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4-多元微分

2019-09-19·Calculus
  • 偏导数:∂f∂xi(P0)=g′(ai)\frac{\partial f}{\partial x_i}(P_0)=g'(a_i)
  • 可微:∃δ>0,U(P0;δ)⊆Df,∃Ai∈R,∀Ps.t.∥ΔP∥<δ\exists\delta >0,U(P_0;\delta)\subseteq D_f,\exists A_i\in\mathbb{R},\forall P s.t. \lVert\Delta P\rVert<\delta 有 f(P0+ΔP)−f(P0)=∑i=1nAiΔxi+R(P0+ΔP)f(P_0+\Delta P)-f(P_0)=\sum_{i=1}^nA_i\Delta x_i+R(P_0+\Delta P) 且 lim⁡ΔP→0R(P0+δP)∥Δ∥\lim_{\Delta P\rightarrow 0}\frac{R(P_0+\delta P)}{\lVert\Delta\rVert}
    • Δf(P0;ΔP)=df(P0;ΔP)+o(∥ΔP∥),ΔP→0\Delta f(P_0;\Delta P)=df(P_0;\Delta P)+o(\lVert\Delta P\rVert),\Delta P\rightarrow 0
    • ∀i,∂f∂xi(P0)=Ai\forall i,\frac{\partial f}{\partial x_i}(P_0)=A_i
  • 微分:df(P0)=∑i=1n∂f∂xi(P0)dxidf(P_0)=\sum_{i=1}^n\frac{\partial f}{\partial x_i}(P_0)dx_i
  • 连续可微:各个偏导函数皆连续
    • 连续可微则可微
  • 链法则:∂f(g1,⋯ ,gm)∂xk∣P=P0=∑i=1m∂f∂ui(Q0)∂gi∂xk(P0)\frac{\partial f(g_1,\cdots,g_m)}{\partial x_k}|_{P=P_0}=\sum_{i=1}^m\frac{\partial f}{\partial u_i}(Q_0)\frac{\partial g_i}{\partial x_k}(P_0)
  • 隐函数求导法
    • F(x1,⋯ ,xn+1)=CF(x_1,\cdots,x_{n+1})=C
    • 由上式决定的隐函数:xn+1=f(x1,⋯ ,xn)x_{n+1}=f(x_1,\cdots,x_n)
    • ∂xn+1∂xi(a1,⋯ ,an+1)=−∂F∂xn+1(a1,⋯ ,an+1)∂F∂xi(a1,⋯ ,an+1)\frac{\partial x_{n+1}}{\partial x_i}(a_1,\cdots,a_{n+1})=-\frac{\frac{\partial F}{\partial x_{n+1}}(a_1,\cdots,a_{n+1})}{\frac{\partial F}{\partial x_i}(a_1,\cdots,a_{n+1})}
  • 求导换序:∂2f∂xi∂xj,∂2f∂xj∂xi\frac{\partial^2 f}{\partial x_i\partial x_j},\frac{\partial^2 f}{\partial x_j\partial x_i} 在 UU 上存在且在 PP 处连续,则∂2f∂xi∂xj(P)=∂2f∂xj∂xi(P)\frac{\partial^2 f}{\partial x_i\partial x_j}(P)=\frac{\partial^2 f}{\partial x_j\partial x_i}(P)
    • 二阶连续可微可换序
  • Fermat 定理:PP 为 ff 极值点且为 DfD_f 内点,ff 在 pp 处可微,则 df(P)=0df(P)=0, PP 为临界点
  • Hesse 阵
    • 二阶连续可微函数
      • ∀k,H(f)(P)\forall k,H(f)(P) 的 kk 阶顺序主子式为正,则 PP 为极小值点
      • ∀k,H(f)(P)\forall k,H(f)(P) 的 kk 阶顺序主子式皆与 (−1)k(-1)^k 同号,则 PP 为 ff 极大值点
      • 鞍点:df(P)=0,∣H(f)(P)∣≠0df(P)=0,|H(f)(P)|\not=0 且不满足上两条,则 PP 非极值点
H(f)(P)=(∂2f∂xi∂xj(P))n×n=[∂2f∂x12∂2f∂x1∂x2⋯∂2f∂x2∂x1⋱⋮⋮⋯∂2f∂xn2]H(f)(P)=(\frac{\partial^2 f}{\partial x_i\partial x_j}(P))_{n\times n}=\begin{bmatrix} \frac{\partial^2 f}{\partial x_1^2} & \frac{\partial^2 f}{\partial x_1\partial x_2} & \cdots \newline \frac{\partial^2 f}{\partial x_2\partial x_1} & \ddots & \vdots \newline \vdots & \cdots & \frac{\partial^2 f}{\partial x_n^2} \end{bmatrix}
  • ff 在 P0P_0 处可微:f:E→Rm,E⊆Rn,∃δ>0,U(P0;δ)⊆E,∃Am×n,∀ΔP∈Rn,∥ΔP∥<δf:E\rightarrow\mathbb{R}^m,E\subseteq\mathbb{R}^n,\exists\delta>0,U(P_0;\delta)\subseteq E,\exists A_{m\times n},\forall\Delta P\in\mathbb{R}^n,\lVert\Delta P\rVert<\delta 有 f(P0+ΔP)−f(P0)=A⋅ΔP+R(P0+ΔP)f(P_0+\Delta P)-f(P_0)=A\cdot\Delta P+R(P_0+\Delta P) 且 ΔP→0,R(P0+ΔP)=o(∥ΔP∥)\Delta P\rightarrow 0,R(P_0+\Delta P)=o(\lVert\Delta P\rVert)
  • 映射可微   ⟺  ∀i,fi\iff\forall i,f_i 可微
  • Jacobi 矩阵:导数推广
Df(P0)=[∂f1∂x1(P0)∂f1∂x2(P0)⋯∂f1∂xn(P0)∂f2∂x1(P0)⋯⋯⋮⋯⋯⋯⋮∂fm∂x1(P0)⋯⋯∂fm∂xn(P0)]Df(P_0) = \begin{bmatrix} \frac{\partial f_1}{\partial x_1}(P_0) & \frac{\partial f_1}{\partial x_2}(P_0) & \cdots & \frac{\partial f_1}{\partial x_n}(P_0) \newline \frac{\partial f_2}{\partial x_1}(P_0) & \cdots & \cdots & \vdots\newline \cdots & \cdots & \cdots & \vdots\newline \frac{\partial f_m}{\partial x_1}(P_0) & \cdots & \cdots & \frac{\partial f_m}{\partial x_n}(P_0) \newline \end{bmatrix}
  • 微分:A:Rn→Rm,A(X)=Df(P0)⋅X\mathbf{A}:\mathbb{R}^n\rightarrow\mathbb{R}^m,\mathbf{A}(X)=Df(P_0)\cdot X
    • Δf(P0;Δ)=Df(P0)⋅ΔP+o(∥ΔP∥)\Delta f(P_0;\Delta)=Df(P_0)\cdot\Delta P+o(\lVert\Delta P\rVert)
    • 链法则:D(f∘g)(P0)=Df(Q0)⋅Dg(P0)D(f\circ g)(P_0)=Df(Q_0)\cdot Dg(P_0)
  • 方向导数:nn 元函数 ff 在 PP 处沿 vv 的方向导数 dvf(P)=Df(P)⋅v=⟨∇f(P),v⟩d_vf(P)=Df(P)\cdot v=\langle \nabla f(P),v\rangle
    • 梯度:∇f(P)=Df(P)T\nabla f(P)=Df(P)^T