version 4.2 authored by Udo Ziegler's avatar Udo Ziegler
......@@ -258,9 +258,9 @@ possible values or a numeric range.
conditions. The type of boundary condition at a physical domain
boundary is characterized by a single capital letter. It are
grouped in a 6-letters word with the individual letter
representing, from left to right, the lower-$x$ (`_C.bc[0]`),
upper-$x$ (`_C.bc[1]`), lower-$y$ (`_C.bc[2]`), upper-$y$
(`_C.bc[3]`), lower-$z$ (`_C.bc[4]`) and upper-$z$ (`_C.bc[5]`)
representing, from left to right, the lower-**x** (`_C.bc[0]`),
upper-**x** (`_C.bc[1]`), lower-**y** (`_C.bc[2]`), upper-**y**
(`_C.bc[3]`), lower-**z** (`_C.bc[4]`) and upper-**z** (`_C.bc[5]`)
domain boundary. Possible boundary condition types are
($u_{i/o}$: inner/outer-domain boundary values of a variable
$u$):
......@@ -297,14 +297,14 @@ possible values or a numeric range.
$u_o=u_i$ for the perpendicular magnetic field component.
- `R`: reflection-on-axis (only of relevance in cylindrical
geometry at the $y$-lower boundary at $R=0$ or in
spherical geometry at the $y$-lower/upper boundaries at
geometry at the **y**-lower boundary at $R=0$ or in
spherical geometry at the **y**-lower/upper boundaries at
$\theta =0,\pi$) - reflecting conditions at the geometric
axis. Same as M except for the azimutal magnetic field
component for which $u_o=-u_i$.
- `C`: reflection-at-center (only of relevance in spherical
geometry at the $x$-lower boundary at $r=0$) - reflecting
geometry at the **x**-lower boundary at $r=0$) - reflecting
conditions at the coordinate center. Same as M except for
the non-radial magnetic field components for which
$u_o=-u_i$.
......@@ -316,9 +316,9 @@ possible values or a numeric range.
(pseudo-vacuum condition) for the magnetic field.
- `F`: free boundary (only of relevance in cylindrical
geometry at the $y$-lower boundary at $R=0$ or in
spherical geometry at the $y$-lower/upper boundaries at
$\theta =0,\pi$ and $x$-lower boundary at $r=0$) -
geometry at the **y**-lower boundary at $R=0$ or in
spherical geometry at the **y**-lower/upper boundaries at
$\theta =0,\pi$ and **x**-lower boundary at $r=0$) -
'natural' boundary condition at the geometric axis. Boundary
values are not set explictely but are implicitly given by
$\pi$-shifted values. Note that when a `F`-type boundary
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