diff --git a/semester3/analysis-ii/cheat-sheet-rb/main.pdf b/semester3/analysis-ii/cheat-sheet-rb/main.pdf index a603ef1..3971c00 100644 Binary files a/semester3/analysis-ii/cheat-sheet-rb/main.pdf and b/semester3/analysis-ii/cheat-sheet-rb/main.pdf differ diff --git a/semester3/analysis-ii/cheat-sheet-rb/parts/05_diff.tex b/semester3/analysis-ii/cheat-sheet-rb/parts/05_diff.tex index ef6453b..ba37544 100644 --- a/semester3/analysis-ii/cheat-sheet-rb/parts/05_diff.tex +++ b/semester3/analysis-ii/cheat-sheet-rb/parts/05_diff.tex @@ -63,7 +63,7 @@ $\\ \underset{x \neq x_0 \to x_0}{\lim} \frac{1}{\big\| x - x_0 \big\|}\Biggl( f(x) - f(x_0) - u(x - x_0) \Biggr) = 0 $$ \end{subbox} -\subtext{Similarly, $f$ is differentiable if this holds for all $x \in X$} +\subtext{Applying this directly can be useful for \textit{strange} functions like $|xy|$.} \lemma \textbf{Properties of Differentiable Functions} @@ -163,7 +163,7 @@ $$ $$ \forall x,y:\quad \partial_{x,y}f = \partial_{y,x}f $$ - \smalltext{This generalizes for $\partial_{x_1,\ldots,x_n}f$.} + \smalltext{This generalizes for $\partial_{x_1,\ldots,x_n}f$ if $k \geq n$.} \end{subbox} \remark Linearity of Partial Derivatives @@ -174,7 +174,7 @@ $$ \definition \textbf{Laplace Operator} $$ - \Delta f := \text{div}\bigl( \nabla f(x) \bigr) = \sum_{i=0}^{n} \frac{\partial}{\partial x_i}\Bigl( \frac{\partial f}{\partial x_i} \Bigr) = \sum_{i=0}^{n} \frac{\partial^2f}{\partial x_i^2} + \Delta f := \text{div}\Bigl( \nabla f(x) \Bigr) = \sum_{i=0}^{n} \frac{\partial}{\partial x_i}\biggl( \frac{\partial f}{\partial x_i} \biggr) = \sum_{i=0}^{n} \frac{\partial^2f}{\partial x_i^2} $$ \begin{subbox}{The Hessian} diff --git a/semester3/analysis-ii/cheat-sheet-rb/parts/06_int.tex b/semester3/analysis-ii/cheat-sheet-rb/parts/06_int.tex index b9d51e9..051e8ad 100644 --- a/semester3/analysis-ii/cheat-sheet-rb/parts/06_int.tex +++ b/semester3/analysis-ii/cheat-sheet-rb/parts/06_int.tex @@ -114,7 +114,8 @@ $$ \remark $\text{curl}(f) = 0 \iff \forall 1 \leq i \neq j \leq 3: \displaystyle\frac{\partial f_i}{\partial x_j} = \displaystyle\frac{\partial f_j}{\partial x_i}$ -\remark $\text{curl}(\nabla f) = 0$ if $f: \R^3 \to \R$ is in $C^2$. +\remark $\text{curl}(\nabla f) = 0$ if $f: \R^n \to \R$ is in $C^2$.\\ +\subtext{i.e. if $f$ has a potential.} \method \textbf{Finding the Potential} @@ -248,27 +249,32 @@ $$ 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} +\remark \textbf{Common Changes} \begin{enumerate} \item Polar Coordinates\\ \smalltext{ - $\varphi(r, \theta) = \bigl(r\cos(\theta),\ r\sin(\theta)\bigr)$\\ - Where $dxdy = r\ dr\ d\theta$ + $\varphi(r, \theta) = \bigl(r\cos(\theta),\ r\sin(\theta)\bigr) \quad \color{gray} \theta \in [0, 2\pi) $\\ + $dxdy = r\ dr\ d\theta$ } \item Cylindrical Coordinates\\ \smalltext{ - $\varphi(r, \theta, z) = \bigl( r\cos(\theta),\ rsin(\theta),\ z \bigr)$\\ - Where $dxdydz = r\ dr\ d\theta\ dz$ + $\varphi(r, \theta, z) = \bigl( r\cos(\theta),\ rsin(\theta),\ z \bigr) \quad \color{gray} \theta \in [0, \pi), \phi \in [0, 2\pi)$\\ + $dxdydz = r\ dr\ d\theta\ dz$ } \item Spherical Coordinates\\ \smalltext{ $\varphi(r, \theta, \phi) = (r\sin(\phi)\cos(\theta),\ r\sin(\phi)\sin(\theta),\ r\cos(\phi))$\\ - Where $dxdydz = r^2\ \sin(\phi)\ dr\ d\theta\ d\phi$ + $dxdydz = r^2\ \sin(\phi)\ dr\ d\theta\ d\phi$ } \end{enumerate} +% https://en.wikipedia.org/wiki/Spherical_coordinate_system#/media/File:3D_Spherical.svg +\begin{center} + \includegraphics[width=0.3\linewidth]{res/spherical-coords.png} +\end{center} + \newpage \subsection{Green's Theorem} \smalltext{An analogue of the Fundamental Theorem of Calculus in $\R^2$.} diff --git a/semester3/analysis-ii/cheat-sheet-rb/res/spherical-coords.png b/semester3/analysis-ii/cheat-sheet-rb/res/spherical-coords.png new file mode 100644 index 0000000..8689745 Binary files /dev/null and b/semester3/analysis-ii/cheat-sheet-rb/res/spherical-coords.png differ