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求解微分方程

文章目录

摘要

解微分方程是我的弱项,就靠这个了

基本概念

定义

含导数或微分的方程称之为微分方程,一般形式为f(x,y′⋯y(n))f(x,y' \cdots y^{(n)})

阶数

微分方程所含的导数或微分的最高阶数称为微分方程的阶数

解

解:使得微分方程成立的函数 特解:不含任意常数 通解:所含的相互独立的任意常数的个数与微分方程的阶数相等

求解

可分离变量微分方程

dydx=f(x)g(y)\frac{\mathrm{d}y}{\mathrm{d}x} = f(x)g(y)

解

∫dyg(y)=∫f(x)dx\int \frac{\mathrm{d}y}{g(y)} = \int f(x)\mathrm{d}x

e.g.

dydx=2xy\frac{\mathrm{d}y}{\mathrm{d}x} = 2xy
解
∫dyy=∫2xdx\int \frac{\mathrm{d}y}{y} = \int 2x\mathrm{d}x
ln⁡y=x2+C\ln y = x^2+C
y=ex2+C=eCex2=C1ex2(C1=eC)\begin{aligned} y {}& = e^{x^2+C} {} \\ & = e^C e^{x^2} {} \\ & = C_1 e^{x^2} {} \\ & \quad(C_1 = e^C) \end{aligned}

一阶齐次线性微分方程

y′+P(x)y=0y' +P(x)y = 0

解

y=Ce−∫P(x)dxy = Ce^{-\int{P(x)\mathrm{d}x}}

e.g.

y′−xy=0y'-xy=0
解
y=Ce∫xdx=Cex22y = Ce^{\int x\mathrm{d}x}=Ce^{\frac{x^2}{2}}

一阶非齐次线性微分方程

y′+P(x)y=Q(x)≠0y'+P(x)y = Q(x) \neq 0

解

y=(∫Q(x)e∫P(x)dxdx+C)e−∫P(x)dxy = (\int Q(x)e^{\int P(x) \mathrm{d}x}\mathrm{d}x+C)e^{-\int P(x) \mathrm{d}x}

e.g.

y′+ytan⁡x=cos⁡xy'+y \tan x = \cos x
解
y=(∫cos⁡xe∫tan⁡xdxdx+C)e−∫tan⁡xdx=(x+C)cos⁡xy = (\int \cos x e^{\int \tan x \mathrm{d}x}\mathrm{d}x+C)e^{-\int\tan x \mathrm{d}x} = (x+C)\cos x

贝努利方程

dydx+P(x)y=Q(x)yn(n≠0)\frac{\mathrm{d}y}{\mathrm{d}x} + P(x)y = Q(x)y^n \quad (n \neq 0)

解 令z=y1−nz = y^{1-n},代入原方程得dzdx+(1−n)P(x)z=(1−n)Q(x)\frac{\mathrm{d}z}{\mathrm{d}x}+(1-n)P(x)z = (1-n)Q(x),再求解该一阶非齐次线性方程即可

e.g.

x2y′+xy=y2x^2y'+xy = y^2
解
z=y1−2=y−1,y′=−1z2z′z = y^{1-2} = y^{-1},\quad y' = -\frac{1}{z^2}z'
代入原式
z′−1xz=−1x2z' - \frac{1}{x}z = -\frac{1}{x^2}
z=(∫(−1x2)e∫−1xdxdx+C)e∫1xdx=(12x2+C)xz = (\int (-\frac{1}{x^2})e^{\int -\frac{1}{x}\mathrm{d}x}\mathrm{d}x +C)e^{\int \frac{1}{x}\mathrm{d}x} = (\frac{1}{2x^2}+C)x
1y=(12x2+C)x\frac{1}{y} = (\frac{1}{2x^2}+C)x

可降阶微分方程

形式一

y(n)=f(x)y^{(n) = f(x)}

解 对方程进行nn次不定积分

e.g.

y′′=x2y'' = x^2
解
y′=13x3+C1y' = \frac{1}{3} x^3 +C_1
y=112x4+C1x+C2y = \frac{1}{12}x^4+C_1 x + C_2

形式二

f(x,y′,y′′)=0f(x,y',y'') = 0

解

  1. 令y′=py' = p,则y′′=p′y''=p',原方程变为f(x,p,p′)=0f(x,p,p') = 0
  2. 解出p=φ(x)p = \varphi(x)
  3. y=∫φ(x)dx+Cy = \int \varphi(x)\mathrm{d}x+C

e.g.

y′′+y′x=0y'' + \frac{y'}{x} = 0
解 令y′=py' = p,则y′′=p′y'' = p',原方程变为p′+px=0p' + \frac{p}{x} = 0
p=C1e∫−1xdx=C1xp = C_1e^{\int -\frac{1}{x}\mathrm{d}x} = \frac{C_1}{x}
dydx=C1x\frac{\mathrm{d}y}{\mathrm{d}x} = \frac{C_1}{x}
y=C1ln⁡∣x∣+C2y = C_1 \ln \lvert x \rvert +C_2

形式三

f(y,y′,y′′)=0f(y,y',y'') = 0

解

  1. 令y′=py' = p,则y′′=dpdx=dpdydydx=pdpdyy'' = \frac{\mathrm{d}p}{\mathrm{d}x} = \frac{\mathrm{d}p}{\mathrm{d}y} \frac{\mathrm{d}y}{\mathrm{d}x} = p \frac{\mathrm{d}p}{\mathrm{d}y},原方程变为f(y,p,p′)=0f(y,p,p') = 0
  2. 解出p=φ(y)p = \varphi(y)
  3. ∫dyφ(y)=x+C\int \frac{\mathrm{d}y}{\varphi(y)} = x+C

e.g.

yy′′=y′2y y'' = y'^2
令y′=py' = p,y′′=pdpdyy'' = p \frac{\mathrm{d}p}{\mathrm{d}y},代入原式
ypdpdy−p2=0⇒p=C1e∫1ydy=C1yyp\frac{\mathrm{d}p}{\mathrm{d}y}-p^2 = 0 \Rightarrow p = C_1 e^{\int \frac{1}{y} \mathrm{d}y = C_1 y }
dydx=C1y⇒∫dyy=∫C1dx\frac{\mathrm{d}y}{\mathrm{d}x} = C_1 y \Rightarrow \int \frac{\mathrm{d}y}{y} = \int C_1 \mathrm{d}x
ln⁡y=C1x+C2⇒y=eC1x+C2=C3eC1x(C3=eC2)\ln y = C_1x+C_2 \Rightarrow y = e^{C_1 x+C_2} = C_3 e^{C_1 x} \quad (C_3 = e^{C_2})

二阶常系数线性微分方程

y′′+py′+qy=0y'' +py' +qy = 0

解

  1. 求解y′′+py′+qy=0y'' +py' +qy = 0的特征方程是r2+pr+q=0r^2+pr+q = 0
  2. 根据方程根的不同分为三种情况
    1. 当特征方程有两个实根r1r_1,r2r_2,且r1≠r2r_1\neq r_2,则y=C1er1x+C2er2xy = C_1e^{r1 x}+C_2e^{r_2 x}
    2. 当特征方程有重根r1=r2r_1 = r_2,则y=(C1+C2x)er1xy = (C_1+C_2x)e^{r_1 x}
    3. 当特征方程有两个共轭重根r1,2=α±βir_{1,2} = \alpha \pm \beta i,则y=eαx(C1cos⁡βx+C2sin⁡βx)y = e^{\alpha x} (C_1 \cos \beta x + C_2 \sin \beta x)

e.g.1

y′′−y′−6y=0y'' - y' - 6y = 0
解
r2−r−6=(r−3)(r+2)=0⇒r1=3,r2=−2r^2-r-6 = (r-3)(r+2) = 0 \Rightarrow r_1 = 3,\quad r_2 = -2
y=C1e3x+C2e−2xy = C_1 e^{3x} + C_2 e^{-2x}
e.g.2
y′′−2y′+y=0y''-2y'+y = 0
解
r2−2r+1=(r−1)2=0⇒r1,2=1r^2-2r+1 = (r-1)^2 = 0 \Rightarrow r_{1,2} = 1
y=(C1+C2x)exy = (C_1 + C_2 x)e^x
e.g.3
y′′−2y′+2y=0y'' - 2y' + 2y = 0
解
r2−2r+2=0⇒r1,2=1±ir^2- 2r +2 = 0 \Rightarrow r_{1,2} = 1 \pm i
y=ex(C1cos⁡x+C2sin⁡x)y = e^x (C_1 \cos x + C_2 \sin x)

二阶常系数非齐次线性微分方程

形式一

y′′+py′+qy=Pn(x)ekxy'' + py' +qy = P_n(x)e^{kx}

其中Pn(x)P_n(x)代表xx的nn阶多项式 解 根据kk的值有以下三种情况:

  1. 若kk非特征值,即k≠r1≠r2k \neq r_1 \neq r_2,则特解 y∗=ekx∑i=0naixiy^* = e^{kx} \sum_{i=0}^n a_i x^i
  2. 若kk与一个特征值相同,则特解 y∗=xekx∑i=0naixiy^* = xe^{kx} \sum_{i=0}^n a_i x^i
  3. 若kk与两个特征值相同,则特解 y∗=x2ekx∑i=0naixiy^* = x^2e^{kx} \sum_{i=0}^n a_i x^i

形式二

y′′+py′+qy=eax[Plcos⁡bx+Pssin⁡bx]y'' + py' + qy = e^{ax} [P_l \cos bx + P_s \sin bx]

其中Pl(x)P_l(x),Ps(x)P_s(x)代表xx的ll,ss阶多项式 解 根据aa,bb的值有以下三种情况

  1. 若a±bia\pm b i不是特征值,则特解 y∗=(Qn(1)(x)cos⁡bx+Qn(2)(x)sin⁡bx)eaxy^* = (Q_n^{(1)}(x)\cos bx+Q_n^{(2)}(x)\sin bx)e^{ax}
  2. 若a±bia\pm b i是特征值,则特解 y∗=x(Qn(1)(x)cos⁡bx+Qn(2)(x)sin⁡bx)eaxy^* = x(Q_n^{(1)}(x)\cos bx+Q_n^{(2)}(x)\sin bx)e^{ax}