Georg Baum wrote:

See attached.


Thanks :)

<>
This should not happen, because lyx should select the correct babel options.
Can you send a minimal example file showing this behaviour?
If the pasted text is not really in a foreign language, mark it and then
reset the language in Format->Character.

Ah, thanks. Resetting the language works. I'm attaching two files anyway in case someone wants to debug the problem further. Try pasting something from chapter 5 to chapter 6 and try a DVI view to see the problem. (using LyX 1.3.3-win32)


(Herbert: thanks for the appendix numbering code)

- Henrik
#LyX 1.3 created this file. For more info see http://www.lyx.org/
\lyxformat 221
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\begin_preamble

%%%%%%%%% REF MACROS %%%%%%%%

\def\apj{ApJ}
\def\mnras{MNRAS}
\def\apjl{ApJL}
\def\aap{A\&A}

%%%%%%%%%%%%%%%%%%%%%%%%


%%%%%%%% LAYOUT %%%%%%%%%%
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\end_preamble
\language british
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\quotes_language english
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\layout Chapter

Results, part I
\layout Standard

This chapter is a first look at the experimental results starting with a
 description of the raw data generated by the simulations and the data reduction
 and analysis routines used to extract useful scientific information.
 We also examine the first stage of the simulation, the cooling phase during
 the first 300 Myrs, which is identical for all simulations.
\layout Section

The raw data
\layout Standard


\noun on 
Enzo
\noun default 
 stores the main grid data in industry standard NCSA Hierarchical Data Format
 (HDF)
\begin_inset Foot
collapsed true

\layout Standard

See 
\family typewriter 
http://hdf.ncsa.uiuc.edu
\family default 
 for details.
\end_inset 

.
 These files contain the 11? variables listed in table X, and some meta
 data, such as variable names.
 The HDF format is valuable because the date can be read directly by standard
 visualisation programs like HDFLook and IDL
\begin_inset Foot
collapsed true

\layout Standard

See: 
\family typewriter 
http://daac.gsfc.nasa.gov/MODIS/HDFLook/
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 and 
\family typewriter 
http://www.rsinc.com/idl/
\family default 
.
\end_inset 

.
 The raw data can therefore be studied directly as the simulation progresses
 to ensure that it develops as expected.
 However, each grid in the grid structure is stored in a separate HDF file,
 and with several thousand such grids it is impractrical to analyse this
 data directly.
 Viewing any one grid file only gives a low resolution view of the domain
 or a high resolution view of a very small region.
 To be scientifically useful, the data is reduced in a number of ways.
 Enzo includes as standard data reduction routines for producing 3-dimensional
 extractions, 2-dimensional projections, and 1-dimensional vectors averaged
 over radial shells.
 A fourth reduction tool was developed during this project to extract an
 arbitrary set of point samples from the domain.
\the_end
#LyX 1.3 created this file. For more info see http://www.lyx.org/
\lyxformat 221
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\begin_preamble

%%%%%%%%% REF MACROS %%%%%%%%

\def\apj{ApJ}
\def\mnras{MNRAS}
\def\apjl{ApJL}

%%%%%%%%%%%%%%%%%%%%%%%%
\end_preamble
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\layout Chapter

Discussion
\layout Section

Previous simulations
\layout Standard

Churazov etal.
 
\begin_inset LatexCommand \cite{Churazov_etal_2001}

\end_inset 

 performed the first significant numerical bubble experiment in 2000.
 The setup was modeled on the M87 galaxy and its surroundings, based on
 ROSAT data by Nulsen and Böhringer 
\begin_inset LatexCommand \cite{Nulsen&Bohringer_1995}

\end_inset 

, with typical densities of 0.02 
\begin_inset Formula $\textrm{cm}^{-3}$
\end_inset 

 and temperatures of 2 keV.
 The simulations were 2-dimensional with medium resolution at 
\begin_inset Formula $200^{2}$
\end_inset 

 cells, and rotational symetry was chosen about an axis parallel with the
 gravitational force.
 The computational domain was limited, reaching out 51kpc from the cluster
 core.
 A 2-dimensional gravitational potential and temperature profile were selected,
 and a corresponding density gradient was constructed in hydrostatic equlibrium.
 A sperical heated bubble with a 5 kpc radius was created at 9 kpc from
 the core and alowed to rise in the gravitational potential.
 The bubble was created by instantaneously replacing the ambient gas with
 material at 100 times the original temperature and 0.01 times the original
 density, thus maintaining pressure equilibrium.
 The simulations were naturally limited to the time it took the bubble to
 cross the computational domain, which in this case was 50-70Myrs.
 The authors argued that this short time scale meant that radiative cooling
 was not important, and therefore was not applied.
 
\the_end

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