Update 3.2 User interfaces authored by Udo Ziegler's avatar Udo Ziegler
......@@ -969,9 +969,9 @@ where (*Â*<sub>*x*</sub>, *Â*<sub>*y*</sub>, *Â*<sub>*z*</sub>) denote
the path integrals
![ic_A](uploads/d7670a3203d0f3a1e2a9a759e69e2e77/ic_A.png)
over corresponding cell edges. The difference operator
*Δ*<sub>`i`*y*</sub>, for instance, is given by
*Δ*<sub>`iy`</sub>, for instance, is given by
*Δ*<sub>`iy`</sub>*Â*<sub>*x*</sub> = *Â*<sub>*x*</sub>(`ix`,`iy`+1,` `iz`) − *Â*<sub>*x*</sub>(`ix`,`iy`,`iz`)
*Δ*<sub>`iy`</sub>*Â*<sub>*x*</sub> = *Â*<sub>*x*</sub>(`ix`,`iy`+1,`iz`) − *Â*<sub>*x*</sub>(`ix`,`iy`,`iz`)
and similarly for others. If the *Â*’s are *unambiguously* computed (or
approximated) on coinciding cell edges in the grid hierarchy, the
......@@ -1011,15 +1011,15 @@ domain of length *L* (given by `_C.up[0]-_C.lo[0]`):
𝜚 = 𝜚<sub>0</sub>
**m** = 𝜚<sub>0</sub>(−sin(2*π* *y*/*L*),sin(2*π* *x*/*L*),0)
**m** = 𝜚<sub>0</sub>(−sin(2*π* *y*/*L*),sin(2*π* *x*/*L*),0)
**B** = *B*<sub>0</sub>(−sin(2*π* *y*/*L*),sin(4*π* *x*/*L*),0)
**B** = *B*<sub>0</sub>(−sin(2*π* *y*/*L*),sin(4*π* *x*/*L*),0)
*e* = *p*<sub>0</sub>/(*γ*1) + **m**<sup>2</sup>/(2𝜚) + **B**<sup>2</sup>/(2*μ*)
*e* = *p*<sub>0</sub>/(*γ*1) + **m**<sup>2</sup>/(2𝜚) + **B**<sup>2</sup>/(2*μ*)
where 𝜚<sub>0</sub> = 2.77778, *p*<sub>0</sub> = 5/3 and
*B*<sub>0</sub> = 1. The adiabatic index *γ* = 5/3 and the magnetic
permeability *μ* = 1.
where 𝜚<sub>0</sub>=2.77778, *p*<sub>0</sub>=5/3 and
*B*<sub>0</sub>=1. The adiabatic index *γ*=5/3 and the magnetic
permeability *μ*=1.
void configUser(GRD **gm)
/**
......@@ -1092,10 +1092,7 @@ expression *a*<sup>2</sup> + *b*<sup>2</sup> + *c*<sup>2</sup>.
IC for the shock-cloud interaction problem simulated in a Cartesian box
given by (*x*, *y*, *z*) ∈ \[ − 1/2, 1/2\]<sup>3</sup>:
$$(\\varrho,p,v\_x,v\_y,v\_z,B\_x,B\_y,B\_z)=\\left\\{\\begin{array}{ll}
(3.86859,167.345,0,0,0,0,2.1826182,-2.1826182) & x&lt;0.1\\\\
(1,1,-11.2536,0,0,0,0.56418958,0.56418958) & x\\ge 0.1
\\end{array}\\right.$$
![ic_example2](uploads/e31ebefeb64b91e0ef74d839ebac4de8/ic_example2.png)
At **x** = (0.3, 0, 0) a spherical clump with radius 0.15 and density of
10 is embedded and co-moving with its surrounding flow under the
assumption of pressure equilibrium. The adiabatic index *γ* = 5/3 and
......@@ -1201,7 +1198,7 @@ magnetic permeability *μ* = 1.
return;
}
### Defining boundary conditions
## Defining boundary conditions
A superblock `g` includes up to 3 ghost cells per side per coordinate
direction beyond its active region. The number of ghost cells depends on
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