第9章 9.8

(1)

In=∫0π2sin⁡nθ dθI_n = \int_0^{\frac{\pi}{2}} \sin^n\theta\, d\theta

θ=π2−t\theta = \dfrac{\pi}{2} - t とおくと dθ=−dtd\theta = -dt θ:0→π2\theta: 0 \to \dfrac{\pi}{2} t:π2→0t: \dfrac{\pi}{2} \to 0 これから

In=∫π20−sin⁡n(π2−t)dθ=∫0π2sin⁡n(π2−t)dθ=∫0π2cos⁡nθ dθI_n = \int_{\frac{\pi}{2}}^{0} -\sin^n\left(\frac{\pi}{2}-t\right) d\theta = \int_0^{\frac{\pi}{2}} \sin^n\left(\frac{\pi}{2}-t\right) d\theta = \int_0^{\frac{\pi}{2}} \cos^n\theta\, d\theta

(2)

I2=∫0π2sin⁡2θ dθ=∫0π21−cos⁡2θ2 dθ=12[θ−12sin⁡2θ]0π2=12(π2)=π4I_2 = \int_0^{\frac{\pi}{2}} \sin^2\theta\, d\theta = \int_0^{\frac{\pi}{2}} \frac{1-\cos2\theta}{2}\, d\theta = \frac{1}{2}\left[\theta - \frac{1}{2}\sin2\theta\right]_0^{\frac{\pi}{2}} = \frac{1}{2}\left(\frac{\pi}{2}\right) = \frac{\pi}{4}

(3)

In+2=∫0π2sin⁡n+2θ dθ=∫0π2sin⁡nθ⋅sin⁡2θ dθ=∫0π2sin⁡nθ⋅(1−cos⁡2θ) dθ=In−∫0π2sin⁡nθ⋅cos⁡2θ dθI_{n+2} = \int_0^{\frac{\pi}{2}} \sin^{n+2}\theta\, d\theta = \int_0^{\frac{\pi}{2}} \sin^n\theta \cdot \sin^2\theta\, d\theta = \int_0^{\frac{\pi}{2}} \sin^n\theta \cdot (1-\cos^2\theta)\, d\theta = I_n - \int_0^{\frac{\pi}{2}} \sin^n\theta \cdot \cos^2\theta\, d\theta

ここで ∫sin⁡nθ⋅cos⁡θ dθ=1n+1sin⁡n+1θ\displaystyle\int \sin^n\theta \cdot \cos\theta\, d\theta = \frac{1}{n+1}\sin^{n+1}\theta から

In+2=In−[1n+1sin⁡n+1θ⋅cos⁡θ]0π2+∫0π2(1n+1sin⁡n+1θ⋅(−sin⁡θ))dθ=In−1n+1∫0π2sin⁡n+2θ dθI_{n+2} = I_n - \left[\frac{1}{n+1}\sin^{n+1}\theta \cdot \cos\theta\right]_0^{\frac{\pi}{2}} + \int_0^{\frac{\pi}{2}} \left(\frac{1}{n+1}\sin^{n+1}\theta \cdot (-\sin\theta)\right) d\theta = I_n - \frac{1}{n+1}\int_0^{\frac{\pi}{2}} \sin^{n+2}\theta\, d\theta

=In−1n+1In+2= I_n - \frac{1}{n+1}I_{n+2}

(1+1n+1)In+2=InIn+2=n+1n+2In\left(1+\frac{1}{n+1}\right)I_{n+2} = I_n \qquad I_{n+2} = \frac{n+1}{n+2}I_n

(4)

(3)より

In+2=n+1n+2In=n+1n+2(n−1nIn−2)=n+1n+2⋅n−1n(n−3n−2In−4)=⋯I_{n+2} = \frac{n+1}{n+2}I_n = \frac{n+1}{n+2}\left(\frac{n-1}{n}I_{n-2}\right) = \frac{n+1}{n+2}\cdot\frac{n-1}{n}\left(\frac{n-3}{n-2}I_{n-4}\right) = \cdots となる

I0=∫0π2dθ=[θ]0π2=π2I_0 = \int_0^{\frac{\pi}{2}} d\theta = [\theta]_0^{\frac{\pi}{2}} = \frac{\pi}{2}

I1=∫0π2sin⁡θ dθ=[−cos⁡θ]0π2=1I_1 = \int_0^{\frac{\pi}{2}} \sin\theta\, d\theta = [-\cos\theta]_0^{\frac{\pi}{2}} = 1 これより

n が偶数のとき In=n−1n⋅n−3n−2⋯⋯12⋅π2I_n = \frac{n-1}{n}\cdot\frac{n-3}{n-2}\cdots\cdots\frac{1}{2}\cdot\frac{\pi}{2}

n が奇数のとき In=n−1n⋅n−3n−2⋯⋯23I_n = \frac{n-1}{n}\cdot\frac{n-3}{n-2}\cdots\cdots\frac{2}{3}

解説: r31bn1z