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题型分析 — Second Order Differential Equations

Type 1:常系数 ODE

Example 1 (w20/21 Q2): Solve 9d2ydx2+6dydx+y=3x2+30x9\frac{d^2y}{dx^2} + 6\frac{dy}{dx} + y = 3x^2 + 30x.

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Auxiliary equation: 9m2+6m+1=09m^2 + 6m + 1 = 0 M1

(3m+1)2=0m=13(3m + 1)^2 = 0 \Rightarrow m = -\frac{1}{3} (repeated) A1

CF: yc=(A+Bx)ex/3y_c = (A + Bx)e^{-x/3} A1

For PI, try yp=αx2+βx+γy_p = \alpha x^2 + \beta x + \gamma M1

yp=2αx+βy_p' = 2\alpha x + \beta, yp=2αy_p'' = 2\alpha

Substitute:

9(2α)+6(2αx+β)+(αx2+βx+γ)=3x2+30x9(2\alpha) + 6(2\alpha x + \beta) + (\alpha x^2 + \beta x + \gamma) = 3x^2 + 30x

αx2+(12α+β)x+(18α+6β+γ)=3x2+30x\alpha x^2 + (12\alpha + \beta)x + (18\alpha + 6\beta + \gamma) = 3x^2 + 30x M1

Comparing coefficients:

x2x^2: α=3\alpha = 3

xx: 12α+β=3036+β=30β=612\alpha + \beta = 30 \Rightarrow 36 + \beta = 30 \Rightarrow \beta = -6

Const: 18α+6β+γ=05436+γ=0γ=1818\alpha + 6\beta + \gamma = 0 \Rightarrow 54 - 36 + \gamma = 0 \Rightarrow \gamma = -18 A1

yp=3x26x18y_p = 3x^2 - 6x - 18

General solution: y=(A+Bx)ex/3+3x26x18y = (A + Bx)e^{-x/3} + 3x^2 - 6x - 18 A1

[Total: 6+1]

Example 2 (s21/21 Q2): Solve d2ydx2+3dydx+2y=2x+1\frac{d^2y}{dx^2} + 3\frac{dy}{dx} + 2y = 2x + 1.

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AE: m2+3m+2=0m^2 + 3m + 2 = 0 M1

(m+1)(m+2)=0m=1,2(m+1)(m+2) = 0 \Rightarrow m = -1, -2 A1

CF: yc=Aex+Be2xy_c = Ae^{-x} + Be^{-2x} A1

PI: try yp=αx+βy_p = \alpha x + \beta M1

yp=αy_p' = \alpha, yp=0y_p'' = 0

0+3α+2(αx+β)=2x+10 + 3\alpha + 2(\alpha x + \beta) = 2x + 1

2αx+(3α+2β)=2x+12\alpha x + (3\alpha + 2\beta) = 2x + 1 M1

xx: 2α=2α=12\alpha = 2 \Rightarrow \alpha = 1

Const: 3α+2β=13+2β=1β=13\alpha + 2\beta = 1 \Rightarrow 3 + 2\beta = 1 \Rightarrow \beta = -1 A1

yp=x1y_p = x - 1

General solution: y=Aex+Be2x+x1y = Ae^{-x} + Be^{-2x} + x - 1 A1

[Total: 6+1]

Example 3 (s20/23 Q1): Solve d2xdt28dxdt9x=9e8t\frac{d^2x}{dt^2} - 8\frac{dx}{dt} - 9x = 9e^{8t}.

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AE: m28m9=0m^2 - 8m - 9 = 0 M1

(m9)(m+1)=0m=9,1(m - 9)(m + 1) = 0 \Rightarrow m = 9, -1 A1

CF: xc=Ae9t+Betx_c = Ae^{9t} + Be^{-t} A1

PI: try xp=Ce8tx_p = Ce^{8t} M1

x˙p=8Ce8t\dot{x}_p = 8Ce^{8t}, x¨p=64Ce8t\ddot{x}_p = 64Ce^{8t}

Sub: 64Ce8t8(8Ce8t)9Ce8t=9e8t64Ce^{8t} - 8(8Ce^{8t}) - 9Ce^{8t} = 9e^{8t}

(64649)C=9(64 - 64 - 9)C = 9

9C=9C=1-9C = 9 \Rightarrow C = -1 A1

xp=e8tx_p = -e^{8t}

General solution: x=Ae9t+Bete8tx = Ae^{9t} + Be^{-t} - e^{8t} A1

[Total: 6]

Example 4 (w20/22 Q6): Solve d2xdt2+8dxdt+15x=102cos3t\frac{d^2x}{dt^2} + 8\frac{dx}{dt} + 15x = 102\cos 3t.

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AE: m2+8m+15=0m^2 + 8m + 15 = 0 M1

(m+3)(m+5)=0m=3,5(m+3)(m+5) = 0 \Rightarrow m = -3, -5 A1

CF: xc=Ae3t+Be5tx_c = Ae^{-3t} + Be^{-5t} A1

PI: try xp=Ccos3t+Dsin3tx_p = C\cos 3t + D\sin 3t M1

x˙p=3Csin3t+3Dcos3t\dot{x}_p = -3C\sin 3t + 3D\cos 3t

x¨p=9Ccos3t9Dsin3t\ddot{x}_p = -9C\cos 3t - 9D\sin 3t

Sub:

(9Ccos3t9Dsin3t)+8(3Csin3t+3Dcos3t)+15(Ccos3t+Dsin3t)(-9C\cos 3t - 9D\sin 3t) + 8(-3C\sin 3t + 3D\cos 3t) + 15(C\cos 3t + D\sin 3t)

=102cos3t= 102\cos 3t M1

cos3t\cos 3t: 9C+24D+15C=6C+24D=102-9C + 24D + 15C = 6C + 24D = 102

sin3t\sin 3t: 9D24C+15D=6D24C=0-9D - 24C + 15D = 6D - 24C = 0 M1

From sin3t\sin 3t: 6D=24CD=4C6D = 24C \Rightarrow D = 4C

From cos3t\cos 3t: 6C+24(4C)=6C+96C=102C=102C=16C + 24(4C) = 6C + 96C = 102C = 102 \Rightarrow C = 1 A1

D=4D = 4

xp=cos3t+4sin3tx_p = \cos 3t + 4\sin 3t A1

General solution: x=Ae3t+Be5t+cos3t+4sin3tx = Ae^{-3t} + Be^{-5t} + \cos 3t + 4\sin 3t A1

[Total: 11]

Example 5 (s25/21 Q5): Solve 6d2xdt2+3dxdt+6x=et6\frac{d^2x}{dt^2} + 3\frac{dx}{dt} + 6x = e^{-t}.

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AE: 6m2+3m+6=06m^2 + 3m + 6 = 0 M1

2m2+m+2=02m^2 + m + 2 = 0

m=1±1164=1±i154m = \frac{-1 \pm \sqrt{1 - 16}}{4} = \frac{-1 \pm i\sqrt{15}}{4} A1

CF: xc=et/4(Acos154t+Bsin154t)x_c = e^{-t/4}\left(A\cos\frac{\sqrt{15}}{4}t + B\sin\frac{\sqrt{15}}{4}t\right) A1

PI: try xp=Cetx_p = Ce^{-t} M1

x˙p=Cet\dot{x}_p = -Ce^{-t}, x¨p=Cet\ddot{x}_p = Ce^{-t}

Sub: 6(Cet)+3(Cet)+6(Cet)=et6(Ce^{-t}) + 3(-Ce^{-t}) + 6(Ce^{-t}) = e^{-t}

(63+6)C=19C=1C=19(6 - 3 + 6)C = 1 \Rightarrow 9C = 1 \Rightarrow C = \frac{1}{9} A1

xp=19etx_p = \frac{1}{9}e^{-t}

General solution: x=et/4(Acos154t+Bsin154t)+19etx = e^{-t/4}\left(A\cos\frac{\sqrt{15}}{4}t + B\sin\frac{\sqrt{15}}{4}t\right) + \frac{1}{9}e^{-t} A1

[Total: 10]

Type 2:Euler-Cauchy 方程

Example 1 (s20/21 Q7): By using the substitution x=t3yx = t^3y, transform t3d2ydt2+t^3\frac{d^2y}{dt^2} + \cdots into a constant coefficient equation.

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Given x=t3yx = t^3y, we have y=xt3y = xt^{-3}.

First, express derivatives:

y=t3xy = t^{-3}x

dydt=3t4x+t3dxdt\frac{dy}{dt} = -3t^{-4}x + t^{-3}\frac{dx}{dt} M1

d2ydt2=12t5x6t4dxdt+t3d2xdt2\frac{d^2y}{dt^2} = 12t^{-5}x - 6t^{-4}\frac{dx}{dt} + t^{-3}\frac{d^2x}{dt^2} M1

Substitute into original ODE and simplify.

The substitution transforms it into a constant coefficient equation in xx:

d2xdt2+Pdxdt+Qx=R(t)\frac{d^2x}{dt^2} + P\frac{dx}{dt} + Qx = R(t) A1

(Continued with solving the transformed equation...) M1 A1

[Total: 4+7]

Example 2: Solve the Euler-Cauchy equation t2d2ydt22tdydt+2y=t3t^2\frac{d^2y}{dt^2} - 2t\frac{dy}{dt} + 2y = t^3.

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This is an Euler-Cauchy equation of the form at2y+bty+cy=f(t)at^2y'' + bty' + cy = f(t).

Use substitution t=eut = e^u or try y=tmy = t^m.

For homogeneous: t2y2ty+2y=0t^2y'' - 2ty' + 2y = 0

Try y=tmy = t^m: t2(m(m1)tm2)2t(mtm1)+2tm=0t^2(m(m-1)t^{m-2}) - 2t(mt^{m-1}) + 2t^m = 0

m(m1)2m+2=0m(m-1) - 2m + 2 = 0

m23m+2=0m^2 - 3m + 2 = 0 M1

(m1)(m2)=0m=1,2(m-1)(m-2) = 0 \Rightarrow m = 1, 2 A1

CF: yc=At+Bt2y_c = At + Bt^2 A1

For PI with RHS t3t^3, try yp=Ct3y_p = Ct^3 M1

yp=3Ct2y_p' = 3Ct^2, yp=6Cty_p'' = 6Ct

Sub: t2(6Ct)2t(3Ct2)+2(Ct3)=t3t^2(6Ct) - 2t(3Ct^2) + 2(Ct^3) = t^3

6Ct36Ct3+2Ct3=2Ct3=t36Ct^3 - 6Ct^3 + 2Ct^3 = 2Ct^3 = t^3 M1

2C=1C=122C = 1 \Rightarrow C = \frac{1}{2} A1

yp=12t3y_p = \frac{1}{2}t^3

General solution: y=At+Bt2+12t3y = At + Bt^2 + \frac{1}{2}t^3 A1

[Total: 8]

Example 3: Solve t2d2ydt2+tdydt+y=lntt^2\frac{d^2y}{dt^2} + t\frac{dy}{dt} + y = \ln t.

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Euler-Cauchy with a=1,b=1,c=1a=1, b=1, c=1.

Try y=tmy = t^m: m(m1)+m+1=0m(m-1) + m + 1 = 0

m2+1=0m=±im^2 + 1 = 0 \Rightarrow m = \pm i M1 A1

CF: yc=Acos(lnt)+Bsin(lnt)y_c = A\cos(\ln t) + B\sin(\ln t) A1

For PI, use substitution t=eut = e^u, so u=lntu = \ln t.

dydt=dydu1t\frac{dy}{dt} = \frac{dy}{du}\cdot\frac{1}{t}, d2ydt2=1t2(d2ydu2dydu)\frac{d^2y}{dt^2} = \frac{1}{t^2}\left(\frac{d^2y}{du^2} - \frac{dy}{du}\right) M1

d2ydu2+y=u\frac{d^2y}{du^2} + y = u M1

AE: m2+1=0m=±im^2 + 1 = 0 \Rightarrow m = \pm i

CF (in uu): yc=Acosu+Bsinuy_c = A\cos u + B\sin u A1

PI (in uu): try yp=αuy_p = \alpha u

0+αu=uα=10 + \alpha u = u \Rightarrow \alpha = 1

yp=u=lnty_p = u = \ln t A1

General solution: y=Acos(lnt)+Bsin(lnt)+lnty = A\cos(\ln t) + B\sin(\ln t) + \ln t A1

[Total: 9]

Type 3:耦合系统(拓展)

Example 1: Solve the coupled system dxdt=3x+4y\frac{dx}{dt} = 3x + 4y, dydt=2x+y\frac{dy}{dt} = 2x + y.

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Matrix form: (x˙y˙)=(3421)(xy)\begin{pmatrix}\dot{x} \\ \dot{y}\end{pmatrix} = \begin{pmatrix}3 & 4 \\ 2 & 1\end{pmatrix}\begin{pmatrix}x \\ y\end{pmatrix} B1

Find eigenvalues of A=(3421)A = \begin{pmatrix}3 & 4 \\ 2 & 1\end{pmatrix}:

det(AλI)=(3λ)(1λ)8=0\det(A - \lambda I) = (3-\lambda)(1-\lambda) - 8 = 0

λ24λ5=0λ=5,1\lambda^2 - 4\lambda - 5 = 0 \Rightarrow \lambda = 5, -1 M1 A1

For λ=5\lambda = 5: (2424)(ab)=0a=2b\begin{pmatrix}-2 & 4 \\ 2 & -4\end{pmatrix}\begin{pmatrix}a \\ b\end{pmatrix} = 0 \Rightarrow a = 2b, eigenvector (21)\begin{pmatrix}2 \\ 1\end{pmatrix} M1

For λ=1\lambda = -1: (4422)(ab)=0a=b\begin{pmatrix}4 & 4 \\ 2 & 2\end{pmatrix}\begin{pmatrix}a \\ b\end{pmatrix} = 0 \Rightarrow a = -b, eigenvector (11)\begin{pmatrix}1 \\ -1\end{pmatrix} M1

General solution:

(xy)=C1(21)e5t+C2(11)et\begin{pmatrix}x \\ y\end{pmatrix} = C_1\begin{pmatrix}2 \\ 1\end{pmatrix}e^{5t} + C_2\begin{pmatrix}1 \\ -1\end{pmatrix}e^{-t} A1

x=2C1e5t+C2etx = 2C_1e^{5t} + C_2e^{-t} y=C1e5tC2ety = C_1e^{5t} - C_2e^{-t}

[Total: 8]