每次忘了都要查半天,自己推导一遍记录下来


Step 1

f(x)f(x)f(x)存在n阶导数,根据一阶导数定义:

lim⁡x→x0f(x)−f(x0)x−x0=f′(x)\lim\limits_{x\rightarrow x_0}\cfrac{f(x)-f(x_0)}{x-x_0}=f'(x)xx0limxx0f(x)f(x0)=f(x)

等式脱帽
f(x)−f(x0)x−x0=f′(x0)+o\cfrac{f(x)-f(x_0)}{x-x_0}=f'(x_0)+oxx0f(x)f(x0)=f(x0)+o
f(x)−f(x0)=(x−x0)f′(x0)+o(x−x0)f(x)-f(x_0)=(x-x_0)f'(x_0)+o(x-x_0)f(x)f(x0)=(xx0)f(x0)+o(xx0)

化简得
{f(x)=f(x0)+(x−x0)f′(x0)+o(x−x0)(1)o(x−x0)=f(x)−f(x0)−(x−x0)f′(x0)(2)\begin{cases} f(x)=f(x_0)+(x-x_0)f'(x_0)+o(x-x_0)(1)\\ o(x-x_0)= f(x)-f(x_0)-(x-x_0)f'(x_0)(2) \end{cases}{f(x)=f(x0)+(xx0)f(x0)+o(xx0)1o(xx0)=f(x)f(x0)(xx0)f(x0)2


Step 2

根据式(2)(2)(2)
lim⁡x→x0o(x−x0)(x−x0)2=lim⁡x→x0f(x)−f(x0)−(x−x0)f′(x0)(x−x0)2\lim\limits_{x\rightarrow x_0}\cfrac{o(x-x_0)}{(x-x_0)^2}=\lim\limits_{x\rightarrow x_0}\cfrac{f(x)-f(x_0)-(x-x_0)f'(x_0)}{(x-x_0)^2}xx0lim(xx0)2o(xx0)=xx0lim(xx0)2f(x)f(x0)(xx0)f(x0) (00型)\big(\frac{0}{0} 型\big)(00)

使用洛必达法则
lim⁡x→x0o(x−x0)(x−x0)2=lim⁡x→x0f′(x)−f′(x0)2(x−x0)=lim⁡x→x0f′′(x)2=f′′(x0)2(常数)\lim\limits_{x\rightarrow x_0}\cfrac{o(x-x_0)}{(x-x_0)^2}=\lim\limits_{x\rightarrow x_0}\cfrac{f'(x)-f'(x_0)}{2(x-x_0)}=\lim\limits_{x\rightarrow x_0}\cfrac{f''(x)}{2}=\cfrac{f''(x_0)}{2}(常数)xx0lim(xx0)2o(xx0)=xx0lim2(xx0)f(x)f(x0)=xx0lim2f(x)=2f(x0)()

所以得出o(x−x0)o(x-x_0)o(xx0)(x−x0)2(x-x_0)^2(xx0)2是等价无穷小
o(x−x0)(x−x0)2=12f′′(x0)+o\cfrac{o(x-x_0)}{(x-x_0)^2}=\cfrac{1}{2}f''(x_0)+o(xx0)2o(xx0)=21f(x0)+o
o(x−x0)=12(x−x0)2f′′(x0)+o(x−x0)2o(x-x_0)=\cfrac{1}{2}(x-x_0)^2f''(x_0)+o(x-x_0)^2o(xx0)=21(xx0)2f(x0)+o(xx0)2

带入式(1)(1)(1)
{f(x)=f(x0)+(x−x0)f′(x0)+12(x−x0)2f′′(x0)+o(x−x0)2(3)o(x−x0)2=f(x)−f(x0)−(x−x0)f′(x0)−12(x−x0)2f′′(x0)(4)\begin{cases} f(x)=f(x_0)+(x-x_0)f'(x_0)+\cfrac{1}{2}(x-x_0)^2f''(x_0)+o(x-x_0)^2(3)\\ o(x-x_0)^2= f(x)-f(x_0)-(x-x_0)f'(x_0)-\cfrac{1}{2}(x-x_0)^2f''(x_0)(4) \end{cases}f(x)=f(x0)+(xx0)f(x0)+21(xx0)2f(x0)+o(xx0)23o(xx0)2=f(x)f(x0)(xx0)f(x0)21(xx0)2f(x0)4


Step 3

根据式(4)(4)(4)
lim⁡x→x0o(x−x0)2(x−x0)3=lim⁡x→x0f(x)−f(x0)−(x−x0)f′(x0)−12(x−x0)2f′′(x0)(x−x0)3\lim\limits_{x\rightarrow x_0}\cfrac{o(x-x_0)^2}{(x-x_0)^3}=\lim\limits_{x\rightarrow x_0}\cfrac{f(x)-f(x_0)-(x-x_0)f'(x_0)-\cfrac{1}{2}(x-x_0)^2f''(x_0)}{(x-x_0)^3}xx0lim(xx0)3o(xx0)2=xx0lim(xx0)3f(x)f(x0)(xx0)f(x0)21(xx0)2f(x0) (00型)\big(\frac{0}{0} 型\big)(00)

使用洛必达法则
lim⁡x→x0o(x−x0)2(x−x0)3=2次lim⁡x→x0f′′(x)−f′′(x0)3⋅2(x−x0)=lim⁡x→x0f′′′(x)6=f′′′(x0)6(常数)\lim\limits_{x\rightarrow x_0}\cfrac{o(x-x_0)^2}{(x-x_0)^3}\xlongequal{2次}\lim\limits_{x\rightarrow x_0}\cfrac{f''(x)-f''(x_0)}{3\cdot2(x-x_0)}=\lim\limits_{x\rightarrow x_0}\cfrac{f'''(x)}{6}=\cfrac{f'''(x_0)}{6}(常数)xx0lim(xx0)3o(xx0)22 xx0lim32(xx0)f(x)f(x0)=xx0lim6f(x)=6f(x0)()

所以得出o(x−x0)2o(x-x_0)^2o(xx0)2(x−x0)3(x-x_0)^3(xx0)3是等价无穷小
o(x−x0)2(x−x0)3=16f′′′(x0)+o\cfrac{o(x-x_0)^2}{(x-x_0)^3}=\cfrac{1}{6}f'''(x_0)+o(xx0)3o(xx0)2=61f(x0)+o
o(x−x0)2=16(x−x0)3f′′′(x0)+o(x−x0)3o(x-x_0)^2=\cfrac{1}{6}(x-x_0)^3f'''(x_0)+o(x-x_0)^3o(xx0)2=61(xx0)3f(x0)+o(xx0)3

带入式(1)(1)(1)
{f(x)=f(x0)+(x−x0)f′(x0)+12(x−x0)2f′′(x0)+16(x−x0)3f′′′(x0)+o(x−x0)3(5)o(x−x0)3=f(x)−f(x0)−(x−x0)f′(x0)−12(x−x0)2f′′(x0)−16(x−x0)3f′′′(x0)(6)\begin{cases} f(x)=f(x_0)+(x-x_0)f'(x_0)+\cfrac{1}{2}(x-x_0)^2f''(x_0)+\cfrac{1}{6}(x-x_0)^3f'''(x_0)+o(x-x_0)^3(5)\\ o(x-x_0)^3= f(x)-f(x_0)-(x-x_0)f'(x_0)-\cfrac{1}{2}(x-x_0)^2f''(x_0)-\cfrac{1}{6}(x-x_0)^3f'''(x_0)(6) \end{cases}f(x)=f(x0)+(xx0)f(x0)+21(xx0)2f(x0)+61(xx0)3f(x0)+o(xx0)35o(xx0)3=f(x)f(x0)(xx0)f(x0)21(xx0)2f(x0)61(xx0)3f(x0)6


结论

以此类推
o(x−x0)n−1=1n!(x−x0)nf(n)(x0)+o(x−x0)no(x-x_0)^{n-1}=\cfrac{1}{n!}(x-x_0)^nf^{(n)}(x_0)+o(x-x_0)^{n}o(xx0)n1=n!1(xx0)nf(n)(x0)+o(xx0)n
f(x)=f(x0)+(x−x0)f′(x0)+12(x−x0)2f′′(x0)+16(x−x0)3f′′′(x0)+⋯+1n!(x−x0)nf(n)(x0)+o(x−x0)nf(x)=f(x_0)+(x-x_0)f'(x_0)+\cfrac{1}{2}(x-x_0)^2f''(x_0)+\cfrac{1}{6}(x-x_0)^3f'''(x_0)+\cdots+\cfrac{1}{n!}(x-x_0)^nf^{(n)}(x_0)+o(x-x_0)^nf(x)=f(x0)+(xx0)f(x0)+21(xx0)2f(x0)+61(xx0)3f(x0)++n!1(xx0)nf(n)(x0)+o(xx0)n


常用麦克劳林展开式

(1)ex=1+x+x22!+⋯+xnn!+o(xn)=∑n=0∞xnn!(1)e^x=1+x+\cfrac{x^2}{2!}+\cdots+\cfrac{x^n}{n!}+o(x^n)=\displaystyle\sum_{n=0}^{\infin}\cfrac{x^n}{n!}1ex=1+x+2!x2++n!xn+o(xn)=n=0n!xn
(2)sin⁡x=x−x33!+⋯+(−1)nx2n+1(2n+1)!+o(x2n+1)=∑n=0∞(−1)nx2n+1(2n+1)!(2)\sin x=x-\cfrac{x^3}{3!}+\cdots+(-1)^n\cfrac{x^{2n+1}}{(2n+1)!}+o(x^{2n+1})=\displaystyle\sum_{n=0}^{\infin}(-1)^n\cfrac{x^{2n+1}}{(2n+1)!}2sinx=x3!x3++(1)n(2n+1)!x2n+1+o(x2n+1)=n=0(1)n(2n+1)!x2n+1
(3)cos⁡x=1−x22!+⋯+(−1)nx2n(2n)!+o(x2n)=∑n=0∞(−1)nx2n(2n)!(3)\cos x=1-\cfrac{x^2}{2!}+\cdots+(-1)^n\cfrac{x^{2n}}{(2n)!}+o(x^{2n})=\displaystyle\sum_{n=0}^{\infin}(-1)^n\cfrac{x^{2n}}{(2n)!}3cosx=12!x2++(1)n(2n)!x2n+o(x2n)=n=0(1)n(2n)!x2n
(4)ln⁡(1+x)=x−x22+⋯+(−1)n−1xn(n)+o(xn)=∑n=1∞(−1)n−1xnn.(x>−1)(4)\ln (1+x)=x-\cfrac{x^2}{2}+\cdots+(-1)^{n-1}\cfrac{x^{n}}{(n)}+o(x^n)=\displaystyle\sum_{n=1}^{\infin}(-1)^{n-1}\cfrac{x^{n}}{n }.(x>-1)4ln(1+x)=x2x2++(1)n1(n)xn+o(xn)=n=1(1)n1nxn.(x>1) [注]: 从n=1开始
(5)11−x=1+x+x2+⋯+xn+o(xn)=∑n=0∞xn(5)\cfrac{1}{1-x}=1+x+x^2+\cdots+x^n+o(x^n)=\displaystyle\sum_{n=0}^\infin x^n51x1=1+x+x2++xn+o(xn)=n=0xn
(6)11+x=1−x+x2−⋯+(−1)nxn+o(xn)=∑n=0∞(−1)nxn(6)\cfrac{1}{1+x}=1-x+x^2-\cdots+(-1)^nx^n+o(x^n)=\displaystyle\sum_{n=0}^\infin (-1)^nx^n61+x1=1x+x2+(1)nxn+o(xn)=n=0(1)nxn
(7)(1+x)α=1+αx+α(α−1)2x2+o(x2)(x→0)(7)(1+x)^\alpha=1+\alpha x+\cfrac{\alpha(\alpha-1)}{2}x^2+o(x^2)(x\rightarrow0)7(1+x)α=1+αx+2α(α1)x2+o(x2)(x0)
(8)tan⁡x=x+13x3+o(x3)(x→0)(8)\tan x = x+\cfrac{1}{3}x^3+o(x^3)(x\rightarrow0)8tanx=x+31x3+o(x3)(x0)
(9)arcsin⁡x=x+16x3+o(x3)(x→0)(9)\arcsin x=x+\cfrac{1}{6}x^3+o(x^3)(x\rightarrow0)9arcsinx=x+61x3+o(x3)(x0)
(10)arctan⁡x=x−13x3+o(x3)(x→0)(10)\arctan x=x-\cfrac{1}{3}x^3+o(x^3)(x\rightarrow0)10arctanx=x31x3+o(x3)(x0)

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