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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
%Tutorial slides on Python.
%
% Author: FOSSEE
% Copyright (c) 2009, FOSSEE, IIT Bombay
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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%\usepackage{times}
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\usepackage{amsmath}
% Taken from Fernando's slides.
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\usepackage{mathpazo,courier,euler}
\usepackage[scaled=.95]{helvet}
\definecolor{darkgreen}{rgb}{0,0.5,0}
\usepackage{listings}
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basicstyle=\ttfamily\bfseries,
commentstyle=\color{red}\itshape,
stringstyle=\color{darkgreen},
showstringspaces=false,
keywordstyle=\color{blue}\bfseries}
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\newcommand{\typ}[1]{\lstinline{#1}}
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%%% This is from Fernando's setup.
% \usepackage{color}
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% \usepackage{listings}
% \lstset{
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% stringstyle=\ttfamily\color{orange},
% showstringspaces=false,
% breaklines=true,
% postbreak = \space\dots
% }
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% Title page
\title[Basic Python]{Matrices, Solution of equations and Integration\\}
\author[FOSSEE] {FOSSEE}
\institute[IIT Bombay] {Department of Aerospace Engineering\\IIT Bombay}
\date[] {31, October 2009\\Day 1, Session 4}
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
%\pgfdeclareimage[height=0.75cm]{iitmlogo}{iitmlogo}
%\logo{\pgfuseimage{iitmlogo}}
%% Delete this, if you do not want the table of contents to pop up at
%% the beginning of each subsection:
\AtBeginSubsection[]
{
\begin{frame}<beamer>
\frametitle{Outline}
\tableofcontents[currentsection,currentsubsection]
\end{frame}
}
%%\AtBeginSection[]
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%%\begin{frame}<beamer>
%% \frametitle{Outline}
%% \tableofcontents[currentsection,currentsubsection]
%%\end{frame}
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% the following command:
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%\includeonlyframes{current,current1,current2,current3,current4,current5,current6}
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% DOCUMENT STARTS
\begin{document}
\begin{frame}
\titlepage
\end{frame}
\begin{frame}
\frametitle{Outline}
\tableofcontents
% \pausesections
\end{frame}
\section{Matrices}
\subsection{Initializing}
\begin{frame}[fragile]
\frametitle{Matrices: Initializing}
\begin{lstlisting}
In []: a = matrix([[1,2,3],
[4,5,6],
[7,8,9]])
In []: a
Out[]:
matrix([[1, 2, 3],
[4, 5, 6],
[7, 8, 9]])
\end{lstlisting}
\end{frame}
\subsection{Basic Operations}
\begin{frame}[fragile]
\frametitle{Inverse of a Matrix}
\begin{small}
\begin{lstlisting}
In []: linalg.inv(a)
Out[]:
matrix([[ 3.15221191e+15, -6.30442381e+15, 3.15221191e+15],
[ -6.30442381e+15, 1.26088476e+16, -6.30442381e+15],
[ 3.15221191e+15, -6.30442381e+15, 3.15221191e+15]])
\end{lstlisting}
\end{small}
\end{frame}
\begin{frame}[fragile]
\frametitle{Determinant}
\begin{lstlisting}
In []: linalg.det(a)
Out[]: -9.5171266700777579e-16
\end{lstlisting}
\end{frame}
\begin{frame}[fragile]
\frametitle{Computing Norms}
\begin{lstlisting}
In []: linalg.norm(a)
Out[]: 16.881943016134134
\end{lstlisting}
\end{frame}
\begin{frame}[fragile]
\frametitle{Eigen Values and Eigen Matrix}
\begin{small}
\begin{lstlisting}
In []: linalg.eigvals(a)
Out[]: array([ 1.61168440e+01, -1.11684397e+00, -1.22196337e-15])
In []: linalg.eig(a)
Out[]:
(array([ 1.61168440e+01, -1.11684397e+00, -1.22196337e-15]),
matrix([[-0.23197069, -0.78583024, 0.40824829],
[-0.52532209, -0.08675134, -0.81649658],
[-0.8186735 , 0.61232756, 0.40824829]]))
\end{lstlisting}
\end{small}
\end{frame}
\section{Solving linear equations}
\begin{frame}[fragile]
\frametitle{Solution of equations}
Example problem: Consider the set of equations
\vspace{-0.1in}
\begin{align*}
3x + 2y - z & = 1 \\
2x - 2y + 4z & = -2 \\
-x + \frac{1}{2}y -z & = 0
\end{align*}
\vspace{-0.08in}
To Solve this,
\begin{lstlisting}
In []: A = array([[3,2,-1],[2,-2,4],[-1, 0.5, -1]])
In []: b = array([1, -2, 0])
In []: x = linalg.solve(A, b)
In []: Ax = dot(A, x)
In []: allclose(Ax, b)
Out[]: True
\end{lstlisting}
\end{frame}
\section{Integration}
\subsection{ODEs}
\begin{frame}[fragile]
\frametitle{ODE Integration}
We shall use the simple ODE of a simple pendulum.
\begin{equation*}
\ddot{\theta} = -\frac{g}{L}sin(\theta)
\end{equation*}
\begin{itemize}
\item This equation can be written as a system of two first order ODEs
\end{itemize}
\begin{align}
\dot{\theta} &= \omega \\
\dot{\omega} &= -\frac{g}{L}sin(\theta) \\
\text{At}\ t &= 0 : \nonumber \\
\theta = \theta_0\quad & \&\quad \omega = 0 \nonumber
\end{align}
\end{frame}
\begin{frame}[fragile]
\frametitle{Solving ODEs using SciPy}
\begin{itemize}
\item We use the \typ{odeint} function from scipy to do the integration
\item Define a function as below
\end{itemize}
\begin{lstlisting}
In []: def pend_int(unknown, t, p):
.... theta, omega = unknown
.... g, L = p
.... f=[omega, -(g/L)*sin(theta)]
.... return f
....
\end{lstlisting}
\end{frame}
\begin{frame}[fragile]
\frametitle{Solving ODEs using SciPy \ldots}
\begin{itemize}
\item \typ{t} is the time variable \\
\item \typ{p} has the constants \\
\item \typ{initial} has the initial values
\end{itemize}
\begin{lstlisting}
In []: t = linspace(0, 10, 101)
In []: p=(-9.81, 0.2)
In []: initial = [10*2*pi/360, 0]
\end{lstlisting}
\end{frame}
\begin{frame}[fragile]
\frametitle{Solving ODEs using SciPy \ldots}
\small{\typ{In []: from scipy.integrate import odeint}}
\begin{lstlisting}
In []: pend_sol = odeint(pend_int,
initial,t,
args=(p,))
\end{lstlisting}
\end{frame}
\subsection{Quadrature}
\begin{frame}[fragile]
\frametitle{Quadrature}
Calculate the area under $(sin(x) + x^2)$ in the range $(0,1)$
\small{\typ{In []: from scipy.integrate import quad}}
\begin{lstlisting}
In []: f(x):
return sin(x)+x**2
In []: integrate.quad(f, 0, 1)
\end{lstlisting}
\end{frame}
\end{document}
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