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[Analysis] More examples
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@@ -291,6 +291,19 @@ $$
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& 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)
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& 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)
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\end{align*}
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\end{align*}
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\begin{footnotesize}
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\textbf{Example:} Approximate $f(x,y) = x\sqrt{y}$ at $f(1.1, 4.4)$ using $(1, 4)$.
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\begin{align*}
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T_1f(y;(1, 4)) &= f(1,4) + \nabla f(1, 4) \cdot (y_1-1, y_2-4) \\
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&= 2 + \begin{bmatrix}
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2 \\
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\frac{1}{4}
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\end{bmatrix} \cdot (y_1-1, y_2-4) \\
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&= 2 + 2(y_1-1) + \frac{1}{4}(y_2-4)
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\end{align*}
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Thus $T_1f\bigl((1.1, 4.4); (1, 4)\bigr) = 2 + 2(1.1-1) + \frac{1}{4}(4.4-4) = 2.3$
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\end{footnotesize}
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\method Calculating $T_kf(y;x_0)$ also yields $\textbf{H}_f$ for $k \geq 2$.
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\method Calculating $T_kf(y;x_0)$ also yields $\textbf{H}_f$ for $k \geq 2$.
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\begin{align*}
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\begin{align*}
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& T_2f((x_0,y_0);(x,y)) = \ldots + ax^2 + by^2 + cxy \\
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& T_2f((x_0,y_0);(x,y)) = \ldots + ax^2 + by^2 + cxy \\
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@@ -217,12 +217,6 @@ $$
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\newpage
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\newpage
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\subsection{Change of Variable}
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\subsection{Change of Variable}
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\smalltext{This is to provide an Analogue of the Change of Variable in $\R$}
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$$
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\int f\Bigl( g(x) \Bigr) g'(x)\ dx = \int f(y)\ dy
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$$
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\textbf{Prerequisites}
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\begin{footnotesize}
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\begin{footnotesize}
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$\bar{X},\bar{Y} \subset \R^n$ compact, $\varphi: \bar{X} \to \bar{Y}$ cont.\\
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$\bar{X},\bar{Y} \subset \R^n$ compact, $\varphi: \bar{X} \to \bar{Y}$ cont.\\
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@@ -259,7 +253,7 @@ $$
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\item Cylindrical Coordinates\\
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\item Cylindrical Coordinates\\
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\smalltext{
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\smalltext{
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$\varphi(r, \theta, z) = \bigl( r\cos(\theta),\ rsin(\theta),\ z \bigr) \quad \color{gray} \theta \in [0, \pi), \phi \in [0, 2\pi)$\\
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$\varphi(r, \theta, z) = \bigl( r\cos(\theta),\ r\sin(\theta),\ z \bigr) \quad \color{gray} \theta \in [0, \pi), \phi \in [0, 2\pi)$\\
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$dxdydz = r\ dr\ d\theta\ dz$
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$dxdydz = r\ dr\ d\theta\ dz$
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}
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}
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@@ -269,11 +263,33 @@ $$
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$dxdydz = r^2\ \sin(\phi)\ dr\ d\theta\ d\phi$
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$dxdydz = r^2\ \sin(\phi)\ dr\ d\theta\ d\phi$
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}
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}
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\end{enumerate}
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\end{enumerate}
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\begin{footnotesize}
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Corresponding Jacobians:
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$$
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\textbf{J}_1 = \begin{bmatrix}
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\cos(\theta) & -r\sin(\theta) \\
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\sin(\theta) & r\cos(\theta) \\
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\end{bmatrix}
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\qquad
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\textbf{J}_2 = \begin{bmatrix}
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\cos(\theta) & -r\sin(\theta) & 0 \\
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\sin(\theta) & r\cos(\theta) & 0 \\
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0 & 0 & z
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\end{bmatrix}
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$$
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$$
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\textbf{J}_3 = \begin{bmatrix}
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\cos(\phi)\sin(\theta) & -r\sin(\phi)\sin(\theta) & r\cos(\phi)\cos(\theta) \\
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\sin(\phi)\sin(\theta) & r\cos(\phi)\sin(\theta) & r\sin(\phi)\cos(\theta) \\
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\cos(\theta) & 0 & -r\sin(\theta)
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\end{bmatrix}
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$$
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\end{footnotesize}
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% https://en.wikipedia.org/wiki/Spherical_coordinate_system#/media/File:3D_Spherical.svg
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% https://en.wikipedia.org/wiki/Spherical_coordinate_system#/media/File:3D_Spherical.svg
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\begin{center}
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% \begin{center}
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\includegraphics[width=0.3\linewidth]{res/spherical-coords.png}
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% \includegraphics[width=0.3\linewidth]{res/spherical-coords.png}
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\end{center}
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% \end{center}
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\newpage
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\newpage
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\subsection{Green's Theorem}
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\subsection{Green's Theorem}
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