User:Pfafrich/Blahtex \mathbf bugs

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 \mathbf,\mathrm follow, \hat or vec inside a math tag. Each occurence \mathbf\hat x' should be replaced by \mathbf{\hat x} and when fixed the pages should be moved to the done section. Feel free to fix as necessary.

grep '\\mathbf\\dot' eqnsJan06.txt
grep '\\mathbf\\hat' eqnsJan06.txt
grep '\\mathrm\\dot' eqnsJan06.txt
grep '\\mathrm\\hat' eqnsJan06.txt
grep '\\mathrm\\frac' eqnsJan06.txt

done

• Four-acceleration $\mathbf {a} ={\dot {\gamma }}\mathbf {u} +\gamma \mathbf {\dot {u}}$
• Four-force $\mathbf {f} =m_{0}\left({\dot {\gamma }}\mathbf {u} +\gamma \mathbf {\dot {u}} \right)$
• Discretization $\mathbf {\dot {x}} (t)=\mathbf {A} \mathbf {x} (t)+\mathbf {B} \mathbf {u} (t)$
• Discretization $e^{-\mathbf {A} t}\mathbf {\dot {x}} (t)=e^{-\mathbf {A} t}\mathbf {A} \mathbf {x} (t)+e^{-\mathbf {A} t}\mathbf {B} \mathbf {u} (t)$
• Vector fields in cylindrical and spherical coordinates $\mathbf {\dot {A}} ={\dot {A}}_{x}\mathbf {\hat {x}} +{\dot {A}}_{y}\mathbf {\hat {y}} +{\dot {A}}_{z}\mathbf {\hat {z}}$
• 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 $\mathbf {\dot {A}} ={\boldsymbol {\hat {\rho }}}({\dot {A}}_{\rho }-A_{\phi }{\dot {\phi }})+{\boldsymbol {\hat {\phi }}}({\dot {A}}_{\phi }+A_{\rho }{\dot {\phi }})+{\boldsymbol {\hat {z}}}{\dot {A}}_{z}$
• Vector fields in cylindrical and spherical coordinates $\mathbf {\dot {A}} ={\dot {A}}_{x}\mathbf {\hat {x}} +{\dot {A}}_{y}\mathbf {\hat {y}} +{\dot {A}}_{z}\mathbf {\hat {z}}$
• 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 $\mathbf {\dot {A}} ={\boldsymbol {\hat {r}}}({\dot {A}}_{r}-A_{\theta }{\dot {\theta }}-A_{\phi }{\dot {\phi }}\sin \theta )+{\boldsymbol {\hat {\theta }}}({\dot {A}}_{\theta }+A_{r}{\dot {\theta }}-A_{\phi }{\dot {\phi }}\cos \theta )+{\boldsymbol {\hat {\phi }}}({\dot {A}}_{\phi }+A_{r}{\dot {\phi }}\sin \theta +A_{\phi }{\dot {\phi }}\cos \theta )$
• Vector fields in cylindrical and spherical coordinates ${\begin{bmatrix}{\boldsymbol {\hat {\rho }}}\\{\boldsymbol {\hat {\phi }}}\\{\boldsymbol {\hat {z}}}\end{bmatrix}}={\begin{bmatrix}\cos \phi &\sin \phi &0\\-\sin \phi &\cos \phi &0\\0&0&1\end{bmatrix}}{\begin{bmatrix}\mathbf {\hat {x}} \\\mathbf {\hat {y}} \\\mathbf {\hat {z}} \end{bmatrix}}$
• Vector fields in cylindrical and spherical coordinates $\mathbf {\dot {A}} ={\dot {A}}_{x}\mathbf {\hat {x}} +{\dot {A}}_{y}\mathbf {\hat {y}} +{\dot {A}}_{z}\mathbf {\hat {z}}$
• Vector fields in cylindrical and spherical coordinates ${\begin{bmatrix}{\boldsymbol {\hat {r}}}\\{\boldsymbol {\hat {\theta }}}\\{\boldsymbol {\hat {\phi }}}\end{bmatrix}}={\begin{bmatrix}\sin \theta \cos \phi &\sin \theta \sin \phi &\cos \theta \\\cos \theta \cos \phi &\cos \theta \sin \phi &-\sin \theta \\-\sin \phi &\cos \phi &0\end{bmatrix}}{\begin{bmatrix}\mathbf {\hat {x}} \\\mathbf {\hat {y}} \\\mathbf {\hat {z}} \end{bmatrix}}$
• Vector fields in cylindrical and spherical coordinates $\mathbf {\dot {A}} ={\dot {A}}_{x}\mathbf {\hat {x}} +{\dot {A}}_{y}\mathbf {\hat {y}} +{\dot {A}}_{z}\mathbf {\hat {z}}$
• Cross product $\mathbf {a} \times \mathbf {b} =\mathbf {\hat {n}} \left|\mathbf {a} \right|\left|\mathbf {b} \right|\sin \theta$
• Vector area $\mathbf {S} =\mathbf {\hat {n}} S$
• D'Hondt method $\mathrm {\frac {V}{s+1}}$
• Diagrams For Foucault Pendulum $\mathrm {\frac {velocity\;vector\;at\;a\;given\;latitude}{velocity\;vector\;at\;equator}}$
• Diagrams For Foucault Pendulum $\mathrm {\frac {1\;EVU\;\times \;cosine\;of\;latitude}{1\;EVU\;\times \;cosine\;of\;zero}}$
• Diagrams For Foucault Pendulum $\mathrm {\frac {cosine\;of\;latitude}{1}}$
• Diagrams For Foucault Pendulum $\mathrm {\frac {velocity\;vector\;at\;latitude\;A}{velocity\;vector\;at\;latitude\;B}}$
• Diagrams For Foucault Pendulum $\mathrm {\frac {1\;EVU\;\times \;cosine\;of\;latitude\;A}{1\;EVU\;\times \;cosine\;of\;latitude\;B}}$
• Diagrams For Foucault Pendulum $\mathrm {\frac {cosine\;of\;latitude\;A}{cosine\;of\;latitude\;B}}$
• Diagrams For Foucault Pendulum $\mathrm {\frac {ORTRP\;at\;a\;given\;latitude}{ORTRP\;at\;the\;North\;Pole}}$
• Diagrams For Foucault Pendulum $\mathrm {\frac {1\;day\;\times \;sine\;of\;90}{1\;day\;\times \;sine\;of\;given\;latitude}}$
• Diagrams For Foucault Pendulum $\mathrm {\frac {1}{sine\;of\;given\;latitude}}$
• Diagrams For Foucault Pendulum $\mathrm {\frac {ORTRP\;at\;latitude\;A}{ORTRP\;at\;latitude\;B}}$
• Diagrams For Foucault Pendulum $\mathrm {\frac {1\;day\;\times \;sine\;of\;latitude\;B}{1\;day\;\times \;sine\;of\;latitude\;A}}$
• Diagrams For Foucault Pendulum $\mathrm {\frac {sine\;of\;latitude\;B}{sine\;of\;latitude\;A}}$