Am 01.10.2010 um 17:41 schrieb Mojca Miklavec:
And the other question: is there some quick trick that would "rotate the whole page" inside a document, so that the page would still be portrait, but text would be rotated with textwidth and textheight swapped, but with preserved main header (in reality I do not care about the header).
I would like to put a narrow, but several lines long equation (\startalign) on left (bottom) and image on the right (top).
I was playing with an approximation
\rotate[rotation=90]{\vbox{ \startformula\startalign[n=6,align={middle,middle,right,middle,left,left}] \NC l \NC\hbox to 1em{}\NC m_l \NC\hbox to 1em{}\NC \text{orb.}\hbox to 2em{} \NC Y_{lm}\NR \NC 0 \NC\NC 0 \NC\NC s \NC \frac{1}{2}\sqrt{\frac{ 1}{π}} \NR \NC 1 \NC\NC 0 \NC\NC p_z \NC \frac{1}{2}\sqrt{\frac{ 3}{π}}\frac{z}{r} \NR \NC 1 \NC\NC \pm1 \NC\NC p_x \NC \frac{1}{2}\sqrt{\frac{ 3}{π}}\frac{x}{r} \NR \NC \NC\NC \NC\NC p_y \NC \frac{1}{2}\sqrt{\frac{ 3}{π}}\frac{y}{r} \NR \NC 2 \NC\NC 0 \NC\NC d_{z^2} \NC \frac{1}{4}\sqrt{\frac{ 5}{π}}\frac{3z^2-r^2}{r^2} \NR \NC 2 \NC\NC \pm1 \NC\NC d_{xz} \NC \frac{1}{2}\sqrt{\frac{15}{π}}\frac{xz}{r^2} \NR \NC \NC\NC \NC\NC d_{yz} \NC \frac{1}{2}\sqrt{\frac{15}{π}}\frac{yz}{r^2} \NR \NC 2 \NC\NC \pm2 \NC\NC d_{xy} \NC \frac{1}{2}\sqrt{\frac{15}{π}}\frac{xy}{r^2} \NR \NC \NC\NC \NC\NC d_{x^2-y^2} \NC \frac{1}{4}\sqrt{\frac{15}{π}}\frac{x^2-y^2}{r^2} \NR \stopalign\stopformula}} % and then externalfigure on the right ...
but the formula takes exactly \textwidth space, I didn't manage to convince it to consume less space (I could probably change textwidth locally).
I know for workarounds (typesetting a different document for example and then include the page), but I really wonder if switching orientation just for a page (to typeset a table for example) is doable in some elegant way.
\starttext \bTABLE[orientation=90,frame=off,width=\textwidth,height=.5\textheight,align=lohi] \bTR \bTD \externalfigure[cow] \eTD \eTR \bTR \bTD \starttabulate[|Mc|Mr|Ml|Ml|] \NC l \NC m_l \NC \text{orb.} \NC Y_{lm} \NC\NR \NC 0 \NC 0 \NC s \NC \frac{1}{2}\sqrt{\frac{1}{π}} \NC\NR \NC 1 \NC 0 \NC p_z \NC \frac{1}{2}\sqrt{\frac{3}{π}}\frac{z}{r} \NC\NR \NC 1 \NC ±1 \NC p_x \NC \frac{1}{2}\sqrt{\frac{3}{π}}\frac{x}{r} \NC\NR \NC \NC \NC p_y \NC \frac{1}{2}\sqrt{\frac{3}{π}}\frac{y}{r} \NC\NR \NC 2 \NC 0 \NC d_{z^2} \NC \frac{1}{4}\sqrt{\frac{5}{π}}\frac{3z^2-r^2}{r^2} \NC\NR \NC 2 \NC ±1 \NC d_{xz} \NC \frac{1}{2}\sqrt{\frac{15}{π}}\frac{xz}{r^2} \NC\NR \NC \NC \NC d_{yz} \NC \frac{1}{2}\sqrt{\frac{15}{π}}\frac{yz}{r^2} \NC\NR \NC 2 \NC ±2 \NC d_{xy} \NC \frac{1}{2}\sqrt{\frac{15}{π}}\frac{xy}{r^2} \NC\NR \NC \NC \NC d_{x^2-y^2} \NC \frac{1}{4}\sqrt{\frac{15}{π}}\frac{x^2-y^2}{r^2} \NC\NR \stoptabulate \eTD \eTR \eTABLE \stoptext Wolfgang