沃利斯积分公式是求解形如∫ 0π2sin nx d x \int_0^{\frac\pi2}\sin^nx\text{d}x∫02πsinnxdx这种积分的公式。
一、正弦函数(sin\sinsin)的沃利斯公式记I n =∫ 0π 2 sin n xdxI_n=\int_0^{\frac\pi2}\sin^nx\text{d}xIn=∫02πsinnxdx。当n≥2n\ge2n≥2时,应用凑微分和分部积分得 I n=∫ 0π2sin nx d x = −∫ 0π2sinn−1x d ( cos x )= −[ sin n − 1xcosx∣0π2 −∫0π2 cos x d (sinn−1 x ) ] = −[ sin n − 1xcosx∣0π2 − ( n − 1 )∫0π2cos2 xsinn−2 x d x ] = −[ 0 − 0 − ( n − 1 )∫0π2 ( 1 −sin2 x )sinn−2 x d x ] = − ( n − 1 )[ −∫0π2sinn−2 x d x +∫0π2sinn x d x ] = ( n − 1 )In−2− ( n − 1 )I n\begin{aligned}I_n&=\int_0^{\frac\pi2}\sin^nx\text{d}x=-\int_0^{\frac\pi2}\sin^{n-1}x\text{d}(\cos x)\\&=-\left[\left.\sin^{n-1}x\cos x\right|_0^{\frac\pi2}-\int_0^{\frac\pi2}\cos x\text{d}(\sin^{n-1}x)\right]\\&=-\left[\left.\sin^{n-1}x\cos x\right|_0^{\frac\pi2}-(n-1)\int_0^{\frac\pi2}\cos^2x\sin^{n-2}x\text{d}x\right]\\&=-\left[0-0-(n-1)\int_0^{\frac\pi2}(1-\sin^2x)\sin^{n-2}x\text{d}x\right]\\&=-(n-1)\left[-\int_0^{\frac\pi2}\sin^{n-2}x\text{d}x+\int_0^{\frac\pi2}\sin^nx\text{d}x\right]\\&=(n-1)I_{n-2}-(n-1)I_n\end{aligned}In=∫02πsinnxdx=−∫02πsinn−1xd(cosx)=−[sinn−1xcosx∣∣02π−∫02πcosxd(sinn−1x)]=−[sinn−1xcosx∣∣02π−(n−1)∫02πcos2xsinn−2xdx]=−[0−0−(n−1)∫02π(1−sin2x)sinn−2xdx]=−(n−1)[−∫02πsinn−2xdx+∫02πsinnxdx]=(n−1)In−2−(n−1)In即I n= ( n − 1 )In−2− ( n − 1 )I nI_n=(n-1)I_{n-2}-(n-1)I_nIn=(n−1)In−2−(n−1)In nI n= ( n − 1 )In−2nI_n=(n-1)I_{n-2}nIn=(n−1)In−2I n= n−1 n In−2I_n=\frac{n-1}{n}I_{n-2}In=nn−1In−2当nnn为奇数时,I n= n−1 n In−2= n−1 n⋅ n−3n−2 In−4= ⋯ = n−1 n⋅ n−3n−2⋅ ⋯ ⋅2 3 I 1I_n=\frac{n-1}{n}I_{n-2}=\frac{n-1}{n}\cdot\frac{n-3}{n-2}I_{n-4}=\cdots=\frac{n-1}{n}\cdot\frac{n-3}{n-2}\cdot\cdots\cdot\frac23I_1In=nn−1In−2=nn−1⋅n−2n−3In−4=⋯=nn−1⋅n−2n−3⋅⋯⋅32I1其中I 1 =∫ 0π 2sinxdx=− cos x ∣0π 2=1I_1=\int_0^{\frac{\pi}{2}}\sin x\text{d}x=-\left.\cos x\right|_0^{\frac\pi2}=1I1=∫02πsinxdx=−cosx∣02π=1,故此时I n = n − 1n ⋅ n − 3 n − 2⋅⋯⋅2 3 I_n=\frac{n-1}{n}\cdot\frac{n-3}{n-2}\cdot\cdots\cdot\frac23In=nn−1⋅n−2n−3⋅⋯⋅32; 当nnn为偶数时,I n= n−1 n⋅ n−3n−2⋅ ⋯ ⋅1 2 I 0I_n=\frac{n-1}{n}\cdot\frac{n-3}{n-2}\cdot\cdots\cdot\frac12I_0In=nn−1⋅n−2n−3⋅⋯⋅21I0而∫ 0π 2 sin 0 xdx=∫ 0π 2dx=π 2 \int_0^{\frac\pi2}\sin^0x\text{d}x=\int_0^{\frac\pi2}\text{d}x=\frac\pi2∫02πsin0xdx=∫02πdx=2π,故此时I n = n − 1n ⋅ n − 3 n − 2⋅⋯⋅1 2 ⋅π 2 I_n=\frac{n-1}{n}\cdot\frac{n-3}{n-2}\cdot\cdots\cdot\frac12\cdot\frac\pi2In=nn−1⋅n−2n−3⋅⋯⋅21⋅2π。 综上所述,I n={n − 1 n⋅n − 3 n − 2 ⋅⋯⋅23,n为奇数,n − 1 n⋅n − 3 n − 2 ⋅⋯⋅12⋅π2,n为偶数。I_n=\begin{cases}\frac{n-1}{n}\cdot\frac{n-3}{n-2}\cdot\cdots\cdot\frac23,\quad&n\text{为奇数,}\\\frac{n-1}{n}\cdot\frac{n-3}{n-2}\cdot\cdots\cdot\frac12\cdot\frac\pi2,\quad&n\text{为偶数。}\end{cases}In={nn−1⋅n−2n−3⋅⋯⋅32,nn−1⋅n−2n−3⋅⋯⋅21⋅2π,n为奇数,n为偶数。记忆时,我们只需牢记递推公式I n= n−1 n In−2I_n=\frac{n-1}{n}I_{n-2}In=nn−1In−2即可。
二、余弦函数(cos\coscos)的沃利斯公式在I n =∫ 0π 2 sin n xdxI_n=\int_0^{\frac\pi2}\sin^nx\text{d}xIn=∫02πsinnxdx中,令u=π 2 −xu=\frac\pi2-xu=2π−x,则cosu=sinx\cos u=\sin xcosu=sinx,du=−dx\text{d}u=-\text{d}xdu=−dx,I n=∫π2 0cos nu ⋅ − d u =∫ 0π2cos nu d u I_n=\int_\frac\pi2^0\cos^n u\cdot-\text{d}u=\int_0^{\frac\pi2}\cos^nu\text{d}uIn=∫2π0cosnu⋅−du=∫02πcosnudu所以余弦函数和正弦函数的公式是完全一样的:I n=∫ 0π2sin nx d x =∫ 0π2cos nx d x ={n − 1 n⋅n − 3 n − 2 ⋅⋯⋅23,n为奇数,n − 1 n⋅n − 3 n − 2 ⋅⋯⋅12⋅π2,n为偶数。I_n=\int_0^{\frac\pi2}\sin^nx\text{d}x=\int_0^{\frac\pi2}\cos^nx\text{d}x=\begin{cases}\frac{n-1}{n}\cdot\frac{n-3}{n-2}\cdot\cdots\cdot\frac23,\quad&n\text{为奇数,}\\\frac{n-1}{n}\cdot\frac{n-3}{n-2}\cdot\cdots\cdot\frac12\cdot\frac\pi2,\quad&n\text{为偶数。}\end{cases}In=∫02πsinnxdx=∫02πcosnxdx={nn−1⋅n−2n−3⋅⋯⋅32,nn−1⋅n−2n−3⋅⋯⋅21⋅2π,n为奇数,n为偶数。
三、扩展到0∼π0\sim\pi0∼π的情况对于∫ 0 πsin n xdx\int_0^\pi\sin^nx\text{d}x∫0πsinnxdx,因为sinx\sin xsinx关于x=π 2 x=\frac\pi2x=2π对称,所以∫ 0 πsin n xdx=2∫ 0π 2 sin n xdx=2I n \int_0^\pi\sin^nx\text{d}x=2\int_0^\frac\pi2\sin^nx\text{d}x=2I_n∫0πsinnxdx=2∫02πsinnxdx=2In。 对于∫ 0 πcos n xdx\int_0^\pi\cos^nx\text{d}x∫0πcosnxdx: (1) 当nnn为奇数时, cos n x\cos^nxcosnx在x=π 2 x=\frac\pi2x=2π两边互为相反数,所以积分值为000; (2) 当nnn为偶数时, cos n x\cos^nxcosnx关于x=π 2 x=\frac\pi2x=2π对称,所以∫ 0 πcos n xdx=2∫ 0π 2 cos n xdx\int_0^\pi\cos^nx\text{d}x=2\int_0^\frac\pi2\cos^nx\text{d}x∫0πcosnxdx=2∫02πcosnxdx。