Blow-up and Extinction Phenomenon for the Generalized Burgers Equation
|
|
- Jeffery Watson
- 5 years ago
- Views:
Transcription
1 Snd Ordrs for Rrins o rrins@bnhamscinca h On Cybrnics & Sysmics Journa On Accss Bow-u and Exincion Phnomnon for h Gnraizd Burgrs Euaion Chn Ning * ian Baodan and Chn Jiian Schoo of Scinc Souhws Univrsiy of Scinc and chnoogy Mianyang 6 China; Souhws Univrsiy of Scinc and chnoogy Mianyang 6 China Absrac: In his ar h auhor considr condiions of ha iniia boundary vau o sudy h dynamic bhavior for Gnraizd Burgrs uaion and giv hs sysm for ha nw condiions of bow-u and Exincion Phnomnon of hs uaion wih in rich using nginring Such as hs horis and mhod can b usd in ohr simiar sysms hy hav a wid rang of aicaions Fina som numrica simuaions ar carrid ou o suor hs nw rsus h auhors xnd dynamic bhavior and h criica vau o coninuum mor rvious work [3 9 3] for in-dh achiv for ay vau Kywords: Bow-u and xincion boundary vau robms gnraizd burgrs uaion noninar sourc INRODUCION AND PRELIMINARIES Lik Burgrs uaion and Schrodingr uaion is on of h mos modrn scinc univrsa uaion as dscrib h noninar wav uaion of h corrsonding ffc of h disrs-on and inracion mod in maria mchanics and fuid mchanics ar ay vau in hysics ara and aso coninuous sochasic rocss in h acua robm in many fids such as hs horis and mhod can b usd in ohr simiar sysms hy hav a wid rang of aicaions Johanns Burgrs firs by using of bow noninar uaion in yar 948 for h u + uu = u x xx ( whr > dno h fuid fow us dscrib ha inracion bwn h convcion and h ffciv sns of fow for h noninar sourc mod Rcny is dynamic im snior bhaviour and is anayica souion and numrica souion wr invsigad o sudy If h burgrs uaion was noninar uaion in h foowing of iniia boundary vau robm u + uu = u a < x < b > x xx u( x = ( x a < x < b u( a = u( b = > ( which > as h viscosiy cofficin (x for a givn funcion Baman gav ou sab of souion Many robms ar basd on h Burgs uaion basic mods o xnsion and aicaion [] manwhi Burgr uaion and Navir- Sok uaion can b hough of as h aroxima uaion [] mak i in h noninar wav gas dynamics h shock wav and coninuous sochasic rocss has a broad aicaion sac c (s [-5] AIkis S rsnov sudy in h foowing of iniia boundary vau robm ( ( u u + g x u u = u+ f (3 formua a condiion guaraning h absnc of h bow-u of a souion and discuss h oimaiy of his condiion [3] In aricuar funcions f ( u = u u u and f ( u = saisfy his condiion E (3 wih f ( u = u ariss in many aicaion (s [4-7] E ( wih g( x u and i is w known ha if f ( u is sur-inar h Phnomnon of h souion bowing u and xincion may occur (s [8-] Concrning h rvniv ffc of h inar gradin rm ( au + b u x ( i= or a s [] Du o h fac ha aramr is ofn sma w wi considr h hfu infunc of h diffusing rm u and u (in xincion; concrning h rvniv ffc of inar and noninar diffusion s [8 ] HE EXINCION PHENOMENON HE BUR- GERS EQUAION n L b a boundd domain of R having sufficiny smooh boundary n b our norma dircion and n u = / x = ( x [ + ha 3 = ( i= i 874-X/4 4 Bnham On
2 94 h On Cybrnics & Sysmics Journa 4 Voum 8 Ning a W considr Burgrs uaion wih highr-ordr rm as foows n u + g( x u u = u+ f( u Q = ( R ( ( i u x n = x i = / ( ( ( u x + u x / n = ( x ( ux ( = u( x x > whr ( ( = + ( + ( g x u a x u a x u b x ( = f u cu c u c u Dfiniion: If hr is ux ( of robm (-(4 saisfy: for souion ( ( [ u( x x u x x ( (3 (4 ( [ ] hn h robm (-(4 wih souion ux ( b cad xincion in fini im W wi giv h horm o xnd som rsus [9] w hav h foowing rsus as mma u x W L + hn for Lmma [] If > xiss C > such ha hods inuaiy: k + ( ( + ( + u C u u N ( + 4( + whr 4+ N ( sac L ( k = N = n (5 imis norm of Proof From Gagiardo-Nirnbrg inuaiy [9] and Hodr inuaiy ha w asy g h concusion horm 3 Assum ha = min a ( x > min a ( x > max ( a a = > hr xiss and saisfis foowing inuaiy: + + a u u x dx + a u u x dx u dx max { } + ( ( max a a u x dx+ u x dx hn u ( x ( L ( L L 4 u x (6 h souion ux ( of robm (-(4 wi b wih xincion in fini im and wih foow dcay sima: ( k k ( * u x dx u x dx C ( k [ u ( x dx = [ (7 Proof By u( x muiis h boh sid of ( and ingraing on for x o combin Grn s formua and boundary condiions w hav: u x dx + a u + u( x dx+ a u + u( x dx + = u dx+ u x dx By (8 and (6 w hav d d u ( x dx { } + + max (8 max a a u x dx u dx Uiiz mma w obain max sc suiing aram- k = ( n { } 4 n( max { } + r * C w obain ha bow inuaiy: d * k udx C ( u ( x dx d By ingra abov inuaiy for and noic iniia condi- u x = u x I is (7 hrfor h souion of ion (-(4 is xincion in fini im and has h rsu of simas ha coms h roof of horm 3 3 HE BLOW-UP PHENOMENON FOR HE BUR- GERS EQUAION Considr h foowing uaion of [3] u + g( x u u = u+ f ( u n in Q = ( R (3 Coud wih iniia and boundary condiions u x = x for ( x Q \{( x : x } Hr > and ar consans ( = (3 g = g g g g = g x u i = n n i i Assum ha g a( x u b( x a( x = a > min Q = + and k
3 Bow-u and Exincion Phnomnon for h Gnraizd Burgrs Euaion h On Cybrnics & Sysmics Journa 4 Voum 8 95 whr ab C( Q and h osiiv consans ar such ha y Rfor any y R If h souion is nonngaiv h as assumion is unncssary Concrning h noninar sourc f ( u w assum ha f f for a and such ha (33 L us formua our rsu Dno b = b( x min m = max u hr is h araboic boundary of { } Q Q i = Q \ x : x Wihou oss of gnraiy suos ha h domain is ying in h sri < x < W wi rov h goba (i for arbirary > cassica sovabiiy of robm (3 (3 undr h foowing assumion: hr xiss a consan M m such ha f M + bm a M + Lmma 3[3] Assum ha ( ( ( C g x u C Q i M M C ( (34 f u M M If condiion (33 and (34 ar saisfid hn for an arbirary > hr xiss a uniu cassica souion of robm (3 (3 such ha u x M (35 Morovr considr dynamic acion in arg im wih comound rm of gnraizd Burgrs uaion Considr h auxiiary uaion ( ( ( ( u+ a x u + a x u + b x u = u+ u u u + in( W sudy h mos yica cas: w omi subscri in x and : ( ( ( ( u+ a x u + a x u + b x u u ( ( = u + u u u + in xx Coud wih iniia and boundary condiions ( = ( x u x for ( x ( ( ( {( x x( } \ : x (36 (37 whr a a bc ( ( and h osiiv consans ar such ha y y R for any y R Undr h basd of corrsonding condiion and combin mma 3 w wi rov h goba cassica sovabiiy of robm (36 (37 undr h foowing assumion: hr xiss a consan M msuch ha + min { } + M + bm a + a M W wi suy h foowing horm: horm 3 Assum ha C ( (38 ( au + au + b C (( ( ( M M + ( + u u u C ( M M + If condiion (33 and (38 ar saisfid hn for an arbirary > hr xiss a uniu cassica souion of robm (36 (37 such ha u x M whr (39 ( ( \{( x : x } = max { } Proof L a ( x = a a ( x = a b( x = b = M M M ( = ( + f u u u u + ( + u + au + a u + b u = u + u u + u in x xx ( ( (3 W assum hr is ha u + and u + ar dfind ohrwis w ak u uand u u I is known ha hr xiss a goba souion of robm (3 and (37 wihou smanss rsricions on iniia daa for + min + whn and zro boundary condiions morovr if > + whn = (or { } = ; (or > max + hn a fini bow u occurs if h iniia daa is sufficiny arg L us ay our Lmma3 o E (39 If w considr wo cas (i and (ii: { } (i < + whn = hn condiion (38 is aways fufid wih M m b a a < + ( = ( + { } = max su / + + < min + whn ; Simiar cas (i hr wih (ii { }
4 96 h On Cybrnics & Sysmics Journa 4 Voum 8 Ning a M + su{ b } = m a + a min { } ( min { } max{ } max < + = + Combin h wo cas and as a consunc for arbirary daa hr xiss a goba souion saisfying h sima u max M M { } Nx considr anohr wo cas wih invrs form: (i Suos ha > + = Condiion (38 bcoms a smanss rsricion In fac rwri (38 in h form M M m such ha a + a Obviousy if + { b} max = a + a m + = max{ b} hn (38 is fufid wih M = m and hr xiss a goba souion such ha u m > max + whn Simiar cas (i hr M m ha is (ii L ha { } + { } m a + a /max b = max min { } { } hn (38 is fufid wih M = m and hr xiss a goba souion such ha u m Now considr h wo criica cas Cas (i = + whn = : + ( u + ( a + a u + b u = u + ( u u x xx For h funcion hav v u (3 = wih μ / ( a a ( μ v + a + a v + bv v = v + + xx ( μ c v = + w x (3 v= for x = { = x } < x=± { } Cas (ii = { } + whn ; min max{ } min { } u + ( a + a u + b u max{ } min { } = u + u u xx Simiar cas (i w hav x μ v + a + a v + bv v = u + + ( c v { } { } μ = max min xx v= for ( x = { = x } { < x=± } x (33 (34 Condiion (38 for E (3 ak h form M m μ such ha 4 ( μ + c M + μ M a + a M μ + Obviousy his condiion fufid wih { } su 4 ( μ + c μ M = max m a + a μ = / ( a + a and h sima u( x M μ is obaind As a consunc h horm guarans h goba sovabiiy of robm (3 (37 and h souion saisfis u x M μ x h sima Simiar cas (i hr M M > w hav M m μ and M m μ such ha 4 ( μ + c M + μ M ( max { } + max { } a a μ + M + Obviousy his condiion fufid wih { μ + c μ} su 4 M = max m a + a ( a + a = ( { } μ = / max + and h sima u( x M is obaind As a consunc h horm guarans h goba sovabiiy of μ
5 Bow-u and Exincion Phnomnon for h Gnraizd Burgrs Euaion ab h On Cybrnics & Sysmics Journa 4 Voum 8 Aking h aramrs of Burgr-E (36 a a b 8 ab 97 c c aking h aramrs of Burgr-E (36 a a b 8 robm (33 (37 and h souion saisfis h sima u ( x M Undr (37 w can show h rnd of dynamics bhavour of Burgr-E (36 wih aking h aramrs in ab (S Fig By (i and (ii w obain sima u ( x {M M } μ = / ( a + a According o cas ab W com his roof of horm CONCLUSION his aric mainy sudis h gnra dynamics bhaviour of Burgr-uaion of basing and Exinguishing hnomnon o discuss hs cas hrough crain aramrs vaus Such uaions aways xhibi a rich hnomnoogy aracs many anion in nginring mchanics maria mchanics and fuid mchanics wih aicaion vau h auhors xnd dynamic bhaviour and h criica vau o coninuum mor rvious work [ ] for in-dh achiv for ay vau CONFLIC OF INERES Fig ( h souion found by numrica ingraion of Burgr-E (36 dscriion aking h aramrs in ab h auhors confirm ha his aric conn has no confic of inrs ACKNOWLEDGEMENS his work is suord by h Naura Scinc Foundaion (NoZB9 of Sichuan Educaion Burau and h ky rogram of Scinc and chnoogy Foundaion (NoZd7 of Souhws Univrsiy of Scinc and chnoogy Fig ( h souion found by numrica ingraion of Burgr-E (36 dscriion aking h aramrs in ab 4 NUMERICAL SIMULAIONS In ordr o iusra our horica anaysis numrica simuaions ar aso incudd in aid of MALAB 7 Mos of aramrs ar aking foow wih from abs and According o cas ab : Figur dscriion aking h aramrs (S ab Undr (37 w can show h rnd of dynamics bhavour of Burgr-E (36 wih aking h aramrs in ab (S Fig Figur dscriion aking h aramrs (S ab REFERENCES [] [] [3] [4] [5] [6] [7] Fchr C A Burgrs uaion: a mod for a rasons in: Noy (d Numrica Souion of Paria Diffrnia Euaions NorhHoand Amsrdam 98 Karman V I Noninar Wavs in Disrsiv Mdia Prgamon Prss Nw York 975 AIkis S rsnov A condiion guaraning h absnc of h bow-u hnomnon for h gnraizd Burgrs uaion Noninar Anaysis No Gurs A Van Bn H Simifid hydrodynamic anaysis of surfuid urbuncin H II: inrna dynamics of inhomognous vorx ang PhysRvB Rao Ch S Sachdv P L Ramaswamy M Sf-simiar souions of a gnraizd Burgrs uaion wih noninar daming Noninar Ana RWA No Sun X Ward M J Masabiiy for a gnraizd Burgrs uaion wih aicaions o roagaing fam frons Euroan J A Mah rsnov AIS On h gnraizd Burgrs uaion NoDEA noninar diffrnia uaions A
6 98 h On Cybrnics & Sysmics Journa 4 Voum 8 Ning a [8] Samarskii A A Gaakionov V A Kurdjumov S P Mikhaiov A P Bow-u in Quasiinar araboic uaions In: d Gruyr Exosiios Mah Vo9 (d Gruyr Brnin [9] CHEN N Exincion of souion for a cass of Ginzbur-Landau racion-diffusion uaion in ouaion robms Jorna of Biomahmaics [] Ladyznska O A Soonnkav V A ra-sva N N Linar and uasi-inar uaion of araboic y Amr Mah Soc Proridn R I 968 [] rsnov AIS h Dirich robm for scond ordr smiinar iic and araboic uaion Diffr Eu A [] rsnov A I S A rmark on h orous mdium wih sourc A Mah L [3] Chn N ian B D and Chn J Q Bow-u of souions for som a cass of gnraizd noninar Schrodingr uaions A Mah Inf Sci6-3S [4] Chn N Chn JQ and ian B D Fixd Poin horms of Mui-vau ma And H s Variaion Iraion A Mah Inf Sci 6-3S [5] Liu XJ Zhou YH ZhangL & Wang JZ Wav souions of Burgrs uaion wih high Rynods numbrs Scinc China (chnoogica Scincs Juy Rcivd: Smbr 6 4 Rvisd: Dcmbr 3 4 Accd: Dcmbr 3 4 Ning a; Licns Bnham On his is an on accss aric icnsd undr h rms of h (hs://craivcommonsorg/icnss/by/4/gacod which rmis unrsricd noncommrcia us disribuion and rroducion in any mdium rovidd h work is rory cid
2. The Laplace Transform
Th aac Tranorm Inroucion Th aac ranorm i a unamna an vry uu oo or uying many nginring robm To in h aac ranorm w conir a comx variab σ, whr σ i h ra ar an i h imaginary ar or ix vau o σ an w viw a a oin
More informationBoyce/DiPrima 9 th ed, Ch 2.1: Linear Equations; Method of Integrating Factors
Boc/DiPrima 9 h d, Ch.: Linar Equaions; Mhod of Ingraing Facors Elmnar Diffrnial Equaions and Boundar Valu Problms, 9 h diion, b William E. Boc and Richard C. DiPrima, 009 b John Wil & Sons, Inc. A linar
More informationLecture 1: Numerical Integration The Trapezoidal and Simpson s Rule
Lcur : Numrical ngraion Th Trapzoidal and Simpson s Rul A problm Th probabiliy of a normally disribud (man µ and sandard dviaion σ ) vn occurring bwn h valus a and b is B A P( a x b) d () π whr a µ b -
More informationOn the Derivatives of Bessel and Modified Bessel Functions with Respect to the Order and the Argument
Inrnaional Rsarch Journal of Applid Basic Scincs 03 Aailabl onlin a wwwirjabscom ISSN 5-838X / Vol 4 (): 47-433 Scinc Eplorr Publicaions On h Driais of Bssl Modifid Bssl Funcions wih Rspc o h Ordr h Argumn
More informationElementary 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 informationLet s look again at the first order linear differential equation we are attempting to solve, in its standard form:
Th Ingraing Facor Mhod In h prvious xampls of simpl firs ordr ODEs, w found h soluions by algbraically spara h dpndn variabl- and h indpndn variabl- rms, and wri h wo sids of a givn quaion as drivaivs,
More informationA Condition for Stability in an SIR Age Structured Disease Model with Decreasing Survival Rate
A Condiion for abiliy in an I Ag rucurd Disas Modl wih Dcrasing urvival a A.K. upriana, Edy owono Dparmn of Mahmaics, Univrsias Padjadjaran, km Bandung-umng 45363, Indonsia fax: 6--7794696, mail: asupria@yahoo.com.au;
More informationMEM 355 Performance Enhancement of Dynamical Systems A First Control Problem - Cruise Control
MEM 355 Prformanc Enhancmn of Dynamical Sysms A Firs Conrol Problm - Cruis Conrol Harry G. Kwany Darmn of Mchanical Enginring & Mchanics Drxl Univrsiy Cruis Conrol ( ) mv = F mg sinθ cv v +.2v= u 9.8θ
More informationAn Indian Journal FULL PAPER. Trade Science Inc. A stage-structured model of a single-species with density-dependent and birth pulses ABSTRACT
[Typ x] [Typ x] [Typ x] ISSN : 974-7435 Volum 1 Issu 24 BioTchnology 214 An Indian Journal FULL PAPE BTAIJ, 1(24), 214 [15197-1521] A sag-srucurd modl of a singl-spcis wih dnsiy-dpndn and birh pulss LI
More informationChapter 5 The Laplace Transform. x(t) input y(t) output Dynamic System
EE 422G No: Chapr 5 Inrucor: Chung Chapr 5 Th Laplac Tranform 5- Inroducion () Sym analyi inpu oupu Dynamic Sym Linar Dynamic ym: A procor which proc h inpu ignal o produc h oupu dy ( n) ( n dy ( n) +
More informationAR(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 informationMidterm exam 2, April 7, 2009 (solutions)
Univrsiy of Pnnsylvania Dparmn of Mahmaics Mah 26 Honors Calculus II Spring Smsr 29 Prof Grassi, TA Ashr Aul Midrm xam 2, April 7, 29 (soluions) 1 Wri a basis for h spac of pairs (u, v) of smooh funcions
More informationDecline 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 informationI) Title: Rational Expectations and Adaptive Learning. II) Contents: Introduction to Adaptive Learning
I) Til: Raional Expcaions and Adapiv Larning II) Conns: Inroducion o Adapiv Larning III) Documnaion: - Basdvan, Olivir. (2003). Larning procss and raional xpcaions: an analysis using a small macroconomic
More informationWave Equation (2 Week)
Rfrnc Wav quaion ( Wk 6.5 Tim-armonic filds 7. Ovrviw 7. Plan Wavs in Losslss Mdia 7.3 Plan Wavs in Loss Mdia 7.5 Flow of lcromagnic Powr and h Poning Vcor 7.6 Normal Incidnc of Plan Wavs a Plan Boundaris
More informationCIVL 8/ D Boundary Value Problems - Quadrilateral Elements (Q4) 1/8
CIVL 8/7111 -D Boundar Vau Prom - Quadriara Emn (Q) 1/8 ISOPARAMERIC ELEMENS h inar rianguar mn and h iinar rcanguar mn hav vra imporan diadvanag. 1. Boh mn ar una o accura rprn curvd oundari, and. h provid
More information4.1 The Uniform Distribution Def n: A c.r.v. X has a continuous uniform distribution on [a, b] when its pdf is = 1 a x b
4. Th Uniform Disribuion Df n: A c.r.v. has a coninuous uniform disribuion on [a, b] whn is pdf is f x a x b b a Also, b + a b a µ E and V Ex4. Suppos, h lvl of unblivabiliy a any poin in a Transformrs
More informationGeneral Article Application of differential equation in L-R and C-R circuit analysis by classical method. Abstract
Applicaion of Diffrnial... Gnral Aricl Applicaion of diffrnial uaion in - and C- circui analysis by classical mhod. ajndra Prasad gmi curr, Dparmn of Mahmaics, P.N. Campus, Pokhara Email: rajndraprasadrgmi@yahoo.com
More informationSpring 2006 Process Dynamics, Operations, and Control Lesson 2: Mathematics Review
Spring 6 Procss Dynamics, Opraions, and Conrol.45 Lsson : Mahmaics Rviw. conx and dircion Imagin a sysm ha varis in im; w migh plo is oupu vs. im. A plo migh imply an quaion, and h quaion is usually an
More informationLecture 2: Current in RC circuit D.K.Pandey
Lcur 2: urrn in circui harging of apacior hrough Rsisr L us considr a capacior of capacianc is conncd o a D sourc of.m.f. E hrough a rsisr of rsisanc R and a ky K in sris. Whn h ky K is swichd on, h charging
More informationTransfer function and the Laplace transformation
Lab No PH-35 Porland Sa Univriy A. La Roa Tranfr funcion and h Laplac ranformaion. INTRODUTION. THE LAPLAE TRANSFORMATION L 3. TRANSFER FUNTIONS 4. ELETRIAL SYSTEMS Analyi of h hr baic paiv lmn R, and
More informationChapter 3: Fourier Representation of Signals and LTI Systems. Chih-Wei Liu
Chapr 3: Fourir Rprsnaion of Signals and LTI Sysms Chih-Wi Liu Oulin Inroducion Complx Sinusoids and Frquncy Rspons Fourir Rprsnaions for Four Classs of Signals Discr-im Priodic Signals Fourir Sris Coninuous-im
More informationOn General Solutions of First-Order Nonlinear Matrix and Scalar Ordinary Differential Equations
saartvlos mcnirbata rovnuli akadmiis moamb 3 #2 29 BULLTN OF TH ORN NTONL DMY OF SNS vol 3 no 2 29 Mahmaics On nral Soluions of Firs-Ordr Nonlinar Mari and Scalar Ordinary Diffrnial uaions uram L Kharaishvili
More informationLecture 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 informationPhys463.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 informationDouble Slits in Space and Time
Doubl Slis in Sac an Tim Gorg Jons As has bn ror rcnly in h mia, a am l by Grhar Paulus has monsra an inrsing chniqu for ionizing argon aoms by using ulra-shor lasr ulss. Each lasr uls is ffcivly on an
More informationRatio-Product Type Exponential Estimator For Estimating Finite Population Mean Using Information On Auxiliary Attribute
Raio-Produc T Exonnial Esimaor For Esimaing Fini Poulaion Man Using Informaion On Auxiliar Aribu Rajsh Singh, Pankaj hauhan, and Nirmala Sawan, School of Saisics, DAVV, Indor (M.P., India (rsinghsa@ahoo.com
More informationH is equal to the surface current J S
Chapr 6 Rflcion and Transmission of Wavs 6.1 Boundary Condiions A h boundary of wo diffrn mdium, lcromagnic fild hav o saisfy physical condiion, which is drmind by Maxwll s quaion. This is h boundary condiion
More informationA THREE COMPARTMENT MATHEMATICAL MODEL OF LIVER
A THREE COPARTENT ATHEATICAL ODEL OF LIVER V. An N. Ch. Paabhi Ramacharyulu Faculy of ahmaics, R D collgs, Hanamonda, Warangal, India Dparmn of ahmaics, Naional Insiu of Tchnology, Warangal, India E-ail:
More informationEXERCISE - 01 CHECK YOUR GRASP
DIFFERENTIAL EQUATION EXERCISE - CHECK YOUR GRASP 7. m hn D() m m, D () m m. hn givn D () m m D D D + m m m m m m + m m m m + ( m ) (m ) (m ) (m + ) m,, Hnc numbr of valus of mn will b. n ( ) + c sinc
More informationCharging of capacitor through inductor and resistor
cur 4&: R circui harging of capacior hrough inducor and rsisor us considr a capacior of capacianc is conncd o a D sourc of.m.f. E hrough a rsisr of rsisanc R, an inducor of inducanc and a y K in sris.
More information2.1. Differential Equations and Solutions #3, 4, 17, 20, 24, 35
MATH 5 PS # Summr 00.. Diffrnial Equaions and Soluions PS.# Show ha ()C #, 4, 7, 0, 4, 5 ( / ) is a gnral soluion of h diffrnial quaion. Us a compur or calculaor o skch h soluions for h givn valus of h
More informationS.Y. B.Sc. (IT) : Sem. III. Applied Mathematics. Q.1 Attempt the following (any THREE) [15]
S.Y. B.Sc. (IT) : Sm. III Applid Mahmaics Tim : ½ Hrs.] Prlim Qusion Papr Soluion [Marks : 75 Q. Amp h following (an THREE) 3 6 Q.(a) Rduc h mari o normal form and find is rank whr A 3 3 5 3 3 3 6 Ans.:
More informationMicroscopic Flow Characteristics Time Headway - Distribution
CE57: Traffic Flow Thory Spring 20 Wk 2 Modling Hadway Disribuion Microscopic Flow Characrisics Tim Hadway - Disribuion Tim Hadway Dfiniion Tim Hadway vrsus Gap Ahmd Abdl-Rahim Civil Enginring Dparmn,
More informationOn Ψ-Conditional Asymptotic Stability of First Order Non-Linear Matrix Lyapunov Systems
In. J. Nonlinar Anal. Appl. 4 (213) No. 1, 7-2 ISSN: 28-6822 (lcronic) hp://www.ijnaa.smnan.ac.ir On Ψ-Condiional Asympoic Sabiliy of Firs Ordr Non-Linar Marix Lyapunov Sysms G. Sursh Kumar a, B. V. Appa
More informationOn the Speed of Heat Wave. Mihály Makai
On h Spd of Ha Wa Mihály Maai maai@ra.bm.hu Conns Formulaion of h problm: infini spd? Local hrmal qulibrium (LTE hypohsis Balanc quaion Phnomnological balanc Spd of ha wa Applicaion in plasma ranspor 1.
More informationCSE 245: Computer Aided Circuit Simulation and Verification
CSE 45: Compur Aidd Circui Simulaion and Vrificaion Fall 4, Sp 8 Lcur : Dynamic Linar Sysm Oulin Tim Domain Analysis Sa Equaions RLC Nwork Analysis by Taylor Expansion Impuls Rspons in im domain Frquncy
More informationDEPARTMENT OF ELECTRICAL &ELECTRONICS ENGINEERING SIGNALS AND SYSTEMS. Assoc. Prof. Dr. Burak Kelleci. Spring 2018
DEPARTMENT OF ELECTRICAL &ELECTRONICS ENGINEERING SIGNALS AND SYSTEMS Aoc. Prof. Dr. Burak Kllci Spring 08 OUTLINE Th Laplac Tranform Rgion of convrgnc for Laplac ranform Invr Laplac ranform Gomric valuaion
More information7.4 QUANTUM MECHANICAL TREATMENT OF FLUCTUATIONS *
Andri Tokmakoff, MIT Dparmn of Chmisry, 5/19/5 7-11 7.4 QUANTUM MECANICAL TREATMENT OF FLUCTUATIONS * Inroducion and Prviw Now h origin of frquncy flucuaions is inracions of our molcul (or mor approprialy
More informationFinal Exam : Solutions
Comp : Algorihm and Daa Srucur Final Exam : Soluion. Rcuriv Algorihm. (a) To bgin ind h mdian o {x, x,... x n }. Sinc vry numbr xcp on in h inrval [0, n] appar xacly onc in h li, w hav ha h mdian mu b
More informationBoyce/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 informationANALYSIS OF VIBRO-IMPACT PROCESSES OF A SINGLE-MASS SYSTEM WITH VISCOUS DAMPING AND A SINGLE LIMITER
Ljubiša Garić hs://doi.org/0.78/tof.4303 ISSN 333-4 ISSN 849-39 NLYSIS OF VIBRO-IMPT PROESSES OF SINGLE-MSS SYSTEM WITH VISOUS MPING N SINGLE LIMITER Summary Th ar rsns an anaysis of h horizona sraigh-in
More informationRevisiting what you have learned in Advanced Mathematical Analysis
Fourir sris Rvisiing wh you hv lrnd in Advncd Mhmicl Anlysis L f x b priodic funcion of priod nd is ingrbl ovr priod. f x cn b rprsnd by rigonomric sris, f x n cos nx bn sin nx n cos x b sin x cosx b whr
More information5. An object moving along an x-coordinate axis with its scale measured in meters has a velocity of 6t
AP CALCULUS FINAL UNIT WORKSHEETS ACCELERATION, VELOCTIY AND POSITION In problms -, drmin h posiion funcion, (), from h givn informaion.. v (), () = 5. v ()5, () = b g. a (), v() =, () = -. a (), v() =
More information1. Inverse Matrix 4[(3 7) (02)] 1[(0 7) (3 2)] Recall that the inverse of A is equal to:
Rfrncs Brnank, B. and I. Mihov (1998). Masuring monary policy, Quarrly Journal of Economics CXIII, 315-34. Blanchard, O. R. Proi (00). An mpirical characrizaion of h dynamic ffcs of changs in govrnmn spnding
More informationFIRST-ORDER SYSTEMS OF ORDINARY DIFFERENTIAL EQUATIONS I: Introduction and Linear Systems
FIRST-ORDER SYSTEMS OF ORDINARY DIFFERENTIAL EQUATIONS I: Inroducion and Linar Sysms David Lvrmor Dparmn of Mahmaics Univrsiy of Maryland 9 Dcmbr 0 Bcaus h prsnaion of his marial in lcur will diffr from
More informationResearch Article Developing a Series Solution Method of q-difference Equations
Appied Mahemaics Voume 2013, Arice ID 743973, 4 pages hp://dx.doi.org/10.1155/2013/743973 Research Arice Deveoping a Series Souion Mehod of q-difference Equaions Hsuan-Ku Liu Deparmen of Mahemaics and
More informationSCHUR S THEOREM REU SUMMER 2005
SCHUR S THEOREM REU SUMMER 2005 1. Combinatorial aroach Prhas th first rsult in th subjct blongs to I. Schur and dats back to 1916. On of his motivation was to study th local vrsion of th famous quation
More informationCPSC 211 Data Structures & Implementations (c) Texas A&M University [ 259] B-Trees
CPSC 211 Daa Srucurs & Implmnaions (c) Txas A&M Univrsiy [ 259] B-Trs Th AVL r and rd-black r allowd som variaion in h lnghs of h diffrn roo-o-laf pahs. An alrnaiv ida is o mak sur ha all roo-o-laf pahs
More informationLogistic equation of Human population growth (generalization to the case of reactive environment).
Logisic quaion of Human populaion growh gnralizaion o h cas of raciv nvironmn. Srg V. Ershkov Insiu for Tim aur Exploraions M.V. Lomonosov's Moscow Sa Univrsi Lninski gor - Moscow 999 ussia -mail: srgj-rshkov@andx.ru
More information( ) ( ) + = ( ) + ( )
Mah 0 Homwork S 6 Soluions 0 oins. ( ps I ll lav i o you vrify ha h omplimnary soluion is : y ( os( sin ( Th guss for h pariular soluion and is drivaivs ar, +. ( os( sin ( ( os( ( sin ( Y ( D 6B os( +
More informationa dt a dt a dt dt If 1, then the poles in the transfer function are complex conjugates. Let s look at f t H t f s / s. So, for a 2 nd order system:
Undrdamd Sysms Undrdamd Sysms nd Ordr Sysms Ouu modld wih a nd ordr ODE: d y dy a a1 a0 y b f If a 0 0, hn: whr: a d y a1 dy b d y dy y f y f a a a 0 0 0 is h naural riod of oscillaion. is h daming facor.
More informationwhereby we can express the phase by any one of the formulas cos ( 3 whereby we can express the phase by any one of the formulas
Third In-Class Exam Soluions Mah 6, Profssor David Lvrmor Tusday, 5 April 07 [0] Th vrical displacmn of an unforcd mass on a spring is givn by h 5 3 cos 3 sin a [] Is his sysm undampd, undr dampd, criically
More informationOn a Class of Two Dimensional Twisted q-tangent Numbers and Polynomials
Inernaiona Maheaica Foru, Vo 1, 17, no 14, 667-675 HIKARI Ld, www-hikarico hps://doiorg/11988/if177647 On a Cass of wo Diensiona wised -angen Nubers and Poynoias C S Ryoo Deparen of Maheaics, Hanna Universiy,
More informationOn the solutions of nonlinear third order boundary value problems
Mahemaica Modeing and Anaysis ISSN: 1392-6292 (Prin) 1648-3510 (Onine) Journa homepage: hps://www.andfonine.com/oi/mma20 On he souions of noninear hird order boundary vaue probems S. Smirnov To cie his
More informationMinistry of Education and Science of Ukraine National Technical University Ukraine "Igor Sikorsky Kiev Polytechnic Institute"
Minisry of Educaion and Scinc of Ukrain Naional Tchnical Univrsiy Ukrain "Igor Sikorsky Kiv Polychnic Insiu" OPERATION CALCULATION Didacic marial for a modal rfrnc work on mahmaical analysis for sudns
More informationAsymptotic Solutions of Fifth Order Critically Damped Nonlinear Systems with Pair Wise Equal Eigenvalues and another is Distinct
Qus Journals Journal of Rsarch in Applid Mahmaics Volum ~ Issu (5 pp: -5 ISSN(Onlin : 94-74 ISSN (Prin:94-75 www.usjournals.org Rsarch Papr Asympoic Soluions of Fifh Ordr Criically Dampd Nonlinar Sysms
More informationInstitute of Actuaries of India
Insiu of Acuaris of India ubjc CT3 Probabiliy and Mahmaical aisics Novmbr Examinaions INDICATIVE OLUTION Pag of IAI CT3 Novmbr ol. a sampl man = 35 sampl sandard dviaion = 36.6 b for = uppr bound = 35+*36.6
More informationUNIT #5 EXPONENTIAL AND LOGARITHMIC FUNCTIONS
Answr Ky Nam: Da: UNIT # EXPONENTIAL AND LOGARITHMIC FUNCTIONS Par I Qusions. Th prssion is quivaln o () () 6 6 6. Th ponnial funcion y 6 could rwrin as y () y y 6 () y y (). Th prssion a is quivaln o
More informationDE Dr. M. Sakalli
DE-0 Dr. M. Sakalli DE 55 M. Sakalli a n n 0 a Lh.: an Linar g Equaions Hr if g 0 homognous non-homognous ohrwis driving b a forc. You know h quaions blow alrad. A linar firs ordr ODE has h gnral form
More informationarxiv: v1 [math.ca] 15 Nov 2016
arxiv:6.599v [mah.ca] 5 Nov 26 Counerexamples on Jumarie s hree basic fracional calculus formulae for non-differeniable coninuous funcions Cheng-shi Liu Deparmen of Mahemaics Norheas Peroleum Universiy
More informationfiziks Institute for NET/JRF, GATE, IIT JAM, JEST, TIFR and GRE in PHYSICAL SCIENCES MATEMATICAL PHYSICS SOLUTIONS are
MTEMTICL PHYSICS SOLUTIONS GTE- Q. Considr an ani-symmric nsor P ij wih indics i and j running from o 5. Th numbr of indpndn componns of h nsor is 9 6 ns: Soluion: Th numbr of indpndn componns of h nsor
More informationCHAPTER CHAPTER14. Expectations: The Basic Tools. Prepared by: Fernando Quijano and Yvonn Quijano
Expcaions: Th Basic Prpard by: Frnando Quijano and Yvonn Quijano CHAPTER CHAPTER14 2006 Prnic Hall Businss Publishing Macroconomics, 4/ Olivir Blanchard 14-1 Today s Lcur Chapr 14:Expcaions: Th Basic Th
More informationVoltage v(z) ~ E(z)D. We can actually get to this wave behavior by using circuit theory, w/o going into details of the EM fields!
Considr a pair of wirs idal wirs ngh >, say, infinily long olag along a cabl can vary! D olag v( E(D W can acually g o his wav bhavior by using circui hory, w/o going ino dails of h EM filds! Thr
More informationSOLUTIONS. 1. Consider two continuous random variables X and Y with joint p.d.f. f ( x, y ) = = = 15. Stepanov Dalpiaz
STAT UIUC Pracic Problms #7 SOLUTIONS Spanov Dalpiaz Th following ar a numbr of pracic problms ha ma b hlpful for compling h homwor, and will lil b vr usful for suding for ams.. Considr wo coninuous random
More information2 Weighted Residual Methods
2 Weighed Residua Mehods Fundamena equaions Consider he probem governed by he differenia equaion: Γu = f in. (83) The above differenia equaion is soved by using he boundary condiions given as foows: u
More informationIntroduction to Fourier Transform
EE354 Signals and Sysms Inroducion o Fourir ransform Yao Wang Polychnic Univrsiy Som slids includd ar xracd from lcur prsnaions prpard y McClllan and Schafr Licns Info for SPFirs Slids his work rlasd undr
More informationXV Exponential and Logarithmic Functions
MATHEMATICS 0-0-RE Dirnial Calculus Marin Huard Winr 08 XV Eponnial and Logarihmic Funcions. Skch h graph o h givn uncions and sa h domain and rang. d) ) ) log. Whn Sarah was born, hr parns placd $000
More informationChapter 12 Introduction To The Laplace Transform
Chapr Inroducion To Th aplac Tranorm Diniion o h aplac Tranorm - Th Sp & Impul uncion aplac Tranorm o pciic uncion 5 Opraional Tranorm Applying h aplac Tranorm 7 Invr Tranorm o Raional uncion 8 Pol and
More informationMath 3301 Homework Set 6 Solutions 10 Points. = +. The guess for the particular P ( ) ( ) ( ) ( ) ( ) ( ) ( ) cos 2 t : 4D= 2
Mah 0 Homwork S 6 Soluions 0 oins. ( ps) I ll lav i o you o vrify ha y os sin = +. Th guss for h pariular soluion and is drivaivs is blow. Noi ha w ndd o add s ono h las wo rms sin hos ar xaly h omplimnary
More information( ) 2! l p. Nonlinear Dynamics for Gear Fault Level. ( ) f ( x) ( ),! = sgn % " p. Open Access. Su Xunwen *,1, Liu Jinhao 1 and Wang Shaoping 2. !
Nonlinar Dynamics for Gar Faul Lvl Su Xunwn Liu Jinhao and Wang Shaoping Snd Ordrs for Rprins o rprins@bnhamscinc.a Th Opn Mchanical Enginring Journal 04 8 487496 487 Opn Accss School of Tchnology Bijing
More informationThe model proposed by Vasicek in 1977 is a yield-based one-factor equilibrium model given by the dynamic
h Vsick modl h modl roosd by Vsick in 977 is yild-bsd on-fcor quilibrium modl givn by h dynmic dr = b r d + dw his modl ssums h h shor r is norml nd hs so-clld "mn rvring rocss" (undr Q. If w u r = b/,
More informationUNSTEADY FLOW OF A FLUID PARTICLE SUSPENSION BETWEEN TWO PARALLEL PLATES SUDDENLY SET IN MOTION WITH SAME SPEED
006-0 Asian Rsarch Publishing work (ARP). All righs rsrvd. USTEADY FLOW OF A FLUID PARTICLE SUSPESIO BETWEE TWO PARALLEL PLATES SUDDELY SET I MOTIO WITH SAME SPEED M. suniha, B. Shankr and G. Shanha 3
More informationA MATHEMATICAL MODEL FOR NATURAL COOLING OF A CUP OF TEA
MTHEMTICL MODEL FOR NTURL COOLING OF CUP OF TE 1 Mrs.D.Kalpana, 2 Mr.S.Dhvarajan 1 Snior Lcurr, Dparmn of Chmisry, PSB Polychnic Collg, Chnnai, India. 2 ssisan Profssor, Dparmn of Mahmaics, Dr.M.G.R Educaional
More informationRelation between Fourier Series and Transform
EE 37-3 8 Ch. II: Inro. o Sinls Lcur 5 Dr. Wih Abu-Al-Su Rlion bwn ourir Sris n Trnsform Th ourir Trnsform T is riv from h finiion of h ourir Sris S. Consir, for xmpl, h prioic complx sinl To wih prio
More informationNumerical 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 informationChap.3 Laplace Transform
Chap. aplac Tranorm Tranorm: An opraion ha ranorm a uncion ino anohr uncion i Dirniaion ranorm: ii x: d dx x x Ingraion ranorm: x: x dx x c Now, conidr a dind ingral k, d,ha ranorm ino a uncion o variabl
More informationNikesh Bajaj. Fourier Analysis and Synthesis Tool. Guess.? Question??? History. Fourier Series. Fourier. Nikesh Bajaj
Guss.? ourir Analysis an Synhsis Tool Qusion??? niksh.473@lpu.co.in Digial Signal Procssing School of Elcronics an Communicaion Lovly Profssional Univrsiy Wha o you man by Transform? Wha is /Transform?
More informationt 2 B F x,t n dsdt t u x,t dxdt
Evoluion Equaions For 0, fixed, le U U0, where U denoes a bounded open se in R n.suppose ha U is filled wih a maerial in which a conaminan is being ranspored by various means including diffusion and convecion.
More informationA HAMILTON-JACOBI TREATMENT OF DISSIPATIVE SYSTEMS
Europan Scinific Journal Ocobr 13 diion vol9, No3 ISSN: 1857 7881 (Prin) - ISSN 1857-7431 A AMILTON-JACOBI TREATMENT OF DISSIPATIVE SYSTEMS Ola A Jarab'ah Tafila Tchnical Univrsiy, Tafila, Jordan Khald
More informationMundell-Fleming I: Setup
Mundll-Flming I: Sup In ISLM, w had: E ( ) T I( i π G T C Y ) To his, w now add n xpors, which is a funcion of h xchang ra: ε E P* P ( T ) I( i π ) G T NX ( ) C Y Whr NX is assumd (Marshall Lrnr condiion)
More informationExistence of positive solution for a third-order three-point BVP with sign-changing Green s function
Elecronic Journal of Qualiaive Theory of Differenial Equaions 13, No. 3, 1-11; hp://www.mah.u-szeged.hu/ejqde/ Exisence of posiive soluion for a hird-order hree-poin BVP wih sign-changing Green s funcion
More informationy = 2xe x + x 2 e x at (0, 3). solution: Since y is implicitly related to x we have to use implicit differentiation: 3 6y = 0 y = 1 2 x ln(b) ln(b)
4. y = y = + 5. Find th quation of th tangnt lin for th function y = ( + ) 3 whn = 0. solution: First not that whn = 0, y = (1 + 1) 3 = 8, so th lin gos through (0, 8) and thrfor its y-intrcpt is 8. y
More informationDISTRIBUTION OF DIFFERENCE BETWEEN INVERSES OF CONSECUTIVE INTEGERS MODULO P
DISTRIBUTION OF DIFFERENCE BETWEEN INVERSES OF CONSECUTIVE INTEGERS MODULO P Tsz Ho Chan Dartmnt of Mathmatics, Cas Wstrn Rsrv Univrsity, Clvland, OH 4406, USA txc50@cwru.du Rcivd: /9/03, Rvisd: /9/04,
More informationLaPlace Transform in Circuit Analysis
LaPlac Tranform in Circui Analyi Obciv: Calcula h Laplac ranform of common funcion uing h dfiniion and h Laplac ranform abl Laplac-ranform a circui, including componn wih non-zro iniial condiion. Analyz
More informationComputational prediction of high ZT of n-type Mg 3 Sb 2 - based compounds with isotropic thermoelectric conduction performance
Elcronic Supplnary Marial (ES for Physical Chisry Chical Physics. This journal is h Ownr Sociis 08 Supporing nforaion Copuaional prdicion of high ZT of n-yp Mg 3 Sb - basd copounds wih isoropic hrolcric
More informationDifference -Analytical Method of The One-Dimensional Convection-Diffusion Equation
Diffrnc -Analytical Mthod of Th On-Dimnsional Convction-Diffusion Equation Dalabav Umurdin Dpartmnt mathmatic modlling, Univrsity of orld Economy and Diplomacy, Uzbistan Abstract. An analytical diffrncing
More informationPart 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 informationCHAPTER. Linear Systems of Differential Equations. 6.1 Theory of Linear DE Systems. ! Nullcline Sketching. Equilibrium (unstable) at (0, 0)
CHATER 6 inar Sysms of Diffrnial Equaions 6 Thory of inar DE Sysms! ullclin Skching = y = y y υ -nullclin Equilibrium (unsabl) a (, ) h nullclin y = υ nullclin = h-nullclin (S figur) = + y y = y Equilibrium
More informationAsymptotic instability of nonlinear differential equations
Elecronic Journal of Differenial Equaions, Vol. 1997(1997), No. 16, pp. 1 7. ISSN: 172-6691. URL: hp://ejde.mah.sw.edu or hp://ejde.mah.un.edu fp (login: fp) 147.26.13.11 or 129.12.3.113 Asympoic insabiliy
More informationUnpriced Quality. Pascal Courty 1. September 2010
npricd Quaiy Pasca Coury Spmbr 200 Absrac: A monopois dibray chargs h sam pric for diffrniad producs whn high uaiy producs ar mor iky o b assignd o ow vauaion consumrs undr uniform pricing. Th argumn can
More informationApplied Statistics and Probability for Engineers, 6 th edition October 17, 2016
Applid Saisics and robabiliy for Enginrs, 6 h diion Ocobr 7, 6 CHATER Scion - -. a d. 679.. b. d. 88 c d d d. 987 d. 98 f d.. Thn, = ln. =. g d.. Thn, = ln.9 =.. -7. a., by symmry. b.. d...6. 7.. c...
More informationCopyright 2012 Pearson Education, Inc. Publishing as Prentice Hall.
Chapr Rviw 0 6. ( a a ln a. This will qual a if an onl if ln a, or a. + k an (ln + c. Thrfor, a an valu of, whr h wo curvs inrsc, h wo angn lins will b prpnicular. 6. (a Sinc h lin passs hrough h origin
More informationFourier Transforms and the Wave Equation. Key Mathematics: More Fourier transform theory, especially as applied to solving the wave equation.
Lur 7 Fourir Transforms and th Wav Euation Ovrviw and Motivation: W first discuss a fw faturs of th Fourir transform (FT), and thn w solv th initial-valu problm for th wav uation using th Fourir transform
More informationConsider a system of 2 simultaneous first order linear equations
Soluon of sysms of frs ordr lnar quaons onsdr a sysm of smulanous frs ordr lnar quaons a b c d I has h alrna mar-vcor rprsnaon a b c d Or, n shorhand A, f A s alrady known from con W know ha h abov sysm
More informationFeedback Control and Synchronization of Chaos for the Coupled Dynamos Dynamical System *
ISSN 746-7659 England UK Jornal of Informaion and Comping Scinc Vol. No. 6 pp. 9- Fdbac Conrol and Snchroniaion of Chaos for h Copld Dnamos Dnamical Ssm * Xdi Wang Liin Tian Shmin Jiang Liqin Y Nonlinar
More informationImpulsive Differential Equations. by using the Euler Method
Applid Mahmaical Scincs Vol. 4 1 no. 65 19 - Impulsiv Diffrnial Equaions by using h Eulr Mhod Nor Shamsidah B Amir Hamzah 1 Musafa bin Mama J. Kaviumar L Siaw Chong 4 and Noor ani B Ahmad 5 1 5 Dparmn
More informationPoisson process Markov process
E2200 Quuing hory and lraffic 2nd lcur oion proc Markov proc Vikoria Fodor KTH Laboraory for Communicaion nwork, School of Elcrical Enginring 1 Cour oulin Sochaic proc bhind quuing hory L2-L3 oion proc
More informationNEW APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA
NE APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA Mirca I CÎRNU Ph Dp o Mathmatics III Faculty o Applid Scincs Univrsity Polithnica o Bucharst Cirnumirca @yahoocom Abstract In a rcnt papr [] 5 th indinit intgrals
More information