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$$ $$
\smalltext{The role of $x_1,x_2$ can be swapped, if $f$ is continuous.} \smalltext{The role of $x_1,x_2$ can be swapped, if $f$ is continuous.}
\end{subbox} \end{subbox}
\newpage \newpage
\definition \textbf{Parametrized $m$-Set in $\R^n$}\\
$f: [a_1,b_1]\times\cdots\times[a_m,b_m] \to \R$\\
s.t. $f \in C^1$ on $(a_1,b_1)\times\cdots\times(a_m,b_m)$\\
\subtext{A param. $1$-set in $\R^n$ is just a param. curve}
\definition \textbf{Negligible Subset}\\
$B \subset \R^n$ s.t. $\exists k \geq 0$ param. $m_i$-sets: $f_i:X_i\to\R^n$ s.t.
$$
B \subset f_1(X_1) \cup \cdots \cup f_k(X_k)
$$
\subtext{$1 \leq i \leq k,\quad m_i < n$}\\
\begin{footnotesize}
\remark For an affine subspace $H \subset \R^n$ with $\dim(H) < n$, any $X \subset \R^n$ contained in $H$ is Negligible
\remark The image of a param. curve $\gamma: [a,b] \to \R^n$ is negligible.\\
\color{gray} $\gamma$ is a $1$-set in $\R^n$ \color{black}
\end{footnotesize}
\lemma \textbf{Integral of Negligible Sets}\\
\smalltext{For continuous $f: X \subset \R^n \to \R$}:
$$
X \text{ negligible } \implies \int_X f(x)\ dx = 0
$$
\subsection{Improper Integrals}
\smalltext{$I \subset \R$ bounded,$\quad J = [a,+\infty]$ for $a \in \R,\quad f$ cont. on $X = J \times I$}
$$
\underset{x \to \infty}{\lim}\int_{[a,x]\times I}f(x,y)\ dxdy = \underbrace{\int_a^\infty \Biggl( \int_I f(x,y)\ dy \Biggr) dx}_\text{Order of Integration may change}
$$
If this Limit is equal for both orders of Integration:
\definition \textbf{Improper Integral in $\R^2$}
$$
\int_{J \times I} f(x,y)\ dxdy := \underset{x \to \infty}{\lim}\int_{[a,x]\times I}f(x,y)\ dxdy
$$
\definition \textbf{Integral over $\R^2$}
$$
\int_{\R^2} f(x,y)\ dxdy := \underset{R \to \infty}{\lim}\int_{[-R,R]^2} f(x,y)\ dxdy
$$
\begin{footnotesize}
\remark if $|f| \leq g$, and an impr. Integr. exists on g, it exists on $f$.
\end{footnotesize}
\newpage
\subsection{Change of Variable}
\smalltext{This is to provide an Analogue of the Change of Variable in $\R$}
$$
\int f\Bigl( g(x) \Bigr) g'(x)\ dx = \int f(y)\ dy
$$
\textbf{Prerequisites}
\begin{footnotesize}
$\bar{X},\bar{Y} \subset \R^n$ compact, $\varphi: \bar{X} \to \bar{Y}$ cont.\\
We have: $\bar{X} = X \cup B,\quad \bar{Y} = Y \cup C$ s.t.
\begin{enumerate}
\item $X,Y$ are open
\item $B,C$ are negligible
\item $\varphi$ on $X$ is a $C^1$ map $\varphi: X \to Y$
\end{enumerate}
\end{footnotesize}
\begin{subbox}{Change of Variable in $\R^n$}
\smalltext{$\bar{X},\bar{Y}$ as above, $\quad f$ cont. on $\bar{Y}$ arbitrary}
$$
\int_{\bar{X}} f\Bigr( \varphi(x) \Bigl) \cdot \left\vert \det(\textbf{J}_\varphi(x)) \right\vert\ dx = \int_{\bar{Y}} f(y)\ dy
$$
\end{subbox}
\begin{footnotesize}
\remark Translations: $\varphi(x) = x + x_0$ have $\textbf{J}_\varphi(x) = \textbf{I}_n$\\
so the volume is preserved: $\displaystyle\int_{\bar{X}}f(x+x_0)\ dx = \int_{x_0 + \bar{X}} f(x)\ dx$
\remark Linear maps: $\varphi(x) = \textbf{A}x$ have $\textbf{J}_\varphi(x) = \textbf{A}$\\
The change of variable is: $\displaystyle\int_{\bar{X}} f\Bigl( \varphi(x) \Bigr)\ dx = \frac{1}{\left\vert \det(\textbf{A}) \right\vert} \int_{\bar{Y}}f(y)\ dy$
\end{footnotesize}
\remark \textbf{Commonly used Changes}
\begin{enumerate}
\item Polar Coordinates\\
\smalltext{
$\varphi(r, \theta) = \bigl(r\cos(\theta),\ r\sin(\theta)\bigr)$\\
Where $dxdy = r\ dr\ d\theta$
}
\item Cylindrical Coordinates\\
\smalltext{
$\varphi(r, \theta, z) = \bigl( r\cos(\theta),\ rsin(\theta),\ z \bigr)$\\
Where $dxdydz = r\ dr\ d\theta\ dz$
}
\item Spherical Coordinates\\
\smalltext{
$\varphi(r, \theta, \phi) = (r\sin(\phi)\cos(\theta),\ r\sin(\phi)\sin(\theta),\ r\cos(\phi))$\\
Where $dxdydz = r^2\ \sin(\phi)\ dr\ d\theta\ d\phi$
}
\end{enumerate}
\newpage
\subsection{Green's Theorem}
\smalltext{An analogue of the Fundamental Theorem of Calculus in $\R^2$.}
\definition \textbf{Simple Closed Parametrized Curve}\\
$\gamma: [a,b] \to \R^2$ closed param. curve s.t.
\begin{enumerate}
\item $\gamma(t) \neq \gamma(s)\quad$ unless $s = t$, or $\{s,t\} = \{a,b\}$
\item $\gamma'(t) \neq 0\quad \forall a < t < b$
\end{enumerate}
\subtext{Example: $\varphi(t) = \Bigl( x_0 + r\cos(t),\ y_0 + r\sin(t) \Bigr)$\\
(A circle, traversed \textit{once}, i.e. for $0 \leq t \leq 2\pi$)}
\begin{subbox}{Green's Theorem}
\smalltext{$X \subset \R^2 \text{ compact with Boundary } \partial X = \displaystyle\underset{1 \leq i \leq n}{\bigcup} \gamma_i$ as above}\\
\smalltext{Assume: $\gamma_i: [a_i,b_i] \to \R^2$ s.t. $X$ is always \textit{left} of $\gamma_i'(t)$ at $\gamma_i(t)$}
$$
\int_X \Biggl( \frac{\partial f_2}{\partial x} - \frac{\partial f_1}{\partial y} \Biggr)\ dxdy = \sum_{i=1}^{k} \int_{\gamma_i} f \cdot ds
$$
\smalltext{For a $C^1$ Vector field $f=(f_1,f_2)$ containing $X$}
\end{subbox}
\subtext{So, some Riemann Integrals can be converted to a sum of line integrals.}
\lemma \textbf{Volume using Green}
$$
\text{Vol}(X) = \sum_{i=1}^{k} \int_{\gamma_i} x \cdot ds = \sum_{i=1}^{k} \int_{a_i}^{b_i} \gamma_{i,1}(t)\cdot \gamma_{i,2}'(t)\ dt
$$
\subtext{Same assumptions as above.}
\remark The \textit{Gauss-Ostrogradski} Formula exists for $\R^3$.