User:Pfafrich/Blahtex \dot bugs

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User:Pfafrich/Blahtex en.wikipedia fixup

This page is part a set of pages devoted to fixing latex bugs in the english wikipedia so that they will be compatable with the meta:Blahtex MathML project.

Below are pages which contain combination of \dot, \hat etc. inside a math tag. Each occurence \dot\hat x should be replaced by \dot{\hat x} and when fixed the pages should be moved to the done section. Feel free to fix as necessary.

The combinations tested here are two consecutive symbols in: \ddot \dot \hat \bar \vec \overrightarrow\ \overleftarrow \widehat \overline \underline \underrightarrow \underleftarrow \overbrace \underbrace.

[edit] done

Lagrangian $m\ddot\vec{x}+\nabla V=0$
Vector fields in cylindrical and spherical coordinates $\mathbf\dot A = \dot A_\rho \boldsymbol\hat\rho + A_\rho \boldsymbol\dot\hat\rho + \dot A_\phi \boldsymbol\hat\phi + A_\phi \boldsymbol\dot\hat\phi + \dot A_z \boldsymbol\hat z + A_z \boldsymbol\dot\hat z$
Vector fields in cylindrical and spherical coordinates $\left[\begin{matrix} \boldsymbol\dot\hat\rho & = & \dot\phi \boldsymbol\hat\phi \\ \boldsymbol\dot\hat\phi & = & - \dot\phi \boldsymbol\hat\rho \\ \boldsymbol\dot\hat z & = & 0 \end{matrix}\right.$
Vector fields in cylindrical and spherical coordinates $\mathbf\dot A = \dot A_r \boldsymbol\hat r + A_r \boldsymbol\dot\hat r + \dot A_\theta \boldsymbol\hat\theta + A_\theta \boldsymbol\dot\hat\theta + \dot A_\phi \boldsymbol\hat\phi + A_\phi \boldsymbol\dot\hat\phi$
Vector fields in cylindrical and spherical coordinates $\begin{bmatrix}\boldsymbol\dot\hat r \\ \boldsymbol\dot\hat\theta \\ \boldsymbol\dot\hat\phi \end{bmatrix} = \begin{bmatrix} 0 & \dot\theta & \dot\phi \sin\theta \\ -\dot\theta & 0 & \dot\phi \cos\theta \\ -\dot\phi \sin\theta & -\dot\phi \cos\theta & 0 \end{bmatrix} \begin{bmatrix} \boldsymbol\hat r \\ \boldsymbol\hat\theta \\ \boldsymbol\hat\phi \end{bmatrix}$
Kinematics $\dot \vec i = \omega \vec k \times \vec i = \omega \vec j$
Kinematics $\dot \vec j = \omega \vec k \times \vec j = - \omega \vec i$
Kinematics $\vec v = \dot x \vec i + x \dot \vec i + \dot y \vec j + y \dot \vec j$
Kinematics $\vec v = (\dot x \vec i + \dot y \vec j) + (y \dot \vec j + x \dot \vec i) = \vec v_{rel} + \vec \omega \times \vec r$
Kinematics $\frac{d (\vec \omega \times \vec r)}{dt} = \dot \vec \omega \times \vec r + \vec \omega \times \dot \vec r$
Kinematics $\dot \vec r$
Kinematics $\frac{d (\vec \omega \times \vec r)}{dt} = \dot \vec \omega \times \vec r + \vec \omega \times (\vec \omega \times \vec r) + \vec \omega \times \vec v_{rel}$
Kinematics $\vec a = \vec a_{rel} + \omega \times \vec v_{rel} + \dot \vec \omega \times \vec r + \vec \omega \times (\vec \omega \times \vec r) + \vec \omega \times \vec v_{rel}$
Kinematics $\vec a = \vec a_{rel} + 2(\omega \times \vec v_{rel}) + \dot \vec \omega \times \vec r + \vec \omega \times (\vec \omega \times \vec r)$
Frame of reference $\vec a = \vec a' + \dot\vec\omega \times \vec r' + 2\vec\omega \times \vec v' + \vec\omega \times (\vec\omega \times \vec r') + \vec A_0$
Frame of reference $\vec F'_\mathrm{transverse} = -m\dot\vec\omega \times \vec r'$
Area (geometry) ${1 \over 2} \oint_{t_0}^{t_1} \vec u \times \dot \vec u \, dt$
Mariner 1 $\bar\dot{r}_n$
Two-element Boolean algebra $\overline\overline{A}=A$

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User:Pmurray bigpond.com/Complex Numbers as a 3 Vector $\bar \hat z = \begin{pmatrix} z_0 \\ - z_1 \\ z_2 \end{pmatrix}$
Talk:Boolean algebra/Archive01 $\overline\overline{A}=A$

for i in 'ddot' 'dot' 'hat' 'bar' 'vec' 'overrightarrow' 'overleftarrow' 'widehat' 'overline' 'underline' 'underrightarrow' 'underleftarrow' 'overbrace' 'underbrace' ; do for j in 'ddot' 'dot' 'hat' 'bar' 'vec' 'overrightarrow' 'overleftarrow' 'widehat' 'overline' 'underline' 'underrightarrow' 'underleftarrow' 'overbrace' 'underbrace' ; do echo "\\$i\\$j" ; egrep "\\\\$i[[:space:]]*\\\\$j" eqnsJan06.txt >> dothat.txt  ; done; done;

User:Pfafrich/Blahtex \dot bugs

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[edit] done

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