SECOND DEGRE (Partie 2)
Yvan Monka – Académie de Strasbourg – www.maths-et-tiques.fr. SECOND DEGRE (Partie 2). I. Résolution d'une équation du second degré.
Seconde Cours résolution déquations - I. Résolution algébrique
Exemple : 6 est solution de l'équation 2 + x = 8 car l'égalité 2 + 6 = 8 est vraie. c) Résolution algébrique d'une équation. Règle du produit nul : Un produit
ÉQUATIONS INÉQUATIONS
Yvan Monka – Académie de Strasbourg – www.maths-et-tiques.fr. ÉQUATIONS INÉQUATIONS Méthode : Vérifier si un nombre est solution d'une équation.
Second degré : Résumé de cours et méthodes 1 Définitions : 2
Résolution dans R de l'équation x2 +2x?3 = 0 : (Par rapport aux formules on a ici : a = 1
RÉSOLUTION DE SYSTÈMES À DEUX INCONNUES
Quoique la première équation du système soit satisfaite la seconde ne l'est pas. Rappelons que
Chapter 5 - Differential equations
The solution u = A cos ct + B sin ct contains two arbitrary constants and is the general solution of the second order ODE ¨u+c2u = 0. This illustrates the fact
SECOND DEGRE (Partie 2)
Yvan Monka – Académie de Strasbourg – www.maths-et-tiques.fr. SECOND DEGRE (Partie 2). I. Résolution d'une équation du second degré.
OSCILLATION OF SOLUTION TO SECOND-ORDER HALF-LINEAR
Mar 15 2016 ftp ejde.math.txstate.edu. OSCILLATION OF SOLUTION TO SECOND-ORDER. HALF-LINEAR DELAY DYNAMIC EQUATIONS. ON TIME SCALES.
Second order linear equations
Solution: given by y = 9 exp(?2t) ? 7 exp(?3t). Graph of solution: Samy T. Second order equations. Differential equations. 11 / 115. Page 12. Example 2.
Math 215 HW #1 Solutions
Solution: We can plug the third equation u+w = 2
Second order linear equations
Samy Tindel
Purdue University
Differential equations - MA 266
Taken fromElementary differential equations
by Boyce and DiPrima Samy T.Second order equationsDifferential equations 1 / 115Outline
1Homogeneous equations with constant coefficients
2Homogeneous equations and Wronskian
3Complex roots of the characteristic equation
4Repeated roots, reduction of order
5Nonhomogeneous equations
6Variation of parameters
7Mechanical vibrations
8Forced vibrations
Samy T.Second order equationsDifferential equations 2 / 115Second order differential equations
General form of equation:
d 2ydt 2=f? t,y,dydt Importance of second order equations:1Instructive methods of resolution2Crucial for modeling in physics:
IFluid mechanics
IHeat transfer
IWave motion
IElectromagnetismSamy T.Second order equationsDifferential equations 3 / 115Outline
1Homogeneous equations with constant coefficients
2Homogeneous equations and Wronskian
3Complex roots of the characteristic equation
4Repeated roots, reduction of order
5Nonhomogeneous equations
6Variation of parameters
7Mechanical vibrations
8Forced vibrations
Samy T.Second order equationsDifferential equations 4 / 115General form of 2nd order linear equation
General form 1:
y ??+p(t)y?+q(t)y=g(t)General form 2:
P(t)y??+Q(t)y?+R(t)y=G(t)
Remark:
2 forms are equivalent ifP(t)?=0
Initial condition:Given byy(t0) =y0andy?(t0) =y?0Two conditions necessary because two integrations performed
Samy T.Second order equationsDifferential equations 5 / 115Homogeneous linear equations
Homogeneous equations:
When g≡0, that is
y ??+p(t)y?+q(t)y=0Remark:
Nonhomogeneous solutions can be deduced from homogeneous onesHomogeneous equations with constant coefficients:
ay ??+by?+cy=0, fora,b,c?R.Samy T.Second order equationsDifferential equations 6 / 115Simple example
Equation:
y ??-y=0.(1)Initial condition:
y(0) =2,andy?(0) =-1.Two simple functions satisfying (1):
y=exp(t),andy=exp(-t).Using linear form of (1):
fo rc1,c2?R, y=c1exp(t) +c2exp(-t). is solution to the equation. Samy T.Second order equationsDifferential equations 7 / 115Simple example (2)
First conclusion:
We obtain an infinite family of solutions indexed byc1,c2.Initial value problem:
with y(0) =2 andy?(0) =-1 we find ?c1+c2=2
c1-c2=-1
Solution:c1=12
andc2=32Solution to initial value problem:
y=12 exp(t) +32 exp(-t).Samy T.Second order equationsDifferential equations 8 / 115Generalization
Equation considered:
fo ra,b,c?R, ay ??+by?+cy=0.(2)Characteristic equation:
ar2+br+c=0.
Hypothesis:
Characteristic equation has 2 distinct real rootsr1,r2.Conclusion:
general solution to (2) given b y: y=c1exp(r1t) +c2exp(r2t).(3)Proposition 1. Samy T.Second order equationsDifferential equations 9 / 115Generalization: initial value
Initial value problem:
under assumptions of Prop osition1, ay ??+by?+cy=0,y(t0) =y0,y?(t0) =y?0.(4)Solution to (4):
given b y y=c1exp(r1t) +c2exp(r2t), with c1=y?0-y0r2r
1-r2exp(-r1t0),c2=y?0-y0r1r
2-r1exp(-r2t0)Samy T.Second order equationsDifferential equations 10 / 115
Example 1
Equation considered:
y ??+5y?+6y=0y(0) =2,y?(0) =3.(5)Solution:
given b y y=9exp(-2t)-7exp(-3t)Graph of solution:
Samy T.Second order equationsDifferential equations 11 / 115Example 2
Equation considered:
4y??-8y?+3y=0y(0) =2,y?(0) =12
Solution:
given b y y=-12 exp?3t2 +52exp?t2
Graph of solution:
Samy T.Second order equationsDifferential equations 12 / 115Asymptotic behavior of solutions
3 cases:
under assumptions of Prop osition1, 1If bothr1,r2<0, then limt→∞y(t) =02Ifr1>0 orr2>0, exponential growth fory3Ifr1<0 andr2=0, then limt→∞y(t) =??RSamy T.Second order equationsDifferential equations 13 / 115
Outline
1Homogeneous equations with constant coefficients
2Homogeneous equations and Wronskian
3Complex roots of the characteristic equation
4Repeated roots, reduction of order
5Nonhomogeneous equations
6Variation of parameters
7Mechanical vibrations
8Forced vibrations
Samy T.Second order equationsDifferential equations 14 / 115Definition of an operator
LetI= (α,β), that is
We defineL[φ] :I→Rby:
L[φ] =φ??+pφ?+qφDefinition 2.
Samy T.Second order equationsDifferential equations 15 / 115Homogeneous equation in terms ofL
Equation considered:
Under conditions of Definition 2,
L[y] =0??y??+py?+qy=0
Initial conditions:
fo rt0?I, y(t0) =y0,andy?(t0) =y?0.Samy T.Second order equationsDifferential equations 16 / 115Existence and uniqueness theorem
General linear equation:
y ??+p(t)y?+q(t)y=g(t),y(t0) =y0,y?(t0) =y?0.(6)Hypothesis:t
0?I, whereI= (α,β).p,qandgcontinuous onI.
Conclusion:
There exists a unique functionysatisfying equation (6) onI.Theorem 3. Samy T.Second order equationsDifferential equations 17 / 115Existence and uniqueness theorem (2)
Important conclusions of the theorem:1There exists a solution to (6).2There is only one solution.
3The solutionyis defined and twice differentiable onI.
Back to equation (5):We had existence part.
Uniqueness is harder to see.
Major difference with first order equations:No general formula for solution to (6). Samy T.Second order equationsDifferential equations 18 / 115Example of maximal interval
Equation considered:
?t2-3t?y??+t y?-(t+3)y=0,y(1) =2,y?(1) =1.Equivalent form:
y ??+1t-3y?+t+3t(t-3)y=0,y(1) =2,y?(1) =1.Application of Theorem 3:g(t) =0 continuous onRp(t) =1t-3continuous on(-∞,3)?(3,∞)q(t) =t+3t(t-3)continuous on(-∞,0)?(0,3)?(3,∞)1?(0,3)
We thus get unique solution on(0,3)Samy T.Second order equationsDifferential equations 19 / 115A trivial example of equation
Equation considered:
y ??+p(t)y?+q(t)y=0,y(t0) =0,y?(t0) =0Hypothesis:pandqcontinuous onIt
0?IApplication of Theorem 3:1y≡0 solves equation.2According to Theorem 3 it is the unique solution.
Samy T.Second order equationsDifferential equations 20 / 115Principle of superposition
Equation considered:
y ??+p(t)y?+q(t)y=0.(7)Hypothesis:y
1andy2are 2 solutions to equation (7).c
1andc2are 2 constants.
Conclusion:
y=c1y1+c2y2also solves (7).Theorem 4.Additional question:
Are all the solutions of the formy=c1y1+c2y2?Samy T.Second order equationsDifferential equations 21 / 115
Proof of Theorem 4
Step 1:
p rovethatL[c1y1+c2y2] =c1L[y1] +c2L[y2].
Step 2:
W eobtain
L[y1] =0,L[y2] =0=?L[c1y1+c2y2] =0.Samy T.Second order equationsDifferential equations 22 / 115Wronskian
Consider:
Equationy??+p(t)y?+q(t)y=0.Two solutionsy1,y2on intervalI.t 0?I.The Wronskian fory1,y2att0is:
W=W[y1,y2](t0) =?
????y1(t0)y2(t0)
y ?1(t0)y?2(t0)? ????.Definition 5. Samy T.Second order equationsDifferential equations 23 / 115Wronskian and determination of solutions
Equation:
back to (6) tha tisL[y] =y??+p(t)y?+q(t)y=0.
Hypothesis:Existence of two solutionsy1,y2.Initial conditiony(t0) =y0andy?(t0) =y?0assigned.Conclusion:
One can find c1,c2such that
y=c1y1+c2y2 satisfies (6) with initial condition iffW[y1,y2](t0)?=0Theorem 6.
Samy T.Second order equationsDifferential equations 24 / 115Complement to Theorem 6
Expression forc1,c2:Under assumptions of Theo rem6 w ehave c 1=? ????y0y2(t0)
y ?0y?2(t0)? ????y1(t0)y2(t0)
y ?1(t0)y?2(t0)? ????,andc2=? ????y1(t0)y0
y ?1(t0)y?0? ????y1(t0)y2(t0)
y ?1(t0)y?2(t0)?Justification:c1,c2are solution to the system
?c1y1(t0) +c2y2(t0) =y0
c1y?1(t0) +c2y?2(t0) =y?0Samy T.Second order equationsDifferential equations 25 / 115
Example 1
Equation considered:
back to (5), that is y ??+5y?+6y=0.2 solutions:
given b y y1=exp(-2t),andy2=exp(-3t)
Expression of Wronskian:
fo rt?R,W[y1,y2](t) =exp(-5t).
Solving the equation:W[y1,y2](t)?=0 for allt?R
=?initial value problem can be solved at anyt?R.Samy T.Second order equationsDifferential equations 26 / 115
Wronskian and uniqueness of solutions
Equation:
back to (6) tha tisL[y] =y??+p(t)y?+q(t)y=0.
Hypothesis:Existence of two solutionsy1,y2.
Conclusion:
The general solution
y=c1y1+c2y2,withc1,c2?R includes all solutions to (6) iff: there existst0?Isuch thatW[y1,y2](t0)?=0.Theorem 7. Samy T.Second order equationsDifferential equations 27 / 115Example: equations with constant coefficients
Equation considered:
fo ra,b,c?R, ay ??+by?+cy=0.(8)quotesdbs_dbs47.pdfusesText_47[PDF] maths 3 eme merciii
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