泰山之管穿石,单极之绠断干。水非石之钻,索非木之锯,渐靡使之然也。

——东汉·班固《汉书·枚乘传》

本文封面为Rocky Ⅱ[1]中Rocky下定决心比赛后,早晨疯狂锻炼的场景。有了目标,便要不顾风雨兼程。

楔子

前两天看到 blackpenredpen曹老师 的视频,有感触,觉得对于数学的学习而言,刷题中才能真正学会东西。有些东西,看了不一定理解,理解了不一定会应用,用了不一定真正掌握。做题能很好的杂糅这一切,让理解更深入,记忆更加清晰。

时间线

4-3~

4-6

收集到22个,感觉没得写了。早上偶然看到mdnice群里有人发导数的笔记,然后又翻到了他之前的极限笔记。然而,笔记里第一题我都做的吃力,NND,再看才知晓是Wu老的高数17天。然后找来翻了翻,光极限就讲了57页😮,当然里面方法还是基本方法,但很多都是“稍稍”延伸了几步,却足以让我手足无措。这两天不能放松,好好理理思路。

4-7

要把等价无穷小推导一遍,不然太不好记了。

4-6

利用泰勒展开式推导出所有常见无穷小(4 →\to 50)

4-15

累觉不爱,多巴胺业已耗尽,五十道,了了之。

初出茅庐

这一部分有27道例题,主要介绍极限计算的基本方法。

lim⁡n→∞ 1n2+1+1n2+2+…1n2+n\begin{equation} \lim_{n\to \infty}\ \frac{1}{\sqrt{n^2+1}}+\frac{1}{\sqrt{n^2+2}}+\dots \frac{1}{\sqrt{n^2+n}} \end{equation}

display

提示:利用夹逼定理(🗣️哪—里—跑—)

1∗nn2+1≤bn≤1∗nn2+n\frac{1*n}{\sqrt{n^2+1}}\le b_n \le \frac{1*n}{\sqrt{n^2+n}}

lim⁡x→0ln⁡(1+4x2)sin⁡x2\begin{equation} \lim _{x \rightarrow 0} \frac{\ln \left(1+4 x^{2}\right)}{\sin x^{2}} \end{equation}

display

提示:等价无穷小

🥕∼sin⁡(🥕)∼ln⁡(1+🥕)🥕 \sim \sin{(🥕)}\sim \ln(1+🥕)

lim⁡x→0ln⁡(1+4x2)sin⁡x2=4x2x2= 4 \begin{aligned} & \lim _{x \rightarrow 0} \frac{\ln \left(1+4 x^{2}\right)}{\sin x^{2}} \\ &= \frac{4 x^{2}}{x^{2}} \\ &=\ 4 \end{aligned}

lim⁡x→0x3sin⁡1x3\begin{equation} \lim _{x \rightarrow 0} x^{3} \sin \frac{1}{x^{3}} \end{equation}

display

提示:注意等价无穷小的条件

∵x→0, x3为无穷小,∣sin⁡1x3∣≤1无穷小与有界变量的乘积仍为无穷小∴lim⁡x→0x3sin⁡1x3=0\because x \to 0,\ x^3\text{为无穷小},|\sin{\frac{1}{x^3}}|\le 1 \\ {\color{blue} \text{无穷小与有界变量的乘积仍为无穷小}}\\ \therefore \lim _{x \rightarrow 0} x^{3} \sin \frac{1}{x^{3}}= 0

lim⁡x→0sin⁡x−tan⁡xx3\begin{equation} \lim _{x \rightarrow 0} \frac{\sin x-\tan x}{x^{3}} \end{equation}

display

提示:拼凑等价无穷小

lim⁡x→0sin⁡x−tan⁡xx3=lim⁡x→0sin⁡x(1−1cos⁡x)x3=lim⁡x→0sin⁡x(cos⁡x−1)x3cos⁡x=lim⁡x→0x⋅(−12x2)x3=−12\begin{aligned} & \lim _{x \rightarrow 0} \frac{\sin x-\tan x}{x^{3}}\\ &=\lim _{x \rightarrow 0} \frac{\sin x\left(1-\frac{1}{\cos x}\right)}{x^{3}} \\ &=\lim _{x \rightarrow 0} \frac{\sin x(\cos x-1)}{x^{3} \cos x} \\ &=\lim _{x \rightarrow 0} \frac{x \cdot\left(-\frac{1}{2} x^{2}\right)}{x^{3}}\\ &=-\frac{1}{2} \end{aligned}

lim⁡x→0(1+xex)1x\begin{equation} \lim _{x \rightarrow 0}\left(1+x e^{x}\right)^{\frac{1}{x}} \end{equation}

display

提示:1∞1^\infty常规思路·第一弹

lim⁡x→0(1+🥕)1🥕=e(🥕≠0)\lim_{x\to 0} (1+🥕)^{\frac{1}{🥕}}=e \quad{(🥕\ne0)}

lim⁡x→0(1+xex)1x=lim⁡x→0(1+xex)1xex⋅xex⋅1x=lim⁡x→0ex=elim⁡x→0ex=e\begin{aligned} & \lim _{x \rightarrow 0}\left(1+x e^{x}\right)^{\frac{1}{x}} \\ &= \lim _{x \rightarrow 0}\left(1+x e^{x}\right)^{\frac{1}{x e^{x}}} \cdot x e^{x} \cdot \frac{1}{x} \\ &= \lim _{x \rightarrow 0} e^{x} \\ &= e^{\lim _{x \rightarrow 0} e^{x}} \\ &= e \end{aligned}

lim⁡x→0(1−tan⁡x1+tan⁡x)1−sin⁡2x\begin{equation} \lim _{x \rightarrow 0}\left(\frac{1-\tan x}{1+\tan x}\right)^{\frac{1}{-\sin 2 x}} \end{equation}

display

提示:1∞1^\infty常规思路·第二弹

lim⁡x→0(1−tan⁡x1+tan⁡x)1−sin⁡2x=lim⁡x→0(1+(1−tan⁡x1+tan⁡x−1))11−tan⁡x1+tan⁡x−1×−2tan⁡x1+tan⁡x1−sin⁡2x=lim⁡x→0e−2tan⁡x1+tan⁡x1−sin⁡2x=lim⁡x→0e−2x1+tan⁡x1−2x=lim⁡x→0e11+tan⁡x=e\begin{aligned} &\lim _{x \rightarrow 0}\left(\frac{1-\tan x}{1+\tan x}\right)^{\frac{1}{-\sin 2 x}}\\ &=\lim _{x \rightarrow 0}\left(1+(\frac{1-\tan x}{1+\tan x}-1)\right)^{\frac{1}{\frac{1-\tan x}{1+\tan x}-1}\times \frac{-2\tan x}{1+\tan x}\frac{1}{-\sin 2 x}}\\ &=\lim _{x \rightarrow 0}e^{ \frac{-2\tan x}{1+\tan x}\frac{1}{-\sin 2 x}}\\ &=\lim _{x \rightarrow 0}e^{ \frac{-2 x}{1+\tan x}\frac{1}{- 2 x}}\\ &=\lim _{x \rightarrow 0}e^{ \frac{1}{1+\tan x}}\\ &=e \end{aligned}

lim⁡n→∞(n2+n−n)\begin{equation} \lim_{n\to \infty} (\sqrt{n^2+n}-n) \end{equation}

From Deyi

提示:常规思路:平方差拼凑

lim⁡n→∞(n2+n−n)=lim⁡n→∞(n2+n−n1)=lim⁡n→∞(n2+n−n2n2+n+n)=lim⁡n→∞(nn2+n+n)=lim⁡n→∞(11+1n+1)=12\begin{aligned} &\lim_{n\to \infty} (\sqrt{n^2+n}-n)\\ &=\lim_{n\to \infty} (\frac{\sqrt{n^2+n}-n}{1})\\ &=\lim_{n\to \infty} (\frac{n^2+n-n^2}{\sqrt{n^2+n}+n)}\\ &=\lim_{n\to \infty} (\frac{n}{\sqrt{n^2+n}+n)}\\ &=\lim_{n\to \infty} (\frac{1}{\sqrt{1+\frac{1}{n}}+1})\\ &=\frac{1}{2}\\ \end{aligned}

lim⁡x→∞x(x+2−x−3)\begin{equation} \lim_{x\to \infty} \sqrt{x}(\sqrt{x+2}-\sqrt{x-3}) \end{equation}

From Deyi

提示:常规思路:平方差拼凑

lim⁡x→∞x(x+2−x−3)=lim⁡x→∞x(x+2−x−3)1=lim⁡x→∞x×5x+2+x−3)=lim⁡x→∞51+2/x+1−3/x)=52\begin{aligned} &\lim_{x\to \infty} \sqrt{x}(\sqrt{x+2}-\sqrt{x-3})\\ &=\lim_{x\to \infty} \frac{\sqrt{x}(\sqrt{x+2}-\sqrt{x-3})}{1}\\ &=\lim_{x\to \infty} \frac{\sqrt{x}\times 5}{\sqrt{x+2}+\sqrt{x-3})}\\ &=\lim_{x\to \infty} \frac{ 5}{\sqrt{1+2/x}+\sqrt{1-3/x})}\\ &=\frac{5}{2} \end{aligned}

lim⁡x→0(1x−1ex−1)\begin{equation} \lim _{x \rightarrow 0}\left(\frac{1}{x}-\frac{1}{e^{x}-1}\right) \end{equation}

1987卷三

提示:凑乘积形式,等价无穷小+洛必达

lim⁡x→0(1x−1ex−1)=lim⁡x→0(ex−1−x(ex−1)x)=lim⁡x→0(ex−1−xx2)=lim⁡x→0(ex−12x)=lim⁡x→0(ex2)=12\begin{aligned} &\lim _{x \rightarrow 0}\left(\frac{1}{x}-\frac{1}{e^{x}-1}\right)\\ &=\lim _{x \rightarrow 0}\left(\frac{e^x-1-x}{(e^x-1)x}\right)\\ &=\lim _{x \rightarrow 0}\left(\frac{e^x-1-x}{x^2}\right)\\ &=\lim _{x \rightarrow 0}\left(\frac{e^x-1}{2x}\right)\\ &=\lim _{x \rightarrow 0}\left(\frac{e^x}{2}\right)\\ &=\frac{1}{2} \end{aligned}

lim⁡x→0(x−sin⁡x)e−x21−x3−1\begin{equation} \lim_{x\to 0} \frac{(x-\sin x) e^{-x^2}}{\sqrt{1-x^3}-1} \end{equation}

display

提示:等价无穷小替换

(1+🥕)a−1∼a🥕(1+🥕)^a-1 \sim a🥕

lim⁡x→0(x−sin⁡x)e−x21−x3−1=lim⁡x→0e−x2×lim⁡x→0x−sin⁡x1/2×(−x3)=−2×lim⁡x→0x−sin⁡xx3洛必达法则=−2×lim⁡x→01−cos⁡x3x2=−2×lim⁡x→01/2×x23x2=−13\begin{aligned} &\lim_{x\to 0} \frac{(x-\sin x) e^{-x^2}}{\sqrt{1-x^3}-1}\\ &= \lim_{x\to 0} e^{-x^2}\times \lim_{x\to 0} \frac{x-\sin x}{1/2\times (-x^3)}\\ &= -2\times \lim_{x\to 0} \frac{x-\sin x}{x^3}\qquad \text{洛必达法则}\\ &= -2\times \lim_{x\to 0} \frac{1-\cos x}{3x^2}\\ &= -2\times \lim_{x\to 0} \frac{1/2 \times x^2}{3x^2}\\ &=- \frac{1}{3} \end{aligned}

lim⁡x→0x−sin⁡2xx+sin⁡5x\begin{equation} \lim_{x\to 0} \frac{x-\sin 2x}{x + \sin 5x} \end{equation}

display

提示:加减法使用等价无穷小的条件

∵\because 当 x→0x \rightarrow 0 时, sin⁡2x∼2x,sin⁡5x∼5x\sin 2 x \sim 2 x, \sin 5 x \sim 5 x, 且 lim⁡x→0sin⁡2xx\lim _{x \rightarrow 0} \frac{\sin 2 x}{x} =2≠1,lim⁡x→0sin⁡5xx=5≠−1=2 \neq 1, \lim _{x \rightarrow 0} \frac{\sin 5 x}{x}=5 \neq-1,

满足等价无穷小替换对加减法成立的条件,

∴lim⁡x→0x−sin⁡2xx+sin⁡5x=lim⁡x→0x−2xx+5x=−16\therefore \lim _{x \rightarrow 0} \frac{x-\sin 2 x}{x+\sin 5 x}=\lim _{x \rightarrow 0} \frac{x-2 x}{x+5 x}=-\frac{1}{6}

lim⁡x→∞(cos⁡1x)x2\begin{equation} \lim _{x \rightarrow \infty}\left(\cos \frac{1}{x}\right)^{x^{2}} \end{equation}

display

提示:1∞1^{\infty}型·第三弹

lim⁡x→∞(cos⁡1x)x2=lim⁡x→∞[1+(1cos⁡x−1)]11cos⁡x−1×(1cos⁡x−1)×x2=elim⁡x→∞(cos⁡1x−1)x2=elim⁡x→∞cos⁡1x−1(1x)2=elim⁡x→∞−12(1x)2(−1x)2=e−12=1e\begin{aligned} &\displaystyle \lim _{x \rightarrow \infty}\left(\cos \frac{1}{x}\right)^{x^{2}}\\ &=\displaystyle\lim_{x\to \infty}[1+(\frac{1}{\cos x}-1)]^{\frac{1}{\frac{1}{\cos x}-1}\times (\frac{1}{\cos x}-1)\times x^2}\\ &=e^{\displaystyle\lim_{x\to \infty}\left(\cos \frac{1}{x}-1\right) x^{2}}\\ &=e^{\displaystyle\lim_{x\to \infty} \frac{\cos \frac{1}{x}-1}{\left(\frac{1}{x}\right)^{2}}}\\ &=e^{\displaystyle\lim_{x\to \infty} \frac{-\frac{1}{2}\left(\frac{1}{x}\right)^{2}}{\left(-\frac{1}{x}\right)^{2}}}\\ &=e^{^{-\frac{1}{2}}}\\ &=\frac{1}{\sqrt{e}} \end{aligned}

lim⁡x→∞(x+a)x+a(x+b)x+b(x+a+b)2x+a+b\begin{equation} \lim _{x \rightarrow \infty} \frac{(x+a)^{x+a}(x+b)^{x+b}}{(x+a+b)^{2 x+a+b}} \end{equation}

From Zhongxiang-17Days

提示:1∞1^{\infty}型·第四弹

lim⁡x→∞(x+a)x+a(x+b)x+b(x+a+b)2x+a+b=lim⁡x→∞(x+a)x+a(x+a+b)x+a⋅(x+b)x+b(x+a+b)x+b=lim⁡x→∞1(1+bx+a)x+a⋅1(1+ax+b)x+b=1eb⋅1ea=e−(a+b)\begin{aligned} &\lim _{x \rightarrow \infty} \frac{(x+a)^{x+a}(x+b)^{x+b}}{(x+a+b)^{2 x+a+b}}\\ &=\lim _{x \rightarrow \infty} \frac{(x+a)^{x+a}}{(x+a+b)^{x+a}} \cdot \frac{(x+b)^{x+b}}{(x+a+b)^{x+b}} \\ &=\lim _{x \rightarrow \infty} \frac{1}{\left(1+\frac{b}{x+a}\right)^{x+a}} \cdot \frac{1}{\left(1+\frac{a}{x+b}\right)^{x+b}} \\ &=\frac{1}{\mathrm{e}^{b}} \cdot \frac{1}{\mathrm{e}^{a}} \\ &=\mathrm{e}^{-(a+b)} \end{aligned}

lim⁡x→0[ln⁡(x+1+x2)x]11−cos⁡x\begin{equation} \lim _{x \rightarrow 0}\left[\frac{\ln (x+\sqrt{1+x^{2}})}{x}\right]^{\frac{1}{1-\cos x}} \end{equation}

From Zhongxiang-17Days

提示:1∞1^{\infty}型·第五弹,常规思路

lim⁡x→0[ln⁡(x+1+x2)x]11−cos⁡x=lim⁡x→0[1+ln⁡(x+1+x2)−xx]11−cos⁡x=lim⁡x→0eln⁡(x+1+x2)−xx(1−cos⁡x)幂化简:lim⁡x→0ln⁡(x+1+x2)−xx⋅12x2=lim⁡x→011+x2−132x2=lim⁡x→0−12x232x2=−13原式=e−13\begin{aligned} &\lim _{x \rightarrow 0}\left[\frac{\ln \left(x+\sqrt{1+x^{2}}\right)}{x}\right]^{\frac{1}{1-\cos x}}\\ &=\lim _{x \rightarrow 0}\left[1+\frac{\ln \left(x+\sqrt{1+x^{2}}\right)-x}{x}\right]^{\frac{1}{1-\cos x}} \\ &=\lim _{x \rightarrow 0} e^{\frac{\ln (x + \sqrt{1+x^2})-x}{x(1-\cos x )}}\\ \text{幂化简:}&\color{blue}\lim _{x \rightarrow 0} \frac{\ln \left(x+\sqrt{1+x^{2}}\right)-x}{x \cdot \frac{1}{2} x^{2}} \\ &\color{blue}=\lim _{x \rightarrow 0} \frac{\frac{1}{\sqrt{1+x^{2}}}-1}{\frac{3}{2} x^{2}} \\ &\color{blue}=\lim _{x \rightarrow 0} \frac{-\frac{1}{2} x^{2}}{\frac{3}{2} x^{2}}\\ &\color{blue}=-\frac{1}{3}\\ \text{原式}&=e^{-\frac{1}{3}}\\ \end{aligned}

lim⁡n→∞(π2−arctan⁡n)1ln⁡n\begin{equation} \lim _{n \rightarrow \infty}\left(\frac{\pi}{2}-\arctan n\right)^{\frac{1}{\ln n}} \end{equation}

From Zhongxiang-17Days

提示:1∞1^{\infty}型·变体,思路还是一样的,幂运算变乘法

lim⁡n→∞(π2−arctan⁡n)1ln⁡n=lim⁡n→∞eln⁡(π/2−arctan⁡x)ln⁡x幂化简:lim⁡n→∞ln⁡(π/2−arctan⁡x)ln⁡x=lim⁡x→+∞1π2−arctan⁡x⋅(−11+x2)1x=−lim⁡x→+∞1xπ2−arctan⁡x=−lim⁡x→+∞−1x2−11+x2=−1原式=e−1\begin{aligned} &\lim _{n \rightarrow \infty}\left(\frac{\pi}{2}-\arctan n\right)^{\frac{1}{\ln n}}\\ &=\lim _{n \rightarrow \infty}e^{\frac{\ln (\pi /2 - \arctan x)}{\ln x}}\\ \text{幂化简:}&\color{blue}\lim _{n \rightarrow \infty} \frac{\ln (\pi /2 - \arctan x)}{\ln x}\\ &\color{blue}=\lim _{x \rightarrow+\infty} \frac{\frac{1}{\frac{\pi}{2}-\arctan x} \cdot\left(-\frac{1}{1+x^{2}}\right)}{\frac{1}{x}}\\ &\color{blue}=-\lim _{x \rightarrow+\infty} \frac{\frac{1}{x}}{\frac{\pi}{2}-\arctan x} \\ &\color{blue}=-\lim _{x \rightarrow+\infty} \frac{-\frac{1}{x^{2}}}{-\frac{1}{1+x^{2}}} \\ &\color{blue}=-1\\ \text{原式}&=e^{-1}\\ \end{aligned}

lim⁡x→01−cos⁡2x−12xsin⁡2xx2(ex2−1)\begin{equation} \lim_{x\to 0} \frac{1-\cos^2x-\frac{1}{2} x \sin 2x}{x^2(e^{x^2}-1)} \end{equation}

display

提示:多次使用洛必达法则

lim⁡x→01−cos⁡2x−12xsin⁡2xx2(ex2−1)=lim⁡x→01−cos⁡2x−12xsin⁡2xx2×x2上下都趋近于0,使用洛必达法则=lim⁡x→02cos⁡xsin⁡x−12sin⁡2x−cos⁡2x×x4x3=lim⁡x→012sin⁡2x−cos⁡2x×x4x3上下都趋近于0,使用洛必达法则=lim⁡x→0cos⁡2x−cos⁡2x+sin⁡2x×2x12x2=lim⁡x→02x×2x12x2=13\begin{aligned} &\displaystyle \lim_{x\to 0} \frac{1-\cos^2x-\frac{1}{2} x \sin 2x}{x^2(e^{x^2}-1)}\\ &=\displaystyle \lim_{x\to 0} \frac{1-\cos^2x-\frac{1}{2} x \sin 2x}{x^2\times x^2}\qquad \text{上下都趋近于0,使用洛必达法则}\\ &=\displaystyle \lim_{x\to 0} \frac{2\cos x\sin x-\frac{1}{2}\sin 2x-\cos 2x\times x}{4x^3}\\ &=\displaystyle \lim_{x\to 0} \frac{\frac{1}{2}\sin 2x-\cos 2x\times x}{4x^3}\qquad \text{上下都趋近于0,使用洛必达法则}\\ &=\displaystyle \lim_{x\to 0} \frac{\cos 2x-\cos 2x+\sin 2x\times 2 x}{12x^2}\\ &=\displaystyle \lim_{x\to 0} \frac{ 2x\times 2 x}{12x^2}\\ &=\frac{1}{3} \end{aligned}

lim⁡x→0(1x2−1sin⁡2x)\begin{equation} \lim _{x\to 0}(\frac{1}{x^2}-\frac{1}{\sin^2x}) \end{equation}

display

提示:多次使用洛必达法则

lim⁡x→0(1x2−1sin⁡2x)=lim⁡x→0sin⁡2x−x2x2sin⁡2x上下都趋近于0,使用洛必达法则=lim⁡x→0sin⁡2x−2x4x3上下都趋近于0,使用洛必达法则=lim⁡x→02cos⁡2x−212x2=lim⁡x→0cos⁡2x−16x2=lim⁡x→012(2x)26x2=13\begin{aligned} &\displaystyle\lim _{x\to 0}(\frac{1}{x^2}-\frac{1}{\sin^2x})\\ &=\displaystyle\lim _{x\to 0}\frac{\sin^2x-x^2}{x^2 \sin^2x}\qquad \text{上下都趋近于0,使用洛必达法则}\\ &=\displaystyle\lim _{x\to 0}\frac{\sin 2x-2x}{4x^3}\qquad \text{上下都趋近于0,使用洛必达法则} \\ &=\displaystyle\lim _{x\to 0}\frac{2\cos 2x-2}{12x^2} \\ &=\displaystyle\lim _{x\to 0}\frac{\cos 2x-1}{6x^2} \\ &=\displaystyle\lim _{x\to 0}\frac{\frac{1}{2} (2x)^2}{6x^2}\\ &=\frac{1}{3} \end{aligned}

lim⁡x→0(cos⁡xcos⁡2x)1x2\begin{equation} \lim _{x \rightarrow 0} (\frac{\cos x}{\cos 2x})^{\frac{1}{x^2}} \end{equation}

display

提示:等价无穷小之 加不反

lim⁡x→0(cos⁡xcos⁡2x)1x2=elim⁡x→0(cos⁡xcos⁡2x−1)x2=elim⁡x→0cos⁡x−cos⁡2xx2cos⁡2x=elim⁡x→0cos⁡x−cos⁡2xx2=elim⁡x→0−sin⁡x+2sin⁡2x2x∵lim⁡x→0−sin⁡x2sin⁡2x≠−1=e32\begin{aligned} &\lim _{x \rightarrow 0} (\frac{\cos x}{\cos 2x})^{\frac{1}{x^2}}\\ &=\mathrm{e}^{\displaystyle \lim_{x\to 0} \frac{\left(\frac{\cos x}{\cos 2 x}-1\right)}{x^{2}}}\\ &=\mathrm{e}^{\displaystyle \lim_{x\to 0} \frac{\cos x-\cos 2x}{x^2 \cos 2 x}}\\ &=\mathrm{e}^{\displaystyle \lim_{x\to 0} \frac{\cos x-\cos 2x}{x^2 }}\\ &=\mathrm{e}^{\displaystyle \lim_{x\to 0} \frac{-\sin x+2 \sin 2 x}{2 x}}\qquad \because \lim_{x\to 0}\frac{-\sin x}{2\sin 2x}\ne -1\\ &=\mathrm{e}^{\frac{3}{2}} \end{aligned}

lim⁡x→0[sin⁡x−sin⁡(sin⁡x)]⋅sin⁡xx4\begin{equation} \lim _{x \rightarrow 0} \frac{[\sin x-\sin (\sin x)] \cdot \sin x}{x^{4}} \end{equation}

display

提示:等价无穷小+洛必达法则

lim⁡x→0[sin⁡x−sin⁡(sin⁡x)]⋅sin⁡xx4=lim⁡x→0cos⁡x−cos⁡(sin⁡x)⋅cos⁡x3x2=lim⁡x→0cos⁡x×lim⁡x→01−cos⁡(sin⁡x)3x2=lim⁡x→012sin⁡2x3x2=lim⁡x→01x26x2=16\begin{aligned} &\lim _{x \rightarrow 0} \frac{[\sin x-\sin (\sin x)] \cdot \sin x}{x^{4}} \\ &=\lim _{x \rightarrow 0} \frac{\cos x-\cos (\sin x) \cdot \cos x}{3 x^{2}} \\ &=\lim _{x \rightarrow 0} \cos x \times \lim _{x \rightarrow 0} \frac{1-\cos (\sin x)}{3 x^{2}} \\ &=\lim _{x \rightarrow 0} \frac{\frac{1}{2} \sin ^{2} x}{3 x^{2}} \\ &=\lim _{x \rightarrow 0} \frac{1 x^{2}}{6 x^{2}} \\ &=\frac{1}{6} \end{aligned}

求正的常数a与b,使下式成立:lim⁡x→01bx−sin⁡x∫0xt2a+t2dt=1\begin{equation} \text{求正的常数a与b,使下式成立:} \lim _{x \rightarrow 0} \frac{1}{b x-\sin x} \int_{0}^{x} \frac{t^{2}}{\sqrt{a+t^{2}}} d t=1 \end{equation}

1987卷一

提示:洛必达+等价无穷小,看见积分,必定洛必达。

lim⁡x→01bx−sin⁡x∫0xt2a+t2dt=1lim⁡x→0x2a+x2b−cos⁡x=1lim⁡x→01a+x2×lim⁡x→0x2b−cos⁡x=11a×lim⁡x→0x2b−cos⁡x=1🥝1a×lim⁡x→01bx21−1bcos⁡x=11a×lim⁡x→01bx212bx2−1b+1=11a×2=1a=4(a=4→🥝)⟹b=1\begin{aligned} \lim _{x \rightarrow 0} \frac{1}{b x-\sin x} \int_{0}^{x} \frac{t^{2}}{\sqrt{a+t^{2}}} d t&=1\\ \lim _{x \rightarrow 0}\frac{ \frac{x^{2}}{\sqrt{a+x^{2}}} }{ {b -\cos x}}&=1\\ \lim _{x \rightarrow 0} \frac{1}{\sqrt{a+x^{2}}}\times \lim _{x \rightarrow 0}\frac{ x^{2} }{ {b -\cos x}}&=1\\ \frac{1}{\sqrt{a}}\times \lim _{x \rightarrow 0}\frac{ x^{2} }{ {b -\cos x}}&=1\qquad \text{🥝}\\ \frac{1}{\sqrt{a}}\times \lim _{x \rightarrow 0}\frac{1}{b} \frac{ x^{2} }{ {1 -\frac{1}{b}\cos x}}&=1\\ \frac{1}{\sqrt{a}}\times \lim _{x \rightarrow 0}\frac{1}{b} \frac{ x^{2} }{ \frac{1}{2b}x^2-\frac{1}{b}+1}&=1\\ \frac{1}{\sqrt{a}}\times2&=1\\ a&=4\\ (a=4\to\text{🥝})\Longrightarrow b&=1 \end{aligned}

lim⁡x→0∫0x(x−t)sin⁡t2 dt(x2+x3)(1−1−x2)\begin{equation} \lim _{x \rightarrow 0} \frac{\int_{0}^{x}(x-t) \sin t^{2} \mathrm{~d} t}{\left(x^{2}+x^{3}\right)\left(1-\sqrt{1-x^{2}}\right)} \end{equation}

ShowTime

提示:看见积分,必定洛必达,但也要注意顺序。

lim⁡x→0∫0x(x−t)sin⁡t2 dt(x2+x3)(1−1−x2)=lim⁡x→0x∫0xsin⁡t2 dt−∫0xtsin⁡t2 dt(x2+x3)⋅12x2=lim⁡x→0x∫0xsin⁡t2 dt−∫0xtsin⁡t2 dt12x4快使用洛必达,哼哼哈嘿!=lim⁡x→0∫0xsin⁡t2 dt+xsin⁡x2−xsin⁡x22x3=lim⁡x→0sin⁡x26x2=16\begin{aligned} &\lim _{x \rightarrow 0} \frac{\int_{0}^{x}(x-t) \sin t^{2} \mathrm{~d} t}{\left(x^{2}+x^{3}\right)\left(1-\sqrt{1-x^{2}}\right)}\\ &=\lim _{x \rightarrow 0} \frac{x \int_{0}^{x} \sin t^{2} \mathrm{~d} t-\int_{0}^{x} t \sin t^{2} \mathrm{~d} t}{\left(x^{2}+x^{3}\right) \cdot \frac{1}{2} x^{2}} \\ &=\lim _{x \rightarrow 0} \frac{ x \int_{0}^{x} \sin t^{2} \mathrm{~d} t- \int_{0}^{x} t \sin t^{2} \mathrm{~d} t}{\frac{1}{2} x^{4}} \quad \text{快使用洛必达,哼哼哈嘿!} \\ &=\lim _{x \rightarrow 0} \frac{\int_{0}^{x} \sin t^{2} \mathrm{~d} t+x \sin x^{2}-x \sin x^{2}}{2 x^{3}} \\ &=\lim _{x \rightarrow 0} \frac{\sin x^{2}}{6 x^{2}}\\&=\frac{1}{6} \end{aligned}

lim⁡x→0[1ex−1−1ln⁡(1+x)]\begin{equation} \lim _{x \rightarrow 0}\left[\frac{1}{e^{x}-1}-\frac{1}{\ln (1+x)}\right] \end{equation}

display

提示:等价无穷小+洛必达法则

lim⁡x→0[1ex−1−1ln⁡(1+x)]=lim⁡x→0ln⁡(1+x)−ex+1(ex−1)ln⁡(1+x)=lim⁡x→0ln⁡(1+x)−ex+1x⋅x=lim⁡x→011+x−ex2x上下都趋近于0,使用洛必达法则=12lim⁡x→01−ex(1+x)x⋅lim⁡x→011+x=12lim⁡x→0(1−ex(1+x))′x′=−12lim⁡x→0(ex(2+x))=−1.\begin{aligned} &\lim _{x \rightarrow 0}\left[\frac{1}{\mathrm{e}^{x}-1}-\frac{1}{\ln (1+x)}\right]\\&=\lim _{x \rightarrow 0} \frac{\ln (1+x)-\mathrm{e}^{x}+1}{\left(\mathrm{e}^{x}-1\right) \ln (1+x)}\\&=\lim _{x \rightarrow 0} \frac{\ln (1+x)-\mathrm{e}^{x}+1}{x \cdot x} \\& = \lim _{x \rightarrow 0} \frac{\frac{1}{1+x}-\mathrm{e}^{x}}{2 x}\qquad \text{上下都趋近于0,使用洛必达法则} \\ &=\frac{1}{2} \lim _{x \rightarrow 0} \frac{1-\mathrm{e}^{x}(1+x)}{x} \cdot \lim _{x \rightarrow 0} \frac{1}{1+x}\\&=\frac{1}{2} \lim _{x \rightarrow 0} \frac{\left(1-\mathrm{e}^{x}(1+x)\right)^{\prime}}{x^{\prime}}\\&=-\frac{1}{2} \lim _{x \rightarrow 0}\left(\mathrm{e}^{x}(2+x)\right)\\&=-1 . \end{aligned}

lim⁡x→0x2sin⁡1xx+sin⁡x\begin{equation} \lim _{x \rightarrow 0} \frac{x^{2} \sin \frac{1}{x}}{x+\sin x} \end{equation}

From Zhongxiang-17Days

提示:请不要用洛必达!!

简单分析一下,可以发现这是一个00\frac{0}{0}型极限,要是你手痒痒直接用了,就会陷入绝境: 原式 =lim⁡x→02xsin⁡1x−cos⁡1x1+cos⁡x\text { 原式 }=\lim _{x \rightarrow 0} \frac{2 x \sin \frac{1}{x}-\cos \frac{1}{x}}{1+\cos x}

实际上这道题的意义就是告诉你要注意洛必达的条件:求导后的极限存在才能用洛必达。

 正解:原式 =lim⁡x→0xsin⁡1x1+sin⁡xx=02=0\text { 正解:原式 }=\lim _{x \rightarrow 0} \frac{x \sin \frac{1}{x}}{1+\frac{\sin x}{x}}=\frac{0}{2}=0


拉格朗日中值定理专区

如果函数 f(x)f(x) 在闭区间 [a,b][a, b] 上连续,在开区间 (a,b)(a, b) 上可㝵,那么在开区间 (a,b)(a, b) 内至少存在一点 ξ\xi 使得 :

f′(ξ)=f(b)−f(a)b−af^{\prime}(\xi)=\frac{f(b)-f(a)}{b-a}

这个方法神奇的紧!

lim⁡x→0cos⁡(sin⁡x)−cos⁡xarcsin⁡4x\begin{equation} \lim _{x \rightarrow 0} \frac{\cos (\sin x)-\cos x}{\arcsin ^{4} x} \end{equation}

From Jin

提示:

lim⁡x→0cos⁡(sin⁡x)−cos⁡xarcsin⁡4x=lim⁡x→0−sin⁡ξ⋅(sin⁡x−x)x4\lim _{x \rightarrow 0} \frac{\cos (\sin x)-\cos x}{\arcsin ^{4} x}=\lim _{x \rightarrow 0} \frac{-\sin \xi \cdot(\sin x-x)}{x^{4}}

ξ\xi介于sin⁡x\sin x 与xx之间,由夹逼定理可以得到lim⁡x→0sin⁡ξx=1\lim_{x\to 0}\frac{\sin \xi}{x}=1

lim⁡x→0cos⁡(sin⁡x)−cos⁡xarcsin⁡4x=lim⁡x→0−(sin⁡x−x)x3=lim⁡x→01−cos⁡x3x2=16\begin{aligned} &\lim _{x \rightarrow 0} \frac{\cos (\sin x)-\cos x}{\arcsin ^{4} x}\\ &=\lim _{x \rightarrow 0} \frac{-(\sin x-x)}{x^{3}}\\ &=\lim _{x \rightarrow 0} \frac{1-\cos x}{3 x^{2}}&\\ &=\frac{1}{6}\\ \end{aligned}

驾轻就熟

lim⁡x→0[ax−(1x2−a2)ln⁡(1+ax)](a≠0)\begin{equation} \lim _{x \rightarrow 0}\left[\frac{a}{x}-\left(\frac{1}{x^{2}}-a^{2}\right) \ln (1+a x)\right](a \neq 0) \end{equation}

1997数三

提示:等价无穷小推论

lim⁡x→0[ax−(1x2−a2)ln⁡(1+ax)]=lim⁡x→0[ax−ln⁡(1+ax)x2]+lim⁡x→0a2ln⁡(1+ax)=lim⁡x→0ax−ln⁡(1+ax)x2=lim⁡x→012(ax)2x2(🥕−ln⁡(1+🥕)∼12🥕2)=a22.\begin{aligned} &\lim _{x \rightarrow 0}\left[\frac{a}{x}-\left(\frac{1}{x^{2}}-a^{2}\right) \ln (1+a x)\right]\\ &=\lim _{x \rightarrow 0}\left[\frac{a}{x}-\frac{\ln (1+a x)}{x^{2}}\right]+\lim _{x \rightarrow 0} a^{2} \ln (1+a x) \\ &=\lim _{x \rightarrow 0} \frac{a x-\ln (1+a x)}{x^{2}} \\ &=\lim _{x \rightarrow 0} \frac{\frac{1}{2}(a x)^{2}}{x^{2}} {\color{red}\quad\left(🥕-\ln (1+🥕) \sim \frac{1}{2} 🥕^{2}\right)} \\ &=\frac{a^{2}}{2} . \end{aligned}

lim⁡x→+∞[(nx)n+1]n+1(x+1)(x2+2)⋯(xn+n)\begin{equation} \lim _{x \rightarrow+\infty} \frac{\sqrt{\left[(n x)^{n}+1\right]^{n+1}}}{(x+1)\left(x^{2}+2\right) \cdots\left(x^{n}+n\right)} \end{equation}

From Zhongxiang-17Days

提示:找到相同的项,消消消,提取出来x,凑出来可以计算的无穷小。

lim⁡x→+∞[(nx)n+1]n+1(x+1)(x2+2)⋯(xn+n)=lim⁡x→+∞(nn+1xn)n+12(1+1x)(1+2x2)⋯(1+nxn)=nn(n+1)2\begin{aligned} &\lim _{x \rightarrow+\infty} \frac{\sqrt{\left[(n x)^{n}+1\right]^{n+1}}}{(x+1)\left(x^{2}+2\right) \cdots\left(x^{n}+n\right)}\\ &=\lim _{x \rightarrow+\infty} \frac{\left(n^{n}+\frac{1}{x^{n}}\right)^{\frac{n+1}{2}}}{\left(1+\frac{1}{x}\right)\left(1+\frac{2}{x^{2}}\right) \cdots\left(1+\frac{n}{x^{n}}\right)}\\ &=n^{\frac{n(n+1)}{2}} \end{aligned}

lim⁡x→0x2(ex−1)1+tan⁡x−1+x\begin{equation} \lim_{x\to 0} \frac{x^2(e^x-1)}{\sqrt{1+\tan x}-\sqrt{1+ x}} \end{equation}

From Deyi

提示:泰勒展开式

tan⁡x=∑n=1∞B2n(−4)n(1−4n)(2n)!x2n−1=x+13x3+215x5+17315x7+622835x9+1382155925x11+218446081075x13+929569638512875x15+⋯x∈(−1,1)\tan x=\sum_{n=1}^{\infty} \frac{B_{2 n}(-4)^{n}\left(1-4^{n}\right)}{(2 n) !} x^{2 n-1}=x+\frac{1}{3} x^{3}+\frac{2}{15} x^{5}+\frac{17}{315} x^{7}+\frac{62}{2835} x^{9}+\frac{1382}{155925} x^{11}+\frac{21844}{6081075} x^{13}+\frac{929569}{638512875} x^{15}+\cdots x \in(-1,1)

lim⁡x→0x2(ex−1)1+tan⁡x−1+x=lim⁡x→0x3×(1+tan⁡x+1+x)tan⁡x−x=lim⁡x→0x3×2tan⁡x−x=lim⁡x→0x3×213x3=6\begin{aligned} &\lim_{x\to 0} \frac{x^2(e^x-1)}{\sqrt{1+\tan x}-\sqrt{1+ x}}\\ &=\lim_{x\to 0} \frac{x^3\times(\sqrt{1+\tan x}+\sqrt{1+ x})}{\tan x-x}\\ &=\lim_{x\to 0} \frac{x^3\times2}{\tan x-x}\\ &=\lim_{x\to 0} \frac{x^3\times2}{\frac{1}{3}x^3}\\ &=6 \end{aligned}

lim⁡x→04x2+x−1+x+1x2+sin⁡x\begin{equation} \lim_{x\to 0} \frac{\sqrt{4x^2+x-1}+x+1}{\sqrt{x^2+\sin x}} \end{equation}

From Deyi

提示:除以出现次数最多的,最讨厌的那一项。

lim⁡x→04x2+x−1+x+1x2+sin⁡x=lim⁡x→∞4+1x−1x2+1+1x1+sin⁡xx2=4+11=3\begin{aligned} &\lim_{x\to 0} \frac{\sqrt{4x^2+x-1}+x+1}{\sqrt{x^2+\sin x}}\\ &=\lim _{x \rightarrow \infty} \frac{\sqrt{4+\frac{1}{x}-\frac{1}{x^{2}}}+1+\frac{1}{x}}{\sqrt{1+\frac{\sin x}{x^{2}}}}\\ &=\frac{\sqrt{4}+1}{1}\\ &=3 \\ \end{aligned}

lim⁡x→0∫0xtln⁡(1+tsin⁡t)dt1−cos⁡x2\begin{equation} \lim _{x \rightarrow 0} \frac{\int_{0}^{x} t \ln (1+t \sin t) \mathrm{d} t}{1-\cos x^{2}} \end{equation}

2016年考研数一

提示:判断极限类型+等价无穷小+洛必达法则

lim⁡x→0∫0xtln⁡(1+tsin⁡t)dt1−cos⁡x2=lim⁡x→0∫0xtln⁡(1+tsin⁡t)x42=lim⁡x→0xln⁡(1+xsin⁡x)2x3=lim⁡x→0x(xsin⁡x)2x3=12\begin{aligned} &\displaystyle \lim _{x \rightarrow 0} \frac{\int_{0}^{x} t \ln (1+t \sin t) \mathrm{d} t}{1-\cos x^{2}}\\ &=\displaystyle \lim _{x \rightarrow 0} \frac{\int_{0}^{x} t \ln (1+t \sin t)}{ \frac{x^4}{2}} \\ &=\displaystyle \lim _{x \rightarrow 0} \frac{x \ln (1+x \sin x)}{2 x^{3}}\\ &=\displaystyle\lim _{x \rightarrow 0} \frac{x(x \sin x)}{2 x^{3}}\\ &=\frac{1}{2} \end{aligned}

lim⁡x→+∞∫1x(t2(e1t−1)−t)dtx2ln⁡(1+1x)\begin{equation} \lim _{x \rightarrow+\infty} \frac{\int_{1}^{x}\left(t^{2}\left(\mathrm{e}^{\frac{1}{t}}-1\right)-t\right) \mathrm{d} t}{x^{2} \ln \left(1+\frac{1}{x}\right)} \end{equation}

2014年考研数一

提示:判断极限类型+等价无穷小+洛必达法则

lim⁡x→+∞∫1x(t2(e1t−1)−t)dtx2ln⁡(1+1x)=lim⁡x→+∞∫1x(t2(e1t−1)−t)dtx2⋅1x=lim⁡x→+∞(∫1x(t2(e1t−1)−t)dt)′(x)′=lim⁡x→+∞(x2(e1x−1)−x)令 t=1x=1xlim⁡t→0+et−1−tt2上下都趋近于0,使用洛必达法则=lim⁡t→0+et−12t=12\begin{aligned} &\lim _{x \rightarrow+\infty} \frac{\int_{1}^{x}\left(t^{2}\left(\mathrm{e}^{\frac{1}{t}}-1\right)-t\right) \mathrm{d} t}{x^{2} \ln \left(1+\frac{1}{x}\right)}\\ &=\lim _{x \rightarrow+\infty} \frac{\int_{1}^{x}\left(t^{2}\left(\mathrm{e}^{\frac{1}{t}}-1\right)-t\right) \mathrm{d} t}{x^{2} \cdot \frac{1}{x}}\\&=\lim _{x \rightarrow+\infty} \frac{\left(\int_{1}^{x}\left(t^{2}\left(\mathrm{e}^{\frac{1}{t}}-1\right)-t\right) \mathrm{d} t\right)^{\prime}}{(x)^{\prime}} \\ &=\lim _{x \rightarrow+\infty}\left(x^{2}\left(\mathrm{e}^{\frac{1}{x}}-1\right)-x\right) \qquad \text{令}\ t=\frac{1}{x} \\ &=\frac{1}{x} \lim _{t \rightarrow 0^{+}} \frac{\mathrm{e}^{t}-1-t}{t^{2}}\qquad \text{上下都趋近于0,使用洛必达法则} \\ &=\lim _{t \rightarrow 0^{+}} \frac{\mathrm{e}^{t}-1}{2 t}\\ &=\frac{1}{2} \end{aligned}

lim⁡n→∞nn2+n+1n(n+1)n(5n−1)\begin{equation} \lim _{n \rightarrow \infty} \frac{n^{\frac{n^{2}+n+1}{n}}}{(n+1)^{n}}(\sqrt[n]{5}-1) \end{equation}

From Zhongxiang-17Days

提示:对数字敏感+对公式敏感+剥洋葱法

a🥕−1🥕∼ln⁡a\frac{ a^{🥕}-1}{🥕}\sim \ln a

lim⁡n→∞nn2+n+1n(n+1)n(5n−1)=lim⁡n→∞nn+1⋅nn(n+1)n(5n−1)=lim⁡n→∞nn(n+1)n5−11/n=lim⁡n→∞1(1+1n)n⋅ln⁡5=ln⁡5e\begin{aligned} & \lim _{n \rightarrow \infty} \frac{n^{\frac{n^{2}+n+1}{n}}}{(n+1)^{n}}(\sqrt[n]{5}-1) \\ =& \lim _{n \rightarrow \infty} \frac{n^{n+1} \cdot \sqrt[n]{n}}{(n+1)^{n}}(\sqrt[n]{5}-1) \\ =& \lim _{n \rightarrow \infty} \frac{n^{n}}{(n+1)^{n}} \frac{\sqrt{5}-1}{1 / n} \\ =& \lim _{n \rightarrow \infty} \frac{1}{\left(1+\frac{1}{n}\right)^{n}} \cdot \ln 5 \\ =& \frac{\ln 5}{e} \end{aligned}

lim⁡x→01ln⁡(1+x2)−1sin⁡2x\begin{equation} \lim_{x\to 0}\frac{1}{\ln(1+x^2)}-\frac{1}{\sin^2x} \end{equation}

From Zhongxiang-17Days

提示:对平方差敏感!

=lim⁡x→0sin⁡2x−ln⁡(1+x2)sin⁡2xln⁡(1+x2)=lim⁡x→0sin⁡2x−ln⁡(1+x2)x4=lim⁡x→0(sin⁡2x−x2)−[ln⁡(1+x2)−x2]x4=lim⁡x→0(sin⁡x+x)(sin⁡x−x)x4−lim⁡x→0−12x4x4=lim⁡x→0(2x)(−16x3)x4+12=−13+12=16\begin{aligned} &=\lim _{x \rightarrow 0} \frac{\sin ^{2} x-\ln \left(1+x^{2}\right)}{\sin ^{2} x \ln \left(1+x^{2}\right)} \\ &=\lim _{x \rightarrow 0} \frac{\sin ^{2} x-\ln \left(1+x^{2}\right)}{x^{4}} \\ &=\lim _{x \rightarrow 0} \frac{\left(\sin ^{2} x-x^{2}\right)-\left[\ln \left(1+x^{2}\right)-x^{2}\right]}{x^{4}} \\ &=\lim _{x \rightarrow 0} \frac{(\sin x+x)(\sin x-x)}{x^{4}}-\lim _{x \rightarrow 0} \frac{-\frac{1}{2} x^{4}}{x^{4}} \\ &=\lim _{x \rightarrow 0} \frac{(2 x)\left(-\frac{1}{6} x^{3}\right)}{x^{4}}+\frac{1}{2} \\ &=-\frac{1}{3}+\frac{1}{2}=\frac{1}{6} \end{aligned}


泰勒级数求极限专用区

lim⁡x→01+x22−1+x2(cos⁡x−ex2)sin⁡x2\begin{equation} \lim _{x \rightarrow 0} \frac{1+\frac{x^{2}}{2}-\sqrt{1+x^{2}}}{\left(\cos x-e^{x^{2}}\right) \sin x^{2}} \end{equation}

From Zhongxiang-17Days

提示:基本泰勒展开式

1+x2=(1+x2)12=1+12x2+12(12−1)2!x4+o(x4)=1+12x2−18x4+o(x4)cos⁡x=1−x22!+o(x2)=1−x22+o(x2)ex2=1+x2+o(x2)\begin{aligned} \sqrt{1+x^{2}} &=\left(1+x^{2}\right)^{\frac{1}{2}}=1+\frac{1}{2} x^{2}+\frac{\frac{1}{2}\left(\frac{1}{2}-1\right)}{2 !} x^{4}+o\left(x^{4}\right) \\ &=1+\frac{1}{2} x^{2}-\frac{1}{8} x^{4}+o\left(x^{4}\right) \\ & \cos x=1-\frac{x^{2}}{2 !}+o\left(x^{2}\right)=1-\frac{x^{2}}{2}+o\left(x^{2}\right) \\ \mathrm{e}^{x^{2}} &=1+x^{2}+o\left(x^{2}\right) \end{aligned}

lim⁡x→01+x22−1+x2(cos⁡x−ex2)sin⁡x2=lim⁡x→01+x22−(1+12x2−18x4+o(x4))[(1−x22+o(x2))−(1+x2+o(x2))]x2=lim⁡x→018x4+o(x4)−32x4+o(x4)=−112\begin{aligned} &\lim _{x \rightarrow 0} \frac{1+\frac{x^{2}}{2}-\sqrt{1+x^{2}}}{\left(\cos x-e^{x^{2}}\right) \sin x^{2}}\\ &=\lim _{x \rightarrow 0} \frac{1+\frac{x^{2}}{2}-\left(1+\frac{1}{2} x^{2}-\frac{1}{8} x^{4}+o\left(x^{4}\right)\right)}{\left[\left(1-\frac{x^{2}}{2}+o\left(x^{2}\right)\right)-\left(1+x^{2}+o\left(x^{2}\right)\right)\right] x^{2}} \\ &=\lim _{x \rightarrow 0} \frac{\frac{1}{8} x^{4}+o\left(x^{4}\right)}{-\frac{3}{2} x^{4}+o\left(x^{4}\right)}\\ &=-\frac{1}{12} \end{aligned}

lim⁡n→∞[(n3−n2+n2)e1n−1+n6]\begin{equation} \lim _{n \rightarrow \infty}\left[\left(n^{3}-n^{2}+\frac{n}{2}\right) \mathrm{e}^{\frac{1}{n}}-\sqrt{1+n^{6}}\right] \end{equation}

From Zhongxiang-17Days

提示:无。😠这谁想得到啊!!!

lim⁡n→∞[(n3−n2+n2)e1n−1+n6]=lim⁡n→∞n3[(1−1n+12n2)e1∗−1+1n6]=lim⁡n→∞n3[(1−1n+12n2)−e−1n1+1n6]=lim⁡n→∞n3[(1−1n+12n2)−(1−1n+12n2−13!1n3+o(1n3))(1+o(1n3))]=16\begin{aligned} &\lim _{n \rightarrow \infty}\left[\left(n^{3}-n^{2}+\frac{n}{2}\right) \mathrm{e}^{\frac{1}{n}}-\sqrt{1+n^{6}}\right]\\ &=\lim _{n \rightarrow \infty} n^{3}\left[\left(1-\frac{1}{n}+\frac{1}{2 n^{2}}\right) \mathrm{e}^{\frac{1}{*}}-\sqrt{1+\frac{1}{n^{6}}}\right] \\ &\color{red}=\lim _{n \rightarrow \infty} n^{3}\left[\left(1-\frac{1}{n}+\frac{1}{2 n^{2}}\right)-\mathrm{e}^{-\frac{1}{n}} \sqrt{1+\frac{1}{n^{6}}}\right] \\ &=\lim _{n \rightarrow \infty} n^{3}\left[\left(1-\frac{1}{n}+\frac{1}{2 n^{2}}\right)-\left(1-\frac{1}{n}+\frac{1}{2 n^{2}}-\frac{1}{3 !} \frac{1}{n^{3}}+o\left(\frac{1}{n^{3}}\right)\right)\left(1+o\left(\frac{1}{n^{3}}\right)\right)\right] \\ &=\frac{1}{6} \end{aligned}

蓦然回首

lim⁡x→0(2+sin⁡x2)x−2sin⁡xx3\begin{equation} \lim _{x \rightarrow 0} \frac{\left(2+\sin x^{2}\right)^{x}-2^{\sin x}}{x^{3}} \end{equation}

From Zhongxiang-17Days

提示:努力拼凑出来等价无穷小,提取相同的项,

lim⁡x→0(2+sin⁡x2)x−2sin⁡xx3=lim⁡x→0(2+sin⁡x2)x−2xx3+lim⁡x→02x−2sin⁡xx3=lim⁡x→02x[(1+sin⁡x22)x−1]x3+lim⁡x→02sin⁡x(2x−sin⁡x−1)x3=lim⁡x→0sin⁡x22⋅xx3+lim⁡x→0(x−sin⁡x)ln⁡2x3=lim⁡x→012x3x3+lim⁡x→0(16x3)ln⁡2x3=12+ln⁡26 =12+ln⁡26\begin{aligned} &\lim _{x \rightarrow 0} \frac{\left(2+\sin x^{2}\right)^{x}-2^{\sin x}}{x^{3}}\\ &=\lim _{x \rightarrow 0} \frac{\left(2+\sin x^{2}\right)^{x}-2^{x}}{x^{3}}+\lim _{x \rightarrow 0} \frac{2^{x}-2^{\sin x}}{x^{3}} \\ &=\lim _{x \rightarrow 0} \frac{2^{x}\left[\left(1+\frac{\sin x^{2}}{2}\right)^{x}-1\right]}{x^{3}}+\lim _{x \rightarrow 0} \frac{2^{\sin x}\left(2^{x-\sin x}-1\right)}{x^{3}} \\ &=\lim _{x \rightarrow 0} \frac{\frac{\sin x^{2}}{2} \cdot x}{x^{3}}+\lim _{x \rightarrow 0} \frac{(x-\sin x) \ln 2}{x^{3}} \\ &=\lim _{x \rightarrow 0} \frac{\frac{1}{2} x^{3}}{x^{3}}+\lim _{x \rightarrow 0} \frac{\left(\frac{1}{6} x^{3}\right) \ln 2}{x^{3}} \\ &=\frac{1}{2}+\frac{\ln 2}{6}\\\ &=\frac{1}{2}+\ln \sqrt[6]{2} \end{aligned}

lim⁡x→1x−xx1−x+ln⁡x\begin{equation} \lim _{x \rightarrow 1} \frac{x-x^{x}}{1-x+\ln x} \end{equation}

From Zhongxiang-17Days

提示:努力拼凑出来等价无穷小,提取相同的项,

用换元法把趋向于1的x转换成趋向于0的h,多次拼凑并利用等价无穷小。

lim⁡x→1x−xx1−x+ln⁡x=lim⁡h→0(1+h)[1−(1+h)h]ln⁡(1+h)−h=lim⁡h→0ehln⁡(1+h)−1h−ln⁡(1+h)=lim⁡h→0hln⁡(1+h)h−ln⁡(1+h)=lim⁡h→0h2h−ln⁡(1+h)=lim⁡h→02h1−11+h=2lim⁡h→0(1+h)=2\begin{aligned} &\lim _{x \rightarrow 1} \frac{x-x^{x}}{1-x+\ln x} \\ &=\lim _{h \rightarrow 0} \frac{(1+h)\left[1-(1+h)^{h}\right]}{\ln (1+h)-h} \\ &=\lim _{h \rightarrow 0} \frac{e^{h \ln (1+h)}-1}{h-\ln (1+h)} \\ &=\lim _{h \rightarrow 0} \frac{h \ln (1+h)}{h-\ln (1+h)} \\ &=\lim _{h \rightarrow 0} \frac{h^{2}}{h-\ln (1+h)} \\ &=\lim _{h \rightarrow 0} \frac{2 h}{1-\frac{1}{1+h}} \\ &=2 \lim _{h \rightarrow 0}(1+h) \\ &=2 \end{aligned}

往死里凑等价无穷小!!!

lim⁡x→1x−xx1−x+ln⁡x=lim⁡x→1−x[e(x−1)ln⁡x−1]ln⁡[1+(x−1)]−(x−1)]=lim⁡x→1−(x−1)ln⁡x−12(x−1)2=2lim⁡x→1(x−1)ln⁡[1+(x−1)](x−1)2=2lim⁡x→1(x−1)2(x−1)2=2\begin{aligned} &\lim _{x \rightarrow 1} \frac{x-x^{x}}{1-x+\ln x} \\ &=\lim _{x \rightarrow 1} \frac{-x\left[\mathrm{e}^{(x-1) \ln x}-1\right]}{\ln{[1+(x-1)]}-(x-1)]}\\ &=\lim _{x \rightarrow 1} \frac{-(x-1) \ln x}{-\frac{1}{2}(x-1)^{2}} \\ &=2 \lim _{x \rightarrow 1} \frac{(x-1) \ln {[1+(x-1)]}}{(x-1)^{2}}\\ &= 2 \lim_{x\to 1} \frac{(x-1)^2}{(x-1)^2}\\ &=2\\ \end{aligned}

lim⁡x→+∞[x3+x2+x+13−x2+x+1ln⁡(ex+x)x]\begin{equation} \lim _{x \rightarrow+\infty}\left[\sqrt[3]{x^{3}+x^{2}+x+1}-\sqrt{x^{2}+x+1} \frac{\ln \left(\mathrm{e}^{x}+x\right)}{x}\right] \end{equation}

From Zhongxiang-17Days

提示:要先推演一番,才能做出来😂

lim⁡x→+∞ln⁡(ex+x)x=lim⁡x→+∞ln⁡[ex(1+xex)]x=1+lim⁡x→+∞ln⁡(1+xex)x\color{blue} \lim _{x \rightarrow+\infty} \frac{\ln \left(\mathrm{e}^{x}+x\right)}{x}=\lim _{x \rightarrow+\infty} \frac{\ln \left[\mathrm{e}^{x}\left(1+\frac{x}{\mathrm{e}^{x}}\right)\right]}{x}=1+\lim _{x \rightarrow+\infty} \frac{\ln \left(1+\frac{x}{\mathrm{e}^{x}}\right)}{x}

lim⁡x→+∞[x3+x2+x+13−x2+x+1ln⁡(ex+x)x]=lim⁡x→+∞(x3+x2+x+13−x2+x+1)−lim⁡x2+x+1x→+∞ln⁡(1+xex)=lim⁡x→+∞x(1+1x+1x2+1x33−1+1x+1x2)−0=lim⁡x→+∞x(1+1x+1x2+1x33−1)−lim⁡x→+∞x(1+1x+1x2−1)=lim⁡x→+∞x[13(1x+1x2+1x3)]−lim⁡x→+∞x[12(1x+1x2)]=13−12=−16\begin{aligned} & \lim _{x \rightarrow+\infty}\left[\sqrt[3]{x^{3}+x^{2}+x+1}-\sqrt{x^{2}+x+1} \frac{\ln \left(\mathrm{e}^{x}+x\right)}{x}\right]\\ =& \lim _{x \rightarrow+\infty}\left(\sqrt[3]{x^{3}+x^{2}+x+1}-\sqrt{x^{2}+x+1}\right)-\lim \frac{\sqrt{x^{2}+x+1}}{x \rightarrow+\infty} \ln \left(1+\frac{x}{\mathrm{e}^{x}}\right) \\ =& \lim _{x \rightarrow+\infty} x\left(\sqrt[3]{1+\frac{1}{x}+\frac{1}{x^{2}}+\frac{1}{x^{3}}}-\sqrt{1+\frac{1}{x}+\frac{1}{x^{2}}}\right)-0 \\ =& \lim _{x \rightarrow+\infty} x\left(\sqrt[3]{1+\frac{1}{x}+\frac{1}{x^{2}}+\frac{1}{x^{3}}}-1\right)-\lim _{x \rightarrow+\infty} x\left(\sqrt{1+\frac{1}{x}+\frac{1}{x^{2}}-1}\right) \\ =& \lim _{x \rightarrow+\infty} x\left[\frac{1}{3}\left(\frac{1}{x}+\frac{1}{x^{2}}+\frac{1}{x^{3}}\right)\right]-\lim _{x \rightarrow+\infty} x\left[\frac{1}{2}\left(\frac{1}{x}+\frac{1}{x^{2}}\right)\right] \\ =& \frac{1}{3}-\frac{1}{2}\\ =&-\frac{1}{6} \end{aligned}

lim⁡x→0∫0x2f(t)dtx2∫0xf(t)dtf(0)=0,f′(0)≠0\begin{equation} \lim _{x \rightarrow 0} \frac{\int_{0}^{x^{2}} f(t) \mathrm{d} t}{x^{2} \int_{0}^{x} f(t) \mathrm{d} t}\quad f(0)=0,f'(0)\ne 0 \end{equation}

From Zhongxiang-17Days

提示:使用了两次洛必达法则(标蓝部分),以及导数的定义(精妙之处)

lim⁡x→0∫0x2f(t)dtx2∫0xf(t)dt=lim⁡x→02xf(x2)2x∫0xf(t)dt+x2f(x)=lim⁡x→02f(x2)2∫0xf(t)dt+xf(x)=lim⁡x→04xf′(x2)3f(x)+xf′(x)=lim⁡x→04f′(x2)3f(x)x+f′(x)=4f′(0)3f′(0)+f′(0)=1\begin{aligned} & \lim _{x \rightarrow 0} \frac{\int_{0}^{x^{2}} f(t) \mathrm{d} t}{x^{2} \int_{0}^{x} f(t) \mathrm{d} t}\\ &={\color{blue} \lim _{x \rightarrow 0} \frac{2 x f\left(x^{2}\right)}{2 x \int_{0}^{x} f(t) \mathrm{d} t+x^{2} f(x)}} \\ &=\lim _{x \rightarrow 0} \frac{2 f\left(x^{2}\right)}{2 \int_{0}^{x} f(t) \mathrm{d} t+x f(x)} \\ &=\color{blue} \lim _{x \rightarrow 0} \frac{4 x f^{\prime}\left(x^{2}\right)}{3 f(x)+x f^{\prime}(x)} \\ &=\lim _{x \rightarrow 0} \frac{4 f^{\prime}\left(x^{2}\right)}{\frac{3 f(x)}{x}+f^{\prime}(x)} \\ &=\color{purple} \frac{4 f^{\prime}(0)}{3 f^{\prime}(0)+f^{\prime}(0)} \\ &=1 \end{aligned}

 设函数 f(x) 可导, 求极限 lim⁡x→x0x0f(x)−xf(x0)x−x0\begin{equation} \text { 设函数 } f(x) \text { 可导, 求极限 } \lim _{x \rightarrow x_{0}} \frac{x_{0} f(x)-x f\left(x_{0}\right)}{x-x_{0}} \end{equation}

From Zhongxiang-17Days

提示:使用导数的定义,尽力去凑导数定义式的形式,另外,值得注意的是:可导不代表着该函数在任意点处的极限都存在

lim⁡x→x0x0f(x)−xf(x0)x−x0=lim⁡x→x0x0f(x)−x0f(x0)x−x0−lim⁡x→x0xf(x0)−x0f(x0)x−x0=x0lim⁡x→x0f(x)−f(x0)x−x0−f(x0)=x0f′(x0)−f(x0)\begin{aligned} &\lim _{x \rightarrow x_{0}} \frac{x_{0} f(x)-x f\left(x_{0}\right)}{x-x_{0}}\\ &=\lim _{x \rightarrow x_{0}} \frac{x_{0} f(x)-x_{0} f\left(x_{0}\right)}{x-x_{0}}-\lim _{x \rightarrow x_{0}} \frac{x f\left(x_{0}\right)-x_{0} f\left(x_{0}\right)}{x-x_{0}} \\ &=x_{0} \lim _{x \rightarrow x_{0}} \frac{f(x)-f\left(x_{0}\right)}{x-x_{0}}-f\left(x_{0}\right) \\ &=x_{0} f^{\prime}\left(x_{0}\right)-f\left(x_{0}\right) \end{aligned}

经验总结

思路

对于求极限问题,首先要判断所求极限的类型,若属于确定型,就按确定型中具体类型进行计算;若属于待定型,则看属于待定型中的“商型”、“积差型”还是“幂指型”,其中“商型”是最基础的待定型,“积差型”和“幂指型”都要经过转化最终转化为“商型”进行计算,其中,1∞1^∞ 型除了可以转化为“商型”进行计算外,还可以利用第二重要极限的推广进行计算。确定所求极限的类型至关重要,只有知道所求极限的类型了,才可以按照相应类型的方法进行计算。[2]

等价无穷小要义

当🥕→0🥕 \to 0时

🥕相当于一个函数,最常见的的就是xx了

🥕∼sin⁡(🥕)∼tan⁡(🥕)∼e🥕−1∼ln⁡(1+🥕)∼arcsin⁡(🥕)∼arctan⁡(🥕)🥕 \sim \sin{(🥕)}\sim \tan{(🥕)}\sim {\color{red} e^{🥕}-1} \sim \ln(1+🥕)\sim \arcsin{(🥕)}\sim \arctan{(🥕)}

1−cos⁡(🥕)∼12🥕2🥕−sin⁡(🥕)∼16🥕31-\cos{(🥕)} \sim \frac{1}{2}🥕^2 \qquad \qquad 🥕-\sin{(🥕)} \sim \frac{1}{6}🥕^3

1−cos⁡(🥕)∼12🥕2⟹1−ncos⁡(🥕)∼n2x2−n+1\color{blue} 1-\cos{(🥕)} \sim \frac{1}{2}🥕^2\Longrightarrow 1-n\cos(🥕) \sim\frac{n}{2}x^2-n+1

ln⁡(🥕+1+🥕2)∼🥕\ln(🥕+\sqrt{1+🥕^2})\sim🥕

ln⁡(1+🥕)∼🥕⟹log⁡🥬(1+🥕)∼🥕ln⁡🥬\color{blue}\ln(1+🥕)\sim 🥕 \Longrightarrow \log_🥬(1+🥕)\sim \frac{🥕}{\ln 🥬}

e🥕−1∼🥕⟹🥬🥕−1∼🥕ln⁡🥬\color{blue}e^{🥕}-1\sim 🥕 \Longrightarrow 🥬^{🥕}-1\sim 🥕\ln 🥬

(1+🥕)🥬−1∼🥬🥕(1+🥕)^🥬-1 \sim 🥬🥕

推广式

🥬🥕−1🥕∼ln⁡🥬\frac{ 🥬^{🥕}-1}{🥕}\sim \ln 🥬

加减法使用等价无穷小[3]

口诀: 加不反,减不同,等价随便换

若 α∼α′,β∼β′\alpha \sim \alpha^{\prime}, \beta \sim \beta^{\prime}, 且 lim⁡αβ=A≠−1\lim \frac{\alpha}{\beta}=A \neq-1, 则 α+β∼α′+β′\alpha+\beta \sim \alpha^{\prime}+\beta^{\prime};

若 α∼α′\alpha \sim \alpha^{\prime}, β∼β′\beta \sim \beta^{\prime}, 且 lim⁡αβ=A≠1\lim \frac{\alpha}{\beta}=A \neq 1, 则 α−β∼α′−β′\alpha-\beta \sim \alpha^{\prime}-\beta^{\prime}.

*等价无穷小的推导

此部分从属于紫晶计划·铁石 #笔尖学术

泰勒展开式

泰勒级数(英语:Taylor series)用无限项连加式——级数来表示一个函数,这些相加的项由函数在某一点的导数求得。泰勒级数是以于1715年发表了泰勒公式的英国数学家布鲁克·泰勒(Sir Brook Taylor)来命名的。通过函数在自变量零点的导数求得的泰勒级数又叫做麦克劳林级数(英语:Maclaurin series),以苏格兰数学家科林·麦克劳林的名字命名[4]。所以,我们经常用的所谓的“泰勒展开式”实际上应该称为“麦克劳林级数”。

刚才差点又陷入误区,准备把无穷级数全部复习一遍,之后再来写这篇文章。实际上,很多东西,只有很少一部分是关键所在,理解了关键,就没有必要从头再来。况且,兴致是会消减的,学着学着就把写文章的激情磨光了,这可能也是多巴胺的规律之一吧。所以本文就从关键开始,从核心开始,以紫晶计划的要义“取其精华,弃其糟粕。”为指导,把我想表达的表达出来。

本文的主要依据是泰勒级数,泰勒级数的标准形式为:

∑n=0∞f(n)(a)n!(x−a)n=f(a)+f′(a)1!(x−a)+f′′(a)2!(x−a)2+f′′′(a)3!(x−a)3+⋯{\displaystyle \sum _{n=0}^{\infty }{\frac {f^{(n)}(a)}{n!}}(x-a)^{n}}={\displaystyle f(a)+{\frac {f'(a)}{1!}}(x-a)+{\frac {f''(a)}{2!}}(x-a)^{2}+{\frac {f'''(a)}{3!}}(x-a)^{3}+\cdots }

以下为常见的麦克劳林展开式(不要怕,只需要记住五个我标注为紫色的\color{purple}\text{紫色的},就足以推导出大多数等价无穷小):

Maclaurin series

11−x=∑n=0∞xn=1+x+x2+⋯+xn+⋯∀x:∣x∣<1(1+x)α=∑n=0∞(αn)xn=1+αx+α(α−1)2!x2+⋯+α(α−1)⋯(α−n+1)n!xn+⋯∀x:∣x∣<1,∀α∈Cex=∑n=0∞xnn!=1+x+x22!+x33!+⋯+xnn!+⋯∀xax=exln⁡a=∑n=0∞(xln⁡a)nn!=1+xln⁡a+(xln⁡a)22!+(xln⁡a)33!+⋯+(xln⁡a)nn!+⋯∀xln⁡(1−x)=−∑n=1∞xnn=−x−x22−x33−⋯−xnn−⋯∀x∈[−1,1)ln⁡(1+x)=∑n=1∞(−1)n+1nxn=x−x22+x33−⋯+(−1)n+1nxn+⋯∀x∈(−1,1]log⁡a(1+x)=ln⁡(1+x)ln⁡a=1ln⁡a∑n=1∞(−1)n+1nxn=xln⁡a−x22ln⁡a+x33ln⁡a−⋯+(−1)n+1nln⁡axn+⋯∀x∈(−1,1]\begin{aligned} &{\displaystyle {\color{red}\frac {1}{1-x}}=\sum _{n=0}^{\infty }x^{n}=1+x+x^{2}+\cdots +x^{n}+\cdots \quad \forall x:\left|x\right|<1}\\ &{\displaystyle{ \color{purple}(1+x)^{\alpha }}=\sum _{n=0}^{\infty }{\binom {\alpha }{n}}x^{n}=1+\alpha x+{\frac {\alpha (\alpha -1)}{2!}}x^{2}+\cdots +{\frac {\alpha (\alpha -1)\cdots (\alpha -n+1)}{n!}}x^{n}+\cdots }\quad {\displaystyle \forall x:\left|x\right|<1,\forall \alpha \in \mathbb {C} }\\ &{\displaystyle {\color{purple} e^{x}}=\sum _{n=0}^{\infty }{\frac {x^{n}}{n!}}=1+x+{\frac {x^{2}}{2!}}+{\frac {x^{3}}{3!}}+\cdots +{\frac {x^{n}}{n!}}+\cdots \quad \forall x}\\ &{\displaystyle {\color{teal} a^{x}}=e^{x \ln a}=\sum _{n=0}^{\infty }{\frac {(x \ln a)^{n}}{n!}}=1+x \ln a+{\frac {(x \ln a)^{2}}{2!}}+{\frac {(x \ln a)^{3}}{3!}}+\cdots +{\frac {(x \ln a)^{n}}{n!}}+\cdots \quad \forall x}\\ & {\displaystyle {\color{red} \ln(1-x)}=-\sum _{n=1}^{\infty }{\frac {x^{n}}{n}}=-x-{\frac {x^{2}}{2}}-{\frac {x^{3}}{3}}-\cdots -{\frac {x^{n}}{n}}-\cdots \quad \forall x\in [-1,1)} \\ &{\displaystyle{\color{purple} \ln(1+x)}=\sum _{n=1}^{\infty }{\frac {(-1)^{n+1}}{n}}x^{n}=x-{\frac {x^{2}}{2}}+{\frac {x^{3}}{3}}-\cdots +{\frac {(-1)^{n+1}}{n}}x^{n}+\cdots \quad \forall x\in (-1,1]} \\ &{\displaystyle{\color{teal} \log_a(1+x)}=\frac{\ln (1+x)}{\ln a}=\frac{1}{\ln a}\sum _{n=1}^{\infty }{\frac {(-1)^{n+1}}{n}}x^{n}=\frac{x}{\ln a}-{\frac {x^{2}}{2{\ln a}}}+{\frac {x^{3}}{3{\ln a}}}-\cdots +{\frac {(-1)^{n+1}}{n{\ln a}}}x^{n}+\cdots \quad \forall x\in (-1,1]} \\ \end{aligned}

sin⁡x=∑n=0∞(−1)n(2n+1)!x2n+1=x−x33!+x55!−⋯∀xcos⁡x=∑n=0∞(−1)n(2n)!x2n=1−x22!+x44!−⋯∀xtan⁡x=∑n=1∞B2n(−4)n(1−4n)(2n)!x2n−1=x+x33+2x515+⋯∀x:∣x∣<π2sec⁡x=∑n=0∞(−1)nE2n(2n)!x2n=1+x22+5x424+⋯∀x:∣x∣<π2arcsin⁡x=∑n=0∞(2n)!4n(n!)2(2n+1)x2n+1=x+x36+3x540+⋯∀x:∣x∣≤1arccos⁡x=π2−arcsin⁡x=π2−∑n=0∞(2n)!4n(n!)2(2n+1)x2n+1=π2−x−x36−3x540+⋯∀x:∣x∣≤1arctan⁡x=∑n=0∞(−1)n2n+1x2n+1=x−x33+x55−⋯∀x:∣x∣≤1, x≠±i{\displaystyle {\begin{aligned} \color{purple} \sin x&=\sum _{n=0}^{\infty }{\frac {(-1)^{n}}{(2n+1)!}}x^{2n+1}&&=x-{\frac {x^{3}}{3!}}+{\frac {x^{5}}{5!}}-\cdots &&\forall x\\[6pt] \color{red} \cos x&=\sum _{n=0}^{\infty }{\frac {(-1)^{n}}{(2n)!}}x^{2n}&&=1-{\frac {x^{2}}{2!}}+{\frac {x^{4}}{4!}}-\cdots &&\forall x\\[6pt] \color{purple} \tan x&=\sum _{n=1}^{\infty }{\frac {B_{2n}(-4)^{n}\left(1-4^{n}\right)}{(2n)!}}x^{2n-1}&&=x+{\frac {x^{3}}{3}}+{\frac {2x^{5}}{15}}+\cdots &&\forall x:|x|<{\frac {\pi }{2}}\\[6pt] \color{red} \sec x&=\sum _{n=0}^{\infty }{\frac {(-1)^{n}E_{2n}}{(2n)!}}x^{2n}&&=1+{\frac {x^{2}}{2}}+{\frac {5x^{4}}{24}}+\cdots &&\forall x:|x|<{\frac {\pi }{2}}\\[6pt] \color{red} \arcsin x&=\sum _{n=0}^{\infty }{\frac {(2n)!}{4^{n}(n!)^{2}(2n+1)}}x^{2n+1}&&=x+{\frac {x^{3}}{6}}+{\frac {3x^{5}}{40}}+\cdots &&\forall x:|x|\leq 1\\[6pt] \color{red} \arccos x&={\frac {\pi }{2}}-\arcsin x\\&={\frac {\pi }{2}}-\sum _{n=0}^{\infty }{\frac {(2n)!}{4^{n}(n!)^{2}(2n+1)}}x^{2n+1}&&={\frac {\pi }{2}}-x-{\frac {x^{3}}{6}}-{\frac {3x^{5}}{40}}+\cdots &&\forall x:|x|\leq 1\\[6pt] \color{red} \arctan x&=\sum _{n=0}^{\infty }{\frac {(-1)^{n}}{2n+1}}x^{2n+1}&&=x-{\frac {x^{3}}{3}}+{\frac {x^{5}}{5}}-\cdots &&\forall x:|x|\leq 1,\ x\neq \pm i \end{aligned} }}

等价运算符

此部分为本人杜撰,结论不够准确严谨,但应付等价无穷小的推导应该绰绰有余。如有错误,还望指正🐰。

等价无穷小的不严格定义:

当x→0x\to 0时,两个函数A(x),B(x)A(x),B(x)同时收敛于一个常数(英文:constant) CC,那么这两个函数为x→0x\to0时等价无穷小,记作A(x)∼B(x)A(x)\sim B(x)

下面介绍一下等价无穷小运算符"∼\sim"的运算规律,当x→0x\to 0时,有如下运算规律:

  1. if A(x)∼B(x),B(x)∼C(x)then A(x)∼C(x)if\ A(x)\sim B(x),B(x)\sim C(x)\quad then\ \color{red} A(x) \sim C(x)

  2. if A(x)∼B(x),C is a constant, then if\ A(x)\sim B(x),C\ is\ a\ constant,\ then \

    A(x)⋅C∼B(x)⋅C\color{red} A(x)\cdot C \sim B(x)\cdot C

    A(x)±C∼B(x)±C\color{red} A(x)\pm C \sim B(x)\pm C

  3. if A(x)∼a ,B(x)∼bif\ A(x)\sim a\ , B(x)\sim b

    A(x)⋅B(x)∼a⋅b\color{red} A(x) \cdot B(x) \sim a \cdot b

    A(x)B(x)∼ab\color{red} \frac{A(x)}{ B(x)} \sim \frac{a}{b}

    A(x)+B(x)∼a+bif and only if lim⁡x→0A(x)B(x)≠−1\color{red} A(x) + B(x) \sim a +b\quad if\ and\ only\ if\ \lim_{x\to0}\frac{A(x)}{B(x)}\ne -1

    A(x)−B(x)∼a−bif and only if lim⁡x→0A(x)B(x)≠1\color{red} A(x) - B(x) \sim a - b\quad if\ and\ only\ if\ \lim_{x\to0}\frac{A(x)}{B(x)}\ne 1

    值得注意的是,对于A(x)−B(x)\color{red}A(x)-B(x)这种情形,往往会出现lim⁡x→0A(x)B(x)=1\displaystyle \lim_{x\to0}\frac{A(x)}{B(x)}= 1, 这个时候可以利用下文所讲的泰勒展开式来进行等价😎

  4. 当函数A(x)A(x)在x→0x\to 0处,收敛于某一值,且其可以展开为如下的多项式a0+a1x+a2x2+⋯anxna_0+a_1x+a_2x^2+\cdots a_nx^n,则:A(x)∼a0+a1x+a2x2+⋯anxn\color{red} A(x) \sim a_0+a_1x+a_2x^2+\cdots a_nx^n

    推论1:这个和高阶等价无穷小有关,应该有更严谨的表达,但鄙人懒得翻了,就按我的意思表达吧。

    When A(x)=a0+a1x+a2x2+⋯anxn, B(x)=b0+b1x+b2x2+⋯+bnxn thenlim⁡x→0A(x)B(x)=a0+a1x+a2x2+⋯anxn=b0+b1x+b2x2+⋯+bnxn if n<mWhen\ A(x) = a_0+a_1x+a_2x^2+\cdots a_nx^n,\ B(x)=b_0+b_1x+b_2x^2+\cdots+b_nx^n\ then \\ \lim_{x\to 0}\frac{A(x)}{B(x)}=\frac{a_0+a_1x+a_2x^2+\cdots a_nx^n} {=b_0+b_1x+b_2x^2+\cdots+b_nx^n}\ \color{teal} if \ n<m

    推论2:泰勒展开式移项A(x)−a0−a1x−⋯ajxj∼aj+1xj+1+⋯anxn\color{red} A(x)-a_0-a_1 x- \cdots a_j x^j \sim \color{blue} a_{j+1}x^{j+1}+\cdots a_n x^n

等价无穷小·推导Plus+Pro

泰勒展开式等价无穷小

由于较高阶次的项,考试也不会考,写下来也麻烦的紧,这里就利用最高次幂为二或三的展开式来推导常见的无穷小。

sin⁡x∼x∼x−x36arcsin⁡x∼x∼x+x36tan⁡x∼x∼x+x33arctan⁡x∼x∼x−x33cos⁡x∼1∼1−x22ex∼1∼1+x∼1+x+x22ax∼1∼1+xln⁡a∼1+xln⁡a+(xln⁡a)22ln⁡(1+x)∼x∼x−x22log⁡a(1+x)∼xln⁡a∼xln⁡a−x22ln⁡a(1+x)a∼1∼1+ax∼1+ax+a(a−1)2x211+x∼1∼1−x∼1−x+x211−x∼1∼1+x∼1+x+x2{\displaystyle {\begin{aligned} \color{purple} \sin x\quad&\sim x &&\sim x-{\frac {x^{3}}{6}}\\[6pt] \color{purple} \arcsin x\quad&\sim x &&\sim x+{\frac {x^{3}}{6}}\\[6pt] \color{purple} \tan x\quad&\sim x &&\sim x+{\frac {x^{3}}{3}}\\[6pt] \color{purple} \arctan x\quad&\sim x &&\sim x-{\frac {x^{3}}{3}}\\[6pt] \color{purple} \cos x\quad&\sim 1 &&\sim 1-{\frac {x^{2}}{2}}\\[6pt] \color{purple} e^x\quad&\sim 1 &&\sim 1+x &&\sim 1+x+{\frac {x^{2}}{2}}\\[6pt] \color{teal} a^x\quad&\sim 1 &&\sim 1+x \ln a &&\sim 1+x \ln a+{\frac {(x \ln a)^{2}}{2}} \\[6pt] \color{purple} \ln(1+x)\quad&\sim x &&\sim x-{\frac {x^{2}}{2}}\\[6pt] \color{teal} \log_a(1+x)\quad&\sim\frac{x}{\ln a} &&\sim\frac{x}{\ln a}-{\frac {x^{2}}{2{\ln a}}}\\[6pt] \color{purple} (1+x)^a\quad&\sim 1 &&\sim 1+ax &&\sim 1+ax+\frac{a(a-1)}{2}x^2 \\[6pt] \color{purple} \frac{1}{1+x}\quad&\sim 1 &&\sim 1-x &&\sim 1-x + x^2 \\[6pt] \color{purple} \frac{1}{1-x}\quad&\sim 1 &&\sim 1+x &&\sim 1+x + x^2 \\[6pt] \end{aligned}}}

这些是原始的等价无穷小,亦可以看作出题者的后台

根据等价运算符的运算规律,特别是推论2,我们可以很容易得到以下推论:

x∼sin⁡(x)∼tan⁡(x)∼ex−1∼ln⁡(1+x)∼arcsin⁡(x)∼arctan⁡(x)x \sim {\color{blue} \sin{(x)}}\sim \tan{(x)}\sim {\color{blue} e^{x}-1} \sim \ln(1+x)\sim {\color{blue} \arcsin{(x)}}\sim \arctan{(x)}

sin⁡x−x∼−x36arcsin⁡x−x∼x36tan⁡x−x∼x33arctan⁡x−x∼−x33cos⁡x−1∼−x22ex−1∼x∼x+x22ax−1∼xln⁡a∼xln⁡a+(xln⁡a)22ln⁡(1+x)−x∼−x22log⁡a(1+x)−xln⁡a∼−x22ln⁡a(1+x)a−1∼ax∼ax+a(a−1)2x2−x1+x∼−x∼−x+x2x1−x∼x∼x+x2{\displaystyle {\begin{aligned} \color{purple} \sin x-x\quad&\sim -{\frac {x^{3}}{6}}\\[6pt] \color{purple} \arcsin x-x\quad&\sim {\frac {x^{3}}{6}}\\[6pt] \color{purple} \tan x-x\quad&\sim {\frac {x^{3}}{3}}\\[6pt] \color{purple} \arctan x-x \quad&\sim -{\frac {x^{3}}{3}}\\[6pt] \color{purple} \cos x-1\quad&\sim -{\frac {x^{2}}{2}}\\[6pt] \color{purple} e^x-1\quad&\sim x &&\sim x+{\frac {x^{2}}{2}}\\[6pt] \color{teal} a^x-1\quad&\sim x \ln a &&\sim x \ln a+{\frac {(x \ln a)^{2}}{2}} \\[6pt] \color{purple} \ln(1+x)-x\quad&\sim -{\frac {x^{2}}{2}}\\[6pt] \color{teal} \log_a(1+x)-\frac{x}{\ln a}\quad&\sim-{\frac {x^{2}}{2{\ln a}}}\\[6pt] \color{purple} (1+x)^a-1\quad&\sim ax &&\sim ax+\frac{a(a-1)}{2}x^2 \\[6pt] \color{purple} \frac{-x}{1+x}\quad&\sim -x &&\sim -x + x^2 \\[6pt] \color{purple} \frac{x}{1-x}\quad&\sim x &&\sim x + x^2 \\[6pt] \end{aligned}}}

等价无穷小·推导 50

通过核心公式(泰勒展开式中标紫的地方):sin⁡x,tan⁡x,ex,ln⁡(x+1)\sin x,\tan x, e^x, \ln(x+1),加上简单的加减乘除,三角函数运算,对数运算,以及上文的等价运算,可以很方便的推导出其他的等价无穷小,太累了,过程省略,给你张图,慢慢推导吧

推导路线图


  1. 维基百科编者. 洛奇[G/OL]. 维基百科. 中文名:《洛奇》,一部1976年的美国电影,由约翰·艾维森执导,西尔维斯特·史泰龙编剧兼主演,讲述一个籍籍无名的拳手洛奇·巴尔博亚在获得与世界重量级冠军阿波罗·奎迪争夺冠军的机会后奋力一搏的美国梦故事。 ↩︎

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  3. 黄星,张倩瑶.利用等价无穷小替换求极限时应注意的问题J.黑龙江科学,2021,12(13):130-131 ↩︎

  4. 维基百科编者. 泰勒级数[G/OL]. 维基百科, 2022(20220324)[2022-03-24]. ↩︎