FourierSpectralMethodsforNumericalSolvingoftheKuramotoSivashinskyEquation

Size: px
Start display at page:

Download "FourierSpectralMethodsforNumericalSolvingoftheKuramotoSivashinskyEquation"

Transcription

1 Global Joral of Rsarhs i Egirig: I rial Mhods Vol Iss Vrsio. Yar Typ: Dobl Blid Pr Rviwd Iraioal Rsarh Joral Pblishr: Global Jorals I. USA Oli ISS: & Pri ISS: orir Spral Mhods for rial Solvig of h Kraoo-Sivashisy Eqaio By Gia Zavalai Polyhi Uivrsiy of Tiraa Albaia Absra- I his papr I prsd a rial hiq for solvig Kraoo-Sivashisy qaio basd o spral orir hods. This qaio dsribs raio diffsio probls ad h dyais of visos-fid fils flowig alog walls. Afr w wro h qaio i ri spa w g a sys. I his as h poial i diffrig hods igra h sys h or araly ha ohr hods si h poial i diffrig hods ass i hir drivaio ha h solio varis slowly i i. Wh valaig h offiis of h poial i diffrig ad h poial i diffrig Rg Ka hods via h Cahy igral. All opaioal wor is do wih Malab paag. Kywords: disr forir rasfor poial i diffrig poial i diffrig rg a hods ahy igral raoo-sivashisy qaio. GJRE-I Classifiaio : OR Cod: 6 6 orirspralmhodsforrialsolvigofhkraoosivashisyeqaio Srily as pr h oplia ad rglaios of:. Gia Zavalai. This is a rsarhrviw papr disribd dr h rs of h Craiv Coos Aribio- oorial. Upord is hp:raivoos.orglissby-. priig all o orial s disribio ad rprodio iay di providd h origial wor is proprly id.

2 orir Spral Mhods for rial Solvig of h Kraoo-Sivashisy Eqaio Gia Zavalai Absra- I his papr I prsd a rial hiq for solvig Kraoo-Sivashisy qaio basd o spral orir hods. This qaio dsribs raio diffsio probls ad h dyais of visos-fid fils flowig alog walls. Afr w wro h qaio i ri spa w g a sys. I his as h poial i diffrig hods igra h sys h or araly ha ohr hods si h poial i diffrig hods ass i hir drivaio ha h solio varis slowly i i. Wh valaig h offiis of h poial i diffrig ad h poial i diffrig Rg Ka hods via h Cahy igral. All opaioal wor is do wih Malab paag. Kywords: disr forir rasfor poial i diffrig poial i diffrig rg a hods ahy igral raoo-sivashisy qaio. I. Irodio orir aalysis ors i h odlig of idpd phoa ha ar aly or approialy priodi. Eapls of his ild h digial prossig of iforaio sh as sph; h aalysis of aral pho sh as arhqas; i h sdy of vibraios of sphrial irlar or raglar srrs; ad i h prossig of iags. I a ypial as orir spral hods wri h solio o h parial diffrial qaio as is orir sris. orir sris doposs a priodi ralvald fio of ral arg io a s of sipl osillaig rigoori fios ssssssssss ha a b robid o obai h origial fio. Sbsiig his sris io h parial diffrial qaio givs a sys of ordiary diffrial qaios for h i-dpd offiis of h rigoori rs i h sris h w hoos a isppig hod o solv hos ordiary diffrial qaios II. orir Sris Th orir sris of a sooh ad priodi ral-vald fio ff [; ] wih priod is ao f a os b si Ahor: Polyhi Uivrsiy of TiraaAlbaia. -ail: zavalaigia@hoail.o os a Si h basis fios si ad ar orhogoal h offiis ar giv by b f si d... f os d... orir sris a b prssd aly i opl for as follows a f Th o a i i i If w dfi b i i ao a ib a ib 5 f i whr h offiis fro h forlas of a ad b as III. i f 6 a b drid d Disr orir Trasfor I ay appliaios parilarly i aalyzig of ral siaios h fio f o b approiad is ow oly o a disr s of saplig pois" of. H h igral 7 ao b valad i a losd for ad orir aalysis ao b applid dirly. I h bos ssary o rpla oios orir aalysis by a disr vrsio of i. Th liar disr orir rasfor of a priodi disr sq of opl vals wih priod is a sq of priodi opl vals dfid by 7 Yar Global Joral of Rsarhs i Egirig I Vol XIV Iss I Vrsio I Global Jorals I. US

3 orir Spral Mhods for rial Solvig of h Kraoo-Sivashisy Eqaio Global Joral of Rsarhs i Egirig I Vol XIV Iss I Vrsio I Yar Th liar ivrs rasforaio is i i 8 9 Th os obvios appliaio of disr orir aalysis osiss i h rial allaio of orir offiis. Sppos w wa o approia a ralvald priodi fio f dfid o h irval [; ] ha is sapld wih a v br of grid pois h h... by i is orir sris. irs w op approia vals of h orir offiis f M i - - Siilarly h ivrs disr orir rasfor has h for M Whr M ad - M Bas h disr orir rasfor ad is ivrs hibi priodiiy wih priod i.. his propry rsls fro h priodi ar of i as o ss o s or ha rs i h sris ad i sffis o alla o fll priod. Th orir sris ford wih h approia offiis is f i Th fio ff o oly approias b aally irpolas ff a h saplig grid pois I ari for h disr orir rasfor 8 a b wri as M... Whr 6 M ad i -... i whr is opl oga of Th T algorih rds h opaioal wor rqird o arry o a disr orir rasfor by rdig h br of lipliaios ad addiios of opaioal i is rdd fro OO o OO log. To apply spral hods o a parial diffrial qaio w d o vala drivaivs of fios. Sppos ha w hav a priodi ral-vald fio f [; ] wih priod ha is disrizd wih a v br of grid pois so ha h grid Global Jorals I. US

4 siz h.th opl for of h orir sris rprsaio of f is A i f i h abov sris givs a r whih alras bw ± a h grid poi h... ad si i ao b diffriad w shold s is drivaiv o b zro a h grid pois. Th rial drivaivs of h fio f a b illsrad as a ari lipliaio.or h firs drivaiv w liply h orir offiis by h orrspodig diffriaio ari for a v br of grid pois. i Λ Diag This ari has o-zro ls oly o h diagoal. or a odd br of grid pois h Th w op a ivrs disr orir rasfor sig o rr o h physial spa ad dd h firs drivaiv of f o h grid. Siilarly aig h sod drivaiv orrspods o i diffriaio ari orrspodig o h firs drivaiv is diagoal wih ls. h lipliaio of h orir offiis by h orrspodig diffriaio ari for a v br of grid pois. i Λ Diag I gral i as of a v br of grid pois approiaig h -h rial drivaivs of a grid fio f orrspods o h lipliaio of h orir offiis by h orrspodig diffriaio ari whih is diagoal i wih ls for wih h pio ha for odd drivaivs w s h drivaiv of h highs od o b zro. IV. orir Spral Mhods for rial Solvig of h Kraoo-Sivashisy Eqaio Epoial Ti Diffrig Th faily of poial i diffrig shs. This lass of shs is spially sid o si-liar probls whih a b spli io a liar par whih oais h siffs par of h dyais of h probl ad a oliar par whih varis or slowly ha h liar par. Epoial i diffrig shs ar i igraio hods ha a b ffiily obid wih spaial approiaios o provid ara sooh solios for siff or highly osillaory si-liar parial diffrial qaios.i his papr I will prs h drivaio of h plii Epoial i diffrig shs for arbirary ordr followig h approah i [ ] [ ] [ ] ad prss h plii Rg-Ka vrsios of hs shs osrd by Co ad Mahws [ ]. W osidr for sipliiy a sigl odl of a siff ordiary diffrial qaio d whr is h d oliar forig r. To driv h s -sp Epoial i diffrig shs w liply hrogh by h igraig faor ad h igra h qaio ovr a sigl i sp fro o o obai. Yar Global Joral of Rsarhs i Egirig I Vol XIV Iss I Vrsio I Global Jorals I. US

5 d Th sp is o driv approiaios o h igral i qaio. This prodr dos o irod a wad fas i sal io h solio ad h shs a b gralizd o arbirary ordr. If w apply h wo Baward Diffr orla w a wri a polyoial approiaio o i h for G G G s s......! s o ha! If w sbsi io w g d G s d G s W will idia h igral by d ϑ If w sbsi ad io w g s ϑ 5 Whih rprs h gral graig forla of h poial i diffrig shs of ordr s Th firs-ordr poial i diffrig sh is obaid by sig s Th sod-ordr poial i diffrig sh is obaid by sig s { } By sig s w g h forh-ordr poial i diffrig sh 6 Θ Θ Θ Θ Θ Θ Θ Θ. orir Spral Mhods for rial Solvig of h Kraoo-Sivashisy Eqaio Global Jorals I. US Global Joral of Rsarhs i Egirig Vol XIV Iss I Vrsio I Yar I

6 V. O h Sabiliy of Edr Mhod Th sabiliy aalysis of h ETDRK hod is as follows s [] or[]. or h oliar ODE d. d wih h oliar par w sppos ha hr iss a fid poi his as ha. iarizig abo his fid poi if is h prrbaio of ad δ ' h whr y d δ. d ad h fid poi is sabl if R δ <. Th appliaio of h ETDRK hod o. lads o a rrr rlaio ivolvig ad. Irodig h prvios oaio δ h ad y h ad sig h Mahaia algbra paag w obai h followig aplifiaio faor r y. y y y y y y y y y y y y y y y y y y y y y y y y y y y y y y y y y y y y y y y y y y y 5 5 y y y y y y y y y y y y y y y y y y y y y y y y y y y y 5 5 y y y y y y y y y y y y y y y y y y y 6 6 y y y y A ipora rar: opig by h abov prssios sffrs fro orir Spral Mhods for rial Solvig of h Kraoo-Sivashisy Eqaio rial isabiliy for y los o zro. Bas of ha for sall y isad of h w will s hir asypoi pasios y y y y y Oy y y y y y Oy y y y y y Oy y y y y y Oy Yar 5 Global Joral of Rsarhs i Egirig I Vol XIV Iss I Vrsio I Global Jorals I. US

7 orir Spral Mhods for rial Solvig of h Kraoo-Sivashisy Eqaio W a wo obsrvaios: As y y or approiaio bos r 6 whih is h sabiliy fio for all h -sag Rg Ka hods of ordr for. Bas ad δ ay b opl h sabiliy rgio of h ETDRK hod is for-disioal ad hrfor qi diffil o rprs. Uforaly w do o ow ay prssio for ry w will oly b abl o plo i. Th os oo ida is o sdy i for ah parilar as; for apl assig o b fid ad ral i [] or ha boh ad δ ar pr iagiary brs i []. Global Joral of Rsarhs i Egirig I Vol XIV Iss I Vrsio I Yar 6 igr : Bodary of sabiliy rgios for svral gaivy igr : Eprial bodaris ad llips for y 75 Global Jorals I. US

8 orir Spral Mhods for rial Solvig of h Kraoo-Sivashisy Eqaio or dissipaiv PDEs wih priodi bodary odiios h salars ha aris wih a orir spral hod ar gaiv. s a for apl Brgr s qaio ε [ ] whr < ε. Trasforig i o h orir spa givs iζ εζ ζ.5 whr ζ is h orir wav-br ad h εζ < spa ovr a wid rag of offiis vals wh all h orir ods ar osidrd. or high vals of ζ h solios ar arad o h slow aifold qily bas < ad <<. I igr. w draw h bodary sabiliy rgios i h opl pla for y Wh h liar par is zro y w rogizd h sabiliy rgio of h forh-ordr Rg Ka hods ad as y h rgio grows. Of ors hs rgios oly giv a idiaio of h sabiliy of h hod. I fa for y < y << h bodaris ha ar obsrvd approah o llipss whos parars hav b fid rially wih h followig rsl. R I y.7.6 I igr. w draw h prial bodaris ad h llipss.6 wih y 75. Th spr of h liar opraor irass as ζ whil h igvals of h liarizaio of h oliar par lay o h iagiary ais ad iras as ζ. O h ohr had aordig o.6 wh R h irsio wih h iagiary ais I irass as y i.. asζ.si h bodary of sabiliy grows fasr ha h ETDRK hod shold hav a vry good bhavior o solv Brgr s qaio whih ofirs h rsls of papr [6]. VI. Epoial Ti Diffrig Rg-Ka Mhods Grally for h o-sp i-disrizaio hods ad h Rg-Ka hods all h iforaio rqird o sar h igraio is availabl.howvr for h li-sp i-disrizaio hods his is o r.ths hods rqir h valaios of a rai br of sarig vals of h oliar r a h -h ad prvios i sps o bild h hisory rqird for h allaios.thrfor i is dsirabl o osr poial i diffrig hods ha ar basd o Rg-Ka hods. Basd i [ ] ad [ ] Pig s i qaio ss 5 o g a ss 6 Th r a approias h val of a Th sp is o approia i h irval wih ad sbsi io ss yild Eqaio ss 8 rprs h firs-ordr Rg Ka poial i diffrig sh I a siilar way w a also for h sodordr Rg Ka poial i diffrig sh a ss 9 As w a s qaio ss 9 is ford by aig half a sp of ss 6 Th sp is o approia i h irval wih By sbsiig ss 9 io ss w g a O ss { a } ss By sig s a forh-ordr Rg Ka poial i diffrig sh is obaid as follows b a a a O ss 7 a a ss 8 Yar 7 Global Joral of Rsarhs i Egirig I Vol XIV Iss I Vrsio I Global Jorals I. US

9 orir Spral Mhods for rial Solvig of h Kraoo-Sivashisy Eqaio Global Jorals I. US Global Joral of Rsarhs i Egirig Vol XIV Iss I Vrsio I Yar 8 I b a { } a b ss I gral h poial i diffrig Rg-Ka hod ss has lassial ordr for b Hohbr ad Osra[] showd ha his hod sffrs fro a ordr rdio. Thy also prsd rial pris whih show ha h ordr rdio prdid by hir hory ay i fa aris i praial apls. I h wors as his lads o a ordr rdio o ordr hr for h Co ad Mahws hod ss []. Howvr for rai probls sh as h rial pris odd by Kassa ad Trfh[] [6] for solvig varios o-disioal diffsio-yp probls ad h rial rsls obaid i for solvig so dissipaiv ad disprsiv PDEs h forh-ordr ovrg of h forh-ordr Rg Ka poial i diffrig hod [] is ofird rially. ially w o ha as i h offiis of h s -ordr poial i diffrig Rg-Ka hods h hods rd o h orrspodig ordr of h Rg-Ka shs. V. Th Kraoo-Sivashisy Eqaio Th Kraoo-Sivashisy qaiois o of h sipls PDEs apabl of dsribig opl bhavior i boh i ad spa. This qaio has b of ahaial irs bas of is rih dyaial propris. I physial rs his qaio dsribs raio diffsio probls ad h dyais of visosfid fils flowig alog walls. Kraoo-Sivashisy qaio i o spa disio a b wri Eqaio a b wri i igral for if w irod ζ h ζ ζ ζ ζ 5 or i for Th Kraoo-Sivashisy qaio wih priodi bodary odiios i orir spa a b wri as follows i 6 i 6. i d d 6. i i 6. i i 6. i i 6.5 If w sbsi io w g i i i i i i i i d d By siplifyig ad o ha

10 orir Spral Mhods for rial Solvig of h Kraoo-Sivashisy Eqaio I fial for will b i i i Whr ϖ d i T[ ] Eqaio a b wri as fllows i ϖ h h i i [ ] T 8 Eqaio has srog dissipaiv dyais whih aris fro h forh ordr dissipaio r ha provids dapig a sall sals. Also i ilds λ igr : Th growh ra λ for prrbaios of h for Kraoo-Sivashisy K-S qaio Th zro solio of h K-S qaio is liarly sabl h growh ra λ > for prrbaios of λ i h for o ods wih wav-brs < for a wavlgh ϑ ad is dapd for ϑ ods wih > lada s igr. hs ods ar opld o ah ohr hrogh h o-liar r lada h haiss of a liar gaiv diffsio r whih is rsposibl for a isabiliy of ods wih larg wavlghi. sall wav-brs. Th oliar adviospig r i h qaio rasfors rgy bw larg ad sall sals. i o h zro solio of h Th siffss i h sys 7 is d o h fa ha h diagoal liar opraor wih h ls has so larg gaiv ral igvals ha rprs day bas of h srog dissipaio o a i sal h shorr ha ha ypial of h oliar r. Th ar of h solios o h h Kraoo-Sivashisy qaio varis wih h sys siz of liar opraor. or larg siz of liar opraor Yar 9 Global Joral of Rsarhs i Egirig Vol XIV Iss I Vrsio I I Global Jorals I. US

11 orir Spral Mhods for rial Solvig of h Kraoo-Sivashisy Eqaio Global Joral of Rsarhs i Egirig I Vol XIV Iss I Vrsio I Yar ogh sabl orir ods is o a h sys haoi. or sall siz of liar opraor isffi orir ods is asig h sys o approah a sady sa solio. I his as h poial i diffrig hods igra h sys vry h or araly ha ohr hods si h h poial i diffrig hods ass i hir drivaio ha h solio varis slowly i i. VI. rial Rsl or h silaio ss w hoos wo priodi iiial odiios os.7 os.si.6 os.si Wh valaig h offiis of h poial i diffrig ad h poial i diffrig Rg Ka hods via h "Cahy igral" approah [ 5][6] w hoos irlar oors of radis R. Eah oor is rd a o of h ls ha ar o h diagoal ari of h liar par [ ] [ ] of h si-disrizd odl. W igra h sys 7 sig forh-ordr Rg Ka poial i diffrig sh sig 6 wih i-sp siz. igr : Ti volio of h rial solio of h Kraoo-Sivashisy p o os 6 wih h iiial odiio [ ] Global Jorals I. US

12 orir Spral Mhods for rial Solvig of h Kraoo-Sivashisy Eqaio Yar igr : Ti volio of h rial solio of h Kraoo-Sivashisy p o os Th solio i h figr wih h iiial ad i- os odiio [ ] wih 6 sp siz 6 wih h iiial odiio [ ] appars as a sh plo ad shows wavs propagaig ravlig priodially i i ad prsisig wiho hag of shap. igr : Ti volio of h rial solio of h Kraoo-Sivashisy p o 6 wih h iiial odiio.7 os.si.6os.si [ ] I h figr wih h iiial odiio.7 os.si.6os.si [ ] wih ad i-sp siz h 6 solio appars as a sh plo ad shows wavs propagaig ravlig priodially i i ad prsisig wiho hag of shap. Global Joral of Rsarhs i Egirig I Vol XIV Iss I Vrsio I Global Jorals I. US

13 orir Spral Mhods for rial Solvig of h Kraoo-Sivashisy Eqaio Global Joral of Rsarhs i Egirig I Vol XIV Iss I Vrsio I Yar igr : Ti volio of h rial solio of h Kraoo-Sivashisy p o si 6 wih h iiial odiio [ ] I h figr wih h iiial odiio si [ ] wih 6 ad i-sp siz h solio appars or lar as a sh plo ad shows wavs propagaig ravlig priodially i i ad prsisig wiho hag of shap. VII. Colsios I his papr h ai obiv of his sdy was for fidig h solio of o disioal siliar forh ordr hyprboli Kraoo-Sivashisy qaio dsribig raio diffsio probls ad h dyais of visos-fid fils flowig alog walls. I ordr o ahiv his w applid orir spral approiaio for h spaial disrizaio. I addiio w valad h offis of h poial i diffrig ad h poial i diffrig forh ordr Rg Ka hods via h Cahy igral.so ypial apls hav b dosrad i ordr o illsra h ffiiy ad aray of h poial i diffrig hods hiq i his as. or h silaio ss w hos priodi bodary odiios ad applid orir spral approiaio for h spaial disrizaio. I addiio w valad h offiis of h Epoial Ti Diffrig Rg-Ka hods via h "Cahy igral" approah. Th qaios a b sd rpadly wih ssary adapaios of h iiial odiios. Rfrs Référs Rfrias. G. Byli J. M. Kisr ad. Vozovoi. A w Class of Ti Disrizaio Shs for h Solio of oliar PDEs. J. Cop. Phys. 7: J. Crai. Th Solio of Ordiary Dirial Eqaios wih arg Ti Cosas. I Mahaial Mhods for Digial Coprs A. Ralso ad H. S. Wilf ds.:8- Wily w Yor 96.. ridli. Gralizd Rg-Ka Mhods for h Solio of Siff Dirial Eqaios. I rial Tra of Dirial Eqaios R. BrlirshR. Grigori ad J. Shr dr ds. 6 r os i Mahais:5-5Sprigr Brli S. P. ors. A A-Sabl Modiaio of h Adas- Bashforh Mhods. I Cof. o rial Solio of Dirial Eqaios r os i Mah. 9969:-9 Sprigr-Vrlag Brli C. Kli. orh Ordr Ti-Sppig for ow Disprsio Korwg-d Vris ad oliar Shr digr Eqaios. Elroi Trasaios o ria Aalysis 9: A. K. Kassa ad.. Trfh. orh-ordr Ti Sppig for Siff PDEs. SIAM J. Si. Cop. 6: R.. Brd ad J. D. airs. rial Aalysis. Wadsworh Grop svh diio. 8. M. Hohbr ad A. Osra. Eplii Epoial Rg-Ka Mhods for Si-liar Paraboli Probls. SIAM J. r. Aal. : S. M. Co ad P. C. Mahws. Epoial Ti Diffrig for Siff Syss. J. Cop. Phys. 76:-55.. A. K. Kassa. High Ordr Ti sppig for Siff Si-iar Parial Diffrial Eqaios. PhD hsis Oford Uivrsiy. Global Jorals I. US

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

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

More information

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

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

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

Boyce/DiPrima/Meade 11 th ed, Ch 4.1: Higher Order Linear ODEs: General Theory

Boyce/DiPrima/Meade 11 th ed, Ch 4.1: Higher Order Linear ODEs: General Theory Bo/DiPima/Mad h d Ch.: High Od Lia ODEs: Gal Tho Elma Diffial Eqaios ad Boda Val Poblms h diio b William E. Bo Rihad C. DiPima ad Dog Mad 7 b Joh Wil & Sos I. A h od ODE has h gal fom d d P P P d d W assm

More information

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

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

More information

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

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

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

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

, R we have. x x. ) 1 x. R and is a positive bounded. det. International Journal of Basic & Applied Sciences IJBAS-IJENS Vol:10 No:06 11

, R we have. x x. ) 1 x. R and is a positive bounded. det. International Journal of Basic & Applied Sciences IJBAS-IJENS Vol:10 No:06 11 raioal Joral of asic & ppli Scics JS-JENS Vol: No:6 So Dirichl ors a Pso Diffrial Opraors wih Coiioall Epoial Cov cio aa. M. Kail Dpar of Mahaics; acl of Scic; Ki laziz Uivrsi Jah Sai raia Eail: fkail@ka..sa

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

( 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

International Journal of Pure and Applied Sciences and Technology

International Journal of Pure and Applied Sciences and Technology I. J. Pr Appl. Sci. Tchol. 4 pp. -4 Iraioal Joral of Pr a Appli Scics a Tcholog ISSN 9-67 Aailabl oli a www.ijopaasa.i Rsarch Papr Variaioal Iraio Mho for Solig So Mols of Noliar Parial Diffrial Eqaios

More information

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

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

More information

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

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

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

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

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

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

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

Variational iteration method: A tools for solving partial differential equations

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

More information

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

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

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

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

More information

Right Angle Trigonometry

Right Angle Trigonometry Righ gl Trigoomry I. si Fs d Dfiiios. Righ gl gl msurig 90. Srigh gl gl msurig 80. u gl gl msurig w 0 d 90 4. omplmry gls wo gls whos sum is 90 5. Supplmry gls wo gls whos sum is 80 6. Righ rigl rigl wih

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

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

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

EEE 304 Test 1 NAME: solutions

EEE 304 Test 1 NAME: solutions EEE 4 NAME: olio Probl : For h oio i ih rafr fio. Fi h rgio of ovrg of orrpoig o:.. a abl... a aal.. Cop h i p rpo x, aig ha i i aal. / / / / } { } {R, }; {R, } {. } {R : }, R { :. L L L L Y L Y x L Caali

More information

DIFFERENTIAL EQUATIONS MTH401

DIFFERENTIAL EQUATIONS MTH401 DIFFERENTIAL EQUATIONS MTH Virual Uivrsi of Pakisa Kowldg bod h boudaris Tabl of Cos Iroduio... Fudamals.... Elms of h Thor.... Spifi Eampls of ODE s.... Th ordr of a quaio.... Ordiar Diffrial Equaio....5

More information

EEE 304 Test 1 NAME:

EEE 304 Test 1 NAME: EEE 0 NME: For h oio i ih rafr fio 0.. Fi h rgio of ovrg of orrpoig o:.. a abl... a aal.. Cop h i p rpo x aig ha i i abl..: { 0. R }. : { 0. R } : 0. { aal / / 0. aal 0. aal { 0. R } {0 R } Probl : For

More information

Iterative Methods of Order Four for Solving Nonlinear Equations

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

More information

LINEAR 2 nd ORDER DIFFERENTIAL EQUATIONS WITH CONSTANT COEFFICIENTS

LINEAR 2 nd ORDER DIFFERENTIAL EQUATIONS WITH CONSTANT COEFFICIENTS Diol Bgyoko (0) I.INTRODUCTION LINEAR d ORDER DIFFERENTIAL EQUATIONS WITH CONSTANT COEFFICIENTS I. Dfiiio All suh diffril quios s i h sdrd or oil form: y + y + y Q( x) dy d y wih y d y d dx dx whr,, d

More information

Variational Iteration Method for Solving Telegraph Equations

Variational Iteration Method for Solving Telegraph Equations Availabl a hp://pvam.d/aam Appl. Appl. Mah. ISSN: 9-9 Vol. I (J 9) pp. (Prvioly Vol. No. ) Applicaio ad Applid Mahmaic: A Iraioal Joral (AAM) Variaioal Iraio Mhod for Solvig Tlgraph Eqaio Syd Taf Mohyd-Di

More information

AE57/AC51/AT57 SIGNALS AND SYSTEMS DECEMBER 2012

AE57/AC51/AT57 SIGNALS AND SYSTEMS DECEMBER 2012 AE7/AC/A7 SIGNALS AND SYSEMS DECEMBER Q. Drmi powr d rgy of h followig igl j i ii =A co iii = Solio: i E P I I l jw l I d jw d d Powr i fii, i i powr igl ii =A cow E P I co w d / co l I I l d wd d Powr

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

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

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

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

More information

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

Fractional Complex Transform for Solving the Fractional Differential Equations

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

More information

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

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

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

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

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

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

More information

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

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

c. What is the average rate of change of f on the interval [, ]? Answer: d. What is a local minimum value of f? Answer: 5 e. On what interval(s) is f

c. What is the average rate of change of f on the interval [, ]? Answer: d. What is a local minimum value of f? Answer: 5 e. On what interval(s) is f Essential Skills Chapter f ( x + h) f ( x ). Simplifying the difference quotient Section. h f ( x + h) f ( x ) Example: For f ( x) = 4x 4 x, find and simplify completely. h Answer: 4 8x 4 h. Finding the

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

Lecture contents. Semiconductor statistics. NNSE508 / NENG452 Lecture #12

Lecture contents. Semiconductor statistics. NNSE508 / NENG452 Lecture #12 Ltur otts Sioutor statistis S58 / G45 Ltur # illig th pty bas: Distributio futio ltro otratio at th rgy (Dsity of stats) (istributio futio): ( ) ( ) f ( ) Pauli lusio Priipl: o two ltros (frios) a hav

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

Controllability and Observability of Matrix Differential Algebraic Equations

Controllability and Observability of Matrix Differential Algebraic Equations NERNAONAL JOURNAL OF CRCUS, SYSEMS AND SGNAL PROCESSNG Corollabiliy ad Obsrvabiliy of Marix Diffrial Algbrai Equaios Ya Wu Absra Corollabiliy ad obsrvabiliy of a lass of marix Diffrial Algbrai Equaio (DAEs)

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

Modified Decomposition Method for Solution of Fractional Partial Differential Equations of Two-Sided

Modified Decomposition Method for Solution of Fractional Partial Differential Equations of Two-Sided Arile Ieraioal Joral of Moder Mahemaial Siee 4: 3-36 Ieraioal Joral of Moder Mahemaial Siee Joral homepage:www.modersieifipre.om/joral/ijmm.ap ISSN: 66-86X Florida USA Modified Deompoiio Mehod for Solio

More information

Laguerre wavelet and its programming

Laguerre wavelet and its programming Iraioal Joural o Mahaics rds ad chology (IJM) Volu 49 Nubr Spbr 7 agurr l ad is prograig B Sayaaraya Y Pragahi Kuar Asa Abdullah 3 3 Dpar o Mahaics Acharya Nagarjua Uivrsiy Adhra pradsh Idia Dpar o Mahaics

More information

3.2. Derivation of Laplace Transforms of Simple Functions

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

More information

Decline Curves. Exponential decline (constant fractional decline) Harmonic decline, and Hyperbolic decline.

Decline Curves. Exponential decline (constant fractional decline) Harmonic decline, and Hyperbolic decline. Dlin Curvs Dlin Curvs ha lo flow ra vs. im ar h mos ommon ools for forasing roduion and monioring wll rforman in h fild. Ths urvs uikly show by grahi mans whih wlls or filds ar roduing as xd or undr roduing.

More information

Approximation of Functions Belonging to. Lipschitz Class by Triangular Matrix Method. of Fourier Series

Approximation of Functions Belonging to. Lipschitz Class by Triangular Matrix Method. of Fourier Series I Jorl of Mh Alysis, Vol 4, 2, o 2, 4-47 Approximio of Fcios Blogig o Lipschiz Clss by Triglr Mrix Mhod of Forir Sris Shym Ll Dprm of Mhmics Brs Hid Uivrsiy, Brs, Idi shym _ll@rdiffmilcom Biod Prsd Dhl

More information

DETERMINATION OF THERMAL STRESSES OF A THREE DIMENSIONAL TRANSIENT THERMOELASTIC PROBLEM OF A SQUARE PLATE

DETERMINATION OF THERMAL STRESSES OF A THREE DIMENSIONAL TRANSIENT THERMOELASTIC PROBLEM OF A SQUARE PLATE DRMINAION OF HRMAL SRSSS OF A HR DIMNSIONAL RANSIN HRMOLASIC PROBLM OF A SQUAR PLA Wrs K. D Dpr o Mics Sr Sivji Co Rjr Mrsr Idi *Aor or Corrspodc ABSRAC prs ppr ds wi driio o prr disribio ow prr poi o

More information

Lecture 4: Laplace Transforms

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

More information

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

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

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

1. Solve by the method of undetermined coefficients and by the method of variation of parameters. (4)

1. Solve by the method of undetermined coefficients and by the method of variation of parameters. (4) 7 Differeial equaios Review Solve by he mehod of udeermied coefficies ad by he mehod of variaio of parameers (4) y y = si Soluio; we firs solve he homogeeous equaio (4) y y = 4 The correspodig characerisic

More information

Lecture contents. Density of states Distribution function Statistic of carriers. Intrinsic Extrinsic with no compensation Compensation

Lecture contents. Density of states Distribution function Statistic of carriers. Intrinsic Extrinsic with no compensation Compensation Ltur otts Dsity of stats Distributio futio Statisti of arrirs Itrisi trisi with o ompsatio ompsatio S 68 Ltur #7 Dsity of stats Problm: alulat umbr of stats pr uit rgy pr uit volum V() Larg 3D bo (L is

More information

Two-Dimensional Quantum Harmonic Oscillator

Two-Dimensional Quantum Harmonic Oscillator D Qa Haroc Oscllaor Two-Dsoal Qa Haroc Oscllaor 6 Qa Mchacs Prof. Y. F. Ch D Qa Haroc Oscllaor D Qa Haroc Oscllaor ch5 Schrödgr cosrcd h cohr sa of h D H.O. o dscrb a classcal arcl wh a wav ack whos cr

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

PURE MATHEMATICS A-LEVEL PAPER 1

PURE MATHEMATICS A-LEVEL PAPER 1 -AL P MATH PAPER HONG KONG EXAMINATIONS AUTHORITY HONG KONG ADVANCED LEVEL EXAMINATION PURE MATHEMATICS A-LEVEL PAPER 8 am am ( hours) This papr must b aswrd i Eglish This papr cosists of Sctio A ad Sctio

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

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

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

EE Control Systems LECTURE 11

EE Control Systems LECTURE 11 Up: Moy, Ocor 5, 7 EE 434 - Corol Sy LECTUE Copyrigh FL Lwi 999 All righ rrv POLE PLACEMET A STEA-STATE EO Uig fc, o c ov h clo-loop pol o h h y prforc iprov O c lo lc uil copor o oi goo y- rcig y uyig

More information

Some Applications of the Poisson Process

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

More information

Digital Signal Processing, Fall 2006

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

More information

Physics 302 Exam Find the curve that passes through endpoints (0,0) and (1,1) and minimizes 1

Physics 302 Exam Find the curve that passes through endpoints (0,0) and (1,1) and minimizes 1 Physis Exam 6. Fid th urv that passs through dpoits (, ad (, ad miimizs J [ y' y ]dx Solutio: Si th itgrad f dos ot dpd upo th variabl of itgratio x, w will us th sod form of Eulr s quatio: f f y' y' y

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

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

Phys463.nb Conductivity. Another equivalent definition of the Fermi velocity is

Phys463.nb Conductivity. Another equivalent definition of the Fermi velocity is 39 Anohr quival dfiniion of h Fri vlociy is pf vf (6.4) If h rgy is a quadraic funcion of k H k L, hs wo dfiniions ar idical. If is NOT a quadraic funcion of k (which could happ as will b discussd in h

More information

Section 8. Paraxial Raytracing

Section 8. Paraxial Raytracing Secio 8 Paraxial aracig 8- OPTI-5 Opical Desig ad Isrmeaio I oprigh 7 Joh E. Greiveamp YNU arace efracio (or reflecio) occrs a a ierface bewee wo opical spaces. The rasfer disace ' allows he ra heigh '

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

(1) (2) sin. nx Derivation of the Euler Formulas Preliminary Orthogonality of trigonometric system

(1) (2) sin. nx Derivation of the Euler Formulas Preliminary Orthogonality of trigonometric system orir Sri Priodi io A io i lld priodi io o priod p i p p > p: ir I boh d r io o priod p h b i lo io o priod p orir Sri Priod io o priod b rprd i rm o rioomri ri o b i I h ri ovr i i lld orir ri o hr b r

More information

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

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

More information

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

Further Results on Pair Sum Graphs

Further Results on Pair Sum Graphs Applid Mathmatis, 0,, 67-75 http://dx.doi.org/0.46/am.0.04 Publishd Oli Marh 0 (http://www.sirp.org/joural/am) Furthr Rsults o Pair Sum Graphs Raja Poraj, Jyaraj Vijaya Xavir Parthipa, Rukhmoi Kala Dpartmt

More information

Outline. Review Homework Problem. Review Homework Problem II. Review Dimensionless Problem. Review Convection Problem

Outline. Review Homework Problem. Review Homework Problem II. Review Dimensionless Problem. Review Convection Problem adial diffsio eqaio Febay 4 9 Diffsio Eqaios i ylidical oodiaes ay aeo Mechaical Egieeig 5B Seia i Egieeig Aalysis Febay 4, 9 Olie eview las class Gadie ad covecio boday codiio Diffsio eqaio i adial coodiaes

More information

Data Structures Lecture 3

Data Structures Lecture 3 Rviw: Rdix sor vo Rdix::SorMgr(isr& i, osr& o) 1. Dclr lis L 2. Rd h ifirs i sr i io lis L. Us br fucio TilIsr o pu h ifirs i h lis. 3. Dclr igr p. Vribl p is h chrcr posiio h is usd o slc h buck whr ifir

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

Boyce/DiPrima 9 th ed, Ch 7.8: Repeated Eigenvalues

Boyce/DiPrima 9 th ed, Ch 7.8: Repeated Eigenvalues Boy/DiPrima 9 h d Ch 7.8: Rpad Eignvalus Elmnary Diffrnial Equaions and Boundary Valu Problms 9 h diion by William E. Boy and Rihard C. DiPrima 9 by John Wily & Sons In. W onsidr again a homognous sysm

More information

1985 AP Calculus BC: Section I

1985 AP Calculus BC: Section I 985 AP Calculus BC: Sctio I 9 Miuts No Calculator Nots: () I this amiatio, l dots th atural logarithm of (that is, logarithm to th bas ). () Ulss othrwis spcifid, th domai of a fuctio f is assumd to b

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

American International Journal of Research in Science, Technology, Engineering & Mathematics

American International Journal of Research in Science, Technology, Engineering & Mathematics Ara raoal oral of ar S oloy r & aa Avalabl ol a //wwwar SSN Pr 38-349 SSN Ol 38-358 SSN D-O 38-369 AS a rfr r-rvw llary a o a joral bl by raoal Aoao of Sf ovao a ar AS SA A Aoao fy S r a Al ar oy rao ra

More information

Using the Lee-Carter Method to Forecast Mortality for Populations with Limited Data

Using the Lee-Carter Method to Forecast Mortality for Populations with Limited Data Dcbr, 00 da las savd: /0/0 3:5 PM da las prid: 06/5/03 4:39 PM Usig h L-Carr Mhod o Forcas Moraliy for Poplaios wih Liid Daa Na Li Dpar of Sociology Uivrsiy of Vicoria Vicoria, Caada lia@vic.ca Roald L

More information

Market Conditions under Frictions and without Dynamic Spanning

Market Conditions under Frictions and without Dynamic Spanning Mar Codiio udr Friio ad wihou Dyai Spaig Jui Kppo Hlii Uivriy of hology Sy Aalyi aboraory O Bo FIN-5 HU Filad hp://wwwhufi/ui/syaalyi ISBN 95--3948-5 Hlii Uivriy of hology ISSN 78-3 Sy Aalyi aboraory iblla

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

Fooling Newton s Method a) Find a formula for the Newton sequence, and verify that it converges to a nonzero of f. A Stirling-like Inequality

Fooling Newton s Method a) Find a formula for the Newton sequence, and verify that it converges to a nonzero of f. A Stirling-like Inequality Foolig Nwto s Mthod a Fid a formla for th Nwto sqc, ad vrify that it covrgs to a ozro of f. ( si si + cos 4 4 3 4 8 8 bt f. b Fid a formla for f ( ad dtrmi its bhavior as. f ( cos si + as A Stirlig-li

More information

MARTIN COUNTY, FLORIDA

MARTIN COUNTY, FLORIDA RA 5 OA. RFFY A A RA RVOAL R F 8+8 O 5+ 5+ 5+ ORI 55 OA. RFFY A A RA RVOAL R 8 F 5+ O 8+8 ROFIL ORIZ: = VR: = 5 ROFIL 5 5 5 5 5+ 5+ 5+ 5+ + 5+ 8+ + + + 8+ 8+ 8+ 8+ + 5+ 8+ 5+ - --A 8-K @.5 -K @.5 -K @.5

More information