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version 4.2
authored
Oct 30, 2025
by
Udo Ziegler
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3-NIRVANA-user-guide/3.2-User-interfaces.md
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@@ -974,7 +974,7 @@ integral form of $\mathbf{B}=\nabla\times \mathbf{A}$:
...
@@ -974,7 +974,7 @@ integral form of $\mathbf{B}=\nabla\times \mathbf{A}$:
where the difference operators
*Δ*
<sub>
ix
</sub>
,
*Δ*
<sub>
iy
</sub>
where the difference operators
*Δ*
<sub>
ix
</sub>
,
*Δ*
<sub>
iy
</sub>
and
*Δ*
<sub>
iz
</sub>
are given by
and
*Δ*
<sub>
iz
</sub>
are given by
*Δ*
<sub>
ix
</sub>
X=X(ix,iy,iz
+1
)-X(ix,iy,iz)
*Δ*
<sub>
ix
</sub>
X=X(ix
+1
,iy,iz)-X(ix,iy,iz)
*Δ*
<sub>
iy
</sub>
X=X(ix,iy+1,iz)-X(ix,iy,iz)
*Δ*
<sub>
iy
</sub>
X=X(ix,iy+1,iz)-X(ix,iy,iz)
...
@@ -1011,10 +1011,19 @@ for two problems: the Orszag-Tang vortex problem (example 1) and a
...
@@ -1011,10 +1011,19 @@ for two problems: the Orszag-Tang vortex problem (example 1) and a
shock-cloud interaction problem (example 2).
shock-cloud interaction problem (example 2).
**Example 1**
(taken from
`/nirvana/testproblems/MHD/problem2`
; cf.
**Example 1**
(taken from
`/nirvana/testproblems/MHD/problem2`
; cf.
\[
[
Z04
](
#references
)
\]
)
[
Z04
](
#references
)
)
IC for the Orszag-Tang vortex problem simulated in a doubly-periodic
IC for the Orszag-Tang vortex problem simulated in a doubly-periodic
square domain of length $L$ (given by
`_C.up[0]-_C.lo[0]`
):
square 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)
**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*
)
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.
$
\v
arrho =
\v
arrho_0$
$
\v
arrho =
\v
arrho_0$
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