第5章 5.38

(1)

∫0∞dxex+e−x\int_0^\infty \frac{dx}{e^x+e^{-x}}

ex=te^x = t とおくと dx=1tdtdx = \dfrac{1}{t}dt x:0→∞x:0\to\infty t:1→∞t:1\to\infty これから

=∫1∞1t+1t⋅1t dt=∫1∞11+t2 dt=[tan⁡−1t]1∞=π2−π4=π4= \int_1^\infty \frac{1}{t+\dfrac{1}{t}}\cdot\frac{1}{t}\,dt = \int_1^\infty \frac{1}{1+t^2}\,dt = \left[\tan^{-1}t\right]_1^\infty = \frac{\pi}{2}-\frac{\pi}{4} = \frac{\pi}{4}

(2)

∫01xlog⁡x dx=[12x2log⁡x]01−12∫01x dx=−12[12x2]01=−14\int_0^1 x\log x\,dx = \left[\frac{1}{2}x^2\log x\right]_0^1 - \frac{1}{2}\int_0^1 x\,dx = -\frac{1}{2}\left[\frac{1}{2}x^2\right]_0^1 = -\frac{1}{4}

(3)

∫1∞log⁡xx2 dx=[−1xlog⁡x]1∞+∫1∞1x2 dx=[−1x]1∞=1\int_1^\infty \frac{\log x}{x^2}\,dx = \left[-\frac{1}{x}\log x\right]_1^\infty + \int_1^\infty \frac{1}{x^2}\,dx = \left[-\frac{1}{x}\right]_1^\infty = 1

(4)

∫0∞tan⁡−1x1+x2 dx\int_0^\infty \frac{\tan^{-1}x}{1+x^2}\,dx

tan⁡−1x=t\tan^{-1}x = t とおくと 11+x2dx=dt\dfrac{1}{1+x^2}dx = dt x:0→∞x:0\to\infty t:0→π2t:0\to\dfrac{\pi}{2} これから

=∫0π2t dt=[12t2]0π2=π28= \int_0^{\frac{\pi}{2}} t\,dt = \left[\frac{1}{2}t^2\right]_0^{\frac{\pi}{2}} = \frac{\pi^2}{8}

(5)

∫0∞x2e−x dx=[−x2e−x]0∞+∫0∞2xe−x dx=[−2xe−x]0∞+∫0∞2e−x dx=2[−e−x]0∞=2\int_0^\infty x^2e^{-x}\,dx = \left[-x^2e^{-x}\right]_0^\infty + \int_0^\infty 2xe^{-x}\,dx = \left[-2xe^{-x}\right]_0^\infty + \int_0^\infty 2e^{-x}\,dx = 2\left[-e^{-x}\right]_0^\infty = 2

(6)

∫01log⁡(1+x2)x2 dx=[−1xlog⁡(1+x2)]01+∫012xx(x2+1) dx=−log⁡2+∫012x2+1 dx\int_0^1 \frac{\log(1+x^2)}{x^2}\,dx = \left[-\frac{1}{x}\log(1+x^2)\right]_0^1 + \int_0^1 \frac{2x}{x(x^2+1)}\,dx = -\log 2 + \int_0^1 \frac{2}{x^2+1}\,dx

=−log⁡2+2[tan⁡−1x]01=−log⁡2+π2= -\log 2 + 2\left[\tan^{-1}x\right]_0^1 = -\log 2 + \frac{\pi}{2}

(7)

∫01x1−xdx\int_0^1\sqrt{\dfrac{x}{1-x}}dx

x1−x=t\sqrt{\dfrac{x}{1-x}}=t とおくと dx=2t(1+t2)2dtdx=\dfrac{2t}{(1+t^2)^2}dt x:0→1x:0\to1 t:0→∞t:0\to\infty これから

=∫0∞t⋅2t(1+t2)2dt=∫0∞2t2(1+t2)2dt=∫0∞{−2(1+t2)2+21+t2}dt=\int_0^\infty t\cdot\dfrac{2t}{(1+t^2)^2}dt=\int_0^\infty\dfrac{2t^2}{(1+t^2)^2}dt=\int_0^\infty\left\{\dfrac{-2}{(1+t^2)^2}+\dfrac{2}{1+t^2}\right\}dt

=−2[−12(tt2+1+tan⁡−1t)]0∞+[2tan⁡−1t]0∞=−π2+π=π2=-2\left[-\dfrac{1}{2}\left(\dfrac{t}{t^2+1}+\tan^{-1}t\right)\right]_0^\infty+\left[2\tan^{-1}t\right]_0^\infty=-\dfrac{\pi}{2}+\pi=\dfrac{\pi}{2}

(8)

∫02x2x−x2dx=∫02x1−(x−1)2dx\int_0^2\dfrac{x}{\sqrt{2x-x^2}}dx=\int_0^2\dfrac{x}{\sqrt{1-(x-1)^2}}dx

x−1=tx-1=t とおくと dx=dtdx=dt x:0→2x:0\to2 t:−1→1t:-1\to1 これから

=∫−11{t1−t2+11−t2}dt=[−1−t2]−11+[sin⁡−1t]−11=π2−(−π2)=π=\int_{-1}^1\left\{\dfrac{t}{\sqrt{1-t^2}}+\dfrac{1}{\sqrt{1-t^2}}\right\}dt=\left[-\sqrt{1-t^2}\right]_{-1}^1+\left[\sin^{-1}t\right]_{-1}^1=\dfrac{\pi}{2}-\left(-\dfrac{\pi}{2}\right)=\pi

解説: r31bn1z