Laguerre wavelet and its programming

Size: px
Start display at page:

Download "Laguerre wavelet and its programming"

Transcription

1 Iraioal Joural o Mahaics rds ad chology (IJM) Volu 49 Nubr Spbr 7 agurr l ad is prograig B Sayaaraya Y Pragahi Kuar Asa Abdullah 3 3 Dpar o Mahaics Acharya Nagarjua Uivrsiy Adhra pradsh Idia Dpar o Mahaics Collg o Naural ad Copuaioal Scics Adigra Uivrsiy Adigra Ehiopia Absrac I his papr h auhor cosrucs w agurr l ucio wih is progra by usig MAAB progra Also h auhor drivaiv ad igraio wih is powrs i rs arics ar cosrucd h icicy o h abov ucios hrough h us o hs vrbs i h soluio o so xapls ha will show us h validiy o wha w hav said Morovr so o h hypohsis was provd as h hors o orhogoaliy ad Covrg Kywords- agurr ls MAAB progra opraioal arix o igraio opraioal arix o drivaiv ad powrs i rs I INRODUCION Firs w show ha h ors ha cu daa io dir rqucy copos ar ahaical ucios [ ] I is show hrough ay sourcs ha ach copo will b sudid wih a rsoluio proporioal o is rag whr hy hav radiioal Fourir hods i cas aalysis i dir Scic or xapl physics [9 ] Ovr h pas yars hr hav b xchags bw sciiic ilds ha iclud h dvlop o ors idpdly i h ilds o girig scic ad gology [3-5] Irchags bw hs ilds durig h pas yars hav ld o ay w l applicaios such as iag coprssio urbulc hua visio radar ad arhqua prdicio [6 3] Wavl aalysis is a powrul ahaical ool ha has b usd widly i iag digial procssig quau ild hory [5-7] urical aalysis ad ay ohr ilds i rc yars oday hr ar ay wors o ls hods or approxiaig h soluio o h probls [8 9] such as Haar ls hod [8] SAC ls hod Haroic ls hod irs ad scod Chbyshv ls [4] ad gdr ls hod [7] I h prs papr gav so ipora characrisics o agurr polyoials wih is will b giv icludig w propris Procssig iag is also discussd i his papr II AGUERRE POYNOMIAS AND IS PROPERIES agurr s dirial quaio: h dirial quaio o agurr s polypial giv by xy " x y ' y () whr =3 his quaio has polyoial soluios calld agurr polyoials is giv by x d x x x () dx Which is also rrrd o as Rodrigu s orula or h agurr polyoials h irs w agurr polyoials ar x x x 3 x x 4x x 6 8x 9x x (3) 3 whr x is a polyoial o dgr Prograig agurr polyoial: By usig Malab ucio =ag() i == =; ls Su = ; or = : su = su+(- )^*acorial()*acorial()*^/ (acorial()*acorial()*acorial(-)); d =su; Ed 3 So ipora propris o agurr polyoials: I h ollowig w lis so propris o h agurr polyoials Graig ucio: x (4)! Rcurrc orula: x x x (5) x x x (6) x x x x (7) ISSN: hp://wwwijjouralorg Pag 9

2 Iraioal Joural o Mahaics rds ad chology (IJM) Volu 49 Nubr Spbr 7 3 Orhogoaliy x x x (8) 4 Sris xpasios: A dx! I x A x! i i h x x dx x (9) 4 Miscllaous orhogoal polyoials ad hir propris: hr ar ay ohr xapls o orhogoal polyoials So o h or ipora os oghr wih hir propris ar giv i h ollowig lis Associad agurr Polyoials x d x x dx () ad saisyig h quaio x y x y y () I h x x w hav x x () x x! x dx p dx p! II AGUERRE WAVEES p (3) I his scio w cosrucd agurr l ro h aily ucio r sr s or sr R s s (4) whr h ls M M ar h basis ucios orhogoal o h [] 3 Cosrucd agurr Wavls: agurr l is dod by (ag) is h yp o ls usd or solvig dirial quaios igral quaios variaio probls dir scics ad girig probls as wll as racioal dirial quaios agurr l hav our argus ordr or agurr polyoials ad oralizd is is ad i I w dilaio by parar s raslaio by parar r ad x us rasor x i (4) h w will g h ollowig quaio ohrwis (5) whr ~! or = 3 Prograig o agurr ls: By MAAB progra w ca g abov ucios or ls ucio o ordr by h ollowig algorihs Cas : ucios o h irval [ 5) ucio = ag() i = = *sqr() ls s = ; or = : s = s + (-) ^ *acorial()*acorial()* ( ddd*) ^/ (acorial()*acorial()*acorial(-)); d =(*sqr()/acorial())*s Ed Cas : ucios o h irval [ 5) ucio = ag() i == =*sqr() ls s = ; or = : s = s +(- )^*acorial()*acorial()*(ddd()) ^/ (acorial()*acorial()*acorial(-)); d =(*sqr()/acorial())*s Ed IV ORHOGONAIY OF AGUERRE WAVEES Fro scio (3) ad quaio (8) w ow x has orhogoaliy wih rspc o h wigh ucio w h s o lagurr ls ar h orhogoal wih rspc o wigh ucio o h irval w I is a sp ucio aig valus ls o 5 ad 5 rspcivly whr is ow ha ay coiuous ucio approxiad uiorly by agurr ucio W will did by usig h agurr ls Dilaios ad ISSN: hp://wwwijjouralorg Pag 3

3 Iraioal Joural o Mahaics rds ad chology (IJM) Volu 49 Nubr Spbr 7 raslaios o h ucio di a R orhogoal basis i h spac o all squar igrabl ucios his as ha ay l i R ay b rprsd as a liar cobiaio (possibly i ii) o hs basis ucios asy hor : h orhogoal o is o chc I is appar ha d (6) Whvr ad is o saisid siulaously I o zro valus o h l (say ) h ar coaid i h s whr h l coais agurr ucio h ha as igral qual o zro I bu h a las o acor i h produc is zro hus h ucio is orhogoal d d i = 8! i (7) V FUNCION APPROXIMAION A ucio approxiaio xpadd as ay b A whr A (8) I quaio (8) do h ir produc wih wigh ucio w o h Hilbr Spac I h iii sris i abov quaio is rucad h quaio (7) ca b wri as (9) M A A Whr A ad giv by ar M arics A A A A A A A M M () M M M () VI SHIFED AGUERRE WAVEES Shiig h agurr ls by usig polyoials h quaio (5) will bco * i ohrwis () Whr or M! M should o i dalig wih agurr ls h wigh ucio ad raslad w w hav o dilad a ucio ovr ca b xpadd as A whr A did (3) I iii sris i (3) is rucad h i ca b wri as M A A (4) o ar M whr A ad arics giv by A A A A MA A M (5) A A M M ISSN: hp://wwwijjouralorg Pag 3

4 Iraioal Joural o Mahaics rds ad chology (IJM) Volu 49 Nubr Spbr 7 (6) hor : M M A ucio N wih liid scod drivaiv say b liid scod say N ca b widd as a uliid aggrga o agurr ls ad h sris covrgs uiorly o ls) or = ad M= by diriaio quaio () Ad h Eploy Marix o Drivaiv or agurr Wavl ha is N A A N 3 4 (7) 4 4 Proo o h hor: D ag() w hav A w d ad A w d O Dag() 4 i by subsiuig O x i yilds ad O x A x x d (8) x A x x dx 3 x whvr x by copl igraio N () is A N 3 his copls h proo o h hor VII EMPOYMEN MARICES FOR AGUERRE WAVEE 7 h Eploy Marix o Drivaiv or agurr l: I his scio w us shid agurr ls i ploy arix o drivaiv or agurr ls Firs w cosruc 6 6 arix ad i dod by D ag() (drivaiv or agurr Fig (h Eploy Marix o Drivaiv or agurr Wavl) hor 3: b h agurr ls vcor did i quaio (6) h drivaiv o his vcor ca b xprssd as d D d ag whr ISSN: hp://wwwijjouralorg Pag 3

5 Iraioal Joural o Mahaics rds ad chology (IJM) Volu 49 Nubr Spbr 7 D is h ag M 4 D ag i which is is M M D ag arix ad i s h l is did as ollows (M ) ohrwis Proo: By usig shid agurr polyoials i h h l o vcor ca b wri as! ohrwis (3) M M ad (9) Diriaio quaio (9) d d! ohrwis ha is M M M So is agurr ls xpasio has h ollowig ro d d i a (3) his iplis ha h ploy D is arix ag() D ag a bloc arix as did i (7) orovr x d d d d M i i or M Cosquly h irs row o arix is zro Now by usig h ollowig quaio g whr (3) C l 3 l i Cli l l Subsiuig quaio (3) ad (3) i quaio (3) d Cli d! i (33) (34) Choos 5 d d M D quaio ag holds 7 Eploy Marix o Igraio or agurr Wavls: I his scio Igraio or agurr ls ar discussd For his ploy arix o igraio or agurr ls P Now id 6 6 arix P I quaio (5) or M=3 h six basis ucios ar giv by: ad (35) By igraio h abov six ucios ro o ad usig quaio (8) w obai d 4 3 d d 4 4 ISSN: hp://wwwijjouralorg Pag 33

6 Iraioal Joural o Mahaics rds ad chology (IJM) Volu 49 Nubr Spbr 7 d 4 3 d d d P6 6 6 whr hus 6 By usig abov quaios h opraioal arix o igraio P is Eploy Marix o Igraio or agurr Wavls P ag A33 O3 3 P ag O3 3 A 33 Fig (h Eploy Marix o Igraio or agurr Wavl) 73 Powrs i rs o agurr Wavls: I his scio w will driv powrs i rs o agurr Wavls or M 3 Ad is h oralizd i will driv h powrs I rs o agurr Wavls which hlp o solv Probls M 3 3 basis Fucios ar giv by: I I arix or h powrs o ca b rwri as ollows Z W ad Whr Z W 5 Z ad W 5 Powrs i rs agurr Wavls: Cosrucig h opraio arix o igraio ad diriaio ha ca b usd i solvig ay probls which ar illusrad i h ollowig xapls VIII APPICAION OF MARICES D ag AND P ag FOR SOVING CACUUS OF VARIAIONA PROBEMS I ordr o solv liar or oliar dirial quaios by usig h ploy arics D ag ad P ag so urical xapls illusra h Procdur [8] I ordr o solv liar or oliar ISSN: hp://wwwijjouralorg Pag 34

7 Iraioal Joural o Mahaics rds ad chology (IJM) Volu 49 Nubr Spbr 7 X Exac soluio Approxia soluio =M=3 Approxia soluio =M= dirial quaio by usig h abov opraioal arics so urical xapls illusra h procdur which will bgi wih x x h xac soluio U x x abl Shows h urical rsuls or his xapl wih 4 M 3 wih rror M 4 rror 5 ar copard wih xac soluio graphically i ig3 abl shows so urical rsuls or xapl () i y A i i i y A d y A P y i i i i i3 y A P y y y Exapl () Cosidr h ollowig variaio probl [8] i y y 8y Wih h boudary codiios d y y h corrspodig Eulr agrag quaio is y y h h xac soluio or his Probl is y wih h abov boudary codiios o solv his probl assuig y A P ha ag Fid y y o go y A D ag y A D ag will copl his xapl s [8] jus rplac old arics by ()s' arics o igraio ad drivaiv rachd h xac soluio Exapl (): Cosidr h ollowig Volrra igro dirial quaio (VIDE) [4] [5] Fig3 (3D o rsuls o xapl ()) U U x x x x U U d wih ISSN: hp://wwwijjouralorg Pag 35

8 Iraioal Joural o Mahaics rds ad chology (IJM) Volu 49 Nubr Spbr 7 wih boudary codiios o solv his probl by usig P ag will solv his probl ad rachd h xac soluio Fig5 (copar h rsuls wih xac soluio o xapl ()) IX CONCUSION h agurr ls opraioal arics o igraios wih h aid o spcral ad collocaio hods ar applid o solv ay probls h ls hod auhorizs h ood o vry as algorihs wh copard o h algorihs app roach usd (agurr Polyoials) Nurical rsuls wih coparisos ar giv o coir h rliabiliy o h proposd hod or solvig ay probls Exapl (3): Cosidr h ollowig variaio probl[8] y y y d Mi wih h boudary codiios y y h corrspodig Eulr agrag quaio is is y y h xac soluio or his probl y xac soluio Firs Chbyshv ls Scod ls Chbyshv agurr ls ISSN: hp://wwwijjouralorg Pag 36

9 Iraioal Joural o Mahaics rds ad chology (IJM) Volu 49 Nubr Spbr 7 X REFERENCES AA Asa Nurical soluio o Opial probls usig w hird id Chbyshv Wavls Opraioal arix o igraio Eg & c Joural 3(): AA Asa Dirc hod or Solvig Noliar Variaioal Probls by Usig Hri Wavls Baghdad Scic Joural Vol() 5 3 AA Asa A Algorih or h Ordr Igro-Dirial Equaios by Usig Hri Wavls Fucios Baghdad Scic Joural Vol(3) 4 4 AA Asa l collocaio hod or solvig igrodirial quaio IOSR Joural o Egirig Vol 5(3) PP B Asady M Kajai AH Vchh A Hydari Solvig Scod Kid Igral Equaios wih Hybrid Fourir ad Blocpuls Fucios Appl Mah Copu CF Ch CH Hsiao A Walsh Sris Dirc Mhod or Solvig Variaioal Probls J Frali Isi RY Chag M Wag Shid gdr Dirc Mhod or Variaioal Probls J Opi hory Appl IR Horg JH Chou Shid Chbyshv Sris Dirc Mhod or Solvig Variaioal Probls I J Sys Sci C Hwag YP Shih Opial Corol o Dlay Syss via Bloc-puls Fucios J Opi hory Appl C Hwag YP Shih agurr Sris Dirc Mhod or Variaioal Probls J Opi hory Appl C Hwag YP Shih Soluio o Igral Equaios via agurr Polyoials J Copu Elc Egi CH Hsiao Haar Wavl Dirc Mhod or Solvig Variaioal Probls Mah Copu Siul H Jddu Dirc Soluio o Noliar Opial Corol Probls Usig Quasiliarizaio ad Chbyshv Polyoials J Frali Is M Razzaghi Fourir Sris Dirc Mhod or Variaioal Probls I J Corol S N Shihab AA Asaa Nurical Soluio o Calculus o Variaios by usig h Scod Chbyshv Wavls Eg & ch Joural 3(8) S N Shihab AA Asa So Nw Rlaioships Bw h Drivaivs o Firs ad Scod Chbyshv Wavls Iraioal Joural o Egirig Busiss ad Erpris Applicaios (IJEBEA) () S S Najb & M A Sarha Covrgc Aalysis o shid Fourh id Chbyshv Wavls IOSR Joural o Mahaics Volu () S N Shihab AAAsa So Approxia Algoihs For Variaioal Probls(Boo) 9 SN Shihab AAAsa Solvig Opial Corol iar Syss by Usig Nw hird id Chbyshv Wavls Opraioal Marix o Drivaiv Baghdad Scic Joural Vol() 4 ISSN: hp://wwwijjouralorg Pag 37

Numerical Simulation for the 2-D Heat Equation with Derivative Boundary Conditions

Numerical Simulation for the 2-D Heat Equation with Derivative Boundary Conditions IOSR Joural of Applid Chmisr IOSR-JAC -ISSN: 78-576.Volum 9 Issu 8 Vr. I Aug. 6 PP 4-8 www.iosrjourals.org Numrical Simulaio for h - Ha Equaio wih rivaiv Boudar Codiios Ima. I. Gorial parm of Mahmaics

More information

Chapter 3 Linear Equations of Higher Order (Page # 144)

Chapter 3 Linear Equations of Higher Order (Page # 144) Ma Modr Dirial Equaios Lcur wk 4 Jul 4-8 Dr Firozzama Darm o Mahmaics ad Saisics Arizoa Sa Uivrsi This wk s lcur will covr har ad har 4 Scios 4 har Liar Equaios o Highr Ordr Pag # 44 Scio Iroducio: Scod

More information

Part B: Transform Methods. Professor E. Ambikairajah UNSW, Australia

Part B: Transform Methods. Professor E. Ambikairajah UNSW, Australia Par B: rasform Mhods Profssor E. Ambikairaah UNSW, Ausralia Chapr : Fourir Rprsaio of Sigal. Fourir Sris. Fourir rasform.3 Ivrs Fourir rasform.4 Propris.4. Frqucy Shif.4. im Shif.4.3 Scalig.4.4 Diffriaio

More information

Chapter 11 INTEGRAL EQUATIONS

Chapter 11 INTEGRAL EQUATIONS hapr INTERAL EQUATIONS hapr INTERAL EUATIONS Dcmbr 4, 8 hapr Igral Eqaios. Normd Vcor Spacs. Eclidia vcor spac. Vcor spac o coios cios ( ). Vcor Spac L ( ) 4. achy-byaowsi iqaliy 5. iowsi iqaliy. Liar

More information

Fourier Techniques Chapters 2 & 3, Part I

Fourier Techniques Chapters 2 & 3, Part I Fourir chiqus Chaprs & 3, Par I Dr. Yu Q. Shi Dp o Elcrical & Compur Egirig Nw Jrsy Isiu o chology Email: shi@i.du usd or h cours: , 4 h Ediio, Lahi ad Dog, Oord

More information

The Development of Suitable and Well-founded Numerical Methods to Solve Systems of Integro- Differential Equations,

The Development of Suitable and Well-founded Numerical Methods to Solve Systems of Integro- Differential Equations, Shiraz Uivrsiy of Tchology From h SlcdWorks of Habibolla Laifizadh Th Dvlopm of Suiabl ad Wll-foudd Numrical Mhods o Solv Sysms of Igro- Diffrial Equaios, Habibolla Laifizadh, Shiraz Uivrsiy of Tchology

More information

Response of LTI Systems to Complex Exponentials

Response of LTI Systems to Complex Exponentials 3 Fourir sris coiuous-im Rspos of LI Sysms o Complx Expoials Ouli Cosidr a LI sysm wih h ui impuls rspos Suppos h ipu sigal is a complx xpoial s x s is a complx umbr, xz zis a complx umbr h or h h w will

More information

Chapter 7 INTEGRAL EQUATIONS

Chapter 7 INTEGRAL EQUATIONS hapr 7 INTERAL EQUATIONS hapr 7 INTERAL EUATIONS hapr 7 Igral Eqaios 7. Normd Vcor Spacs. Eclidia vcor spac. Vcor spac o coios cios ( ). Vcor Spac L ( ) 4. ach-baowsi iqali 5. iowsi iqali 7. Liar Opraors

More information

MAT3700. Tutorial Letter 201/2/2016. Mathematics III (Engineering) Semester 2. Department of Mathematical sciences MAT3700/201/2/2016

MAT3700. Tutorial Letter 201/2/2016. Mathematics III (Engineering) Semester 2. Department of Mathematical sciences MAT3700/201/2/2016 MAT3700/0//06 Tuorial Lr 0//06 Mahmaics III (Egirig) MAT3700 Smsr Dparm of Mahmaical scics This uorial lr coais soluios ad aswrs o assigms. BARCODE CONTENTS Pag SOLUTIONS ASSIGNMENT... 3 SOLUTIONS ASSIGNMENT...

More information

( A) ( B) ( C) ( D) ( E)

( A) ( B) ( C) ( D) ( E) d Smsr Fial Exam Worksh x 5x.( NC)If f ( ) d + 7, h 4 f ( ) d is 9x + x 5 6 ( B) ( C) 0 7 ( E) divrg +. (NC) Th ifii sris ak has h parial sum S ( ) for. k Wha is h sum of h sris a? ( B) 0 ( C) ( E) divrgs

More information

Continous system: differential equations

Continous system: differential equations /6/008 Coious sysm: diffrial quaios Drmiisic modls drivaivs isad of (+)-( r( compar ( + ) R( + r ( (0) ( R ( 0 ) ( Dcid wha hav a ffc o h sysm Drmi whhr h paramrs ar posiiv or gaiv, i.. giv growh or rducio

More information

Mathematical Preliminaries for Transforms, Subbands, and Wavelets

Mathematical Preliminaries for Transforms, Subbands, and Wavelets Mahmaical Prlimiaris for rasforms, Subbads, ad Wavls C.M. Liu Prcpual Sigal Procssig Lab Collg of Compur Scic Naioal Chiao-ug Uivrsiy hp://www.csi.cu.du.w/~cmliu/courss/comprssio/ Offic: EC538 (03)5731877

More information

The Solution of Advection Diffusion Equation by the Finite Elements Method

The Solution of Advection Diffusion Equation by the Finite Elements Method Iraioal Joural of Basic & Applid Scics IJBAS-IJES Vol: o: 88 T Soluio of Advcio Diffusio Equaio by Fii Els Mod Hasa BULUT, Tolga AKTURK ad Yusuf UCAR Dpar of Maaics, Fira Uivrsiy, 9, Elazig-TURKEY Dpar

More information

Infinite Continued Fraction (CF) representations. of the exponential integral function, Bessel functions and Lommel polynomials

Infinite Continued Fraction (CF) representations. of the exponential integral function, Bessel functions and Lommel polynomials Ifii Coiu Fraio CF rraio of h oial igral fuio l fuio a Lol olyoial Coiu Fraio CF rraio a orhogoal olyoial I hi io w rall h rlaio bw ifi rurry rlaio of olyoial orroig orhogoaliy a aroria ifii oiu fraio

More information

Fourier Series: main points

Fourier Series: main points BIOEN 3 Lcur 6 Fourir rasforms Novmbr 9, Fourir Sris: mai pois Ifii sum of sis, cosis, or boh + a a cos( + b si( All frqucis ar igr mulipls of a fudamal frqucy, o F.S. ca rprs ay priodic fucio ha w ca

More information

2 Dirac delta function, modeling of impulse processes. 3 Sine integral function. Exponential integral function

2 Dirac delta function, modeling of impulse processes. 3 Sine integral function. Exponential integral function Chapr VII Spcial Fucios Ocobr 7, 7 479 CHAPTER VII SPECIAL FUNCTIONS Cos: Havisid sp fucio, filr fucio Dirac dla fucio, modlig of impuls procsss 3 Si igral fucio 4 Error fucio 5 Gamma fucio E Epoial igral

More information

ISSN: [Bellale* et al., 6(1): January, 2017] Impact Factor: 4.116

ISSN: [Bellale* et al., 6(1): January, 2017] Impact Factor: 4.116 IESRT INTERNTIONL OURNL OF ENGINEERING SCIENCES & RESERCH TECHNOLOGY HYBRID FIED POINT THEOREM FOR NONLINER DIFFERENTIL EQUTIONS Sidhshwar Sagram Bllal*, Gash Babrwa Dapk * Dparm o Mahmaics, Daaad Scic

More information

Bernstein Direct Method for Solving. Variational Problems

Bernstein Direct Method for Solving. Variational Problems Ieraioal Maheaical Foru, 5,, o. 48, 35-37 Bersei Direc Mehod for Solvig Variaioal Probles Sadeep Dixi*, Viee K. Sigh**, Ai K. Sigh*, O P. Sigh* *Depare of Applied Maheaics, Isiue of echology, Baaras Hidu

More information

An Analytical Study on Fractional Partial Differential Equations by Laplace Transform Operator Method

An Analytical Study on Fractional Partial Differential Equations by Laplace Transform Operator Method Iraioal Joural o Applid Egirig Rsarch ISSN 973-456 Volum 3 Numbr (8 pp 545-549 Rsarch Idia Publicaios hp://wwwripublicaiocom A Aalical Sud o Fracioal Parial Dirial Euaios b aplac Trasorm Opraor Mhod SKElaga

More information

1973 AP Calculus BC: Section I

1973 AP Calculus BC: Section I 97 AP Calculus BC: Scio I 9 Mius No Calculaor No: I his amiaio, l dos h aural logarihm of (ha is, logarihm o h bas ).. If f ( ) =, h f ( ) = ( ). ( ) + d = 7 6. If f( ) = +, h h s of valus for which f

More information

x, x, e are not periodic. Properties of periodic function: 1. For any integer n,

x, x, e are not periodic. Properties of periodic function: 1. For any integer n, Chpr Fourir Sri, Igrl, d Tror. Fourir Sri A uio i lld priodi i hr i o poiiv ur p uh h p, p i lld priod o R i,, r priodi uio.,, r o priodi. Propri o priodi uio:. For y igr, p. I d g hv priod p, h h g lo

More information

Ring of Large Number Mutually Coupled Oscillators Periodic Solutions

Ring of Large Number Mutually Coupled Oscillators Periodic Solutions Iraioal Joural of horical ad Mahmaical Physics 4, 4(6: 5-9 DOI: 59/jijmp446 Rig of arg Numbr Muually Coupld Oscillaors Priodic Soluios Vasil G Aglov,*, Dafika z Aglova Dparm Nam of Mahmaics, Uivrsiy of

More information

Web-appendix 1: macro to calculate the range of ( ρ, for which R is positive definite

Web-appendix 1: macro to calculate the range of ( ρ, for which R is positive definite Wb-basd Supplmary Marials for Sampl siz cosidraios for GEE aalyss of hr-lvl clusr radomizd rials by Sv Trsra, Big Lu, oh S. Prissr, Tho va Achrbrg, ad Gorg F. Borm Wb-appdix : macro o calcula h rag of

More information

Review Topics from Chapter 3&4. Fourier Series Fourier Transform Linear Time Invariant (LTI) Systems Energy-Type Signals Power-Type Signals

Review Topics from Chapter 3&4. Fourier Series Fourier Transform Linear Time Invariant (LTI) Systems Energy-Type Signals Power-Type Signals Rviw opics from Chapr 3&4 Fourir Sris Fourir rasform Liar im Ivaria (LI) Sysms Ergy-yp Sigals Powr-yp Sigals Fourir Sris Rprsaio for Priodic Sigals Dfiiio: L h sigal () b a priodic sigal wih priod. ()

More information

What Is the Difference between Gamma and Gaussian Distributions?

What Is the Difference between Gamma and Gaussian Distributions? Applid Mahmaics,,, 85-89 hp://ddoiorg/6/am Publishd Oli Fbruary (hp://wwwscirporg/joural/am) Wha Is h Diffrc bw Gamma ad Gaussia Disribuios? iao-li Hu chool of Elcrical Egirig ad Compur cic, Uivrsiy of

More information

Poisson Arrival Process

Poisson Arrival Process 1 Poisso Arrival Procss Arrivals occur i) i a mmorylss mar ii) [ o arrival durig Δ ] = λδ + ( Δ ) P o [ o arrival durig Δ ] = 1 λδ + ( Δ ) P o P j arrivals durig Δ = o Δ for j = 2,3, ( ) o Δ whr lim =

More information

Approximate solutions for the time-space fractional nonlinear of partial differential equations using reduced differential transform method

Approximate solutions for the time-space fractional nonlinear of partial differential equations using reduced differential transform method Global Joral o Pr ad Applid Mahmaics ISSN 97-768 Volm Nmbr 6 7 pp 5-6 sarch Idia Pblicaios hp://wwwripblicaiocom Approima solios or h im-spac racioal oliar o parial dirial qaios sig rdcd dirial rasorm

More information

In this section we will study periodic signals in terms of their frequency f t is said to be periodic if (4.1)

In this section we will study periodic signals in terms of their frequency f t is said to be periodic if (4.1) Fourier Series Iroducio I his secio we will sudy periodic sigals i ers o heir requecy is said o be periodic i coe Reid ha a sigal ( ) ( ) ( ) () or every, where is a uber Fro his deiiio i ollows ha ( )

More information

Poisson Arrival Process

Poisson Arrival Process Poisso Arrival Procss Arrivals occur i) i a mmylss mar ii) [ o arrival durig Δ ] = λδ + ( Δ ) P o [ o arrival durig Δ ] = λδ + ( Δ ) P o P j arrivals durig Δ = o Δ f j = 2,3, o Δ whr lim =. Δ Δ C C 2 C

More information

Overview. Review Elliptic and Parabolic. Review General and Hyperbolic. Review Multidimensional II. Review Multidimensional

Overview. Review Elliptic and Parabolic. Review General and Hyperbolic. Review Multidimensional II. Review Multidimensional Mlil idd variabls March 9 Mlidisioal Parial Dirial Eaios arr aro Mchaical Egirig 5B iar i Egirig Aalsis March 9 Ovrviw Rviw las class haracrisics ad classiicaio o arial dirial aios Probls i or ha wo idd

More information

Practice papers A and B, produced by Edexcel in 2009, with mark schemes. Practice Paper A. 5 cosh x 2 sinh x = 11,

Practice papers A and B, produced by Edexcel in 2009, with mark schemes. Practice Paper A. 5 cosh x 2 sinh x = 11, Prai paprs A ad B, produd by Edl i 9, wih mark shms Prai Papr A. Fid h valus of for whih 5 osh sih =, givig your aswrs as aural logarihms. (Toal 6 marks) k. A = k, whr k is a ral osa. 9 (a) Fid valus of

More information

DEFLECTIONS OF THIN PLATES: INFLUENCE OF THE SLOPE OF THE PLATE IN THE APLICATION OF LINEAR AND NONLINEAR THEORIES

DEFLECTIONS OF THIN PLATES: INFLUENCE OF THE SLOPE OF THE PLATE IN THE APLICATION OF LINEAR AND NONLINEAR THEORIES Procdigs of COBEM 5 Coprigh 5 b BCM 8h Iraioal Cogrss of Mchaical Egirig Novmbr 6-, 5, Ouro Pro, MG DEFLECIONS OF HIN PLES: INFLUENCE OF HE SLOPE OF HE PLE IN HE PLICION OF LINER ND NONLINER HEORIES C..

More information

ELECTROMAGNETIC COMPATIBILITY HANDBOOK 1. Chapter 12: Spectra of Periodic and Aperiodic Signals

ELECTROMAGNETIC COMPATIBILITY HANDBOOK 1. Chapter 12: Spectra of Periodic and Aperiodic Signals ELECTOMAGNETIC COMPATIBILITY HANDBOOK Chapr : Spcra of Priodic ad Apriodic Sigals. Drmi whhr ach of h followig fucios ar priodic. If hy ar priodic, provid hir fudamal frqucy ad priod. a) x 4cos( 5 ) si(

More information

Digital Signal Processing, Fall 2006

Digital Signal Processing, Fall 2006 Digital Sigal Procssig, Fall 6 Lctur 9: Th Discrt Fourir Trasfor Zhg-Hua Ta Dpartt of Elctroic Systs Aalborg Uivrsity, Dar zt@o.aau.d Digital Sigal Procssig, I, Zhg-Hua Ta, 6 Cours at a glac MM Discrt-ti

More information

Some Applications of the Poisson Process

Some Applications of the Poisson Process Applid Maaics, 24, 5, 3-37 Publishd Oli Novbr 24 i SciRs. hp://www.scirp.org/oural/a hp://dx.doi.org/.4236/a.24.59288 So Applicaios of Poisso Procss Kug-Ku s Dpar of Maaics, Ka Uivrsiy, Uio, USA Eail:

More information

OPTIMUM ORDER QUANTITY FOR DETERIORATING ITEMS IN LARGEST LIFETIME WITH PERMISSIBLE DELAY PERIOD S. C. SHARMA & VIVEK VIJAY

OPTIMUM ORDER QUANTITY FOR DETERIORATING ITEMS IN LARGEST LIFETIME WITH PERMISSIBLE DELAY PERIOD S. C. SHARMA & VIVEK VIJAY Iraioal Joural of Mahaics a opur Applicaios Rsarch (IJMAR) ISSN(P): 9-6955; ISSN(E): 9-86 Vol. 6, Issu, Aug 6, - @JPR Pv. L. OPIMUM ORDER QUANIY FOR DEERIORAING IEMS IN LARGES LIFEIME WIH PERMISSIBLE DELAY

More information

Midterm exam 2, April 7, 2009 (solutions)

Midterm exam 2, April 7, 2009 (solutions) Univrsiy of Pnnsylvania Dparmn of Mahmaics Mah 26 Honors Calculus II Spring Smsr 29 Prof Grassi, TA Ashr Aul Midrm xam 2, April 7, 29 (soluions) 1 Wri a basis for h spac of pairs (u, v) of smooh funcions

More information

Analysis of Non-Sinusoidal Waveforms Part 2 Laplace Transform

Analysis of Non-Sinusoidal Waveforms Part 2 Laplace Transform Aalyi o No-Siuoidal Wavorm Par Laplac raorm I h arlir cio, w lar ha h Fourir Sri may b wri i complx orm a ( ) C jω whr h Fourir coici C i giv by o o jωo C ( ) d o I h ymmrical orm, h Fourir ri i wri wih

More information

Modeling of the CML FD noise-to-jitter conversion as an LPTV process

Modeling of the CML FD noise-to-jitter conversion as an LPTV process Modlig of h CML FD ois-o-ir covrsio as a LPV procss Marko Alksic. Rvisio hisory Vrsio Da Comms. //4 Firs vrsio mrgd wo docums. Cyclosaioary Nois ad Applicaio o CML Frqucy Dividr Jir/Phas Nois Aalysis fil

More information

Akpan s Algorithm to Determine State Transition Matrix and Solution to Differential Equations with Mixed Initial and Boundary Conditions

Akpan s Algorithm to Determine State Transition Matrix and Solution to Differential Equations with Mixed Initial and Boundary Conditions IOSR Joural o Elcrcal ad Elcrocs Egrg IOSR-JEEE -ISSN: 78-676,p-ISSN: 3-333, Volu, Issu 5 Vr. III Sp - Oc 6, PP 9-96 www.osrourals.org kpa s lgorh o Dr Sa Traso Marx ad Soluo o Dral Euaos wh Mxd Ial ad

More information

Linear Systems Analysis in the Time Domain

Linear Systems Analysis in the Time Domain Liar Sysms Aalysis i h Tim Domai Firs Ordr Sysms di vl = L, vr = Ri, d di L + Ri = () d R x= i, x& = x+ ( ) L L X() s I() s = = = U() s E() s Ls+ R R L s + R u () = () =, i() = L i () = R R Firs Ordr Sysms

More information

Iterative Methods of Order Four for Solving Nonlinear Equations

Iterative Methods of Order Four for Solving Nonlinear Equations Itrativ Mods of Ordr Four for Solvig Noliar Equatios V.B. Kumar,Vatti, Shouri Domii ad Mouia,V Dpartmt of Egirig Mamatis, Formr Studt of Chmial Egirig Adhra Uivrsity Collg of Egirig A, Adhra Uivrsity Visakhapatam

More information

NON-LINEAR PARAMETER ESTIMATION USING VOLTERRA SERIES WITH MULTI-TONE EXCITATION

NON-LINEAR PARAMETER ESTIMATION USING VOLTERRA SERIES WITH MULTI-TONE EXCITATION NON-LINER PRMETER ESTIMTION USING VOLTERR SERIES WIT MULTI-TONE ECITTION imsh Char Dparm of Mchaical Egirig Visvsvaraya Rgioal Collg of Egirig Nagpur INDI-00 Naliash Vyas Dparm of Mchaical Egirig Iia Isiu

More information

EEE 303: Signals and Linear Systems

EEE 303: Signals and Linear Systems 33: Sigls d Lir Sysms Orhogoliy bw wo sigls L us pproim fucio f () by fucio () ovr irvl : f ( ) = c( ); h rror i pproimio is, () = f() c () h rgy of rror sigl ovr h irvl [, ] is, { }{ } = f () c () d =

More information

Fourier Eigenfunctions, Uncertainty Gabor Principle And Isoresolution Wavelets

Fourier Eigenfunctions, Uncertainty Gabor Principle And Isoresolution Wavelets XX SIMPÓSIO BRASILEIRO DE TELECOMUNICAÇÕES-SBT 0, 05-08 DE OUTUBRO DE 00, RIO DE JANEIRO, RJ Fourir Eigucios, Ucraiy Gabor Pricipl Ad Isorsoluio Wavls L.R. Soars, H.M. d Olivira, R.J.S. Cira ad R.M. Campllo

More information

On the Derivatives of Bessel and Modified Bessel Functions with Respect to the Order and the Argument

On the Derivatives of Bessel and Modified Bessel Functions with Respect to the Order and the Argument Inrnaional Rsarch Journal of Applid Basic Scincs 03 Aailabl onlin a wwwirjabscom ISSN 5-838X / Vol 4 (): 47-433 Scinc Eplorr Publicaions On h Driais of Bssl Modifid Bssl Funcions wih Rspc o h Ordr h Argumn

More information

New Families of Fourth-Order Derivative-Free Methods for Solving Nonlinear Equations with Multiple Roots

New Families of Fourth-Order Derivative-Free Methods for Solving Nonlinear Equations with Multiple Roots Arica Joural o Coputatioal ad Applid Mathatics (4: 7- DOI:.59/j.ajca.4. Nw Failis o Fourth-Ordr Drivativ-Fr Mthods or Solvig Noliar Equatios with Multipl Roots R. Thukral Padé Rsarch Ctr 9 Daswood Hill

More information

ECE351: Signals and Systems I. Thinh Nguyen

ECE351: Signals and Systems I. Thinh Nguyen ECE35: Sigals ad Sysms I Thih Nguy FudamalsofSigalsadSysms x Fudamals of Sigals ad Sysms co. Fudamals of Sigals ad Sysms co. x x] Classificaio of sigals Classificaio of sigals co. x] x x] =xt s =x

More information

Note 6 Frequency Response

Note 6 Frequency Response No 6 Frqucy Rpo Dparm of Mchaical Egirig, Uivriy Of Sakachwa, 57 Campu Driv, Sakaoo, S S7N 59, Caada Dparm of Mchaical Egirig, Uivriy Of Sakachwa, 57 Campu Driv, Sakaoo, S S7N 59, Caada. alyical Exprio

More information

An Asymptotic Expansion for the Non-Central Chi-square Distribution. By Jinan Hamzah Farhood Department of Mathematics College of Education

An Asymptotic Expansion for the Non-Central Chi-square Distribution. By Jinan Hamzah Farhood Department of Mathematics College of Education A Asypoic Expasio fo h o-cal Chi-squa Disibuio By Jia Hazah ahood Dpa of Mahaics Collg of Educaio 6 Absac W div a asypoic xpasio fo h o-cal chi-squa disibuio as wh X i is h o-cal chi-squa vaiabl wih dg

More information

BE.430 Tutorial: Linear Operator Theory and Eigenfunction Expansion

BE.430 Tutorial: Linear Operator Theory and Eigenfunction Expansion BE.43 Tuorial: Liear Operaor Theory ad Eigefucio Expasio (adaped fro Douglas Lauffeburger) 9//4 Moivaig proble I class, we ecouered parial differeial equaios describig rasie syses wih cheical diffusio.

More information

Worksheet: Taylor Series, Lagrange Error Bound ilearnmath.net

Worksheet: Taylor Series, Lagrange Error Bound ilearnmath.net Taylor s Thorm & Lagrag Error Bouds Actual Error This is th ral amout o rror, ot th rror boud (worst cas scario). It is th dirc btw th actual () ad th polyomial. Stps:. Plug -valu ito () to gt a valu.

More information

Mixing time with Coupling

Mixing time with Coupling Mixig im wih Couplig Jihui Li Mig Zhg Saisics Dparm May 7 Goal Iroducio o boudig h mixig im for MCMC wih couplig ad pah couplig Prsig a simpl xampl o illusra h basic ida Noaio M is a Markov chai o fii

More information

ECEN620: Network Theory Broadband Circuit Design Fall 2014

ECEN620: Network Theory Broadband Circuit Design Fall 2014 ECE60: work Thory Broadbad Circui Dig Fall 04 Lcur 6: PLL Trai Bhavior Sam Palrmo Aalog & Mixd-Sigal Cr Txa A&M Uivriy Aoucm, Agda, & Rfrc HW i du oday by 5PM PLL Trackig Rpo Pha Dcor Modl PLL Hold Rag

More information

Software Development Cost Model based on NHPP Gompertz Distribution

Software Development Cost Model based on NHPP Gompertz Distribution Idia Joural of Scic ad Tchology, Vol 8(12), DOI: 10.17485/ijs/2015/v8i12/68332, Ju 2015 ISSN (Pri) : 0974-6846 ISSN (Oli) : 0974-5645 Sofwar Dvlopm Cos Modl basd o NHPP Gomprz Disribuio H-Chul Kim 1* ad

More information

) and furthermore all X. The definition of the term stationary requires that the distribution fulfills the condition:

) and furthermore all X. The definition of the term stationary requires that the distribution fulfills the condition: Assigm Thomas Aam, Spha Brumm, Haik Lor May 6 h, 3 8 h smsr, 357, 7544, 757 oblm For R b X a raom variabl havig ormal isribuio wih ma µ a variac σ (his is wri as ~ (,) X. by: R a. Is X ) a urhrmor all

More information

Semi-Parametric Method to Estimate the Time-to- Failure Distribution and its Percentiles for Simple Linear Degradation Model

Semi-Parametric Method to Estimate the Time-to- Failure Distribution and its Percentiles for Simple Linear Degradation Model Joural o Modr Applid Saisical Mods Volum 6 Issu Aricl 7 --07 Smi-Paramric Mod o Esima Tim-o- Failur isriuio ad is Prcils or Simpl Liar gradaio Modl Laila Nai Ba ak Yarmouk Uivrsiy, Irid, Jorda, la00_ma@yaoo.com

More information

Revisiting what you have learned in Advanced Mathematical Analysis

Revisiting what you have learned in Advanced Mathematical Analysis Fourir sris Rvisiing wh you hv lrnd in Advncd Mhmicl Anlysis L f x b priodic funcion of priod nd is ingrbl ovr priod. f x cn b rprsnd by rigonomric sris, f x n cos nx bn sin nx n cos x b sin x cosx b whr

More information

CSE 245: Computer Aided Circuit Simulation and Verification

CSE 245: Computer Aided Circuit Simulation and Verification CSE 45: Compur Aidd Circui Simulaion and Vrificaion Fall 4, Sp 8 Lcur : Dynamic Linar Sysm Oulin Tim Domain Analysis Sa Equaions RLC Nwork Analysis by Taylor Expansion Impuls Rspons in im domain Frquncy

More information

Optimum Demodulation. Lecture Notes 9: Intersymbol Interference

Optimum Demodulation. Lecture Notes 9: Intersymbol Interference d d Lcur os 9: Irsybol Irrc I his lcur w xai opiu dodulaio wh h rasid sigal is ilrd by h chal ad hr is addiiv whi Gaussia ois. h opiu dodulaor chooss h possibl rasid vcor ha would rsul i h rcivd vcor (i

More information

15. Numerical Methods

15. Numerical Methods S K Modal' 5. Numrical Mhod. Th quaio + 4 4 i o b olvd uig h Nwo-Rapho mhod. If i ak a h iiial approimaio of h oluio, h h approimaio uig hi mhod will b [EC: GATE-7].(a (a (b 4 Nwo-Rapho iraio chm i f(

More information

The Variance-Covariance Matrix

The Variance-Covariance Matrix Th Varanc-Covaranc Marx Our bggs a so-ar has bn ng a lnar uncon o a s o daa by mnmzng h las squars drncs rom h o h daa wh mnsarch. Whn analyzng non-lnar daa you hav o us a program l Malab as many yps o

More information

Intrinsic formulation for elastic line deformed on a surface by an external field in the pseudo-galilean space 3. Nevin Gürbüz

Intrinsic formulation for elastic line deformed on a surface by an external field in the pseudo-galilean space 3. Nevin Gürbüz risic formuaio for asic i form o a surfac by a xra fi i h psuo-aia spac Nvi ürbüz Eskişhir Osmaazi Uivrsiy Mahmaics a Compur Scics Dparm urbuz@ouur Absrac: his papr w riv irisic formuaio for asic i form

More information

The geometry of surfaces contact

The geometry of surfaces contact Applid ad ompuaioal Mchaics (007 647-656 h gomry of surfacs coac J. Sigl a * J. Švíglr a a Faculy of Applid Scics UWB i Pils Uivrzií 0 00 Pils zch public civd 0 Spmbr 007; rcivd i rvisd form 0 Ocobr 007

More information

Review Lecture 5. The source-free R-C/R-L circuit Step response of an RC/RL circuit. The time constant = RC The final capacitor voltage v( )

Review Lecture 5. The source-free R-C/R-L circuit Step response of an RC/RL circuit. The time constant = RC The final capacitor voltage v( ) Rviw Lcur 5 Firs-ordr circui Th sourc-fr R-C/R-L circui Sp rspons of an RC/RL circui v( ) v( ) [ v( 0) v( )] 0 Th i consan = RC Th final capacior volag v() Th iniial capacior volag v( 0 ) Volag/currn-division

More information

1.7 Vector Calculus 2 - Integration

1.7 Vector Calculus 2 - Integration cio.7.7 cor alculus - Igraio.7. Ordiary Igrals o a cor A vcor ca b igrad i h ordiary way o roduc aohr vcor or aml 5 5 d 6.7. Li Igrals Discussd hr is h oio o a dii igral ivolvig a vcor ucio ha gras a scalar.

More information

An Indian Journal FULL PAPER. Trade Science Inc. A stage-structured model of a single-species with density-dependent and birth pulses ABSTRACT

An Indian Journal FULL PAPER. Trade Science Inc. A stage-structured model of a single-species with density-dependent and birth pulses ABSTRACT [Typ x] [Typ x] [Typ x] ISSN : 974-7435 Volum 1 Issu 24 BioTchnology 214 An Indian Journal FULL PAPE BTAIJ, 1(24), 214 [15197-1521] A sag-srucurd modl of a singl-spcis wih dnsiy-dpndn and birh pulss LI

More information

Control Systems (Lecture note #6)

Control Systems (Lecture note #6) 6.5 Corol Sysms (Lcur o #6 Las Tm: Lar algbra rw Lar algbrac quaos soluos Paramrzao of all soluos Smlary rasformao: compao form Egalus ad gcors dagoal form bg pcur: o brach of h cours Vcor spacs marcs

More information

REACHABILITY OF FRACTIONAL CONTINUOUS-TIME LINEAR SYSTEMS USING THE CAPUTO-FABRIZIO DERIVATIVE

REACHABILITY OF FRACTIONAL CONTINUOUS-TIME LINEAR SYSTEMS USING THE CAPUTO-FABRIZIO DERIVATIVE ECHLY OF FCONL CONNUOUS-ME LNE SYSEMS USNG HE CPUO-FZO DEVVE usz Kczor iłyso Uivrsiy o chology Fculy o Elcricl Egirig Wijs 45D, 5-5 iłyso E-il: czor@isppwupl KEYWODS Frciol, coiuous-i, lir, sys, Cpuo-

More information

Chapter 3: Fourier Representation of Signals and LTI Systems. Chih-Wei Liu

Chapter 3: Fourier Representation of Signals and LTI Systems. Chih-Wei Liu Chapr 3: Fourir Rprsnaion of Signals and LTI Sysms Chih-Wi Liu Oulin Inroducion Complx Sinusoids and Frquncy Rspons Fourir Rprsnaions for Four Classs of Signals Discr-im Priodic Signals Fourir Sris Coninuous-im

More information

Strictly as per the compliance and regulations of :

Strictly as per the compliance and regulations of : Global Joural of Scic Froir Rsarch Mahaics & Dcisio Scics Volu Issu Vrsio. Typ : Doubl lid Pr Rviwd Iraioal Rsarch Joural Publishr: Global Jourals Ic. US Oli ISSN: 9-66 & i ISSN: 975-5896 Oscillaory Fr

More information

ON H-TRICHOTOMY IN BANACH SPACES

ON H-TRICHOTOMY IN BANACH SPACES CODRUTA STOICA IHAIL EGA O H-TRICHOTOY I BAACH SPACES Absrac: I his papr w mphasiz h oio of skw-oluio smiflows cosidrd a gralizaio of smigroups oluio opraors ad skw-produc smiflows which aris i h sabiliy

More information

DEPARTMENT OF MATHEMATICS BIT, MESRA, RANCHI MA2201 Advanced Engg. Mathematics Session: SP/ 2017

DEPARTMENT OF MATHEMATICS BIT, MESRA, RANCHI MA2201 Advanced Engg. Mathematics Session: SP/ 2017 DEARMEN OF MAEMAICS BI, MESRA, RANCI MA Advad Egg. Mathatis Sssio: S/ 7 MODULE I. Cosidr th two futios f utorial Sht No. -- ad g o th itrval [,] a Show that thir Wroskia W f, g vaishs idtially. b Show

More information

Department of Electronics & Telecommunication Engineering C.V.Raman College of Engineering

Department of Electronics & Telecommunication Engineering C.V.Raman College of Engineering Lcur No Lcur-6-9 Ar rdig his lsso, you will lr ou Fourir sris xpsio rigoomric d xpoil Propris o Fourir Sris Rspos o lir sysm Normlizd powr i Fourir xpsio Powr spcrl dsiy Ec o rsr ucio o PSD. FOURIER SERIES

More information

Page 1. Before-After Control-Impact (BACI) Power Analysis For Several Related Populations (With Unknown Variance Matrix) Richard A.

Page 1. Before-After Control-Impact (BACI) Power Analysis For Several Related Populations (With Unknown Variance Matrix) Richard A. Pag Bfor-Afr Corol-Impac (BACI) Powr Aalysis For Svral Rlad Populaios (Wih Ukow Variac Marix) Richard A. Hirichs Spmbr 0, 00 Cava: This xprimal dsig ool is a idalizd powr aalysis buil upo svral simplifyig

More information

, then the old equilibrium biomass was greater than the new B e. and we want to determine how long it takes for B(t) to reach the value B e.

, then the old equilibrium biomass was greater than the new B e. and we want to determine how long it takes for B(t) to reach the value B e. SURPLUS PRODUCTION (coiud) Trasiio o a Nw Equilibrium Th followig marials ar adapd from lchr (978), o h Rcommdd Radig lis caus () approachs h w quilibrium valu asympoically, i aks a ifii amou of im o acually

More information

Boyce/DiPrima 9 th ed, Ch 7.9: Nonhomogeneous Linear Systems

Boyce/DiPrima 9 th ed, Ch 7.9: Nonhomogeneous Linear Systems BoDiPrima 9 h d Ch 7.9: Nohomogou Liar Sm Elmar Diffrial Equaio ad Boudar Valu Prolm 9 h diio William E. Bo ad Rihard C. DiPrima 9 Joh Wil & So I. Th gral hor of a ohomogou m of quaio g g aralll ha of

More information

An Exact Solution for the Free Vibration Analysis of Timoshenko Beams

An Exact Solution for the Free Vibration Analysis of Timoshenko Beams www.seipub.org/rap Review of Applied Physics Volue 3, 4 A Exac Soluio for he Free Vibraio Aalysis of Tiosheko Beas Raaza A. Jafari-Talookolaei *, Marya Abedi School of Mechaical Egieerig, Babol Noshirvai

More information

Lecture 4: Laplace Transforms

Lecture 4: Laplace Transforms Lur 4: Lapla Transforms Lapla and rlad ransformaions an b usd o solv diffrnial quaion and o rdu priodi nois in signals and imags. Basially, hy onvr h drivaiv opraions ino mulipliaion, diffrnial quaions

More information

The Importance of Ordering the Number of Lattice Points Inside a Rational Polyhedron Using Generating Functions

The Importance of Ordering the Number of Lattice Points Inside a Rational Polyhedron Using Generating Functions Ieraioal Joural of Copuer Sciece ad Elecroics Egieerig (IJCSEE Volue Issue ( ISSN 48 (Olie he Iporace of Orderig he Nuber of Laice ois Iside a Raioal olyhedro Usig Geeraig Fucios Halil Sopce Absrac I pure

More information

Advanced Engineering Mathematics, K.A. Stroud, Dexter J. Booth Engineering Mathematics, H.K. Dass Higher Engineering Mathematics, Dr. B.S.

Advanced Engineering Mathematics, K.A. Stroud, Dexter J. Booth Engineering Mathematics, H.K. Dass Higher Engineering Mathematics, Dr. B.S. Rfrc: (i) (ii) (iii) Advcd Egirig Mhmic, K.A. Sroud, Dxr J. Booh Egirig Mhmic, H.K. D Highr Egirig Mhmic, Dr. B.S. Grwl Th mhod of m Thi coi of h followig xm wih h giv coribuio o h ol. () Mid-rm xm : 3%

More information

Series of New Information Divergences, Properties and Corresponding Series of Metric Spaces

Series of New Information Divergences, Properties and Corresponding Series of Metric Spaces Srs of Nw Iforao Dvrgcs, Proprs ad Corrspodg Srs of Mrc Spacs K.C.Ja, Praphull Chhabra Profssor, Dpar of Mahacs, Malavya Naoal Isu of Tchology, Japur (Rajasha), Ida Ph.d Scholar, Dpar of Mahacs, Malavya

More information

Chapter4 Time Domain Analysis of Control System

Chapter4 Time Domain Analysis of Control System Chpr4 im Domi Alyi of Corol Sym Rouh biliy cririo Sdy rror ri rpo of h fir-ordr ym ri rpo of h cod-ordr ym im domi prformc pcificio h rliohip bw h prformc pcificio d ym prmr ri rpo of highr-ordr ym Dfiiio

More information

whereby we can express the phase by any one of the formulas cos ( 3 whereby we can express the phase by any one of the formulas

whereby we can express the phase by any one of the formulas cos ( 3 whereby we can express the phase by any one of the formulas Third In-Class Exam Soluions Mah 6, Profssor David Lvrmor Tusday, 5 April 07 [0] Th vrical displacmn of an unforcd mass on a spring is givn by h 5 3 cos 3 sin a [] Is his sysm undampd, undr dampd, criically

More information

MODIFIED ADOMIAN DECOMPOSITION METHOD FOR SOLVING RICCATI DIFFERENTIAL EQUATIONS

MODIFIED ADOMIAN DECOMPOSITION METHOD FOR SOLVING RICCATI DIFFERENTIAL EQUATIONS Review of he Air Force Academy No 3 (3) 15 ODIFIED ADOIAN DECOPOSIION EHOD FOR SOLVING RICCAI DIFFERENIAL EQUAIONS 1. INRODUCION Adomia decomposiio mehod was foud by George Adomia ad has recely become

More information

1a.- Solution: 1a.- (5 points) Plot ONLY three full periods of the square wave MUST include the principal region.

1a.- Solution: 1a.- (5 points) Plot ONLY three full periods of the square wave MUST include the principal region. INEL495 SIGNALS AND SYSEMS FINAL EXAM: Ma 9, 8 Pro. Doigo Rodrígz SOLUIONS Probl O: Copl Epoial Forir Sri A priodi ri ar wav l ad a daal priod al o o od. i providd wi a a 5% d a.- 5 poi: Plo r ll priod

More information

Recovery of Valuable Incompletely-Recorded Return- Stroke Current Derivative Signals

Recovery of Valuable Incompletely-Recorded Return- Stroke Current Derivative Signals Rcovry of Valuabl Icomplly-Rcordd Rur- Srok Curr Drivaiv Sigals Lakmii Prra Elcrical ad Compur Egirig Dparm Ryrso Uivrsiy Toroo, Caada lakmii.prra@ryrso.ca Ali M. Hussi Elcrical ad Compur Egirig Dparm

More information

THE ROYAL STATISTICAL SOCIETY 2016 EXAMINATIONS SOLUTIONS GRADUATE DIPLOMA MODULE 1

THE ROYAL STATISTICAL SOCIETY 2016 EXAMINATIONS SOLUTIONS GRADUATE DIPLOMA MODULE 1 TH ROAL TATITICAL OCIT 6 AINATION OLTION GRADAT DILOA ODL T oci i providig olio o ai cadida prparig or aiaio i 7. T olio ar idd a larig aid ad old o b a "odl awr". r o olio old alwa b awar a i a ca r ar

More information

Reconfiguration for Sensor Failure of Aero-engine Electronic Control System Based on the MRAC

Reconfiguration for Sensor Failure of Aero-engine Electronic Control System Based on the MRAC lid Mchaics ad Maials Sbid: 4-6- SSN: 66-748, ols. 6-65, 367-37 ccd: 4-6- doi:.48/www.sciiic./mm.6-65.367 Oli: 4-8- 4 ras ch blicaios, Swizrlad Rcoigraio or Ssor ailr o ro-gi Elcoic Cool Sys asd o h MRC

More information

Assessing Reliable Software using SPRT based on LPETM

Assessing Reliable Software using SPRT based on LPETM Iraioal Joural of Compur Applicaios (75 888) Volum 47 No., Ju Assssig Rliabl Sofwar usig SRT basd o LETM R. Saya rasad hd, Associa rofssor Dp. of CS &Egg. AcharyaNagarjua Uivrsiy D. Hariha Assisa rofssor

More information

Modified Variational Iteration Method for the Solution of nonlinear Partial Differential Equations

Modified Variational Iteration Method for the Solution of nonlinear Partial Differential Equations Iraioal Joral of Sciific & Egirig Rsarch Volm Iss Oc- ISSN 9-558 Modifid Variaioal Iraio Mhod for h Solio of oliar Parial Diffrial Eqaios Olayiwola M O Akipl F O Gbolagad A W Absrac-Th Variaioal Iraio

More information

PRELIMINARY DEFINITIONS AND RELATIONS

PRELIMINARY DEFINITIONS AND RELATIONS Prliinary Dfiniions and Rlaions 1 CHAPTER 2 PRELIMINARY DEFINITIONS AND RELATIONS يتكون حجم معيه مه التربة مه حبيبات صلببة هولواو هملاو اميلاي جوفيللة أه ميللاي (.للصدر همقلل ) ال للو فللي التربللة وللو

More information

UNIT I FOURIER SERIES T

UNIT I FOURIER SERIES T UNIT I FOURIER SERIES PROBLEM : Th urig mom T o h crkh o m gi i giv or ri o vu o h crk g dgr 6 9 5 8 T 5 897 785 599 66 Epd T i ri o i. Souio: L T = i + i + i +, Sic h ir d vu o T r rpd gc o T T i T i

More information

Final Exam : Solutions

Final Exam : Solutions Comp : Algorihm and Daa Srucur Final Exam : Soluion. Rcuriv Algorihm. (a) To bgin ind h mdian o {x, x,... x n }. Sinc vry numbr xcp on in h inrval [0, n] appar xacly onc in h li, w hav ha h mdian mu b

More information

EXISTENCE THEORY OF RANDOM DIFFERENTIAL EQUATIONS D. S. Palimkar

EXISTENCE THEORY OF RANDOM DIFFERENTIAL EQUATIONS D. S. Palimkar Ieraioal Joural of Scieific ad Research Publicaios, Volue 2, Issue 7, July 22 ISSN 225-353 EXISTENCE THEORY OF RANDOM DIFFERENTIAL EQUATIONS D S Palikar Depare of Maheaics, Vasarao Naik College, Naded

More information

Variational iteration method: A tools for solving partial differential equations

Variational iteration method: A tools for solving partial differential equations Elham Salhpoor Hossi Jafari/ TJMCS Vol. o. 388-393 Th Joral of Mahmaics a Compr Scic Availabl oli a hp://www.tjmcs.com Th Joral of Mahmaics a Compr Scic Vol. o. 388-393 Variaioal iraio mho: A ools for

More information

Fractional Complex Transform for Solving the Fractional Differential Equations

Fractional Complex Transform for Solving the Fractional Differential Equations Global Joral of Pr ad Applid Mahmaics. SSN 97-78 Volm Nmbr 8 pp. 7-7 Rsarch dia Pblicaios hp://www.ripblicaio.com Fracioal Compl rasform for Solvig h Fracioal Diffrial Eqaios A. M. S. Mahdy ad G. M. A.

More information

New Sixteenth-Order Derivative-Free Methods for Solving Nonlinear Equations

New Sixteenth-Order Derivative-Free Methods for Solving Nonlinear Equations Amrica Joural o Computatioal ad Applid Mathmatics 0 (: -8 DOI: 0.59/j.ajcam.000.08 Nw Sixtth-Ordr Drivativ-Fr Mthods or Solvig Noliar Equatios R. Thukral Padé Rsarch Ctr 9 Daswood Hill Lds Wst Yorkshir

More information

3.2. Derivation of Laplace Transforms of Simple Functions

3.2. Derivation of Laplace Transforms of Simple Functions 3. aplac Tarform 3. PE TRNSFORM wid rag of girig ym ar modld mahmaically by uig diffrial quaio. I gral, h diffrial quaio of h ordr ym i wri: d y( a d d d y( dy( a a y( f( (3. d Which i alo ow a a liar

More information

ANALYTICAL EXPRESSION FOR THE NON-ISOTHERMAL EFFECTIVENESS FACTOR: The n th -order reaction in a slab geometry

ANALYTICAL EXPRESSION FOR THE NON-ISOTHERMAL EFFECTIVENESS FACTOR: The n th -order reaction in a slab geometry ANALYTICAL XPRSSION FOR T NON-ISOTRMAL FFCTIVNSS FACTOR: Th h -ordr racio i a slab gomry riqu Muñoz Tavra Dparm o Biogirig, Ric Uivrsiy, ouso, TX 775-89 USA muoz@ric.du Absrac Th problm o calculaig h civss

More information