Schroers D.B.J.-Ordinary Differential Equations a Practical Guide-Cambridge University Press (2011)

Schroers D.B.J.-Ordinary Differential Equations a Practical Guide-Cambridge University Press (2011)

9781107697492book CUP/SCHL3 August 25, 2011 19:15 Page-1 1 First order di↵erential equations 1.1 General remarks about di↵erential equations 1.1.1 Terminology A di↵erential equation is an equation involving a function and its derivatives. An example which we will study in detail in this book is the pendulum equation d2x = sin(x), (1.1) dt2 − which is a di↵erential equation for a real-valued function x of one real variable t. The equation expresses the equality of two functions. To make this clear we could write (1.1) more explicitly as d2x (t)= sin(x(t)) for all t R, dt2 − 2 but this would lead to very messy expressions in more complicated equations. We therefore often suppress the independent variable. When formulating a mathematical problem involving an equa- tion, we need to specify where we are supposed to look for solu- tions. For example, when looking for a solution of the equation x2 + 1 = 0 we might require that the unknown x is a real number, in which case there is no solution, or we might allow x to be com- plex, in which case we have the two solutions x = i. In trying ± to solve the di↵erential equation (1.1) we are looking for a twice- di↵erentiable function x : R R. The set of all such functions is ! very big (bigger than the set of all real numbers, in a sense that can be made precise by using the notion of cardinality), and this 1 9781107697492book CUP/SCHL3 August 25, 2011 19:15 Page-2 2 First order di↵erential equations is one basic reason why, generally speaking, finding solutions of di↵erential equations is not easy. Di↵erential equations come in various forms, which can be clas- sified as follows. If only derivatives of the unknown function with respect to one variable appear, we call the equation an ordinary di↵erential equation, or ODE for short. If the function depends on several variables, and if partial derivatives with respect to at least two variables appear in the equation, we call it a partial di↵eren- tial equation, or PDE for short. In both cases, the order of the di↵erential equation is the order of the highest derivative occur- ring in it. The independent variable(s) may be real or complex, and the unknown function may take values in the real or complex numbers, or in Rn of Cn for some positive integer n. In the lat- ter case we can also think of the di↵erential equation as a set of di↵erential equations for each of the n components. Such a set is called a system of di↵erential equations of dimension n. Finally we note that there may be parameters in a di↵erential equation, which play a di↵erent role from the variables. The di↵erence be- tween parameters and variables is usually clear from the context, but you can tell that something is a parameter if no derivatives with respect to it appear in the equation. Nonetheless, solutions still depend on these parameters. Examples illustrating the terms we have just introduced are shown in Fig. 1.1. In this book we are concerned with ordinary di↵erential equa- tions for functions of one real variable and, possibly, one or more parameters. We mostly consider real-valued functions but complex- valued functions also play an important role. 1.1.2 Approaches to problems involving di↵erential equations Many mathematical models in the natural and social sciences in- volve di↵erential equations. Di↵erential equations also play an important role in many branches of pure mathematics. The fol- lowing system of ODEs for real-valued functions a, b and c of one 1.1 General remarks about di↵erential equations 3 1.1 General remarks about di↵erential equations 3 usually clear from the context, but you can tell that some- 1.1 General remarksusuathingllyabcilearouts a difrpomarame↵erenthetiteraconl eifqutext,natoionderivbuts yativou3 cesanwtellith thatrespseome-ct to it thingappearis ainparamethe eqteruationif n. oNonethelesderivativess, soluwithtionsrespwillect tostilitl de- usually clear from theappconeartext,in thebuteqyuationou can. Nonethelestell that some-s, solutions will still de- 9781107697492book CUP/SCHL3pe Augustnd on 25,these 2011parame 19:15ters. Page-3 thing is a parameterpenifd nono thderiveseativparesamewters.ith respect to it appear in the equation. Nonetheless, solutions will still de- pend on these parameExters.ample 1.1 Exdyample 1.1 1.1 General remarks aboutdy di↵erentialxy = 0 equationsis a 1st order3ODE. dx −xy = 0 is a 1st order ODE. Example 1.1 dx − 1.1 General remarks about di↵erentidual equationdvs 3 dy du = vdv, = u xy = 0 is a 1st1.1ordtG=derenervODE.−,al rdemarks=t u about di↵erential equations 3 these parameters. Exampdx − les illustrat1.1ingGdtentheer−nomenclatural remarksdt eabout di↵erential equations 3 are shown in Fig. 1.1.firstdu order ordinaryusuadv firstlly ordercisleara systemsysfromtem ofthe of ordinary1stconor text,der, dimensionbut you ctwo.an tell that some- differential= equationv, = uisdifferentialisa sysa systemtem equations,of 1stof 1st order,order,dimensiondimensiontwo. 1.1 Gendteral−remarksusuadtllyabclearout difrom↵erenthetiaconl equtext,ationbuts you3 can tell that some- 1.1 General remarksthing abis outa2dimensionpdiarame↵eren twotertialifequnoatiderivons ativ3es with respect to it two. d y dy 3 thingappearis adin2yparamethe=dye(qteruation) ifisn.aoNonetheles2ndderivorderativODE.ess, soluwithtionsrespwillect tostilitl de- usuausuallyllyclearclearfromfromthetheconcontext,text,dxb=utb2ut(yyououdx)3ciscananatell2ndtellthatorthatderssODE.ome-ome- 2 2 appear3 in the2 equation. Nonetheless, solutions will still de- d yd y dy dy3pend ondxthese2 dxparame2 ters. thingthingis ias aparamep2arame= (=terter) ifisifnaon2ndoderivderiv1or@derativativu ODE.eses@wwuithithrreespspeectct toto itit dxdx2 dxpedxnd on th1 e@se2upar=@ame2u ters.is a 2nd order PDE, with parameter c. appappearearininthetheeqeuationquation . .NonethelesNonethelesc2 @t=2s,s,solusolu@xtionsis2tionsa 2ndwillwillorderstilstillPlde-DE,de- with parameter c. 1 @2u @2Exu amplec2 @t1.2 1 @x2 pepnednond onththesecondseesepar parorder=ameame ordinaryters.ters.is a 2nd order PDE, with parameter c. c2 @t2 Ex@xdy2ample second1.In1this ordercour partialse w e are only concerned with ordinary di↵eren- differential equation Indifferentialthis cour equationse we are only concerned with ordinary di↵eren- dy xy tial= 0equis ationsa 1st fororderfunctionODE.s of a real variable and, in some dx −xy tial= with0equis parameterationsa 1st orfor cderfunctionODE.s of a real variable and, in some ExampleIn1.th1is courdxse we are oncaslyesconce, onernedor morewith orparametedinary dris↵.erWene- will consider systems Example 1.1 du− cases,dvone or more parameters. We will consider systems dydy tial equations for functionand shighof aerrealordervariabequationle ansd,anindswomeill allow the functions to xy = 0 is a 1stdu order= andODE.vdv, high=er oru der equations and will allow the functions to dx −xy =casFig.0 ises 1.1.,aon1st Terminologye orordt=moreder vODE.− for,parameteb die↵dcomerential=t uprsle. equationsxW-value willed. consider systems dx − dt − bedcomt plex-valued. du anddvhigher order equations and will allow the functions to firstdu order= ordinarv, dvy =firstu orisdera systemsystem of of ordinar1st ory der, dimension two. differrealential= variable equationv,bercomarises=pleuis inxdiff-isv diaalu↵ersysaerentialentialedsystemt.em equations, geometry:of 1stof 1st order,order,dimensiondimensiontwo. dtdt −− dtdt 2dimension two two. da d y 1 2dy 3 1.1.2 2 Approaches to problems involving is a system of 1st dor2=der,y dimension=(dya( ()b1.1.isctwo.)2a) 2ndApproroacheder ODE.s to problems involving dr dx22rc dx−3 − di↵erential equations 2 2 = ( ) is a 2nd orderdiODE.↵erential equations d y dy db dx b dx2 2 d2=y ( dy)3 is a1.1.2nd2=1orAppr@der2uoODE.(achebMan@2(sauytomco)pdelsr)oblaremisisnginvolviin thengnatural and social sciences are dx2 =dx( )3 is dra 2nd 2or2acrderManODE.2−y m−odels arising in the natural and social sciences are 2 dc 1 @2 u1 2 =di@b↵euster2exprentialis eass2ndedequationsinortermsder PofDE,di↵ewreinthtialparequatiameterons.c.Di↵eren- dx dx =c @t=(bc2est@(exprxais bea)ss22nd)ed, inortermsder PofDE,di↵ewreitnhtialparequatiameterons.c.Di↵eren- 1 @2u @2u dr c2 @t22ra @tial−x2 equ− ations also arise in many branches of pure mathe- second1 @ or2u=der orMan@dinar2uisy yma o2nddels arorisderingtialPinDE,equtheationnatuwithsralpalsoaranameterdarisesocialincms.cieannycesbrancarehes of pure mathe- cdiff2 One@ertential2 is looking =equation@x2 for is solutionsa 2ndsecondIn thor onis deror thecourdermaticsP interval parDE,setialw. w eThe [⇡iaret,h pfollo)onar subjectameterlywinconceg tosyc thesr.temnedofwithODEorsdifornarythedreal-vi↵erealuedn- c2 @t2 b@estx2expreInssdiffedtherisinentialcourtermsmatics equationseofw.edTheiare↵ erefolloon1ntilyalwinconceequatig syrsons.temned ofDiwith↵ODEerorensdi- fornarythedreal-vi↵erealuedn- initial conditions tial equationsfunctionfors a,functionb and c sofofonae rrealeal vvariariabableler ariansd,es inin disome↵eren- tial equationtialwiths equalso parameterationsarisefunctioninfor cms a,anfunctionbyanbrdanccsofhofesonofae realrpeureal vvarimathe-ariabableler anarid,sesinin sdiome↵eren- InInthisthiscourcourmaticssesweaew(⇡.aree)=0Theareon,bcasonfollolylyes(conce⇡win,)=conceong⇡er,csnedyrorsnedtem(⇡morewith)=withof ODE⇡orparameteor. didisnarynaryfor thdrdiesi↵.↵real-veerWreenne--aluedwill consider systems cases, one or more paramete− rs. We will consider systems tialtialequequationsationsfunctionforforfsunctionfa,unctionbandandshighcsofofofaeonrarealeorrealrderealvariabvvariabeariquationableleleanranarisd,d,ansinesindinsswomeomediill↵alloeren-w

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