{ In general, we are presented with a quadratic function of a random vector X

Size: px
Start display at page:

Download "{ In general, we are presented with a quadratic function of a random vector X"

Transcription

1 Quadratc VAR odel Mchael Carter à Prelnares Introducton Suppose we wsh to quantfy the value-at-rsk of a Japanese etals tradng fr that has exposure to forward and opton postons n platnu. Soe of the postons are denonated n USDs. We dentfy three key rsk factors æ spot prce of platnu n yen (X ) æ a representatve pled volatlty of platnu (X ) æ spot JPY/USD exchange rate (X 3 ) and assue that X = HX, X, X 3 L s norally dstrbuted NH, SL wth =(53.50, 0.670,07.80) and y S = k z { We value the portfolo usng applcable forward and opton prcng forulas, and quadratcally approxate ths as Y = a + D T X + X T G X Our obectve s to estate certan quantles of Y. In general, we are presented wth a quadratc functon of a rando vector X Y = a + D T X + X T G X where X ~ N H, S L. Ths ght arse as above fro a delta-gaa approxaton to a VAR easure of a portfolo contanng dervatves, or soe alternatve approxaton. Then, as we wll show, Y can be expressed as a lnear cobnaton of ndependent ch-squared and noral rando varables. Based on ths representaton, we can calculate the oents and the dstrbuton functon of Y. For exposton, let us start wth a nuercally spler specfc exaple. Suppose that X s ultvarate noral wth ean and varance µ = 8,, 0<; Σ = 0 y 0 z ; k 5 {

2 VARQuadratc.nb and that Y s gven by wth Y = a + D T X + X T G X a = ; = 88, 3, <; Γ = y z ; k { In other words, Y s deterned by the followng quadratc functon of correlated noral rando varables. Y = + 8 X + 3 X + 3 X + X X + 6 X - X 3-6 X X 3 - X X X 3 Defne new rando varables as follows Z = X -, Z = X - + HX - L - HX 3-3 L, Z 3 = - HX - L + HX 3-3 L The Z are ndependent standard noral rando varables. Exercse: Verfy that the Z, Z, Z 3 are ndependent standard noral rando varables. The rando vector Z = HZ, Z, Z 3 L s defned by the transforaton where Z = A HX - L 0 0 y A = - z k 0 - { Z has ean 0 and varance-convarance atrx A S A T = I. Solvng for X gves X = A - Z + Substtutng n the equaton defnng Y and splfyng, we have Y = + 8 X + 3 X + 3 X + X X + 6 X - X 3-6 X X 3 - X X X 3 = Z + Z + 3 Z + 6 Z 3 By "copletng the square" for Z, we can express ths as Y = Z + 3 HZ + 4 Z L + 6 Z 3 = Z + 3 HZ + L Z 3 = Z + 3 HZ + L + 6 Z 3

3 VARQuadratc.nb 3 We have expressed Y as a lnear cobnaton of 3 ndependent rando varables: Z ~ c H, 0L, Z ~ c H, 4L, Z 3 ~ NH0, L. In atheatcal ters, we have acheved two thngs. æ We have expressed Y n ters of ndependent standard noral rando varables Z (Cholesky decoposton). æ We have dagonalzed the quadratc for wth respect to these varables so that there are no crossters Z Z (Prncpal axs theore). The transforaton A s the coposton of these two steps. We now exane the condtons requred for ths n general. Suppose that Y s a quadratc functon of rando vector X Y = a + D T X + X T G X where X ~ N H, S L. Wthout loss of generalty, we can assue that = 0, snce any ean effect can be ncorporated nto a new constant ter a. Further, we can assue that S s postve defnte. There exsts a lower trangular atrx H such that S =HH T and X = H Z è where Z è s standard noral. Ths s known as the Cholesky decoposton. Substtutng where Y = a + D T H Z è + HH Z è L T G H Z è = a +D T Z è + Z è T GZ è D = H T D and G = H T G H Snce G s syetrc, so s G and there exsts an orthogonal atrx P such that P T GP = L or G = P L P T where L s a dagonal atrx contanng the egenvalues of G (Spectral theore). Therefore where Y = a +D T Z è + Z è T GZ è = a +D T PP T Z è + Z è T P L P T Z è = a + B T Z + Z T L Z B =P T D = P T H T D and Z = P T Z è Snce P s orthogonal, Z = HZ, Z,,Z L s also a vector of ndependent standard noral rando varables. Therefore, Y can be expressed as a lnear cobnaton of noral and ch-squared rando varables Y = a + B T Z + Z T L Z = a + Hb Z + l Z L = We suarze n the followng theore. Theore Suppose that Y s a quadratc functon of rando vector X

4 4 VARQuadratc.nb Y = a + D T X + X T G X where X ~ N H, S L, and S s postve defnte. Then there exsts a lnear transforaton A such that X = A - Z + and Y = a + B T Z + Z T L Z where L s a dagonal atrx and Z,Z,,Z are ndependent standard noral rando varables. Consequently Y can be wrtten as Y = a + Hb Z + l Z L = Ths theore shows that Y s a lnear cobnaton of ndependent noral and ch-square rando varables or non-central ch-square rando varables (see copleentary lecture note Quadratc functons of noral rando varables). Consequently, the characterstc functon of Y can be readly deterned, fro whch the exact dstrbuton functon can be calculated. Alternatvely, a nuber of coputatonally easer approxatons for the quantles are avalable, ncludng æ Cornsh-Fsher expanson æ saddlepont approxaton Both of these approxatons are based upon the cuulant generatng functon. The dstrbuton of Y Our frst goal s to deterne the oent generatng functon, fro whch we can derve both the cuulant generatng functon and the characterstc functon. Fro the latter, we can obtan the dstrbuton functon by Fourer nverson. à Moent generatng functon By drect ntegraton, we can readly deterne that the oent generatng functon of a sngle ter of the for b Z + l Z s where M HtL = EA b Z +l Z E = - Hb z +l z L t fhzl z = ÅÅÅÅ ÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅ è!!!!!!!!!!!!!!!!! ÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅ - t l b t ÅÅÅÅÅÅÅÅ - ÅÅÅÅÅÅÅÅ l t fhzl = ÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅ è!!!!!! p - z ÅÅÅÅÅ s the standard noral densty functon. Therefore, the oent generatng functon of Y = a + = Hb Z + l Z L s

5 VARQuadratc.nb 5 M Y HtL = E@ ty D = a t M HtL M HtL M n HtL = n a t ÅÅÅÅ Â ÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅ è!!!!!!!!!!!!!!!!! ÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅ k - t l = b t ÅÅÅÅÅÅÅÅ - ÅÅÅÅÅÅÅÅ l t y z = { a t Exp n ÅÅÅÅÅ k = n b t y ÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅ - l t z  { = y ÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅ è!!!!!!!!!!!!!!!!! ÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅ z k - t l { fro whch the oents can be edately derved by dfferentaton. (Holton 003: 49 gves a coplcated recursve forula for the oents of Y.) In the prevous exaple, a =5, B =H0,, 6L and L =H4, 3, 0L. The oents of Y are EV@YD EV@Y D 374 EV@Y 3 D 338 EV@Y 4 D EV@Y 5 D The varance of Y s therefore E@Y D - E@YD = = 30. à The cuulant generatng functon Cuulants are analogous to oents. The frst cuulant s the sae as the frst oent (the expected value); the second and thrd cuulants are respectvely the second (varance) and thrd central oents; but the hgher cuulants are nether oents nor central oents, but rather ore coplcated polynoal functons of the oents. The cuulant generatng functon s gven by the log of the oent generatng functon, that s KHtL = log M HtL = at - ÅÅÅÅÅ n = logh - l tl + ÅÅÅÅÅ n = b t ÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅ - l t fro whch the cuulants can be derved by dfferentaton. In the prevous exaple, wth a =5, B =H0,, 6L and L =H4, 3, 0L, the cuulants of Y are κ κ 30 κ κ κ

6 6 VARQuadratc.nb à Characterstc functon The characterstc functon of any rando varable Y s YHwL = E@  wy D Consequently, t can be obtaned by substtutng t = Âw nto the oent generatng functon. The characterstc functon of Y s YHwL = M H wl = Exp  aw- ÅÅÅÅÅ k = n n w b y ÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅ -  w l z  { = ÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅ è!!!!!!!!!!!!!!!! ÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅ!!!!!! ÅÅÅÅÅÅÅÅ -  w l à The dstrbuton functon The dstrbuton functon of Y can be obtaned by nvertng the characterstc functon (Holton 003: 59, Quadratc functons of noral rando varables) FHyL = ÅÅÅÅÅ - ÅÅÅÅÅ p IH YHwL - wy L ÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅ ÅÅÅÅÅÅÅÅÅÅÅÅÅÅ w 0 w Substtutng the characterstc functon and splfyng gves where FHyL = ÅÅÅÅÅ + ÅÅÅÅÅ p A snhb + CL ÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅ ÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅ w 0 D A = - ÅÅÅÅÅÅÅÅ w = C = ÅÅÅÅÅ = b ÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅ + 4 l w, B = w y b y l -a+w ÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅ + 4 l k w z, = { tan - H- l wl, D = w H + 4 l w L ê4 = For gven values of b, l ( =,,, ) and y, ths expresson can be nuercally ntegrated to gve a very accurate approxaton of dstrbuton functon. The cuulatve dstrbuton functon of Y for the exaple wth a =5, B =H0,, 6L and L =H4, 3, 0L s depcted below, together wth the CDF of a noral dstrbuton wth the sae ean and varance (red).

7 VARQuadratc.nb The CDF of Y Y Noral Fro the dstrbuton functon, the quantles can be coputed drectly. The Fast Fourer Transfor provdes a potental alternatve ethod of coputng the dstrbuton functon of Y. Approxatng the quantles of Y A nuber of ethods have been suggested for approxatng the quantles of Y. Two of the ost prosng are the Cornsh-Fsher expanson and saddlepont approxatons. Coparatve studes suggest that the Cornsh- Fsher expanson s coputatonally faster, whle the saddlepont approxaton s ore accurate, especally n the tals. à Cornsh-Fsher expanson The Cornsh-Fsher expanson approxates the quantles of a dstrbuton as a polynoal of ts cuulants. That s, the a quantle of Y s F Ȳ HaL º a 0 + a k 3 + a k 4 + a 3 k 3 + a 4 k 5 + a 5 k 3 k 4 + a 6 k 3 3 where the coeffcents a 0, a,, a 6 are polynoals of the quantles of the standard noral dstrbuton. a 0 = F - HaL, a = ÅÅÅÅÅ 6 IF- HaL - M, a = ÅÅÅÅÅÅÅÅ 4 IF- HaL 3-3 F - HaLM, a 3 = - ÅÅÅÅÅÅÅÅ 36 I F- HaL 3-5 F - HaLM a 4 = ÅÅÅÅÅÅÅÅÅÅÅ 0 IF- HaL 4-6 F - HaL + 3M, a 5 =- ÅÅÅÅÅÅÅÅ 4 IF- HaL 4-5 F - HaL + M, a 6 = ÅÅÅÅÅÅÅÅÅÅÅ 34 I F- HaL 4-53 F - HaL + 7M The cuulants are readly obtaned fro the cuulant generatng functon.

8 8 VARQuadratc.nb The followng graph shows the Cornsh-Fsher expanson superposed on the exact dstrbuton functon of Y. The Cornsh-Fsher expanson à Saddlepont approxaton The saddlepont approxaton to the cuulatve dstrbuton functon of Y (due to Lugannan and Rce) s gven by F Y HyL º FHrL - nhrl J ÅÅÅÅÅ () u - ÅÅÅÅÅ r N where F and n are respectvely the dstrbuton functon and densty functon of the standard noral dstrbuton, and r = è!!! è!!!!!!!!!!!!!!!! f y - KHfL!!!!!!! and u = f è!!!!!!!!!!!! K '' HfL K s the cuulant generatng functon KHtL = log M HtL = at - ÅÅÅÅÅ = logh - l tl + ÅÅÅÅÅ = b t ÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅ - l t and the saddlepont f solves K ' HfL = y An alternatve approxaton, due to Barndorff-Nelsen, s gven by () F Y HyL º FJr - ÅÅÅÅÅ r log ÅÅÅÅÅ u N

9 VARQuadratc.nb 9 Wthout loss of generalty, assue that l = n l and l = ax l. If l < 0, then we ust have t > ê l. Slarly, f l > 0, then we ust have t < ê l. In any case, K s defned on an nterval around the orgn. Coputng the saddlepont approxaton for a specfc y nvolves solvng equaton () for the saddlepont f, and then calculatng F Y HyL usng equaton (). The frst and second dervatves of K are K ' HtL = a + = l ÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅ - l t b + th -l tl ÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅ H - l tl = K '' HtL = = l ÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅ H - l tl + = b ÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅÅ H - l tl 3 SaddlePont Approxaton à Coparson The followng graph copares the errors of the two approxaton ethods, relatve to the cuulatve dstrbuton functon of Y.

10 0 VARQuadratc.nb Errors of saddlepont and Cornsh-Fsher approxatons 0.00 Cornsh-Fsher expanson Saddlepont approxaton Exaple (adapted fro Holton 003) A Japanese etals tradng fr has exposure to forward and opton postons n platnu. Soe of the postons are denonated n USDs. We dentfy three key rsk factors X æ spot prce of platnu (JPY) æ a representatve pled volatlty of platnu æ spot JPY/USD exchange rate and assue that X s norally dstrbuted NH, SL wth µ = , 0.670, 07.80< ; Σ = y k z ; { We value the portfolo usng applcable forward and opton prcng forulas, and quadratcally approxate ths as wth P = a + D T X + X T G X a = ; = , , <; Γ = y k z ; 5673 {

11 VARQuadratc.nb Hz = CholeskyDecoposton@ΣD êê TransposeL êê MatrxFor y z k { H8Λ, u< = Egensyste@Transpose@zD.Γ.zD L; 8Λ, MatrxFor@uD< , 858., 845.9<, y z = k { Transpose@uD.u êê Chop êê TableFor HA = u.inverse@zdl êê MatrxFor k Usng the substtuton y z { Z = A HX - L we transfor P nto a quadratc functon of ndependent ch-squared rando varables, naely ChopA a +.X+ X.Γ.X ê. X Inverse@AD. 8Z,Z,Z 3 < + µ êê Expand, 0 8 E Z Z Z 858. Z Z Z 3 That s P = a + Hb Z + l Z L = wth a = µ 0 9, B =H µ 0 8, µ 0 6, µ 0 6 L and L =H µ 0 6, -858., 845.9L.

12 VARQuadratc.nb A. êê Chop êê MatrxFor k y z { paraeters = 8 = 3, α = , β = , β = , β 3 = , λ = , λ = 858., λ 3 = 845.9<; The cuulants of P are Table@8κ k,d@k@td, 8t, k<d ê. t 0<, 8k, 5<D êê TableFor κ κ κ κ κ The standard devaton s è!!!!!!!!!!!!!!! K''@0D The portfolo's -day standard devaton s JPY 358 llon. Applyng the Cornsh-Fsher expanson, the 5% quantle of P s approxately JPY 8.7 bllon. CFQuantle@0.05D Based on the expected ean of JPY 9.3 bllon, the portfolo has a -day 95% VAR of approxately JPY 583 llon, whch s close to.65 standard devatons. K'@0D CFQuantle@0.05D è!!!!!!!!!!!!!!! K''@0D

13 VARQuadratc.nb 3 Suppose that we sply gnored the non-noralty, and calculated the standard devaton lnearly, n effect gnorng the quadratc ter. P = a + D T X + X T G X In ths case, we over-estate the standard devaton. è!!!!!!!!!!!!!!!!. Σ Our 95% VAR estate s then.65 è!!!!!!!!!!!!!!!!. Σ whch overestates the rsk by 6%

BAYESIAN CURVE FITTING USING PIECEWISE POLYNOMIALS. Dariusz Biskup

BAYESIAN CURVE FITTING USING PIECEWISE POLYNOMIALS. Dariusz Biskup BAYESIAN CURVE FITTING USING PIECEWISE POLYNOMIALS Darusz Bskup 1. Introducton The paper presents a nonparaetrc procedure for estaton of an unknown functon f n the regresson odel y = f x + ε = N. (1) (

More information

Introducing Entropy Distributions

Introducing Entropy Distributions Graubner, Schdt & Proske: Proceedngs of the 6 th Internatonal Probablstc Workshop, Darstadt 8 Introducng Entropy Dstrbutons Noel van Erp & Peter van Gelder Structural Hydraulc Engneerng and Probablstc

More information

Slobodan Lakić. Communicated by R. Van Keer

Slobodan Lakić. Communicated by R. Van Keer Serdca Math. J. 21 (1995), 335-344 AN ITERATIVE METHOD FOR THE MATRIX PRINCIPAL n-th ROOT Slobodan Lakć Councated by R. Van Keer In ths paper we gve an teratve ethod to copute the prncpal n-th root and

More information

System in Weibull Distribution

System in Weibull Distribution Internatonal Matheatcal Foru 4 9 no. 9 94-95 Relablty Equvalence Factors of a Seres-Parallel Syste n Webull Dstrbuton M. A. El-Dacese Matheatcs Departent Faculty of Scence Tanta Unversty Tanta Egypt eldacese@yahoo.co

More information

Least Squares Fitting of Data

Least Squares Fitting of Data Least Squares Fttng of Data Davd Eberly Geoetrc Tools, LLC http://www.geoetrctools.co/ Copyrght c 1998-2014. All Rghts Reserved. Created: July 15, 1999 Last Modfed: February 9, 2008 Contents 1 Lnear Fttng

More information

XII.3 The EM (Expectation-Maximization) Algorithm

XII.3 The EM (Expectation-Maximization) Algorithm XII.3 The EM (Expectaton-Maxzaton) Algorth Toshnor Munaata 3/7/06 The EM algorth s a technque to deal wth varous types of ncoplete data or hdden varables. It can be appled to a wde range of learnng probles

More information

Applied Mathematics Letters

Applied Mathematics Letters Appled Matheatcs Letters 2 (2) 46 5 Contents lsts avalable at ScenceDrect Appled Matheatcs Letters journal hoepage: wwwelseverco/locate/al Calculaton of coeffcents of a cardnal B-splne Gradr V Mlovanovć

More information

The Parity of the Number of Irreducible Factors for Some Pentanomials

The Parity of the Number of Irreducible Factors for Some Pentanomials The Party of the Nuber of Irreducble Factors for Soe Pentanoals Wolfra Koepf 1, Ryul K 1 Departent of Matheatcs Unversty of Kassel, Kassel, F. R. Gerany Faculty of Matheatcs and Mechancs K Il Sung Unversty,

More information

Denote the function derivatives f(x) in given points. x a b. Using relationships (1.2), polynomials (1.1) are written in the form

Denote the function derivatives f(x) in given points. x a b. Using relationships (1.2), polynomials (1.1) are written in the form SET OF METHODS FO SOUTION THE AUHY POBEM FO STIFF SYSTEMS OF ODINAY DIFFEENTIA EUATIONS AF atypov and YuV Nulchev Insttute of Theoretcal and Appled Mechancs SB AS 639 Novosbrs ussa Introducton A constructon

More information

Finite Vector Space Representations Ross Bannister Data Assimilation Research Centre, Reading, UK Last updated: 2nd August 2003

Finite Vector Space Representations Ross Bannister Data Assimilation Research Centre, Reading, UK Last updated: 2nd August 2003 Fnte Vector Space epresentatons oss Bannster Data Asslaton esearch Centre, eadng, UK ast updated: 2nd August 2003 Contents What s a lnear vector space?......... 1 About ths docuent............ 2 1. Orthogonal

More information

Determination of the Confidence Level of PSD Estimation with Given D.O.F. Based on WELCH Algorithm

Determination of the Confidence Level of PSD Estimation with Given D.O.F. Based on WELCH Algorithm Internatonal Conference on Inforaton Technology and Manageent Innovaton (ICITMI 05) Deternaton of the Confdence Level of PSD Estaton wth Gven D.O.F. Based on WELCH Algorth Xue-wang Zhu, *, S-jan Zhang

More information

y new = M x old Feature Selection: Linear Transformations Constraint Optimization (insertion)

y new = M x old Feature Selection: Linear Transformations Constraint Optimization (insertion) Feature Selecton: Lnear ransforatons new = M x old Constrant Optzaton (nserton) 3 Proble: Gven an objectve functon f(x) to be optzed and let constrants be gven b h k (x)=c k, ovng constants to the left,

More information

COS 511: Theoretical Machine Learning

COS 511: Theoretical Machine Learning COS 5: Theoretcal Machne Learnng Lecturer: Rob Schapre Lecture #0 Scrbe: José Sões Ferrera March 06, 203 In the last lecture the concept of Radeacher coplexty was ntroduced, wth the goal of showng that

More information

Our focus will be on linear systems. A system is linear if it obeys the principle of superposition and homogenity, i.e.

Our focus will be on linear systems. A system is linear if it obeys the principle of superposition and homogenity, i.e. SSTEM MODELLIN In order to solve a control syste proble, the descrptons of the syste and ts coponents ust be put nto a for sutable for analyss and evaluaton. The followng ethods can be used to odel physcal

More information

Least Squares Fitting of Data

Least Squares Fitting of Data Least Squares Fttng of Data Davd Eberly Geoetrc Tools, LLC http://www.geoetrctools.co/ Copyrght c 1998-2015. All Rghts Reserved. Created: July 15, 1999 Last Modfed: January 5, 2015 Contents 1 Lnear Fttng

More information

1 Review From Last Time

1 Review From Last Time COS 5: Foundatons of Machne Learnng Rob Schapre Lecture #8 Scrbe: Monrul I Sharf Aprl 0, 2003 Revew Fro Last Te Last te, we were talkng about how to odel dstrbutons, and we had ths setup: Gven - exaples

More information

Preference and Demand Examples

Preference and Demand Examples Dvson of the Huantes and Socal Scences Preference and Deand Exaples KC Border October, 2002 Revsed Noveber 206 These notes show how to use the Lagrange Karush Kuhn Tucker ultpler theores to solve the proble

More information

PROBABILITY AND STATISTICS Vol. III - Analysis of Variance and Analysis of Covariance - V. Nollau ANALYSIS OF VARIANCE AND ANALYSIS OF COVARIANCE

PROBABILITY AND STATISTICS Vol. III - Analysis of Variance and Analysis of Covariance - V. Nollau ANALYSIS OF VARIANCE AND ANALYSIS OF COVARIANCE ANALYSIS OF VARIANCE AND ANALYSIS OF COVARIANCE V. Nollau Insttute of Matheatcal Stochastcs, Techncal Unversty of Dresden, Gerany Keywords: Analyss of varance, least squares ethod, odels wth fxed effects,

More information

What is LP? LP is an optimization technique that allocates limited resources among competing activities in the best possible manner.

What is LP? LP is an optimization technique that allocates limited resources among competing activities in the best possible manner. (C) 998 Gerald B Sheblé, all rghts reserved Lnear Prograng Introducton Contents I. What s LP? II. LP Theor III. The Splex Method IV. Refneents to the Splex Method What s LP? LP s an optzaton technque that

More information

Excess Error, Approximation Error, and Estimation Error

Excess Error, Approximation Error, and Estimation Error E0 370 Statstcal Learnng Theory Lecture 10 Sep 15, 011 Excess Error, Approxaton Error, and Estaton Error Lecturer: Shvan Agarwal Scrbe: Shvan Agarwal 1 Introducton So far, we have consdered the fnte saple

More information

arxiv: v2 [math.co] 3 Sep 2017

arxiv: v2 [math.co] 3 Sep 2017 On the Approxate Asyptotc Statstcal Independence of the Peranents of 0- Matrces arxv:705.0868v2 ath.co 3 Sep 207 Paul Federbush Departent of Matheatcs Unversty of Mchgan Ann Arbor, MI, 4809-043 Septeber

More information

On Pfaff s solution of the Pfaff problem

On Pfaff s solution of the Pfaff problem Zur Pfaff scen Lösung des Pfaff scen Probles Mat. Ann. 7 (880) 53-530. On Pfaff s soluton of te Pfaff proble By A. MAYER n Lepzg Translated by D. H. Delpenc Te way tat Pfaff adopted for te ntegraton of

More information

Quantum Particle Motion in Physical Space

Quantum Particle Motion in Physical Space Adv. Studes Theor. Phys., Vol. 8, 014, no. 1, 7-34 HIKARI Ltd, www.-hkar.co http://dx.do.org/10.1988/astp.014.311136 Quantu Partcle Moton n Physcal Space A. Yu. Saarn Dept. of Physcs, Saara State Techncal

More information

Gradient Descent Learning and Backpropagation

Gradient Descent Learning and Backpropagation Artfcal Neural Networks (art 2) Chrstan Jacob Gradent Descent Learnng and Backpropagaton CSC 533 Wnter 200 Learnng by Gradent Descent Defnton of the Learnng roble Let us start wth the sple case of lnear

More information

PARAMETER ESTIMATION IN WEIBULL DISTRIBUTION ON PROGRESSIVELY TYPE- II CENSORED SAMPLE WITH BETA-BINOMIAL REMOVALS

PARAMETER ESTIMATION IN WEIBULL DISTRIBUTION ON PROGRESSIVELY TYPE- II CENSORED SAMPLE WITH BETA-BINOMIAL REMOVALS Econoy & Busness ISSN 1314-7242, Volue 10, 2016 PARAMETER ESTIMATION IN WEIBULL DISTRIBUTION ON PROGRESSIVELY TYPE- II CENSORED SAMPLE WITH BETA-BINOMIAL REMOVALS Ilhan Usta, Hanef Gezer Departent of Statstcs,

More information

NUMERICAL DIFFERENTIATION

NUMERICAL DIFFERENTIATION NUMERICAL DIFFERENTIATION 1 Introducton Dfferentaton s a method to compute the rate at whch a dependent output y changes wth respect to the change n the ndependent nput x. Ths rate of change s called the

More information

Fermi-Dirac statistics

Fermi-Dirac statistics UCC/Physcs/MK/EM/October 8, 205 Fer-Drac statstcs Fer-Drac dstrbuton Matter partcles that are eleentary ostly have a type of angular oentu called spn. hese partcles are known to have a agnetc oent whch

More information

Outline. Prior Information and Subjective Probability. Subjective Probability. The Histogram Approach. Subjective Determination of the Prior Density

Outline. Prior Information and Subjective Probability. Subjective Probability. The Histogram Approach. Subjective Determination of the Prior Density Outlne Pror Inforaton and Subjectve Probablty u89603 1 Subjectve Probablty Subjectve Deternaton of the Pror Densty Nonnforatve Prors Maxu Entropy Prors Usng the Margnal Dstrbuton to Deterne the Pror Herarchcal

More information

LECTURE :FACTOR ANALYSIS

LECTURE :FACTOR ANALYSIS LCUR :FACOR ANALYSIS Rta Osadchy Based on Lecture Notes by A. Ng Motvaton Dstrbuton coes fro MoG Have suffcent aount of data: >>n denson Use M to ft Mture of Gaussans nu. of tranng ponts If

More information

1 Definition of Rademacher Complexity

1 Definition of Rademacher Complexity COS 511: Theoretcal Machne Learnng Lecturer: Rob Schapre Lecture #9 Scrbe: Josh Chen March 5, 2013 We ve spent the past few classes provng bounds on the generalzaton error of PAClearnng algorths for the

More information

Integral Transforms and Dual Integral Equations to Solve Heat Equation with Mixed Conditions

Integral Transforms and Dual Integral Equations to Solve Heat Equation with Mixed Conditions Int J Open Probles Copt Math, Vol 7, No 4, Deceber 214 ISSN 1998-6262; Copyrght ICSS Publcaton, 214 www-csrsorg Integral Transfors and Dual Integral Equatons to Solve Heat Equaton wth Mxed Condtons Naser

More information

Solutions for Homework #9

Solutions for Homework #9 Solutons for Hoewor #9 PROBEM. (P. 3 on page 379 n the note) Consder a sprng ounted rgd bar of total ass and length, to whch an addtonal ass s luped at the rghtost end. he syste has no dapng. Fnd the natural

More information

LECTURE 8-9: THE BAKER-CAMPBELL-HAUSDORFF FORMULA

LECTURE 8-9: THE BAKER-CAMPBELL-HAUSDORFF FORMULA LECTURE 8-9: THE BAKER-CAMPBELL-HAUSDORFF FORMULA As we have seen, 1. Taylor s expanson on Le group, Y ] a(y ). So f G s an abelan group, then c(g) : G G s the entty ap for all g G. As a consequence, a()

More information

Fall 2012 Analysis of Experimental Measurements B. Eisenstein/rev. S. Errede. ) with a symmetric Pcovariance matrix of the y( x ) measurements V

Fall 2012 Analysis of Experimental Measurements B. Eisenstein/rev. S. Errede. ) with a symmetric Pcovariance matrix of the y( x ) measurements V Fall Analyss o Experental Measureents B Esensten/rev S Errede General Least Squares wth General Constrants: Suppose we have easureents y( x ( y( x, y( x,, y( x wth a syetrc covarance atrx o the y( x easureents

More information

Special Relativity and Riemannian Geometry. Department of Mathematical Sciences

Special Relativity and Riemannian Geometry. Department of Mathematical Sciences Tutoral Letter 06//018 Specal Relatvty and Reannan Geoetry APM3713 Seester Departent of Matheatcal Scences IMPORTANT INFORMATION: Ths tutoral letter contans the solutons to Assgnent 06. BAR CODE Learn

More information

Bezier curves. Michael S. Floater. August 25, These notes provide an introduction to Bezier curves. i=0

Bezier curves. Michael S. Floater. August 25, These notes provide an introduction to Bezier curves. i=0 Bezer curves Mchael S. Floater August 25, 211 These notes provde an ntroducton to Bezer curves. 1 Bernsten polynomals Recall that a real polynomal of a real varable x R, wth degree n, s a functon of the

More information

Centroid Uncertainty Bounds for Interval Type-2 Fuzzy Sets: Forward and Inverse Problems

Centroid Uncertainty Bounds for Interval Type-2 Fuzzy Sets: Forward and Inverse Problems Centrod Uncertanty Bounds for Interval Type-2 Fuzzy Sets: Forward and Inverse Probles Jerry M. Mendel and Hongwe Wu Sgnal and Iage Processng Insttute Departent of Electrcal Engneerng Unversty of Southern

More information

ON THE NUMBER OF PRIMITIVE PYTHAGOREAN QUINTUPLES

ON THE NUMBER OF PRIMITIVE PYTHAGOREAN QUINTUPLES Journal of Algebra, Nuber Theory: Advances and Applcatons Volue 3, Nuber, 05, Pages 3-8 ON THE NUMBER OF PRIMITIVE PYTHAGOREAN QUINTUPLES Feldstrasse 45 CH-8004, Zürch Swtzerland e-al: whurlann@bluewn.ch

More information

Homework Notes Week 7

Homework Notes Week 7 Homework Notes Week 7 Math 4 Sprng 4 #4 (a Complete the proof n example 5 that s an nner product (the Frobenus nner product on M n n (F In the example propertes (a and (d have already been verfed so we

More information

Modified parallel multisplitting iterative methods for non-hermitian positive definite systems

Modified parallel multisplitting iterative methods for non-hermitian positive definite systems Adv Coput ath DOI 0.007/s0444-0-9262-8 odfed parallel ultsplttng teratve ethods for non-hertan postve defnte systes Chuan-Long Wang Guo-Yan eng Xue-Rong Yong Receved: Septeber 20 / Accepted: 4 Noveber

More information

1 Matrix representations of canonical matrices

1 Matrix representations of canonical matrices 1 Matrx representatons of canoncal matrces 2-d rotaton around the orgn: ( ) cos θ sn θ R 0 = sn θ cos θ 3-d rotaton around the x-axs: R x = 1 0 0 0 cos θ sn θ 0 sn θ cos θ 3-d rotaton around the y-axs:

More information

Linear Approximation with Regularization and Moving Least Squares

Linear Approximation with Regularization and Moving Least Squares Lnear Approxmaton wth Regularzaton and Movng Least Squares Igor Grešovn May 007 Revson 4.6 (Revson : March 004). 5 4 3 0.5 3 3.5 4 Contents: Lnear Fttng...4. Weghted Least Squares n Functon Approxmaton...

More information

,..., k N. , k 2. ,..., k i. The derivative with respect to temperature T is calculated by using the chain rule: & ( (5) dj j dt = "J j. k i.

,..., k N. , k 2. ,..., k i. The derivative with respect to temperature T is calculated by using the chain rule: & ( (5) dj j dt = J j. k i. Suppleentary Materal Dervaton of Eq. 1a. Assue j s a functon of the rate constants for the N coponent reactons: j j (k 1,,..., k,..., k N ( The dervatve wth respect to teperature T s calculated by usng

More information

On the number of regions in an m-dimensional space cut by n hyperplanes

On the number of regions in an m-dimensional space cut by n hyperplanes 6 On the nuber of regons n an -densonal space cut by n hyperplanes Chungwu Ho and Seth Zeran Abstract In ths note we provde a unfor approach for the nuber of bounded regons cut by n hyperplanes n general

More information

Numerical Solution of Ordinary Differential Equations

Numerical Solution of Ordinary Differential Equations Numercal Methods (CENG 00) CHAPTER-VI Numercal Soluton of Ordnar Dfferental Equatons 6 Introducton Dfferental equatons are equatons composed of an unknown functon and ts dervatves The followng are examples

More information

CHAPTER 7 CONSTRAINED OPTIMIZATION 1: THE KARUSH-KUHN-TUCKER CONDITIONS

CHAPTER 7 CONSTRAINED OPTIMIZATION 1: THE KARUSH-KUHN-TUCKER CONDITIONS CHAPER 7 CONSRAINED OPIMIZAION : HE KARUSH-KUHN-UCKER CONDIIONS 7. Introducton We now begn our dscusson of gradent-based constraned optzaton. Recall that n Chapter 3 we looked at gradent-based unconstraned

More information

, are assumed to fluctuate around zero, with E( i) 0. Now imagine that this overall random effect, , is composed of many independent factors,

, are assumed to fluctuate around zero, with E( i) 0. Now imagine that this overall random effect, , is composed of many independent factors, Part II. Contnuous Spatal Data Analyss 3. Spatally-Dependent Rando Effects Observe that all regressons n the llustratons above [startng wth expresson (..3) n the Sudan ranfall exaple] have reled on an

More information

Atmospheric Radiation Fall 2008

Atmospheric Radiation Fall 2008 MIT OpenCourseWare http://ocw.t.edu.85 Atospherc Radaton Fall 8 For nforaton about ctng these aterals or our Ters of Use, vst: http://ocw.t.edu/ters. .85, Atospherc Radaton Dr. Robert A. McClatchey and

More information

CHAPTER 5 NUMERICAL EVALUATION OF DYNAMIC RESPONSE

CHAPTER 5 NUMERICAL EVALUATION OF DYNAMIC RESPONSE CHAPTER 5 NUMERICAL EVALUATION OF DYNAMIC RESPONSE Analytcal soluton s usually not possble when exctaton vares arbtrarly wth tme or f the system s nonlnear. Such problems can be solved by numercal tmesteppng

More information

ANSWERS. Problem 1. and the moment generating function (mgf) by. defined for any real t. Use this to show that E( U) var( U)

ANSWERS. Problem 1. and the moment generating function (mgf) by. defined for any real t. Use this to show that E( U) var( U) Econ 413 Exam 13 H ANSWERS Settet er nndelt 9 deloppgaver, A,B,C, som alle anbefales å telle lkt for å gøre det ltt lettere å stå. Svar er gtt . Unfortunately, there s a prntng error n the hnt of

More information

Difference Equations

Difference Equations Dfference Equatons c Jan Vrbk 1 Bascs Suppose a sequence of numbers, say a 0,a 1,a,a 3,... s defned by a certan general relatonshp between, say, three consecutve values of the sequence, e.g. a + +3a +1

More information

LECTURE 9 CANONICAL CORRELATION ANALYSIS

LECTURE 9 CANONICAL CORRELATION ANALYSIS LECURE 9 CANONICAL CORRELAION ANALYSIS Introducton he concept of canoncal correlaton arses when we want to quantfy the assocatons between two sets of varables. For example, suppose that the frst set of

More information

Lecture 12: Discrete Laplacian

Lecture 12: Discrete Laplacian Lecture 12: Dscrete Laplacan Scrbe: Tanye Lu Our goal s to come up wth a dscrete verson of Laplacan operator for trangulated surfaces, so that we can use t n practce to solve related problems We are mostly

More information

Multipoint Analysis for Sibling Pairs. Biostatistics 666 Lecture 18

Multipoint Analysis for Sibling Pairs. Biostatistics 666 Lecture 18 Multpont Analyss for Sblng ars Bostatstcs 666 Lecture 8 revously Lnkage analyss wth pars of ndvduals Non-paraetrc BS Methods Maxu Lkelhood BD Based Method ossble Trangle Constrant AS Methods Covered So

More information

Small-Sample Equating With Prior Information

Small-Sample Equating With Prior Information Research Report Sall-Saple Equatng Wth Pror Inforaton Sauel A Lvngston Charles Lews June 009 ETS RR-09-5 Lstenng Learnng Leadng Sall-Saple Equatng Wth Pror Inforaton Sauel A Lvngston and Charles Lews ETS,

More information

Departure Process from a M/M/m/ Queue

Departure Process from a M/M/m/ Queue Dearture rocess fro a M/M// Queue Q - (-) Q Q3 Q4 (-) Knowledge of the nature of the dearture rocess fro a queue would be useful as we can then use t to analyze sle cases of queueng networs as shown. The

More information

Lecture 3. Camera Models 2 & Camera Calibration. Professor Silvio Savarese Computational Vision and Geometry Lab. 13- Jan- 15.

Lecture 3. Camera Models 2 & Camera Calibration. Professor Silvio Savarese Computational Vision and Geometry Lab. 13- Jan- 15. Lecture Caera Models Caera Calbraton rofessor Slvo Savarese Coputatonal Vson and Geoetry Lab Slvo Savarese Lecture - - Jan- 5 Lecture Caera Models Caera Calbraton Recap of caera odels Caera calbraton proble

More information

Xiangwen Li. March 8th and March 13th, 2001

Xiangwen Li. March 8th and March 13th, 2001 CS49I Approxaton Algorths The Vertex-Cover Proble Lecture Notes Xangwen L March 8th and March 3th, 00 Absolute Approxaton Gven an optzaton proble P, an algorth A s an approxaton algorth for P f, for an

More information

On the Calderón-Zygmund lemma for Sobolev functions

On the Calderón-Zygmund lemma for Sobolev functions arxv:0810.5029v1 [ath.ca] 28 Oct 2008 On the Calderón-Zygund lea for Sobolev functons Pascal Auscher october 16, 2008 Abstract We correct an naccuracy n the proof of a result n [Aus1]. 2000 MSC: 42B20,

More information

VERIFICATION OF FE MODELS FOR MODEL UPDATING

VERIFICATION OF FE MODELS FOR MODEL UPDATING VERIFICATION OF FE MODELS FOR MODEL UPDATING G. Chen and D. J. Ewns Dynacs Secton, Mechancal Engneerng Departent Iperal College of Scence, Technology and Medcne London SW7 AZ, Unted Kngdo Eal: g.chen@c.ac.uk

More information

Final Exam Solutions, 1998

Final Exam Solutions, 1998 58.439 Fnal Exa Solutons, 1998 roble 1 art a: Equlbru eans that the therodynac potental of a consttuent s the sae everywhere n a syste. An exaple s the Nernst potental. If the potental across a ebrane

More information

By M. O'Neill,* I. G. Sinclairf and Francis J. Smith

By M. O'Neill,* I. G. Sinclairf and Francis J. Smith 52 Polynoal curve fttng when abscssas and ordnates are both subject to error By M. O'Nell,* I. G. Snclarf and Francs J. Sth Departents of Coputer Scence and Appled Matheatcs, School of Physcs and Appled

More information

CHAPTER 6 CONSTRAINED OPTIMIZATION 1: K-T CONDITIONS

CHAPTER 6 CONSTRAINED OPTIMIZATION 1: K-T CONDITIONS Chapter 6: Constraned Optzaton CHAPER 6 CONSRAINED OPIMIZAION : K- CONDIIONS Introducton We now begn our dscusson of gradent-based constraned optzaton. Recall that n Chapter 3 we looked at gradent-based

More information

AN ANALYSIS OF A FRACTAL KINETICS CURVE OF SAVAGEAU

AN ANALYSIS OF A FRACTAL KINETICS CURVE OF SAVAGEAU AN ANALYI OF A FRACTAL KINETIC CURE OF AAGEAU by John Maloney and Jack Hedel Departent of Matheatcs Unversty of Nebraska at Oaha Oaha, Nebraska 688 Eal addresses: aloney@unoaha.edu, jhedel@unoaha.edu Runnng

More information

Chapter 7 Generalized and Weighted Least Squares Estimation. In this method, the deviation between the observed and expected values of

Chapter 7 Generalized and Weighted Least Squares Estimation. In this method, the deviation between the observed and expected values of Chapter 7 Generalzed and Weghted Least Squares Estmaton The usual lnear regresson model assumes that all the random error components are dentcally and ndependently dstrbuted wth constant varance. When

More information

Georgia Tech PHYS 6124 Mathematical Methods of Physics I

Georgia Tech PHYS 6124 Mathematical Methods of Physics I Georga Tech PHYS 624 Mathematcal Methods of Physcs I Instructor: Predrag Cvtanovć Fall semester 202 Homework Set #7 due October 30 202 == show all your work for maxmum credt == put labels ttle legends

More information

Solutions Homework 4 March 5, 2018

Solutions Homework 4 March 5, 2018 1 Solutons Homework 4 March 5, 018 Soluton to Exercse 5.1.8: Let a IR be a translaton and c > 0 be a re-scalng. ˆb1 (cx + a) cx n + a (cx 1 + a) c x n x 1 cˆb 1 (x), whch shows ˆb 1 s locaton nvarant and

More information

Chapter 12 Lyes KADEM [Thermodynamics II] 2007

Chapter 12 Lyes KADEM [Thermodynamics II] 2007 Chapter 2 Lyes KDEM [Therodynacs II] 2007 Gas Mxtures In ths chapter we wll develop ethods for deternng therodynac propertes of a xture n order to apply the frst law to systes nvolvng xtures. Ths wll be

More information

Revision: December 13, E Main Suite D Pullman, WA (509) Voice and Fax

Revision: December 13, E Main Suite D Pullman, WA (509) Voice and Fax .9.1: AC power analyss Reson: Deceber 13, 010 15 E Man Sute D Pullan, WA 99163 (509 334 6306 Voce and Fax Oerew n chapter.9.0, we ntroduced soe basc quanttes relate to delery of power usng snusodal sgnals.

More information

3.1 Expectation of Functions of Several Random Variables. )' be a k-dimensional discrete or continuous random vector, with joint PMF p (, E X E X1 E X

3.1 Expectation of Functions of Several Random Variables. )' be a k-dimensional discrete or continuous random vector, with joint PMF p (, E X E X1 E X Statstcs 1: Probablty Theory II 37 3 EPECTATION OF SEVERAL RANDOM VARIABLES As n Probablty Theory I, the nterest n most stuatons les not on the actual dstrbuton of a random vector, but rather on a number

More information

Salmon: Lectures on partial differential equations. Consider the general linear, second-order PDE in the form. ,x 2

Salmon: Lectures on partial differential equations. Consider the general linear, second-order PDE in the form. ,x 2 Salmon: Lectures on partal dfferental equatons 5. Classfcaton of second-order equatons There are general methods for classfyng hgher-order partal dfferental equatons. One s very general (applyng even to

More information

Description of the Force Method Procedure. Indeterminate Analysis Force Method 1. Force Method con t. Force Method con t

Description of the Force Method Procedure. Indeterminate Analysis Force Method 1. Force Method con t. Force Method con t Indeternate Analyss Force Method The force (flexblty) ethod expresses the relatonshps between dsplaceents and forces that exst n a structure. Prary objectve of the force ethod s to deterne the chosen set

More information

On the Eigenspectrum of the Gram Matrix and the Generalisation Error of Kernel PCA (Shawe-Taylor, et al. 2005) Ameet Talwalkar 02/13/07

On the Eigenspectrum of the Gram Matrix and the Generalisation Error of Kernel PCA (Shawe-Taylor, et al. 2005) Ameet Talwalkar 02/13/07 On the Egenspectru of the Gra Matr and the Generalsaton Error of Kernel PCA Shawe-aylor, et al. 005 Aeet alwalar 0/3/07 Outlne Bacground Motvaton PCA, MDS Isoap Kernel PCA Generalsaton Error of Kernel

More information

BAYESIAN AND NON BAYESIAN ESTIMATION OF ERLANG DISTRIBUTION UNDER PROGRESSIVE CENSORING

BAYESIAN AND NON BAYESIAN ESTIMATION OF ERLANG DISTRIBUTION UNDER PROGRESSIVE CENSORING www.arpapress.co/volues/volissue3/ijrras 3_8.pdf BAYESIAN AND NON BAYESIAN ESTIMATION OF ERLANG DISTRIBUTION UNDER PROGRESSIVE CENSORING R.A. Bakoban Departent of Statstcs, Scences Faculty for Grls, Kng

More information

Bernoulli Numbers and Polynomials

Bernoulli Numbers and Polynomials Bernoull Numbers and Polynomals T. Muthukumar tmk@tk.ac.n 17 Jun 2014 The sum of frst n natural numbers 1, 2, 3,..., n s n n(n + 1 S 1 (n := m = = n2 2 2 + n 2. Ths formula can be derved by notng that

More information

THE ADJACENCY-PELL-HURWITZ NUMBERS. Josh Hiller Department of Mathematics and Computer Science, Adelpi University, New York

THE ADJACENCY-PELL-HURWITZ NUMBERS. Josh Hiller Department of Mathematics and Computer Science, Adelpi University, New York #A8 INTEGERS 8 (8) THE ADJACENCY-PELL-HURWITZ NUMBERS Josh Hller Departent of Matheatcs and Coputer Scence Adelp Unversty New York johller@adelphedu Yeş Aküzü Faculty of Scence and Letters Kafkas Unversty

More information

Lecture 3: Probability Distributions

Lecture 3: Probability Distributions Lecture 3: Probablty Dstrbutons Random Varables Let us begn by defnng a sample space as a set of outcomes from an experment. We denote ths by S. A random varable s a functon whch maps outcomes nto the

More information

An Optimal Bound for Sum of Square Roots of Special Type of Integers

An Optimal Bound for Sum of Square Roots of Special Type of Integers The Sxth Internatonal Syposu on Operatons Research and Its Applcatons ISORA 06 Xnang, Chna, August 8 12, 2006 Copyrght 2006 ORSC & APORC pp. 206 211 An Optal Bound for Su of Square Roots of Specal Type

More information

CIS526: Machine Learning Lecture 3 (Sept 16, 2003) Linear Regression. Preparation help: Xiaoying Huang. x 1 θ 1 output... θ M x M

CIS526: Machine Learning Lecture 3 (Sept 16, 2003) Linear Regression. Preparation help: Xiaoying Huang. x 1 θ 1 output... θ M x M CIS56: achne Learnng Lecture 3 (Sept 6, 003) Preparaton help: Xaoyng Huang Lnear Regresson Lnear regresson can be represented by a functonal form: f(; θ) = θ 0 0 +θ + + θ = θ = 0 ote: 0 s a dummy attrbute

More information

Econ107 Applied Econometrics Topic 3: Classical Model (Studenmund, Chapter 4)

Econ107 Applied Econometrics Topic 3: Classical Model (Studenmund, Chapter 4) I. Classcal Assumptons Econ7 Appled Econometrcs Topc 3: Classcal Model (Studenmund, Chapter 4) We have defned OLS and studed some algebrac propertes of OLS. In ths topc we wll study statstcal propertes

More information

Calculus of Variations Basics

Calculus of Variations Basics Chapter 1 Calculus of Varatons Bascs 1.1 Varaton of a General Functonal In ths chapter, we derve the general formula for the varaton of a functonal of the form J [y 1,y 2,,y n ] F x,y 1,y 2,,y n,y 1,y

More information

Computational and Statistical Learning theory Assignment 4

Computational and Statistical Learning theory Assignment 4 Coputatonal and Statstcal Learnng theory Assgnent 4 Due: March 2nd Eal solutons to : karthk at ttc dot edu Notatons/Defntons Recall the defnton of saple based Radeacher coplexty : [ ] R S F) := E ɛ {±}

More information

Chapter 1. Theory of Gravitation

Chapter 1. Theory of Gravitation Chapter 1 Theory of Gravtaton In ths chapter a theory of gravtaton n flat space-te s studed whch was consdered n several artcles by the author. Let us assue a flat space-te etrc. Denote by x the co-ordnates

More information

Maximum Likelihood Estimation of Binary Dependent Variables Models: Probit and Logit. 1. General Formulation of Binary Dependent Variables Models

Maximum Likelihood Estimation of Binary Dependent Variables Models: Probit and Logit. 1. General Formulation of Binary Dependent Variables Models ECO 452 -- OE 4: Probt and Logt Models ECO 452 -- OE 4 Maxmum Lkelhood Estmaton of Bnary Dependent Varables Models: Probt and Logt hs note demonstrates how to formulate bnary dependent varables models

More information

On the Transient and Steady-State Analysis of a Special Single Server Queuing System with HOL Priority Scheduling

On the Transient and Steady-State Analysis of a Special Single Server Queuing System with HOL Priority Scheduling 96 On the Transent and Steady-State Analyss of a Specal On the Transent and Steady-State Analyss of a Specal Sngle Server Queung Syste wth HOL Prorty Schedulng Faou Kaoun Duba Uversty College, College

More information

Economics 130. Lecture 4 Simple Linear Regression Continued

Economics 130. Lecture 4 Simple Linear Regression Continued Economcs 130 Lecture 4 Contnued Readngs for Week 4 Text, Chapter and 3. We contnue wth addressng our second ssue + add n how we evaluate these relatonshps: Where do we get data to do ths analyss? How do

More information

EXACT TRAVELLING WAVE SOLUTIONS FOR THREE NONLINEAR EVOLUTION EQUATIONS BY A BERNOULLI SUB-ODE METHOD

EXACT TRAVELLING WAVE SOLUTIONS FOR THREE NONLINEAR EVOLUTION EQUATIONS BY A BERNOULLI SUB-ODE METHOD www.arpapress.co/volues/vol16issue/ijrras_16 10.pdf EXACT TRAVELLING WAVE SOLUTIONS FOR THREE NONLINEAR EVOLUTION EQUATIONS BY A BERNOULLI SUB-ODE METHOD Chengbo Tan & Qnghua Feng * School of Scence, Shandong

More information

14 The Postulates of Quantum mechanics

14 The Postulates of Quantum mechanics 14 The Postulates of Quantum mechancs Postulate 1: The state of a system s descrbed completely n terms of a state vector Ψ(r, t), whch s quadratcally ntegrable. Postulate 2: To every physcally observable

More information

1.3 Hence, calculate a formula for the force required to break the bond (i.e. the maximum value of F)

1.3 Hence, calculate a formula for the force required to break the bond (i.e. the maximum value of F) EN40: Dynacs and Vbratons Hoework 4: Work, Energy and Lnear Moentu Due Frday March 6 th School of Engneerng Brown Unversty 1. The Rydberg potental s a sple odel of atoc nteractons. It specfes the potental

More information

Lecture 19. Endogenous Regressors and Instrumental Variables

Lecture 19. Endogenous Regressors and Instrumental Variables Lecture 19. Endogenous Regressors and Instrumental Varables In the prevous lecture we consder a regresson model (I omt the subscrpts (1) Y β + D + u = 1 β The problem s that the dummy varable D s endogenous,.e.

More information

Modelli Clamfim Equazione del Calore Lezione ottobre 2014

Modelli Clamfim Equazione del Calore Lezione ottobre 2014 CLAMFIM Bologna Modell 1 @ Clamfm Equazone del Calore Lezone 17 15 ottobre 2014 professor Danele Rtell danele.rtell@unbo.t 1/24? Convoluton The convoluton of two functons g(t) and f(t) s the functon (g

More information

Designing Fuzzy Time Series Model Using Generalized Wang s Method and Its application to Forecasting Interest Rate of Bank Indonesia Certificate

Designing Fuzzy Time Series Model Using Generalized Wang s Method and Its application to Forecasting Interest Rate of Bank Indonesia Certificate The Frst Internatonal Senar on Scence and Technology, Islac Unversty of Indonesa, 4-5 January 009. Desgnng Fuzzy Te Seres odel Usng Generalzed Wang s ethod and Its applcaton to Forecastng Interest Rate

More information

Limited Dependent Variables

Limited Dependent Variables Lmted Dependent Varables. What f the left-hand sde varable s not a contnuous thng spread from mnus nfnty to plus nfnty? That s, gven a model = f (, β, ε, where a. s bounded below at zero, such as wages

More information

ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM

ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM An elastc wave s a deformaton of the body that travels throughout the body n all drectons. We can examne the deformaton over a perod of tme by fxng our look

More information

Implicit scaling of linear least squares problems

Implicit scaling of linear least squares problems RAL-TR-98-07 1 Iplct scalng of lnear least squares probles by J. K. Red Abstract We consder the soluton of weghted lnear least squares probles by Householder transforatons wth plct scalng, that s, wth

More information

First Year Examination Department of Statistics, University of Florida

First Year Examination Department of Statistics, University of Florida Frst Year Examnaton Department of Statstcs, Unversty of Florda May 7, 010, 8:00 am - 1:00 noon Instructons: 1. You have four hours to answer questons n ths examnaton.. You must show your work to receve

More information

Statistical Inference. 2.3 Summary Statistics Measures of Center and Spread. parameters ( population characteristics )

Statistical Inference. 2.3 Summary Statistics Measures of Center and Spread. parameters ( population characteristics ) Ismor Fscher, 8//008 Stat 54 / -8.3 Summary Statstcs Measures of Center and Spread Dstrbuton of dscrete contnuous POPULATION Random Varable, numercal True center =??? True spread =???? parameters ( populaton

More information

Elastic Collisions. Definition: two point masses on which no external forces act collide without losing any energy.

Elastic Collisions. Definition: two point masses on which no external forces act collide without losing any energy. Elastc Collsons Defnton: to pont asses on hch no external forces act collde thout losng any energy v Prerequstes: θ θ collsons n one denson conservaton of oentu and energy occurs frequently n everyday

More information

International Journal of Mathematical Archive-9(3), 2018, Available online through ISSN

International Journal of Mathematical Archive-9(3), 2018, Available online through   ISSN Internatonal Journal of Matheatcal Archve-9(3), 208, 20-24 Avalable onlne through www.ja.nfo ISSN 2229 5046 CONSTRUCTION OF BALANCED INCOMPLETE BLOCK DESIGNS T. SHEKAR GOUD, JAGAN MOHAN RAO M AND N.CH.

More information

Approximate Technique for Solving Class of Fractional Variational Problems

Approximate Technique for Solving Class of Fractional Variational Problems Appled Matheatcs, 5, 6, 837-846 Publshed Onlne May 5 n ScRes. http://www.scrp.org/journal/a http://dx.do.org/.436/a.5.6578 Approxate Technque for Solvng Class of Fractonal Varatonal Probles Ead M. Soloua,,

More information