隐函数存在定理
例题:
1.设有二元函数x y − z ln y + z 2 = 1 x y-z \ln y+z^{2}=1xy−zlny+z2=1,根据隐函数存在定理,存在点( 1 , 1 , 0 ) (1,1,0)(1,1,0)的一个邻域,在此邻域内该方程()
A.只能确定一个具有连续偏导数的隐函数z = z ( x , y ) z=z(x, y)z=z(x,y)
B.可确定两个具有连续偏导数的隐函数y = y ( x , z ) y=y(x, z)y=y(x,z)和z = z ( x , y ) z=z(x, y)z=z(x,y)
C.可确定两个具有连续偏导数的隐函数x = x ( y , z ) x=x(y, z)x=x(y,z)和z = z ( x , y ) z=z(x, y)z=z(x,y)
D.可确定两个具有连续偏导数的隐函数x = x ( y , z ) x=x(y, z)x=x(y,z)和y = y ( x , z ) y=y(x, z)y=y(x,z)
解析:令
F ( x , y , z ) = x y − z ln y + z 2 − 1 F(x, y, z)=x y-z \ln y+z^{2}-1F(x,y,z)=xy−zlny+z2−1
则
F ( 1 , 1 , 0 ) = 0 F(1,1,0)=0F(1,1,0)=0
且
F x ′ = y , F y ′ = x − z y , F z ′ = − ln y + 2 z F x ′ ( 1 , 1 , 0 ) = 1 , F y ′ ( 1 , 1 , 0 ) = 1 , F z ′ ( 1 , 1 , 0 ) = 0 \begin{array}{c} F_{x}^{\prime}=y, F_{y}^{\prime}=x-\frac{z}{y}, F_{z}^{\prime}=-\ln y+2 z \\ F_{x}^{\prime}(1,1,0)=1, F_{y}^{\prime}(1,1,0)=1, F_{z}^{\prime}(1,1,0)=0 \end{array}Fx′=y,Fy′=x−yz,Fz′=−lny+2zFx′(1,1,0)=1,Fy′(1,1,0)=1,Fz′(1,1,0)=0
由隐函数存在定理可知,只能确定两个具有连续偏导数的函数x = x ( y , z ) x=x(y, z)x=x(y,z)和y = y ( x , z ) y=y(x, z)y=y(x,z),故应选D。
注解:
隐函数存在定理1:设函数F ( x , y ) F(x, y)F(x,y)在点P ( x 0 , y 0 ) P\left(x_{0}, y_{0}\right)P(x0,y0)的某一邻域内具有连续偏导数,且F ( x 0 , y 0 ) = 0 , F y ( x 0 , y 0 ) ≠ 0 F\left(x_{0}, y_{0}\right)=0, F_{y}\left(x_{0}, y_{0}\right) \neq 0F(x0,y0)=0,Fy(x0,y0)=0,则方程F ( x , y ) = 0 F(x, y)=0F(x,y)=0在点( x 0 , y 0 ) \left(x_{0}, y_{0}\right)(x0,y0)的某一个邻域内恒内确定一个连续且具有连续导数的函数y = f ( x ) y=f(x)y=f(x),它满足条件y 0 = f ( x 0 ) y_{0}=f\left(x_{0}\right)y0=f(x0),并有
d y d x = − F x F y \frac{\mathrm{d} y}{\mathrm{d} x}=-\frac{F_{x}}{F_{y}}dxdy=−FyFx
隐函数存在定理2:设函数F ( x , y , z ) F(x, y, z)F(x,y,z)在点P ( x 0 , y 0 , z 0 ) P\left(x_{0}, y_{0}, z_{0}\right)P(x0,y0,z0)的某一邻域内具有连续偏导数,且F ( x 0 , y 0 , z 0 ) = 0 , F z ( x 0 , y 0 , z 0 ) ≠ 0 F\left(x_{0}, y_{0}, z_{0}\right)=0, F_{z}\left(x_{0}, y_{0}, z_{0}\right) \neq 0F(x0,y0,z0)=0,Fz(x0,y0,z0)=0,则方程F ( x , y , z ) = 0 F(x, y, z)=0F(x,y,z)=0在点( x 0 , y 0 , z 0 ) \left(x_{0}, y_{0}, z_{0}\right)(x0,y0,z0)的某一邻域内恒能唯一确定一个连续且具有连续偏导数的函数z = f ( x , y ) z=f(x,y)z=f(x,y),他满足条件z 0 = f ( x 0 , y 0 ) z_{0}=f\left(x_{0}, y_{0}\right)z0=f(x0,y0),并有
∂ z ∂ x = − F x F z , ∂ z ∂ y = − F y F z \frac{\partial z}{\partial x}=-\frac{F_{x}}{F_{z}}, \frac{\partial z}{\partial y}=-\frac{F_{y}}{F_{z}}∂x∂z=−FzFx,∂y∂z=−FzFy
隐函数存在定理3:设F ( x , y , u , v ) , G ( x , y , u , v ) F(x, y, u, v), G(x, y, u, v)F(x,y,u,v),G(x,y,u,v)在点P ( x 0 , y 0 , u 0 , v 0 ) P\left(x_{0}, y_{0}, u_{0}, v_{0}\right)P(x0,y0,u0,v0)的某一邻域内具有对各个变量的连续偏导数,又F ( x 0 , y 0 , u 0 , v 0 ) = 0 , G ( x 0 , y 0 , u 0 , v 0 ) = 0 F\left(x_{0}, y_{0}, u_{0}, v_{0}\right)=0, G\left(x_{0}, y_{0}, u_{0}, v_{0}\right)=0F(x0,y0,u0,v0)=0,G(x0,y0,u0,v0)=0,且偏导数所组成的函数行列式
J = ∂ ( F , G ) ∂ ( u , v ) = ∣ ∂ F ∂ u ∂ F ∂ v ∂ G ∂ u ∂ G ∂ v ∣ J=\frac{\partial(F, G)}{\partial(u, v)}=\left|\begin{array}{ll} \frac{\partial F}{\partial u} & \frac{\partial F}{\partial v} \\ \frac{\partial G}{\partial u} & \frac{\partial G}{\partial v} \end{array}\right|J=∂(u,v)∂(F,G)=∣∣∣∣∂u∂F∂u∂G∂v∂F∂v∂G∣∣∣∣
在点P ( x 0 , y 0 , u 0 , v 0 ) P\left(x_{0}, y_{0}, u_{0}, v_{0}\right)P(x0,y0,u0,v0)不等于零,则方程则F ( x , y , u , v ) = 0 , G ( x , y , u , v ) = 0 F(x, y, u, v)=0, G(x, y, u, v)=0F(x,y,u,v)=0,G(x,y,u,v)=0在点( x 0 , y 0 , u 0 , v 0 ) \left(x_{0}, y_{0}, u_{0}, v_{0}\right)(x0,y0,u0,v0)的某一邻域内恒能确定一组连续且具有连续偏导数的函数u = u ( x , y ) , v = v ( x , y ) u=u(x, y), v=v(x, y)u=u(x,y),v=v(x,y),他们满足条件u 0 = u ( x 0 , y 0 ) , v 0 = v ( x 0 , y 0 ) u_{0}=u\left(x_{0}, y_{0}\right), v_{0}=v\left(x_{0}, y_{0}\right)u0=u(x0,y0),v0=v(x0,y0)
隐函数存在定理的应用:
例一:方程
x 2 y 2 − 3 y + 2 x 3 = 0 x^{2} y^{2}-3 y+2 x^{3}=0x2y2−3y+2x3=0
在点( 1 , 1 ) (1,1)(1,1)与( 1 , 2 ) (1,2)(1,2)两点的近旁定义着y yy为x xx的函数,试求f ′ ( 1 ) f^{\prime}(1)f′(1)
解析:令F ( x , y ) = x 2 y 2 − 3 y + 2 x 3 F(x, y)=x^{2} y^{2}-3 y+2 x^{3}F(x,y)=x2y2−3y+2x3,我们有F ( 1 , 1 ) = 0 F(1,1)=0F(1,1)=0及F ( 1 , 2 ) = 0 F(1,2)=0F(1,2)=0,此外:
∂ F ∂ y ( x , y ) = 2 x 2 y − 3 \frac{\partial F}{\partial y}(x, y)=2 x^{2} y-3∂y∂F(x,y)=2x2y−3
∂ F ∂ y ( 1 , 1 ) = − 1 , ∂ F ∂ y ( 1 , 2 ) = 1 \frac{\partial F}{\partial y}(1,1)=-1, \frac{\partial F}{\partial y}(1,2)=1∂y∂F(1,1)=−1,∂y∂F(1,2)=1
因此在( 1 , 1 ) (1,1)(1,1)近旁
f ′ ( 1 ) = − ∂ F ∂ x ( 1 , 1 ) ∂ F ∂ y ( 1 , 1 ) = − 8 − 1 = 8 f^{\prime}(1)=-\frac{\frac{\partial F}{\partial x}(1,1)}{\frac{\partial F}{\partial y}(1,1)}=\frac{-8}{-1}=8f′(1)=−∂y∂F(1,1)∂x∂F(1,1)=−1−8=8
在( 1 , 2 ) (1,2)(1,2)近旁
f ′ ( 1 ) = − ∂ F ∂ x ( 1 , 2 ) ∂ F ∂ y ( 1 , 2 ) = − 14 1 = − 14 f^{\prime}(1)=\frac{-\frac{\partial F}{\partial x}(1,2)}{\frac{\partial F}{\partial y}(1,2)}=\frac{-14}{1}=-14f′(1)=∂y∂F(1,2)−∂x∂F(1,2)=1−14=−14
这个例子不通过隐函数定理也能算出需要的答案,因为方程x 2 y 2 − 3 y + 2 x 3 = 0 x^{2} y^{2}-3 y+2 x^{3}=0x2y2−3y+2x3=0可以看做是y yy的二次方程,从中容易解出y yy对于x xx的依赖关系,然后直接求导即可。
例二:方程
sin x + log y − x y 3 = 0 \sin x+\log y-x y^{3}=0sinx+logy−xy3=0
在点( 0 , 1 ) (0,1)(0,1)的近旁确定函数y = f ( x ) y=f(x)y=f(x),求f ′ ( 0 ) f^{\prime}(0)f′(0)
解析:令F ( x , y ) = sin x + log y − x y 3 F(x, y)=\sin x+\log y-x y^{3}F(x,y)=sinx+logy−xy3,那么F ( 0 , 1 ) = 0 F(0,1)=0F(0,1)=0,而且:
∂ F ( 0 , 1 ) ∂ x = 0 , ∂ F ( 0 , 1 ) ∂ y = 1 \frac{\partial F(0,1)}{\partial x}=0, \frac{\partial F(0,1)}{\partial y}=1∂x∂F(0,1)=0,∂y∂F(0,1)=1
因此:
f ′ ( 0 ) = − ∂ F ∂ x ( 0 , 1 ) ∂ F ∂ y ( 0 , 1 ) = 0 f^{\prime}(0)=-\frac{\frac{\partial F}{\partial x}(0,1)}{\frac{\partial F}{\partial y}(0,1)}=0f′(0)=−∂y∂F(0,1)∂x∂F(0,1)=0
这个例子就非用隐函数定理不可,因为从给出的方程中无法解出y yy对x xx的显示关系