第10章 10.7

(1)

x2y′′+xy′−y=0x^2y'' + xy' - y = 0

m(m−1)x2+mx2−x2=m2x2−m2x2+mx2−x2=x2(m2−1)m(m-1)x^2 + mx^2 - x^2 = m^2x^2 - m^2x^2 + mx^2 - x^2 = x^2(m^2 - 1)

m=±1m = \pm1 より、y=x±1y = x^{\pm1} を解に持つ

y=xvy = xv とおくと、y′=v+xv′y' = v + xv'、y′′=2v+xv′′y'' = 2v + xv'' から、与式は

x2(2v+xv′′)+x(v+xv′)−xv=0x^2(2v + xv'') + x(v + xv') - xv = 0 ⋯ x3v′′+3x2v′=0x^3v'' + 3x^2v' = 0 ⋯ v′′+3xv′=0v'' + \frac{3}{x}v' = 0 ⋯ v′=Pv' = P とおくと

P′+3xP=0P' + \frac{3}{x}P = 0

α=3x,β=0\alpha = \frac{3}{x}, \beta = 0 とおくと ∫αdx=3log⁡x\int\alpha dx = 3\log x これから

P=1x3{∫0dx+C1}=1x3C1P = \frac{1}{x^3}\{\int 0dx + C_1\} = \frac{1}{x^3}C_1 元に戻して

v′=1x3C1v' = \frac{1}{x^3}C_1 ⋯ v=−12x2C1+C2v = -\frac{1}{2x^2}C_1 + C_2 元に戻して

yx=−12x2C1+C2\frac{y}{x} = -\frac{1}{2x^2}C_1 + C_2 ⋯ −12C1=A,C2=B-\frac{1}{2}C_1 = A, C_2 = B とおくと

y=1xA+Bxy = \frac{1}{x}A + Bx (A,B は任意定数)

(2)

(1−x)y′′+xy′−y=0(1-x)y'' + xy' - y = 0

P=1−x,Q=x,R=−1 かちP = 1-x, Q = x, R = -1 \text{ かち}

m(m−1)(1−x)+mx⋅x−x2=0m2−m−m2x+mx+mx2−x2=0m(m-1)(1-x) + mx \cdot x - x^2 = 0 \quad m^2 - m - m^2 x + mx + mx^2 - x^2 = 0

(x2−xm+m)(m−1)=0m=1,x±3ix2x2 これらを y=x を解に持つ(x^2 - xm + m)(m-1) = 0 \quad m = 1, \frac{x \pm \sqrt{3ix}}{2x^2} \text{ これらを } y = x \text{ を解に持つ}

y=xv とおくと y′=v+xv′y′′=2v+xv′′ かつ、与式はy = xv \text{ とおくと } \quad y' = v + xv' \quad y'' = 2v + xv'' \quad \text{ かつ、\text{与式は}}

(1−x)(2v+xv′′)+x(v+xv′)−xv=02v′+xv′′−2xv′−x2v′′+xv+x2v′−xv=0(1-x)(2v + xv'') + x(v + xv') - xv = 0 \quad 2v' + xv'' - 2xv' - x^2v'' + xv + x^2v' - xv = 0

(x(1−x))v′′+(x2−2x+2)v′=0v′=P とおくと v′′=P′ から(x(1-x))v'' + (x^2 - 2x + 2)v' = 0 \quad v' = P \text{ とおくと } \quad v'' = P' \text{ から}

x(1−x)P′+(x2−2x+2)P=01PP′=x2−2x+2x(1−x)=−1−2x+1x−1x(1-x)P' + (x^2 - 2x + 2)P = 0 \quad \frac{1}{P} P' = \frac{x^2 - 2x + 2}{x(1-x)} = -1 - \frac{2}{x} + \frac{1}{x-1}

∫1PdP=∫(1−2x+1x−1)dxlog⁡P=x−2log⁡x+log⁡(x−1)+C1eC1=C2 とおくと\int \frac{1}{P} dP = \int \left(1 - \frac{2}{x} + \frac{1}{x-1}\right)dx \quad \log P = x - 2\log x + \log(x-1) + C_1 \quad e^{C_1} = C_2 \text{ とおくと}

P=C2exx−1x2元に戻してP = C_2 e^x \frac{x-1}{x^2} \quad \text{元に戻して}

v′=C2(−exx2+exx)∫dv=∫C2(−exx2+exx)dxv' = C_2 \left(-\frac{e^x}{x^2} + \frac{e^x}{x}\right) \quad \int dv = \int C_2 \left(-\frac{e^x}{x^2} + \frac{e^x}{x}\right)dx

ここで I=C2∫(−exx2+exx)dx=C2(exx−∫exxdx+exx+∫exxdx)=2C2xex−∫C2(−exx2+exx)dx\text{ここで } I = C_2 \int \left(-\frac{e^x}{x^2} + \frac{e^x}{x}\right)dx = C_2 \left(\frac{e^x}{x} - \int \frac{e^x}{x} dx + \frac{e^x}{x} + \int \frac{e^x}{x} dx\right) = \frac{2C_2}{x} e^x - \int C_2 \left(-\frac{e^x}{x^2} + \frac{e^x}{x}\right)dx

=2C2xex−I= \frac{2C_2}{x} e^x - I

I=C2xexこれからI = \frac{C_2}{x} e^x \quad \text{これから}

v=C2xex+C3元に戻してv = \frac{C_2}{x} e^x + C_3 \quad \text{元に戻して}

y=x(C2xex+C3)C2=A,C3=B とおくとy = x\left(\frac{C_2}{x} e^x + C_3\right) \quad C_2 = A, C_3 = B \text{ とおくと}

y=Aex+Bx(A,B は任意定数)y = Ae^x + Bx \quad (A,B \text{ は任意定数})

(3)

(1+x2)y′′+2xy′−2y=0(1+x^2)y''+2xy'-2y=0

m(m−1)(1+x2)+mx⋅2x−2x2=0m(m-1)(1+x^2)+mx \cdot 2x-2x^2=0 m2+m2x2−m−mx2+2mx2−2x2=0m^2+m^2x^2-m-mx^2+2mx^2-2x^2=0

(m+mx2+2x2)(m−1)=0(m+mx^2+2x^2)(m-1)=0 m=1m=1 これかもy=xを解に持つ

y=xvy=xvとおくと y′=v+xv′y'=v+xv' y′′=2v′+xv′′y''=2v'+xv'' から、与式は

(1+x2)(2v+xv′′)+2x(v+xv′)−2xv=0(1+x^2)(2v+xv'')+2x(v+xv')-2xv=0 x(1+x2)v′′+(4x2+2)=0x(1+x^2)v''+(4x^2+2)=0

v′=Pv'=Pとおくと

x(1+x2)P′+(4x2+2)P=0x(1+x^2)P'+(4x^2+2)P=0 1PP′=−4x2+2x(1+x2)=−2x−2x1+x2\frac{1}{P}P'=-\frac{4x^2+2}{x(1+x^2)}=-\frac{2}{x}-\frac{2x}{1+x^2}

∫1PdP=∫(−2x−2x1+x2)dx\int\frac{1}{P}dP=\int\left(-\frac{2}{x}-\frac{2x}{1+x^2}\right)dx log⁡P=−2log⁡x−log⁡(1+x2)+C1\log P=-2\log x-\log(1+x^2)+C_1 eC1=C2e^{C_1}=C_2とおくと

P=C2x2(1+x2)P=\frac{C_2}{x^2(1+x^2)} 元に戻して

v′=C2x2(1+x2)=C2(1x2−11+x2)v'=\frac{C_2}{x^2(1+x^2)}=C_2\left(\frac{1}{x^2}-\frac{1}{1+x^2}\right)

∫dv=C2∫(1x2−11+x2)dx\int dv=C_2\int\left(\frac{1}{x^2}-\frac{1}{1+x^2}\right)dx v=C2(−1x−tan⁡−1x)+C3v=C_2\left(-\frac{1}{x}-\tan^{-1}x\right)+C_3 元に戻して

y=x{C2(−1x−tan⁡−1x)+C3}y=x\left\{C_2\left(-\frac{1}{x}-\tan^{-1}x\right)+C_3\right\} −C2=A,C3=B-C_2=A, C_3=Bとおくと

y=A(1+xtan⁡−1x)+Bxy=A(1+x\tan^{-1}x)+Bx (A,Bは任意定数)

解説: r31bn1z