Open and closed boundaries in large-scale convective dynamos

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Table 2:

Summary of the runs with varying ${\rm Co}$ and ${\rm Sh}$ .
Run	Grid	${\rm Co}$	$\tilde\lambda$	$\epsilon_{\rm f}$	$k_{\rm f}^{(\omega)}/k_{\rm f}$	bc
VF11	128³	0.07	0.000	-0.014	1.29	VF
VF12	128³	0.16	0.006	-0.022	1.40	VF
VF13	128³	0.34	0.023	-0.041	1.52	VF
VF14	128³	0.63	0.038	-0.068	1.60	VF
VF15	128³	1.36	0.054	-0.097	1.76	VF
PC9	128³	0.07	-0.008	-0.012	1.30	PC
PC10	128³	0.16	0.003	-0.022	1.41	PC
PC11	128³	0.38	0.014	-0.042	1.50	PC
PC12	128³	0.75	0.028	-0.072	1.58	PC
PC13	128³	1.55	0.034	-0.098	1.74	PC

Notes. Here ${\rm Ma}\approx0.045$ , ${\rm Rm}\approx35$ , ${\rm Pm}=2.5$ , and ${\rm Sh}=-{\textstyle{1\over2}}{\rm Co}$ (i.e. $S=-\Omega$ ) in all runs. All numbers are given for the kinematic state.

Source LaTeX | All tables | In the text

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