卷二 · 数学之美27 分钟阅读

函数导数十:隐函数、隐映射定理

定义1:隐式方程

设D⊂R2D \subset \mathbb{R}^2是一开集,F:D→RF: D \to \mathbb{R}是一个含有两个自变量x,yx,y的函数,对于DD中的点(x,y)(x,y)满足方程

F(x,y)=0 F(x,y) = 0

的点的全体组成DD内的一条曲线,而方程就称为该曲线的隐式方程。

定理1:隐函数定理

设开集D⊂R2D \subset \mathbb{R}^2,函数F:D→RF: D \to \mathbb{R}满足条件:
(a)F∈C1(D)F \in C^1(D);
(b)点(x0,y0)∈D(x_0,y_0) \in D使得F(x0,y0)=0F(x_0,y_0) = 0;
(c)∂F(x0,y0)∂y≠0\dfrac{\partial F(x_0,y_0)}{\partial y} \ne 0
那么存在一个包含(x0,y0)(x_0,y_0)的开矩形I×J⊂DI \times J \subset D,使得:
(1)对每一个x∈Ix \in I,方程F(x,y)=0F(x,y)=0在JJ中有唯一的解f(x)f(x);
(2)y0=f(x0)y_0 = f(x_0);
(3)f∈C1(I)f \in C^1(I);
(4)当x∈Ix \in I时,有

f′(x)=−∂F∂x(x,y)∂F∂y(x,y) f^\prime(x) = -\frac{\frac{\partial F}{\partial x}(x,y)}{\frac{\partial F}{\partial y}(x,y)}

其中y=f(x)y = f(x)。

证:不妨设∂F(x0,y0)∂y>0\displaystyle \frac{\partial F(x_0,y_0)}{\partial y} > 0,由条件(a)(a)可知,存在一个包含(x0,y0)(x_0,y_0)的开矩形I′×JI^\prime \times J,满足I′×Jˉ⊂DI^\prime \times \bar J \subset D,且在I′×JˉI^\prime \times \bar J上有∂F∂y>0\displaystyle \frac{\partial F}{\partial y} > 0。从而对任意给定的x∈I′x \in I^\prime,F(x,y)F(x,y)在闭区间Jˉ\bar J上是严格递增的连续函数。设J=(c,d)J = (c,d),由条件(b)(b)可知必有

F(x0,c)<0,F(x0,d)>0 F(x_0, c) < 0, \quad F(x_0, d) > 0

由条件(a)(a)能推出F∈C(D)F \in C(D),因此存在含x0x_0的开区间I⊂I′I \subset I^\prime,使得当x∈Ix \in I时,
F(x,c)<0,F(x,d)>0 F(x, c) < 0, \quad F(x, d) > 0

由连续函数的零值定理和严格单调性可知,对每一个x∈Ix \in I,存在唯一的一个数,记作f(x)∈(c,d)=Jf(x) \in (c, d) = J,使得F(x,f(x))=0F(x, f(x)) = 0,这就证明了(1),显然ff满足(2)。
为了证明(3)和(4),先证明ff在开区间II上连续。特别地,x0∈Ix_0 \in I,由上面的证明可知无论区间JJ取得多小,一定存在足够小的区间II使得对每一个x∈Ix \in I时,有f(x)∈Jf(x) \in J;这时∣f(x)−f(x0)∣<∣J∣|f(x) - f(x_0)| < |J|,其中∣J∣|J|表示区间JJ的长度。即证明了ff在x0x_0处连续。现任取x1∈Ix_1 \in I,设y1=f(x1)y_1 = f(x_1),则(x1,y1)∈I×J(x_1,y_1) \in I \times J。因为有F(x1,y1)=0F(x_1,y_1)=0,∂F(x1,y1)∂y>0\displaystyle \frac{\partial F(x_1,y_1)}{\partial y} > 0,所以FF在点(x1,y1)(x_1,y_1)处满足它在(x0,y0)(x_0,y_0)处的同样条件,所以ff在x1x_1处也是连续的,从而ff在整个区间II上连续。
再证(3)和(4)。设x∈Ix \in I,取hh很小,使得x+h∈Ix+h \in I。令y=f(x)y = f(x),k=f(x+h)−f(x)k = f(x+h) - f(x)。由FF的可微性,并利用函数导数八的定理1可得
0=F(x+h,y+k)−F(x,y)=∂F∂x(x,y)h+∂F∂y(x,y)k+αh+βk 0 = F(x+h, y+k) - F(x, y) = \frac{\partial F}{\partial x}(x, y) h + \frac{\partial F}{\partial y}(x, y) k + \alpha h + \beta k

其中当h→0h \to 0时,α→0\alpha \to 0,当k→0k \to 0时,β→0\beta \to 0。又由于f∈C(I)f \in C(I),所以当h→0h \to 0时,k→0k \to 0,从而β→0\beta \to 0。从而
lim⁡h→0f(x+h)−f(x)h=lim⁡h→0kh=lim⁡h→0−∂F∂x+α∂F∂y+β \lim \limits_{h \to 0} \frac{f(x + h) - f(x)}{h} = \lim \limits_{h \to 0} \frac{k}{h} = \lim\limits_{h \to 0} \frac{-\frac{\partial F}{\partial x} + \alpha}{\frac{\partial F}{\partial y} + \beta}

即
f′(x)=−∂F∂x(x,y)∂F∂y(x,y) f^\prime(x) = - \frac{\frac{\partial F}{\partial x} (x, y)}{\frac{\partial F}{\partial y} (x,y)}

其中x∈Ix \in I且y=f(x)y = f(x)。由于(a)(a)知,f′f^\prime在II上连续。

Q.E.D.

定理2

设开集D⊂Rn+1D \subset \mathbb{R}^{n+1},F:D→RF: D \to \mathbb{R},满足条件:
(a)F∈C1(D)F \in C^1(D);
(b)F(x0,y0)=0F(\boldsymbol{x}_0, y_0) = 0,这里x0∈Rn,y0∈R\boldsymbol{x}_0 \in \mathbb{R}^n,y_0 \in \mathbb{R}且(x0,y0)∈D(\boldsymbol{x}_0, y_0) \in D;
(c)∂F(x0,y0)∂y≠0\dfrac{\partial F(\boldsymbol{x}_0, y_0)}{\partial y} \ne 0。
那么存在(x0,y0)(\boldsymbol{x}_0, y_0)的一个邻域G×JG \times J,其中GG是x0\boldsymbol{x_0}在Rn\mathbb{R}^n的一个邻域,JJ是R\mathbb{R}中的一个开区间,使得:
(1)对每一个x∈G\boldsymbol{x} \in G,方程

F(x,y)=0 F(\boldsymbol{x}, y) = 0

在JJ中存在唯一的解,记为f(x)f(\boldsymbol{x});
(2)y0=f(x0)y_0 = f(\boldsymbol{x}_0);
(3)f∈C1(G)f \in C^1(G);
(4)当x∈G\boldsymbol{x} \in G时,
∂f∂xi=−∂F∂xi(x,y)∂F∂y(x,y)(i=1,2,⋯ ,n) \frac{\partial f}{\partial x_i} = - \frac{\frac{\partial F}{\partial x_i}(\boldsymbol{x}, y)}{\frac{\partial F}{\partial y}(\boldsymbol{x}, y)} \quad (i=1,2,\cdots,n)

其中y=f(x)y = f(\boldsymbol{x})。

证:由定理1的证明,可知(1)(2)的证明方式一模一样;而在证明(3)(4)时,只需令h=(0,⋯ ,hi,⋯ ,0)T\boldsymbol{h} = (0, \cdots, h_i, \cdots, 0)^T,固定xix_i,其他证明过程一样,即可证得(3)和(4)。

Q.E.D.


设有mm个方程组成的方程组

{F1(x1,x2,⋯ ,xn,y1,⋯ ,ym)=0⋯ ,Fm(x1,x2,⋯ ,xn,y1,⋯ ,ym)=0 \left\{ \begin{aligned} & F_1(x_1,x_2,\cdots,x_n, y_1,\cdots, y_m) = 0 \\ & \cdots, \\ & F_m(x_1,x_2,\cdots,x_n, y_1,\cdots, y_m) = 0 \end{aligned} \right.

按照隐函数的想法,是否可以解出
{y1=f1(x1,⋯ ,xn)⋯ym=fm(x1,⋯ ,xn) \left\{ \begin{aligned} & y_1 = f_1(x_1,\cdots,x_n) \\ & \cdots \\ & y_m = f_m(x_1,\cdots,x_n) \end{aligned} \right.

为了缩短记号,可令
F=[F1⋮Fm],f=[f1⋮fm] \boldsymbol{F} = \left[ \begin{matrix} F_1 \\ \vdots \\ F_m \end{matrix} \right], \quad \boldsymbol{f} = \left[ \begin{matrix} f_1 \\ \vdots \\ f_m \end{matrix} \right]

从而可以把方程改写为
F(x,y)=0 \boldsymbol{F}(\boldsymbol{x}, \boldsymbol{y}) = \boldsymbol{0}

而解出式可改写为
y=f(x) \boldsymbol{y} = \boldsymbol{f}(\boldsymbol{x})

需要再定义几个记号,设F\boldsymbol{F}定义在开集D⊂Rm+nD \subset \mathbb{R}^{m+n}上,在m×(m+n)m \times (m+n)矩阵
JF=[∂F1∂x1⋯∂F1∂xn∂F1∂y1⋯∂F1∂ym⋮⋮⋮⋮∂Fm∂x1⋯∂Fm∂xn∂Fm∂y1⋯∂Fm∂ym] J\boldsymbol{F} = \left[ \begin{matrix} \frac{\partial F_1}{\partial x_1} & \cdots & \frac{\partial F_1}{\partial x_n} & \frac{\partial F_1}{\partial y_1} & \cdots & \frac{\partial F_1}{\partial y_m} \\ \vdots & & \vdots & \vdots & & \vdots \\ \frac{\partial F_m}{\partial x_1} & \cdots & \frac{\partial F_m}{\partial x_n} & \frac{\partial F_m}{\partial y_1} & \cdots & \frac{\partial F_m}{\partial y_m} \end{matrix} \right]

中做分块:JF=(JxF,JyF)J\boldsymbol{F} = (J_{\boldsymbol{x}}\boldsymbol{F}, J_{\boldsymbol{y}}\boldsymbol{F}),其中
JxF=[∂F1∂x1⋯∂F1∂xn⋮⋮∂Fm∂x1⋯∂Fm∂xn],JyF=[∂F1∂y1⋯∂F1∂ym⋮⋮∂Fm∂y1⋯∂Fm∂ym] J_{\boldsymbol{x}}\boldsymbol{F} = \left[ \begin{matrix} \frac{\partial F_1}{\partial x_1} & \cdots & \frac{\partial F_1}{\partial x_n} \\ \vdots & & \vdots\\ \frac{\partial F_m}{\partial x_1} & \cdots & \frac{\partial F_m}{\partial x_n} \end{matrix} \right], \quad J_{\boldsymbol{y}}\boldsymbol{F} = \left[ \begin{matrix} \frac{\partial F_1}{\partial y_1} & \cdots & \frac{\partial F_1}{\partial y_m} \\ \vdots & & \vdots \\ \frac{\partial F_m}{\partial y_1} & \cdots & \frac{\partial F_m}{\partial y_m} \end{matrix} \right]

JxFJ_{\boldsymbol{x}}\boldsymbol{F}是一个m×nm \times n矩阵,JyFJ_{\boldsymbol{y}}\boldsymbol{F}是一个mm阶方阵。

定理3:隐映射定理

设开集D⊂Rn+mD \subset \mathbb{R}^{n+m},F:D→Rm\boldsymbol{F}: D \to \mathbb{R}^m,满足下列条件:
(a)F∈C1(D)\boldsymbol{F} \in C^1(D);
(b)有一点(x0,y0)∈D(\boldsymbol{x}_0, \boldsymbol{y}_0) \in D,使得F(x0,y0)=0\boldsymbol{F}(\boldsymbol{x}_0, \boldsymbol{y}_0) = \boldsymbol{0};
(c)行列式det⁡JyF(x0,y0)≠0\det J_{\boldsymbol{y}} \boldsymbol{F}(\boldsymbol{x}_0, \boldsymbol{y}_0) \ne 0
那么存在(x0,y0)(\boldsymbol{x}_0, \boldsymbol{y}_0)的一个邻域G×HG \times H,使得:
(1)对每一个x∈G\boldsymbol{x} \in G,方程F(x,y)=0\boldsymbol{F}(\boldsymbol{x}, \boldsymbol{y})=\boldsymbol{0}在HH中有唯一的解,记为f(x)\boldsymbol{f}(\boldsymbol{x});
(2)y0=f(x0)\boldsymbol{y}_0 = \boldsymbol{f}(\boldsymbol{x}_0)
(3)f∈C1(D)\boldsymbol{f} \in C^1(D)
(4)当x∈G\boldsymbol{x} \in G时,

Jf(x)=−(JyF(x,y)−1)JxF(x,y) J\boldsymbol{f}(\boldsymbol{x}) = -(J_{\boldsymbol{y}}\boldsymbol{F}(\boldsymbol{x}, \boldsymbol{y})^{-1})J_{\boldsymbol{x}}\boldsymbol{F}(\boldsymbol{x}, \boldsymbol{y})

其中y=f(x)\boldsymbol{y} = \boldsymbol{f}(\boldsymbol{x})

证:对方程组的个数mm进行归纳。当m=1m=1时,即为该定理定理2。先设方程组个数为m−1m-1时该定理成立,再证明在mm时依然成立即可。
由于det⁡JyF(x0,y0)≠0\det J_{\boldsymbol{y}}\boldsymbol{F}(\boldsymbol{x}_0, \boldsymbol{y}_0) \ne 0,且F∈C1(D)\boldsymbol{F} \in C^1(D),所以总可以找到一个包含(x0,y0)(\boldsymbol{x}_0, \boldsymbol{y}_0)的开集D′D^\prime满足(x0,y0)∈D′⊂D(\boldsymbol{x}_0, \boldsymbol{y}_0) \in D^\prime \subset D,且在D′D^\prime上的每一个点处都有det⁡JyF≠0\det J_{\boldsymbol{y}}\boldsymbol{F} \ne 0。由条件(c)(c)可知mm阶方阵JyF(x0,y0)J_{\boldsymbol{y}}\boldsymbol{F}(\boldsymbol{x}_0, \boldsymbol{y}_0)的元素不全为00,不妨设

∂Fm∂yj(x0,y0)≠0(1) \frac{\partial F_m}{\partial y_j}(\boldsymbol{x}_0, \boldsymbol{y}_0) \ne 0 \tag{1}

同时令
u=(y1,⋯ ,ym−1),t=ym,y=(u,t) \boldsymbol{u} = (y_1, \cdots, y_{m-1}), \quad t = y_m, \quad \boldsymbol{y} = (\boldsymbol{u}, t)

同样可以定义y0=(u0,t0)\boldsymbol{y}_0 = (\boldsymbol{u}_0, t_0)来规定u0\boldsymbol{u}_0和t0t_0的意义,从而式(1)可写成
∂Fm∂t(x0,u0,t0)≠0 \frac{\partial F_m}{\partial t}(\boldsymbol{x}_0, \boldsymbol{u}_0, t_0) \ne 0

又有
Fm(x0,u0,t0)=Fm(x0,y0)=0 F_m (\boldsymbol{x}_0, \boldsymbol{u}_0, t_0) = F_m(\boldsymbol{x}_0, \boldsymbol{y}_0) = 0

由定理2可知,存在(x0,u0,t0)(\boldsymbol{x}_0, \boldsymbol{u}_0, t_0)的一个邻域(Gn×Gm−1)×J⊂D′(G_n \times G_{m-1}) \times J \subset D^\prime,使得:
(i)对每一点(x,u)∈Gn×Gm=1(\boldsymbol{x}, \boldsymbol{u}) \in G_{n} \times G_{m=1},方程
Fm(x,u,t)=0 F_m(\boldsymbol{x}, \boldsymbol{u}, t) = 0

在JJ中有唯一的解t=φ(x,u)t = \varphi(\boldsymbol{x}, \boldsymbol{u}),这里函数φ:Gn×Gm−1→J\varphi: G_n \times G_{m-1} \to J;
(ii)φ(x0,u0)=t0\varphi(\boldsymbol{x}_0, \boldsymbol{u}_0) = t_0;
(iii)φ∈C1(Gn×Gm−1)\varphi \in C^1(G_{n} \times G_{m-1});
这时将t=φ(x,u)t = \varphi(\boldsymbol{x}, \boldsymbol{u})代入到原始方程中,即将ymy_m用x1,⋯ ,xn,y1,⋯ ,ym−1x_1,\cdots,x_n,y_1,\cdots,y_{m-1}代入,
Φi(x,u)=Fi(x,u,φ(x,u))=0(i=1,2,⋯ ,m−1)(2) \Phi_i(\boldsymbol{x}, \boldsymbol{u}) = F_i(\boldsymbol{x}, \boldsymbol{u}, \varphi(\boldsymbol{x}, \boldsymbol{u})) = 0 \quad (i=1,2,\cdots,m-1) \tag{2}

考虑映射
Φ=[Φ1⋮Φm−1]:Gn×Gm−1→Rm−1 \boldsymbol{\Phi} = \left[\begin{matrix} \Phi_1 \\ \vdots \\ \Phi_{m-1} \end{matrix}\right]: G_n \times G_{m-1} \to \mathbb{R}^{m-1}

若能证明Φ\boldsymbol{\Phi}满足定理的三个条件,便可使用归纳假设了。显然Φ∈C1\boldsymbol{\Phi} \in C^1,并且
ϕi(x0,u0)=Fi(x0,u0,φ(x0,u0))=0(i=1,2⋯ ,m−1) \phi_i(\boldsymbol{x}_0, \boldsymbol{u}_0) = F_i(\boldsymbol{x}_0, \boldsymbol{u}_0, \varphi(\boldsymbol{x}_0, \boldsymbol{u}_0)) = 0 \quad (i=1,2\cdots,m-1)

所以Φ(x0,y0)=0\boldsymbol{\Phi}(\boldsymbol{x}_0, \boldsymbol{y}_0)=\boldsymbol{0}。对式(2)两边同时关于uju_j(即yjy_j)(j=1,2,⋯ ,m−1)(j=1,2,\cdots,m-1)求导,得
∂Φi∂uj=∂Fi∂yj+∂Fi∂ym∂φ∂uj(i,j=1,2,⋯ ,m−1) \frac{\partial \Phi_i}{\partial u_j} = \frac{\partial F_i}{\partial y_j} + \frac{\partial F_i}{\partial y_m} \frac{\partial \varphi}{\partial u_j} \quad (i,j=1,2,\cdots,m-1)

又由(i)可知
Fm(x,u,φ(x,u))=0 F_m(\boldsymbol{x}, \boldsymbol{u}, \varphi(\boldsymbol{x}, \boldsymbol{u})) = 0

对上式也关于uju_j(即yjy_j)(j=1,2,⋯ ,m−1)(j=1,2,\cdots,m-1)求导得
∂Fm∂yj+∂Fm∂ym∂φ∂uj=0(j=1,2,⋯ ,m−1) \frac{\partial F_m}{\partial y_j} + \frac{\partial F_m}{\partial y_m} \frac{\partial \varphi}{\partial u_j} = 0 \quad (j=1,2,\cdots,m-1)

从而由
∣∂F1∂y1⋯∂F1∂ym⋮⋮∂Fm∂y1⋯∂Fm∂ym∣=∣∂F1∂y1+∂F1∂ym∂φ∂u1∂F1∂y2+∂F1∂ym∂φ∂u2⋯∂F1∂ym⋮⋮⋮∂Fm∂y1+∂Fm∂ym∂φ∂u1∂Fm∂y2+∂Fm∂ym∂φ∂u2⋯∂Fm∂ym∣=∣∂Φ1∂u1⋯∂Φ1∂um−1∂F1∂ym⋮⋮⋮∂Φm−1∂u1⋯∂Φm−1∂um−1∂Fm−1∂ym0⋯0∂Fm∂ym∣=∂Fm∂ym(x0,u0,t0)det⁡(JuΦ(x0,u0))(3) \begin{aligned} \left| \begin{matrix} \frac{\partial F_1}{\partial y_1} & \cdots & \frac{\partial F_1}{\partial y_m} \\ \vdots & & \vdots \\ \frac{\partial F_m}{\partial y_1} & \cdots & \frac{\partial F_m}{\partial y_m} \end{matrix} \right| & = \left| \begin{matrix} \frac{\partial F_1}{\partial y_1} + \frac{\partial F_1}{\partial y_m}\frac{\partial \varphi}{\partial u_1} & \frac{\partial F_1}{\partial y_2} + \frac{\partial F_1}{\partial y_m}\frac{\partial \varphi}{\partial u_2} & \cdots & \frac{\partial F_1}{\partial y_m} \\ \vdots & \vdots & & \vdots \\ \frac{\partial F_m}{\partial y_1} + \frac{\partial F_m}{\partial y_m}\frac{\partial \varphi}{\partial u_1} & \frac{\partial F_m}{\partial y_2} + \frac{\partial F_m}{\partial y_m}\frac{\partial \varphi}{\partial u_2} & \cdots & \frac{\partial F_m}{\partial y_m} \end{matrix} \right| \\ & = \left| \begin{matrix} \frac{\partial \Phi_1}{\partial u_1} & \cdots & \frac{\partial \Phi_1}{\partial u_{m-1}} & \frac{\partial F_1}{\partial y_m} \\ \vdots & & \vdots & \vdots \\ \frac{\partial \Phi_{m-1}}{\partial u_1} & \cdots & \frac{\partial \Phi_{m-1}}{\partial u_{m-1}} & \frac{\partial F_{m-1}}{\partial y_m} \\ 0 & \cdots & 0 & \frac{\partial F_m}{\partial y_m} \end{matrix} \right| \\ & = \frac{\partial F_m}{\partial y_m}(\boldsymbol{x}_0, \boldsymbol{u}_0, t_0) \det(J_{\boldsymbol{u}} \boldsymbol{\Phi}(\boldsymbol{x}_0, \boldsymbol{u}_0)) \end{aligned} \tag{3}

根据条件(c),式子(3)的左边不等于0,因为有
det⁡(JuΦ(x0,u0))≠0 \det(J_{\boldsymbol{u}} \boldsymbol{\Phi}(\boldsymbol{x}_0, \boldsymbol{u}_0)) \ne 0

从而证明了Φ\boldsymbol{\Phi}满足本定理中的三个条件,从而对Φ\boldsymbol{\Phi}使用归纳假设,可知定理中的结论(1),(2)和(3)对Φ\boldsymbol{\Phi}都成立。即存在点(x0,y0)(\boldsymbol{x}_0, \boldsymbol{y}_0)的邻域G×Hm−1⊂Gn×Gm−1G \times H_{m-1} \subset G_n \times G_{m-1}使得:
(aa)当x∈G\boldsymbol{x} \in G时,方程ϕ(x,u)=0\boldsymbol{\phi}(\boldsymbol{x}, \boldsymbol{u}) = \boldsymbol{0}在Hm−1H_{m-1}中有唯一解u=g(x)\boldsymbol{u} = \boldsymbol{g}(\boldsymbol{x}),其中映射g:G→Hm−1\boldsymbol{g}: G \to H_{m-1};
(ab)x0=u0\boldsymbol{\boldsymbol{x}_0} = \boldsymbol{u}_0;
(ac)g∈C1(G)\boldsymbol{g} \in C^1(G)
令
f(x)=(g(x),φ(x,g(x)))(x∈G) \boldsymbol{f}(\boldsymbol{x}) = (\boldsymbol{g}(\boldsymbol{x}), \varphi(\boldsymbol{x}, \boldsymbol{g}(\boldsymbol{x}))) \quad (\boldsymbol{x} \in G)

H=Hm−1×J H = H_{m-1} \times J

于是f:G→H\boldsymbol{f}: G \to H。我们要证明f\boldsymbol{f}满足条件(1),(2)和(3)。当x∈G\boldsymbol{x} \in G,(x,g(x))∈G×Hm−1⊂Gn×Gm−1(\boldsymbol{x}, \boldsymbol{g}(\boldsymbol{x})) \in G \times H_{m-1} \subset G_n \times G_{m-1},从而由(aa)可得
Fi(x,f(x))=Fi(x,g(x),φ(x,g(x)))=Φi(x,g(x))=0(i=1,2,⋯ ,m−1) F_i(\boldsymbol{x}, \boldsymbol{f}(\boldsymbol{x})) = F_i(\boldsymbol{x}, \boldsymbol{g}(\boldsymbol{x}), \varphi(\boldsymbol{x}, \boldsymbol{g}(\boldsymbol{x}))) = \Phi_i(\boldsymbol{x}, \boldsymbol{g}(\boldsymbol{x})) = 0 \quad (i=1,2,\cdots,m-1)

另外由(i)可知
Fm(x,g(x))=Fm(x,g(x),φ(x,g(x)))=0 F_m(\boldsymbol{x}, \boldsymbol{g}(\boldsymbol{x})) = F_m(\boldsymbol{x}, \boldsymbol{g}(\boldsymbol{x}), \varphi(\boldsymbol{x}, \boldsymbol{g}(\boldsymbol{x}))) = 0

从而f\boldsymbol{f}满足(1)。由(ab)和(ii)可知
f(x0)=(g(x0),φ(x0,g(x0)))=(u0,φ(x0,u0))=(u0,t0)=y0 \boldsymbol{f}(\boldsymbol{x}_0) = (\boldsymbol{g}(\boldsymbol{x}_0), \varphi(\boldsymbol{x}_0, \boldsymbol{g}(\boldsymbol{x}_0))) = (\boldsymbol{u}_0, \varphi(\boldsymbol{x}_0, \boldsymbol{u}_0)) = (\boldsymbol{u}_0, t_0) = \boldsymbol{y}_0

所以f\boldsymbol{f}满足(2)。再由(ac)和(iii)即知f\boldsymbol{f}满足(3)。再由恒等式
F(x,f(x))=0 \boldsymbol{F}(\boldsymbol{x}, \boldsymbol{f}(\boldsymbol{x})) = \boldsymbol{0}

对上式复合求导,得
JxF(x,f(x))+JyF(x,f(x))Jf(x)=0 J_{\boldsymbol{x}} \boldsymbol{F}(\boldsymbol{x}, \boldsymbol{f}(\boldsymbol{x})) + J_y \boldsymbol{F}(\boldsymbol{x}, \boldsymbol{f}(\boldsymbol{x})) J\boldsymbol{f}(\boldsymbol{x}) = \boldsymbol{0}

由于在D′D^\prime上det⁡JyF\det J_{\boldsymbol{y}}\boldsymbol{F}处处不为0,所以JyFJ_{\boldsymbol{y}}\boldsymbol{F}是可逆方阵,在上式中取逆方阵,得出
Jf(x)=−(JyF(x,f(x)))−1JxF(x,f(x)) J\boldsymbol{f}(\boldsymbol{x}) = -(J_{\boldsymbol{y}}\boldsymbol{F}(\boldsymbol{x}, \boldsymbol{f}(\boldsymbol{x})))^{-1}J_{\boldsymbol{x}}\boldsymbol{F}(\boldsymbol{x}, \boldsymbol{f}(\boldsymbol{x}))

即表明f\boldsymbol{f}满足(4)。

Q.E.D.

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