A NEW SPECTRAL ALGORITHM FOR TIME-SPACE FRACTIONAL PARTIAL DIFFERENTIAL EQUATIONS WITH SUBDIFFUSION AND SUPERDIFFUSION

Size: px
Start display at page:

Download "A NEW SPECTRAL ALGORITHM FOR TIME-SPACE FRACTIONAL PARTIAL DIFFERENTIAL EQUATIONS WITH SUBDIFFUSION AND SUPERDIFFUSION"

Transcription

1 HE UBISHIG HOUSE ROCEEDIGS OF HE ROAIA ACADEY Seres A OF HE ROAIA ACADEY Vole 7 ber /6 pp A EW SECRA AGORIH FOR IE-SACE FRACIOA ARIA DIFFEREIA EQUAIOS WIH SUBDIFFUSIO AD SUERDIFFUSIO A.H. BHRAWY Kng Abdlzz Unversy Fcly o Scence Depren o hecs Jeddh Sd Arb Ben-Se Unversy Fcly o Scence Depren o hecs Ben-Se Egyp E-l: lbhry@yhoo.co.k Absrc. hs pper repors ne specrl collocon lgorh or solvng e-spce rconl prl derenl eons h sbdson nd sperdson. In hs schee e eploy he shed egendre Gss-obo collocon schee nd he shed Chebyshev Gss-Rd collocon pproons or spl nd eporl dscrezons respecvely. We ocs on pleenng he ne lgorh or o physcl probles nely e rconl oded nolos sbdson nd rconl nonlner sperdson eons. he nercl resls obned by sng hs lgorh hve been copred h noher nercl schee n order o deonsre he hgh ccrcy nd ecency o he proposed ehod. Key ords: e nd spce rconl dson eon sbdson nd sperdson legendre Gss-obo nd Chebyshev Gss-Rd drres.. IRODUCIO In recen yers here hs been hgh level o neres o eployng specrl ehods or nerclly solvng ny ypes o negrl nd derenl eons de o her ese n pleenon over ne nd nne dons [ 6]. he speed o convergence s one o he gre dvnges o specrl ehods. Besdes specrl ehods hve eponenl res o convergence; hey lso hve hgh level o ccrcy. Specrl ehods hve been clssed o hree ypes nely collocon [7 8] [9 ] nd Glerkn [ ] ehods. Frconl derenl eons FDEs [3 8] odel ny phenoen n severl elds sch s ld echncs chesry bology vscoelscy engneerng nnce nd physcs [9 3]. os FDEs do no hve ec solons so pprove ehods nd nercl echnes hve been proposed nd developed o nd he solons o sch eons. Fne eleen ehods hve been presened n [4 6] o obn he nercl solons o rconl derenl eons. ercl reens bsed on ne derence ehods ere developed or solvng FDEs [7 9]. Recenly severl specrl lgorhs ere desgned nd developed or nercl solons o FDEs see or eple [3 34]. he collocon ehod hs de rnge o pplcons de o s ese o se nd dpbly n vros probles. We ocs bsclly on proposng ne specrl collocon ehod or o ell-knon FDEs ro hecl physcs besdes deonsrng he ccrcy o hs proposed collocon ehod. he n obecve o hs rcle s o propose ne collocon ehod or he nercl solons o o ypes o rconl prl derenl eons FDEs nely he oded nolos rconl sbdson nd he rconl nonlner sperdson eons. he proposed ehod s bsed pon he shed egendre Gss-obo collocon schee or spl dscrezon n conncon h Chebyshev Gss-Rd collocon schee or eporl dscrezon. hereore e presen lly collocon schee or solvng sch probles. he proble s hen redced o syse o lgebrc eons. Fnlly he ccrcy o he proposed ehod s deonsred by es proble hch corresponds o physclly enngl cse. o he bes o or knoledge here re no resls on he collocon ehod or solvng nonlner rconl sbdson or sperdson eons. hs pper s orgnzed s ollos. We presen e relevn properes o rconl dervves nd shed Jcob polynols n Sec.. he proposed schee s

2 4 A.H. BHRAWY nvesged nd pleened or he e rconl dson odel n Sec. 3. Secon 4 s devoed o solve e-spce rconl sperdson eon. A nercl slon s presened n Sec. 5. Fnlly soe concldng rerks re gven n he ls secon.. FRACIOA CACUUS AD JACOBI OYOIAS here re severl denons o rconl negron o order > nd no necessrly evlen o ech oher [35]. Renn-ovlle nd Cpo rconl denons re he o os sed ro ll he oher denons o rconl clcls. Denon.. he negrl o order rconl ccordng o Renn-ovlle s gven by Γ J d > > J he operor J sses he ollong properes + β Γ β + β + J J J J J J J J. Γ β + + Denon.. he Renn-ovlle rconl dervves o order s dened s d D d < > Γ d 3 here s he celng ncon o. Denon.3. he Cpo rconl dervves o order s dened s c d D d < >. Γ 4 d Here e rend he reder o soe sel properes o shed Jcob polynols h re os relevn o specrl pproons [36 37]. I ncldes egendre nd Chebyshev polynols s o specl cses. he θ ϑ h dervve o Jcob polynol cn be obned ro D Γ + θ + ϑ + + Γ + θ + ϑ + θ ϑ θ + ϑ +. 5 θ ϑ he se o k consss coplee θ ϑ -orhogonl syse h θ + ϑ + θ ϑ Γ k + θ + Γ k + ϑ + k θ ϑ hk. 6 k + θ + ϑ + Γ k + Γ k + θ + ϑ + θ ϑ θ ϑ We denoe by k k > he shed Jcob polynol o degree k dened on he nervl []. In vre o 5 e dedce h D θ ϑ k k Γ k + ϑ + k + θ + ϑ + Γ k + Γ + ϑ + 7 D θ ϑ k Γ k + θ + k + θ + ϑ + Γ k + Γ + θ + 8

3 3 A ne specrl lgorh or e-spce rconl prl derenl eons h sbdson nd sperdson 4 D θ ϑ Γ + k + θ + ϑ + θ + ϑ k k. Γ k + θ + ϑ e le θ ϑ θ ϑ hen e dene he eghed spce θ ϑ [ ] ollong nner prodc nd nor n he sl y h he θ ϑ v θ ϑ v d v θ ϑ v v θ ϑ. he se o shed Jcob polynols ors coplee [ ] -orhogonl syse. De o e obn θ ϑ We denoe by θ ϑ k θ ϑ θ ϑ θ + ϑ + h θ ϑ k h θ ϑ k he nodes o he sndrd Jcob-Gss nerpolon on he nervl θ ϑ [ ]. her correspondng Chrsoel nbers re ϖ. he nodes o he shed Jcob- θ ϑ θϑ Gss nerpolon on he nervl [] re he zeros o + hch e denoe by. θ ϑ θ ϑ Clerly + nd her correspondng Chrsoel nbers re θϑ θ + ϑ + ϖ θϑ ϖ. e S be he se o polynols o degree os. hnks o he propery o he sndrd Jcob-Gss drre ollos h or ny φ S +. θ+ ϑ+ θ ϑ θ ϑ φ d + φ + d θ+ ϑ+ θϑ θϑ θϑ θϑ ϖ φ + ϖ φ. he bove negrl s ec or φ S nd θ ϑ θ ϑ φ S n cses o selecng ϖ he zeros nd eghs o Jcob Gss-Rd nd Jcob Gss-obo drres respecvely. 3. IE FRACIOA ODIFIED AOAOUS SUBDIFFUSIO EQUAIO We propose egendre-chebyshev collocon ehod nd descrbe s pleenon or he nercl solon o e-rconl oded nolos sbdson eon. We pproe he solon o sch eon or spl nd eporl dscrezons by dpng he egendre Gss-obo [38] ehod n conncon h Chebyshev Gss-Rd collocon ehod [39]. Recenly soe odels hve been sed or descrbng processes h becoe less nolos s e progresses by he nclson o secondry rconl e dervve cng on dson operor h nonlner sorce er [4 4 4]: h he nl condon + + R [ ] [ ] 3 g [ ] 4

4 4 A.H. BHRAWY 4 nd he bondry condons ] [ g g 5 here < re rel consns he nonlner sorce er ] [ C R nd g g g re gven ncons. he rconl e dervve operors nd re dened n ers o he Renn-ovlle rconl dervve. o e olne he n seps o pplyng he shed egendre Gss-obo nerpolon pons s collocon nodes or he spl pproon enhle he shed Chebyshev Gss-Rd nerpolon pons s nvesged s collocon nodes or he eporl pproon. o hs end le s epnd he pproe solon by ens o egendre nd Chebyshev seres n he or 6 here. Frherore he pproon o he spl prl dervve cn be coped s 7 here. he pproon o he eporl prl dervve cn be coped s 8 nd 3 9 h. 3 Bsed on he bove reen o eporl nd spl prl dervves he rs coponen o he rgh hnd sde o 3 cn be obned eplcly by here. 4 + he bove relon s epressed eplcly by dpng he Renn-ovlle rconl dervve o he poer seres o he shed Chebyshev polynol. hereore dopng 6 enbles one o epress 3 n he or:

5 5 A ne specrl lgorh or e-spce rconl prl derenl eons h sbdson nd sperdson 43 + R [ ] []. 4 I rens o desgn n pproon or he nl nd bondry condons. We y pproe hese condons by ens o egendre nd Chebyshev polynols s g g g o E. s colloced o collocon nodes. oreover he nl-bondry condons n s lso colloced egendre nd Chebyshev collocon nodes. Frs e obn lgebrc eons or he nknon coecens ro F r s. R ζ r η r ; s here Fr s ζ r η s 4 ζ r η s hle ζ r nd η s re he shed egendre Gss- obo nd he shed Chebyshev Gss-Rd drres nodes respecvely. Second reng he nl condon he egendre Gss-obo nodes leds o lgebrc eons r r s 3 ζ g ζ r. 4 Fnlly he pproon o he bondry condons he Chebyshev Gss-Rd nodes leds o + lgebrc eons η s η s g η s g η s hs n rn yelds syse o + + lgebrc eons F r s R ζ r η η g s s g η g ζ η s. ζ r η s ζ r η s r ; s r s s r s s. he bove syse o nonlner lgebrc eons n he epnson coecens y be solved nerclly n sep-by-sep nner by sng eon s erve ehod. 5 6

6 44 A.H. BHRAWY 6 4. IE-SACE FRACIOA OIEAR SUERDIFFUSIO EQUAIO In hs secon e propose n ecen solon or he e-spce rconl dson eon reled o Renn-ovlle nd Cpo rconl dervves h nonlner er [43]: sbec o c R [ ] [ ] 7 g [ ] 8 g g [ ] 9 here nd re consns hle R g g nd g re gven ncons. he pproe solon hs seres o he or he Cpo rconl dervve o he pproe solon s gven by c 3 c 5 3 c nd y be epressed n n eplc or by dpng he Cpo rconl dervve or he poer seres o he shed Chebyshev polynol. oreover he Renn-ovlle rconl prl dervve or spce vrble s obned by here 6 nd y be obned n n eplc or by pplyng he Renn-ovlle rconl dervve o he poer seres o he shed egendre polynol. hereore he lly collocon schee o 7 9 er eployng 3 3 leds o syse o + + lgebrc eons + 5 ζ r η s ζ rη s ζ rη s 6 r s r s ζ r ζ r η s s η s s + ζ η + R ζ η r ; s g r g η s g η s. Fnlly he bove syse o nonlner lgebrc eons n he epnson coecens y be solved by sng eon s erve ehod. 33

7 7 A ne specrl lgorh or e-spce rconl prl derenl eons h sbdson nd sperdson ble bsole errors sng he presen ehod nd he CD schee [44] Or schee CD schee [44] UERICA RESUS In hs secon e shll hghlgh he ccrcy nd he ecency o or ehod. Consder he rconl sbdson eon h enn condons [44]: Γ e Γ + 34 he ec solon s gven by [] []. 35 e + [] []. In ble e sho nd copre he bsole errors sng he egendre Gss-obo ehod n conncon h Chebyshev Gss-Rd collocon ehod or schee nd hose h hve been presened by Ren e l. [44] by pleenng he copc derence CD schee [44]. Fro hs ble e conclde h he presen ehod s ore ccre hn he CD schee [44]. I s lso observed h he bsole error s very sll despe he relvely sll nber o grd pons sed. hs nercl eperen deonsres he ly o he ehod COCUSIOS In hs pper e hve proposed n ecen nd ccre lgorh bsed on he egendre Gss- obo ehod n cobnon h Chebyshev Gss-Rd collocon ehod o obn he nercl solons o e-spce rconl prl derenl eons FDEs h sbdson nd sperdson. he ehod s bsed pon redcng he enoned proble no syse o lgebrc eons n he epnson coecen o he solon. We hve olned he pplcon o egendre nd Chebyshev collocon ehods or solvng FDEs. In prncple hs lgorh y be eended o reled probles sch s o copled nonlner FDEs. One gh lso consder e-spce cople rconl Schrödnger eons nd o-sded spce FDEs. We shold noe h s nercl ehod e re resrced o solvng probles over ne don. Hence hs ehod s prclrly ell sed or bondry vle probles h ne spl dons. We hope o eend he proposed ehod sng generlzed gerre polynols or spl dscrezon or probles on hl-lne [3]. oreover hs ehod y be eended o he o-densonl cse or slr probles.

8 46 A.H. BHRAWY 8 ACKOWEDGES hs pper s nded by he Denshp o Scenc Reserch DSR Kng Abdlzz Unversy Jeddh nder grn no. 9/838/434. he hor hereore cknoledges h hnks DSR echncl nd nncl sppor. REFERECES. C. CAUO e l. Specrl ehods: Fndenls n Sngle Dons Sprnger-Verlg e York 6.. A.H. BHRAWY.A. ZAKY A ehod bsed on he Jcob pproon or solvng l-er e-spce rconl prl derenl eons J. Cop. hys. 8 pp A.H. BHRAWY An ecen Jcob psedospecrl pproon or nonlner cople generlzed Zkhrov syse Appl. h. Cop. 47 pp E.H. DOHA e l. An ccre egendre collocon schee or copled hyperbolc eons h vrble coecens. Ro. J. hys. 59 pp H. SCHAE K. ESÄSSER he pplcon o he specrl ehod o nonlner ve propgon J. Cop. hys. pp E.H. DOHA e l. ercl reen o copled nonlner hyperbolc Klen-Gordon eons Ro. J. hys. 59 pp J. A B-W. I J.R. HOWE herl rdon he rnser n one- nd o-densonl enclosres sng he specrl collocon ehod h ll specr k-dsrbon odel In. J. He ss rnser 7 pp X. A C. HUAG Specrl collocon ehod or lner rconl negro-derenl eons Appl. h. odell. 38 pp E.H. DOHA A.H. BHRAWY R.. HAFEZ On shed Jcob specrl ehod or hgh-order l-pon bondry vle probles Con. onlner Sc. er. Sl. 7 pp S.R. AU H. RICE Sprse specrl- ehod or he hree-densonl helclly redced ve eon on o-cener dons J. Cop. hys. 3 pp A. E-KHAEB.E. A-HOHAY H.S. HUSSIE Specrl Glerkn ehod or opl conrol probles governed by negrl nd negro- derenl eons hecl Scences eers pp Y.YAG Jcob specrl Glerkn ehods or rconl negro-derenl eons Clcolo DOI.7/s ZAYEROURI. AISWORH G.E. KARIADAKIS A ned erov-glerkn specrl ehod or rconl DEs Coper ehods n Appled echncs nd Engneerng do:.6/.c G.W. WAG.Z. XU he proved rconl sb-eon ehod nd s pplcons o nonlner rconl prl derenl eons Ro. Rep. hys. 66 pp A. AKIAR e l. ercl Solon o Frconl Benney Eon Appl h. Inor. Sc. 8 pp S.J. SADAI e l. Soe rconl coprson resls nd sbly heore or rconl e dely syses Ro. Rep. hys. 65 pp A..O. AWAR e l. Frconl Cpo he eon hn he doble plce rnsor Ro. J. hys. 58 pp A. BORHAIFAR KH. SADRI A ne operonl pproch or nercl solon o generlzed nconl negroderenl eons J. Cop. Appl. h. 79 pp H. HEYDARI e l. Wveles ehod or he e rconl dson-ve eon hys. e. A 379 pp H.A.A. E-SAKA he Frconl-order SIR nd SIRS Epdec odels h Vrble oplon Sze h. Sc. e. pp G.A. EES D.V. AGHE Frconl eclson sscs n non-hoogeneos nercng prcle syses Ro. Rep. hys. 66 pp A.A.. ARAFA S.Z. RIDA. KHAI Solons o Frconl Order odel o Chldhood Dseses h Consn Vccnon Sregy hecl Scences eers pp D. CAFAGA Frconl clcls: hecl ool ro he ps or he presen engneer IEEE rnscons on Indsrl Elecroncs pp J. A J. IU Z. ZHOU Convergence nlyss o ovng ne eleen ehods or spce rconl derenl eons J. Cop. Appl. h. 55 pp B. JI R. AZAROV Y. IU Z. ZHOU he Glerkn ne eleen ehod or l-er e-rconl dson eon J. Cop. hys. 8 pp I D. XU. UO Alernng drecon plc Glerkn ne eleen ehod or he o-densonl rconl dson-ve eon J. Cop. hys. 55 pp EERSCHAER C. ADJERA Fne derence pproons or o-sded spce-rconl prl derenl eons Appl. er. h. 56 pp Z. DIG A. XIAO. I Weghed ne derence ehods or clss o spce rconl prl derenl eons h vrble coecens J. Cop. Appl. h. 33 pp

9 9 A ne specrl lgorh or e-spce rconl prl derenl eons h sbdson nd sperdson H. WAG. DU Fs lernng-drecon ne derence ehods or hree-densonl spce-rconl dson eons J. Cop. hys. 58 pp A.H. BHRAWY A.A. A-ZAHRAI Y.A. AHAED D. BAEAU A ne generlzed gerre-gss collocon schee or nercl solon o generlzed rconl pnogrph eons Ro. J. hys. 59 pp OKHARY Reconsrcon o eponenlly re o convergence o egendre collocon solon o clss o rconl negro-derenl eons J. Cop. Appl. h. 79 pp E.H. DOHA D. BAEAU A.H. BHRAWY R.. HAFEZ A Jcob collocon ehod or roesch s proble n pls physcs roc. Ronn Acd. Seres A 5 pp A. KAYEDI-BARDEH. ESAHCHI. DEHGHA A ehod or obnng he operonl r o rconl Jcob ncons nd pplcons Jornl o Vbron nd Conrol pp S. IRADOUS-AKCHI e l. ercl solon or clss o rconl convecon dson eons sng he lle oble lveles Jornl o Vbron nd Conrol pp K. IER B. ROSS An Inrodcon o he Frconl Clcls nd Frconl Derenl Eons John Wley & Sons Inc. e York G. SZEGÖ Orhogonl olynols Collo blcons XXIII Aercn hecl Socey Y. UKE he Specl Fncons nd her Approons Vol. Acdec ress e York A.H. BHRAWY.A. ZAKY D. BAEAU e nercl pproons or spce-e rconl Brgers eons v egendre specrl-collocon ehod Ro. Rep. hys E.H. DOHA A.H. BHRAWY R.. HAFEZ.A. ABDEKAWY A Chebyshev-Gss-Rd schee or nonlner hyperbolc syse o rs order Appl. h. Inor. Sc. 8 pp F. IU C. YAG K. BURRAGE ercl ehod nd nlycl echne o he oded nolos sbdson eon h nonlner sorce er J. Cop. Appl. h. 3 pp Q. IU F. IU I. URER V. AH Fne eleen pproon or oded nolos sbdson eon Appl. h. odel. 35 pp A. OHEBBI. ABBASZADEH. DEHGHA A hgh-order nd ncondonlly sble schee or he oded nolos rconl sb-dson eon h nonlner sorce er J. Cop. hys. 4 pp C. I Z. ZHAO Y.Q. CHE ercl pproon o nonlner rconl derenl eons h sbdson nd sperdson Cop. h. Appl. 6 pp J. RE Z-Z. SU X. ZHAO Copc derence schee or he rconl sb-dson eon h enn bondry condons J. Cop. hys. 3 pp Receved Deceber 4

Supporting information How to concatenate the local attractors of subnetworks in the HPFP

Supporting information How to concatenate the local attractors of subnetworks in the HPFP n Effcen lgorh for Idenfyng Prry Phenoype rcors of Lrge-Scle Boolen Newor Sng-Mo Choo nd Kwng-Hyun Cho Depren of Mhecs Unversy of Ulsn Ulsn 446 Republc of Kore Depren of Bo nd Brn Engneerng Kore dvnced

More information

1.B Appendix to Chapter 1

1.B Appendix to Chapter 1 Secon.B.B Append o Chper.B. The Ordnr Clcl Here re led ome mporn concep rom he ordnr clcl. The Dervve Conder ncon o one ndependen vrble. The dervve o dened b d d lm lm.b. where he ncremen n de o n ncremen

More information

NUMERICAL SOLUTION OF THIN FILM EQUATION IN A CLASS OF DISCONTINUOUS FUNCTIONS

NUMERICAL SOLUTION OF THIN FILM EQUATION IN A CLASS OF DISCONTINUOUS FUNCTIONS Eropen Scenfc Jornl Ags 5 /SPECAL/ eon SSN: 857 788 Prn e - SSN 857-74 NMERCAL SOLON OF HN FLM EQAON N A CLASS OF DSCONNOS FNCONS Bn Snsoysl Assoc Prof Mr Rslov Prof Beyen nversy Deprmen of Memcs n Compng

More information

ANOTHER CATEGORY OF THE STOCHASTIC DEPENDENCE FOR ECONOMETRIC MODELING OF TIME SERIES DATA

ANOTHER CATEGORY OF THE STOCHASTIC DEPENDENCE FOR ECONOMETRIC MODELING OF TIME SERIES DATA Tn Corn DOSESCU Ph D Dre Cner Chrsn Unversy Buchres Consnn RAISCHI PhD Depren of Mhecs The Buchres Acdey of Econoc Sudes ANOTHER CATEGORY OF THE STOCHASTIC DEPENDENCE FOR ECONOMETRIC MODELING OF TIME SERIES

More information

II The Z Transform. Topics to be covered. 1. Introduction. 2. The Z transform. 3. Z transforms of elementary functions

II The Z Transform. Topics to be covered. 1. Introduction. 2. The Z transform. 3. Z transforms of elementary functions II The Z Trnsfor Tocs o e covered. Inroducon. The Z rnsfor 3. Z rnsfors of eleenry funcons 4. Proeres nd Theory of rnsfor 5. The nverse rnsfor 6. Z rnsfor for solvng dfference equons II. Inroducon The

More information

THE EXISTENCE OF SOLUTIONS FOR A CLASS OF IMPULSIVE FRACTIONAL Q-DIFFERENCE EQUATIONS

THE EXISTENCE OF SOLUTIONS FOR A CLASS OF IMPULSIVE FRACTIONAL Q-DIFFERENCE EQUATIONS Europen Journl of Mhemcs nd Compuer Scence Vol 4 No, 7 SSN 59-995 THE EXSTENCE OF SOLUTONS FOR A CLASS OF MPULSVE FRACTONAL Q-DFFERENCE EQUATONS Shuyun Wn, Yu Tng, Q GE Deprmen of Mhemcs, Ynbn Unversy,

More information

Chapter 6 DETECTION AND ESTIMATION: Model of digital communication system. Fundamental issues in digital communications are

Chapter 6 DETECTION AND ESTIMATION: Model of digital communication system. Fundamental issues in digital communications are Chaper 6 DCIO AD IMAIO: Fndaenal sses n dgal concaons are. Deecon and. saon Deecon heory: I deals wh he desgn and evalaon of decson ang processor ha observes he receved sgnal and gesses whch parclar sybol

More information

Jordan Journal of Physics

Jordan Journal of Physics Volume, Number, 00. pp. 47-54 RTICLE Jordn Journl of Physcs Frconl Cnoncl Qunzon of he Free Elecromgnec Lgrngn ensy E. K. Jrd, R. S. w b nd J. M. Khlfeh eprmen of Physcs, Unversy of Jordn, 94 mmn, Jordn.

More information

ISSN 075-7 : (7) 0 007 C ( ), E-l: ssolos@glco FPGA LUT FPGA EM : FPGA, LUT, EM,,, () FPGA (feldprogrble ge rrs) [, ] () [], () [] () [5] [6] FPGA LUT (Look-Up-Tbles) EM (Ebedded Meor locks) [7, 8] LUT

More information

P-Convexity Property in Musielak-Orlicz Function Space of Bohner Type

P-Convexity Property in Musielak-Orlicz Function Space of Bohner Type J N Sce & Mh Res Vol 3 No (7) -7 Alble ole h://orlwlsogocd/deh/sr P-Coey Proery Msel-Orlcz Fco Sce o Boher ye Yl Rodsr Mhecs Edco Deree Fcly o Ss d echology Uerss sl Neger Wlsogo Cerl Jdoes Absrcs Corresodg

More information

Modeling of magnetic levitation system

Modeling of magnetic levitation system 7 s Inernonl Conference on Process Conrol (PC) June 6 7 Šrbské Pleso Slovk Modelng of gnec levon syse Peer Blko Dnc Rosnová Insue of uoove Mechroncs Slovk Unversy of Technology n Brslv Brslv Slovk dnc.rosnov@sub.sk

More information

Background and Motivation: Importance of Pressure Measurements

Background and Motivation: Importance of Pressure Measurements Imornce of Pressre Mesremens: Pressre s rmry concern for mny engneerng lcons e.g. lf nd form drg. Cvon : Pressre s of fndmenl mornce n ndersndng nd modelng cvon. Trblence: Velocy-Pressre-Grden ensor whch

More information

Introduction. Voice Coil Motors. Introduction - Voice Coil Velocimeter Electromechanical Systems. F = Bli

Introduction. Voice Coil Motors. Introduction - Voice Coil Velocimeter Electromechanical Systems. F = Bli UNIVERSITY O TECHNOLOGY, SYDNEY ACULTY O ENGINEERING 4853 Elecroechncl Syses Voce Col Moors Topcs o cover:.. Mnec Crcus 3. EM n Voce Col 4. orce n Torque 5. Mhecl Moel 6. Perornce Voce cols re wely use

More information

Chapter 6. Isoparametric Formulation

Chapter 6. Isoparametric Formulation ME 78 FIIE ELEME MEHOD Chper. Ioprerc Forlon Se fncon h ed o defne he eleen geoer ed o defne he dplceen whn he eleen ode r Eleen Lner geoer Lner dplceen ode Be Eleen Qdrc geoer Qdrc dplceen We gn he e

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

Chebyshev Polynomial Solution of Nonlinear Fredholm-Volterra Integro- Differential Equations

Chebyshev Polynomial Solution of Nonlinear Fredholm-Volterra Integro- Differential Equations Çny Ünvee Fen-Edeby Füle Jounl of A nd Scence Sy : 5 y 6 Chebyhev Polynol Soluon of onlne Fedhol-Vole Inego- Dffeenl Equon Hndn ÇERDİK-YASA nd Ayşegül AKYÜZ-DAŞCIOĞU Abc In h ppe Chebyhev collocon ehod

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

Review: Transformations. Transformations - Viewing. Transformations - Modeling. world CAMERA OBJECT WORLD CSE 681 CSE 681 CSE 681 CSE 681

Review: Transformations. Transformations - Viewing. Transformations - Modeling. world CAMERA OBJECT WORLD CSE 681 CSE 681 CSE 681 CSE 681 Revew: Trnsforons Trnsforons Modelng rnsforons buld cople odels b posonng (rnsforng sple coponens relve o ech oher ewng rnsforons plcng vrul cer n he world rnsforon fro world coordnes o cer coordnes Perspecve

More information

EL-GENDI NODAL GALERKIN METHOD FOR SOLVING LINEAR AND NONLINEAR PARTIAL FRACTIONAL SPACE EQUATIONS

EL-GENDI NODAL GALERKIN METHOD FOR SOLVING LINEAR AND NONLINEAR PARTIAL FRACTIONAL SPACE EQUATIONS Inernon Jorn o es Reserch n Scence nd Technoogy Vome Isse 6: Pge o-7 ovemer-ecemer 3 hp://wwwmnornscom/rshm ISS (Onne):78-599 E-GEI OA GAERKI ETO FOR SOVIG IEAR A OIEAR PARTIA FRACTIOA SPACE EQATIOS *

More information

UNIVERSAL BOUNDS FOR EIGENVALUES OF FOURTH-ORDER WEIGHTED POLYNOMIAL OPERATOR ON DOMAINS IN COMPLEX PROJECTIVE SPACES

UNIVERSAL BOUNDS FOR EIGENVALUES OF FOURTH-ORDER WEIGHTED POLYNOMIAL OPERATOR ON DOMAINS IN COMPLEX PROJECTIVE SPACES wwwrresscom/volmes/vol7isse/ijrras_7 df UNIVERSAL BOUNDS FOR EIGENVALUES OF FOURTH-ORDER WEIGHTED POLYNOIAL OPERATOR ON DOAINS IN COPLEX PROJECTIVE SPACES D Feng & L Ynl * Scool of emcs nd Pyscs Scence

More information

Numerical Simulations of Femtosecond Pulse. Propagation in Photonic Crystal Fibers. Comparative Study of the S-SSFM and RK4IP

Numerical Simulations of Femtosecond Pulse. Propagation in Photonic Crystal Fibers. Comparative Study of the S-SSFM and RK4IP Appled Mhemcl Scences Vol. 6 1 no. 117 5841 585 Numercl Smulons of Femosecond Pulse Propgon n Phoonc Crysl Fbers Comprve Sudy of he S-SSFM nd RK4IP Mourd Mhboub Scences Fculy Unversy of Tlemcen BP.119

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

Physics 201 Lecture 2

Physics 201 Lecture 2 Physcs 1 Lecure Lecure Chper.1-. Dene Poson, Dsplcemen & Dsnce Dsngush Tme nd Tme Inerl Dene Velocy (Aerge nd Insnneous), Speed Dene Acceleron Undersnd lgebrclly, hrough ecors, nd grphclly he relonshps

More information

Power Series Solutions for Nonlinear Systems. of Partial Differential Equations

Power Series Solutions for Nonlinear Systems. of Partial Differential Equations Appled Mhemcl Scences, Vol. 6, 1, no. 14, 5147-5159 Power Seres Soluons for Nonlner Sysems of Prl Dfferenl Equons Amen S. Nuser Jordn Unversy of Scence nd Technology P. O. Bo 33, Irbd, 11, Jordn nuser@us.edu.o

More information

Chapter 2. Review of Hydrodynamics and Vector Analysis

Chapter 2. Review of Hydrodynamics and Vector Analysis her. Ree o Hdrodmcs d Vecor Alss. Tlor seres L L L L ' ' L L " " " M L L! " ' L " ' I s o he c e romed he Tlor seres. O he oher hd ' " L . osero o mss -dreco: L L IN ] OUT [mss l [mss l] mss ccmled h me

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

[ ] 2. [ ]3 + (Δx i + Δx i 1 ) / 2. Δx i-1 Δx i Δx i+1. TPG4160 Reservoir Simulation 2018 Lecture note 3. page 1 of 5

[ ] 2. [ ]3 + (Δx i + Δx i 1 ) / 2. Δx i-1 Δx i Δx i+1. TPG4160 Reservoir Simulation 2018 Lecture note 3. page 1 of 5 TPG460 Reservor Smulaon 08 page of 5 DISCRETIZATIO OF THE FOW EQUATIOS As we already have seen, fne dfference appromaons of he paral dervaves appearng n he flow equaons may be obaned from Taylor seres

More information

Stochastic Programming handling CVAR in objective and constraint

Stochastic Programming handling CVAR in objective and constraint Sochasc Programmng handlng CVAR n obecve and consran Leondas Sakalaskas VU Inse of Mahemacs and Informacs Lhana ICSP XIII Jly 8-2 23 Bergamo Ialy Olne Inrodcon Lagrangan & KKT condons Mone-Carlo samplng

More information

The Characterization of Jones Polynomial. for Some Knots

The Characterization of Jones Polynomial. for Some Knots Inernon Mhemc Forum,, 8, no, 9 - The Chrceron of Jones Poynom for Some Knos Mur Cncn Yuuncu Y Ünversy, Fcuy of rs nd Scences Mhemcs Deprmen, 8, n, Turkey m_cencen@yhoocom İsm Yr Non Educon Mnsry, 8, n,

More information

Exponents and Powers

Exponents and Powers EXPONENTS AND POWERS 9 Exponents nd Powers CHAPTER. Introduction Do you know? Mss of erth is 5,970,000,000,000, 000, 000, 000, 000 kg. We hve lredy lernt in erlier clss how to write such lrge nubers ore

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

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

Solvability of nonlinear Klein-Gordon equation by Laplace Decomposition Method

Solvability of nonlinear Klein-Gordon equation by Laplace Decomposition Method Vol. 84 pp. 37-4 Jly 5 DOI:.5897/JMCSR4.57 icle Nbe: 63F95459 ISSN 6-973 Copyigh 5 hos ein he copyigh of his icle hp://www.cdeicjonls.og/jmcsr ficn Jonl of Mheics nd Cope Science Resech Fll Lengh Resech

More information

4. Runge-Kutta Formula For Differential Equations. A. Euler Formula B. Runge-Kutta Formula C. An Example for Fourth-Order Runge-Kutta Formula

4. Runge-Kutta Formula For Differential Equations. A. Euler Formula B. Runge-Kutta Formula C. An Example for Fourth-Order Runge-Kutta Formula NCTU Deprme o Elecrcl d Compuer Egeerg Seor Course By Pro. Yo-Pg Ce. Ruge-Ku Formul For Derel Equos A. Euler Formul B. Ruge-Ku Formul C. A Emple or Four-Order Ruge-Ku Formul

More information

Lump Solutions to a Jimbo-Miwa Like Equations

Lump Solutions to a Jimbo-Miwa Like Equations Lump Soluons o Jmbo-Mw Lke Equons Hrun-Or-Roshd * M. Zulkr Al b Deprmen o Mhemcs Pbn Unvers o Scence nd Technolog Bngldesh b Deprmen o Mhemcs Rjshh Unvers Bngldesh * Eml: hrunorroshdmd@gml.com Absrc A

More information

Observer Design for Nonlinear Systems using Linear Approximations

Observer Design for Nonlinear Systems using Linear Approximations Observer Desgn for Nonlnear Ssems sng Lnear Appromaons C. Navarro Hernandez, S.P. Banks and M. Aldeen Deparmen of Aomac Conrol and Ssems Engneerng, Unvers of Sheffeld, Mappn Sree, Sheffeld S 3JD. e-mal:

More information

Introduction. Section 9: HIGHER ORDER TWO DIMENSIONAL SHAPE FUNCTIONS

Introduction. Section 9: HIGHER ORDER TWO DIMENSIONAL SHAPE FUNCTIONS Secon 9: HIGHER ORDER TWO DIMESIO SHPE FUCTIOS Inroducon We ne conder hpe funcon for hgher order eleen. To do h n n orderl fhon we nroduce he concep of re coordne. Conder ere of rngulr eleen depced n he

More information

Investigation of the Evolution Equations of the. Three-Body Problem with Variable Masses

Investigation of the Evolution Equations of the. Three-Body Problem with Variable Masses led Mhecl cences Vol. 7 no. 89 9-5 HIKRI Ld www.-hkr.co h://dx.do.org/.988/s.. Invesgon o he Evoluon Euons o he hree-ody Proble wh Vrble Msses M. Zh. Mnglbyev Deren o Mechncs l-frb Kzkh Nonl Unversy l-frb

More information

Spectral Galerkin Method for Optimal Control Problems Governed by Integral and Integro- Differential Equations

Spectral Galerkin Method for Optimal Control Problems Governed by Integral and Integro- Differential Equations Mh. Sci. Le. Vol. o. 33-4 Mheicl Sciences Leers An Inernionl Journl @ SP url Sciences Publishing Cor. Specrl Glerin Mehod or Opil Conrol Probles Governed by Inegrl nd Inegro- Dierenil Equions Mos A. El-Kheb

More information

Research Article Oscillatory Criteria for Higher Order Functional Differential Equations with Damping

Research Article Oscillatory Criteria for Higher Order Functional Differential Equations with Damping Journl of Funcon Spces nd Applcons Volume 2013, Arcle ID 968356, 5 pges hp://dx.do.org/10.1155/2013/968356 Reserch Arcle Oscllory Crer for Hgher Order Funconl Dfferenl Equons wh Dmpng Pegung Wng 1 nd H

More information

A NEW INTERPRETATION OF INTERVAL-VALUED FUZZY INTERIOR IDEALS OF ORDERED SEMIGROUPS

A NEW INTERPRETATION OF INTERVAL-VALUED FUZZY INTERIOR IDEALS OF ORDERED SEMIGROUPS ScInLhore),7),9-37,4 ISSN 3-536; CODEN: SINTE 8 9 A NEW INTERPRETATION O INTERVAL-VALUED UZZY INTERIOR IDEALS O ORDERED SEMIGROUPS Hdy Ullh Khn, b, Nor Hnz Srmn, Asghr Khn c nd z Muhmmd Khn d Deprmen of

More information

4. Runge-Kutta Formula For Differential Equations

4. Runge-Kutta Formula For Differential Equations NCTU Deprme o Elecrcl d Compuer Egeerg 5 Sprg Course by Pro. Yo-Pg Ce. Ruge-Ku Formul For Derel Equos To solve e derel equos umerclly e mos useul ormul s clled Ruge-Ku ormul

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

THIS PAGE DECLASSIFIED IAW EO IRIS u blic Record. Key I fo mation. Ma n: AIR MATERIEL COMM ND. Adm ni trative Mar ings.

THIS PAGE DECLASSIFIED IAW EO IRIS u blic Record. Key I fo mation. Ma n: AIR MATERIEL COMM ND. Adm ni trative Mar ings. T H S PA G E D E CLA SSFED AW E O 2958 RS u blc Recod Key fo maon Ma n AR MATEREL COMM ND D cumen Type Call N u b e 03 V 7 Rcvd Rel 98 / 0 ndexe D 38 Eneed Dae RS l umbe 0 0 4 2 3 5 6 C D QC d Dac A cesson

More information

THE FINITE HAUSDORFF AND FRACTAL DIMENSIONS OF THE GLOBAL ATTRACTOR FOR A CLASS KIRCHHOFF-TYPE EQUATIONS

THE FINITE HAUSDORFF AND FRACTAL DIMENSIONS OF THE GLOBAL ATTRACTOR FOR A CLASS KIRCHHOFF-TYPE EQUATIONS European Journal of Maheaics and Copuer Science Vol 4 No 7 ISSN 59-995 HE FINIE HAUSDORFF AND FRACAL DIMENSIONS OF HE GLOBAL ARACOR FOR A CLASS KIRCHHOFF-YPE EQUAIONS Guoguang Lin & Xiangshuang Xia Deparen

More information

Some algorthim for solving system of linear volterra integral equation of second kind by using MATLAB 7 ALAN JALAL ABD ALKADER

Some algorthim for solving system of linear volterra integral equation of second kind by using MATLAB 7 ALAN JALAL ABD ALKADER . Soe lgoi o solving syse o line vole inegl eqion o second ind by sing MATLAB 7 ALAN JALAL ABD ALKADER College o Edcion / Al- Msnsiiy Univesiy Depen o Meics تقديم البحث :-//7 قبول النشر:- //. Absc ( /

More information

Chapter Bisection Method of Solving a Nonlinear Equation

Chapter Bisection Method of Solving a Nonlinear Equation Chpter 00 Bisection Method o Solving Nonliner Eqtion Ater reding this chpter, yo shold be ble to: 1 ollow the lgorith o the bisection ethod o solving nonliner eqtion, se the bisection ethod to solve eples

More information

ON THE WEAK LIMITS OF SMOOTH MAPS FOR THE DIRICHLET ENERGY BETWEEN MANIFOLDS

ON THE WEAK LIMITS OF SMOOTH MAPS FOR THE DIRICHLET ENERGY BETWEEN MANIFOLDS ON THE WEA LIMITS OF SMOOTH MAPS FOR THE DIRICHLET ENERGY BETWEEN MANIFOLDS FENGBO HANG Absrac. We denfy all he weak sequenal lms of smooh maps n W (M N). In parcular, hs mples a necessary su cen opologcal

More information

CHAPTER 10: LINEAR DISCRIMINATION

CHAPTER 10: LINEAR DISCRIMINATION CHAPER : LINEAR DISCRIMINAION Dscrmnan-based Classfcaon 3 In classfcaon h K classes (C,C,, C k ) We defned dscrmnan funcon g j (), j=,,,k hen gven an es eample, e chose (predced) s class label as C f g

More information

CHAPTER ARCH models. 1.1 Introduction

CHAPTER ARCH models. 1.1 Introduction CHAPTER. ARCH odels. Inrodcon A crcl sson n ny sscl odels s o consn vrnce. Lely, ly o e seres odels s been develoed relxng e sson o consn vrnce rog e. Ts ly s clled Aoregressve Condonl Heeroskedscy (ARCH)

More information

, t 1. Transitions - this one was easy, but in general the hardest part is choosing the which variables are state and control variables

, t 1. Transitions - this one was easy, but in general the hardest part is choosing the which variables are state and control variables Opmal Conrol Why Use I - verss calcls of varaons, opmal conrol More generaly More convenen wh consrans (e.g., can p consrans on he dervaves More nsghs no problem (a leas more apparen han hrogh calcls of

More information

Application of Homotopy Analysis Method for Solving various types of Problems of Partial Differential Equations

Application of Homotopy Analysis Method for Solving various types of Problems of Partial Differential Equations Applicaion of Hooopy Analysis Mehod for olving various ypes of Probles of Parial Differenial Equaions V.P.Gohil, Dr. G. A. anabha,assisan Professor, Deparen of Maheaics, Governen Engineering College, Bhavnagar,

More information

Differential Equation of Eigenvalues for Sturm Liouville Boundary Value Problem with Neumann Boundary Conditions

Differential Equation of Eigenvalues for Sturm Liouville Boundary Value Problem with Neumann Boundary Conditions Ierol Reserc Jorl o Aled d Bsc Sceces 3 Avlle ole www.rjs.co ISSN 5-838X / Vol 4 : 997-33 Scece Exlorer Plcos Derel Eqo o Eevles or Sr Lovlle Bodry Vle Prole w Ne Bodry Codos Al Kll Gold Dere o Mecs Azr

More information

PEGN 513 Reservoir Simulation I Fall 2009

PEGN 513 Reservoir Simulation I Fall 2009 Hmer #3 l The smples rm r aerld a lear cre ally saraed h l ad a resdal aer sara h gravy r capllary eecs s represeed by he -dmesal Bcley-Levere maeral balace eqa () Eplc sl Csderg he space dscreza sh Fgre

More information

F l a s h-b a s e d S S D s i n E n t e r p r i s e F l a s h-b a s e d S S D s ( S o-s ltiad t e D r i v e s ) a r e b e c o m i n g a n a t t r a c

F l a s h-b a s e d S S D s i n E n t e r p r i s e F l a s h-b a s e d S S D s ( S o-s ltiad t e D r i v e s ) a r e b e c o m i n g a n a t t r a c L i f e t i m e M a n a g e m e n t o f F l a-b s ah s e d S S D s U s i n g R e c o v e r-a y w a r e D y n a m i c T h r o t t l i n g S u n g j i n L e, e T a e j i n K i m, K y u n g h o, Kainmd J

More information

EE757 Numerical Techniques in Electromagnetics Lecture 9

EE757 Numerical Techniques in Electromagnetics Lecture 9 EE757 uericl Techiques i Elecroeics Lecure 9 EE757 06 Dr. Mohed Bkr Diereil Equios Vs. Ierl Equios Ierl equios ke severl ors e.. b K d b K d Mos diereil equios c be epressed s ierl equios e.. b F d d /

More information

Vol. 5, No. 5 May 2014 ISSN Journal of Emerging Trends in Computing and Information Sciences CIS Journal. All rights reserved.

Vol. 5, No. 5 May 2014 ISSN Journal of Emerging Trends in Computing and Information Sciences CIS Journal. All rights reserved. Vol. 5, No. 5 y 04 ISSN 079-8407 Jornl of Emergng Trends n Comptng nd Informton Scences 009-04 CIS Jornl. ll rghts reserved. http://www.csornl.org Notes on lt Soft trces D.Sngh, Onyeozl, I.., 3 lkl..j.,

More information

HEAT CONDUCTION PROBLEM IN A TWO-LAYERED HOLLOW CYLINDER BY USING THE GREEN S FUNCTION METHOD

HEAT CONDUCTION PROBLEM IN A TWO-LAYERED HOLLOW CYLINDER BY USING THE GREEN S FUNCTION METHOD Journal of Appled Mahemacs and Compuaonal Mechancs 3, (), 45-5 HEAT CONDUCTION PROBLEM IN A TWO-LAYERED HOLLOW CYLINDER BY USING THE GREEN S FUNCTION METHOD Sansław Kukla, Urszula Sedlecka Insue of Mahemacs,

More information

Solving Parabolic Partial Delay Differential. Equations Using The Explicit Method And Higher. Order Differences

Solving Parabolic Partial Delay Differential. Equations Using The Explicit Method And Higher. Order Differences Jornal of Kfa for Maemacs and Compe Vol. No.7 Dec pp 77-5 Solvng Parabolc Paral Delay Dfferenal Eqaons Usng e Eplc Meod And Hger Order Dfferences Asss. Prof. Amal Kalaf Haydar Kfa Unversy College of Edcaon

More information

Different kind of oscillation

Different kind of oscillation PhO 98 Theorecal Qeson.Elecrcy Problem (8 pons) Deren knd o oscllaon e s consder he elecrc crc n he gre, or whch mh, mh, nf, nf and kω. The swch K beng closed he crc s copled wh a sorce o alernang crren.

More information

Quantum Chemistry. Lecture 1. Disposition. Sources. Matti Hotokka Department of Physical Chemistry Åbo Akademi University

Quantum Chemistry. Lecture 1. Disposition. Sources. Matti Hotokka Department of Physical Chemistry Åbo Akademi University Lere Q hesry M Hookk epre of Physl hesry Åbo Akde Uversy oes Irodo o hs orse The HrreeFok eqos sposo Sores ) The Hükel ehod ) The HrreeFok eqos ) Bss ses d oher prles 4) Wh be lled 5) orrelo 6) The FT

More information

The Properties of Probability of Normal Chain

The Properties of Probability of Normal Chain I. J. Coep. Mah. Sceces Vol. 8 23 o. 9 433-439 HIKARI Ld www.-hkar.co The Properes of Proaly of Noral Cha L Che School of Maheacs ad Sascs Zheghou Noral Uversy Zheghou Cy Hea Provce 4544 Cha cluu6697@sa.co

More information

Parameter estimation method using an extended Kalman Filter

Parameter estimation method using an extended Kalman Filter Unvers o Wollongong Reserch Onlne cul o Engneerng nd Inormon cences - Ppers: Pr A cul o Engneerng nd Inormon cences 007 Prmeer esmon mehod usng n eended lmn ler Emmnuel D. Blnchrd Unvers o Wollongong eblnch@uow.edu.u

More information

IMPLICIT SOLUTION OF 1D NONLINEAR POROUS MEDIUM EQUATION USING THE FOUR-POINT NEWTON-EGMSOR ITERATIVE METHOD

IMPLICIT SOLUTION OF 1D NONLINEAR POROUS MEDIUM EQUATION USING THE FOUR-POINT NEWTON-EGMSOR ITERATIVE METHOD Jornl of Appled Mthetcs nd Copttonl Mechncs 06 5() - www.c.pcz.pl p-issn 99-9965 DOI: 0.75/c.06..0 e-issn 353-0588 IMPLICIT SOLUTION OF D NONLINEAR POROUS MEDIUM EQUATION USING THE FOUR-POINT NEWTON- ITERATIVE

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

The Covenant Renewed. Family Journal Page. creation; He tells us in the Bible.)

The Covenant Renewed. Family Journal Page. creation; He tells us in the Bible.) i ell orie o go ih he picure. L, up ng i gro ve el ur Pren, ho phoo picure; u oher ell ee hey (T l. chi u b o on hi pge y ur ki kn pl. (We ee Hi i H b o b o kn e hem orie.) Compre h o ho creion; He ell

More information

v v at 1 2 d vit at v v 2a d

v v at 1 2 d vit at v v 2a d SPH3UW Unt. Accelerton n One Denon Pge o 9 Note Phyc Inventory Accelerton the rte o chnge o velocty. Averge ccelerton, ve the chnge n velocty dvded by the te ntervl, v v v ve. t t v dv Intntneou ccelerton

More information

Solutions to Problems from Chapter 2

Solutions to Problems from Chapter 2 Soluions o Problems rom Chper Problem. The signls u() :5sgn(), u () :5sgn(), nd u h () :5sgn() re ploed respecively in Figures.,b,c. Noe h u h () :5sgn() :5; 8 including, bu u () :5sgn() is undeined..5

More information

Laplace Transform. Definition of Laplace Transform: f(t) that satisfies The Laplace transform of f(t) is defined as.

Laplace Transform. Definition of Laplace Transform: f(t) that satisfies The Laplace transform of f(t) is defined as. Lplce Trfor The Lplce Trfor oe of he hecl ool for olvg ordry ler dfferel equo. - The hoogeeou equo d he prculr Iegrl re olved oe opero. - The Lplce rfor cover he ODE o lgerc eq. σ j ple do. I he pole o

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

Analytical Study of a Special Case of Complex Canonical Transform

Analytical Study of a Special Case of Complex Canonical Transform lobl Jornl o Mhmcl Scncs: hory n Prccl Volm, Nmbr 3 00, pp 6--70 Inrnonl Rsrch Pblcon Hos hp://wwwrphoscom Anlycl Sy o Spcl Cs o Complx Cnoncl rnsorm PR Dshmkh n AS h Pro Rm Mgh Ins o chnology & Rsrch,

More information

Variational method to the second-order impulsive partial differential equations with inconstant coefficients (I)

Variational method to the second-order impulsive partial differential equations with inconstant coefficients (I) Avalable onlne a www.scencedrec.com Proceda Engneerng 6 ( 5 4 Inernaonal Worksho on Aomoble, Power and Energy Engneerng Varaonal mehod o he second-order mlsve aral dfferenal eqaons wh nconsan coeffcens

More information

Calculus 241, section 12.2 Limits/Continuity & 12.3 Derivatives/Integrals notes by Tim Pilachowski r r r =, with a domain of real ( )

Calculus 241, section 12.2 Limits/Continuity & 12.3 Derivatives/Integrals notes by Tim Pilachowski r r r =, with a domain of real ( ) Clculu 4, econ Lm/Connuy & Devve/Inel noe y Tm Plchow, wh domn o el Wh we hve o : veco-vlued uncon, ( ) ( ) ( ) j ( ) nume nd ne o veco The uncon, nd A w done wh eul uncon ( x) nd connuy e he componen

More information

Multivariate Time Series Analysis

Multivariate Time Series Analysis Mulvre me Sere Anl Le { : } be Mulvre me ere. Denon: () = men vlue uncon o { : } = E[ ] or. (,) = Lgged covrnce mr o { : } = E{[ - ()][ - ()]'} or, Denon: e me ere { : } onr e jon drbuon o,,, e me e jon

More information

Dynamic Model of the Axially Moving Viscoelastic Belt System with Tensioner Pulley Yanqi Liu1, a, Hongyu Wang2, b, Dongxing Cao3, c, Xiaoling Gai1, d

Dynamic Model of the Axially Moving Viscoelastic Belt System with Tensioner Pulley Yanqi Liu1, a, Hongyu Wang2, b, Dongxing Cao3, c, Xiaoling Gai1, d Inernaonal Indsral Informacs and Comper Engneerng Conference (IIICEC 5) Dynamc Model of he Aally Movng Vscoelasc Bel Sysem wh Tensoner Plley Yanq L, a, Hongy Wang, b, Dongng Cao, c, Xaolng Ga, d Bejng

More information

Relative controllability of nonlinear systems with delays in control

Relative controllability of nonlinear systems with delays in control Relave conrollably o nonlnear sysems wh delays n conrol Jerzy Klamka Insue o Conrol Engneerng, Slesan Techncal Unversy, 44- Glwce, Poland. phone/ax : 48 32 37227, {jklamka}@a.polsl.glwce.pl Keywor: Conrollably.

More information

Solution of a diffusion problem in a non-homogeneous flow and diffusion field by the integral representation method (IRM)

Solution of a diffusion problem in a non-homogeneous flow and diffusion field by the integral representation method (IRM) Appled and ompaonal Mahemacs 4; 3: 5-6 Pblshed onlne Febrary 4 hp://www.scencepblshnggrop.com//acm do:.648/.acm.43.3 olon of a dffson problem n a non-homogeneos flow and dffson feld by he negral represenaon

More information

Second degree generalized gauss-seidel iteration method for solving linear system of equations. ABSTRACT

Second degree generalized gauss-seidel iteration method for solving linear system of equations. ABSTRACT Ethiop. J. Sci. & Technol. 7( 5-, 0 5 Second degree generlized guss-seidel itertion ethod for solving liner syste of equtions Tesfye Keede Bhir Dr University, College of Science, Deprtent of Mthetics tk_ke@yhoo.co

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

Approximate Analytic Solution of (2+1) - Dimensional Zakharov-Kuznetsov(Zk) Equations Using Homotopy

Approximate Analytic Solution of (2+1) - Dimensional Zakharov-Kuznetsov(Zk) Equations Using Homotopy Arcle Inernaonal Journal of Modern Mahemacal Scences, 4, (): - Inernaonal Journal of Modern Mahemacal Scences Journal homepage: www.modernscenfcpress.com/journals/jmms.aspx ISSN: 66-86X Florda, USA Approxmae

More information

Exact solitary-wave Special Solutions for the Nonlinear Dispersive K(m,n) Equations by Means of the Homotopy Analysis Method

Exact solitary-wave Special Solutions for the Nonlinear Dispersive K(m,n) Equations by Means of the Homotopy Analysis Method Available a hp://pva.ed/aa Appl. Appl. Mah. ISSN: 93-9466 Special Isse No. (Ags ) pp. 8 93 Applicaions Applied Maheaics: An Inernaional Jornal (AAM) Eac soliary-wave Special Solions for he Nonlinear Dispersive

More information

Fingerprint Registration Using Centroid Structure and Line Segments 1

Fingerprint Registration Using Centroid Structure and Line Segments 1 IJCSS Inernonl Journl of Copuer Scence nd ewor Secur, VOL.6 o.3, Mrch 006 97 Fngerprn Regsron Usng Cenrod Srucure nd Lne Segens Deun Zho, Fe Su nd nn C ejng Unvers of Poss nd elecouncons, School of elecouncon

More information

M. Y. Adamu Mathematical Sciences Programme, AbubakarTafawaBalewa University, Bauchi, Nigeria

M. Y. Adamu Mathematical Sciences Programme, AbubakarTafawaBalewa University, Bauchi, Nigeria IOSR Journal of Mahemacs (IOSR-JM e-issn: 78-578, p-issn: 9-765X. Volume 0, Issue 4 Ver. IV (Jul-Aug. 04, PP 40-44 Mulple SolonSoluons for a (+-dmensonalhroa-sasuma shallow waer wave equaon UsngPanlevé-Bӓclund

More information

Acoustic and flexural wave energy conservation for a thin plate in a fluid

Acoustic and flexural wave energy conservation for a thin plate in a fluid cousc nd fleurl wve energy conservon for hn ple n flud rryl MCMHON 1 Mrme vson efence Scence nd Technology Orgnson HMS Srlng W usrl STRCT lhough he equons of fleurl wve moon for hn ple n vcuum nd flud

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

Research Article Cubic B-spline for the Numerical Solution of Parabolic Integro-differential Equation with a Weakly Singular Kernel

Research Article Cubic B-spline for the Numerical Solution of Parabolic Integro-differential Equation with a Weakly Singular Kernel Researc Jornal of Appled Scences, Engneerng and Tecnology 7(): 65-7, 4 DOI:.96/afs.7.5 ISS: 4-7459; e-iss: 4-7467 4 Mawell Scenfc Pblcaon Corp. Sbmed: Jne 8, Acceped: Jly 9, Pblsed: Marc 5, 4 Researc Arcle

More information

I M P O R T A N T S A F E T Y I N S T R U C T I O N S W h e n u s i n g t h i s e l e c t r o n i c d e v i c e, b a s i c p r e c a u t i o n s s h o

I M P O R T A N T S A F E T Y I N S T R U C T I O N S W h e n u s i n g t h i s e l e c t r o n i c d e v i c e, b a s i c p r e c a u t i o n s s h o I M P O R T A N T S A F E T Y I N S T R U C T I O N S W h e n u s i n g t h i s e l e c t r o n i c d e v i c e, b a s i c p r e c a u t i o n s s h o u l d a l w a y s b e t a k e n, i n c l u d f o l

More information

THEORETICAL AUTOCORRELATIONS. ) if often denoted by γ. Note that

THEORETICAL AUTOCORRELATIONS. ) if often denoted by γ. Note that THEORETICAL AUTOCORRELATIONS Cov( y, y ) E( y E( y))( y E( y)) ρ = = Var( y) E( y E( y)) =,, L ρ = and Cov( y, y ) s ofen denoed by whle Var( y ) f ofen denoed by γ. Noe ha γ = γ and ρ = ρ and because

More information

A DECOMPOSITION METHOD FOR SOLVING DIFFUSION EQUATIONS VIA LOCAL FRACTIONAL TIME DERIVATIVE

A DECOMPOSITION METHOD FOR SOLVING DIFFUSION EQUATIONS VIA LOCAL FRACTIONAL TIME DERIVATIVE S13 A DECOMPOSITION METHOD FOR SOLVING DIFFUSION EQUATIONS VIA LOCAL FRACTIONAL TIME DERIVATIVE by Hossen JAFARI a,b, Haleh TAJADODI c, and Sarah Jane JOHNSTON a a Deparen of Maheacal Scences, Unversy

More information

b denotes trend at time point t and it is sum of two

b denotes trend at time point t and it is sum of two Inernaional Conference on Innovaive Applicaions in Engineering and Inforaion echnology(iciaei207) Inernaional Journal of Advanced Scienific echnologies,engineering and Manageen Sciences (IJASEMSISSN: 2454356X)

More information

Numbers Related to Bernoulli-Goss Numbers

Numbers Related to Bernoulli-Goss Numbers ursh Journl of Anlyss n Nuber heory, 4, Vol., No., -8 Avlble onlne t htt://ubs.sceub.co/tnt///4 Scence n Eucton Publshng OI:.69/tnt---4 Nubers Relte to Bernoull-Goss Nubers Mohe Oul ouh Benough * érteent

More information

A L A BA M A L A W R E V IE W

A L A BA M A L A W R E V IE W A L A BA M A L A W R E V IE W Volume 52 Fall 2000 Number 1 B E F O R E D I S A B I L I T Y C I V I L R I G HT S : C I V I L W A R P E N S I O N S A N D TH E P O L I T I C S O F D I S A B I L I T Y I N

More information

Scalar Conservation Laws

Scalar Conservation Laws MATH-459 Nmerical Mehods for Conservaion Laws by Prof. Jan S. Heshaven Solion se : Scalar Conservaion Laws Eercise. The inegral form of he scalar conservaion law + f ) = is given in Eq. below. ˆ 2, 2 )

More information

A CHEBYSHEV-LAGUERRE-GAUSS-RADAU COLLOCATION SCHEME FOR SOLVING A TIME FRACTIONAL SUB-DIFFUSION EQUATION ON A SEMI-INFINITE DOMAIN

A CHEBYSHEV-LAGUERRE-GAUSS-RADAU COLLOCATION SCHEME FOR SOLVING A TIME FRACTIONAL SUB-DIFFUSION EQUATION ON A SEMI-INFINITE DOMAIN THE PUBISHIG HOUSE PROCEEIGS OF THE ROAIA ACAEY See A OF THE ROAIA ACAEY Volme 6 mbe 4/5 pp. 49 498 A CHEBYSHEV-AGUERRE-GAUSS-RAAU COOCATIO SCHEE FOR SOVIG A TIE FRACTIOA SUB-IFFUSIO EQUATIO O A SEI-IFIITE

More information

Chapter 1 - Free Vibration of Multi-Degree-of-Freedom Systems - I

Chapter 1 - Free Vibration of Multi-Degree-of-Freedom Systems - I CEE49b Chaper - Free Vbrao of M-Degree-of-Freedo Syses - I Free Udaped Vbrao The basc ype of respose of -degree-of-freedo syses s free daped vbrao Aaogos o sge degree of freedo syses he aayss of free vbrao

More information

15/03/1439. Lecture 4: Linear Time Invariant (LTI) systems

15/03/1439. Lecture 4: Linear Time Invariant (LTI) systems Lecre 4: Liner Time Invrin LTI sysems 2. Liner sysems, Convolion 3 lecres: Implse response, inp signls s coninm of implses. Convolion, discree-ime nd coninos-ime. LTI sysems nd convolion Specific objecives

More information

An analytical solution versus half space BEM formulation for acoustic radiation and scattering from a rigid sphere

An analytical solution versus half space BEM formulation for acoustic radiation and scattering from a rigid sphere Journl of Phyc: Conference Sere PAPER OPEN ACCESS An nlycl oluon veru hlf pce forulon for couc rdon nd cerng fro rgd phere To ce h rcle: B. Soenrko nd D. Sedkrun 06 J. Phy.: Conf. Ser. 776 0065 Reled conen

More information

I N A C O M P L E X W O R L D

I N A C O M P L E X W O R L D IS L A M I C E C O N O M I C S I N A C O M P L E X W O R L D E x p l o r a t i o n s i n A g-b eanste d S i m u l a t i o n S a m i A l-s u w a i l e m 1 4 2 9 H 2 0 0 8 I s l a m i c D e v e l o p m e

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

Available online Journal of Scientific and Engineering Research, 2017, 4(2): Research Article

Available online   Journal of Scientific and Engineering Research, 2017, 4(2): Research Article Avlble onlne www.jse.com Jonl of Scenfc nd Engneeng Resech, 7, 4():5- Resech Acle SSN: 394-63 CODEN(USA): JSERBR Exc Solons of Qselsc Poblems of Lne Theoy of Vscoelscy nd Nonlne Theoy Vscoelscy fo echnclly

More information