real teff:
The effective temperature is one of the basic model parameters and is
specified e.g. with
real teff f=F13.3 b=4 n='Effective Temperature' u=K
3500.0
(for a relatively cool star).
Note that the actual effective temperature can only be determined a posteriori
and that the entropy of the instreaming entropy (see below) is more important
than teff itself. In fact, teff is only used to control
material properties at the outer boundary. Its value should be close to
the expected effective temperature of the model.
character grav_mode:
Gravity is another characteristic of a stellar atmosphere. The type (or geometry)
of the external gravity field has to be specified e.g. with
character grav_mode f=A80 b=80 n='Type of gravity field' &
c0='constant/central'
central
Three values are possible so far:
real grav:
In the case of a constant gravity the amount of the acceleration has to specified with
real grav f=E15.8 b=4 n='Gravity' u=cm/s^2
27500.0
Setting this value to zero switches off gravity (oh wonder).
real mass_star:
In the case of a central the mass (in cgs units) of the star has to be specified with
real mass_star f=E15.8 b=4 n='Stellar Mass' u=g
9.94500e+33
real r0_grav:
To avoid the central singularity in a 1/r potential it is smoothed in
the center to give a central potential of 1/r0_grav, specified with
real r0_grav f=E15.8 b=4 n='Inner Smoothing Radius' u=cm
9.45833e+12
This parameter should always be non-zero for a central potential.
real r1_grav:
The density in an atmosphere in hydrostatic equilibrium can decline to very
low values. To artificial enlarge the pressure (and density) scale height
in the outer layers of the star (the corners of the box) the gravity can
be reduced by defining the potential at infinity to be
1/r1_grav, specified with
real r1_grav f=E15.8 b=4 n='Outer Smoothing Radius' u=cm &
c0='0.0: Not used'
11.35000e+13
Setting this parameter to zero gives the usual
behavior of the potential
in the outer layers but also chooses another smoothing formula in the central
part (where real r0_grav is relevant).
But a value somewhat larger than the remotest corner of the box effectively
cancels this artificial smoothing in the outer layers without changing
the formula for the potential.
real r2_grav:
Using real r2_grav instead of real r1_grav means that a potential
function more appropriate for a polytropic stellar interior model is used.
It can be set, e.g. with
real r2_grav f=E15.8 b=4 n='Outer Smoothing Radius' u=cm &
c0='0.0: Not used'
11.35000e+13
Setting this parameter to zero means the potential parametrized with real r1_grav
is used.
This parameter is similar to real r1_grav, i.e., it enlarges the pressure
scale hight in the outer layers but does not change the smoothing
formula in the center. This parameter is only effective if real r1_grav is
set to zero.
real r1_rad:
For a ``Star-in-a-Box'' and particularly when only ``simple'' ray directions are allowed
in the radiation transport step the temperature in the outer corners of the box tends to
become very small. To artificially increase the effect of radiative heating the
parameter real r1_rad can specify a radius beyond which only positive contributions
of the radiative energy transport to the energy budget are taken into account. This
ruins the conservativity of the code in these layers and should be applied only in very
remote corners which are then considered only as sort of extended boundary region but
not as part of the ``real'' model.
The parameter can be specified e.g. with
real r1_rad f=E15.8 b=4 n='Outer radiation transport radius' u=cm &
c0='0.0: Not used'
8.00000e+13
A value of 0.0 (default) or below deactivates this feature.
real r0_core:
To insert energy in a sphere different with a radius other than r0_grav,
the heating radius r0_core can be specified separately, e.g. with
real r0_core f=E15.8 b=4 n='Core Radius' u=cm
9.45833e+12
If this parameter is not specified r0_grav is used as the radius of the core.
character centrifugal_force:
Usually, a centrifugal force is applied if nu_rotation
0. To switch it off
even for non-zero rotation rate, the parameter centrifugal_force can be used,
e.g. by setting
character centrifugal_force f=A80 b=80 n='Switch on/off the centrifugal force' &
c0='on: default, off: no centrifugal force, even for non-zero nu_rotation'
off
Three values are possible so far:
on: This is the default and can be set even for non-rotating objects.
off: This skips the application of the centrifugal force in case of
a non-zero rotation rate. In this case, only the Coriolis force is applied.
By default, the centrifugal force is activated.
real nu_rotation:
To transform onto a coordinate system rotation
around the x3 axis,
a rotation rate can be specified with e.g.
real nu_rotation f=E15.8 b=4 n='Rotation frequency' u=1/s
0.0
The potential is modified by adding terms due to a
centrifugal force
unless centrifugal_force is set to off.
In addition, a Coriolis force
are applied during the hydrodynamics step.
real ar_RotationAxis:
The radii of the dust grains
are specified with e.g.
real ar_rotationaxis f=E10.4 b=4 p=1 d=(1:3) n='Rotation axis' u=1
1.0
0.0
0.0
The default value is (0.0,0.0,1.0).