[Analysis] More examples

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RobinB27
2026-02-03 18:45:18 +01:00
parent 8a12d3a196
commit 6de43e098b
3 changed files with 39 additions and 10 deletions

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@@ -291,6 +291,19 @@ $$
& T_2f(y;x_0) = f(x_0) + \nabla f(x_0) \cdot y + \frac{1}{2} \Bigl( y^\top \cdot \textbf{H}_f(x_0) \cdot y\Bigr) & T_2f(y;x_0) = f(x_0) + \nabla f(x_0) \cdot y + \frac{1}{2} \Bigl( y^\top \cdot \textbf{H}_f(x_0) \cdot y\Bigr)
\end{align*} \end{align*}
\begin{footnotesize}
\textbf{Example:} Approximate $f(x,y) = x\sqrt{y}$ at $f(1.1, 4.4)$ using $(1, 4)$.
\begin{align*}
T_1f(y;(1, 4)) &= f(1,4) + \nabla f(1, 4) \cdot (y_1-1, y_2-4) \\
&= 2 + \begin{bmatrix}
2 \\
\frac{1}{4}
\end{bmatrix} \cdot (y_1-1, y_2-4) \\
&= 2 + 2(y_1-1) + \frac{1}{4}(y_2-4)
\end{align*}
Thus $T_1f\bigl((1.1, 4.4); (1, 4)\bigr) = 2 + 2(1.1-1) + \frac{1}{4}(4.4-4) = 2.3$
\end{footnotesize}
\method Calculating $T_kf(y;x_0)$ also yields $\textbf{H}_f$ for $k \geq 2$. \method Calculating $T_kf(y;x_0)$ also yields $\textbf{H}_f$ for $k \geq 2$.
\begin{align*} \begin{align*}
& T_2f((x_0,y_0);(x,y)) = \ldots + ax^2 + by^2 + cxy \\ & T_2f((x_0,y_0);(x,y)) = \ldots + ax^2 + by^2 + cxy \\

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@@ -217,12 +217,6 @@ $$
\newpage \newpage
\subsection{Change of Variable} \subsection{Change of Variable}
\smalltext{This is to provide an Analogue of the Change of Variable in $\R$}
$$
\int f\Bigl( g(x) \Bigr) g'(x)\ dx = \int f(y)\ dy
$$
\textbf{Prerequisites}
\begin{footnotesize} \begin{footnotesize}
$\bar{X},\bar{Y} \subset \R^n$ compact, $\varphi: \bar{X} \to \bar{Y}$ cont.\\ $\bar{X},\bar{Y} \subset \R^n$ compact, $\varphi: \bar{X} \to \bar{Y}$ cont.\\
@@ -259,7 +253,7 @@ $$
\item Cylindrical Coordinates\\ \item Cylindrical Coordinates\\
\smalltext{ \smalltext{
$\varphi(r, \theta, z) = \bigl( r\cos(\theta),\ rsin(\theta),\ z \bigr) \quad \color{gray} \theta \in [0, \pi), \phi \in [0, 2\pi)$\\ $\varphi(r, \theta, z) = \bigl( r\cos(\theta),\ r\sin(\theta),\ z \bigr) \quad \color{gray} \theta \in [0, \pi), \phi \in [0, 2\pi)$\\
$dxdydz = r\ dr\ d\theta\ dz$ $dxdydz = r\ dr\ d\theta\ dz$
} }
@@ -269,11 +263,33 @@ $$
$dxdydz = r^2\ \sin(\phi)\ dr\ d\theta\ d\phi$ $dxdydz = r^2\ \sin(\phi)\ dr\ d\theta\ d\phi$
} }
\end{enumerate} \end{enumerate}
\begin{footnotesize}
Corresponding Jacobians:
$$
\textbf{J}_1 = \begin{bmatrix}
\cos(\theta) & -r\sin(\theta) \\
\sin(\theta) & r\cos(\theta) \\
\end{bmatrix}
\qquad
\textbf{J}_2 = \begin{bmatrix}
\cos(\theta) & -r\sin(\theta) & 0 \\
\sin(\theta) & r\cos(\theta) & 0 \\
0 & 0 & z
\end{bmatrix}
$$
$$
\textbf{J}_3 = \begin{bmatrix}
\cos(\phi)\sin(\theta) & -r\sin(\phi)\sin(\theta) & r\cos(\phi)\cos(\theta) \\
\sin(\phi)\sin(\theta) & r\cos(\phi)\sin(\theta) & r\sin(\phi)\cos(\theta) \\
\cos(\theta) & 0 & -r\sin(\theta)
\end{bmatrix}
$$
\end{footnotesize}
% https://en.wikipedia.org/wiki/Spherical_coordinate_system#/media/File:3D_Spherical.svg % https://en.wikipedia.org/wiki/Spherical_coordinate_system#/media/File:3D_Spherical.svg
\begin{center} % \begin{center}
\includegraphics[width=0.3\linewidth]{res/spherical-coords.png} % \includegraphics[width=0.3\linewidth]{res/spherical-coords.png}
\end{center} % \end{center}
\newpage \newpage
\subsection{Green's Theorem} \subsection{Green's Theorem}