\begin{table}%tB.4
%\centering
\par
  \caption {\label{Tab:3d-models-2}Continuation of \tabref{Tab:3d-models-1}.  For the MBI
    model with $b_0^z = 10 ~{\rm G}$, we do not provide values for
    the Maxwell stress, because the magnetic field behaves similar to
    a purely passive field.
    %%
  }
\begin{tabular}{lccccccccccc}
    \hline\hline
    Field
    & Grid size
    & Resolution
    & Rot
    & $\partial_{\varpi} S$
    & $b^z_0$
    & BC
    & $\sigma$ 
    & $M_{\varpi \phi}^{\rm term}$
    & $M_{\varpi \phi}^{\rm max}$
    & $\left\langle M_{\varpi \phi} \right\rangle$
    \\
    & $[\textrm{km}^3]$
    &
    & 
    & $\left[{\rm km}^{-1}\right]$
    & $\left[10^{12}~{\rm G}\right]$
    &
    & $\left[{\rm ms}^{-1}\right]$
    & $\left[10^{28}~{\rm G}^2 ~ {\rm cm}^{-3}\right]$
    & $\left[10^{28}~{\rm G}^2 ~ {\rm cm}^{-3}\right]$
    & $\left[10^{28}~{\rm G}^2 ~ {\rm cm}^{-3}\right]$
    \\
\par
    \hline 
    V3
    & $1 \times 1 \times 1$
    & $50 \times 50 \times 50$
    & d & 0
    & 10
    & d
    & 0.66
    & 0.13
    & 0.24
    & 0.16
    \\
    & $1 \times 1 \times 1$
    & $50 \times 50 \times 50$
    & d & 0
    & 20
    & d
    & 0.96
    & 0.53
    & 0.53
    & 0.21
    \\
    & $1 \times 1 \times 1$
    & $50 \times 50 \times 50$
    & d & 0
    & 40
    & d
    & 1.03
    & 1.5
    & 1.5
    & 0.27
    \\
    & $1 \times 4 \times 1$
    & $50 \times 200 \times 50$
    & d & 0
    & 10
    & d
    & 0.66
    & 0.13
    & 0.52
    & 0.24
    \\
    & $1 \times 4 \times 1$
    & $50 \times 200 \times 50$
    & d & 0
    & 20
    & d
    & 0.90
    & 0.36
    & 0.80
    & 0.43
    \\
    & $1 \times 4 \times 1$
    & $100 \times 400 \times 100$
    & d & 0
    & 20
    & d
    & 1.08
    & 1.1
    & 1.1
    & 0.20
    \\
    & $1 \times 4 \times 1$
    & $100 \times 400 \times 100$
    & d & 0
    & 20
    & p
    & 1.08
    & 1.5
    & 1.5
    & 0.21
    \\
    U3
    & $1 \times 2 \times 1$
    & $26 \times 50 \times 26$
    & d & $-0.038$
    & 20
    & d
    & 1.5
    & 1.9
    & 5.3
    & 0.83
    \\
    & $1 \times 2 \times 1$
    & $26 \times 50 \times 26$
    & d & $-0.038$
    & 40
    & d
    & 1.7
    & 4.1
    & 7.2
    & 1.1
    \\
    & $1 \times 2 \times 1$
    & $50 \times 100 \times 50$
    & d & $-0.038$
    & 20
    & d
    & 1.7
    & 3.1
    & 3.1
    & 0.16
    \\
    & $1 \times 2 \times 1$
    & $50 \times 100 \times 50$
    & d & $-0.038$
    & 40
    & d
    & 1.9
    & 4.4
    & 4.4
    & 0.23
    \\
    & $1 \times 2 \times 1$
    & $50 \times 100 \times 50$
    & $r{}^{1900}$ & $-0.10$
    & $10^{-11}$ & d
    & 2.6
    \\
    & $1 \times 2 \times 1$
    & $50 \times 100 \times 50$
    & $r{}^{1900}$ & $-0.10$
    & 0.01 & d
    & 2.6
    & $2.3 \times 10^{-8}$
    & 0.11
    & 0.040
    \\
    & $1 \times 2 \times 1$
    & $50 \times 100 \times 50$
    & $r{}^{1900}$ & $-0.10$
    & 20 & d
    & 2.6
    & 0.060
    & 0.87
    & 0.30
    \\
    V3
    & $1 \times 2 \times 1$
    & $50 \times 100 \times 50$
    & d & $-0.038$
    & 20
    & d
    & 1.6
    & 0.54
    & 0.54
    & 0.011
    \\
    \hline
   \end{tabular}
 \end{table}