φ p ( B) AR polynomial of B of order p, p Non-seasonal differencing operator = 1 B

Size: px
Start display at page:

Download "φ p ( B) AR polynomial of B of order p, p Non-seasonal differencing operator = 1 B"

Transcription

1 ARIMA Noion The ARIMA roceure coues he reer esies for given sesonl or non-sesonl univrie ARIMA oel. I lso coues he fie vlues, forecsing vlues, n oher rele vribles for he oel. The following noion is use hroughou his cher unless oherwise se: y (=, 2,..., N) N ( =, 2,..., N) q P Q D s Univrie ie series uner invesigion Tol nuber of observions Whie noise series norlly isribue wih en zero n vrince σ 2 Orer of he non-sesonl uoregressive r of he oel Orer of he non-sesonl oving verge r of he oel Orer of he non-sesonl ifferencing Orer of he sesonl uoregressive r of he oel Orer of he sesonl oving-verge r of he oel Orer of he sesonl ifferencing Sesonliy or erio of he oel φ ( B) AR olynoil of B of orer, φ ( B) = ϕb ϕ2b 2... ϕ B θ q ( B) MA olynoil of B of orer q, θ ( B) = ϑb ϑ2b 2... ϑ B q q q Φ P ( B) SAR olynoil of B of orer P, Φ ( B) = ΦB Φ2B 2... Φ B P P P Θ Q ( B) SMA olynoil of B of orer Q, Θ ( B) = ΘB Θ2B 2... Θ B s Q Q Q Non-sesonl ifferencing oeror = B Sesonl ifferencing oeror wih sesonliy s, = B B Bckwr shif oeror wih By = y n B s = s 44

2 ARIMA 45 Moels A sesonl univrie ARIMA(,,q)(P,D,Q) s oel is given by φ ( B) Φ ( B)[ y µ ] = θ ( B) Θ ( B) =, K, N () P s D q Q where µ is n oionl oel consn. I is lso clle he sionry series en, ssuing h, fer ifferencing, he series is sionry. When NOCONSTANT is secifie, µ is ssue o be zero. When P= Q = D =0, he oel is reuce o (non-sesonl) ARIMA(,,q) oel: φ ( B)[ y µ ] = θ ( B) =, K, N (2) q An oionl log scle rnsforion cn be lie o y before he oel is fie. In his cher, he se sybol, y, is use o enoe he series eiher before or fer log scle rnsforion. Ineenen vribles x, x 2,, x cn lso be inclue in he oel. The oel wih ineenen vribles is given by φ ( B) Φ ( B)[ ( y c x ) µ ] = θ ( B) Θ ( B) P s D i i q Q or Φ( B)[ ( B)( y c x ) µ ] = Θ( B) (3) where Φ( B) = φ ( B) Φ P ( B) ( B) = s D Θ( B) = θ q ( B) Θ Q ( B) i i n ci, i = 2K,,,, re he regression coefficiens for he ineenen vribles.

3 46 ARIMA Esiion Bsiclly, wo ifferen esiion lgorihs re use o coue xiu likelihoo (ML) esies for he reers in n ARIMA oel: Melr s lgorih is use for he esiion when here is no issing in he ie series. The lgorih coues he xiu likelihoo esies of he oel reers. The eils of he lgorih re escribe in Melr (984), Perln (980), n Morf, Sihu, n Kilh (974). A Kln filering lgorih is use for he esiion when soe observions in he ie series re issing. The lgorih efficienly coues he rginl likelihoo of n ARIMA oel wih issing observions. The eils of he lgorih re escribe in he following lierure: Kohn n Ansley (986) n Kohn n Ansley (985). Dignosic Sisics The following efiniions re use in he sisics below: N Nuber of reers R S T q P Q N = q+ P+ Q+ + wihou oel consn wih oel consn SSQ Resiul su of squres SSQ = ee, where e is he resiul vecor $σ 2 Esie resiul vrince $σ 2 SSQ =, where f = N N f SSQ' Ajuse resiul su of squres N SSQ' =SSQfΩ /, where Ω is he heoreicl covrince rix of he observion vecor coue MLE

4 ARIMA 47 Log-Likelihoo SSQ' N ln( 2π ) L= Nln( σ$ ) 2σ$ 2 2 Akike Inforion Crierion (AIC) AIC = 2L + 2N Schwrz Byesin Crierion (SBC) SBC = 2L + lnbg N N Genere Vribles Preice Vlues Forecsing Meho: Coniionl Les Squres (CLS or AUTOINT) In generl, he oel use for fiing n forecsing (fer esiion, if involve) cn be escribe by Equion (3), which cn be wrien s y D( B) y = Φ( B) µ + Θ( B) + c Φ( B) ( B) x i where f Bf f f Φ f DB = Φ B B Φ µ = µ i

5 48 ARIMA Thus, he reice vlues (FIT) re coue s follows: f = = i FIT y$ D( B)$ y Φ( B) µ Θ( B)$ c Φ( B) ( B) x i (4) where $ = y y$ n Sring Vlues for Couing Fie Series. To sr he couion for fie vlues using Equion (4), ll unvilble beginning resiuls re se o zero n unvilble beginning vlues of he fie series re se ccoring o he selece eho: CLS. The couion srs he (+sd)-h erio. Afer secifie log scle rnsforion, if ny, he originl series is ifference n/or sesonlly ifference ccoring o he oel secificion. Fie vlues for he ifference series re coue firs. All unvilble beginning fie vlues in he couion re relce by he sionry series en, which is equl o he oel consn in he oel secificion. The fie vlues re hen ggrege o he originl series n roerly rnsfore bck o he originl scle. The firs +sd fie vlues re se o issing (SYSMIS). AUTOINIT. The couion srs he [++s(d+p)]-h erio. Afer ny secifie log scle rnsforion, he cul ++s(d+p) beginning observions in he series re use s beginning fie vlues in he couion. The firs ++s(d+p) fie vlues re se o issing. The fie vlues re hen rnsfore bck o he originl scle, if log rnsforion is secifie. Forecsing Meho: Unconiionl Les Squres (EXACT) As wih he CLS eho, he couions sr he (+sd)-h erio. Firs, he originl series (or he log-rnsfore series if rnsforion is secifie) is ifference n/or sesonlly ifference ccoring o he oel secificion. Then he fie vlues for he ifference series re coue. The fie vlues re one-se-he, les-squres reicors clcule using he heoreicl uocorrelion funcion of he sionry uoregressive oving verge (ARMA) rocess corresoning o he ifference series. The uocorrelion funcion is coue by reing he esie reers s he rue reers. The fie vlues re hen ggrege o he originl series n roerly rnsfore bck o he originl scle. The firs +sd fie vlues re se o issing (SYSMIS). The eils of he les-squres reicion lgorih for he ARMA oels cn be foun in Brockwell n Dvis (99).

6 ARIMA 49 Resiuls Resiul series re lwys coue in he rnsfore log scle, if rnsforion is secifie. ( ERR) = y ( FIT ) =2K,,, N Snr Errors of he Preice Vlues Snr errors of he reice vlues re firs coue in he rnsfore log scle, if rnsforion is secifie. Forcsing Meho: Coniionl Les Squres (CLS or AUTOINIT) ( SEP) = σ$ = 2K,,, N Forecsing Meho: Unconiionl Les Squres (EXACT) In he EXACT eho, unlike he CLS eho, here is no sile exression for he snr errors of he reice vlues. The snr errors of he reice vlues will, however, be given by he les-squres reicion lgorih s byrouc. Snr errors of he reice vlues re hen rnsfore bck o he originl scle for ech reice vlue, if rnsforion is secifie. Confience Liis of he Preice Vlues Confience liis of he reice vlues re firs coue in he rnsfore log scle, if rnsforion is secifie: ( LCL) = ( FIT) α / 2, f ( SEP) = 2,, K, N ( UCL) = ( FIT) + α / 2, ( SEP) = 2,, K, N f b where α / 2, f is he α / 2g-h ercenile of isribuion wih f egrees of freeo n α is he secifie confience level (by eful α = 005. ). Confience liis of he reice vlues re hen rnsfore bck o he originl scle for ech reice vlue, if rnsforion is secifie.

7 50 ARIMA Forecsing Forecsing Vlues Forcsing Meho: Coniionl Les Squres (CLS or AUTOINIT) The following forecsing equion cn be erive fro Equion (3): y$ () l = D( B)$ y+ l + Φ( B) µ + Θ( B)$ + l + ciφ( B) ( B) x, i+ l (5) where f f f f f DB = Φ B B, Φ Bµ = Φ µ y$ () l enoes he l-se-he forecs of y + l he ie. y$ $ + l i + l j = = R S T R S T y+ l i if l i y$ ( l i) if l > i y+ l i y$ + l i () if l i 0 if l > i Noe h y$ () is he one-se-he forecs of y + ie, which is excly he reice vlue $y + s given in Equion (4). Forecsing Meho: Unconiionl Les Squres (EXACT) The forecss wih his oion re finie eory, les-squres forecss coue using he heoreicl uocorrelion funcion of he series. The eils of he lessqures forecsing lgorih for he ARIMA oels cn be foun in Brockwell n Dvis (99).

8 ARIMA 5 Snr Errors of he Forecsing Vlues Forcsing Meho: Coniionl Les Squres (CLS or AUTOINIT) For he urose of couing snr errors of he forecsing vlues, Equion () cn be wrien in he for of ψ weighs (ignoring he oel consn): ϑq( B ) Θ Q ( B ) i y = B ib B P B = ψ( ) = φ ψ ( ) Φ ( ) 0 i, ψ 0 = (6) Le y$ () l enoe he l-se-he forecs of y + l ie. Then 2 2 se[ y$ ()] l = { + ψ + ψ ψ } σ$ l Noe h, for he reice vlue, l =. Hence, ( SEP) = σ $ ny ie. Couion of ψ Weighs. ψ weighs cn be coue by exning boh sies of he following equion n solving he liner equion syse esblishe by equing he corresoning coefficiens on boh sies of he exnsion: φ ( B) Φ ( B) ψ( B) = θ ( B) Θ ( B) P s D q Q An exlici exression of ψ weighs cn be foun in Box n Jenkins (976). Forecsing Meho: Unconiionl Les Squres (EXACT) References As wih he snr errors of he reice vlues, he snr errors of he forecsing vlues re byrouc uring he les-squres forecsing couion. The eils cn be foun in Brockwell n Dvis (99). Box n Jenkins (976) Brockwell n Dvis (99)

SOME USEFUL MATHEMATICS

SOME USEFUL MATHEMATICS SOME USEFU MAHEMAICS SOME USEFU MAHEMAICS I is esy o mesure n preic he behvior of n elecricl circui h conins only c volges n currens. However, mos useful elecricl signls h crry informion vry wih ime. Since

More information

P441 Analytical Mechanics - I. Coupled Oscillators. c Alex R. Dzierba

P441 Analytical Mechanics - I. Coupled Oscillators. c Alex R. Dzierba Lecure 3 Mondy - Deceber 5, 005 Wrien or ls upded: Deceber 3, 005 P44 Anlyicl Mechnics - I oupled Oscillors c Alex R. Dzierb oupled oscillors - rix echnique In Figure we show n exple of wo coupled oscillors,

More information

USING ITERATIVE LINEAR REGRESSION MODEL TO TIME SERIES MODELS

USING ITERATIVE LINEAR REGRESSION MODEL TO TIME SERIES MODELS Elecronic Journl of Applied Sisicl Anlysis EJASA (202), Elecron. J. App. S. Anl., Vol. 5, Issue 2, 37 50 e-issn 2070-5948, DOI 0.285/i20705948v5n2p37 202 Universià del Sleno hp://sib-ese.unile.i/index.php/ejs/index

More information

5.1-The Initial-Value Problems For Ordinary Differential Equations

5.1-The Initial-Value Problems For Ordinary Differential Equations 5.-The Iniil-Vlue Problems For Ordinry Differenil Equions Consider solving iniil-vlue problems for ordinry differenil equions: (*) y f, y, b, y. If we know he generl soluion y of he ordinry differenil

More information

e t dt e t dt = lim e t dt T (1 e T ) = 1

e t dt e t dt = lim e t dt T (1 e T ) = 1 Improper Inegrls There re wo ypes of improper inegrls - hose wih infinie limis of inegrion, nd hose wih inegrnds h pproch some poin wihin he limis of inegrion. Firs we will consider inegrls wih infinie

More information

Probability, Estimators, and Stationarity

Probability, Estimators, and Stationarity Chper Probbiliy, Esimors, nd Sionriy Consider signl genered by dynmicl process, R, R. Considering s funcion of ime, we re opering in he ime domin. A fundmenl wy o chrcerize he dynmics using he ime domin

More information

[5] Solving Multiple Linear Equations A system of m linear equations and n unknown variables:

[5] Solving Multiple Linear Equations A system of m linear equations and n unknown variables: [5] Solving Muliple Liner Equions A syse of liner equions nd n unknown vribles: + + + nn = b + + + = b n n : + + + nn = b n n A= b, where A =, : : : n : : : : n = : n A = = = ( ) where, n j = ( ); = :

More information

THE IMPACT OF SEASONAL ADJUSTMENT ON TIME SERIES PREDICTION

THE IMPACT OF SEASONAL ADJUSTMENT ON TIME SERIES PREDICTION Review of he Air Force Acaemy No 3 (27) 2014 THE IMPACT OF SEASONAL ADJUSTMENT ON TIME SERIES PREDICTION Aela SASU Transilvania Universiy of Braşov Absrac: In his aricle we inen o comare he erformance

More information

Practice Problems - Week #4 Higher-Order DEs, Applications Solutions

Practice Problems - Week #4 Higher-Order DEs, Applications Solutions Pracice Probles - Wee #4 Higher-Orer DEs, Applicaions Soluions 1. Solve he iniial value proble where y y = 0, y0 = 0, y 0 = 1, an y 0 =. r r = rr 1 = rr 1r + 1, so he general soluion is C 1 + C e x + C

More information

14. The fundamental theorem of the calculus

14. The fundamental theorem of the calculus 4. The funmenl heorem of he clculus V 20 00 80 60 40 20 0 0 0.2 0.4 0.6 0.8 v 400 200 0 0 0.2 0.5 0.8 200 400 Figure : () Venriculr volume for subjecs wih cpciies C = 24 ml, C = 20 ml, C = 2 ml n (b) he

More information

Motion. Part 2: Constant Acceleration. Acceleration. October Lab Physics. Ms. Levine 1. Acceleration. Acceleration. Units for Acceleration.

Motion. Part 2: Constant Acceleration. Acceleration. October Lab Physics. Ms. Levine 1. Acceleration. Acceleration. Units for Acceleration. Moion Accelerion Pr : Consn Accelerion Accelerion Accelerion Accelerion is he re of chnge of velociy. = v - vo = Δv Δ ccelerion = = v - vo chnge of velociy elpsed ime Accelerion is vecor, lhough in one-dimensionl

More information

Minimum Squared Error

Minimum Squared Error Minimum Squred Error LDF: Minimum Squred-Error Procedures Ide: conver o esier nd eer undersood prolem Percepron y i > for ll smples y i solve sysem of liner inequliies MSE procedure y i = i for ll smples

More information

Minimum Squared Error

Minimum Squared Error Minimum Squred Error LDF: Minimum Squred-Error Procedures Ide: conver o esier nd eer undersood prolem Percepron y i > 0 for ll smples y i solve sysem of liner inequliies MSE procedure y i i for ll smples

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

Laplace Examples, Inverse, Rational Form

Laplace Examples, Inverse, Rational Form Lecure 3 Ouline: Lplce Exple, Invere, Rionl For Announceen: Rein: 6: Lplce Trnfor pp. 3-33, 55.5-56.5, 7 HW 8 poe, ue nex We. Free -y exenion OcenOne Roo Tour will e fer cl y 7 (:3-:) Lunch provie ferwr.

More information

Impact of International Information Technology Transfer on National Productivity. Online Supplement

Impact of International Information Technology Transfer on National Productivity. Online Supplement Impac of Inernaional Informaion Technology Transfer on Naional Prouciviy Online Supplemen Jungsoo Park Deparmen of Economics Sogang Universiy Seoul, Korea Email: jspark@sogang.ac.kr, Tel: 82-2-705-8697,

More information

0 for t < 0 1 for t > 0

0 for t < 0 1 for t > 0 8.0 Sep nd del funcions Auhor: Jeremy Orloff The uni Sep Funcion We define he uni sep funcion by u() = 0 for < 0 for > 0 I is clled he uni sep funcion becuse i kes uni sep = 0. I is someimes clled he Heviside

More information

THREE IMPORTANT CONCEPTS IN TIME SERIES ANALYSIS: STATIONARITY, CROSSING RATES, AND THE WOLD REPRESENTATION THEOREM

THREE IMPORTANT CONCEPTS IN TIME SERIES ANALYSIS: STATIONARITY, CROSSING RATES, AND THE WOLD REPRESENTATION THEOREM THR IMPORTANT CONCPTS IN TIM SRIS ANALYSIS: STATIONARITY, CROSSING RATS, AND TH WOLD RPRSNTATION THORM Prof. Thoms B. Fomb Deprmen of conomics Souhern Mehodis Universi June 8 I. Definiion of Covrince Sionri

More information

Lecture 6 - Testing Restrictions on the Disturbance Process (References Sections 2.7 and 2.10, Hayashi)

Lecture 6 - Testing Restrictions on the Disturbance Process (References Sections 2.7 and 2.10, Hayashi) Lecure 6 - esing Resricions on he Disurbance Process (References Secions 2.7 an 2.0, Hayashi) We have eveloe sufficien coniions for he consisency an asymoic normaliy of he OLS esimaor ha allow for coniionally

More information

A Kalman filtering simulation

A Kalman filtering simulation A Klmn filering simulion The performnce of Klmn filering hs been esed on he bsis of wo differen dynmicl models, ssuming eiher moion wih consn elociy or wih consn ccelerion. The former is epeced o beer

More information

t v a t area Dynamic Physics for Simulation and Game Programming F a m v v a t x x v t Discrete Dynamics

t v a t area Dynamic Physics for Simulation and Game Programming F a m v v a t x x v t Discrete Dynamics Dynic Physics for Siulion n Ge Progring F Discree Dynics. Force equls ss ies ccelerion (F=) v v v v Mike Biley This work is license uner Creive Coons Aribuion-NonCoercil- NoDerivives.0 Inernionl License

More information

Chapter Direct Method of Interpolation

Chapter Direct Method of Interpolation Chper 5. Direc Mehod of Inerpolion Afer reding his chper, you should be ble o:. pply he direc mehod of inerpolion,. sole problems using he direc mehod of inerpolion, nd. use he direc mehod inerpolns o

More information

3. Renewal Limit Theorems

3. Renewal Limit Theorems Virul Lborories > 14. Renewl Processes > 1 2 3 3. Renewl Limi Theorems In he inroducion o renewl processes, we noed h he rrivl ime process nd he couning process re inverses, in sens The rrivl ime process

More information

(b) 10 yr. (b) 13 m. 1.6 m s, m s m s (c) 13.1 s. 32. (a) 20.0 s (b) No, the minimum distance to stop = 1.00 km. 1.

(b) 10 yr. (b) 13 m. 1.6 m s, m s m s (c) 13.1 s. 32. (a) 20.0 s (b) No, the minimum distance to stop = 1.00 km. 1. Answers o Een Numbered Problems Chper. () 7 m s, 6 m s (b) 8 5 yr 4.. m ih 6. () 5. m s (b).5 m s (c).5 m s (d) 3.33 m s (e) 8. ().3 min (b) 64 mi..3 h. ().3 s (b) 3 m 4..8 mi wes of he flgpole 6. (b)

More information

Characteristic Function for the Truncated Triangular Distribution., Myron Katzoff and Rahul A. Parsa

Characteristic Function for the Truncated Triangular Distribution., Myron Katzoff and Rahul A. Parsa Secion on Survey Reserch Mehos JSM 009 Chrcerisic Funcion for he Trunce Tringulr Disriuion Jy J. Kim 1 1, Myron Kzoff n Rhul A. Prs 1 Nionl Cener for Helh Sisics, 11Toleo Ro, Hysville, MD. 078 College

More information

NONLINEAR MODEL OF THE VEHICLE HYDROPNEUMATIC SUSPENSION UNIT

NONLINEAR MODEL OF THE VEHICLE HYDROPNEUMATIC SUSPENSION UNIT Nuber, olue II, Deceber NONLINEAR MODEL OF THE EHICLE HYDROPNEUMATIC UPENION UNIT Libor Kuk ury: The lue reers oel of he hyroneuic susension uni n is verificion is escribe in he er. The relions effecive

More information

ECONOMETRIC THEORY. MODULE IV Lecture - 16 Predictions in Linear Regression Model

ECONOMETRIC THEORY. MODULE IV Lecture - 16 Predictions in Linear Regression Model ECONOMETRIC THEORY MODULE IV Lecture - 16 Predictions in Liner Regression Model Dr. Shlbh Deprtent of Mthetics nd Sttistics Indin Institute of Technology Knpur Prediction of vlues of study vrible An iportnt

More information

D.I. Survival models and copulas

D.I. Survival models and copulas D- D. SURVIVAL COPULA D.I. Survival moels an copulas Definiions, relaionships wih mulivariae survival isribuion funcions an relaionships beween copulas an survival copulas. D.II. Fraily moels Use of a

More information

Homework 2 Solutions

Homework 2 Solutions Mah 308 Differenial Equaions Fall 2002 & 2. See he las page. Hoework 2 Soluions 3a). Newon s secon law of oion says ha a = F, an we know a =, so we have = F. One par of he force is graviy, g. However,

More information

Online Learning with Partial Feedback. 1 Online Mirror Descent with Estimated Gradient

Online Learning with Partial Feedback. 1 Online Mirror Descent with Estimated Gradient Avance Course in Machine Learning Spring 2010 Online Learning wih Parial Feeback Hanous are joinly prepare by Shie Mannor an Shai Shalev-Shwarz In previous lecures we alke abou he general framework of

More information

DETERMINISTIC TREND / DETERMINISTIC SEASON MODEL. Professor Thomas B. Fomby Department of Economics Southern Methodist University Dallas, TX June 2008

DETERMINISTIC TREND / DETERMINISTIC SEASON MODEL. Professor Thomas B. Fomby Department of Economics Southern Methodist University Dallas, TX June 2008 DTRMINISTIC TRND / DTRMINISTIC SASON MODL Professor Toms B. Fomby Deprmen of conomics Souern Meodis Universiy Dlls, TX June 008 I. Inroducion Te Deerminisic Trend / Deerminisic Seson DTDS model is one

More information

ISSUES RELATED WITH ARMA (P,Q) PROCESS. Salah H. Abid AL-Mustansirya University - College Of Education Department of Mathematics (IRAQ / BAGHDAD)

ISSUES RELATED WITH ARMA (P,Q) PROCESS. Salah H. Abid AL-Mustansirya University - College Of Education Department of Mathematics (IRAQ / BAGHDAD) Eoen Jonl of Sisics n Poiliy Vol. No..9- Mc Plise y Eoen Cene fo Resec Tinin n Develoen UK www.e-onls.o ISSUES RELATED WITH ARMA PQ PROCESS Sl H. Ai AL-Msnsiy Univesiy - Collee Of Ecion Deen of Meics IRAQ

More information

INTEGRALS. Exercise 1. Let f : [a, b] R be bounded, and let P and Q be partitions of [a, b]. Prove that if P Q then U(P ) U(Q) and L(P ) L(Q).

INTEGRALS. Exercise 1. Let f : [a, b] R be bounded, and let P and Q be partitions of [a, b]. Prove that if P Q then U(P ) U(Q) and L(P ) L(Q). INTEGRALS JOHN QUIGG Eercise. Le f : [, b] R be bounded, nd le P nd Q be priions of [, b]. Prove h if P Q hen U(P ) U(Q) nd L(P ) L(Q). Soluion: Le P = {,..., n }. Since Q is obined from P by dding finiely

More information

ENGR 1990 Engineering Mathematics The Integral of a Function as a Function

ENGR 1990 Engineering Mathematics The Integral of a Function as a Function ENGR 1990 Engineering Mhemics The Inegrl of Funcion s Funcion Previously, we lerned how o esime he inegrl of funcion f( ) over some inervl y dding he res of finie se of rpezoids h represen he re under

More information

More on Magnetically C Coupled Coils and Ideal Transformers

More on Magnetically C Coupled Coils and Ideal Transformers Appenix ore on gneiclly C Couple Coils Iel Trnsformers C. Equivlen Circuis for gneiclly Couple Coils A imes, i is convenien o moel mgneiclly couple coils wih n equivlen circui h oes no involve mgneic coupling.

More information

Chapter 2 The Derivative Applied Calculus 107. We ll need a rule for finding the derivative of a product so we don t have to multiply everything out.

Chapter 2 The Derivative Applied Calculus 107. We ll need a rule for finding the derivative of a product so we don t have to multiply everything out. Chaper The Derivaive Applie Calculus 107 Secion 4: Prouc an Quoien Rules The basic rules will le us ackle simple funcions. Bu wha happens if we nee he erivaive of a combinaion of hese funcions? Eample

More information

Forms of Energy. Mass = Energy. Page 1. SPH4U: Introduction to Work. Work & Energy. Particle Physics:

Forms of Energy. Mass = Energy. Page 1. SPH4U: Introduction to Work. Work & Energy. Particle Physics: SPH4U: Inroducion o ork ork & Energy ork & Energy Discussion Definiion Do Produc ork of consn force ork/kineic energy heore ork of uliple consn forces Coens One of he os iporn conceps in physics Alernive

More information

1. Find a basis for the row space of each of the following matrices. Your basis should consist of rows of the original matrix.

1. Find a basis for the row space of each of the following matrices. Your basis should consist of rows of the original matrix. Mh 7 Exm - Prcice Prolem Solions. Find sis for he row spce of ech of he following mrices. Yor sis shold consis of rows of he originl mrix. 4 () 7 7 8 () Since we wn sis for he row spce consising of rows

More information

Chapter 2. Motion along a straight line. 9/9/2015 Physics 218

Chapter 2. Motion along a straight line. 9/9/2015 Physics 218 Chper Moion long srigh line 9/9/05 Physics 8 Gols for Chper How o describe srigh line moion in erms of displcemen nd erge elociy. The mening of insnneous elociy nd speed. Aerge elociy/insnneous elociy

More information

THE COMBINED FORECASTING MODEL OF GRAY MODEL BASED ON LINEAR TIME-VARIANT AND ARIMA MODEL

THE COMBINED FORECASTING MODEL OF GRAY MODEL BASED ON LINEAR TIME-VARIANT AND ARIMA MODEL IJRRAS 6 (3) Sepember 03 www.rppress.com/volumes/vol6issue3/ijrras_6_3_0.pdf THE COMINED FORECASTING MODEL OF GRAY MODEL ASED ON LINEAR TIME-VARIANT AND ARIMA MODEL Xi Long,, Yong Wei, Jie Li 3 & Zho Long

More information

September 20 Homework Solutions

September 20 Homework Solutions College of Engineering nd Compuer Science Mechnicl Engineering Deprmen Mechnicl Engineering A Seminr in Engineering Anlysis Fll 7 Number 66 Insrucor: Lrry Creo Sepember Homework Soluions Find he specrum

More information

LAPLACE TRANSFORMS. 1. Basic transforms

LAPLACE TRANSFORMS. 1. Basic transforms LAPLACE TRANSFORMS. Bic rnform In hi coure, Lplce Trnform will be inroduced nd heir properie exmined; ble of common rnform will be buil up; nd rnform will be ued o olve ome dierenil equion by rnforming

More information

Physics Worksheet Lesson 4: Linear Motion Section: Name:

Physics Worksheet Lesson 4: Linear Motion Section: Name: Physics Workshee Lesson 4: Liner Moion Secion: Nme: 1. Relie Moion:. All moion is. b. is n rbirry coorine sysem wih reference o which he posiion or moion of somehing is escribe or physicl lws re formule.

More information

Contraction Mapping Principle Approach to Differential Equations

Contraction Mapping Principle Approach to Differential Equations epl Journl of Science echnology 0 (009) 49-53 Conrcion pping Principle pproch o Differenil Equions Bishnu P. Dhungn Deprmen of hemics, hendr Rn Cmpus ribhuvn Universiy, Khmu epl bsrc Using n eension of

More information

A Simple Method to Solve Quartic Equations. Key words: Polynomials, Quartics, Equations of the Fourth Degree INTRODUCTION

A Simple Method to Solve Quartic Equations. Key words: Polynomials, Quartics, Equations of the Fourth Degree INTRODUCTION Ausrlin Journl of Bsic nd Applied Sciences, 6(6): -6, 0 ISSN 99-878 A Simple Mehod o Solve Quric Equions Amir Fhi, Poo Mobdersn, Rhim Fhi Deprmen of Elecricl Engineering, Urmi brnch, Islmic Ad Universi,

More information

Stationary Time Series

Stationary Time Series 3-Jul-3 Time Series Analysis Assoc. Prof. Dr. Sevap Kesel July 03 Saionary Time Series Sricly saionary process: If he oin dis. of is he same as he oin dis. of ( X,... X n) ( X h,... X nh) Weakly Saionary

More information

Physics 2A HW #3 Solutions

Physics 2A HW #3 Solutions Chper 3 Focus on Conceps: 3, 4, 6, 9 Problems: 9, 9, 3, 41, 66, 7, 75, 77 Phsics A HW #3 Soluions Focus On Conceps 3-3 (c) The ccelerion due o grvi is he sme for boh blls, despie he fc h he hve differen

More information

FM Applications of Integration 1.Centroid of Area

FM Applications of Integration 1.Centroid of Area FM Applicions of Inegrion.Cenroid of Are The cenroid of ody is is geomeric cenre. For n ojec mde of uniform meril, he cenroid coincides wih he poin which he ody cn e suppored in perfecly lnced se ie, is

More information

PHYSICS 1210 Exam 1 University of Wyoming 14 February points

PHYSICS 1210 Exam 1 University of Wyoming 14 February points PHYSICS 1210 Em 1 Uniersiy of Wyoming 14 Februry 2013 150 poins This es is open-noe nd closed-book. Clculors re permied bu compuers re no. No collborion, consulion, or communicion wih oher people (oher

More information

can be viewed as a generalized product, and one for which the product of f and g. That is, does

can be viewed as a generalized product, and one for which the product of f and g. That is, does Boyce/DiPrim 9 h e, Ch 6.6: The Convoluion Inegrl Elemenry Differenil Equion n Bounry Vlue Problem, 9 h eiion, by Willim E. Boyce n Richr C. DiPrim, 9 by John Wiley & Son, Inc. Someime i i poible o wrie

More information

4.8 Improper Integrals

4.8 Improper Integrals 4.8 Improper Inegrls Well you ve mde i hrough ll he inegrion echniques. Congrs! Unforunely for us, we sill need o cover one more inegrl. They re clled Improper Inegrls. A his poin, we ve only del wih inegrls

More information

ARMAX Modelling of International Tourism Demand

ARMAX Modelling of International Tourism Demand ARMAX Modelling of Inernionl Tourism Demnd Lim, C. 1, Min, J.C.H. 2 nd McAleer, M. 3 1 Deprmen of Tourism nd Hospiliy Mngemen, Universiy of Wiko, New Zelnd 2 Deprmen of Tourism, Hsing Wu College, Tipei,

More information

6. Gas dynamics. Ideal gases Speed of infinitesimal disturbances in still gas

6. Gas dynamics. Ideal gases Speed of infinitesimal disturbances in still gas 6. Gs dynmics Dr. Gergely Krisóf De. of Fluid echnics, BE Februry, 009. Seed of infiniesiml disurbnces in sill gs dv d, dv d, Coninuiy: ( dv)( ) dv omenum r r heorem: ( ( dv) ) d 3443 4 q m dv d dv llievi

More information

Mathematics 805 Final Examination Answers

Mathematics 805 Final Examination Answers . 5 poins Se he Weiersrss M-es. Mhemics 85 Finl Eminion Answers Answer: Suppose h A R, nd f n : A R. Suppose furher h f n M n for ll A, nd h Mn converges. Then f n converges uniformly on A.. 5 poins Se

More information

Modeling Data Containing Outliers using ARIMA Additive Outlier (ARIMA-AO)

Modeling Data Containing Outliers using ARIMA Additive Outlier (ARIMA-AO) Journl of Physics: Conference Series PAPER OPEN ACCESS Modeling D Conining Ouliers using ARIMA Addiive Oulier (ARIMA-AO) To cie his ricle: Ansri Sleh Ahmr e l 018 J. Phys.: Conf. Ser. 954 01010 View he

More information

- The whole joint distribution is independent of the date at which it is measured and depends only on the lag.

- The whole joint distribution is independent of the date at which it is measured and depends only on the lag. Saionary Processes Sricly saionary - The whole join disribuion is indeenden of he dae a which i is measured and deends only on he lag. - E y ) is a finie consan. ( - V y ) is a finie consan. ( ( y, y s

More information

The solution is often represented as a vector: 2xI + 4X2 + 2X3 + 4X4 + 2X5 = 4 2xI + 4X2 + 3X3 + 3X4 + 3X5 = 4. 3xI + 6X2 + 6X3 + 3X4 + 6X5 = 6.

The solution is often represented as a vector: 2xI + 4X2 + 2X3 + 4X4 + 2X5 = 4 2xI + 4X2 + 3X3 + 3X4 + 3X5 = 4. 3xI + 6X2 + 6X3 + 3X4 + 6X5 = 6. [~ o o :- o o ill] i 1. Mrices, Vecors, nd Guss-Jordn Eliminion 1 x y = = - z= The soluion is ofen represened s vecor: n his exmple, he process of eliminion works very smoohly. We cn elimine ll enries

More information

Caution on causality analysis of ERP data

Caution on causality analysis of ERP data 4h Inernionl Conference on Mechronics, Merils, Cheisry nd Copuer Engineering (ICMMCCE 05) Cuion on cusliy nlysis of ERP d Jikn ue,, Snqing Hu,b, Jinhi Zhng, Wnzeng Kong College of Copuer Science, Hngzhou

More information

Multi-Input Intervention Analysis for Evaluating of the Domestic Airline Passengers in an International Airport

Multi-Input Intervention Analysis for Evaluating of the Domestic Airline Passengers in an International Airport Science Journl of Applied Mhemics nd Sisics 7; 5(3): -6 hp://www.sciencepublishinggroup.com//sms doi:.648/.sms.753.3 ISSN: 376-949 (Prin); ISSN: 376-953 (Online) Muli-Inpu Inervenion Anlysis for Evluing

More information

Advanced Integration Techniques: Integration by Parts We may differentiate the product of two functions by using the product rule:

Advanced Integration Techniques: Integration by Parts We may differentiate the product of two functions by using the product rule: Avance Inegraion Techniques: Inegraion by Pars We may iffereniae he prouc of wo funcions by using he prouc rule: x f(x)g(x) = f (x)g(x) + f(x)g (x). Unforunaely, fining an anierivaive of a prouc is no

More information

Chapter 2: Evaluative Feedback

Chapter 2: Evaluative Feedback Chper 2: Evluive Feedbck Evluing cions vs. insrucing by giving correc cions Pure evluive feedbck depends olly on he cion ken. Pure insrucive feedbck depends no ll on he cion ken. Supervised lerning is

More information

SUPPLEMENTARY NOTES ON THE CONNECTION FORMULAE FOR THE SEMICLASSICAL APPROXIMATION

SUPPLEMENTARY NOTES ON THE CONNECTION FORMULAE FOR THE SEMICLASSICAL APPROXIMATION Physics 8.06 Apr, 2008 SUPPLEMENTARY NOTES ON THE CONNECTION FORMULAE FOR THE SEMICLASSICAL APPROXIMATION c R. L. Jffe 2002 The WKB connection formuls llow one to continue semiclssicl solutions from n

More information

Technical Appendix to Modeling Movie Lifecycles and Market Share. All our models were estimated using Markov Chain Monte Carlo simulation (MCMC).

Technical Appendix to Modeling Movie Lifecycles and Market Share. All our models were estimated using Markov Chain Monte Carlo simulation (MCMC). Technical Appenix o Moeling Movie Lifecycles an Marke Share Deman Moel All our moels were esimae using Markov Chain Mone Carlo simulaion (MCMC). This meho is wiely use in he markeing leraure an is escribe

More information

Homework 5 for BST 631: Statistical Theory I Solutions, 09/21/2006

Homework 5 for BST 631: Statistical Theory I Solutions, 09/21/2006 Homewok 5 fo BST 63: Sisicl Theoy I Soluions, 9//6 Due Time: 5:PM Thusy, on 9/8/6. Polem ( oins). Book olem.8. Soluion: E = x f ( x) = ( x) f ( x) + ( x ) f ( x) = xf ( x) + xf ( x) + f ( x) f ( x) Accoing

More information

IX.1.1 The Laplace Transform Definition 700. IX.1.2 Properties 701. IX.1.3 Examples 702. IX.1.4 Solution of IVP for ODEs 704

IX.1.1 The Laplace Transform Definition 700. IX.1.2 Properties 701. IX.1.3 Examples 702. IX.1.4 Solution of IVP for ODEs 704 Chper IX The Inegrl Trnform Mehod IX. The plce Trnform November 4, 7 699 IX. THE APACE TRANSFORM IX.. The plce Trnform Definiion 7 IX.. Properie 7 IX..3 Emple 7 IX..4 Soluion of IVP for ODE 74 IX..5 Soluion

More information

5.4, 6.1, 6.2 Handout. As we ve discussed, the integral is in some way the opposite of taking a derivative. The exact relationship

5.4, 6.1, 6.2 Handout. As we ve discussed, the integral is in some way the opposite of taking a derivative. The exact relationship 5.4, 6.1, 6.2 Hnout As we ve iscusse, the integrl is in some wy the opposite of tking erivtive. The exct reltionship is given by the Funmentl Theorem of Clculus: The Funmentl Theorem of Clculus: If f is

More information

r = cos θ + 1. dt ) dt. (1)

r = cos θ + 1. dt ) dt. (1) MTHE 7 Proble Set 5 Solutions (A Crdioid). Let C be the closed curve in R whose polr coordintes (r, θ) stisfy () Sketch the curve C. r = cos θ +. (b) Find pretriztion t (r(t), θ(t)), t [, b], of C in polr

More information

!" #$% &"' (!" (C-table) Kumer

! #$% &' (! (C-table) Kumer 5 8 [9] ARMA,! ** % & ' * #,-! #$% &'! ARMA, ' - / #'! /! - 4$!,- - - '$ #!!! ' - 78 & 5! 6! #$ &'! %,- 9 5 # 6

More information

Modeling Economic Time Series with Stochastic Linear Difference Equations

Modeling Economic Time Series with Stochastic Linear Difference Equations A. Thiemer, SLDG.mcd, 6..6 FH-Kiel Universiy of Applied Sciences Prof. Dr. Andreas Thiemer e-mail: andreas.hiemer@fh-kiel.de Modeling Economic Time Series wih Sochasic Linear Difference Equaions Summary:

More information

White noise processes

White noise processes Whie noise processes A d-dimensional ime series X = {, Z} is said o be whie noise wih mean 0 and covariance marix Σ, if WN(0, Σ), E = 0, E( ) = Σ, E( X( + u) ) = 0 for u 0. Example: iid N (0, 1) 3 2 1

More information

Optimization and Application of initial Value of Non-equidistant New Information GM(1,1) Model

Optimization and Application of initial Value of Non-equidistant New Information GM(1,1) Model IJCSI Inernionl Journl of Copuer Science Issues, Vol., Issue, No, Mrch 3 ISSN Prin: 694-84 ISSN Online: 694-784 www.ijcsi.org 8 Opiizion nd Applicion of iniil Vlue of Non-equidisn New Inforion GM, Model

More information

REAL ANALYSIS I HOMEWORK 3. Chapter 1

REAL ANALYSIS I HOMEWORK 3. Chapter 1 REAL ANALYSIS I HOMEWORK 3 CİHAN BAHRAN The quesions re from Sein nd Shkrchi s e. Chper 1 18. Prove he following sserion: Every mesurble funcion is he limi.e. of sequence of coninuous funcions. We firs

More information

Technical Vibration - text 2 - forced vibration, rotational vibration

Technical Vibration - text 2 - forced vibration, rotational vibration Technicl Viion - e - foced viion, oionl viion 4. oced viion, viion unde he consn eenl foce The viion unde he eenl foce. eenl The quesion is if he eenl foce e is consn o vying. If vying, wh is he foce funcion.

More information

THEORY OF CUMULATIVE FUEL CONSUMPTION BY LPG POWERED CARS

THEORY OF CUMULATIVE FUEL CONSUMPTION BY LPG POWERED CARS Journal of KONES Powerrain an Transor, Vol. 22, No. 4 205 THEORY OF CUMULATIVE FUEL CONSUMPTION BY LPG POWERED CARS Lech Jerzy Sinik Wroclaw Universiy of Technology Faculy of Mechanical Engineering Wysianskiego

More information

DETERMINISTIC TREND / DETERMINISTIC SEASON MODEL

DETERMINISTIC TREND / DETERMINISTIC SEASON MODEL DTRMINISTIC TRND / DTRMINISTIC SASON MODL Professor Toms B. Fomby Deprmen of conomics Souern Meodis Universiy Dlls, TX June 008 Appendix B on NP Trend Tess Added Sep. 00 I. Inroducion Te Deerminisic Trend

More information

Let. x y. denote a bivariate time series with zero mean.

Let. x y. denote a bivariate time series with zero mean. Linear Filer Le x y : T denoe a bivariae ime erie wih zero mean. Suppoe ha he ime erie {y : T} i conruced a follow: y a x The ime erie {y : T} i aid o be conruced from {x : T} by mean of a Linear Filer.

More information

Chapter Three Systems of Linear Differential Equations

Chapter Three Systems of Linear Differential Equations Chaper Three Sysems of Linear Differenial Equaions In his chaper we are going o consier sysems of firs orer orinary ifferenial equaions. These are sysems of he form x a x a x a n x n x a x a x a n x n

More information

A Time Truncated Improved Group Sampling Plans for Rayleigh and Log - Logistic Distributions

A Time Truncated Improved Group Sampling Plans for Rayleigh and Log - Logistic Distributions ISSNOnline : 39-8753 ISSN Prin : 347-67 An ISO 397: 7 Cerified Orgnizion Vol. 5, Issue 5, My 6 A Time Trunced Improved Group Smpling Plns for Ryleigh nd og - ogisic Disribuions P.Kvipriy, A.R. Sudmni Rmswmy

More information

Optimality of Myopic Policy for a Class of Monotone Affine Restless Multi-Armed Bandit

Optimality of Myopic Policy for a Class of Monotone Affine Restless Multi-Armed Bandit Univeriy of Souhern Cliforni Opimliy of Myopic Policy for Cl of Monoone Affine Rele Muli-Armed Bndi Pri Mnourifrd USC Tr Jvidi UCSD Bhkr Krihnmchri USC Dec 0, 202 Univeriy of Souhern Cliforni Inroducion

More information

Exact Minimization of # of Joins

Exact Minimization of # of Joins A Quer Rewriing Algorihm: Ec Minimizion of # of Joins Emple (movie bse) selec.irecor from movie, movie, movie m3, scheule, scheule s2 where.irecor =.irecor n.cor = m3.cor n.ile =.ile n m3.ile = s2.ile

More information

RESPONSE UNDER A GENERAL PERIODIC FORCE. When the external force F(t) is periodic with periodτ = 2π

RESPONSE UNDER A GENERAL PERIODIC FORCE. When the external force F(t) is periodic with periodτ = 2π RESPONSE UNDER A GENERAL PERIODIC FORCE When he exernl force F() is periodic wih periodτ / ω,i cn be expnded in Fourier series F( ) o α ω α b ω () where τ F( ) ω d, τ,,,... () nd b τ F( ) ω d, τ,,... (3)

More information

MAT 266 Calculus for Engineers II Notes on Chapter 6 Professor: John Quigg Semester: spring 2017

MAT 266 Calculus for Engineers II Notes on Chapter 6 Professor: John Quigg Semester: spring 2017 MAT 66 Clculus for Engineers II Noes on Chper 6 Professor: John Quigg Semeser: spring 7 Secion 6.: Inegrion by prs The Produc Rule is d d f()g() = f()g () + f ()g() Tking indefinie inegrls gives [f()g

More information

Y 0.4Y 0.45Y Y to a proper ARMA specification.

Y 0.4Y 0.45Y Y to a proper ARMA specification. HG Jan 04 ECON 50 Exercises II - 0 Feb 04 (wih answers Exercise. Read secion 8 in lecure noes 3 (LN3 on he common facor problem in ARMA-processes. Consider he following process Y 0.4Y 0.45Y 0.5 ( where

More information

22.615, MHD Theory of Fusion Systems Prof. Freidberg Lecture 9: The High Beta Tokamak

22.615, MHD Theory of Fusion Systems Prof. Freidberg Lecture 9: The High Beta Tokamak .65, MHD Theory of Fusion Sysems Prof. Freidberg Lecure 9: The High e Tokmk Summry of he Properies of n Ohmic Tokmk. Advnges:. good euilibrium (smll shif) b. good sbiliy ( ) c. good confinemen ( τ nr )

More information

Surds and Indices. Surds and Indices. Curriculum Ready ACMNA: 233,

Surds and Indices. Surds and Indices. Curriculum Ready ACMNA: 233, Surs n Inies Surs n Inies Curriulum Rey ACMNA:, 6 www.mthletis.om Surs SURDS & & Inies INDICES Inies n surs re very losely relte. A numer uner (squre root sign) is lle sur if the squre root n t e simplifie.

More information

Box-Jenkins Modelling of Nigerian Stock Prices Data

Box-Jenkins Modelling of Nigerian Stock Prices Data Greener Journal of Science Engineering and Technological Research ISSN: 76-7835 Vol. (), pp. 03-038, Sepember 0. Research Aricle Box-Jenkins Modelling of Nigerian Sock Prices Daa Ee Harrison Euk*, Barholomew

More information

IX.1.1 The Laplace Transform Definition 700. IX.1.2 Properties 701. IX.1.3 Examples 702. IX.1.4 Solution of IVP for ODEs 704

IX.1.1 The Laplace Transform Definition 700. IX.1.2 Properties 701. IX.1.3 Examples 702. IX.1.4 Solution of IVP for ODEs 704 Chper IX The Inegrl Trnform Mehod IX. The plce Trnform November 6, 8 699 IX. THE APACE TRANSFORM IX.. The plce Trnform Definiion 7 IX.. Properie 7 IX..3 Emple 7 IX..4 Soluion of IVP for ODE 74 IX..5 Soluion

More information

Design flood calculation for ungauged small basins in China

Design flood calculation for ungauged small basins in China 236 Preicions in Ungauge Basins: PUB Kick-off (Proceeings of he PUB Kick-off meeing hel in Brasilia, 20 22 November 2002). IAHS Publ. 309, 2007. Design floo calculaion for ungauge small basins in China

More information

Physics 240: Worksheet 16 Name

Physics 240: Worksheet 16 Name Phyic 4: Workhee 16 Nae Non-unifor circular oion Each of hee proble involve non-unifor circular oion wih a conan α. (1) Obain each of he equaion of oion for non-unifor circular oion under a conan acceleraion,

More information

Circle the single best answer for each multiple choice question. Your choice should be made clearly.

Circle the single best answer for each multiple choice question. Your choice should be made clearly. TEST #1 STA 4853 March 6, 2017 Name: Please read the following directions. DO NOT TURN THE PAGE UNTIL INSTRUCTED TO DO SO Directions This exam is closed book and closed notes. There are 32 multiple choice

More information

EE3723 : Digital Communications

EE3723 : Digital Communications EE373 : Digial Communicaions Week 6-7: Deecion Error Probabiliy Signal Space Orhogonal Signal Space MAJU-Digial Comm.-Week-6-7 Deecion Mached filer reduces he received signal o a single variable zt, afer

More information

Problems on transformer main dimensions and windings

Problems on transformer main dimensions and windings Probles_Trn_winding Probles on rnsforer in diensions nd windings. Deerine he in diensions of he core nd window for 500 ka, /400, 50Hz, Single phse core ype, oil iersed, self cooled rnsforer. Assue: Flux

More information

Problem set 2 for the course on. Markov chains and mixing times

Problem set 2 for the course on. Markov chains and mixing times J. Seif T. Hirscher Soluions o Proble se for he course on Markov chains and ixing ies February 7, 04 Exercise 7 (Reversible chains). (i) Assue ha we have a Markov chain wih ransiion arix P, such ha here

More information

The order of reaction is defined as the number of atoms or molecules whose concentration change during the chemical reaction.

The order of reaction is defined as the number of atoms or molecules whose concentration change during the chemical reaction. www.hechemisryguru.com Re Lw Expression Order of Recion The order of recion is defined s he number of oms or molecules whose concenrion chnge during he chemicl recion. Or The ol number of molecules or

More information

Sturm-Liouville Theory

Sturm-Liouville Theory LECTURE 1 Sturm-Liouville Theory In the two preceing lectures I emonstrte the utility of Fourier series in solving PDE/BVPs. As we ll now see, Fourier series re just the tip of the iceerg of the theory

More information

How to Prove the Riemann Hypothesis Author: Fayez Fok Al Adeh.

How to Prove the Riemann Hypothesis Author: Fayez Fok Al Adeh. How o Prove he Riemnn Hohesis Auhor: Fez Fok Al Adeh. Presiden of he Srin Cosmologicl Socie P.O.Bo,387,Dmscus,Sri Tels:963--77679,735 Emil:hf@scs-ne.org Commens: 3 ges Subj-Clss: Funcionl nlsis, comle

More information

S Radio transmission and network access Exercise 1-2

S Radio transmission and network access Exercise 1-2 S-7.330 Rdio rnsmission nd nework ccess Exercise 1 - P1 In four-symbol digil sysem wih eqully probble symbols he pulses in he figure re used in rnsmission over AWGN-chnnel. s () s () s () s () 1 3 4 )

More information

Seminar 5 Sustainability

Seminar 5 Sustainability Seminar 5 Susainabiliy Soluions Quesion : Hyperbolic Discouning -. Suppose a faher inheris a family forune of 0 million NOK an he wans o use some of i for himself (o be precise, he share ) bu also o beques

More information

Chapter 10. Simple Harmonic Motion and Elasticity. Goals for Chapter 10

Chapter 10. Simple Harmonic Motion and Elasticity. Goals for Chapter 10 Chper 0 Siple Hronic Moion nd Elsiciy Gols or Chper 0 o ollow periodic oion o sudy o siple hronic oion. o sole equions o siple hronic oion. o use he pendulu s prooypicl syse undergoing siple hronic oion.

More information

EXISTENCE AND UNIQUENESS OF SOLUTIONS FOR A SECOND-ORDER ITERATIVE BOUNDARY-VALUE PROBLEM

EXISTENCE AND UNIQUENESS OF SOLUTIONS FOR A SECOND-ORDER ITERATIVE BOUNDARY-VALUE PROBLEM Elecronic Journl of Differenil Equions, Vol. 208 (208), No. 50, pp. 6. ISSN: 072-669. URL: hp://ejde.mh.xse.edu or hp://ejde.mh.un.edu EXISTENCE AND UNIQUENESS OF SOLUTIONS FOR A SECOND-ORDER ITERATIVE

More information