Table 2: Parametrisation of the initial magnetic fields for the models of series AaBbGg-DdMm by the radius of the field generating current loop centered at $r_{{\rm mag}}$ (parametrized by d = 1, 2, 3, 4, 0) and the field strength in the core's center $B_0=\sqrt {4\pi }b_0$ (parametrized by m = 10, 11, 12, 13). For models AaBbGg-D0Mm the field generating current loop is located at infinity yielding a uniform magnetic field throughout the entire core.
Model $r_{{\rm mag}} \ [{\rm km}]$ Model $b_0 \ [{\rm G}]$

D1 100 M10 10¹⁰

D2 200 M11 10¹¹

D3 400 M12 10¹²

D4 800 M13 10¹³

D0 $\infty$

**Table 2:** Parametrisation of the initial magnetic fields for the models of series AaBbGg-DdMm by the radius of the field generating current loop centered at $r_{{\rm mag}}$ (parametrized by d = 1, 2, 3, 4, 0) and the field strength in the core's center $B_0=\sqrt {4\pi }b_0$ (parametrized by m = 10, 11, 12, 13). For models AaBbGg-D0Mm the field generating current loop is located at infinity yielding a uniform magnetic field throughout the entire core.
Model	$r_{{\rm mag}} \ [{\rm km}]$	Model	$b_0 \ [{\rm G}]$
D1	100	M10	10¹⁰
D2	200	M11	10¹¹
D3	400	M12	10¹²
D4	800	M13	10¹³
D0	$\infty$

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