Commit acab3cfa authored by Claude Meny's avatar Claude Meny

Update textbook.fr.md

parent f94ab1de
Pipeline #13993 canceled with stage
...@@ -511,7 +511,7 @@ $`\overrightarrow{e_{\theta}}=-\sin\theta\;\overrightarrow{e_x}+\cos\theta\;\ove ...@@ -511,7 +511,7 @@ $`\overrightarrow{e_{\theta}}=-\sin\theta\;\overrightarrow{e_x}+\cos\theta\;\ove
------------------------ ------------------------
$`\begin{align} $`\begin{align}
\mathbf{\dfrac{d\overrightarrow{e_{\rho}}}{dt}}&=\dfrac{d}{dt}\bigg(\cos\theta\;\overrightarrow{e_x}+\sin\theta\;\overrightarrow{e_z}\bigg)\\ \dfrac{d\overrightarrow{e_{\rho}}}{dt}&=\dfrac{d}{dt}\bigg(\cos\theta\;\overrightarrow{e_x}+\sin\theta\;\overrightarrow{e_z}\bigg)\\
\\ \\
&=\bigg[\dfrac{d\cos\theta}{dt}\;\overrightarrow{e_x} + \sin\theta\;\underbrace{\dfrac{d\overrightarrow{e_z}}{dt}}_{=\,\vec{0}}\bigg]\\ &=\bigg[\dfrac{d\cos\theta}{dt}\;\overrightarrow{e_x} + \sin\theta\;\underbrace{\dfrac{d\overrightarrow{e_z}}{dt}}_{=\,\vec{0}}\bigg]\\
&\quad\quad+\bigg[\dfrac{d(-\sin\theta)}{dt}\;\overrightarrow{e_z}+\cos\theta\;\underbrace{\dfrac{d\overrightarrow{e_z}}{dt}}_{=\,\vec{0}}\bigg]\\ &\quad\quad+\bigg[\dfrac{d(-\sin\theta)}{dt}\;\overrightarrow{e_z}+\cos\theta\;\underbrace{\dfrac{d\overrightarrow{e_z}}{dt}}_{=\,\vec{0}}\bigg]\\
...@@ -521,15 +521,15 @@ $`\begin{align} ...@@ -521,15 +521,15 @@ $`\begin{align}
\\ \\
&=\omega\;\big(-\sin\theta\;\overrightarrow{e_x}+\cos\theta\;\overrightarrow{e_z}\big)\\ &=\omega\;\big(-\sin\theta\;\overrightarrow{e_x}+\cos\theta\;\overrightarrow{e_z}\big)\\
\\ \\
&\mathbf{=\omega\;\overrightarrow{e_{\theta}}} &=\omega\;\overrightarrow{e_{\theta}}
\end{align}`$ \end{align}`$
-------------- --------------
$`\begin{align} $`\begin{align}
\mathbf{\dfrac{d\overrightarrow{e_{\theta}}}{dt}}&=\dfrac{d}{dt}\big(-\sin\theta\;\overrightarrow{e_x}+\cos\theta\;\overrightarrow{e_z}\big)\\ \dfrac{d\overrightarrow{e_{\theta}}}{dt}&=\dfrac{d}{dt}\big(-\sin\theta\;\overrightarrow{e_x}+\cos\theta\;\overrightarrow{e_z}\big)\\
\\ \\
&=\\bigg[\dfrac{d(-\sin\theta)}{dt}\;\overrightarrow{e_x} - \sin\theta\;\underbrace{\dfrac{d\overrightarrow{e_z}}{dt}}_{=\,\vec{0}}\\bigg]\\ &=\\bigg[\dfrac{d(-\sin\theta)}{dt}\;\overrightarrow{e_x} - \sin\theta\;\underbrace{\dfrac{d\overrightarrow{e_z}}{dt}}_{=\,\vec{0}}\bigg]\\
&\quad\quad+\bigg[\dfrac{d\cos\theta}{dt}\;\overrightarrow{e_z}+\cos\theta\;\underbrace{\dfrac{d\overrightarrow{e_z}}{dt}}_{=\,\vec{0}}\bigg]\\ &\quad\quad+\bigg[\dfrac{d\cos\theta}{dt}\;\overrightarrow{e_z}+\cos\theta\;\underbrace{\dfrac{d\overrightarrow{e_z}}{dt}}_{=\,\vec{0}}\bigg]\\
\\ \\
&=\dfrac{d(-\sin\theta)}{d\theta}\;\underbrace{\dfrac{d\theta}{dt}}_{=\,\omega}\;\overrightarrow{e_x} &=\dfrac{d(-\sin\theta)}{d\theta}\;\underbrace{\dfrac{d\theta}{dt}}_{=\,\omega}\;\overrightarrow{e_x}
...@@ -537,13 +537,13 @@ $`\begin{align} ...@@ -537,13 +537,13 @@ $`\begin{align}
\\ \\
&=\omega\;\Big(-\cos\theta\;\overrightarrow{e_x}-\sin\theta\;\overrightarrow{e_z}\Big)\\ &=\omega\;\Big(-\cos\theta\;\overrightarrow{e_x}-\sin\theta\;\overrightarrow{e_z}\Big)\\
\\ \\
&\mathbf{=-\;\omega\;\overrightarrow{e_{\rho}}} &=-\;\omega\;\overrightarrow{e_{\rho}}
\end{align}`$ \end{align}`$
--------------- ---------------
$`\begin{align} $`\begin{align}
\mathbf{\dfrac{d^2\overrightarrow{e_{\rho}}}{dt^2}}&=\dfrac{d}{dt}\bigg(\underbrace{\dfrac{d\overrightarrow{e_{\rho}}}{dt}}_{=\,\omega\,\vec{e_{\theta}}}\bigg)\\ \dfrac{d^2\overrightarrow{e_{\rho}}}{dt^2}&=\dfrac{d}{dt}\bigg(\underbrace{\dfrac{d\overrightarrow{e_{\rho}}}{dt}}_{=\,\omega\,\vec{e_{\theta}}}\bigg)\\
\\ \\
&=\dfrac{d}{dt}\left(\omega\,\overrightarrow{e_{\theta}}\right)\\ &=\dfrac{d}{dt}\left(\omega\,\overrightarrow{e_{\theta}}\right)\\
\\ \\
...@@ -551,13 +551,13 @@ $`\begin{align} ...@@ -551,13 +551,13 @@ $`\begin{align}
\\ \\
&=\dfrac{d\omega}{dt}\;\overrightarrow{e_{\theta}}\;+\;\omega\;\big(-\,\omega\;\overrightarrow{e_{\rho}}\big)\\ &=\dfrac{d\omega}{dt}\;\overrightarrow{e_{\theta}}\;+\;\omega\;\big(-\,\omega\;\overrightarrow{e_{\rho}}\big)\\
\\ \\
&\mathbf{=\dfrac{d\omega}{dt}\;\overrightarrow{e_{\theta}}\;-\;\omega^2\;\overrightarrow{e_{\rho}}} &=\dfrac{d\omega}{dt}\;\overrightarrow{e_{\theta}}\;-\;\omega^2\;\overrightarrow{e_{\rho}}
\end{align}`$ \end{align}`$
--------------- ---------------
$`\begin{align} $`\begin{align}
\mathbf{\dfrac{d^2\overrightarrow{e_{\theta}}}{dt^2}} \dfrac{d^2\overrightarrow{e_{\theta}}}{dt^2}
&=\dfrac{d}{dt}\bigg(\underbrace{\dfrac{d\overrightarrow{e_{\theta}}}{dt}}_{=-\omega\,\vec{e_{\rho}}}\bigg)\\ &=\dfrac{d}{dt}\bigg(\underbrace{\dfrac{d\overrightarrow{e_{\theta}}}{dt}}_{=-\omega\,\vec{e_{\rho}}}\bigg)\\
\\ \\
&=\dfrac{d}{dt}\left(-\omega\,\overrightarrow{e_{\rho}}\right)\\ &=\dfrac{d}{dt}\left(-\omega\,\overrightarrow{e_{\rho}}\right)\\
...@@ -566,7 +566,7 @@ $`\begin{align} ...@@ -566,7 +566,7 @@ $`\begin{align}
\\ \\
&=-\dfrac{d\omega}{dt}\;\overrightarrow{e_{\rho}}\;-\;\omega\;\big(\omega\;\overrightarrow{e_{\theta}}\big)\\ &=-\dfrac{d\omega}{dt}\;\overrightarrow{e_{\rho}}\;-\;\omega\;\big(\omega\;\overrightarrow{e_{\theta}}\big)\\
\\ \\
&\mathbf{=\dfrac{d\omega}{dt}\;\overrightarrow{e_{\rho}}\;-\;\omega^2\;\overrightarrow{e_{\theta}}} &=\dfrac{d\omega}{dt}\;\overrightarrow{e_{\rho}}\;-\;\omega^2\;\overrightarrow{e_{\theta}}
\end{align}`$ \end{align}`$
......
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