha such a funcion

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

Week 1 Lecture 2 Problems 2, 5. What if something oscillates with no obvious spring? What is ω? (problem set problem)

Week 1 Lecture 2 Problems 2, 5. What if something oscillates with no obvious spring? What is ω? (problem set problem) Week 1 Lecure Problems, 5 Wha if somehing oscillaes wih no obvious spring? Wha is ω? (problem se problem) Sar wih Try and ge o SHM form E. Full beer can in lake, oscillaing F = m & = ge rearrange: F =

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

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

A Bayesian Approach to Spectral Analysis

A Bayesian Approach to Spectral Analysis Chirped Signals A Bayesian Approach o Specral Analysis Chirped signals are oscillaing signals wih ime variable frequencies, usually wih a linear variaion of frequency wih ime. E.g. f() = A cos(ω + α 2

More information

Linear Response Theory: The connection between QFT and experiments

Linear Response Theory: The connection between QFT and experiments Phys540.nb 39 3 Linear Response Theory: The connecion beween QFT and experimens 3.1. Basic conceps and ideas Q: How do we measure he conduciviy of a meal? A: we firs inroduce a weak elecric field E, and

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

Notes on Kalman Filtering

Notes on Kalman Filtering Noes on Kalman Filering Brian Borchers and Rick Aser November 7, Inroducion Daa Assimilaion is he problem of merging model predicions wih acual measuremens of a sysem o produce an opimal esimae of he curren

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

Designing Information Devices and Systems I Spring 2019 Lecture Notes Note 17

Designing Information Devices and Systems I Spring 2019 Lecture Notes Note 17 EES 16A Designing Informaion Devices and Sysems I Spring 019 Lecure Noes Noe 17 17.1 apaciive ouchscreen In he las noe, we saw ha a capacior consiss of wo pieces on conducive maerial separaed by a nonconducive

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

= ( ) ) 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

FITTING EQUATIONS TO DATA

FITTING EQUATIONS TO DATA TANTON S TAKE ON FITTING EQUATIONS TO DATA CURRICULUM TIDBITS FOR THE MATHEMATICS CLASSROOM MAY 013 Sandard algebra courses have sudens fi linear and eponenial funcions o wo daa poins, and quadraic funcions

More information

0.1 MAXIMUM LIKELIHOOD ESTIMATION EXPLAINED

0.1 MAXIMUM LIKELIHOOD ESTIMATION EXPLAINED 0.1 MAXIMUM LIKELIHOOD ESTIMATIO EXPLAIED Maximum likelihood esimaion is a bes-fi saisical mehod for he esimaion of he values of he parameers of a sysem, based on a se of observaions of a random variable

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

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

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

14 Autoregressive Moving Average Models

14 Autoregressive Moving Average Models 14 Auoregressive Moving Average Models In his chaper an imporan parameric family of saionary ime series is inroduced, he family of he auoregressive moving average, or ARMA, processes. For a large class

More information

R t. C t P t. + u t. C t = αp t + βr t + v t. + β + w t

R t. C t P t. + u t. C t = αp t + βr t + v t. + β + w t Exercise 7 C P = α + β R P + u C = αp + βr + v (a) (b) C R = α P R + β + w (c) Assumpions abou he disurbances u, v, w : Classical assumions on he disurbance of one of he equaions, eg. on (b): E(v v s P,

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

SMT 2014 Calculus Test Solutions February 15, 2014 = 3 5 = 15.

SMT 2014 Calculus Test Solutions February 15, 2014 = 3 5 = 15. SMT Calculus Tes Soluions February 5,. Le f() = and le g() =. Compue f ()g (). Answer: 5 Soluion: We noe ha f () = and g () = 6. Then f ()g () =. Plugging in = we ge f ()g () = 6 = 3 5 = 5.. There is a

More information

Lab #2: Kinematics in 1-Dimension

Lab #2: Kinematics in 1-Dimension Reading Assignmen: Chaper 2, Secions 2-1 hrough 2-8 Lab #2: Kinemaics in 1-Dimension Inroducion: The sudy of moion is broken ino wo main areas of sudy kinemaics and dynamics. Kinemaics is he descripion

More information

5.1 - Logarithms and Their Properties

5.1 - Logarithms and Their Properties Chaper 5 Logarihmic Funcions 5.1 - Logarihms and Their Properies Suppose ha a populaion grows according o he formula P 10, where P is he colony size a ime, in hours. When will he populaion be 2500? We

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

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

3.1 More on model selection

3.1 More on model selection 3. More on Model selecion 3. Comparing models AIC, BIC, Adjused R squared. 3. Over Fiing problem. 3.3 Sample spliing. 3. More on model selecion crieria Ofen afer model fiing you are lef wih a handful of

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

CHAPTER 2: Mathematics for Microeconomics

CHAPTER 2: Mathematics for Microeconomics CHAPTER : Mahemaics for Microeconomics The problems in his chaper are primarily mahemaical. They are inended o give sudens some pracice wih he conceps inroduced in Chaper, bu he problems in hemselves offer

More information

Non-parametric techniques. Instance Based Learning. NN Decision Boundaries. Nearest Neighbor Algorithm. Distance metric important

Non-parametric techniques. Instance Based Learning. NN Decision Boundaries. Nearest Neighbor Algorithm. Distance metric important on-parameric echniques Insance Based Learning AKA: neares neighbor mehods, non-parameric, lazy, memorybased, or case-based learning Copyrigh 2005 by David Helmbold 1 Do no fi a model (as do LDA, logisic

More information

Section 4.4 Logarithmic Properties

Section 4.4 Logarithmic Properties Secion. Logarihmic Properies 59 Secion. Logarihmic Properies In he previous secion, we derived wo imporan properies of arihms, which allowed us o solve some asic eponenial and arihmic equaions. Properies

More information

Section 4.4 Logarithmic Properties

Section 4.4 Logarithmic Properties Secion. Logarihmic Properies 5 Secion. Logarihmic Properies In he previous secion, we derived wo imporan properies of arihms, which allowed us o solve some asic eponenial and arihmic equaions. Properies

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

STRUCTURAL CHANGE IN TIME SERIES OF THE EXCHANGE RATES BETWEEN YEN-DOLLAR AND YEN-EURO IN

STRUCTURAL CHANGE IN TIME SERIES OF THE EXCHANGE RATES BETWEEN YEN-DOLLAR AND YEN-EURO IN Inernaional Journal of Applied Economerics and Quaniaive Sudies. Vol.1-3(004) STRUCTURAL CHANGE IN TIME SERIES OF THE EXCHANGE RATES BETWEEN YEN-DOLLAR AND YEN-EURO IN 001-004 OBARA, Takashi * Absrac The

More information

STA 114: Statistics. Notes 2. Statistical Models and the Likelihood Function

STA 114: Statistics. Notes 2. Statistical Models and the Likelihood Function STA 114: Saisics Noes 2. Saisical Models and he Likelihood Funcion Describing Daa & Saisical Models A physicis has a heory ha makes a precise predicion of wha s o be observed in daa. If he daa doesn mach

More information

References are appeared in the last slide. Last update: (1393/08/19)

References are appeared in the last slide. Last update: (1393/08/19) SYSEM IDEIFICAIO Ali Karimpour Associae Professor Ferdowsi Universi of Mashhad References are appeared in he las slide. Las updae: 0..204 393/08/9 Lecure 5 lecure 5 Parameer Esimaion Mehods opics o be

More information

Nature Neuroscience: doi: /nn Supplementary Figure 1. Spike-count autocorrelations in time.

Nature Neuroscience: doi: /nn Supplementary Figure 1. Spike-count autocorrelations in time. Supplemenary Figure 1 Spike-coun auocorrelaions in ime. Normalized auocorrelaion marices are shown for each area in a daase. The marix shows he mean correlaion of he spike coun in each ime bin wih he spike

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

Sections 2.2 & 2.3 Limit of a Function and Limit Laws

Sections 2.2 & 2.3 Limit of a Function and Limit Laws Mah 80 www.imeodare.com Secions. &. Limi of a Funcion and Limi Laws In secion. we saw how is arise when we wan o find he angen o a curve or he velociy of an objec. Now we urn our aenion o is in general

More information

Chapter 7: Solving Trig Equations

Chapter 7: Solving Trig Equations Haberman MTH Secion I: The Trigonomeric Funcions Chaper 7: Solving Trig Equaions Le s sar by solving a couple of equaions ha involve he sine funcion EXAMPLE a: Solve he equaion sin( ) The inverse funcions

More information

Time series Decomposition method

Time series Decomposition method Time series Decomposiion mehod A ime series is described using a mulifacor model such as = f (rend, cyclical, seasonal, error) = f (T, C, S, e) Long- Iner-mediaed Seasonal Irregular erm erm effec, effec,

More information

ACE 562 Fall Lecture 8: The Simple Linear Regression Model: R 2, Reporting the Results and Prediction. by Professor Scott H.

ACE 562 Fall Lecture 8: The Simple Linear Regression Model: R 2, Reporting the Results and Prediction. by Professor Scott H. ACE 56 Fall 5 Lecure 8: The Simple Linear Regression Model: R, Reporing he Resuls and Predicion by Professor Sco H. Irwin Required Readings: Griffihs, Hill and Judge. "Explaining Variaion in he Dependen

More information

5.2. The Natural Logarithm. Solution

5.2. The Natural Logarithm. Solution 5.2 The Naural Logarihm The number e is an irraional number, similar in naure o π. Is non-erminaing, non-repeaing value is e 2.718 281 828 59. Like π, e also occurs frequenly in naural phenomena. In fac,

More information

1 Differential Equation Investigations using Customizable

1 Differential Equation Investigations using Customizable Differenial Equaion Invesigaions using Cusomizable Mahles Rober Decker The Universiy of Harford Absrac. The auhor has developed some plaform independen, freely available, ineracive programs (mahles) for

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

dt = C exp (3 ln t 4 ). t 4 W = C exp ( ln(4 t) 3) = C(4 t) 3.

dt = C exp (3 ln t 4 ). t 4 W = C exp ( ln(4 t) 3) = C(4 t) 3. Mah Rahman Exam Review Soluions () Consider he IVP: ( 4)y 3y + 4y = ; y(3) = 0, y (3) =. (a) Please deermine he longes inerval for which he IVP is guaraneed o have a unique soluion. Soluion: The disconinuiies

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

ACE 564 Spring Lecture 7. Extensions of The Multiple Regression Model: Dummy Independent Variables. by Professor Scott H.

ACE 564 Spring Lecture 7. Extensions of The Multiple Regression Model: Dummy Independent Variables. by Professor Scott H. ACE 564 Spring 2006 Lecure 7 Exensions of The Muliple Regression Model: Dumm Independen Variables b Professor Sco H. Irwin Readings: Griffihs, Hill and Judge. "Dumm Variables and Varing Coefficien Models

More information

The Arcsine Distribution

The Arcsine Distribution The Arcsine Disribuion Chris H. Rycrof Ocober 6, 006 A common heme of he class has been ha he saisics of single walker are ofen very differen from hose of an ensemble of walkers. On he firs homework, we

More information

4.1 - Logarithms and Their Properties

4.1 - Logarithms and Their Properties Chaper 4 Logarihmic Funcions 4.1 - Logarihms and Their Properies Wha is a Logarihm? We define he common logarihm funcion, simply he log funcion, wrien log 10 x log x, as follows: If x is a posiive number,

More information

Non-parametric techniques. Instance Based Learning. NN Decision Boundaries. Nearest Neighbor Algorithm. Distance metric important

Non-parametric techniques. Instance Based Learning. NN Decision Boundaries. Nearest Neighbor Algorithm. Distance metric important on-parameric echniques Insance Based Learning AKA: neares neighbor mehods, non-parameric, lazy, memorybased, or case-based learning Copyrigh 2005 by David Helmbold 1 Do no fi a model (as do LTU, decision

More information

GENERALIZATION OF THE FORMULA OF FAA DI BRUNO FOR A COMPOSITE FUNCTION WITH A VECTOR ARGUMENT

GENERALIZATION OF THE FORMULA OF FAA DI BRUNO FOR A COMPOSITE FUNCTION WITH A VECTOR ARGUMENT Inerna J Mah & Mah Sci Vol 4, No 7 000) 48 49 S0670000970 Hindawi Publishing Corp GENERALIZATION OF THE FORMULA OF FAA DI BRUNO FOR A COMPOSITE FUNCTION WITH A VECTOR ARGUMENT RUMEN L MISHKOV Received

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

Radical Expressions. Terminology: A radical will have the following; a radical sign, a radicand, and an index.

Radical Expressions. Terminology: A radical will have the following; a radical sign, a radicand, and an index. Radical Epressions Wha are Radical Epressions? A radical epression is an algebraic epression ha conains a radical. The following are eamples of radical epressions + a Terminology: A radical will have he

More information

Analyze patterns and relationships. 3. Generate two numerical patterns using AC

Analyze patterns and relationships. 3. Generate two numerical patterns using AC envision ah 2.0 5h Grade ah Curriculum Quarer 1 Quarer 2 Quarer 3 Quarer 4 andards: =ajor =upporing =Addiional Firs 30 Day 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 andards: Operaions and Algebraic Thinking

More information

2. Nonlinear Conservation Law Equations

2. Nonlinear Conservation Law Equations . Nonlinear Conservaion Law Equaions One of he clear lessons learned over recen years in sudying nonlinear parial differenial equaions is ha i is generally no wise o ry o aack a general class of nonlinear

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

18 Biological models with discrete time

18 Biological models with discrete time 8 Biological models wih discree ime The mos imporan applicaions, however, may be pedagogical. The elegan body of mahemaical heory peraining o linear sysems (Fourier analysis, orhogonal funcions, and so

More information

Navneet Saini, Mayank Goyal, Vishal Bansal (2013); Term Project AML310; Indian Institute of Technology Delhi

Navneet Saini, Mayank Goyal, Vishal Bansal (2013); Term Project AML310; Indian Institute of Technology Delhi Creep in Viscoelasic Subsances Numerical mehods o calculae he coefficiens of he Prony equaion using creep es daa and Herediary Inegrals Mehod Navnee Saini, Mayank Goyal, Vishal Bansal (23); Term Projec

More information

NCSS Statistical Software. , contains a periodic (cyclic) component. A natural model of the periodic component would be

NCSS Statistical Software. , contains a periodic (cyclic) component. A natural model of the periodic component would be NCSS Saisical Sofware Chaper 468 Specral Analysis Inroducion This program calculaes and displays he periodogram and specrum of a ime series. This is someimes nown as harmonic analysis or he frequency approach

More information

Empirical Process Theory

Empirical Process Theory Empirical Process heory 4.384 ime Series Analysis, Fall 27 Reciaion by Paul Schrimpf Supplemenary o lecures given by Anna Mikusheva Ocober 7, 28 Reciaion 7 Empirical Process heory Le x be a real-valued

More information

Introduction to Numerical Analysis. In this lesson you will be taken through a pair of techniques that will be used to solve the equations of.

Introduction to Numerical Analysis. In this lesson you will be taken through a pair of techniques that will be used to solve the equations of. Inroducion o Nuerical Analysis oion In his lesson you will be aen hrough a pair of echniques ha will be used o solve he equaions of and v dx d a F d for siuaions in which F is well nown, and he iniial

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

Measurement Error 1: Consequences Page 1. Definitions. For two variables, X and Y, the following hold: Expectation, or Mean, of X.

Measurement Error 1: Consequences Page 1. Definitions. For two variables, X and Y, the following hold: Expectation, or Mean, of X. Measuremen Error 1: Consequences of Measuremen Error Richard Williams, Universiy of Nore Dame, hps://www3.nd.edu/~rwilliam/ Las revised January 1, 015 Definiions. For wo variables, X and Y, he following

More information

Kriging Models Predicting Atrazine Concentrations in Surface Water Draining Agricultural Watersheds

Kriging Models Predicting Atrazine Concentrations in Surface Water Draining Agricultural Watersheds 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 Kriging Models Predicing Arazine Concenraions in Surface Waer Draining Agriculural Waersheds Paul L. Mosquin, Jeremy Aldworh, Wenlin Chen Supplemenal Maerial Number

More information

MATH 31B: MIDTERM 2 REVIEW. x 2 e x2 2x dx = 1. ue u du 2. x 2 e x2 e x2] + C 2. dx = x ln(x) 2 2. ln x dx = x ln x x + C. 2, or dx = 2u du.

MATH 31B: MIDTERM 2 REVIEW. x 2 e x2 2x dx = 1. ue u du 2. x 2 e x2 e x2] + C 2. dx = x ln(x) 2 2. ln x dx = x ln x x + C. 2, or dx = 2u du. MATH 3B: MIDTERM REVIEW JOE HUGHES. Inegraion by Pars. Evaluae 3 e. Soluion: Firs make he subsiuion u =. Then =, hence 3 e = e = ue u Now inegrae by pars o ge ue u = ue u e u + C and subsiue he definiion

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

Bias in Conditional and Unconditional Fixed Effects Logit Estimation: a Correction * Tom Coupé

Bias in Conditional and Unconditional Fixed Effects Logit Estimation: a Correction * Tom Coupé Bias in Condiional and Uncondiional Fixed Effecs Logi Esimaion: a Correcion * Tom Coupé Economics Educaion and Research Consorium, Naional Universiy of Kyiv Mohyla Academy Address: Vul Voloska 10, 04070

More information

Math 333 Problem Set #2 Solution 14 February 2003

Math 333 Problem Set #2 Solution 14 February 2003 Mah 333 Problem Se #2 Soluion 14 February 2003 A1. Solve he iniial value problem dy dx = x2 + e 3x ; 2y 4 y(0) = 1. Soluion: This is separable; we wrie 2y 4 dy = x 2 + e x dx and inegrae o ge The iniial

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

Block Diagram of a DCS in 411

Block Diagram of a DCS in 411 Informaion source Forma A/D From oher sources Pulse modu. Muliplex Bandpass modu. X M h: channel impulse response m i g i s i Digial inpu Digial oupu iming and synchronizaion Digial baseband/ bandpass

More information

Module 2 F c i k c s la l w a s o s f dif di fusi s o i n

Module 2 F c i k c s la l w a s o s f dif di fusi s o i n Module Fick s laws of diffusion Fick s laws of diffusion and hin film soluion Adolf Fick (1855) proposed: d J α d d d J (mole/m s) flu (m /s) diffusion coefficien and (mole/m 3 ) concenraion of ions, aoms

More information

RANDOM LAGRANGE MULTIPLIERS AND TRANSVERSALITY

RANDOM LAGRANGE MULTIPLIERS AND TRANSVERSALITY ECO 504 Spring 2006 Chris Sims RANDOM LAGRANGE MULTIPLIERS AND TRANSVERSALITY 1. INTRODUCTION Lagrange muliplier mehods are sandard fare in elemenary calculus courses, and hey play a cenral role in economic

More information