工科数学分析-3.23
2026-03-23
二元函数z=f(x,y),目标函数,g(x,y)=0约束条件设方程g(x,y)=0确定的隐函数y=y(x),g_y(P_0)\neq 0,P_0(x_0,y_0)若极值点在点P_{0}(x_{0},y_{0})取到,则z=f(x,y(x))在x=x_{0}取到极值,于是\frac{dz}{dx}=f_{x}+f_{y}\frac{dy}{dx}=0\frac{d}{dx}g(x,y(x))=g_{x}+g_{y}\frac{dy}{dx}=0\nabla f,\nabla g \perp(1,\frac{dy}{dx}=\vec{T}),\nabla f//\nabla g 因此,存在常数\lambda_{0},使得\nabla f(P_{0})=\lambda_{0}\nabla g(P{0}),g(p_{0})=0(*2)引入变量\lambda与函数L(x,y,\lambda)=f(x,y)-\lambda g(x,y)(*3)因为
741 words
|
4 minutes
工科数学分析-3.19
2026-03-19
设函数f定义在一个点p_{0}的某个领域U_{p_{0}}内,若对于任何p\in U_{p_{0}},有f(p)\le f_{p_{0}},此时称f在p_{0}取到极大值,若不等号反向,则称f在p_{0}取到极小值。设f(x,y)在点P(x_{0},y_{0})取到极值,则对任何实数h,考虑两个一元函数\varphi(t)=f(x_{0}+th,y_{0}),\psi(t)=f(x_{0},y_{0}+th)(要求偏导数存在)均在t=0取极值,有Fermat引理\varphi'(0)=f_{x}(x_{0},y_{0})h=0,\psi'(0)=f_{y}(x_{0},y_{0})h=0由于h的任意性,f_{x}(x_{0},y_{0})=f_{y}(x_{0},y_{0})=0
853 words
|
4 minutes
工科数学分析-3.16
2026-03-16
z=f(x,y)\frac{\partial z}{\partial x}=f_{x}(x,y)\frac{\partial}{\partial x}(\frac{\partial z}{\partial x})=\frac{\partial^2 z}{\partial x^{2}}=f_{xx}(x,y)=f_{11}\frac{\partial}{\partial x}(\frac{\partial z}{\partial y})=\frac{\partial^2 z}{\partial x\partial y}=f_{xy}(x,y)=f_{12}\frac{\partial}{\partial y}(\frac{\partial z}{\partial y})=\frac{\partial^2 z}{\partial y^{2}}=f_{yy}(x,y)=f_{22}\frac{\partial}{\partial y}(\frac{\partial z}{\partial x})=\frac{\partial^2 z}{\partial y\partial x}=f_{yx}(x,y)=f_{21}
892 words
|
4 minutes