深度学习机器学习的数学基础

机器学习的数学基础

高等数学

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1.导数定义:

导数和微分的概念

f ′ ( x 0 ) = lim ⁡ Δ x → 0   f ( x 0 + Δ x ) − f ( x 0 ) Δ x f'({ {x}_{0}})=\underset{\Delta x\to 0}{\mathop{\lim }}\,\frac{f({ {x}_{0}}+\Delta x)-f({ {x}_{0}})}{\Delta x} f(x0)=Δx0limΔxf(x0+Δx)f(x0) (1)

或者:

f ′ ( x 0 ) = lim ⁡ x → x 0   f ( x ) − f ( x 0 ) x − x 0 f'({ {x}_{0}})=\underset{x\to { {x}_{0}}}{\mathop{\lim }}\,\frac{f(x)-f({ {x}_{0}})}{x-{ {x}_{0}}} f(x0)=xx0limxx0f(x)f(x0) (2)

2.左右导数导数的几何意义和物理意义

函数 f ( x ) f(x) f(x) x 0 x_0 x0处的左、右导数分别定义为:

左导数: f ′ − ( x 0 ) = lim ⁡ Δ x → 0 −   f ( x 0 + Δ x ) − f ( x 0 ) Δ x = lim ⁡ x → x 0 −   f ( x ) − f ( x 0 ) x − x 0 , ( x = x 0 + Δ x ) { { {f}'}_{-}}({ {x}_{0}})=\underset{\Delta x\to { {0}^{-}}}{\mathop{\lim }}\,\frac{f({ {x}_{0}}+\Delta x)-f({ {x}_{0}})}{\Delta x}=\underset{x\to x_{0}^{-}}{\mathop{\lim }}\,\frac{f(x)-f({ {x}_{0}})}{x-{ {x}_{0}}},(x={ {x}_{0}}+\Delta x) f(x0)=Δx0limΔxf(x0+Δx)f(x0)=xx0limxx0f(x)f(x0),(x=x0+Δx)

右导数: f ′ + ( x 0 ) = lim ⁡ Δ x → 0 +   f ( x 0 + Δ x ) − f ( x 0 ) Δ x = lim ⁡ x → x 0 +   f ( x ) − f ( x 0 ) x − x 0 { { {f}'}_{+}}({ {x}_{0}})=\underset{\Delta x\to { {0}^{+}}}{\mathop{\lim }}\,\frac{f({ {x}_{0}}+\Delta x)-f({ {x}_{0}})}{\Delta x}=\underset{x\to x_{0}^{+}}{\mathop{\lim }}\,\frac{f(x)-f({ {x}_{0}})}{x-{ {x}_{0}}} f+(x0)=Δx0+limΔxf(x0+Δx)f(x0)=xx0+limxx0f(x)f(x0)

3.函数的可导性与连续性之间的关系

Th1: 函数 f ( x ) f(x) f(x) x 0 x_0 x0处可微 ⇔ f ( x ) \Leftrightarrow f(x) f(x) x 0 x_0 x0处可导

Th2: 若函数在点 x 0 x_0 x0处可导,则 y = f ( x ) y=f(x) y=f(x)在点 x 0 x_0 x0处连续,反之则不成立。即函数连续不一定可导。

Th3: f ′ ( x 0 ) {f}'({ {x}_{0}}) f(x0)存在 ⇔ f ′ − ( x 0 ) = f ′ + ( x 0 ) \Leftrightarrow { { {f}'}_{-}}({ {x}_{0}})={ { {f}'}_{+}}({ {x}_{0}}) f(x0)=f+(x0)

4.平面曲线的切线和法线

切线方程 : y − y 0 = f ′ ( x 0 ) ( x − x 0 ) y-{ {y}_{0}}=f'({ {x}_{0}})(x-{ {x}_{0}}) yy0=f(x0)(xx0)
法线方程: y − y 0 = − 1 f ′ ( x 0 ) ( x − x 0 ) , f ′ ( x 0 ) ≠ 0 y-{ {y}_{0}}=-\frac{1}{f'({ {x}_{0}})}(x-{ {x}_{0}}),f'({ {x}_{0}})\ne 0 yy0=f(x0)1(xx0),f(x0)=0

5.四则运算法则
设函数 u = u ( x ) , v = v ( x ) u=u(x),v=v(x) u=u(x)v=v(x)]在点 x x x可导则
(1) ( u ± v ) ′ = u ′ ± v ′ (u\pm v{)}'={u}'\pm {v}' (u±v)=u±v d ( u ± v ) = d u ± d v d(u\pm v)=du\pm dv d(u±v)=du±dv
(2) ( u v ) ′ = u v ′ + v u ′ (uv{)}'=u{v}'+v{u}' (uv)=uv+vu d ( u v ) = u d v + v d u d(uv)=udv+vdu d(uv)=udv+vdu
(3) ( u v ) ′ = v u ′ − u v ′ v 2 ( v ≠ 0 ) (\frac{u}{v}{)}'=\frac{v{u}'-u{v}'}{ { {v}^{2}}}(v\ne 0) (vu)=v2vuuv(v=0) d ( u v ) = v d u − u d v v 2 d(\frac{u}{v})=\frac{vdu-udv}{ { {v}^{2}}} d(vu)=v2vduudv

6.基本导数与微分表
(1) y = c ​ y=c​ y=c(常数) y ′ = 0 ​ {y}'=0​ y=0​ d y = 0 ​ dy=0​ dy=0​
(2) y = x α ​ y={ {x}^{\alpha }}​ y=xα( α ​ \alpha ​ α为实数) y ′ = α x α − 1 ​ {y}'=\alpha { {x}^{\alpha -1}}​ y=αxα1 d y = α x α − 1 d x ​ dy=\alpha { {x}^{\alpha -1}}dx​ dy=αxα1dx
(3) y = a x ​ y={ {a}^{x}}​ y=ax y ′ = a x ln ⁡ a ​ {y}'={ {a}^{x}}\ln a​ y=axlna d y = a x ln ⁡ a d x ​ dy={ {a}^{x}}\ln adx​ dy=axlnadx
特例: ( e x ) ′ = e x ​ ({ { {e}}^{x}}{)}'={ { {e}}^{x}}​ (ex)=ex d ( e x ) = e x d x ​ d({ { {e}}^{x}})={ { {e}}^{x}}dx​ d(ex)=exdx

(4) y = log ⁡ a x y={ {\log }_{a}}x y=logax y ′ = 1 x ln ⁡ a {y}'=\frac{1}{x\ln a} y=xlna1

d y = 1 x ln ⁡ a d x dy=\frac{1}{x\ln a}dx dy=xlna1dx
特例: y = ln ⁡ x y=\ln x y=lnx ( ln ⁡ x ) ′ = 1 x (\ln x{)}'=\frac{1}{x} (lnx)=x1 d ( ln ⁡ x ) = 1 x d x d(\ln x)=\frac{1}{x}dx d(lnx)=x1dx

(5) y = sin ⁡ x y=\sin x y=sinx

y ′ = cos ⁡ x {y}'=\cos x y=cosx d ( sin ⁡ x ) = cos ⁡ x d x d(\sin x)=\cos xdx d(sinx)=cosxdx

(6) y = cos ⁡ x y=\cos x y=cosx

y ′ = − sin ⁡ x {y}'=-\sin x y=sinx d ( cos ⁡ x ) = − sin ⁡ x d x d(\cos x)=-\sin xdx d(cosx)=sinxdx

(7) y = tan ⁡ x y=\tan x y=tanx

y ′ = 1 cos ⁡ 2 x = sec ⁡ 2 x {y}'=\frac{1}{ { {\cos }^{2}}x}={ {\sec }^{2}}x y=cos2x1=sec2x d ( tan ⁡ x ) = sec ⁡ 2 x d x d(\tan x)={ {\sec }^{2}}xdx d(tanx)=sec2xdx
(8) y = cot ⁡ x y=\cot x y=cotx y ′ = − 1 sin ⁡ 2 x = − csc ⁡ 2 x {y}'=-\frac{1}{ { {\sin }^{2}}x}=-{ {\csc }^{2}}x y=sin2x1=csc2x d ( cot ⁡ x ) = − csc ⁡ 2 x d x d(\cot x)=-{ {\csc }^{2}}xdx d(cotx)=csc2xdx
(9) y = sec ⁡ x y=\sec x y=secx y ′ = sec ⁡ x tan ⁡ x {y}'=\sec x\tan x y=secxtanx

d ( sec ⁡ x ) = sec ⁡ x tan ⁡ x d x d(\sec x)=\sec x\tan xdx d(secx)=secxtanxdx
(10) y = csc ⁡ x y=\csc x y=cscx y ′ = − csc ⁡ x cot ⁡ x {y}'=-\csc x\cot x y=cscxcotx

d ( csc ⁡ x ) = − csc ⁡ x cot ⁡ x d x d(\csc x)=-\csc x\cot xdx d(cscx)=cscxcotxdx
(11) y = arcsin ⁡ x y=\arcsin x y=arcsinx

y ′ = 1 1 − x 2 {y}'=\frac{1}{\sqrt{1-{ {x}^{2}}}} y=1x2 1

d ( arcsin ⁡ x ) = 1 1 − x 2 d x d(\arcsin x)=\frac{1}{\sqrt{1-{ {x}^{2}}}}dx d(arcsinx)=1x2 1dx
(12) y = arccos ⁡ x y=\arccos x y=arccosx

y ′ = − 1 1 − x 2 {y}'=-\frac{1}{\sqrt{1-{ {x}^{2}}}} y=1x2 1 d ( arccos ⁡ x ) = − 1 1 − x 2 d x d(\arccos x)=-\frac{1}{\sqrt{1-{ {x}^{2}}}}dx d(arccosx)=1x2 1dx

(13) y = arctan ⁡ x y=\arctan x y=arctanx

y ′ = 1 1 + x 2 {y}'=\frac{1}{1+{ {x}^{2}}} y=1+x21 d ( arctan ⁡ x ) = 1 1 + x 2 d x d(\arctan x)=\frac{1}{1+{ {x}^{2}}}dx d(arctanx)=1+x21dx

(14) y = arc ⁡ cot ⁡ x y=\operatorname{arc}\cot x y=arccotx

y ′ = − 1 1 + x 2 {y}'=-\frac{1}{1+{ {x}^{2}}} y=1+x21

d ( arc ⁡ cot ⁡ x ) = − 1 1 + x 2 d x d(\operatorname{arc}\cot x)=-\frac{1}{1+{ {x}^{2}}}dx d(arccotx)=1+x21dx
(15) y = s h x y=shx y=shx

y ′ = c h x {y}'=chx y=chx d ( s h x ) = c h x d x d(shx)=chxdx d(shx)=chxdx

(16) y = c h x y=chx y=chx

y ′ = s h x {y}'=shx y=shx d ( c h x ) = s h x d x d(chx)=shxdx d(chx)=shxdx

7.复合函数,反函数,隐函数以及参数方程所确定的函数的微分法

(1) 反函数的运算法则: 设 y = f ( x ) y=f(x) y=f(x)在点 x x x的某邻域内单调连续,在点 x x x处可导且 f ′ ( x ) ≠ 0 {f}'(x)\ne 0 f(x)=0,则其反函数在点 x x x所对应的 y y y处可导,并且有 d y d x = 1 d x d y \frac{dy}{dx}=\frac{1}{\frac{dx}{dy}} dxdy=dydx1
(2) 复合函数的运算法则:若 μ = φ ( x ) \mu =\varphi (x) μ=φ(x)在点 x x x可导,而 y = f ( μ ) y=f(\mu ) y=f(μ)在对应点$\mu ( ( (\mu =\varphi (x) ) 可导 , 则复合函数 )可导,则复合函数 )可导,则复合函数y=f(\varphi (x)) 在点 在点 在点x 可导 , 且 可导,且 可导,{y}‘={f}’(\mu )\cdot {\varphi }'(x)$
(3) 隐函数导数 d y d x \frac{dy}{dx} dxdy的求法一般有三种方法:
1)方程两边对 x x x求导,要记住 y y y x x x的函数,则 y y y的函数是 x x x的复合函数.例如 1 y \frac{1}{y} y1 y 2 { {y}^{2}} y2 l n y ln y lny e y { { {e}}^{y}} ey等均是 x x x的复合函数.
x x x求导应按复合函数连锁法则做.
2)公式法.由 F ( x , y ) = 0 F(x,y)=0 F(x,y)=0 d y d x = − F ′ x ( x , y ) F ′ y ( x , y ) \frac{dy}{dx}=-\frac{ { { { {F}'}}_{x}}(x,y)}{ { { { {F}'}}_{y}}(x,y)} dxdy=Fy(x,y)Fx(x,y),其中, F ′ x ( x , y ) { { {F}'}_{x}}(x,y) Fx(x,y)
F ′ y ( x , y ) { { {F}'}_{y}}(x,y) Fy(x,y)分别表示 F ( x , y ) F(x,y) F(x,y) x x x y y y的偏导数
3)利用微分形式不变性

8.常用高阶导数公式

(1) ( a x )   ( n ) = a x ln ⁡ n a ( a > 0 ) ( e x )   ( n ) = e   x ({ {a}^{x}}){ {\,}^{(n)}}={ {a}^{x}}{ {\ln }^{n}}a\quad (a>{0})\quad \quad ({ { {e}}^{x}}){ {\,}^{(n)}}={e}{ {\,}^{x}} (ax)(n)=axlnna(a>0)(ex)(n)=ex
(2) ( sin ⁡ k x )   ( n ) = k n sin ⁡ ( k x + n ⋅ π 2 ) (\sin kx{)}{ {\,}^{(n)}}={ {k}^{n}}\sin (kx+n\cdot \frac{\pi }{ {2}}) (sinkx)(n)=knsin(kx+n2π)
(3) ( cos ⁡ k x )   ( n ) = k n cos ⁡ ( k x + n ⋅ π 2 ) (\cos kx{)}{ {\,}^{(n)}}={ {k}^{n}}\cos (kx+n\cdot \frac{\pi }{ {2}}) (coskx)(n)=kncos(kx+n2π)
(4) ( x m )   ( n ) = m ( m − 1 ) ⋯ ( m − n + 1 ) x m − n ({ {x}^{m}}){ {\,}^{(n)}}=m(m-1)\cdots (m-n+1){ {x}^{m-n}} (xm)(n)=m(m1)(mn+1)xmn
(5) ( ln ⁡ x )   ( n ) = ( − 1 ) ( n − 1 ) ( n − 1 ) ! x n (\ln x){ {\,}^{(n)}}={ {(-{1})}^{(n-{1})}}\frac{(n-{1})!}{ { {x}^{n}}} (lnx)(n)=(1)(n1)xn(n1)!
(6)莱布尼兹公式:若 u ( x )   , v ( x ) u(x)\,,v(x) u(x),v(x) n n n阶可导,则
( u v ) ( n ) = ∑ i = 0 n c n i u ( i ) v ( n − i ) { {(uv)}^{(n)}}=\sum\limits_{i={0}}^{n}{c_{n}^{i}{ {u}^{(i)}}{ {v}^{(n-i)}}} (uv)(n)=i=0ncniu(i)v(ni),其中 u ( 0 ) = u { {u}^{({0})}}=u u(0)=u v ( 0 ) = v { {v}^{({0})}}=v v(0)=v

9.微分中值定理,泰勒公式

Th1:(费马定理)

若函数 f ( x ) f(x) f(x)满足条件:
(1)函数 f ( x ) f(x) f(x) x 0 { {x}_{0}} x0的某邻域内有定义,并且在此邻域内恒有
f ( x ) ≤ f ( x 0 ) f(x)\le f({ {x}_{0}}) f(x)f(x0) f ( x ) ≥ f ( x 0 ) f(x)\ge f({ {x}_{0}}) f(x)f(x0),

(2) f ( x ) f(x) f(x) x 0 { {x}_{0}} x0处可导,则有 f ′ ( x 0 ) = 0 {f}'({ {x}_{0}})=0 f(x0)=0

Th2:(罗尔定理)

设函数 f ( x ) f(x) f(x)满足条件:
(1)在闭区间 [ a , b ] [a,b] [a,b]上连续;

(2)在 ( a , b ) (a,b) (a,b)内可导;

(3) f ( a ) = f ( b ) f(a)=f(b) f(a)=f(b)

则在 ( a , b ) (a,b) (a,b)内一存在个$\xi $,使 f ′ ( ξ ) = 0 {f}'(\xi )=0 f(ξ)=0
Th3: (拉格朗日中值定理)

设函数 f ( x ) f(x) f(x)满足条件:
(1)在 [ a , b ] [a,b] [a,b]上连续;

(2)在 ( a , b ) (a,b) (a,b)内可导;

则在 ( a , b ) (a,b) (a,b)内一存在个$\xi $,使 f ( b ) − f ( a ) b − a = f ′ ( ξ ) \frac{f(b)-f(a)}{b-a}={f}'(\xi ) baf(b)f(a)=f(ξ)

Th4: (柯西中值定理)

设函数 f ( x ) f(x) f(x) g ( x ) g(x) g(x)满足条件:
(1) 在 [ a , b ] [a,b] [a,b]上连续;

(2) 在 ( a , b ) (a,b) (a,b)内可导且 f ′ ( x ) {f}'(x) f(x) g ′ ( x ) {g}'(x) g(x)均存在,且 g ′ ( x ) ≠ 0 {g}'(x)\ne 0 g(x)=0

则在 ( a , b ) (a,b) (a,b)内存在一个$\xi $,使 f ( b ) − f ( a ) g ( b ) − g ( a ) = f ′ ( ξ ) g ′ ( ξ ) \frac{f(b)-f(a)}{g(b)-g(a)}=\frac{ {f}'(\xi )}{ {g}'(\xi )} g(b)g(a)f(b)f(a)=g(ξ)f(ξ)

10.洛必达法则
法则Ⅰ ( 0 0 \frac{0}{0} 00型)
设函数 f ( x ) , g ( x ) f\left( x \right),g\left( x \right) f(x),g(x)满足条件:
lim ⁡ x → x 0   f ( x ) = 0 , lim ⁡ x → x 0   g ( x ) = 0 \underset{x\to { {x}_{0}}}{\mathop{\lim }}\,f\left( x \right)=0,\underset{x\to { {x}_{0}}}{\mathop{\lim }}\,g\left( x \right)=0 xx0limf(x)=0,xx0limg(x)=0;

f ( x ) , g ( x ) f\left( x \right),g\left( x \right) f(x),g(x) x 0 { {x}_{0}} x0的邻域内可导,(在 x 0 { {x}_{0}} x0处可除外)且 g ′ ( x ) ≠ 0 {g}'\left( x \right)\ne 0 g(x)=0;

lim ⁡ x → x 0   f ′ ( x ) g ′ ( x ) \underset{x\to { {x}_{0}}}{\mathop{\lim }}\,\frac{ {f}'\left( x \right)}{ {g}'\left( x \right)} xx0limg(x)f(x)存在(或$\infty $)。

则:
lim ⁡ x → x 0   f ( x ) g ( x ) = lim ⁡ x → x 0   f ′ ( x ) g ′ ( x ) \underset{x\to { {x}_{0}}}{\mathop{\lim }}\,\frac{f\left( x \right)}{g\left( x \right)}=\underset{x\to { {x}_{0}}}{\mathop{\lim }}\,\frac{ {f}'\left( x \right)}{ {g}'\left( x \right)} xx0limg(x)f(x)=xx0limg(x)f(x)
法则 I ′ { {I}'} I ( 0 0 \frac{0}{0} 00型)设函数 f ( x ) , g ( x ) f\left( x \right),g\left( x \right) f(x),g(x)满足条件:
lim ⁡ x → ∞   f ( x ) = 0 , lim ⁡ x → ∞   g ( x ) = 0 \underset{x\to \infty }{\mathop{\lim }}\,f\left( x \right)=0,\underset{x\to \infty }{\mathop{\lim }}\,g\left( x \right)=0 xlimf(x)=0,xlimg(x)=0;

存在一个 X > 0 X>0 X>0,当 ∣ x ∣ > X \left| x \right|>X x>X时, f ( x ) , g ( x ) f\left( x \right),g\left( x \right) f(x),g(x)可导,且 g ′ ( x ) ≠ 0 {g}'\left( x \right)\ne 0 g(x)=0; lim ⁡ x → x 0   f ′ ( x ) g ′ ( x ) \underset{x\to { {x}_{0}}}{\mathop{\lim }}\,\frac{ {f}'\left( x \right)}{ {g}'\left( x \right)} xx0limg(x)f(x)存在(或$\infty $)。

则:
lim ⁡ x → x 0   f ( x ) g ( x ) = lim ⁡ x → x 0   f ′ ( x ) g ′ ( x ) \underset{x\to { {x}_{0}}}{\mathop{\lim }}\,\frac{f\left( x \right)}{g\left( x \right)}=\underset{x\to { {x}_{0}}}{\mathop{\lim }}\,\frac{ {f}'\left( x \right)}{ {g}'\left( x \right)} xx0limg(x)f(x)=xx0limg(x)f(x)
法则Ⅱ( ∞ ∞ \frac{\infty }{\infty } 型) 设函数 f ( x ) , g ( x ) f\left( x \right),g\left( x \right) f(x),g(x)满足条件:
$\underset{x\to { {x}{0}}}{\mathop{\lim }},f\left( x \right)=\infty ,\underset{x\to { {x}{0}}}{\mathop{\lim }},g\left( x \right)=\infty $; f ( x ) , g ( x ) f\left( x \right),g\left( x \right) f(x),g(x) x 0 { {x}_{0}} x0 的邻域内可导(在 x 0 { {x}_{0}} x0处可除外)且 g ′ ( x ) ≠ 0 {g}'\left( x \right)\ne 0 g(x)=0; lim ⁡ x → x 0   f ′ ( x ) g ′ ( x ) \underset{x\to { {x}_{0}}}{\mathop{\lim }}\,\frac{ {f}'\left( x \right)}{ {g}'\left( x \right)} xx0limg(x)f(x)存在(或$\infty $)。则
lim ⁡ x → x 0   f ( x ) g ( x ) = lim ⁡ x → x 0   f ′ ( x ) g ′ ( x ) . \underset{x\to { {x}_{0}}}{\mathop{\lim }}\,\frac{f\left( x \right)}{g\left( x \right)}=\underset{x\to { {x}_{0}}}{\mathop{\lim }}\,\frac{ {f}'\left( x \right)}{ {g}'\left( x \right)}. xx0limg(x)f(x)=xx0limg(x)f(x).同理法则 I I ′ {I{I}'} II( ∞ ∞ \frac{\infty }{\infty } 型)仿法则 I ′ { {I}'} I可写出。

11.泰勒公式

设函数 f ( x ) f(x) f(x)在点 x 0 { {x}_{0}} x0处的某邻域内具有 n + 1 n+1 n+1阶导数,则对该邻域内异于 x 0 { {x}_{0}} x0的任意点 x x x,在 x 0 { {x}_{0}} x0 x x x之间至少存在
一个$\xi $,使得:
$f(x)=f({ {x}{0}})+{f}'({ {x}{0}})(x-{ {x}{0}})+\frac{1}{2!}{f}‘’({ {x}{0}}){ {(x-{ {x}_{0}})}^{2}}+\cdots $
+ f ( n ) ( x 0 ) n ! ( x − x 0 ) n + R n ( x ) +\frac{ { {f}^{(n)}}({ {x}_{0}})}{n!}{ {(x-{ {x}_{0}})}^{n}}+{ {R}_{n}}(x) +n!f(n)(x0)(xx0)n+Rn(x)
其中 R n ( x ) = f ( n + 1 ) ( ξ ) ( n + 1 ) ! ( x − x 0 ) n + 1 { {R}_{n}}(x)=\frac{ { {f}^{(n+1)}}(\xi )}{(n+1)!}{ {(x-{ {x}_{0}})}^{n+1}} Rn(x)=(n+1)!f(n+1)(ξ)(xx0)n+1称为 f ( x ) f(x) f(x)在点 x 0 { {x}_{0}} x0处的 n n n阶泰勒余项。

x 0 = 0 { {x}_{0}}=0 x0=0,则 n n n阶泰勒公式
f ( x ) = f ( 0 ) + f ′ ( 0 ) x + 1 2 ! f ′ ′ ( 0 ) x 2 + ⋯ + f ( n ) ( 0 ) n ! x n + R n ( x ) f(x)=f(0)+{f}'(0)x+\frac{1}{2!}{f}''(0){ {x}^{2}}+\cdots +\frac{ { {f}^{(n)}}(0)}{n!}{ {x}^{n}}+{ {R}_{n}}(x) f(x)=f(0)+f(0)x+2!1f′′(0)x2++n!f(n)(0)xn+Rn(x)……(1)
其中 R n ( x ) = f ( n + 1 ) ( ξ ) ( n + 1 ) ! x n + 1 { {R}_{n}}(x)=\frac{ { {f}^{(n+1)}}(\xi )}{(n+1)!}{ {x}^{n+1}} Rn(x)=(n+1)!f(n+1)(ξ)xn+1,$\xi 在 0 与 在0与 0x$之间.(1)式称为麦克劳林公式

常用五种函数在 x 0 = 0 { {x}_{0}}=0 x0=0处的泰勒公式

(1) e x = 1 + x + 1 2 ! x 2 + ⋯ + 1 n ! x n + x n + 1 ( n + 1 ) ! e ξ { { {e}}^{x}}=1+x+\frac{1}{2!}{ {x}^{2}}+\cdots +\frac{1}{n!}{ {x}^{n}}+\frac{ { {x}^{n+1}}}{(n+1)!}{ {e}^{\xi }} ex=1+x+2!1x2++n!1xn+(n+1)!xn+1eξ

= 1 + x + 1 2 ! x 2 + ⋯ + 1 n ! x n + o ( x n ) =1+x+\frac{1}{2!}{ {x}^{2}}+\cdots +\frac{1}{n!}{ {x}^{n}}+o({ {x}^{n}}) =1+x+2!1x2++n!1xn+o(xn)

(2) sin ⁡ x = x − 1 3 ! x 3 + ⋯ + x n n ! sin ⁡ n π 2 + x n + 1 ( n + 1 ) ! sin ⁡ ( ξ + n + 1 2 π ) \sin x=x-\frac{1}{3!}{ {x}^{3}}+\cdots +\frac{ { {x}^{n}}}{n!}\sin \frac{n\pi }{2}+\frac{ { {x}^{n+1}}}{(n+1)!}\sin (\xi +\frac{n+1}{2}\pi ) sinx=x3!1x3++n!xnsin2+(n+1)!xn+1sin(ξ+2n+1π)

= x − 1 3 ! x 3 + ⋯ + x n n ! sin ⁡ n π 2 + o ( x n ) =x-\frac{1}{3!}{ {x}^{3}}+\cdots +\frac{ { {x}^{n}}}{n!}\sin \frac{n\pi }{2}+o({ {x}^{n}}) =x3!1x3++n!xnsin2+o(xn)

(3) cos ⁡ x = 1 − 1 2 ! x 2 + ⋯ + x n n ! cos ⁡ n π 2 + x n + 1 ( n + 1 ) ! cos ⁡ ( ξ + n + 1 2 π ) \cos x=1-\frac{1}{2!}{ {x}^{2}}+\cdots +\frac{ { {x}^{n}}}{n!}\cos \frac{n\pi }{2}+\frac{ { {x}^{n+1}}}{(n+1)!}\cos (\xi +\frac{n+1}{2}\pi ) cosx=12!1x2++n!xncos2+(n+1)!xn+1cos(ξ+2n+1π)

= 1 − 1 2 ! x 2 + ⋯ + x n n ! cos ⁡ n π 2 + o ( x n ) =1-\frac{1}{2!}{ {x}^{2}}+\cdots +\frac{ { {x}^{n}}}{n!}\cos \frac{n\pi }{2}+o({ {x}^{n}}) =12!1x2++n!xncos2+o(xn)

(4) ln ⁡ ( 1 + x ) = x − 1 2 x 2 + 1 3 x 3 − ⋯ + ( − 1 ) n − 1 x n n + ( − 1 ) n x n + 1 ( n + 1 ) ( 1 + ξ ) n + 1 \ln (1+x)=x-\frac{1}{2}{ {x}^{2}}+\frac{1}{3}{ {x}^{3}}-\cdots +{ {(-1)}^{n-1}}\frac{ { {x}^{n}}}{n}+\frac{ { {(-1)}^{n}}{ {x}^{n+1}}}{(n+1){ {(1+\xi )}^{n+1}}} ln(1+x)=x21x2+31x3+(1)n1nxn+(n+1)(1+ξ)n+1(1)nxn+1

= x − 1 2 x 2 + 1 3 x 3 − ⋯ + ( − 1 ) n − 1 x n n + o ( x n ) =x-\frac{1}{2}{ {x}^{2}}+\frac{1}{3}{ {x}^{3}}-\cdots +{ {(-1)}^{n-1}}\frac{ { {x}^{n}}}{n}+o({ {x}^{n}}) =x21x2+31x3+(1)n1nxn+o(xn)

(5) ( 1 + x ) m = 1 + m x + m ( m − 1 ) 2 ! x 2 + ⋯ + m ( m − 1 ) ⋯ ( m − n + 1 ) n ! x n { {(1+x)}^{m}}=1+mx+\frac{m(m-1)}{2!}{ {x}^{2}}+\cdots +\frac{m(m-1)\cdots (m-n+1)}{n!}{ {x}^{n}} (1+x)m=1+mx+2!m(m1)x2++n!m(m1)(mn+1)xn
+ m ( m − 1 ) ⋯ ( m − n + 1 ) ( n + 1 ) ! x n + 1 ( 1 + ξ ) m − n − 1 +\frac{m(m-1)\cdots (m-n+1)}{(n+1)!}{ {x}^{n+1}}{ {(1+\xi )}^{m-n-1}} +(n+1)!m(m1)(mn+1)xn+1(1+ξ)mn1

或 ${ {(1+x)}{m}}=1+mx+\frac{m(m-1)}{2!}{ {x}{2}}+\cdots $ + m ( m − 1 ) ⋯ ( m − n + 1 ) n ! x n + o ( x n ) +\frac{m(m-1)\cdots (m-n+1)}{n!}{ {x}^{n}}+o({ {x}^{n}}) +n!m(m1)(mn+1)xn+o(xn)

12.函数单调性的判断
Th1: 设函数 f ( x ) f(x) f(x) ( a , b ) (a,b) (a,b)区间内可导,如果对 ∀ x ∈ ( a , b ) \forall x\in (a,b) x(a,b),都有KaTeX parse error: Got group of unknown type: 'internal'(或KaTeX parse error: Got group of unknown type: 'internal'),则函数 f ( x ) f(x) f(x) ( a , b ) (a,b) (a,b)内是单调增加的(或单调减少)

Th2: (取极值的必要条件)设函数 f ( x ) f(x) f(x) x 0 { {x}_{0}} x0处可导,且在 x 0 { {x}_{0}} x0处取极值,则KaTeX parse error: Got group of unknown type: 'internal'

Th3: (取极值的第一充分条件)设函数 f ( x ) f(x) f(x) x 0 { {x}_{0}} x0的某一邻域内可微,且KaTeX parse error: Got group of unknown type: 'internal'(或 f ( x ) f(x) f(x) x 0 { {x}_{0}} x0处连续,但KaTeX parse error: Got group of unknown type: 'internal'不存在。)
(1)若当 x x x经过 x 0 { {x}_{0}} x0时,KaTeX parse error: Got group of unknown type: 'internal'由“+”变“-”,则 f ( x 0 ) f({ {x}_{0}}) f(x0)为极大值;
(2)若当 x ​ x​ x经过 x 0 ​ { {x}_{0}}​ x0时,KaTeX parse error: Got group of unknown type: 'internal'由“-”变“+”,则 f ( x 0 ) f({ {x}_{0}}) f(x0)为极小值;
(3)若KaTeX parse error: Got group of unknown type: 'internal'经过 x = x 0 x={ {x}_{0}} x=x0的两侧不变号,则 f ( x 0 ) f({ {x}_{0}}) f(x0)不是极值。

Th4: (取极值的第二充分条件)设 f ( x ) f(x) f(x)在点 x 0 { {x}_{0}} x0处有 f ′ ′ ( x ) ≠ 0 f''(x)\ne 0 f′′(x)=0,且KaTeX parse error: Got group of unknown type: 'internal',则 当KaTeX parse error: Got group of unknown type: 'internal'时, f ( x 0 ) f({ {x}_{0}}) f(x0)为极大值;
KaTeX parse error: Got group of unknown type: 'internal'时, f ( x 0 ) f({ {x}_{0}}) f(x0)为极小值。
注:如果KaTeX parse error: Got group of unknown type: 'internal',此方法失效。

13.渐近线的求法
(1)水平渐近线 若 lim ⁡ x → + ∞   f ( x ) = b \underset{x\to +\infty }{\mathop{\lim }}\,f(x)=b x+limf(x)=b,或 lim ⁡ x → − ∞   f ( x ) = b \underset{x\to -\infty }{\mathop{\lim }}\,f(x)=b xlimf(x)=b,则

y = b y=b y=b称为函数 y = f ( x ) y=f(x) y=f(x)的水平渐近线。

(2)铅直渐近线 若$\underset{x\to x_{0}^{-}}{\mathop{\lim }},f(x)=\infty ,或 ,或 ,或\underset{x\to x_{0}^{+}}{\mathop{\lim }},f(x)=\infty $,则

x = x 0 x={ {x}_{0}} x=x0称为 y = f ( x ) y=f(x) y=f(x)的铅直渐近线。

(3)斜渐近线 若 a = lim ⁡ x → ∞   f ( x ) x , b = lim ⁡ x → ∞   [ f ( x ) − a x ] a=\underset{x\to \infty }{\mathop{\lim }}\,\frac{f(x)}{x},\quad b=\underset{x\to \infty }{\mathop{\lim }}\,[f(x)-ax] a=xlimxf(x),b=xlim[f(x)ax],则
y = a x + b y=ax+b y=ax+b称为 y = f ( x ) y=f(x) y=f(x)的斜渐近线。

14.函数凹凸性的判断
Th1: (凹凸性的判别定理)若在I上 f ′ ′ ( x ) < 0 f''(x)<0 f′′(x)<0(或 f ′ ′ ( x ) > 0 f''(x)>0 f′′(x)>0),则 f ( x ) f(x) f(x)在I上是凸的(或凹的)。

Th2: (拐点的判别定理1)若在 x 0 { {x}_{0}} x0 f ′ ′ ( x ) = 0 f''(x)=0 f′′(x)=0,(或 f ′ ′ ( x ) f''(x) f′′(x)不存在),当 x x x变动经过 x 0 { {x}_{0}} x0时, f ′ ′ ( x ) f''(x) f′′(x)变号,则 ( x 0 , f ( x 0 ) ) ({ {x}_{0}},f({ {x}_{0}})) (x0,f(x0))为拐点。

Th3: (拐点的判别定理2)设 f ( x ) f(x) f(x) x 0 { {x}_{0}} x0点的某邻域内有三阶导数,且 f ′ ′ ( x ) = 0 f''(x)=0 f′′(x)=0 f ′ ′ ′ ( x ) ≠ 0 f'''(x)\ne 0 f′′′(x)=0,则 ( x 0 , f ( x 0 ) ) ({ {x}_{0}},f({ {x}_{0}})) (x0,f(x0))为拐点。

15.弧微分

d S = 1 + y ′ 2 d x dS=\sqrt{1+y{ {'}^{2}}}dx dS=1+y2 dx

16.曲率

曲线 y = f ( x ) y=f(x) y=f(x)在点 ( x , y ) (x,y) (x,y)处的曲率 k = ∣ y ′ ′ ∣ ( 1 + y ′ 2 ) 3 2 k=\frac{\left| y'' \right|}{ { {(1+y{ {'}^{2}})}^{\tfrac{3}{2}}}} k=(1+y2)23y′′
对于参数方程KaTeX parse error: {align} can be used only in display mode. k = ∣ φ ′ ( t ) ψ ′ ′ ( t ) − φ ′ ′ ( t ) ψ ′ ( t ) ∣ [ φ ′ 2 ( t ) + ψ ′ 2 ( t ) ] 3 2 k=\frac{\left| \varphi '(t)\psi ''(t)-\varphi ''(t)\psi '(t) \right|}{ { {[\varphi { {'}^{2}}(t)+\psi { {'}^{2}}(t)]}^{\tfrac{3}{2}}}} k=[φ2(t)+ψ2(t)]23φ(t)ψ′′(t)φ′′(t)ψ(t)

17.曲率半径

曲线在点 M M M处的曲率 k ( k ≠ 0 ) k(k\ne 0) k(k=0)与曲线在点 M M M处的曲率半径$\rho 有如下关系: 有如下关系: 有如下关系:\rho =\frac{1}{k}$。

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