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Table 4:

Some properties of the 2D and 3D hydrodynamic models based on initial model SC.

Run
Grid w $\Delta r$ $\Delta\theta$ $\Delta\phi$ $R_{\rm e1}$ $R_{\rm e2}$ $v_{\rm c1}$ $v_{\rm c2}$ $\tau_{\rm cnv1}$ $\tau_{\rm cnv2}$ $t_{\rm max}$
$\mbox{[name]}$ $N_{\rm r} \times N_\theta \times$N$_\phi$ [ $\mbox{$^\circ$ }$] [106 cm] [ $\mbox{$^\circ$ }$] [ $\mbox{$^\circ$ }$]     [ $10^{6}~\mbox{\ cm~s${}^{-1}$ }$] [ $10^{6}~\mbox{\ cm~s${}^{-1}$ }$] [ s ] [ s ] [ s ]

heflpopIII.2d.1
$720 \times 50$ 50 7.6 1 - 103 102 1.3 1.0 2900 2400 1400
heflpopIII.2d.2 $1500 \times 120$ 120 3.7 1 - 105 103 1.7 1.0 2200 2400 6400
heflpopIII.3d $720 \times 50 \times 50$ 50 7.6 1 1 102 102 0.4 0.3 9500 8000 1400

Notes. Number of grid zones, wedge size w, grid resolution in r, $\theta$ and $\phi$ direction, estimated Reynolds numbers $R_{\rm e1}$, $R_{\rm e2}$, characteristic flow velocities, $v_{\rm c1}$ and $v_{\rm c2}$, and typical convective turnover timescales, $\tau_{\rm cnv1}$ and $\tau_{\rm cnv2}$, for the CVZ-1 and CVZ-2 part of the convection zone, respectively. $t_{\rm max}$ is the maximum evolution time.


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