LECTURE 4 : ARMA PROCESSES
|
|
- Ἀπολλωνία Κουρμούλης
- 7 χρόνια πριν
- Προβολές:
Transcript
1 LECTURE 4 : ARMA PROCESSES Movng-Average Processes The MA(q) process, s defned by (53) y(t) =µ ε(t)+µ 1 ε(t 1) + +µ q ε(t q) =µ(l)ε(t), where µ(l) =µ +µ 1 L+ +µ q L q and where ε(t) s whte nose An MA model should be nvertble such that µ 1 (L)y(t) =ε(t) Ths AR( ) representaton s s avalable f and only f all the roots of µ(z) =le outsde the unt crcle Example Consder the MA(1) process (54) y(t) =ε(t) θε(t 1)=(1 θl)ε(t) Provded that θ < 1, ths can be wrtten n autoregressve form as (55) ε(t) =(1 θl) 1 y(t) = { y(t)+θy(t 1) + θ y(t ) + } Imagne that θ > 1 nstead Then we have to wrte (56) y(t +1)=ε(t+1) θε(t) = θ(1 L 1 /θ)ε(t), where L 1 ε(t) =ε(t+ 1) Ths gves (57) ε(t) = θ 1 (1 L 1 /θ) 1 y(t +1) = θ 1{ y(t+1)/θ + y(t +)/θ + y(t 3)/θ 3 + } Normally, an expresson such as ths, whch embodes future values of y(t), would have no reasonable meanng 1
2 DSG POLLOCK : LECTURES IN THE CITY 4 The Autocovarances of an MA Process Consder (58) γ τ = E(y t y t τ ) { } = E µ ε t µ ε t τ = µ µ E(ε t ε t τ ) Snce ε(t) s whte nose, t follows that {, f τ + ; (59) E(ε t ε t τ )= σε, f = τ + Therefore (51) γ τ = σε µ µ +τ Now let τ =,1,,q Ths gves (511) γ = σε(µ + µ 1 + +µ q), γ 1 =σε(µ µ 1 +µ 1 µ + +µ q 1 µ q ), γ q =σ εµ µ q Also, γ τ = for all τ>q Example The MA(1) process y(t) = ε(t) θε(t 1) has (51) γ = σε(1 + θ ), γ 1 = σεθ, γ τ = f τ>1 Thus the dsperson matrx of y =[y 1,y,,y T ] s 1+θ θ θ 1+θ θ (513) D(y) =σε θ 1+θ 1+θ
3 LECTURE 4 : ARMA PROCESSES Autocovarance Generatng Functon Ths s denoted by (514) γ(z) = τ γ τ z τ ; wth τ = {, ±1, ±,} and γ τ = γ τ To fnd the autocovarance generatng functon of the MA(q) process, consder µ(z)µ(z 1 )= µ z µ z (515) From (1) t follows that = = τ µ µ z ( µ µ +τ )z τ, τ = (516) γ(z) =σ εµ(z)µ(z 1 ) 3
4 DSG POLLOCK : LECTURES IN THE CITY 4 Autoregressve Processes The AR(p) process, s defned by (517) α y(t)+α 1 y(t 1) + +α p y(t p)=ε(t) Ths can be wrtten as α(l)y(t) =ε(t), where α(l) =α +α 1 L+ +α p L p For the process to be statonary, the roots of α(z) = must le outsde the unt crcle In that case the AR process can be wrtten as an MA( ) process: y(t) =α 1 (L)ε(t) The autocovarance generatng functon for the AR(p) process s (53) γ(z) = σ ε α(z)α(z 1 ) Example Consder the AR(1) process defned by ε(t) =y(t) φy(t 1) (518) =(1 φl)y(t) Provded that φ < 1, ths can be represented n MA form as y(t) =(1 φl) 1 ε(t) (519) = { ε(t)+φε(t 1) + φ ε(t ) + } The autocovarances of the AR(1) process can be obtaned va the formula (1) for the autocovarances of an MA process Thus (5) and t follows from (9) that γ τ = E(y t y t τ ) { } = E φ ε t φ ε t τ = φ φ E(ε t ε t τ ); γ τ = σε φ φ +τ (51) = σ εφ τ 1 φ The dsperson matrx of y =[y 1,y,,y T ] s (5) D(y) = σ ε 1 φ 1 φ φ φ T 1 φ 1 φ φ T φ φ 1 φ T 3 φ T 1 φ T φ T 3 1 4
5 The Yule-Walker Equatons LECTURE 4 : ARMA PROCESSES For an alternatve way of fndng the AR autocovarances, consder multplyng α y t = ε t by y t τ and takng expectatons to gve (54) α E(y t y t τ )=E(ε t y t τ ) Gven that α = 1, t follows that { σ ε, f τ =; (55) E(ε t y t τ )=, f τ> Therefore, on settng E(y t y t τ )=γ τ, equaton (4) gves { σ ε, f τ =; (56) α γ τ =, f τ> The second of these s a homogeneous dfference equaton whch enables us to generate the sequence {γ p,γ p+1,} once p startng values γ,γ 1,,γ p 1 are known By lettng τ =,1,,p n (6), we generate a set of p + 1 equatons whch can be arrayed n matrx form as follows: (57) γ γ 1 γ γ p 1 γ 1 γ γ 1 γ p 1 α 1 γ γ 1 γ γ p α = γ p γ p 1 γ p γ α p These are called the Yule Walker equatons, and they can be used ether for generatng the values γ,γ 1,,γ p from the values α 1,,α p,σ ε or vce versa Example Consder the second-order autoregressve process We have γ γ 1 γ γ 1 γ γ 1 α α 1 = α γ α 1 α γ α α 1 α 1 γ γ γ 1 γ α α α 1 α γ 1 (58) γ = α α 1 α α 1 α +α γ γ 1 = σ ε α α 1 α γ Gven α = 1 and the values for γ,γ 1,γ, we can fnd σ ε and α 1,α Conversely, gven α,α 1,α and σ ε, we can fnd γ,γ 1,γ 5 σ ε
6 DSG POLLOCK : LECTURES IN THE CITY 4 The Partal Autocorrelaton Functon Let α r(r) be the coeffcent assocated wth y(t r) n an autoregressve process of order r whose parameters correspond to the autocovarances γ,γ 1,,γ r Then the sequence {α r(r) ; r =1,,}of such coeffcents, whose ndex corresponds to models of ncreasng orders, consttutes the partal autocorrelaton functon In effect, α r(r) ndcates the role n explanng the varance of y(t) whch s due to y(t r) when y(t 1),,y(t r+ 1) are also taken nto account The sequence of partal autocorrelatons may be computed effcently va the recursve Durbn Levnson Algorthm whch uses the coeffcents of the AR model of order r as the bass for calculatng the coeffcents of the model of order r +1 Imagne that we already have the values α (r) =1,α 1(r),,α r(r) Then, by extendng the set of rth-order Yule Walker equatons to whch these values correspond, we can derve the system γ γ 1 γ r γ r+1 1 σ (r) γ 1 γ γ r 1 γ r (59) α 1(r) = γ r γ r 1 γ γ 1 α r(r), γ r+1 γ r γ 1 γ g wheren (53) g = r α (r) γ r+1 wth α (r) =1 = The system can also be wrtten as γ γ 1 γ r γ r+1 γ 1 γ γ r 1 γ r (531) α r(r) γ r γ r 1 γ γ 1 α 1(r) γ r+1 γ r γ 1 γ 1 = g σ (r) The two systems of equatons (9) and (31) can be combned to gve γ γ 1 γ r γ r+1 1 σ(r) γ 1 γ γ r 1 γ r (53) α 1(r) + cα r(r) + cg = γ r γ r 1 γ γ 1 α r(r) + cα 1(r) γ r+1 γ r γ 1 γ c g + cσ(r) 6
7 LECTURE 4 : ARMA PROCESSES If we take the coeffcent of the combnaton to be (533) c = g σ(r), then the fnal element n the vector on the RHS becomes zero and the system becomes the set of Yule Walker equatons of order r + 1 The soluton of the equatons, from the last element α r+1(r+1) = c through to the varance term σ(r+1) s gven by (534) α r+1(r+1) = 1 { r } σ(r) α (r) γ r+1 = α 1(r+1) α r(r+1) = α 1(r) α r(r) + α r+1(r+1) α r(r) α 1(r) σ (r+1) = σ (r){ 1 (αr+1(r+1) ) } Thus the soluton of the Yule Walker system of order r + 1 s easly derved from the soluton of the system of order r, and there s scope for devsng a recursve procedure The startng values for the recurson are (535) α 1(1) = γ 1 /γ and σ (1) = γ { 1 (α1(1) ) } 7
8 DSG POLLOCK : LECTURES IN THE CITY 4 Autoregressve Movng Average Processes The ARMA(p, q) process, s defned by (536) α y(t)+α 1 y(t 1) + +α p y(t p) =µ ε(t)+µ 1 ε(t 1) + +µ q ε(t q) Ths can also be wrtten as α(l)y(t) =µ(l)ε(t) If the roots of α(z) = le outsde the unt crcle, then the process has an MA( ) form: y(t) = α 1 (L)µ(L)ε(t) If the roots of µ(z) = le outsde the unt crcle, then t has an AR( ) form: µ 1 (L)α(L)y(t) =ε(t) The autocovarance generatng functon for the ARMA process s (537) γ(z) =σ ε µ(z)µ(z 1 ) α(z)α(z 1 ) To fnd the autocovarances n practce, consder multplyng the equaton α y t = µ ε t by y t τ and takng expectatons Ths gves (538) α γ τ = µ δ τ, where γ τ = E(y t τ y t ) and δ τ = E(y t τ ε t ) Snce ε t s uncorrelated wth y t τ whenever t s subsequent to the latter, t follows that δ τ =f τ> Snce the ndex n the RHS of the equaton (38) runs from to q, t follows that (539) α γ τ = f τ>q Gven the q+1 nonzero values δ,δ 1,,δ q, and p ntal values γ,γ 1,,γ p 1, the equatons can be solved recursvely for {γ p,γ p+1,} To fnd the requste values δ,δ 1,,δ q, consder multplyng the equaton α y t = µ ε t by ε t τ and takng expectatons Ths gves (54) α δ τ = µ τ σε, where δ τ = E(y t ε t τ ) The equaton may be rewrtten as (541) δ τ = 1 ( µ τ σε δ τ ), α =1 and, by settng τ =,1,,q, we can generate recursvely the requred values δ,δ 1,,δ q 8
9 LECTURE 4 : ARMA PROCESSES Example Consder the ARMA(, ) model whch gves the equaton (54) α y t + α 1 y t 1 + α y t = µ ε t + µ 1 ε t 1 + µ ε t Multplyng by y t, y t 1 and y t and takng expectatons gves (543) γ γ 1 γ γ 1 γ γ 1 α α 1 = δ δ 1 δ δ δ 1 µ µ 1 γ γ 1 γ α δ µ Multplyng by ε t, ε t 1 and ε t and takng expectatons gves (544) δ δ 1 δ α α 1 = σ ε σε µ µ 1 δ δ 1 δ α σε µ When the latter equatons are wrtten as (545) α α 1 α δ δ 1 = σ µ ε µ 1, α α 1 α δ µ they can be solved recursvely for δ, δ 1 and δ on the assumpton that that the values of α, α 1, α and σε are known Notce that, when we adopt the normalsaton α = µ = 1, we get δ = σε When the equatons (43) are rewrtten as (546) α α 1 α α 1 α + α γ γ 1 = µ µ 1 µ µ 1 µ δ δ 1, α α 1 α γ µ δ they can be solved for γ, γ 1 and γ Thus the startng values are obtaned whch enable the equaton (547) α γ τ + α 1 γ τ 1 + α γ τ =; τ> to be solved recursvely to generate the succeedng values {γ 3, γ 4,} of the autocovarances 9
α & β spatial orbitals in
The atrx Hartree-Fock equatons The most common method of solvng the Hartree-Fock equatons f the spatal btals s to expand them n terms of known functons, { χ µ } µ= consder the spn-unrestrcted case. We
Πανεπιστήµιο Κρήτης - Τµήµα Επιστήµης Υπολογιστών. ΗΥ-570: Στατιστική Επεξεργασία Σήµατος. ιδάσκων : Α. Μουχτάρης. εύτερη Σειρά Ασκήσεων.
Πανεπιστήµιο Κρήτης - Τµήµα Επιστήµης Υπολογιστών ΗΥ-570: Στατιστική Επεξεργασία Σήµατος 2015 ιδάσκων : Α. Μουχτάρης εύτερη Σειρά Ασκήσεων Λύσεις Ασκηση 1. 1. Consder the gven expresson for R 1/2 : R 1/2
One and two particle density matrices for single determinant HF wavefunctions. (1) = φ 2. )β(1) ( ) ) + β(1)β * β. (1)ρ RHF
One and two partcle densty matrces for sngle determnant HF wavefunctons One partcle densty matrx Gven the Hartree-Fock wavefuncton ψ (,,3,!, = Âϕ (ϕ (ϕ (3!ϕ ( 3 The electronc energy s ψ H ψ = ϕ ( f ( ϕ
Multi-dimensional Central Limit Theorem
Mult-dmensonal Central Lmt heorem Outlne () () () t as () + () + + () () () Consder a sequence of ndependent random proceses t, t, dentcal to some ( t). Assume t 0. Defne the sum process t t t t () t tme
Multi-dimensional Central Limit Theorem
Mult-dmensonal Central Lmt heorem Outlne () () () t as () + () + + () () () Consder a sequence of ndependent random proceses t, t, dentcal to some ( t). Assume t 0. Defne the sum process t t t t () t ();
A Class of Orthohomological Triangles
A Class of Orthohomologcal Trangles Prof. Claudu Coandă Natonal College Carol I Craova Romana. Prof. Florentn Smarandache Unversty of New Mexco Gallup USA Prof. Ion Pătraşcu Natonal College Fraţ Buzeşt
Finite Field Problems: Solutions
Finite Field Problems: Solutions 1. Let f = x 2 +1 Z 11 [x] and let F = Z 11 [x]/(f), a field. Let Solution: F =11 2 = 121, so F = 121 1 = 120. The possible orders are the divisors of 120. Solution: The
6.3 Forecasting ARMA processes
122 CHAPTER 6. ARMA MODELS 6.3 Forecasting ARMA processes The purpose of forecasting is to predict future values of a TS based on the data collected to the present. In this section we will discuss a linear
1 Complete Set of Grassmann States
Physcs 610 Homework 8 Solutons 1 Complete Set of Grassmann States For Θ, Θ, Θ, Θ each ndependent n-member sets of Grassmann varables, and usng the summaton conventon ΘΘ Θ Θ Θ Θ, prove the dentty e ΘΘ dθ
EE512: Error Control Coding
EE512: Error Control Coding Solution for Assignment on Finite Fields February 16, 2007 1. (a) Addition and Multiplication tables for GF (5) and GF (7) are shown in Tables 1 and 2. + 0 1 2 3 4 0 0 1 2 3
4.6 Autoregressive Moving Average Model ARMA(1,1)
84 CHAPTER 4. STATIONARY TS MODELS 4.6 Autoregressive Moving Average Model ARMA(,) This section is an introduction to a wide class of models ARMA(p,q) which we will consider in more detail later in this
CHAPTER 25 SOLVING EQUATIONS BY ITERATIVE METHODS
CHAPTER 5 SOLVING EQUATIONS BY ITERATIVE METHODS EXERCISE 104 Page 8 1. Find the positive root of the equation x + 3x 5 = 0, correct to 3 significant figures, using the method of bisection. Let f(x) =
Example Sheet 3 Solutions
Example Sheet 3 Solutions. i Regular Sturm-Liouville. ii Singular Sturm-Liouville mixed boundary conditions. iii Not Sturm-Liouville ODE is not in Sturm-Liouville form. iv Regular Sturm-Liouville note
8.1 The Nature of Heteroskedasticity 8.2 Using the Least Squares Estimator 8.3 The Generalized Least Squares Estimator 8.
8.1 The Nature of Heteroskedastcty 8. Usng the Least Squares Estmator 8.3 The Generalzed Least Squares Estmator 8.4 Detectng Heteroskedastcty E( y) = β+β 1 x e = y E( y ) = y β β x 1 y = β+β x + e 1 Fgure
8.324 Relativistic Quantum Field Theory II
Lecture 8.3 Relatvstc Quantum Feld Theory II Fall 00 8.3 Relatvstc Quantum Feld Theory II MIT OpenCourseWare Lecture Notes Hon Lu, Fall 00 Lecture 5.: RENORMALIZATION GROUP FLOW Consder the bare acton
Ordinal Arithmetic: Addition, Multiplication, Exponentiation and Limit
Ordinal Arithmetic: Addition, Multiplication, Exponentiation and Limit Ting Zhang Stanford May 11, 2001 Stanford, 5/11/2001 1 Outline Ordinal Classification Ordinal Addition Ordinal Multiplication Ordinal
Variance of Trait in an Inbred Population. Variance of Trait in an Inbred Population
Varance of Trat n an Inbred Populaton Varance of Trat n an Inbred Populaton Varance of Trat n an Inbred Populaton Revew of Mean Trat Value n Inbred Populatons We showed n the last lecture that for a populaton
C.S. 430 Assignment 6, Sample Solutions
C.S. 430 Assignment 6, Sample Solutions Paul Liu November 15, 2007 Note that these are sample solutions only; in many cases there were many acceptable answers. 1 Reynolds Problem 10.1 1.1 Normal-order
ΗΥ537: Έλεγχος Πόρων και Επίδοση σε Ευρυζωνικά Δίκτυα,
ΗΥ537: Έλεγχος Πόρων και Επίδοση σε Ευρυζωνικά Δίκτυα Βασίλειος Σύρης Τμήμα Επιστήμης Υπολογιστών Πανεπιστήμιο Κρήτης Εαρινό εξάμηνο 2008 Economcs Contents The contet The basc model user utlty, rces and
Concrete Mathematics Exercises from 30 September 2016
Concrete Mathematics Exercises from 30 September 2016 Silvio Capobianco Exercise 1.7 Let H(n) = J(n + 1) J(n). Equation (1.8) tells us that H(2n) = 2, and H(2n+1) = J(2n+2) J(2n+1) = (2J(n+1) 1) (2J(n)+1)
Introduction to the ML Estimation of ARMA processes
Introduction to the ML Estimation of ARMA processes Eduardo Rossi University of Pavia October 2013 Rossi ARMA Estimation Financial Econometrics - 2013 1 / 1 We consider the AR(p) model: Y t = c + φ 1 Y
Solutions for Mathematical Physics 1 (Dated: April 19, 2015)
Solutons for Mathematcal Physcs 1 Dated: Aprl 19, 215 3.2.3 Usng the vectors P ê x cos θ + ê y sn θ, Q ê x cos ϕ ê y sn ϕ, R ê x cos ϕ ê y sn ϕ, 1 prove the famlar trgonometrc denttes snθ + ϕ sn θ cos
Matrices and Determinants
Matrices and Determinants SUBJECTIVE PROBLEMS: Q 1. For what value of k do the following system of equations possess a non-trivial (i.e., not all zero) solution over the set of rationals Q? x + ky + 3z
2 Composition. Invertible Mappings
Arkansas Tech University MATH 4033: Elementary Modern Algebra Dr. Marcel B. Finan Composition. Invertible Mappings In this section we discuss two procedures for creating new mappings from old ones, namely,
Lecture 2: Dirac notation and a review of linear algebra Read Sakurai chapter 1, Baym chatper 3
Lecture 2: Dirac notation and a review of linear algebra Read Sakurai chapter 1, Baym chatper 3 1 State vector space and the dual space Space of wavefunctions The space of wavefunctions is the set of all
LECTURE 2 : MODELS AND METHODS. Time-Series Models: Feedback Form and Transfer-Function Form
LECTURE 2 : MODELS AND METHODS Time-Series Models: Feedback Form and Transfer-Function Form A dynamic regression model is a relationship comprising any number of consecutive elements of x(t), y(t) and
The challenges of non-stable predicates
The challenges of non-stable predicates Consider a non-stable predicate Φ encoding, say, a safety property. We want to determine whether Φ holds for our program. The challenges of non-stable predicates
The Simply Typed Lambda Calculus
Type Inference Instead of writing type annotations, can we use an algorithm to infer what the type annotations should be? That depends on the type system. For simple type systems the answer is yes, and
Every set of first-order formulas is equivalent to an independent set
Every set of first-order formulas is equivalent to an independent set May 6, 2008 Abstract A set of first-order formulas, whatever the cardinality of the set of symbols, is equivalent to an independent
Solution Series 9. i=1 x i and i=1 x i.
Lecturer: Prof. Dr. Mete SONER Coordinator: Yilin WANG Solution Series 9 Q1. Let α, β >, the p.d.f. of a beta distribution with parameters α and β is { Γ(α+β) Γ(α)Γ(β) f(x α, β) xα 1 (1 x) β 1 for < x
Lecture 15 - Root System Axiomatics
Lecture 15 - Root System Axiomatics Nov 1, 01 In this lecture we examine root systems from an axiomatic point of view. 1 Reflections If v R n, then it determines a hyperplane, denoted P v, through the
Symplecticity of the Störmer-Verlet algorithm for coupling between the shallow water equations and horizontal vehicle motion
Symplectcty of the Störmer-Verlet algorthm for couplng between the shallow water equatons and horzontal vehcle moton by H. Alem Ardakan & T. J. Brdges Department of Mathematcs, Unversty of Surrey, Guldford
Απόκριση σε Μοναδιαία Ωστική Δύναμη (Unit Impulse) Απόκριση σε Δυνάμεις Αυθαίρετα Μεταβαλλόμενες με το Χρόνο. Απόστολος Σ.
Απόκριση σε Δυνάμεις Αυθαίρετα Μεταβαλλόμενες με το Χρόνο The time integral of a force is referred to as impulse, is determined by and is obtained from: Newton s 2 nd Law of motion states that the action
Duals of the QCQP and SDP Sparse SVM. Antoni B. Chan, Nuno Vasconcelos, and Gert R. G. Lanckriet
Duals of the QCQP and SDP Sparse SVM Anton B. Chan, Nuno Vasconcelos, and Gert R. G. Lanckret SVCL-TR 007-0 v Aprl 007 Duals of the QCQP and SDP Sparse SVM Anton B. Chan, Nuno Vasconcelos, and Gert R.
Phasor Diagram of an RC Circuit V R
ESE Lecture 3 Phasor Dagram of an rcut VtV m snt V t V o t urrent s a reference n seres crcut KVL: V m V + V V ϕ I m V V m ESE Lecture 3 Phasor Dagram of an L rcut VtV m snt V t V t L V o t KVL: V m V
Homework 3 Solutions
Homework 3 Solutions Igor Yanovsky (Math 151A TA) Problem 1: Compute the absolute error and relative error in approximations of p by p. (Use calculator!) a) p π, p 22/7; b) p π, p 3.141. Solution: For
forms This gives Remark 1. How to remember the above formulas: Substituting these into the equation we obtain with
Week 03: C lassification of S econd- Order L inear Equations In last week s lectures we have illustrated how to obtain the general solutions of first order PDEs using the method of characteristics. We
Chapter 6: Systems of Linear Differential. be continuous functions on the interval
Chapter 6: Systems of Linear Differential Equations Let a (t), a 2 (t),..., a nn (t), b (t), b 2 (t),..., b n (t) be continuous functions on the interval I. The system of n first-order differential equations
Lecture 26: Circular domains
Introductory lecture notes on Partial Differential Equations - c Anthony Peirce. Not to be copied, used, or revised without eplicit written permission from the copyright owner. 1 Lecture 6: Circular domains
Second Order Partial Differential Equations
Chapter 7 Second Order Partial Differential Equations 7.1 Introduction A second order linear PDE in two independent variables (x, y Ω can be written as A(x, y u x + B(x, y u xy + C(x, y u u u + D(x, y
HOMEWORK 4 = G. In order to plot the stress versus the stretch we define a normalized stretch:
HOMEWORK 4 Problem a For the fast loading case, we want to derive the relationship between P zz and λ z. We know that the nominal stress is expressed as: P zz = ψ λ z where λ z = λ λ z. Therefore, applying
Estimators when the Correlation Coefficient. is Negative
It J Cotemp Math Sceces, Vol 5, 00, o 3, 45-50 Estmators whe the Correlato Coeffcet s Negatve Sad Al Al-Hadhram College of Appled Sceces, Nzwa, Oma abur97@ahoocouk Abstract Rato estmators for the mea of
Other Test Constructions: Likelihood Ratio & Bayes Tests
Other Test Constructions: Likelihood Ratio & Bayes Tests Side-Note: So far we have seen a few approaches for creating tests such as Neyman-Pearson Lemma ( most powerful tests of H 0 : θ = θ 0 vs H 1 :
SCHOOL OF MATHEMATICAL SCIENCES G11LMA Linear Mathematics Examination Solutions
SCHOOL OF MATHEMATICAL SCIENCES GLMA Linear Mathematics 00- Examination Solutions. (a) i. ( + 5i)( i) = (6 + 5) + (5 )i = + i. Real part is, imaginary part is. (b) ii. + 5i i ( + 5i)( + i) = ( i)( + i)
Exercises 10. Find a fundamental matrix of the given system of equations. Also find the fundamental matrix Φ(t) satisfying Φ(0) = I. 1.
Exercises 0 More exercises are available in Elementary Differential Equations. If you have a problem to solve any of them, feel free to come to office hour. Problem Find a fundamental matrix of the given
derivation of the Laplacian from rectangular to spherical coordinates
derivation of the Laplacian from rectangular to spherical coordinates swapnizzle 03-03- :5:43 We begin by recognizing the familiar conversion from rectangular to spherical coordinates (note that φ is used
HW 3 Solutions 1. a) I use the auto.arima R function to search over models using AIC and decide on an ARMA(3,1)
HW 3 Solutions a) I use the autoarima R function to search over models using AIC and decide on an ARMA3,) b) I compare the ARMA3,) to ARMA,0) ARMA3,) does better in all three criteria c) The plot of the
ST5224: Advanced Statistical Theory II
ST5224: Advanced Statistical Theory II 2014/2015: Semester II Tutorial 7 1. Let X be a sample from a population P and consider testing hypotheses H 0 : P = P 0 versus H 1 : P = P 1, where P j is a known
Estimation for ARMA Processes with Stable Noise. Matt Calder & Richard A. Davis Colorado State University
Estimation for ARMA Processes with Stable Noise Matt Calder & Richard A. Davis Colorado State University rdavis@stat.colostate.edu 1 ARMA processes with stable noise Review of M-estimation Examples of
Neutralino contributions to Dark Matter, LHC and future Linear Collider searches
Neutralno contrbutons to Dark Matter, LHC and future Lnear Collder searches G.J. Gounars Unversty of Thessalonk, Collaboraton wth J. Layssac, P.I. Porfyrads, F.M. Renard and wth Th. Dakonds for the γz
Partial Differential Equations in Biology The boundary element method. March 26, 2013
The boundary element method March 26, 203 Introduction and notation The problem: u = f in D R d u = ϕ in Γ D u n = g on Γ N, where D = Γ D Γ N, Γ D Γ N = (possibly, Γ D = [Neumann problem] or Γ N = [Dirichlet
Constant Elasticity of Substitution in Applied General Equilibrium
Constant Elastct of Substtuton n Appled General Equlbru The choce of nput levels that nze the cost of producton for an set of nput prces and a fed level of producton can be epressed as n sty.. f Ltng for
Statistical Inference I Locally most powerful tests
Statistical Inference I Locally most powerful tests Shirsendu Mukherjee Department of Statistics, Asutosh College, Kolkata, India. shirsendu st@yahoo.co.in So far we have treated the testing of one-sided
A Note on Intuitionistic Fuzzy. Equivalence Relation
International Mathematical Forum, 5, 2010, no. 67, 3301-3307 A Note on Intuitionistic Fuzzy Equivalence Relation D. K. Basnet Dept. of Mathematics, Assam University Silchar-788011, Assam, India dkbasnet@rediffmail.com
Math221: HW# 1 solutions
Math: HW# solutions Andy Royston October, 5 7.5.7, 3 rd Ed. We have a n = b n = a = fxdx = xdx =, x cos nxdx = x sin nx n sin nxdx n = cos nx n = n n, x sin nxdx = x cos nx n + cos nxdx n cos n = + sin
Fractional Colorings and Zykov Products of graphs
Fractional Colorings and Zykov Products of graphs Who? Nichole Schimanski When? July 27, 2011 Graphs A graph, G, consists of a vertex set, V (G), and an edge set, E(G). V (G) is any finite set E(G) is
Pricing of Options on two Currencies Libor Rates
Prcng o Optons on two Currences Lbor Rates Fabo Mercuro Fnancal Models, Banca IMI Abstract In ths document we show how to prce optons on two Lbor rates belongng to two derent currences the ormer s domestc,
k A = [k, k]( )[a 1, a 2 ] = [ka 1,ka 2 ] 4For the division of two intervals of confidence in R +
Chapter 3. Fuzzy Arithmetic 3- Fuzzy arithmetic: ~Addition(+) and subtraction (-): Let A = [a and B = [b, b in R If x [a and y [b, b than x+y [a +b +b Symbolically,we write A(+)B = [a (+)[b, b = [a +b
2 Lagrangian and Green functions in d dimensions
Renormalzaton of φ scalar feld theory December 6 Pdf fle generated on February 7, 8. TODO Examne ε n the two-pont functon cf Sterman. Lagrangan and Green functons n d dmensons In these notes, we ll use
Section 8.3 Trigonometric Equations
99 Section 8. Trigonometric Equations Objective 1: Solve Equations Involving One Trigonometric Function. In this section and the next, we will exple how to solving equations involving trigonometric functions.
ANSWERSHEET (TOPIC = DIFFERENTIAL CALCULUS) COLLECTION #2. h 0 h h 0 h h 0 ( ) g k = g 0 + g 1 + g g 2009 =?
Teko Classes IITJEE/AIEEE Maths by SUHAAG SIR, Bhopal, Ph (0755) 3 00 000 www.tekoclasses.com ANSWERSHEET (TOPIC DIFFERENTIAL CALCULUS) COLLECTION # Question Type A.Single Correct Type Q. (A) Sol least
TMA4115 Matematikk 3
TMA4115 Matematikk 3 Andrew Stacey Norges Teknisk-Naturvitenskapelige Universitet Trondheim Spring 2010 Lecture 12: Mathematics Marvellous Matrices Andrew Stacey Norges Teknisk-Naturvitenskapelige Universitet
8.323 Relativistic Quantum Field Theory I
MIT OpenCourseWare http://ocwmtedu 8323 Relatvstc Quantum Feld Theory I Sprng 2008 For nformaton about ctng these materals or our Terms of Use, vst: http://ocwmtedu/terms 1 The Lagrangan: 8323 Lecture
2. ARMA 1. 1 This part is based on H and BD.
2. ARMA 1 1 This part is based on H and BD. 1 1 MA 1.1 MA(1) Let ε t be WN with variance σ 2 and consider the zero mean 2 process Y t = ε t + θε t 1 (1) where θ is a constant. MA(1). This time series is
Inverse trigonometric functions & General Solution of Trigonometric Equations. ------------------ ----------------------------- -----------------
Inverse trigonometric functions & General Solution of Trigonometric Equations. 1. Sin ( ) = a) b) c) d) Ans b. Solution : Method 1. Ans a: 17 > 1 a) is rejected. w.k.t Sin ( sin ) = d is rejected. If sin
( y) Partial Differential Equations
Partial Dierential Equations Linear P.D.Es. contains no owers roducts o the deendent variables / an o its derivatives can occasionall be solved. Consider eamle ( ) a (sometimes written as a ) we can integrate
Second Order RLC Filters
ECEN 60 Circuits/Electronics Spring 007-0-07 P. Mathys Second Order RLC Filters RLC Lowpass Filter A passive RLC lowpass filter (LPF) circuit is shown in the following schematic. R L C v O (t) Using phasor
Reminders: linear functions
Reminders: linear functions Let U and V be vector spaces over the same field F. Definition A function f : U V is linear if for every u 1, u 2 U, f (u 1 + u 2 ) = f (u 1 ) + f (u 2 ), and for every u U
Journal of Theoretics Vol.4-5
Journal of Theoretcs Vol.4- A Unfed Feld Theory Peter Hckman peter.hckman@ntlworld.com Abstract: In ths paper, the extenson of Remann geometry to nclude an asymmetrc metrc tensor s presented. A new co-varant
PARTIAL NOTES for 6.1 Trigonometric Identities
PARTIAL NOTES for 6.1 Trigonometric Identities tanθ = sinθ cosθ cotθ = cosθ sinθ BASIC IDENTITIES cscθ = 1 sinθ secθ = 1 cosθ cotθ = 1 tanθ PYTHAGOREAN IDENTITIES sin θ + cos θ =1 tan θ +1= sec θ 1 + cot
ω ω ω ω ω ω+2 ω ω+2 + ω ω ω ω+2 + ω ω+1 ω ω+2 2 ω ω ω ω ω ω ω ω+1 ω ω2 ω ω2 + ω ω ω2 + ω ω ω ω2 + ω ω+1 ω ω2 + ω ω+1 + ω ω ω ω2 + ω
0 1 2 3 4 5 6 ω ω + 1 ω + 2 ω + 3 ω + 4 ω2 ω2 + 1 ω2 + 2 ω2 + 3 ω3 ω3 + 1 ω3 + 2 ω4 ω4 + 1 ω5 ω 2 ω 2 + 1 ω 2 + 2 ω 2 + ω ω 2 + ω + 1 ω 2 + ω2 ω 2 2 ω 2 2 + 1 ω 2 2 + ω ω 2 3 ω 3 ω 3 + 1 ω 3 + ω ω 3 +
6.1. Dirac Equation. Hamiltonian. Dirac Eq.
6.1. Dirac Equation Ref: M.Kaku, Quantum Field Theory, Oxford Univ Press (1993) η μν = η μν = diag(1, -1, -1, -1) p 0 = p 0 p = p i = -p i p μ p μ = p 0 p 0 + p i p i = E c 2 - p 2 = (m c) 2 H = c p 2
Numerical Analysis FMN011
Numerical Analysis FMN011 Carmen Arévalo Lund University carmen@maths.lth.se Lecture 12 Periodic data A function g has period P if g(x + P ) = g(x) Model: Trigonometric polynomial of order M T M (x) =
Appendix to On the stability of a compressible axisymmetric rotating flow in a pipe. By Z. Rusak & J. H. Lee
Appendi to On the stability of a compressible aisymmetric rotating flow in a pipe By Z. Rusak & J. H. Lee Journal of Fluid Mechanics, vol. 5 4, pp. 5 4 This material has not been copy-edited or typeset
Phys460.nb Solution for the t-dependent Schrodinger s equation How did we find the solution? (not required)
Phys460.nb 81 ψ n (t) is still the (same) eigenstate of H But for tdependent H. The answer is NO. 5.5.5. Solution for the tdependent Schrodinger s equation If we assume that at time t 0, the electron starts
Appendix. Appendix I. Details used in M-step of Section 4. and expect ultimately it will close to zero. αi =α (r 1) [δq(α i ; α (r 1)
Appendx Appendx I. Detals used n M-step of Secton 4. Now wrte h (r) and expect ultmately t wll close to zero. and h (r) = [δq(α ; α (r) )/δα ] α =α (r 1) = [δq(α ; α (r) )/δα ] α =α (r 1) δ log L(α (r
Sequent Calculi for the Modal µ-calculus over S5. Luca Alberucci, University of Berne. Logic Colloquium Berne, July 4th 2008
Sequent Calculi for the Modal µ-calculus over S5 Luca Alberucci, University of Berne Logic Colloquium Berne, July 4th 2008 Introduction Koz: Axiomatisation for the modal µ-calculus over K Axioms: All classical
F19MC2 Solutions 9 Complex Analysis
F9MC Solutions 9 Complex Analysis. (i) Let f(z) = eaz +z. Then f is ifferentiable except at z = ±i an so by Cauchy s Resiue Theorem e az z = πi[res(f,i)+res(f, i)]. +z C(,) Since + has zeros of orer at
Homework 8 Model Solution Section
MATH 004 Homework Solution Homework 8 Model Solution Section 14.5 14.6. 14.5. Use the Chain Rule to find dz where z cosx + 4y), x 5t 4, y 1 t. dz dx + dy y sinx + 4y)0t + 4) sinx + 4y) 1t ) 0t + 4t ) sinx
Lecture 2. Soundness and completeness of propositional logic
Lecture 2 Soundness and completeness of propositional logic February 9, 2004 1 Overview Review of natural deduction. Soundness and completeness. Semantics of propositional formulas. Soundness proof. Completeness
Module 5. February 14, h 0min
Module 5 Stationary Time Series Models Part 2 AR and ARMA Models and Their Properties Class notes for Statistics 451: Applied Time Series Iowa State University Copyright 2015 W. Q. Meeker. February 14,
DESIGN OF MACHINERY SOLUTION MANUAL h in h 4 0.
DESIGN OF MACHINERY SOLUTION MANUAL -7-1! PROBLEM -7 Statement: Design a double-dwell cam to move a follower from to 25 6, dwell for 12, fall 25 and dwell for the remader The total cycle must take 4 sec
Areas and Lengths in Polar Coordinates
Kiryl Tsishchanka Areas and Lengths in Polar Coordinates In this section we develop the formula for the area of a region whose boundary is given by a polar equation. We need to use the formula for the
Stationary ARMA Processes
Stationary ARMA Processes Eduardo Rossi University of Pavia October 2013 Rossi Stationary ARMA Financial Econometrics - 2013 1 / 45 Moving Average of order 1 (MA(1)) Y t = µ + ɛ t + θɛ t 1 t = 1,..., T
ΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 6/5/2006
Οδηγίες: Να απαντηθούν όλες οι ερωτήσεις. Ολοι οι αριθμοί που αναφέρονται σε όλα τα ερωτήματα είναι μικρότεροι το 1000 εκτός αν ορίζεται διαφορετικά στη διατύπωση του προβλήματος. Διάρκεια: 3,5 ώρες Καλή
Solutions to Exercise Sheet 5
Solutions to Eercise Sheet 5 jacques@ucsd.edu. Let X and Y be random variables with joint pdf f(, y) = 3y( + y) where and y. Determine each of the following probabilities. Solutions. a. P (X ). b. P (X
( )( ) ( ) ( )( ) ( )( ) β = Chapter 5 Exercise Problems EX α So 49 β 199 EX EX EX5.4 EX5.5. (a)
hapter 5 xercise Problems X5. α β α 0.980 For α 0.980, β 49 0.980 0.995 For α 0.995, β 99 0.995 So 49 β 99 X5. O 00 O or n 3 O 40.5 β 0 X5.3 6.5 μ A 00 β ( 0)( 6.5 μa) 8 ma 5 ( 8)( 4 ) or.88 P on + 0.0065
Chapter 6: Systems of Linear Differential. be continuous functions on the interval
Chapter 6: Systems of Linear Differential Equations Let a (t), a 2 (t),..., a nn (t), b (t), b 2 (t),..., b n (t) be continuous functions on the interval I. The system of n first-order differential equations
Main source: "Discrete-time systems and computer control" by Α. ΣΚΟΔΡΑΣ ΨΗΦΙΑΚΟΣ ΕΛΕΓΧΟΣ ΔΙΑΛΕΞΗ 4 ΔΙΑΦΑΝΕΙΑ 1
Main source: "Discrete-time systems and computer control" by Α. ΣΚΟΔΡΑΣ ΨΗΦΙΑΚΟΣ ΕΛΕΓΧΟΣ ΔΙΑΛΕΞΗ 4 ΔΙΑΦΑΝΕΙΑ 1 A Brief History of Sampling Research 1915 - Edmund Taylor Whittaker (1873-1956) devised a
Approximation of distance between locations on earth given by latitude and longitude
Approximation of distance between locations on earth given by latitude and longitude Jan Behrens 2012-12-31 In this paper we shall provide a method to approximate distances between two points on earth
Lecture 13 - Root Space Decomposition II
Lecture 13 - Root Space Decomposition II October 18, 2012 1 Review First let us recall the situation. Let g be a simple algebra, with maximal toral subalgebra h (which we are calling a CSA, or Cartan Subalgebra).
Generalized Fibonacci-Like Polynomial and its. Determinantal Identities
Int. J. Contemp. Math. Scences, Vol. 7, 01, no. 9, 1415-140 Generalzed Fbonacc-Le Polynomal and ts Determnantal Identtes V. K. Gupta 1, Yashwant K. Panwar and Ompraash Shwal 3 1 Department of Mathematcs,
ECE Spring Prof. David R. Jackson ECE Dept. Notes 2
ECE 634 Spring 6 Prof. David R. Jackson ECE Dept. Notes Fields in a Source-Free Region Example: Radiation from an aperture y PEC E t x Aperture Assume the following choice of vector potentials: A F = =
On a four-dimensional hyperbolic manifold with finite volume
BULETINUL ACADEMIEI DE ŞTIINŢE A REPUBLICII MOLDOVA. MATEMATICA Numbers 2(72) 3(73), 2013, Pages 80 89 ISSN 1024 7696 On a four-dimensional hyperbolic manifold with finite volume I.S.Gutsul Abstract. In
IIT JEE (2013) (Trigonomtery 1) Solutions
L.K. Gupta (Mathematic Classes) www.pioeermathematics.com MOBILE: 985577, 677 (+) PAPER B IIT JEE (0) (Trigoomtery ) Solutios TOWARDS IIT JEE IS NOT A JOURNEY, IT S A BATTLE, ONLY THE TOUGHEST WILL SURVIVE
2. THEORY OF EQUATIONS. PREVIOUS EAMCET Bits.
EAMCET-. THEORY OF EQUATIONS PREVIOUS EAMCET Bits. Each of the roots of the equation x 6x + 6x 5= are increased by k so that the new transformed equation does not contain term. Then k =... - 4. - Sol.
Εργαστήριο Ανάπτυξης Εφαρμογών Βάσεων Δεδομένων. Εξάμηνο 7 ο
Εργαστήριο Ανάπτυξης Εφαρμογών Βάσεων Δεδομένων Εξάμηνο 7 ο Procedures and Functions Stored procedures and functions are named blocks of code that enable you to group and organize a series of SQL and PL/SQL
2. Let H 1 and H 2 be Hilbert spaces and let T : H 1 H 2 be a bounded linear operator. Prove that [T (H 1 )] = N (T ). (6p)
Uppsala Universitet Matematiska Institutionen Andreas Strömbergsson Prov i matematik Funktionalanalys Kurs: F3B, F4Sy, NVP 2005-03-08 Skrivtid: 9 14 Tillåtna hjälpmedel: Manuella skrivdon, Kreyszigs bok
8. ΕΠΕΞΕΡΓΑΣΊΑ ΣΗΜΆΤΩΝ. ICA: συναρτήσεις κόστους & εφαρμογές
8. ΕΠΕΞΕΡΓΑΣΊΑ ΣΗΜΆΤΩΝ ICA: συναρτήσεις κόστους & εφαρμογές ΚΎΡΤΩΣΗ (KUROSIS) Αθροιστικό (cumulant) 4 ης τάξεως μίας τ.μ. x με μέσο όρο 0: kurt 4 [ x] = E[ x ] 3( E[ y ]) Υποθέτουμε διασπορά=: kurt[ x]
MATH423 String Theory Solutions 4. = 0 τ = f(s). (1) dτ ds = dxµ dτ f (s) (2) dτ 2 [f (s)] 2 + dxµ. dτ f (s) (3)
1. MATH43 String Theory Solutions 4 x = 0 τ = fs). 1) = = f s) ) x = x [f s)] + f s) 3) equation of motion is x = 0 if an only if f s) = 0 i.e. fs) = As + B with A, B constants. i.e. allowe reparametrisations