第10章 10.24

(1)

(1−x2)d2ydx2−xdydx+4y=0(1-x^2)\frac{d^2y}{dx^2} - x\frac{dy}{dx} + 4y = 0

x=cos⁡tx = \cos t とおくと t=cos⁡−1xt = \cos^{-1} x

dydx=dydt⋅dtdx\frac{dy}{dx} = \frac{dy}{dt} \cdot \frac{dt}{dx}

dtdx=−11−x2=−1sin⁡t\frac{dt}{dx} = \frac{-1}{\sqrt{1-x^2}} = \frac{-1}{\sin t}

d2ydx2=(d2ydt2⋅dtdx)dtdx+dydtd2tdx2\frac{d^2y}{dx^2} = \left(\frac{d^2y}{dt^2} \cdot \frac{dt}{dx}\right)\frac{dt}{dx} + \frac{dy}{dt}\frac{d^2t}{dx^2}

d2tdx2=−x(1−x2)3=−cos⁡tsin⁡3t\frac{d^2t}{dx^2} = \frac{-x}{\sqrt{(1-x^2)^3}} = \frac{-\cos t}{\sin^3 t}

ここから与式は

(1−cos⁡2t)[(−1sin⁡t)2d2ydt2+−cos⁡tsin⁡tdydt]−cos⁡t⋅−1sin⁡tdydt+4y=0(1-\cos^2 t)\left[\left(\frac{-1}{\sin t}\right)^2 \frac{d^2y}{dt^2} + \frac{-\cos t}{\sin t}\frac{dy}{dt}\right] - \cos t \cdot \frac{-1}{\sin t}\frac{dy}{dt} + 4y = 0

d2ydt2+cos⁡tsin⁡tdydt+cos⁡tsin⁡tdydt+4y=0\frac{d^2y}{dt^2} + \frac{\cos t}{\sin t}\frac{dy}{dt} + \frac{\cos t}{\sin t}\frac{dy}{dt} + 4y = 0

d2ydt2+4y=0\frac{d^2y}{dt^2} + 4y = 0

特性方程式は s2+4=0s^2 + 4 = 0 ∴s=±2i\therefore s = \pm 2i これから

y=Asin⁡2t+Bcos⁡2ty = A\sin 2t + B\cos 2t

元に戻して

y=Asin⁡(2cos⁡−1x)+Bcos⁡(2cos⁡−1x)y = A\sin(2\cos^{-1} x) + B\cos(2\cos^{-1} x)

=A[2sin⁡(cos⁡−1x)cos⁡(cos⁡−1x)]+B[cos⁡2(cos⁡−1x)−sin⁡2(cos⁡−1x)]= A[2\sin(\cos^{-1} x)\cos(\cos^{-1} x)] + B[\cos^2(\cos^{-1} x) - \sin^2(\cos^{-1} x)]

=2A1−x2⋅x+B{x2−(1−x2)}= 2A\sqrt{1-x^2} \cdot x + B\{x^2 - (1-x^2)\} 2A=A2A = A 書き直して

=Ax1−x2+B(2x2−1)= Ax\sqrt{1-x^2} + B(2x^2-1)

(A,B は任意定数)

(2)

4xd2ydx2+2dydx+y=04x\frac{d^2y}{dx^2} + 2\frac{dy}{dx} + y = 0

x=t2x = t^2 とおくと t=xt = \sqrt{x}

dtdx=12x=12t\frac{dt}{dx} = \frac{1}{2\sqrt{x}} = \frac{1}{2t}

d2tdx2=−14x3=−14t3\frac{d^2t}{dx^2} = -\frac{1}{4\sqrt{x^3}} = -\frac{1}{4t^3} これから与式は

4t2[(12t)2d2ydt2+(−14t3)dydt]+2⋅12tdydt+y=04t^2\left[\left(\frac{1}{2t}\right)^2 \frac{d^2y}{dt^2} + \left(-\frac{1}{4t^3}\right)\frac{dy}{dt}\right] + 2 \cdot \frac{1}{2t}\frac{dy}{dt} + y = 0

d2ydt2+y=0\frac{d^2y}{dt^2} + y = 0

特性方程式は s2+1=0s^2 + 1 = 0 ∴s=±i\therefore s = \pm i これから

y=Asin⁡t+Bcos⁡ty = A\sin t + B\cos t

元に戻して

y=Asin⁡x+Bcos⁡xy = A\sin \sqrt{x} + B\cos \sqrt{x} (A,B は任意定数)

(3)

(x+1)d2ydx2+xdydx−y=0(x+1)\frac{d^2y}{dx^2} + x\frac{dy}{dx} - y = 0

y=e−xuy = e^{-x}u とおくと y′=−e−xu+e−xu′y' = -e^{-x}u + e^{-x}u' y′′=e−xu−2e−xu′+e−xu′′y'' = e^{-x}u - 2e^{-x}u' + e^{-x}u'' これから与式は

(x+1)(e−xu−2e−xu′+e−xu′′)+x(−e−xu+e−xu′)−e−xu=0(x+1)(e^{-x}u - 2e^{-x}u' + e^{-x}u'') + x(-e^{-x}u + e^{-x}u') - e^{-x}u = 0 (x+1)u′′−(x+2)u′=0(x+1)u'' - (x+2)u' = 0

u′=Pu' = P とおくと (x+1)P′−(x+2)P=0(x+1)P' - (x+2)P = 0 P′−x+2x+1P=0P' - \frac{x+2}{x+1}P = 0

∫1PdP=∫x+2x+1dx=∫(1+1x+1)dx\int \frac{1}{P}dP = \int \frac{x+2}{x+1}dx = \int\left(1 + \frac{1}{x+1}\right)dx

log⁡P=x+log⁡(x+1)+C1\log P = x + \log(x+1) + C_1 eC1=C2e^{C_1} = C_2 とおくと

P=C2ex(x+1)P = C_2 e^x(x+1) 元に戻して

u′=C2ex(x+1)u' = C_2 e^x(x+1)

u=C2{ex+xe−x−∫exdx}+C3=C2xe−x+C3u = C_2 \{e^x + xe^{-x} - \int e^x dx\} + C_3 = C_2 xe^{-x} + C_3 C2=AC_2 = A、C3=BC_3 = B として元に戻して

y=Ax+Be−xy = Ax + Be^{-x} (A,B は任意定数)

(4)

x2d2ydx2−(2a−1)xdydx+a2y=0x^2\frac{d^2y}{dx^2} - (2a-1)x\frac{dy}{dx} + a^2y = 0

y=xauy = x^a u とおくと y′=axa−1u+xau′y' = ax^{a-1}u + x^au' y′′=a(a−1)xa−2u+2axa−1u′+xau′′y'' = a(a-1)x^{a-2}u + 2ax^{a-1}u' + x^au'' これから与式は

x2{a(a−1)xa−2u+2axa−1u′+xau′′}−(2a−1)x(axa−1u+xau′)+a2xau=0x^2\{a(a-1)x^{a-2}u + 2ax^{a-1}u' + x^au''\} - (2a-1)x(ax^{a-1}u + x^au') + a^2x^au = 0

xu′+u′=0xu' + u' = 0 u′=Pu' = P とおくと

xP′+P=0xP' + P = 0

∫1PdP=−∫1xdx\int \frac{1}{P}dP = -\int \frac{1}{x}dx

log⁡P=−log⁡x+C1\log P = -\log x + C_1 eC1=C2e^{C_1} = C_2 とおくと

P=C21xP = C_2 \frac{1}{x} 元に戻して

u′=C2xu' = \frac{C_2}{x} u=C2log⁡x+C3u = C_2 \log x + C_3 C1=AC_1 = A、C2=BC_2 = B として元に戻して

y=xa(Alog⁡x+B)y = x^a(A\log x + B) (A,B は任意定数)

解説: r31bn1z