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常用公式结论

𝓳𝓭𝔂𝓼𝔂𝓪大约 6 分钟高数公式结论

常用公式结论

基础公式

an−bn=(a−b)∑i=0n−1aibn−1−i=(a−b)(a0bn−1+abn−2+a2bn−3+⋯+an−3b2+an−2b+an−1b0) \begin{aligned} a^{n}-b^{n}& \begin{aligned}&=(a-b)\sum_{i=0}^{n-1}a^i b^{n-1-i}\end{aligned} \\ &=(a-b)(a^0b^{n-1}+ab^{n-2}+a^2b^{n-3}+\cdots+a^{n-3}b^2+a^{n-2}b+a^{n-1}b^0) \end{aligned}

详聊如何理解open in new windowan−bna^n-b^n因式分解

a3+b3=(a+b)(a2−ab+b2)a3−b3=(a−b)(a2+ab+b2) \begin{align*} a^3+b^3&=(a+b)(a^2-ab+b^2)\\ a^3-b^3&=(a-b)(a^2+ab+b^2) \end{align*}

12+22+⋯+n2=n(n+1)(2n+1)6 1^2+2^2+\dots+n^2=\frac{n(n+1)(2n+1)}{6}

如何求解open in new window12+22+⋯+n21^2+2^2+\dots+n^2

13+23+⋯+n3=(n(n+1)2)2 1^3+2^3+\dots+n^3=\left(\frac{n(n+1)}{2}\right)^2

自然数立方和公式推导方法汇总open in new window

x1+x<ln⁡(1+x)<x \frac{x}{1+x}<\ln(1+x)<x

数列

等比数列

an=a1×qn−1an=am×qn−m \begin{align*} a_{n}&=a_{1}\times q^{n-1} \\ a_{n}&=a_{m}\times q^{n-m} \end{align*}

Sn={na1,q=1a1×(1−qn)1−q=a1−anq1−q,q≠1 S_n=\begin{cases} &na_{1},\quad q=1 \\ & \displaystyle\frac{a_1\times (1-q^n)}{1-q}=\frac{a_{1}-a_{n}q}{1-q},\quad q\neq 1 \end{cases}

lim⁡n→∞Sn=a11−q(∣q∣<1) \lim_{ n \to \infty } S_{n}= \frac{a_{1}}{1-q}(|q|<1)

点到直线距离

对于直线ax+by+c=0ax+by+c=0,点(x0,y0)(x_{0},y_{0})到直线的距离为ax0+by0+ca2+b2\displaystyle \frac{ax_{0}+by_{0}+c}{\sqrt{a^2+b^2 }}

三角函数

x∈(0,π/2),sin⁡x<x<tan⁡xx\in(0, \pi/2),\sin x<x<\tan x

诱导公式

sin⁡(π2+α)=cos⁡α \sin\left( \frac{\pi}{2}+\alpha \right)=\cos\alpha

sin⁡(π2−α)=cos⁡α \sin\left( \frac{\pi}{2}-\alpha \right)=\cos\alpha

cos⁡(π2+α)=−sin⁡α \cos\left( \frac{\pi}{2}+\alpha \right)=-\sin\alpha

cos⁡(π2−α)=sin⁡α \cos\left( \frac{\pi}{2}-\alpha \right)=\sin\alpha

和差化积

sin⁡xcos⁡y=12[sin⁡(x+y)+sin⁡(x−y)] \sin x\cos y=\frac{1}{2}[\sin(x+y)+\sin(x-y)] \\

cos⁡xsin⁡y=12[sin⁡(x+y)−sin⁡(x−y)] \cos x\sin y=\frac{1}{2}[\sin(x+y)-\sin(x-y)] \\

sin⁡xsin⁡y=12[cos⁡(x−y)−cos⁡(x+y)] \sin x\sin y=\frac{1}{2}[\cos(x-y)-\cos(x+y)] \\

cos⁡xcos⁡y=12[cos⁡(x+y)+cos⁡(x−y)] \cos x\cos y=\frac{1}{2}[\cos(x+y)+\cos(x-y)] \\

sin⁡x+sin⁡y=2sin⁡x+y2cos⁡x−y2 \sin x+\sin y=2\sin\frac{x+y}{2}\cos\frac{x-y}{2} \\

sin⁡x−sin⁡y=2cos⁡x+y2sin⁡x−y2 \sin x-\sin y=2\cos\frac{x+y}{2}\sin\frac{x-y}{2} \\

cos⁡x+cos⁡y=2cos⁡x+y2cos⁡x−y2 \cos x+\cos y=2\cos\frac{x+y}{2}\cos\frac{x-y}{2} \\

cos⁡x−cos⁡y=−2sin⁡x+y2sin⁡x−y2 \cos x-\cos y=-2\sin\frac{x+y}{2}\sin\frac{x-y}{2} \\

函数

设φ(x)\varphi(x)是可微函数f(x)f(x)的反函数,则

φ([f(x)])=x \varphi([f(x)])=x

极限

常用的等价无穷小

当x→0x\rightarrow 0时,有

sin⁡x∼xarcsin⁡x∼x1−cos⁡x∼12x2tan⁡x∼xarctan⁡x∼xax−1∼xln⁡a(a>0)(1+x)α−1∼αx(α为任意常数)1+x−1−x∼xx−ln⁡(1+x)∼12x2x−sin⁡x∼16x3x−arcsin⁡x∼−16x3x−arctan⁡x∼13x3x−tan⁡x∼−13x3 \begin{align*} \sin x&\sim x \\ \arcsin x&\sim x \\ 1-\cos x &\sim \frac{1}{2}x^2 \\\tan x&\sim x\\ \arctan x&\sim x\\ a^x-1&\sim x\ln a(a>0)\\ (1+x)^\alpha-1&\sim \alpha x(\alpha \text{为任意常数})\\ \sqrt{1+x}-\sqrt{1-x}&\sim x\\ x-\ln{(1+x)}&\sim \frac{1}{2}x^2 \\ x-\sin x &\sim \frac{1}{6}x^3 \\ x-\arcsin x &\sim -\frac{1}{6}x^3 \\ x-\arctan x &\sim \frac{1}{3}x^3 \\ x-\tan x &\sim -\frac{1}{3}x^3 \end{align*}

函数常用极限

lim⁡n→−∞arctan⁡x=−π2\lim\limits_{ n \to -\infty }\arctan x=-\frac{\pi}{2},lim⁡n→+∞arctan⁡x=π2\lim\limits_{ n \to +\infty }\arctan x=\frac{\pi}{2}

两个重要极限

lim⁡x→0sin⁡xx=1lim⁡x→0(1+x)1x=e \begin{array}{c} \displaystyle\lim_{x\rightarrow 0} \frac{\sin x}{x}=1\\ \displaystyle{\lim_{x\rightarrow 0}(1+x)^{\frac{1}{x}}}=e \end{array}

一些解题公式

lim⁡x→0x−sin⁡xx3=16lim⁡x→0arcsin⁡x−xx3=16lim⁡x→0tan⁡x−xx3=13lim⁡x→0x−arctan⁡xx3=13 \begin{aligned} &\displaystyle\lim_{x\rightarrow 0} \frac{x-\sin x}{x^3}=\frac{1}{6} \\&\displaystyle\lim_{x\rightarrow 0}\frac{\arcsin x-x}{x^3}=\frac{1}{6} \\&\displaystyle\lim_{x\rightarrow 0}\frac{\tan x-x}{x^3}=\frac{1}{3} \\&\displaystyle\lim_{x\rightarrow 0}\frac{x-\arctan x}{x^3}=\frac{1}{3} \end{aligned}

需要注意的是,当x→0x\rightarrow 0时,有

sin⁡x<x<tan⁡x \sin x< x<\tan x

对ln⁡u(x)\ln u(x)型的无穷小,做如下等价变换

ln⁡u(x)=ln⁡[1+u(x)−1]∼u(x)−1 \ln u(x)= \ln[1+u(x)-1]\sim u(x)-1

微分学

一元函数微分学




(ax)(n)=axln⁡na (a^x)^{(n)}=a^x\ln^n a

(1ax+b)(n)=(−1)nan⋅n!(ax+b)n+1 \left( \frac{1}{ax+b} \right)^{(n)}=(-1)^n \frac{a^n\cdot n \text{!}}{(ax+b)^{n+1}}

常用麦克劳林公式

1x−x2\frac{1}{\sqrt{ x- x^2}}

ex=1+x+x22!+x33!+o(x3) e^x=1+x+\frac{x^2}{2!}+\frac{x^3}{3!}+o(x^3)

ln⁡(1+x)=x−x22+x33+o(x3) \ln(1+x)=x-\frac{x^2}{2}+\frac{x^3}{3}+o(x^3)

(1+x)α=1+αx+α(α−1)2!x2+α(α−1)(α−2)3!x3+o(x3) (1+x)^{\alpha}=1+\alpha x+\frac{\alpha(\alpha-1)}{2!}x^2+\frac{\alpha(\alpha-1)(\alpha-2)}{3!}x^3+o(x^3)

11−x=1+x+x2+x3+o(x3) \frac{1}{1-x}=1+x+x^2+x^3+o(x^3)

11+x=1−x+x2−x3+o(x3) \frac{1}{1+x}=1-x+x^2-x^3+o(x^3)

sin⁡x=x−x33!+x55!+o(x5) \sin x=x-\frac{x^3}{3!}+\frac{x^5}{5!}+o(x^5)

arcsin⁡x=x+12×x33+1×32×4×x55+1×3×52×4×6×x77+o(x7) \arcsin x=x+\frac{1}{2}\times\frac{x^3}{3}+\frac{1\times3}{2\times4}\times\frac{x^5}{5}+\frac{1\times3\times5}{2\times4\times6}\times\frac{x^7}{7}+o(x^7)

cos⁡x=1−x22!+x44!+o(x4) \cos x=1-\frac{x^2}{2!}+\frac{x^4}{4!}+o(x^4)

1+x=1+x2−x28+x316+o(x3) \sqrt{1+x}=1+\frac{x}{2}-\frac{x^2}{8}+\frac{x^3}{16}+o(x^3)

tan⁡x=x+x33+2x515+o(x5) \tan x=x+\frac{x^3}{3}+\frac{2x^5}{15}+o(x^5)

arctan⁡x=x−x33+x55+o(x5) \arctan x=x-\frac{x^3}{3}+\frac{x^5}{5}+o(x^5)

积分

不定积分

基础公式

∫dxx=ln⁡∣x∣+C∫dxcos⁡2x=∫sec⁡2x dx=tan⁡x+C∫1sin⁡2xdx=∫csc⁡2xdx=−cot⁡x+C∫sec⁡xtan⁡x dx=∫sin⁡xcos⁡2xdx=∫d(1cos⁡x)dx=sec⁡x+C∫csc⁡xcot⁡x dx=∫cos⁡xsin⁡2xdx=∫d(1sin⁡x)dx=−csc⁡x+C∫1x2−1=ln⁡(x+x2−1)+C∫tan⁡xdx=−ln⁡∣cos⁡x∣+C∫cot⁡xdx=ln⁡∣sin⁡x∣+C∫sec⁡xdx=ln⁡∣sec⁡x+tan⁡x∣+C∫csc⁡xdx=ln⁡∣csc⁡x−cot⁡x∣+C∫dxa2+x2=1aarctan⁡xa+C∫dxx2−a2=12aln⁡∣x−ax+a∣+C∫dxa2−x2=arcsin⁡xa+C∫dxx2+a2=ln⁡(x+x2+a2)+C∫dxx2−a2=ln⁡∣x+x2−a2∣+C \begin{align} &\int \frac{dx}{x} = \ln|x|+C\\ &\int \frac{dx}{\cos^2 x}=\int \sec^2x \, dx =\tan x+C \\ &\int \frac{1}{\sin^2x} dx=\int \csc^2x dx=-\cot x+C \\ &\int \sec x\tan x \,dx =\int \frac{\sin x}{\cos^2 x} dx =\int \mathrm{d}\left( \frac{1}{\cos x} \right) dx =\sec x+C \\ &\int \csc x\cot x \, dx =\int \frac{\cos x}{\sin^2 x} dx =\int \mathrm{d}\left( \frac{1}{\sin x} \right) dx =-\csc x+C \\ &\int \frac{1}{\sqrt{ x^2-1 }} = \ln(x+\sqrt{ x^2-1 })+C \\ &\int\tan x dx=-\ln|\cos x|+C \\ & \int\cot xdx=\ln|\sin x|+C \\ & \int \sec xdx=\ln|\sec x+\tan x|+C \\ &\int \csc xdx=\ln|\csc x-\cot x|+C \\ & \int\frac{dx}{a^2+x^2}=\frac{1}{a}\arctan\frac{x}{a}+C \\ & \int\frac{dx}{x^2-a^2}=\frac{1}{2a}\ln\left|\frac{x-a}{x+a}\right|+C \\ & \int\frac{dx}{\sqrt{a^2-x^2}}=\arcsin \frac{x}{a}+C \\ & \int\frac{dx}{\sqrt{x^2+a^2}}=\ln(x+\sqrt{x^2+a^2})+C \\ & \int\frac{dx}{\sqrt{x^2-a^2}}=\ln|x+\sqrt{x^2-a^2}|+C \end{align}

常见积分

∫cos⁡(ln⁡t)dt=∫excos⁡xdx(令x=ln⁡t)=12ex(sin⁡x+cos⁡x)+C \int \cos(\ln t) dt =\int e^x\cos x dx (\text{令}x=\ln t)=\frac{1}{2}e^x(\sin x+\cos x)+C

∫1+x2dx=x1+x2−∫xd(1+x2)d=x1+x2−∫x21+x2dx=x1+x2−∫(x2+1)−11+x2dx=x1+x2−∫1+x2dx+∫11+x2dx  ⟹  2∫1+x2dx=x1+x2+ln⁡(x+1+x2)  ⟹  ∫1+x2dx=12(x1+x2+ln⁡(x+1+x2)) \begin{align*} \int \sqrt{ 1+x^2 } dx &=x\sqrt{ 1+x^2 }-\int x\mathrm{d}(\sqrt{ 1+x^2 }) d\\ &=x\sqrt{ 1+x^2 }-\int \frac{x^2}{\sqrt{ 1+x^2 }} dx\\ &=x\sqrt{ 1+x^2 }-\int \frac{(x^2+1)-1}{\sqrt{ 1+x^2 }}dx\\ &=x\sqrt{ 1+x^2 }-\int \sqrt{ 1+x^2 } dx +\int \frac{1}{\sqrt{1+x^2 } } dx \\ \implies 2\int \sqrt{ 1+x^2 } dx&=x\sqrt{ 1+x^2 }+\ln(x+\sqrt{ 1+x^2 })\\ \implies \int \sqrt{ 1+x^2 } dx&=\frac{1}{2} (x\sqrt{ 1+x^2 }+\ln(x+\sqrt{ 1+x^2 })) \end{align*}

定积分

∫0π/2sin⁡nxdx=∫0π/2cos⁡nxdx={n−1n⋅n−3n−2⋅⋯⋅12⋅π2,当 n 为正偶数, I0=π2.n−1n⋅n−3n−2⋅⋯⋅23,当 n 为大于1的正奇数, I1=1. \begin{align*} \int_0^{\pi/2} \sin^n x dx &= \int_0^{\pi/2} \cos^n x dx \\ &= \begin{cases} \displaystyle\frac{n-1}{n} \cdot \frac{n-3}{n-2} \cdot \dots \cdot \frac{1}{2} \cdot \frac{\pi}{2}, & \text{当 } n \text{ 为正偶数, } I_0 = \frac{\pi}{2}. \\ \displaystyle\frac{n-1}{n} \cdot \frac{n-3}{n-2} \cdot \dots \cdot \frac{2}{3}, & \text{当 } n \text{ 为大于1的正奇数, } I_1 = 1. \end{cases} \end{align*}

设f(x)f(x)为连续函数,则

∫abf(x)dx=∫abf(a+b−x)dx \int_{a}^{b}f\left(x\right)\mathrm{d}x=\int_{a}^{b}f\left(a+b-x\right)\mathrm{d}x

提示

  1. 令t=π−xt=\pi-x

∫0πxf(sin⁡x)dx=π2∫0πf(sin⁡x)dx(其中f(x)连续) \int _{0}^{\pi}xf(\sin x) dx=\frac{\pi}{2}\int _{0}^\pi f(\sin x) dx \quad (\text{其中}f(x)\text{连续})

常见积分

见反常积分

∫−∞+∞e−x2dx=2∫0+∞e−x2dx=π \int _{-\infty}^{+\infty}e^{-x^2} dx=2\int _{0}^{+\infty}e^{-x^2}dx =\sqrt{ \pi }

特殊点

驻点:导数为0的点,极值点一定是驻点,驻点不一定是极值点
拐点:凹凸性改变的点,可能是二阶导等于0的点也可能二阶导是不存在的点
极值点:这个点是x的值,而不是一个坐标

f(x)可导  ⟹  连续  ⟹  可积  ⟹  有界 f(x)\text{可导}\implies \text{连续}\implies \text{可积}\implies \text{有界}