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Move to common headers

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This commit is contained in:
Nathanaël Restori 2015-12-23 20:37:35 +01:00
parent 2f817d6698
commit 7e6f72d9ad
5 changed files with 44 additions and 115 deletions
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31
analyse-I.tex
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@ -1,38 +1,9 @@
\documentclass[a4paper,10pt]{article} \documentclass[a4paper,10pt]{article}
%\documentclass[a4paper,10pt]{scrartcl} %\documentclass[a4paper,10pt]{scrartcl}
\usepackage{xltxtra} \input{common.tex}
\usepackage{pbox}
\usepackage{mathtools}
\usepackage{amssymb}
\usepackage{tabularx}
\usepackage[top=13pt, bottom=12pt, left=13pt, right=12pt]{geometry}
% \setromanfont[Mapping=tex-text]{Linux Libertine O}
% \setsansfont[Mapping=tex-text]{DejaVu Sans}
% \setmonofont[Mapping=tex-text]{DejaVu Sans Mono}
\title{}
\author{}
\date{}
\let\oldcdot\cdot
\let\oldbullet\bullet
\let\oldvec\vec
\let\olddot\dot
\let\oldddot\ddot
% \renewcommand{\cdot}{ }
\renewcommand{\bullet}{\circ}
% \renewcommand{\vec}{\mathbf}
% \renewcommand{\dot}[1]{\frac{\mathrm{d}#1}{\mathrm{d}t}}
% \renewcommand{\ddot}[1]{\frac{\mathrm{d^2}#1}{\mathrm{d}t^2}}
\newcommand{\ccdot}{ }
\setlength{\parindent}{0pt}
\setlength{\parskip}{0pt}
\begin{document} \begin{document}
% \maketitle
\begin{tabularx}{\textwidth}{ |X|X| } \begin{tabularx}{\textwidth}{ |X|X| }
\hline \hline

19
chimie.tex
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@ -1,26 +1,9 @@
\documentclass[a4paper,10pt]{article} \documentclass[a4paper,10pt]{article}
%\documentclass[a4paper,10pt]{scrartcl} %\documentclass[a4paper,10pt]{scrartcl}
\usepackage{xltxtra} \input{common.tex}
\usepackage{pbox}
\usepackage{mathtools}
\usepackage{amssymb}
\usepackage{tabularx}
\usepackage{siunitx}
\usepackage[top=13pt, bottom=12pt, left=13pt, right=12pt]{geometry}
% \setromanfont[Mapping=tex-text]{Linux Libertine O}
% \setsansfont[Mapping=tex-text]{DejaVu Sans}
% \setmonofont[Mapping=tex-text]{DejaVu Sans Mono}
\title{}
\author{}
\date{}
\setlength{\parindent}{0pt}
\setlength{\parskip}{0pt}
\begin{document} \begin{document}
% \maketitle
\begin{tabularx}{\textwidth}{ |X|X| } \begin{tabularx}{\textwidth}{ |X|X| }
\hline \hline

36
common.tex Normal file
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@ -0,0 +1,36 @@
\usepackage{xltxtra}
\usepackage{pbox}
\usepackage{mathtools}
\usepackage{amssymb}
\usepackage{tabularx}
\usepackage{siunitx}
\usepackage{unicode-math}
\usepackage[top=13pt, bottom=12pt, left=13pt, right=12pt]{geometry}
% \setromanfont[Mapping=tex-text]{Linux Libertine O}
% \setsansfont[Mapping=tex-text]{DejaVu Sans}
% \setmonofont[Mapping=tex-text]{DejaVu Sans Mono}
\title{}
\author{}
\date{}
\let\oldcdot\cdot
\let\oldbullet\bullet
\let\oldvec\vec
\let\olddot\dot
\let\oldddot\ddot
% \renewcommand{\cdot}{ }
\renewcommand{\bullet}{\circ}
% \renewcommand{\vec}{\mathbf}
% \renewcommand{\dot}[1]{\frac{\mathrm{d}#1}{\mathrm{d}t}}
% \renewcommand{\ddot}[1]{\frac{\mathrm{d^2}#1}{\mathrm{d}t^2}}
% \renewcommand{\frac}[2]{#1 / #2}
\newcommand{\cdotbis}{ }
\newcommand{\dif}{\mathrm{d}}
\setlength{\parindent}{0pt}
\setlength{\parskip}{0pt}
% \everymath{\displaystyle}

40
physique-I.tex
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@ -1,39 +1,9 @@
\documentclass[a4paper,10pt]{article} \documentclass[a4paper,10pt]{article}
%\documentclass[a4paper,10pt]{scrartcl} %\documentclass[a4paper,10pt]{scrartcl}
\usepackage{xltxtra} \input{common.tex}
\usepackage{pbox}
\usepackage{mathtools}
\usepackage{amssymb}
\usepackage{tabularx}
\usepackage[top=13pt, bottom=12pt, left=13pt, right=12pt]{geometry}
% \setromanfont[Mapping=tex-text]{Linux Libertine O}
% \setsansfont[Mapping=tex-text]{DejaVu Sans}
% \setmonofont[Mapping=tex-text]{DejaVu Sans Mono}
\title{}
\author{}
\date{}
\let\oldcdot\cdot
\let\oldbullet\bullet
\let\oldvec\vec
\let\olddot\dot
\let\oldddot\ddot
% \renewcommand{\cdot}{ }
\renewcommand{\bullet}{\circ}
% \renewcommand{\vec}{\mathbf}
% \renewcommand{\dot}[1]{\frac{\mathrm{d}#1}{\mathrm{d}t}}
% \renewcommand{\ddot}[1]{\frac{\mathrm{d^2}#1}{\mathrm{d}t^2}}
% \renewcommand{\frac}[2]{#1 / #2}
\newcommand{\cdotbis}{ }
\setlength{\parindent}{0pt}
\setlength{\parskip}{0pt}
\begin{document} \begin{document}
% \maketitle
\begin{tabularx}{\textwidth}{ |X|X|X| } \begin{tabularx}{\textwidth}{ |X|X|X| }
\hline \hline
@ -169,10 +139,10 @@
$ \vec{r} = r \cdotbis \vec{e_r}$ \newline $ \vec{r} = r \cdotbis \vec{e_r}$ \newline
$ \vec{v} = \dot{r} \cdotbis \vec{e_r} + r \cdotbis \dot{\theta} \cdotbis \vec{e}_{\theta} + r \cdotbis \dot{\varphi} \cdotbis \sin(\theta) \cdotbis \vec{e}_{\varphi} $ \newline $ \vec{v} = \dot{r} \cdotbis \vec{e_r} + r \cdotbis \dot{\theta} \cdotbis \vec{e}_{\theta} + r \cdotbis \dot{\varphi} \cdotbis \sin(\theta) \cdotbis \vec{e}_{\varphi} $ \newline
$ \vec{a} = \begin{pmatrix} $ \vec{a} = \begin{pmatrix}
\ddot{r} - \dot{r} \cdotbis \dot{\theta}^2 - r \cdotbis \dot{\varphi}^2 \cdotbis \sin^2(\theta) \\ \ddot{r} - \dot{r} \cdotbis \dot{\theta}^2 - r \cdotbis \dot{\varphi}^2 \cdotbis \sin^2(\theta) \\
2 \cdotbis \dot{r} \cdotbis \dot{\theta} + r \cdotbis \ddot{\theta} - r \cdotbis \dot{\varphi}^2 \cdotbis \sin(\theta) \cdotbis \cos(\theta) \\ 2 \cdotbis \dot{r} \cdotbis \dot{\theta} + r \cdotbis \ddot{\theta} - r \cdotbis \dot{\varphi}^2 \cdotbis \sin(\theta) \cdotbis \cos(\theta) \\
2 \cdotbis \dot{r} \cdotbis \dot{\varphi} \cdotbis \sin(\theta) + r \cdotbis \ddot{\varphi} \cdotbis \sin(\theta) + 2 \cdotbis r \cdotbis \dot{\varphi} \cdotbis \dot{\theta} \cdotbis \cos(\theta) \\ 2 \cdotbis \dot{r} \cdotbis \dot{\varphi} \cdotbis \sin(\theta) + r \cdotbis \ddot{\varphi} \cdotbis \sin(\theta) + 2 \cdotbis r \cdotbis \dot{\varphi} \cdotbis \dot{\theta} \cdotbis \cos(\theta) \\
\end{pmatrix} $ \newline \end{pmatrix} $ \newline
$ \frac{\mathrm{d}}{\mathrm{d}t} \cdotbis \vec{e_r} = \dot{\theta} \cdotbis \vec{e}_{\theta} + \dot{\varphi} \cdotbis \sin(\theta) \cdotbis \vec{e}_{\varphi} $ \newline $ \frac{\mathrm{d}}{\mathrm{d}t} \cdotbis \vec{e_r} = \dot{\theta} \cdotbis \vec{e}_{\theta} + \dot{\varphi} \cdotbis \sin(\theta) \cdotbis \vec{e}_{\varphi} $ \newline
$ \frac{\mathrm{d}}{\mathrm{d}t} \cdotbis \vec{e}_{\theta} = -\dot{\theta} \cdotbis \vec{e_r} + \dot{\varphi} \cdotbis \cos(\theta) \cdotbis \vec{e}_{\varphi} $ \newline $ \frac{\mathrm{d}}{\mathrm{d}t} \cdotbis \vec{e}_{\theta} = -\dot{\theta} \cdotbis \vec{e_r} + \dot{\varphi} \cdotbis \cos(\theta) \cdotbis \vec{e}_{\varphi} $ \newline
$ \frac{\mathrm{d}}{\mathrm{d}t} \cdotbis \vec{e}_{\varphi} = -\dot{\varphi} \cdotbis \sin(\theta) \cdotbis \vec{e_r} - \dot{\varphi} \cdotbis \cos(\theta) \cdotbis \vec{e}_{\theta} $ \newline $ \frac{\mathrm{d}}{\mathrm{d}t} \cdotbis \vec{e}_{\varphi} = -\dot{\varphi} \cdotbis \sin(\theta) \cdotbis \vec{e_r} - \dot{\varphi} \cdotbis \cos(\theta) \cdotbis \vec{e}_{\theta} $ \newline

33
physique-II.tex
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@ -1,40 +1,9 @@
\documentclass[a4paper,10pt]{article} \documentclass[a4paper,10pt]{article}
%\documentclass[a4paper,10pt]{scrartcl} %\documentclass[a4paper,10pt]{scrartcl}
\usepackage{xltxtra} \input{common.tex}
\usepackage{pbox}
\usepackage{mathtools}
\usepackage{amssymb}
\usepackage{tabularx}
\usepackage{siunitx}
\usepackage[top=13pt, bottom=12pt, left=13pt, right=12pt]{geometry}
% \setromanfont[Mapping=tex-text]{Linux Libertine O}
% \setsansfont[Mapping=tex-text]{DejaVu Sans}
% \setmonofont[Mapping=tex-text]{DejaVu Sans Mono}
\title{}
\author{}
\date{}
\let\oldcdot\cdot
\let\oldbullet\bullet
\let\oldvec\vec
\let\olddot\dot
\let\oldddot\ddot
% \renewcommand{\cdot}{ }
\renewcommand{\bullet}{\circ}
% \renewcommand{\vec}{\mathbf}
% \renewcommand{\dot}[1]{\frac{\mathrm{d}#1}{\mathrm{d}t}}
% \renewcommand{\ddot}[1]{\frac{\mathrm{d^2}#1}{\mathrm{d}t^2}}
% \renewcommand{\frac}[2]{#1 / #2}
\newcommand{\cdotbis}{ }
\setlength{\parindent}{0pt}
\setlength{\parskip}{0pt}
\begin{document} \begin{document}
% \maketitle
\begin{tabularx}{\textwidth}{ |X|X| } \begin{tabularx}{\textwidth}{ |X|X| }
\hline \hline