A posteriori pointwise error estimation for compressible fluid flows using adjoint parameters and Lagrange remainder

Size: px
Start display at page:

Download "A posteriori pointwise error estimation for compressible fluid flows using adjoint parameters and Lagrange remainder"

Transcription

1 A posriori poiwis rror simaio for comprssibl fluid flows usig adjoi paramrs ad Lagrag rmaidr Sor il: A posriori poiwis rror simaio usig adjoi paramrs A.K. Alsv a ad I. M. avo b a Dparm of Arodamics ad Ha Trasfr RSC EERGIA Korolv Moscow Rgio 47 Russia Fdraio b Dparm of Mamaics ad C.S.I.T. Florida Sa ivrsi Tallaass FL 6-4 SA SMMAR T poiwis rror of a fii-diffrc calculaio of suprsoic flow is discussd. T local rucaio rror is drmid b a Talor sris wi rmaidr big i a Lagrag form. T coribuio of local rucaio rror o oal poiwis approimaio rror is simad via adjoi paramrs. I is dmosrad b umrical ss a rsuls of umrical calculaio of gasdamics paramr a a obsrvaio poi ma b rfid ad a rror boud ma b simad. T rsuls of umrical ss for cas of parabolizd avir- Sos PS ar prsd as a illusraio of proposd mod. Kwords: adjoi problm a posriori rror simaio parabolizd avir-sos. ITRODCTIO A prs Ricardso rapolaio [ ad ] is mos popular mod for simaio of discrizaio rror i CFD. forual a corrc us of Ricardso rapolaio rquirs a s of grids o prov moooous covrgc ad o drmi ral ordr of covrgc for cosidrd soluio. Tis ma ur ou o b vr psiv from viwpoi of compur rsourcs. T raso for is siuaio is isc of ma ffcs a ma cag omial ordr of grid covrgc. T simpls ampl is covrgc ordr rducio i prsc of socs. For scms of ird ad four accurac ordr rducio of covrgc ra was dmosrad i [4] for comprssio wav. T wors of [5-7] cofirm is ffc. Spaial ouiformi of grid ma also rduc covrgc ra [8]. A alraiv approac for a posriori rror simaio as isivl b dvlopd for las dcad Rfs. [9-5]. I is usd for simaio of rror of som quaiis of irs goal fucioals poi-wis paramrs c usig rsidual rucaio rror ad adjoi dual quaios. I Rf. [8] is approac is usd for wav quaios i Rf [] i is usd for raspor quaio. I Rfs. [-5] a posriori rror simaio is obaid for avir-sos ad Eulr quaios. I s wors Galri mod is usd for local rror simaio wil adjoi quaios ar usd for calculaig ir wigs i arg fucioal rror. A similar approac was usd i [6-7] for rfim of pracicall usful fucioals bo b fii-lm ad fii-diffrc mods. T local rucaio rror rsidual was simad roug acio of diffrial opraor o irpolad soluio wil is coribuio o fucioal was calculad usig a adjoi problm. T rror is dmosrad o b composd of wo compos firs big compuabl usig adjoi paramrs ad rsidual wil scod big icompuabl dpdig o rrors of soluio of bo primal ad adjoi problms. I [6-8] iformaio o spaial disribuio of rsiduals was usd for

2 ms rfiig for dimiisig icompuabl rror abov simaio of compuabl rror. A surv of a posriori rror simaio usig adjoi quaios ma b foud i [4]. I prs wor w cosidr aor approac for simaio of compuabl rror if compard wi [6-7]. I is basd o a diffrial approimaio DA [8] isad of o rsidual simaio ad is mor aural for fii-diffrcs. Tis provids crai pculiariis bo i applicabili domai ad faurs of mods. W us a local rucaio rror drmid b a Talor sris wi rmaidr i Lagrag form ad adjoi quaios i a coiuous form. Tis abls us o corrc rror ad o obai a asmpoic rror boud for rfid soluio. T rfim ad rror boud ar obaid o sam grid as a mplod for primal problm soluio ad rquir idical compur im. Tis approac was usd for a rasfr quaio i [7 47]. Hri w cosidr a applicaio of approac o a fii-diffrc approimaio of parabolizd avir-sos ad Eulr quaios. For illusraig mai ida w us quaio ad is fiidiffrc approimaio ; l soluio b smoo oug o possss all cssar drivaivs o b boudd. L us us Talor sris wi rmaidr i Lagrag form paramrs ar uow. α β α β Tus a fii-diffrc quaio is quival o a approimad quaio wi a addiioal prurbaio rm. Mamaical dails of is quivalc ma b foud i [ 8]. L us fid rror of fucioal as a fucio of rucaio rror. For is purpos l us iroduc Lagragia dd s s Ω δ δ ε dd L ψ ε Ω. I ma b sow from is Lagragia variaio a for soluios of dirc ad adjoi s s δ δ ψ ψ problms variaio of fucioal causd b rucaio rror compo from drivaiv quals dd ψ α δ ε Ω Is discr form i ma b rcas o assum form ψ α δ ε 4 sig a Talor pasio prssio 4 ma b wri as ψ α δ ε 5 T firs par of sum 5 ma b usd for rfiig fucioal; rror is causd b scod par du o uow paramrs. Ts paramrs blog o ui irval so w ma obai a boud of is prssio α α

3 α ψ ψ sig suc simas for bo coordias w ca drmi a boud of fucioal rror afr rfim corr corr sup sup < 7 ac Tis approac also provids a sima of igr ordr rms i 4. For ampl a sima of scod ordr ovr α as form 4 α 4 ψ 4 < ψ For a scod ordr sima w obai sup sup < 4 4 sup corr 9 ac For a ifiil smoo soluio w ma wri corr corr s sris covrg du o ac < s sup s s sup s sup. If all drivaivs ar boudd s s s α ψ C s <. vrlss is dos s!! s o guara simaio o b small oug o b of a pracical sigificac. W sould us umrical prssios for ig ordr drivaivs i abov formulaios. If umrical soluio as oscillaios s simas ma b oo larg ad b of o pracical us. So cosidrd approac ma b usd ol for fii diffrc scms wic ar moooous oug. Eprssio 7 is corrc for ac valus of adjoi paramr. I rali adjoi problm is solvd b som fii-diffrc mod so i coais som approimaio rror ψ ψ ac ψ. Hc simaio of fucioal variaio as a compo drmid b adjoi problm rror. ε δ ψ dd Ω Tis rm corrspods o rmaiig rror accordig o [9] ad is associad o rrors of approimaio of bo adjoi ad primal quaios. Wors [6-8] cocr a cosrucio of a ms for miimizaio of is rm. As a alraiv w ma us scod ordr adjoi quaios [4 44 ad 47] for calculaig is rm. If primal ad adjoi problms ar p solvd b mods of ordr O ad a p a O is rm is of O ordr. For scms of ig oug ordr p or a is rm is asmpoicall small if compard wi rror bouds drmid b 6.. THE ESTIMATE OF APPROIMATIO ERROR FOR FIITE-DIFFERECE CALCLATIO OF A FLOW PARAMETER Cosidr discussd mod of approimaio rror for simaig wo dimsioal suprsoic viscous flow Fig.. T odivrg form of parabolizd avir-sos quaios PS is usd. T flow is calculad b marc alog ais. 6 8

4 4 R P R 4 P R 4 Pr R κ 4 P RT; RT C T v ; Ω<< ma ; << ma ; O iflow boudar A Fig. w av: ; ; ; ; O laral boudaris B D ma codiios f/ ar imposd. f i T dsi a som poi is cosidrd as a simad paramr. L us wri simad valu i form of a fucioal. s s dd s s s Ω δ δ ε 5 W d o calcula gradi of arg fucioal wi rspc o local disurbacs rucaio rror. I is ow a mos ffici wa for gradi calculaio is basd o usig adjoi quaios [6]. Ts quaios ma b obaid i a sadard wa b uifig i a sigl Lagragia simad fucioal ad wa formulaio of flow damics problm. Hri w prs rsul. Addiioal dails ma b foud i [9 4]. i δ f. ADJOIT PROBLEM / / P P R 4 R R 4 RPr s s δ δ 6 T sourc i 6 corrspods o locaio of simad paramr. P R 8 R 7

5 5 P 4 R 8 9 R Pr Paramrs ar adjoi aalogs of dsi vloci compos ad rg. ma Iiial codiios C ma : ; boudar Eprssio for ma. corrspods o locaio of a simad paramr o f Boudar codiios o BD ; ma : ; Adjoi problm is calculad i rvrs dircio alog. For poi-wis rror simaio quaios av sigular sourcs Dirac s dla fucios Equaio 6. forual rgulari bo of parabolizd avir-sos ad corrspodig adjoi ssm ar uow. Bo s ssms of quaios ar of mid prbolic-parabolic aur. Accordig o [48] a rasfr parabolic problm wi similar sourc is wll-posd for α H Ω α Ω R. From is aalog cosidrd problm ma b wllposd i H Ω > a fac a gdrs corrspodig compuaioal difficulis. Howvr if β w smoo sourc rm accordig o [4546] w ma obai a soluio s H Ω β > aloug coaiig a rror proporioal o smooig paramr s s > wic ma b as small as cssar. Mods of fii diffrc soluio for suc quaios ar also prsd i [4546]. T arg fucioal variaio as a fucio of rucaio rror as followig form: δε δ δ δ δ dd Ω I ss prsd blow w compar rsuls of fii-diffrc calculaios wi aalical soluios corrspodig o iviscid gas flows. I is co ifluc of viscous rms i quaios -4 o a simad paramr is of irs. W cosidr soluio of quaios wiou viscosi as a o-prurbd o. L viscous rms disurb is soluio. For ampl for logiudial vloci udisurbd valus ar govrd b quaio wil disurbd os ar govrd b. T variaio of arg fucioal R du o viscous rms assums form δε... d Ω R Ω

6 6 I coras o 6-9 corrspodig adjoi quaios av o viscous rms. Crail is approac is valid ol w ifluc of viscous rms is small oug i.. w do o caus a radical cag of flow srucur. Aor raso for dvlopm of is ciqu ariss for discoiuiis a ar pical of suprsoic flows dscribd b Eulr quaios for ampl. T approac basd o diffrial approimaio is o applicabl for suprsoic Eulr quaios du o uboud drivaivs. vrlss w ma us parabolizd avir-sos for basic flow calculaio cosidr viscous rms as a prurbaio ad calcula ffc of is prurbaio o soluio. Tis ma abl us o pad applicabili of diffrial approimaio approac o discoiuous flows dscribd b Eulr quaios. 4. FIITE DIFFERECE SCHEME To sud approimaio rror ri w d a fii diffrc scm avig largs rucaio rror. As a cosquc w us a firs ordr scm covciv rms big obaid b upwid diffrcs [4]. vrlss svral rms ar approimad b smmrical diffrcs wi rsul a av scod ordr. A fii-diffrc scm for opio is prsd blow. I coais wo sps prdicor ad corrcor. Bo sps ar calculad implicil usig r poi Tomas algorim. T ild mars paramrs compud a firs sp. > Prdicor 4 R P P. 5 R 4 P P. 6 RPr Φ 7 Corrcor. 8 R P P. 9 R 4 P P. RPr Φ T fii diffrc scm as a similar form for adjoi ssm. T mai faur is prsc of sourc rm i 6 wic is rlad o locaio of simad poi. For fi oug grids a mollificaio smoo approimaio of s s δ δ δ -fucio ma b cssar for approimaio of is sourc rm []. T mods of fii diffrc soluio of quaios wi suc sourcs ar prsd i [4546].

7 7 5. ESTIMATIO OF THE TRCATIO ERROR T oal approimaio rror dpds o a local rucaio rror. I ordr o drmi i w pad fii diffrcs i Talor sris wi Lagrag rmaidr. For illusraio l us prs is simaio for o of fii-diffrc rms i 9. α T corrspodig compo of arg fucioal variaio s assums form: dd Ω α δ ε Is discr form is α δ ε. For a firs ordr ovr i ma b prsd as α α δ ε 4 T firs par of is sum ma b usd for rfiig of fucioal corr 5 olimiad rror is gdrd b scod par of 4. I as a uppr boud: sup α 6 Toal rfim of fucioal drmid b all firs ordr rms of fii-diffrc scm 8- follows: corr 7

8 8 Toal prssio for rror boud causd b firs ordr rms of 8- as form: sup 8 Similar prssios ar obaid for covciv rms of scod ordr accurac ad for viscous rms. A boud of rfid fucioal rror ma b drmid b s prssios as: sup < ac corr 9 Tis boud dos o accou for icompuabl rror prssios similar o or rrors causd b boudar codiio approimaio c. I also uss drivaivs wos bouddss ca o b prov a prs. So i rquirs a cofirmaio via umrical ss. 6. MERICAL TESTS 6.. COTIOS FLOW FIELD A compariso bw compuaios b fii-diffrcs ad aalic prssios ad a aalsis of rror simas is prformd for Pradl-Mar flow. T rror of flow dsi pas pasio fa was addrssd frsram Mac umbr M4 agl of flow roaio α. L us drmi approimaio rror usig adjoi approac ad compar i wi dviaio of fii-diffrc soluio from aalic o. Fig. prss dsi isolis i flow-fild Fig. illusras adjoi dsi isolis a cocraio of isolis corrspods o a poi of simaio. Fig. 4 prss spaial disribuio of dsi of rror boud 8 ad Fig. 5 dpics isolis of dsi of rror causd b viscous rms. Figs. 4 ad 5 drmi os spaial rgios a gra mai par of rror for paramr a simad poi. Rsuls prsd i Figs. -5 corrspod o calculaios aig io accou viscosi PS R. Fig. 6 prss rlaiv rror of flow dsi calculaio for R as a fucio of rciprocal of spaial sp i dircio umbr of ods. T par of rror causd b

9 9 corr visc ac viscous rms rlaiv dviaio of rfid soluio from aalical o ad boud of rfid soluio rror 6 ar prsd. I ca b s a mai par of rror is drmid b viscosi ad i ma b compud ad limiad. T rfid rsul is clos o aalical o ad is locad wii irval of rror boud. vrlss r is o covrgc of rror boud as pcd from prssio 6. L us cosidr rlad rsuls for iviscid flow. Fig. 7 prss dviaio of fiidiffrc soluio from aalic o ad corrcio of rror i accordac wi 5. T rfim of soluio usig adjoi paramrs accordig 5 abls limiaio of major par of discrizaio rror. T firs ordr of compuabl rror 5 ma b dcd if aalz Fig. 7. Calculaios dmosrad a good coicidc of rfid soluio wi aalical o ad rliabili of rror boud sima Fig. 8. vrlss pcabl scod ordr of accurac 6 dos o maifs islf. W ms is fi oug rror boud pracicall dos o dpd o sp siz. Tis is causd b grow of ird drivaivs of flow paramrs as sp siz dcrass. I ma b du o formaio of wa discoiuiis i flowfild. A compariso of Figurs 6 ad 8 dmosras a impac of viscosi ffc usig adjoi quaios abls us o obai rsul clos o iviscid compuaio as far as accurac is cocrd. Tus r is fasibili for calculaio of iviscid flow Eulr quaios ad a posriori rror simaio o basis of PS. Tis ds applicabili of cosidrd mod wic is o dircl applicabl o suprsoic Eulr quaios du o isc of discoiuous soluios. Fig. 9 prss dpdc of rror of rfid soluio i compariso wi iiial rror of soluio causd bo b viscous rms ad b approimaio rror as a fucio of R umbr. As viscosi dcrass a crai icras of rror boud sima is visibl du o grow of ird drivaivs of gasdamical paramrs. For small oug R umbrs rror of fii-diffrc calculaio bras rror boud a is causd b sigifica disorio of flow par compar Fig. R ad Fig. R. I gral for a smoo flow rrors bo for iviscid flow ad for viscous flow rfid via adjoi paramrs ar clos. 6.. DISCOTIOS FLOW FIELD o As aor s rror of dsi pas crossig socs α ±. M4 R is calculad. Fig. prss dsi isolis wii flowfild Fig. illusras isolis of adjoi dsi Fig. sows dsi of rror boud accordig 8 ad Fig. 4 prss isolis of rror causd b viscous rms. Tis s is mor complicad du o uboudd drivaivs of gasdamics paramrs for iviscid flow. T prsc of viscosi abls us o calcula flows wi socs wil a sam im i iroducs a rror proporioal o /R. W viscosi dcrass is rror dimiiss oo uforual rror rlad o uboudd drivaivs icrass simulaousl. Fig. 5 prss rsuls for R as a fucio of spaial sp siz. T viscous compo of rror is small oug dviaio of fii-diffrc soluio from aalical o is small also ad wal dpds o sp siz ad is ffc ma b aribud o ucorolld rrors o-divrgc of scm possibl. Fig. 6 prss rsuls for iviscid flow as a fucio of spaial sp siz. Bo rror ad rror boud av a ordr of covrgc ovr grid siz of O. Fig. 7 sows dpdc of rror o Rolds umbr. As viscosi dcrass rror ad rror boud icras ad approac asmpo a iviscid limi.

10 A aural wa o limia rrors cocd wi a odivrg scm is coic of divrg o. T followig ssms of divrg Eulr quaios wo-dimsioal ad rlad adjoi quaios wr usd i umrical ss. i Pδ Divrg Eulr quaios: ; 4 i ; 4 4 ; Hr P is alp / is i oal alp. Adjoi quaios: i i / ; 4 i i i ; 44 ; 45 Svral varias of firs ordr fii-diffrc scms wo dimsioal wr usd icludig "door clls" [4] ad a scm of Coura-Isaacso-Rs [4]. As pcd dviaio of fii-diffrc soluio from aalic o for divrg scm is sigifical smallr compard wi odivrg o. forual rror simas us drivaivs a ar uboudd i divrg cas also cludig o-dimsioal flow. T rsuls of s compuaios ar aalogous o rsuls obaid usig odivrg scm. W ma compar grid covrgc for odivrg scm Fig. 6 wi rsuls for divrg o Fig. 8 iviscid flow. If w iroduc viscosi w ca obai covrg simas of rror for divrg scm oo Fig. 9. T abov ss ar orid owards compariso wi aalical soluios a blog o iviscid flows. Tis cras som spcifics. For ampl prvious s flowfild is composd of rgios of cosa gasdamical paramrs sparad b socs. So i is o bs problm from rror simas viwpoi usig drivaivs of gasdamical paramrs. Tus i is pdi o cosidr a s problm mor pical of viscous gas flows. L us cosidr a viscous R suprsoic wal udrpadd / j i suprsoic flow. Fig. prss isolis of dsi i flowfild Fig. prss isolis of adjoi dsi ad Fig. prss spaial dsi of rror boud sima 8. forual corrspodig aalical soluios for is problm ar uow. Hc soluio o fis ms was rgardd as a ac o. Fig. prss rror boud ad dviaio of soluio from ac o i dpdc o grid sp. T covrgc ordr for rror boud is clos o o sligl blow ad dcrass as ms is rfid. Tis rsul ma b a idirc vidc of prsc of discoiuiis i drivaivs of gasdamical paramrs. p j p

11 7. THE EALATIO OF COMPTABLE ERROR SIG RESIDAL T rsidual basd approac closl rlad o [9] is usd ri for a simaio of compuabl rror wiou plici us of diffrial approimaio. T mai diffrc bw is approac ad a of [9] is i rsidual calculaio. W do o us a irpolaio of flow paramrs from grid pois o oal domai. Isad w us a igr ordr scm o sam umrical soluio. L us cosidr is approac a a urisic lvl. Assum w av a flow-fild compud via crai fii-diffrc mod. W r o sima rror of is calculaio. L us us quaio as a ampl. L flowfild b calculad via firs ordr fii-diffrc approimaio ; 46 T diffrial approimaio of 44 ma b wri as δ. L us wri i i mor dail usig a Talor sris wi rmaidr i a Lagrag form. paramrs ar uow. α β 6 6 α β 47 L us rplac 46 b scil of scod ordr of accurac ad calcula rsidual arisig from applig ig ordr scm o flowfild calculad usig low ordr scm. η η 48 Eprssio 48 ma b padd i Talor sris as 6 6 χ η 49 T fucio is obaid from soluio of 46 ad so complis wi codiio 47. L us subsiu 47 i 49 rsidual assums form 6 6 χ η 6 6 α β 5 Corrspodigl lowr ordr rm of rucaio rror 47 as a form 6 6 β η η α χ Tus lowr rm of diffrial approimaio 47 ma b simad via a rsidual obaid from usig ig ordr scil o soluio calculad usig mai fii-diffrc

12 scm. As a rsul w obai fild of rsiduals a locall disurb ac soluio. Accordig o variaio of simad valu as a form ε δ δψ dd. Taig io accou 5 w obai ε δ δψ dd ηψ dd 5 Ω I coras o prssio 5 ma b asil calculad wiou owldg of diffrial approimaio. O or ad diffrial approimaio approac provids a mor accura accou of igr rms ad simaio of rfid soluio bouds. L us compar s approacs usig firs ordr upwid scm ad divrg form of Eulr quaios 8-4. For simaio of rsidual w us scod ordr approimaio 48. T dviaio of calculaio from aalical rror simaio usig DA basd 5 ad rsidual basd mods ar prsd i Fig. 4 for Pradl-Mar flow. T clos corrlaio of simas 5 ad 5 for coiuous flow is visibl. If w rcas Fig. 4 o a logarim scal all s fucios ma b dscribd b a firs ordr curv O. I coras o prssio 5 ma b dd o discoiuous flows if divrg fii diffrc scms ar usd. For discoiuous flow bo drivaivs i 48 ar uboud vrlss s sigulariis ar muuall compsad du o cosrvaio law ad rsidual is boudd. Tis rsidual ma b calculad usig ol a boudd combiaio of drivaivs of flow paramrs ad applid for rror simaio. A corrspodig ampl is prsd i Fig. 5 for crossig socs. I prss rror simaio usig a rsidual basd mod 5 DA basd 5 o ad dviaio of calculaio from aalical valu. Fig. 5 dmosras rsidual approac 5 o provid a muc mor accura simaio of rror if compard wi diffrial approimaio 5 wic plicil divrgs. forual rsidual basd approac dos o provid a rror boud. Ω Ω η 8. DISCSSIO T difficulis cocd wi usig adjoi approac ar of sam aur as os arisig wil usig Ricardso rapolaio. T ar causd b prsc of discoiuiis a drmi ordr of accurac obsrvabl i umrical ss. L us cosidr is problm a a urisic lvl. For is purpos l us wri 5 i mor dail. L m b umbr of boudd drivaivs drivaivs of ordr m ad igr ma av a fii umbr of jump discoiuiis p is ordr of approimad drivaiv j is formal ordr of accurac D of a fii-diffrc scm. L us approima drivaivs b fii diffrcs. D p j j D T limi lim corrspods o firs rm 5. Cosidr is p j Ω D m m asmpoic form. T drivaiv of ordr m as a asmpoic / / for jump discoiui wil drivaiv of ordr m as asmpoic / / / / corrspodigl drivaiv of ordr p j as p j j D j asmpoic. Tus lim p jm lim. Tr is a limid p j p jm D umbr of ods a paricipa i summaio i vicii of discoiui so muliplir apparig durig summaio sould b a io accou ildig

13 r s p j j D m p. p j D r s Tus rms of j- formal ordr of accurac coai a compo of j- ordr apparig du o igraio ovr smoo par of soluio ad a compo avig ordr i m p gdrd b jump discoiui of m ordr drivaiv. So ordr of covrgc dpds o soluio ad ma asmpoicall d o a miimal ordr i m p as grid siz dcrass. I [47] ifluc of discoiuiis o rror is cosidrd for ampl a of spaial drivaiv of mpraur. T calculaio of approimaio rrors b cosidrd mod rquirs isc of boudd drivaivs of rlaivl ig ordr. T do o is alwas so for suprsoic Eulr quaios s simas ma b calculad ol for smoo soluios. If discoiuiis ar pcd for sudid flow us of viscosi abls us o coduc s simas. T viscosi gdrs is ow compo of rror wic ma also b limiad usig adjoi quaios. Tis approac prmis o obai rror simas for iviscid suprsoic flows usig is mod. aurall w ca sima o ol rror of dsi wri as a fucioal 5 bu rror of or fucioals. T diffrcs ar ol i form of sourc rms i adjoi quaios 6-9. For jusificaio of rror simas w sould vrif a uaccoud rror compo iducd b approimaio rror of adjoi quaios is small oug. For calculaio of is compo w ca solv scod ordr adjoi quaios[4]. Suc a suiabl ampl is prsd i [47] for a coducio quaio. For rror simas w us umrical rsuls a ma b sigifical lss smoo compud psical fild. Tus for crai fii-diffrc scms o-moooic rror bouds ma b oo larg. T applicabili of mod cosidrd abov is rsricd o umrical scms wic do o ibi opsical oscillaios. 9. COCLSIO T compuabl poiwis rror of viscous flow paramr causd b a fii-diffrc approimaio ma b valuad usig diffrial approimaio rms ad adjoi quaios. T asmpoic boud of rfid soluio rror ma b drmid simulaousl. umrical ss carrid ou dmosrad fficic of is mod for parabolizd avir-sos. T ifluc of viscous rms ma b calculad similarl ad a provids also for fasibili of simaig rrors of Eulr quaios. T compur im rquird for poi-wis rfiig of a sigl paramr a a sigl poi ad rror boud calculaio is qual o im rquird for flow-fild calculaio o sam grid. APPEDI A. OMECLATRE C v - spcific volum a capaci; - spcific rg C v T f - flow paramrs -alp -oal alp - spaial sps alog ad ; M - Mac umbr -umbr of im sps umbr of spaial ods alog umbr of spaial ods alog L- Lagragia P -prssur PR - Pradl umbr PrµC v /λ R - gas cosa

14 4 R µ ma -Rolds umbr T-mpraur - vloci compo alog - vloci compo alog coordias Gr lrs α β - cofficis i Talor-Lagrag sris δ -Dirac s dla fucio; corr sup - corrcabl rror cocd wi pasio alog ; - corrcabl rror; - corr compo of boud of ir rror cocd wi pasio i coordia ; - compo of boud of ir rror - spcific a raio ε - fucioal; µ -viscosi λ - rmal coducivi; - dsi; -mporal sp - adjoi variabls Ω- domai of calculaio Subscrips: rac boudar paramrs; a- aalical soluio; corr- corrcd rror; s simad poi; ac- ac soluio; - umbr of spaial ms od alog ; -umbr of sp alog ; sup- boud of ir rror; -compo of rucaio rror cocd wi Talor pasio i coordia ; - compo of rucaio rror cocd wi Talor pasio i im. sup

15 5 REFERECES. Marcu GI ad Saidurov. Diffrc mods ad ir rapolaios. Sprigr: Roac P. J. Quaificaio of crai i Compuaioal Fluid Damics. Aual Rviw of Fluid Mcaics 997; 9: 6.. Ro C. J. Grid Covrgc Error Aalsis for Mid-Ordr umrical Scms. AIAA Joural ; 44: Carpr M. H. ad Caspr J.H. Accurac of Soc Capurig i Two spaial Dimsios. AIAA J. 999; 79: Efraimsso G. ad Kriss G. A Rmar o umrical rrors Dowsram of Sligl iscous Socs. SIAM J. of umrical Aalsis 999; 6: Egquis B. ad Sjogr B. T Covrgc Ra of fii Diffrc Scms i Prsc of Socs. SIAM Joural of umric l Aalsis 998; 5: Ro C. J. McWrr-Pa M.A. ad Obrampf W. L. rificaio ad alidaio for Lamiar Hprsoic Flowfilds. AIAA Joural ; 4 : amalv. K. ad Carpr M. H. O Accurac of Adapiv Grid Mods for Capurd Socs. ASA/TM--45: Aiswor M. ad Od J. T. A Posriori Error Esimaio i Fii Elm Aalsis. Wil Irscic:.. Od J.T. ad Prudomm S. Goal-Orid Error Esimaio ad Adapivi for Fii Elm Mod. Compurs&Mamaics wi Applic. ; 4: Od J.T. ad Prudomm S. Esimaio of modlig rror i compuaioal mcaics. Joural of Compuaioal Psics ; 8: Od J.T. ad Prudomm S. O goal-orid rror simaio for llipic problms: Applicaio o corol of poiwis rrors. Compur Mods i Applid Mcaics ad Egirig 999; 76: -.. Joso C. O Compuabili ad Error Corol i CFD. Iraioal J. for umrical Mods i Fluids 995; : Hoffma J. ad Joso C. Compuabili ad adapivi i CFD. o appar i Ecclopdia of Compuaioal Mcaics 5. Harma R. ad Houso P. Goal-Orid A Posriori Error Esimaio for Comprssibl Fluid Flows. I umrical Mamaics ad Advacd Applicaios Brzzi F. Buffa A. Corsaro S. ad Murli A. ds Sprigr-rlag: ; pp dii D. ad Darmofal D. Adjoi rror simaio ad grid adapaio for fucioal oupus: Applicaio o quasi-o-dimsioal flow. J. Compu. Ps. ; 64: dii D. ad Darmofal D. Grid Adapaio for Fucioal Oupus: Applicaio o Two- Dimsioal Iviscid Flow. J. Compu. Ps. ; 76: D. Darmofal ad D. dii. Aisoropic grid adapaio for fucioal oupus: applicaio o wo-dimsioal viscous flows. J. Compu. Ps. ; 87: Gils M. B. O adjoi quaios for rror aalsis ad opimal grid adapaio i CFD. I Compuig Fuur II: Advacs ad Prospcs i Compuaioal Arodamics. Hafz M. ad Caug D. A. ds Wil: w or: 998; pp Pirc. A. ad Gils M. B. Adjoi rcovr of suprcovrg fucioals from PDE approimaios. SIAM Rv. ; 4: Gils M. ad Pirc.A. Improvd Lif ad Drag Esimas sig Adjoi Eulr Equaios". Tcical Rpor 99-9 AIAA Ro 999: -.. Par M. A. Tr Dimsioal Turbul RAS Adjoi Basd Error Corrcio AIAA Papr -849: -4.. Par M. A. Adjoi Basd Tr Dimsioal Error Prdicio ad Grid Adapaio. AIAA Papr 86 : Gils M. B. Ad Suli E. Adjoi mods for PDEs: a posriori rror aalsis ad posprocssig b duali. Aca umrica ; M.B. Gils.A. Pirc ad E. Suli. Progrss i adjoi rror corrcio for igral fucioals Compuig ad isualizaio i Scic 4; 6: A. Pirc ad M.B. Gils. Adjoi ad Dfc Error Boudig ad Corrcio for Fucioal Esimas o appar i Joural of Compuaioal Psics 4

16 6 7..A. Pirc ad M.B. Gils. Adjoi ad dfc rror boudig ad corrcio for fucioal simas AIAA Papr ; W. Bagr R. Raacr Fii Elm Approimaio of Acousic Wav Equaio: Error Corol ad Ms Rfim Eas-Ws J. of umr. Ma. 996; 7/4: R. Bcr R. Raacr A opimal corol approac o a posriori rror simaio i fii lm mods. I A. Isrls dior Aca umrica Cambridg iv. Prss ;-.. Huvli R. Raacr Duali-basd adapivi i p-fii lm mod J. umr. Ma. ; o. 8. P. Houso R. Raacr ad E. Suli. A posriori rror aalsis for sabilizd fii lm approimaios of raspor problms. Compu. Mods Appl. Mc. Egrg. ; 9 - : P. Mo ad E. Suli. T adapiv compuaio of far fild pars b a posriori rror simas of liar fucioals. SIAM J. umr. Aal. 998; 6: E. Suli P. Houso Adjoi rror corrcio for igral oupus i: Adapiv Fii Elm Approimaio of Hprbolic Problms Sprigr 4. E. Suli ad P. Houso. Fii lm mods for prbolic problms: a posriori rror aalsis ad adapivi. I: I. Duff ad G.A. Waso ds. T Sa of Ar i umrical Aalsis. Oford ivrsi Prss 997; E. Suli. A posriori rror aalsis ad adapivi for fii lm approimaios of prbolic problms. I: D. Krur M. Olbrgr ad C Rod Eds. A Iroducio o Rc Dvlopms i Tor ad umrics for Cosrvaio Laws. Lcur os i Compuaioal Scic ad Egirig. olum 5. Sprigr-rlag 998; Marcu G. I. Adjoi Equaios ad Aalsis of Compl Ssms. Kluwr Acadmic Publisrs: Dordrc Hardboud A.K.Alsv Corol of a Error of a Fii-Diffrc Soluio of Ha-Coducio Equaio b Cojuga Equaio Joural of Egirig Psics ad Trmopsics. 4; 77 iss Soi u.i. Mod of diffrial approimaio. Sprigr-rlag Alsv A.K. D Ivrs Covcio Domiad problm for Esimaio of Iflow Paramrs from Ouflow Masurms. Ivrs Problms i Eg. ; 8: Alsv A.K. ad avo I.M. Calculaio of crai Propagaio usig Adjoi Equaios. Iraioal Joural of Compuaioal Fluid Damics ; 7 4: Roac P. Compuaioal Fluid damics. Hrmosa publisr Kuliovsii A.G. Pogorlov.. ad Smov A.u. Mamaical Aspcs of umrical Soluio of Hprbolic Ssms. Moograps ad Survs i Pur ad Applid Mamaics 88 Capma&Hall/CRC: Boca Rao Fl. 4. Wag Zi avo I. M. L Dim F.. ad Zou.. T Scod Ordr Adjoi Aalsis: Tor ad Applicaios. Morol. Amos. Ps. 99; 5: Alsv A. ad avo M. O Esimaio of Tmpraur crai sig Scod Ordr Adjoi Problm. I. Joural of Compu. Fluid Damics ; 6 : A.K. Torbrg ad B. Egquis. Rgularizaio ciqus for umrical approimaio of PDEs wi sigulariis. J. of Sci. Compu. ; 9: J.Wald. O approimaio of sigular sourc rms i diffrial quaios. umr. M. Par. D 5 999; A.K. Alsv ad I. M. avo O a-posriori poiwis rror simaio usig adjoi mpraur ad Lagrag rmaidr Compur Mods i Appl. Mc. ad Eg. 4 accpd 48. J.L. Lios Poiwis Corol of Disribud Ssms i H.T. Bas d. Corol ad simaio i disribud Paramr ssms. Froirs i applid mamaics v. SIAM 99-9 Figur Capios Fig.. Flow sc. A- Erac boudar BD- laral boudaris *-locaio of simad paramr Fig.. Isolis of dsi Pradl-Mar flow

17 7 Fig.. Isolis of adjoi dsi cocraio corrlas wi simad poi Fig. 4. Isolis of dsi of rror boud 8 Fig. 5. Isolis of rror dsi causd b viscosi. Fig. 6. T rror of calculaio as a fucio of rciprocal of ms sp viscous flow R. -rror du o viscous rms -dviaio of rfid soluio from aalical o ad 4- bouds of rror Fig. 7. T rror of calculaio as a fucio of rciprocal of ms sp iviscid flow. -dviaio of fii-diffrc soluio from aalical o rror corrcio accordig 7. Fig. 8. T rror of calculaio as a fucio of rciprocal of ms sp iviscid flow. -dviaio of rfid soluio from aalical o rror bouds 8 Fig. 9. T rror of calculaio as a fucio of Rolds umbr. - dviaio of fiidiffrc soluio from aalical o - rror du o viscous rms - dviaio of rfid soluio from aalical o 4 5 rror bouds 8 Fig.. Isolis of dsi for small R R Fig.. Isolis of dsi crossig socs Fig.. Isolis of adjoi dsi cocraio corrlas wi simad poi Fig.. Isolis of rror boud dsi 8 Fig. 4. Isolis of rror dsi causd b viscosi. Fig. 5. T rror of calculaio as a fucio of rciprocal of ms sp viscous flow. - dviaio of rfid soluio from aalical o - rror dsi causd b viscosi 4 rror bouds 8 Fig. 6. T rror of calculaio i dpdc o rciprocal of ms sp iviscid flow. - dviaio of rfid soluio from aalical o rror bouds 8. Fig. 7. T rror of calculaio as a fucio of Rolds umbr. - dviaio of fiidiffrc soluio from aalical o - rror causd b viscosi. - rror boud 8 Fig. 8. T rror of calculaio as a fucio of rciprocal of ms sp iviscid flow divrg scm. -dviaio of fii-diffrc soluio from aalical o - corrcio 7 - boud of rror Fig. 9. T rror of calculaio as a fucio of rciprocal of ms sp viscous flow divrg scm. - dviaio of rfid soluio from aalical o rror bouds 8 Fig.. Isolis of dsi Fig.. Isolis of adjoi dsi Fig.. T dsi of rror boud 8. Fig.. T rror of calculaio as a fucio of rciprocal of ms sp. - dviaio of rfid soluio from ac o - boud of rror. Fig. 4. T compariso of diffr rror valuaios as a fucio of rciprocal of ms sp. - DA basd rror - rsidual basd rror 5 diffrc of aalical ad umrical valus. Fig. 5. T rrors as fucios of rciprocal of ms sp. - diffrc of aalical ad umrical valus - DA basd rror - rsidual basd rror 5.

18 8 B A f C D * s Fig.. Flow sc. A- Erac boudar BD- laral boudaris *-locaio of simad paramr D Ja 4 d Dirc D Ja 4 d Adjoi Fig.. Isolis of dsi Pradl-Mar flow 5 5 Fig.. Isolis of adjoi dsi cocraio corrlas wi simad poi D Ja 4 d Gridg D Ja 4 d Gridg Fig. 4. Isolis of dsi of rror boud Fig. 5. Isolis of rror dsi causd b

19 9 viscosi.e- 5.E- dro/ro 4.E -5.E- -.E- -.5E Fig. 6. T rror of calculaio as a fucio of rciprocal of ms sp viscous flow R. - rror du o viscous rms -dviaio of rfid soluio from aalical o 4- bouds of rror - LogdRo Log Fig. 7. T rror of calculaio as a fucio of rciprocal of ms sp iviscid flow. -dviaio of fii-diffrc soluio from aalical o rror corrcio accordig 7.

20 8.E- 6.E- 4.E-.E- dro/ro.e -.E- -4.E- -6.E- -8.E Fig. 8. T rror of calculaio as a fucio of rciprocal of ms sp iviscid flow. -dviaio of rfid soluio from aalical o rror bouds 8 6.E- 4.E-.E- dro/ro 4 5.E -.E- -4.E- -6.E- LogR -8.E Fig. 9. T rror of calculaio as a fucio of Rolds umbr. - dviaio of fii-diffrc soluio from aalical o - rror du o viscous rms - dviaio of rfid soluio from aalical o 4 5 rror bouds 8

21 D Ja 4 d Dirc Fig.. Isolis of dsi for small R R D Ja 4 d Dirc D Ja 4 d Adjoi Fig.. Isolis of dsi crossig socs 5 5 Fig.. Isolis of adjoi dsi cocraio corrlas wi simad poi D Ja 4 d Gridg D Ja 4 d Gridg Fig.. Isolis of rror boud dsi Fig. 4. Isolis of rror dsi causd b

22 viscosi. 4.E-.E-.E-.E- dro/ro 4.E -.E- -.E- -.E- -4.E Fig. 5. T rror of calculaio as a fucio of rciprocal of ms sp viscous flow. - dviaio of rfid soluio from aalical o - rror dsi causd b viscosi 4 rror bouds 8 4.E-.5E- dro/ro.e-.5e-.e-.5e-.e- 5.E-.E Fig. 6. T rror of calculaio as a fucio of rciprocal of ms sp iviscid flow. - dviaio of rfid soluio from aalical o rror bouds 8.

23 .5E- dro/ro.e-.5e-.e-.5e-.e- 5.E-.E -5.E R Fig. 7. T rror of calculaio as a fucio of Rolds umbr. - dviaio of fii-diffrc soluio from aalical o - rror causd b viscosi. - rror boud dro/ro Fig. 8. T rror of calculaio as a fucio of rciprocal of ms sp iviscid flow divrg scm. -dviaio of fii-diffrc soluio from aalical o -corrcio 7 - boud of

24 4 rror..5 dro/ro Fig. 9. T rror of calculaio as a fucio of rciprocal of ms sp viscous flow divrg scm. - dviaio of rfid soluio from aalical o rror bouds 8 D Ja 4 d Dirc D Ja 4 d Adjoi Fig.. Isolis of dsi 5 5 Fig.. Isolis of adjoi dsi

25 5 D Ja 4 d Gridg Fig.. T dsi of rror boud 8..E- dro/ro.e- 8.E- 6.E- 4.E-.E-.E -.E Fig.. T rror of calculaio as a fucio of rciprocal of ms sp. - dviaio of rfid soluio from ac o - boud of rror.

26 6.E-.8E- dro/ro.6e-.4e-.e-.e- 8.E-4 6.E-4 4.E-4.E-4.E Fig. 4. A compariso of diffr rror valuaios as a fucio of rciprocal of ms sp. - DA basd rror - rsidual basd rror 5 diffrc of aalical ad umrical valus. 5.E-.E dro/ro -5.E- -.E- -.5E- -.E- -.5E- -.E Fig. 5. T rrors as fucios of rciprocal of ms sp. - diffrc of aalical ad umrical valus - DA basd rror - rsidual basd rror 5.

27 7

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

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

( 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

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

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

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

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

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

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

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

(1) f ( Ω) Keywords: adjoint problem, a posteriori error estimation, global norm of error.

(1) f ( Ω) Keywords: adjoint problem, a posteriori error estimation, global norm of error. O a poseriori esimaio of umerical global error orms usig adjoi equaio A.K. Aleseev a ad I. M. Navo b a Deparme of Aerodyamics ad Hea Trasfer, RSC ENERGIA, Korolev, Moscow Regio, 4070, Russia Federaio b

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

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

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

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

Chapter Taylor Theorem Revisited

Chapter Taylor Theorem Revisited Captr 0.07 Taylor Torm Rvisitd Atr radig tis captr, you sould b abl to. udrstad t basics o Taylor s torm,. writ trascdtal ad trigoomtric uctios as Taylor s polyomial,. us Taylor s torm to id t valus o

More information

Option 3. b) xe dx = and therefore the series is convergent. 12 a) Divergent b) Convergent Proof 15 For. p = 1 1so the series diverges.

Option 3. b) xe dx = and therefore the series is convergent. 12 a) Divergent b) Convergent Proof 15 For. p = 1 1so the series diverges. Optio Chaptr Ercis. Covrgs to Covrgs to Covrgs to Divrgs Covrgs to Covrgs to Divrgs 8 Divrgs Covrgs to Covrgs to Divrgs Covrgs to Covrgs to Covrgs to Covrgs to 8 Proof Covrgs to π l 8 l a b Divrgt π Divrgt

More information

Adomian Decomposition Method for Dispersion. Phenomena Arising in Longitudinal Dispersion of. Miscible Fluid Flow through Porous Media

Adomian Decomposition Method for Dispersion. Phenomena Arising in Longitudinal Dispersion of. Miscible Fluid Flow through Porous Media dv. Thor. ppl. Mch. Vol. 3 o. 5 - domia Dcomposiio Mhod for Disprsio Phoma risig i ogiudial Disprsio of Miscibl Fluid Flow hrough Porous Mdia Ramakaa Mhr ad M.N. Mha Dparm of Mahmaics S.V. Naioal 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

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

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

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

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

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

Variational Iteration Method for Solving Initial and Boundary Value Problems of Bratu-type

Variational Iteration Method for Solving Initial and Boundary Value Problems of Bratu-type Availabl a hp://pvamd/aam Appl Appl Mah ISSN: 9-9 Vol Iss J 8 pp 89 99 Prviosl Vol No Applicaios ad Applid Mahmaics: A Iraioal Joral AAM Variaioal Iraio Mhod for Solvig Iiial ad Bodar Val Problms of Bra-p

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

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

, 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

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

NAME: SOLUTIONS EEE 203 HW 1

NAME: SOLUTIONS EEE 203 HW 1 NAME: SOLUIONS EEE W Problm. Cosir sigal os grap is so blo. Sc folloig sigals: -, -, R, r R os rflcio opraio a os sif la opraio b. - - R - Problm. Dscrib folloig sigals i rms of lmar fcios,,r, a comp a.

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

y y y

y y y Esimaors Valus of α Valus of α PRE( i) s 0 0 00 0 09.469 5 49.686 8 5.89 MSE( 9)mi 6.98-0.8870 854.549 THE EFFIIET USE OF SUPPLEMETARY IFORMATIO I FIITE POPULATIO SAMPLIG Rajs Sig Dparm of Saisics, BHU,

More information

Analysis of TE (Transverse Electric) Modes of Symmetric Slab Waveguide

Analysis of TE (Transverse Electric) Modes of Symmetric Slab Waveguide Adv. Sudis Thor. Phs., Vol. 6,, o. 7, 33-336 Aalsis of T (Trasvrs lcric Mods of Smmric Slab Wavguid arr Rama SPCTC (Spcrum Tcholog Rsarch Group Dparm of lcrical, lcroic ad Ssms girig Naioal Uivrsi of Malasia

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

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

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

Log-periodogram regression with odd Fourier frequencies

Log-periodogram regression with odd Fourier frequencies Log-priodogram rgrssio wih odd Fourir frqucis Erhard Rschhofr Dparm of Saisics ad Opraios Rsarch, Uivrsiy of Via, Ausria Uivrsiässr. 5, Via, Ausria E-mail: rhard.rschhofr@uivi.ac.a Absrac I his papr, a

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

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

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

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

Control Systems. Transient and Steady State Response.

Control Systems. Transient and Steady State Response. Corol Sym Trai a Say Sa Ro chibum@oulch.ac.kr Ouli Tim Domai Aalyi orr ym Ui ro Ui ram ro Ui imul ro Chibum L -Soulch Corol Sym Tim Domai Aalyi Afr h mahmaical mol of h ym i obai, aalyi of ym rformac i.

More information

Numerical Solution of Parabolic Volterra Integro-Differential Equations via Backward-Euler Scheme

Numerical Solution of Parabolic Volterra Integro-Differential Equations via Backward-Euler Scheme America Joural of Compuaioal ad Applied Maemaics, (6): 77-8 DOI:.59/.acam.6. Numerical Soluio of Parabolic Volerra Iegro-Differeial Equaios via Bacward-Euler Sceme Ali Filiz Deparme of Maemaics, Ada Mederes

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

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

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

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

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

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

CS 688 Pattern Recognition. Linear Models for Classification

CS 688 Pattern Recognition. Linear Models for Classification //6 S 688 Pr Rcogiio Lir Modls for lssificio Ø Probbilisic griv modls Ø Probbilisic discrimiiv modls Probbilisic Griv Modls Ø W o ur o robbilisic roch o clssificio Ø W ll s ho modls ih lir dcisio boudris

More information

(A) 1 (B) 1 + (sin 1) (C) 1 (sin 1) (D) (sin 1) 1 (C) and g be the inverse of f. Then the value of g'(0) is. (C) a. dx (a > 0) is

(A) 1 (B) 1 + (sin 1) (C) 1 (sin 1) (D) (sin 1) 1 (C) and g be the inverse of f. Then the value of g'(0) is. (C) a. dx (a > 0) is [STRAIGHT OBJECTIVE TYPE] l Q. Th vlu of h dfii igrl, cos d is + (si ) (si ) (si ) Q. Th vlu of h dfii igrl si d whr [, ] cos cos Q. Vlu of h dfii igrl ( si Q. L f () = d ( ) cos 7 ( ) )d d g b h ivrs

More information

UNIT III STANDARD DISTRIBUTIONS

UNIT III STANDARD DISTRIBUTIONS UNIT III STANDARD DISTRIBUTIONS Biomial, Poisso, Normal, Gomric, Uiform, Eoial, Gamma disribuios ad hir roris. Prard by Dr. V. Valliammal Ngaiv biomial disribuios Prard by Dr.A.R.VIJAYALAKSHMI Sadard Disribuios

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

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

Almost unbiased exponential estimator for the finite population mean

Almost unbiased exponential estimator for the finite population mean Almos ubasd poal smaor for f populao ma Rajs Sg, Pakaj aua, ad rmala Saa, Scool of Sascs, DAVV, Idor (M.P., Ida (rsgsa@aoo.com Flor Smaradac ar of Dparm of Mamacs, Uvrs of Mco, Gallup, USA (smarad@um.du

More information

AR(1) Process. The first-order autoregressive process, AR(1) is. where e t is WN(0, σ 2 )

AR(1) Process. The first-order autoregressive process, AR(1) is. where e t is WN(0, σ 2 ) AR() Procss Th firs-ordr auorgrssiv procss, AR() is whr is WN(0, σ ) Condiional Man and Varianc of AR() Condiional man: Condiional varianc: ) ( ) ( Ω Ω E E ) var( ) ) ( var( ) var( σ Ω Ω Ω Ω E Auocovarianc

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

Paper 3A3 The Equations of Fluid Flow and Their Numerical Solution Handout 1

Paper 3A3 The Equations of Fluid Flow and Their Numerical Solution Handout 1 Paper 3A3 The Equaios of Fluid Flow ad Their Numerical Soluio Hadou Iroducio A grea ma fluid flow problems are ow solved b use of Compuaioal Fluid Damics (CFD) packages. Oe of he major obsacles o he good

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

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

BMM3553 Mechanical Vibrations

BMM3553 Mechanical Vibrations BMM3553 Mhaial Vibraio Chapr 3: Damp Vibraio of Sigl Dgr of From Sym (Par ) by Ch Ku Ey Nizwa Bi Ch Ku Hui Fauly of Mhaial Egirig mail: y@ump.u.my Chapr Dripio Ep Ouom Su will b abl o: Drmi h aural frquy

More information

EE757 Numerical Techniques in Electromagnetics Lecture 8

EE757 Numerical Techniques in Electromagnetics Lecture 8 757 Numerical Techiques i lecromageics Lecure 8 2 757, 206, Dr. Mohamed Bakr 2D FDTD e i J e i J e i J T TM 3 757, 206, Dr. Mohamed Bakr T Case wo elecric field compoes ad oe mageic compoe e i J e i J

More information

82A Engineering Mathematics

82A Engineering Mathematics Class Nos 5: Sod Ordr Diffrial Eqaio No Homoos 8A Eiri Mahmais Sod Ordr Liar Diffrial Eqaios Homoos & No Homoos v q Homoos No-homoos q ar iv oios fios o h o irval I Sod Ordr Liar Diffrial Eqaios Homoos

More information

Compact Finite Difference Schemes for Solving a Class of Weakly- Singular Partial Integro-differential Equations

Compact Finite Difference Schemes for Solving a Class of Weakly- Singular Partial Integro-differential Equations Ma. Sci. Le. Vol. No. 53-0 (0 Maemaical Scieces Leers A Ieraioal Joural @ 0 NSP Naural Scieces Publisig Cor. Compac Fiie Differece Scemes for Solvig a Class of Weakly- Sigular Parial Iegro-differeial Equaios

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

P a g e 5 1 of R e p o r t P B 4 / 0 9

P a g e 5 1 of R e p o r t P B 4 / 0 9 P a g e 5 1 of R e p o r t P B 4 / 0 9 J A R T a l s o c o n c l u d e d t h a t a l t h o u g h t h e i n t e n t o f N e l s o n s r e h a b i l i t a t i o n p l a n i s t o e n h a n c e c o n n e

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

Comparison between Fourier and Corrected Fourier Series Methods

Comparison between Fourier and Corrected Fourier Series Methods Malaysia Joural of Mahemaical Scieces 7(): 73-8 (13) MALAYSIAN JOURNAL OF MATHEMATICAL SCIENCES Joural homepage: hp://eispem.upm.edu.my/oural Compariso bewee Fourier ad Correced Fourier Series Mehods 1

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

Advection! Discontinuous! solutions shocks! Shock Speed! ! f. !t + U!f. ! t! x. dx dt = U; t = 0

Advection! Discontinuous! solutions shocks! Shock Speed! ! f. !t + U!f. ! t! x. dx dt = U; t = 0 p://www.d.edu/~gryggva/cfd-course/ Advecio Discoiuous soluios socks Gréar Tryggvaso Sprig Discoiuous Soluios Cosider e liear Advecio Equaio + U = Te aalyic soluio is obaied by caracerisics d d = U; d d

More information

MA6451-PROBABILITY AND RANDOM PROCESSES

MA6451-PROBABILITY AND RANDOM PROCESSES MA645-PROBABILITY AND RANDOM PROCESSES UNIT I RANDOM VARIABLES Dr. V. Valliammal Darm of Alid Mahmaics Sri Vkaswara Collg of Egirig Radom variabl Radom Variabls A ral variabl whos valu is drmid by h oucom

More information

Outline. simplest HMM (1) simple HMMs? simplest HMM (2) Parameter estimation for discrete hidden Markov models

Outline. simplest HMM (1) simple HMMs? simplest HMM (2) Parameter estimation for discrete hidden Markov models Oulie Parameer esimaio for discree idde Markov models Juko Murakami () ad Tomas Taylor (2). Vicoria Uiversiy of Welligo 2. Arizoa Sae Uiversiy Descripio of simple idde Markov models Maximum likeliood esimae

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

Inference of the Second Order Autoregressive. Model with Unit Roots

Inference of the Second Order Autoregressive. Model with Unit Roots Ieraioal Mahemaical Forum Vol. 6 0 o. 5 595-604 Iferece of he Secod Order Auoregressive Model wih Ui Roos Ahmed H. Youssef Professor of Applied Saisics ad Ecoomerics Isiue of Saisical Sudies ad Research

More information

Approximating Solutions for Ginzburg Landau Equation by HPM and ADM

Approximating Solutions for Ginzburg Landau Equation by HPM and ADM Available a hp://pvamu.edu/aam Appl. Appl. Mah. ISSN: 193-9466 Vol. 5, No. Issue (December 1), pp. 575 584 (Previously, Vol. 5, Issue 1, pp. 167 1681) Applicaios ad Applied Mahemaics: A Ieraioal Joural

More information

MONTGOMERY COLLEGE Department of Mathematics Rockville Campus. 6x dx a. b. cos 2x dx ( ) 7. arctan x dx e. cos 2x dx. 2 cos3x dx

MONTGOMERY COLLEGE Department of Mathematics Rockville Campus. 6x dx a. b. cos 2x dx ( ) 7. arctan x dx e. cos 2x dx. 2 cos3x dx MONTGOMERY COLLEGE Dpartmt of Mathmatics Rockvill Campus MATH 8 - REVIEW PROBLEMS. Stat whthr ach of th followig ca b itgratd by partial fractios (PF), itgratio by parts (PI), u-substitutio (U), or o of

More information

Modeling of Reductive Biodegradation of TCE to ETH. Adam Worsztynowicz, Dorota Rzychon, Sebastian Iwaszenko, Tomasz Siobowicz

Modeling of Reductive Biodegradation of TCE to ETH. Adam Worsztynowicz, Dorota Rzychon, Sebastian Iwaszenko, Tomasz Siobowicz Modlig of Rduciv Biodgradaio of o ETH Adam Worszyowicz, Doroa Rzycho, Sbasia Iwaszo, Tomasz Siobowicz Isiu for Ecology of Idusrial Aras Kossuha S., Kaowic, Polad l. (+-) 5, fax: (+-) 5 7 7 -mail: iu@iu.aowic.pl

More information

Chapter 2 Infinite Series Page 1 of 11. Chapter 2 : Infinite Series

Chapter 2 Infinite Series Page 1 of 11. Chapter 2 : Infinite Series Chatr Ifiit Sris Pag of Sctio F Itgral Tst Chatr : Ifiit Sris By th d of this sctio you will b abl to valuat imror itgrals tst a sris for covrgc by alyig th itgral tst aly th itgral tst to rov th -sris

More information

Research on the Decomposition of the Economic Impact Factors of Air. Pollution in Hubei Province in China

Research on the Decomposition of the Economic Impact Factors of Air. Pollution in Hubei Province in China d raioal Cofrc o ducaio, Maagm ad formaio cholog (CM 5) Rsarch o h Dcomposiio of h coomic mpac Facors of Air olluio i Hubi rovic i Chia Luo Jua, a, Aglia N.lchko, b, H Qiga, c Collg of Mahmaics ad Compur

More information

Study on Light Dynamic Penetration to Test Coarse Sand Relative Density in Bridge Culvert Back Sand Filling

Study on Light Dynamic Penetration to Test Coarse Sand Relative Density in Bridge Culvert Back Sand Filling 217 Iraioal Cofrc o Trasporaio Ifrasrucur ad Marials (ICTIM 217) ISBN: 978-1-6595-442-4 Sudy o Lig Dyamic Praio o Ts Coars Sad Rlaiv Dsiy i Bridg Culvr Back Sad Fillig J.B. Lv, Y.M. Yi, Z.T. Yu, Z.C. Xu,

More information

Optimization of Rotating Machines Vibrations Limits by the Spring - Mass System Analysis

Optimization of Rotating Machines Vibrations Limits by the Spring - Mass System Analysis Joural of aerials Sciece ad Egieerig B 5 (7-8 (5 - doi: 765/6-6/57-8 D DAVID PUBLISHING Opimizaio of Roaig achies Vibraios Limis by he Sprig - ass Sysem Aalysis BENDJAIA Belacem sila, Algéria Absrac: The

More information

An Introduction to Asymptotic Expansions

An Introduction to Asymptotic Expansions A Itroductio to Asmptotic Expasios R. Shaar Subramaia Asmptotic xpasios ar usd i aalsis to dscrib th bhavior of a fuctio i a limitig situatio. Wh a fuctio ( x, dpds o a small paramtr, ad th solutio of

More information

Outline. Overlook. Controllability measures. Observability measures. Infinite Gramians. MOR: Balanced truncation based on infinite Gramians

Outline. Overlook. Controllability measures. Observability measures. Infinite Gramians. MOR: Balanced truncation based on infinite Gramians Ouli Ovrlook Corollabiliy masurs Obsrvabiliy masurs Ifii Gramias MOR: alacd rucaio basd o ifii Gramias Ovrlook alacd rucaio: firs balacig h ruca. Giv a I sysm: / y u d d For covic of discussio w do h sysm

More information

An Efficient Method to Reduce the Numerical Dispersion in the HIE-FDTD Scheme

An Efficient Method to Reduce the Numerical Dispersion in the HIE-FDTD Scheme Wireless Egieerig ad Techolog, 0,, 30-36 doi:0.436/we.0.005 Published Olie Jauar 0 (hp://www.scirp.org/joural/we) A Efficie Mehod o Reduce he umerical Dispersio i he IE- Scheme Jua Che, Aue Zhag School

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

Pricing and Hedging of Long-term Futures and Forward Contracts by a Three-Factor Model

Pricing and Hedging of Long-term Futures and Forward Contracts by a Three-Factor Model CIRJE-F-68 Pricig ad Hdgig of Log-rm Fuurs ad Forward Coracs by a hr-facor Modl Kichiro Shiraya Mizuho-DL Fiacial chology Co. Ld. Akihiko akahashi Uivrsiy of okyo April 009 CIRJE Discussio Paprs ca b dowloadd

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

Naive Parameter Estimation Technique of Equity Return Models Based on Short and Long Memory Processes

Naive Parameter Estimation Technique of Equity Return Models Based on Short and Long Memory Processes 6 pp.-6 004 Naiv Paramr Eimaio Tchiqu of Equiy Rur Mol Ba o Shor a Log Mmory Proc Koichi Miyazai Abrac Th aalyi o variac of Japa quiy rur from h poi of obrvaio irval i qui fw hough i i impora i maagig

More information

Lecture 12: Introduction to nonlinear optics II.

Lecture 12: Introduction to nonlinear optics II. Lcur : Iroduco o olar opcs II r Kužl ropagao of srog opc sgals propr olar ffcs Scod ordr ffcs! Thr-wav mxg has machg codo! Scod harmoc grao! Sum frqucy grao! aramrc grao Thrd ordr ffcs! Four-wav mxg! Opcal

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

8(4 m0) ( θ ) ( ) Solutions for HW 8. Chapter 25. Conceptual Questions

8(4 m0) ( θ ) ( ) Solutions for HW 8. Chapter 25. Conceptual Questions Solutios for HW 8 Captr 5 Cocptual Qustios 5.. θ dcrass. As t crystal is coprssd, t spacig d btw t plas of atos dcrass. For t first ordr diffractio =. T Bragg coditio is = d so as d dcrass, ust icras for

More information

Elementary Differential Equations and Boundary Value Problems

Elementary Differential Equations and Boundary Value Problems Elmnar Diffrnial Equaions and Boundar Valu Problms Boc. & DiPrima 9 h Ediion Chapr : Firs Ordr Diffrnial Equaions 00600 คณ ตศาสตร ว ศวกรรม สาขาว ชาว ศวกรรมคอมพ วเตอร ป การศ กษา /55 ผศ.ดร.อร ญญา ผศ.ดร.สมศ

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

Numerical Method for Ordinary Differential Equation

Numerical Method for Ordinary Differential Equation Numerical ehod for Ordiar Differeial Equaio. J. aro ad R. J. Lopez, Numerical Aalsis: A Pracical Approach, 3rd Ed., Wadsworh Publishig Co., Belmo, CA (99): Chap. 8.. Iiial Value Problem (IVP) d (IVP):

More information

VIM for Determining Unknown Source Parameter in Parabolic Equations

VIM for Determining Unknown Source Parameter in Parabolic Equations ISSN 1746-7659, Eglad, UK Joural of Iformaio ad Compuig Sciece Vol. 11, No., 16, pp. 93-1 VIM for Deermiig Uko Source Parameer i Parabolic Equaios V. Eskadari *ad M. Hedavad Educaio ad Traiig, Dourod,

More information

Calculus BC 2015 Scoring Guidelines

Calculus BC 2015 Scoring Guidelines AP Calculus BC 5 Scorig Guidelies 5 The College Board. College Board, Advaced Placeme Program, AP, AP Ceral, ad he acor logo are regisered rademarks of he College Board. AP Ceral is he official olie home

More information

z 1+ 3 z = Π n =1 z f() z = n e - z = ( 1-z) e z e n z z 1- n = ( 1-z/2) 1+ 2n z e 2n e n -1 ( 1-z )/2 e 2n-1 1-2n -1 1 () z

z 1+ 3 z = Π n =1 z f() z = n e - z = ( 1-z) e z e n z z 1- n = ( 1-z/2) 1+ 2n z e 2n e n -1 ( 1-z )/2 e 2n-1 1-2n -1 1 () z Sris Expasio of Rciprocal of Gamma Fuctio. Fuctios with Itgrs as Roots Fuctio f with gativ itgrs as roots ca b dscribd as follows. f() Howvr, this ifiit product divrgs. That is, such a fuctio caot xist

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

) 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

Euler s Method for Solving Initial Value Problems in Ordinary Differential Equations.

Euler s Method for Solving Initial Value Problems in Ordinary Differential Equations. Eulr s Mthod for Solvig Iitial Valu Problms i Ordiar Diffrtial Equatios. Suda Fadugba, M.Sc. * ; Bosd Ogurid, Ph.D. ; ad Tao Okulola, M.Sc. 3 Dpartmt of Mathmatical ad Phsical Scics, Af Babalola Uivrsit,

More information