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Lesson 95 — 2nd-order linear ODEs with constant coefficients

ay'' + by' + cy = 0. Characteristic equation and three regimes: distinct real roots, repeated real root, complex conjugate roots.

Used in: Spécialité Maths (France, Terminale) · Math III japonês (avançado) · Leistungskurs alemão Klasse 12

ay+by+cy=0    aλ2+bλ+c=0ay'' + by' + cy = 0 \;\Longrightarrow\; a\lambda^2 + b\lambda + c = 0
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Rigorous notation, full derivation, hypotheses

Characteristic equation — three cases

General problem

Ansatz and characteristic equation

Substitute y=eλxy = e^{\lambda x}: y=λeλxy' = \lambda e^{\lambda x}, y=λ2eλxy'' = \lambda^2 e^{\lambda x}.

aλ2eλx+bλeλx+ceλx=0    aλ2+bλ+c=0a\lambda^2 e^{\lambda x} + b\lambda e^{\lambda x} + c e^{\lambda x} = 0 \;\Rightarrow\; a\lambda^2 + b\lambda + c = 0

Since eλx0e^{\lambda x} \neq 0, everything reduces to the quadratic algebraic equation.

"If b24ac>0b^2 - 4ac > 0, the characteristic equation has two distinct real roots r1,r2r_1, r_2, and the general solution of [the ODE] is y=c1er1x+c2er2xy = c_1 e^{r_1 x} + c_2 e^{r_2 x}." — Lebl, Notes on Diffy Qs, §2.2

The repeated root case

Qualitative diagram — behavior by case

Case 1: distinct realCase 2: repeated rootCase 3: complex

Qualitative profiles: case 1 (pure exponential), case 2 (critical boundary), case 3 (oscillatory).

Non-homogeneous equations

For ay+by+cy=q(x)ay'' + by' + cy = q(x): general solution y=yh+ypy = y_h + y_p.

yhy_h: solution to the homogeneous equation (two free parameters).

ypy_p: any particular solution — obtained by undetermined coefficients (when qq is a combination of polynomials, exponentials, sines/cosines) or variation of parameters (general).

Solved examples

Exercise list

30 exercises · 7 with worked solution (25%)

Application 18Understanding 3Modeling 4Challenge 3Proof 2
  1. Ex. 95.1Application

    Solve y3y+2y=0y'' - 3y' + 2y = 0.

  2. Ex. 95.2Application

    Solve y+4y+4y=0y'' + 4y' + 4y = 0.

  3. Ex. 95.3ApplicationAnswer key

    Solve y+9y=0y'' + 9y = 0.

  4. Ex. 95.4Application

    Solve y+2y+10y=0y'' + 2y' + 10y = 0.

  5. Ex. 95.5Application

    Solve y+4y+3y=0y'' + 4y' + 3y = 0, y(0)=1y(0) = 1, y(0)=0y'(0) = 0.

  6. Ex. 95.6Application

    Solve y2y+y=0y'' - 2y' + y = 0, y(0)=2y(0) = 2, y(0)=1y'(0) = -1.

  7. Ex. 95.7Application

    Solve y+4y=0y'' + 4y = 0, y(0)=0y(0) = 0, y(0)=1y'(0) = 1.

  8. Ex. 95.8Application

    Solve yy6y=0y'' - y' - 6y = 0.

  9. Ex. 95.9Application

    Solve y+2y+5y=0y'' + 2y' + 5y = 0.

  10. Ex. 95.10ApplicationAnswer key

    Solve y+6y+9y=0y'' + 6y' + 9y = 0.

  11. Ex. 95.11UnderstandingAnswer key

    What is the correct general solution form for y2y+2y=0y'' - 2y' + 2y = 0?

  12. Ex. 95.12Understanding

    y+by+cy=0y'' + by' + cy = 0 with a=1a = 1. Under what condition(s) on b,cb, c does the solution decay to zero?

  13. Ex. 95.13Application

    Solve yy=e2xy'' - y = e^{2x}.

  14. Ex. 95.14Application

    Solve y+4y=3sinxy'' + 4y = 3\sin x.

  15. Ex. 95.15ApplicationAnswer key

    Solve y+2y=4x2y'' + 2y' = 4x^2.

  16. Ex. 95.16ApplicationAnswer key

    Solve y+4y=sin2xy'' + 4y = \sin 2x (resonance case).

  17. Ex. 95.17Application

    Calculate the Wronskian of y1=exy_1 = e^x and y2=e2xy_2 = e^{2x} and confirm they form a fundamental set of solutions for y3y+2y=0y'' - 3y' + 2y = 0.

  18. Ex. 95.18Application

    LC circuit: Lq¨+q/C=0L\ddot q + q/C = 0, q(0)=Q0q(0) = Q_0, q˙(0)=0\dot q(0) = 0. Find q(t)q(t) and ω0\omega_0.

  19. Ex. 95.19Understanding

    Is {cos3x,sin3x}\{\cos 3x, \sin 3x\} a fundamental set of solutions for y+9y=0y'' + 9y = 0?

  20. Ex. 95.20Modeling

    Mass-spring without friction: m=2kgm = 2\,\text{kg}, k=500N/mk = 500\,\text{N/m}, y(0)=0,1my(0) = 0{,}1\,\text{m}, y(0)=0y'(0) = 0. Find ω0\omega_0, period, and displacement y(t)y(t).

  21. Ex. 95.21Modeling

    Damped oscillator: y+5y+6y=0y'' + 5y' + 6y = 0, y(0)=1y(0) = 1, y(0)=0y'(0) = 0. Classify (under/over/critically) and solve.

  22. Ex. 95.22ModelingAnswer key

    Critical damping: 2y+4y+2y=02y'' + 4y' + 2y = 0, y(0)=1y(0) = 1, y(0)=1y'(0) = -1. Solve and classify.

  23. Ex. 95.23Modeling

    Underdamped system: y+4y+13y=0y'' + 4y' + 13y = 0, y(0)=1y(0) = 1, y(0)=0y'(0) = 0. Solve and identify damped frequency ωd\omega_d.

  24. Ex. 95.24Application

    Solve y+4y+3y=5exy'' + 4y' + 3y = 5e^{-x} (modification rule required).

  25. Ex. 95.25Application

    Solve y4y+4y=e2xy'' - 4y' + 4y = e^{2x} (repeated root — guess increases to x2x^2).

  26. Ex. 95.26Challenge

    Apply variation of parameters to yy=secxy'' - y = \sec x. Does the result have a closed form?

  27. Ex. 95.27Challenge

    Cauchy-Euler equation: x2y+xy+y=0x^2 y'' + xy' + y = 0. Try y=xmy = x^m and solve for mm.

  28. Ex. 95.28Challenge

    Use reduction of order with y1=e3xy_1 = e^{3x} to find the second solution of yy6y=0y'' - y' - 6y = 0.

  29. Ex. 95.29Proof

    Demonstrate that, when λ\lambda is a repeated root of aλ2+bλ+c=0a\lambda^2 + b\lambda + c = 0, the function y2=xeλxy_2 = xe^{\lambda x} satisfies ay+by+cy=0ay'' + by' + cy = 0.

  30. Ex. 95.30ProofAnswer key

    State and justify the existence-uniqueness theorem for ay+by+cy=q(x)ay'' + by' + cy = q(x), y(x0)=y0y(x_0) = y_0, y(x0)=y1y'(x_0) = y_1.

Sources

Updated on 2025-05-14 · Author(s): Clube da Matemática

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