$$ %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% % Self-defined math definitions %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% % Math symbol commands \newcommand{\intd}{\,{\rm d}} % Symbol 'd' used in integration, such as 'dx' \newcommand{\diff}{{\rm d}} % Symbol 'd' used in differentiation \newcommand{\Diff}{{\rm D}} % Symbol 'D' used in differentiation \newcommand{\pdiff}{\partial} % Partial derivative \newcommand{DD}[2]{\frac{\diff}{\diff #2}\left( #1 \right)} \newcommand{Dd}[2]{\frac{\diff #1}{\diff #2}} \newcommand{PD}[2]{\frac{\pdiff}{\pdiff #2}\left( #1 \right)} \newcommand{Pd}[2]{\frac{\pdiff #1}{\pdiff #2}} \newcommand{\rme}{{\rm e}} % Exponential e \newcommand{\rmi}{{\rm i}} % Imaginary unit i \newcommand{\rmj}{{\rm j}} % Imaginary unit j \newcommand{\vect}[1]{\boldsymbol{#1}} % Vector typeset in bold and italic \newcommand{\phs}[1]{\dot{#1}} % Scalar phasor \newcommand{\phsvect}[1]{\boldsymbol{\dot{#1}}} % Vector phasor \newcommand{\normvect}{\vect{n}} % Normal vector: n \newcommand{\dform}[1]{\overset{\rightharpoonup}{\boldsymbol{#1}}} % Vector for differential form \newcommand{\cochain}[1]{\overset{\rightharpoonup}{#1}} % Vector for cochain \newcommand{\bigabs}[1]{\bigg\lvert#1\bigg\rvert} % Absolute value (single big vertical bar) \newcommand{\Abs}[1]{\big\lvert#1\big\rvert} % Absolute value (single big vertical bar) \newcommand{\abs}[1]{\lvert#1\rvert} % Absolute value (single vertical bar) \newcommand{\bignorm}[1]{\bigg\lVert#1\bigg\rVert} % Norm (double big vertical bar) \newcommand{\Norm}[1]{\big\lVert#1\big\rVert} % Norm (double big vertical bar) \newcommand{\norm}[1]{\lVert#1\rVert} % Norm (double vertical bar) \newcommand{\ouset}[3]{\overset{#3}{\underset{#2}{#1}}} % over and under set % Super/subscript for column index of a matrix, which is used in tensor analysis. \newcommand{\cscript}[1]{\;\; #1} % Star symbol used as prefix in front of a paragraph with no indent \newcommand{\prefstar}{\noindent$\ast$ } % Big vertical line restricting the function. % Example: $u(x)\restrict_{\Omega_0}$ \newcommand{\restrict}{\big\vert} % Math operators which are typeset in Roman font \DeclareMathOperator{\sgn}{sgn} % Sign function \DeclareMathOperator{\erf}{erf} % Error function \DeclareMathOperator{\Bd}{Bd} % Boundary of a set, used in topology \DeclareMathOperator{\Int}{Int} % Interior of a set, used in topology \DeclareMathOperator{\rank}{rank} % Rank of a matrix \DeclareMathOperator{\divergence}{div} % Curl \DeclareMathOperator{\curl}{curl} % Curl \DeclareMathOperator{\grad}{grad} % Gradient \DeclareMathOperator{\tr}{tr} % Trace \DeclareMathOperator{\span}{span} % Span $$

止于至善

As regards numerical analysis and mathematical electromagnetism

James Munkres Topology: Sec 18 Exer 12

Theorem 18.4 in James Munkres “Topology” states that if a function \(f : A \rightarrow X \times Y\) is continuous, its coordinate functions \(f_1 : A \rightarrow X\) and \(f_2 : A \rightarrow Y\) are also continuous, and the converse is also true. This is what we have been familiar with, such as a continuous parametric curve \(f: [0, 1] \rightarrow \mathbb{R}^3\) defined as \(f(t) = (x(t), y(t), z(t))^T\) with its three components being continuous. However, if a function \(g: A \times B \rightarrow X\) is separately continuous in each of its components, i.e. both \(g_1: A \rightarrow X\) and \(g_2 : B \rightarrow X\) are continuous, \(g\) is not necessarily continuous.

Here, the said “separately continuous in each of its components” means arbitrarily selecting the value of one component variable from its domain and fix it, then the original function depending only on the other component is continuous. In the above, the function \(g\) can be envisaged as a curved surface in 3D space. With \(g_1\) being continuous, the intersection profiles between this curved surface and those planes perpendicular to the coordinate axis for \(B\) are continuous. Similarly, because \(g_2\) is continuous, the intersection profiles obtained from those planes perpendicular to the coordinate axis for \(A\) are also continuous. The continuity of intersection curves is only ensured in these two special directions, so it is not guaranteed that the original function \(g\) is continuous.

In Exercise 12 of Section 18, an example is given as
\[
F(x \times y) = \begin{cases}
\frac{xy}{x^2 + y^2} & (x \neq 0, y \neq 0) \\
0 & (x = 0, y = 0)
\end{cases},
\]
where \(F\) is continuous separately in each of its component variables but is not continuous by itself. This is function is visualized below.

Fix \(y\) at \(y_0\), we have \(F_{y_0}(x) = F(x \times y_0)\). When \(y_0 \neq 0\), \(F_{y_0}(x)\) is continuous with respect to \(x\) because it is only a composition of continuous real valued functions via simple arithmetic. When \(y_0 = 0\), if \(x \neq 0\), \(F_0(x) = 0\); if \(x =0\), \(F_0(x)\) is also 0 due to the definition of \(F(x \times y)\). Therefore, \(F_0(x)\) is a constant function, which is continuous due to Theorem 18.2 (a). Similarly, \(F_{x_0}(y)\) is also continuous with respect to \(y\).

However, if we let \(x = y\) and approach \((x, y) = (x, x)\) to \((0, 0)\), it can be seen that \(F(x \times x)\) is not continuous, because

  • when \(x \neq 0\), \(F(x \times x) = \frac{x^2}{x^2 + x^2} = \frac{1}{2}\);
  • when \(x = 0\), \(F(x \times x) = 0\).

If we let \(x = -y\) and approach \((x ,y) = (x, -x)\) to \((0, 0)\), \(F = -\frac{1}{2}\) when \(x \neq 0\) and \(F = 0\) when \(x = 0\).

Then, if we select an open set such as \((-\frac{1}{4}, \frac{1}{4})\) around the function value \(0\) in \(\mathbb{R}\), its pre-image \(U\) in \(\mathbb{R} \times \mathbb{R}\) should include the point \((0, 0)\) and exclude the rays \((x, x)\) and \((x, -x)\) with \(x \in \mathbb{R}\) and \(x \neq 0\). Due to these excluded rays, there is no neighborhood of \((0, 0)\) in \(\mathbb{R} \times \mathbb{R}\) that is contained completely in \(U\). Therefore, \(U\) is not an open set and \(F(x \times y)\) is not continuous.

From the above analysis, some lessons can be learned.

  1. Pure analysis can be made and general conclusions can be obtained before entering into the real world with a solid example.
  2. A tangible counter example is a sound proof for negation of a proposition. Just one is enough!

 

posted @ 2018-12-18 21:35  皮波迪博士  阅读(269)  评论(0编辑  收藏  举报