极限

等价无穷小

sin⁡x∼arcsin⁡x∼tan⁡x∼arctan⁡x∼x\sin x \sim \arcsin x \sim \tan x \sim \arctan x \sim x

ln⁡(1+x)∼ex−1∼1+x−1−x∼x\ln {(1+x)} \sim e^x - 1 \sim \sqrt{1 + x} - \sqrt{1 - x}\sim x

1−cos⁡x∼sec⁡x−1∼x−ln⁡(1+x)∼12x21 - \cos x \sim \sec x - 1 \sim x - \ln {(1 + x)} \sim \frac{1}{2}x^2

1−cos⁡ax∼a2x21-\cos ^{a} x \sim \frac{a}{2} x^{2}

(1+x)a−1∼ax(1 + x)^a -1 \sim ax

ax−1∼xlnaa^x - 1 \sim xlna

log⁡a(1+x)∼xlna\log a ^{(1 + x)} \sim \frac{x}{lna}

tan⁡x−x∼x−arctan⁡x∼x33\tan x - x \sim x - \arctan x \sim \frac{x^3}{3}

x−sin⁡x∼arcsin⁡x−x∼x36x - \sin x \sim \arcsin x - x \sim \frac{x^3}{6}

泰勒公式

ex=1+x+x22!+⋅⋅⋅+xnn!+o(xn)e^x = 1 + x + \frac{x^2}{2!} + ··· + \frac{x^n}{n!} +o(x^n)

11−x=1+x+x2+...+xn+o(xn)\frac{1}{1-x}=1 + x + x^2 + ...+ x^n + o(x^n)

11+x=1−x+x2+...+(−1)nxn+o(xn)\frac{1}{1+x}=1 - x + x^2 + ...+ (-1)^nx^n + o(x^n)

(1+x)α=1+αx+α(α−1)2!x2+⋅⋅⋅+α(α−1)⋅⋅⋅(α−n+1)n!xn+o(xn)(1 + x)^\alpha = 1 + \alpha x + \frac{\alpha (\alpha - 1)}{2!}x^2 + ··· + \frac{\alpha (\alpha - 1) ··· (\alpha - n + 1)}{n!}x^n + o(x^n)

ln⁡(1+x)=x−12x2+13x3−⋅⋅⋅+(−1)n1n+1xn+1+o(xn+1)\ln(1 + x) = x - \frac{1}{2}x^2 + \frac{1}{3}x^3 - ··· + (-1)^{n }\frac{1}{n+1}x^{n+1} + o(x^{n+1})

cos⁡x=1−12!x2+14!x4+o(x4)\cos x = 1 - \frac{1}{2!}x^2 + \frac{1}{4!}x^4 + o(x^{4})

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

tan⁡x=x+x33+215x5+o(x5)\tan x = x + \frac{x^3}{3} + \frac{2}{15} x^5 + o(x^5)

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

arcsin⁡x=x+16x3+340x5+o(x5)\arcsin x = x +\frac{1}{6} x^{3}+\frac{3}{40} x^{5} + o(x^{5})

sec⁡x=1+12x2+524x4+o(x4)\sec x = 1+\frac{1}{2} x^{2}+\frac{5}{24} x^{4}+o(x^{4})

csc⁡x=1x+16x+7360x3+o(x3)\csc x = \frac{1}{x}+\frac{1}{6} x+\frac{7}{360} x^{3}+o(x^3)

cot⁡x=1x−13x−145x3+o(x3)\cot x = \frac{1}{x}-\frac{1}{3} x-\frac{1}{45} x^{3}+o(x^3)

其他

当 x>0x>0 时, ln⁡(1+x)<x;sin⁡x<x\ln (1+x)<x ; \quad \sin x<x

lim⁡x→0\lim \atop {x \rightarrow 0}sin⁡xx=1\frac{\sin x}{x}=1

lim⁡x→0\lim\atop {x \rightarrow 0}(1+x)1x=e(1+x)^{\frac{1}{x}}=\mathrm{e}

lim⁡x→∞\lim \atop {x \rightarrow \infty}(1+1x)x=e\left(1+\frac{1}{x}\right)^{x}=\mathrm{e}

lim⁡x→0\lim \atop {x \rightarrow 0}ax−1x=ln⁡a\frac{a^{x}-1}{x}=\ln a

lim⁡x→∞\lim \atop {x \rightarrow \infty}nn=1\sqrt[n]{n}=1

lim⁡x→∞\lim \atop {x \rightarrow \infty}an=1,(a>0)\sqrt[n]{a}=1,(a>0)

lim⁡x→∞\lim\atop {x \rightarrow \infty}anxn+an−1xn−1+⋯+a1x+a0bmxm+bn−1xm−1+⋯+b1x+b0={anbm,n=m0,n<m∞,n>m\frac{a_{n} x^{n}+a_{n-1} x^{n-1}+\cdots+a_{1} x+a_{0}}{b_{m} x^{m}+b_{n-1} x^{m-1}+\cdots+b_{1} x+b_{0}}=\left\{\begin{array}{ll}\frac{a_{n}}{b_{m}}, & n=m \\ 0, & n<m \\ \infty, & n>m\end{array}\right.

x→+∞x \rightarrow+\infty 时
ln⁡αx≪xβ≪ax, 其中 α>0,β>0,a>1\ln ^{\alpha} x \ll x^{\beta} \ll a^{x}, \text { 其中 } \alpha>0, \beta>0, a>1
x→∞x \rightarrow \infty时
ln⁡αn≪nβ≪an≪n!≪nn,其中α>0,β>0,a>1\ln ^{\alpha} n \ll n^{\beta} \ll a^{n} \ll n ! \ll n^{n}, 其中\alpha>0, \beta>0, a>1

lim⁡n→∞\lim \atop {n \rightarrow \infty} a1n+a2n+⋯+amnn=a\sqrt[n]{a_{1}^{n}+a_{2}^{n}+\cdots+a_{m}^{n}}=a


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