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九州大学 システム情報科学府 共通 2015年8月実施 微分方程

Author

思齐塾, 祭音Myyura

Description

x>0x>0 で定義された関数 y(x)y(x) に関する以下の微分方程式において,変数変換 x=etx = e^t を用いて一般解を求めよ.なお, yy' は関数 y(x)y(x)xx に関する1階導関数を表している.

(1) x2yxyx3y=0x^2y'' - xy' - x - 3y = 0 (2) x3y+6x2y+4xy4y=0x^3y''' + 6x^2y'' + 4xy' - 4y = 0

题目描述

y(x)y(x) 定义在 x>0x>0 上。使用变量代换

x=etx=e^t

求下列微分方程的通解;其中 y,y,yy',y'',y''' 分别表示 y(x)y(x) 关于 xx 的一、二、三阶导数:

x2yxyx3y=0.x^2y''-xy'-x-3y=0.
x3y+6x2y+4xy4y=0.x^3y'''+6x^2y''+4xy'-4y=0.

Kai

Solution to (1): x2yxyx3y=0x^2y'' - xy' - x - 3y = 0

Let x=etx = e^t , then t=lnxt = \ln x . We have:

dydx=dydtdtdx=dydt1x=etdydt\frac{dy}{dx} = \frac{dy}{dt} \cdot \frac{dt}{dx} = \frac{dy}{dt} \cdot \frac{1}{x} = e^{-t} \frac{dy}{dt}

y=etdydty' = e^{-t} \frac{dy}{dt}

d2ydx2=ddx(etdydt)=ddt(etdydt)dtdx=(etdydt+etd2ydt2)et=e2t(d2ydt2dydt)\frac{d^2y}{dx^2} = \frac{d}{dx} (e^{-t} \frac{dy}{dt}) = \frac{d}{dt} (e^{-t} \frac{dy}{dt}) \cdot \frac{dt}{dx} = (-e^{-t} \frac{dy}{dt} + e^{-t} \frac{d^2y}{dt^2}) \cdot e^{-t} = e^{-2t} (\frac{d^2y}{dt^2} - \frac{dy}{dt})

y=e2t(d2ydt2dydt)y'' = e^{-2t} (\frac{d^2y}{dt^2} - \frac{dy}{dt})

Substitute into the original equation:

e2te2t(d2ydt2dydt)etetdydtet3y=0e^{2t} \cdot e^{-2t} (\frac{d^2y}{dt^2} - \frac{dy}{dt}) - e^t \cdot e^{-t} \frac{dy}{dt} - e^t - 3y = 0

d2ydt2dydtdydtet3y=0\frac{d^2y}{dt^2} - \frac{dy}{dt} - \frac{dy}{dt} - e^t - 3y = 0

d2ydt22dydt3y=et\frac{d^2y}{dt^2} - 2\frac{dy}{dt} - 3y = e^t

Let D=ddtD = \frac{d}{dt} . The characteristic equation is D22D3=0D^2 - 2D - 3 = 0 , so (D3)(D+1)=0(D-3)(D+1) = 0 . Thus D=3D = 3 or D=1D = -1 .

The homogeneous solution is yh=c1e3t+c2ety_h = c_1e^{3t} + c_2e^{-t} .

For the particular solution, let yp=Aety_p = Ae^t . Then yp=Aety_p' = Ae^t and yp=Aety_p'' = Ae^t .

Aet2Aet3Aet=etAe^t - 2Ae^t - 3Ae^t = e^t

4Aet=et-4Ae^t = e^t , so A=14A = -\frac{1}{4} . Thus yp=14ety_p = -\frac{1}{4}e^t .

The general solution is y=c1e3t+c2et14et=c1x3+c2x14xy = c_1e^{3t} + c_2e^{-t} - \frac{1}{4}e^t = c_1x^3 + \frac{c_2}{x} - \frac{1}{4}x .

Solution to (2): x3y+6x2y+4xy4y=0x^3y''' + 6x^2y'' + 4xy' - 4y = 0

Let x=etx = e^t , then t=lnxt = \ln x . We have:

y=etdydty' = e^{-t} \frac{dy}{dt}

y=e2t(d2ydt2dydt)y'' = e^{-2t} (\frac{d^2y}{dt^2} - \frac{dy}{dt})

y=e3t(d3ydt33d2ydt2+2dydt)y''' = e^{-3t} (\frac{d^3y}{dt^3} - 3\frac{d^2y}{dt^2} + 2\frac{dy}{dt})

Substitute into the original equation:

e3te3t(d3ydt33d2ydt2+2dydt)+6e2te2t(d2ydt2dydt)+4etetdydt4y=0e^{3t} e^{-3t} (\frac{d^3y}{dt^3} - 3\frac{d^2y}{dt^2} + 2\frac{dy}{dt}) + 6e^{2t} e^{-2t} (\frac{d^2y}{dt^2} - \frac{dy}{dt}) + 4e^t e^{-t} \frac{dy}{dt} - 4y = 0

d3ydt33d2ydt2+2dydt+6d2ydt26dydt+4dydt4y=0\frac{d^3y}{dt^3} - 3\frac{d^2y}{dt^2} + 2\frac{dy}{dt} + 6\frac{d^2y}{dt^2} - 6\frac{dy}{dt} + 4\frac{dy}{dt} - 4y = 0

d3ydt3+3d2ydt2+0dydt4y=0\frac{d^3y}{dt^3} + 3\frac{d^2y}{dt^2} + 0\frac{dy}{dt} - 4y = 0

d3ydt3+3d2ydt24y=0\frac{d^3y}{dt^3} + 3\frac{d^2y}{dt^2} - 4y = 0

Let D=ddtD = \frac{d}{dt} . The characteristic equation is D3+3D24=0D^3 + 3D^2 - 4 = 0 , so (D1)(D+2)2=0(D-1)(D+2)^2 = 0 . Thus D=1D = 1 or D=2D = -2 .

The general solution is y=c1et+c2e2t+c3te2t=c1x+c2x2+c3lnxx2y = c_1e^{t} + c_2e^{-2t} + c_3te^{-2t} = c_1x + \frac{c_2}{x^2} + \frac{c_3\ln x}{x^2} .