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Udo Ziegler
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3-NIRVANA-user-guide/3.2-User-interfaces.md
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@@ -258,9 +258,9 @@ possible values or a numeric range.
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conditions. The type of boundary condition at a physical domain
conditions. The type of boundary condition at a physical domain
boundary is characterized by a single capital letter. It are
boundary is characterized by a single capital letter. It are
grouped in a 6-letters word with the individual letter
grouped in a 6-letters word with the individual letter
representing, from left to right, the lower-
$x$
(`_C.bc[0]`),
representing, from left to right, the lower-
**x**
(`_C.bc[0]`),
upper-
$x$
(`_C.bc[1]`), lower-
$y$
(`_C.bc[2]`), upper-
$y$
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]`)
(`_C.bc[3]`), lower-
**z**
(`_C.bc[4]`) and upper-
**z**
(`_C.bc[5]`)
domain boundary. Possible boundary condition types are
domain boundary. Possible boundary condition types are
($u_{i/o}$: inner/outer-domain boundary values of a variable
($u_{i/o}$: inner/outer-domain boundary values of a variable
$u$):
$u$):
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$u_o=u_i$ for the perpendicular magnetic field component.
$u_o=u_i$ for the perpendicular magnetic field component.
- `R`: reflection-on-axis (only of relevance in cylindrical
- `R`: reflection-on-axis (only of relevance in cylindrical
geometry at the
$y$
-lower boundary at $R=0$ or in
geometry at the
**y**
-lower boundary at $R=0$ or in
spherical geometry at the
$y$
-lower/upper boundaries at
spherical geometry at the
**y**
-lower/upper boundaries at
$\theta =0,\pi$) - reflecting conditions at the geometric
$\theta =0,\pi$) - reflecting conditions at the geometric
axis. Same as M except for the azimutal magnetic field
axis. Same as M except for the azimutal magnetic field
component for which $u_o=-u_i$.
component for which $u_o=-u_i$.
- `C`: reflection-at-center (only of relevance in spherical
- `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
conditions at the coordinate center. Same as M except for
the non-radial magnetic field components for which
the non-radial magnetic field components for which
$u_o=-u_i$.
$u_o=-u_i$.
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(pseudo-vacuum condition) for the magnetic field.
(pseudo-vacuum condition) for the magnetic field.
- `F`: free boundary (only of relevance in cylindrical
- `F`: free boundary (only of relevance in cylindrical
geometry at the
$y$
-lower boundary at $R=0$ or in
geometry at the
**y**
-lower boundary at $R=0$ or in
spherical geometry at the
$y$
-lower/upper boundaries at
spherical geometry at the
**y**
-lower/upper boundaries at
$\theta =0,\pi$ and
$x$
-lower boundary at $r=0$) -
$\theta =0,\pi$ and
**x**
-lower boundary at $r=0$) -
'natural' boundary condition at the geometric axis. Boundary
'natural' boundary condition at the geometric axis. Boundary
values are not set explictely but are implicitly given by
values are not set explictely but are implicitly given by
$\pi$-shifted values. Note that when a `F`-type boundary
$\pi$-shifted values. Note that when a `F`-type boundary
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