An effective model for magnetic field amplification by the magnetorotational and parasitic instabilities

Open Access

Table C.2.

Same as Table C.1, but using now a shear parameter q = 1.25 and different initial amplitudes to make a better comparison with the results from Rembiasz et al. (2016b).

NAME	B₀[10⁻³]	v₀[10⁻³]	q	$k_{h}^{ini}$ $k_{\mathrm{h}}^{\mathrm{ini}}$	θⁱⁿⁱ [° ]	$k_{h}^{sat}$ $k_{\mathrm{h}}^{\mathrm{sat}}$	θ^sat [° ]	t_sat [Orbits]	𝒜
`b0vl-dvl-q125`	3.33	0.112	1.25	3.76	176.76	0.65	19.16	2.613	47.69
`b0vl-dl-q125`	3.33	0.370	1.25	4.13	176.70	0.74	18.84	2.584	42.61
`b0vl-dm-q125`	3.33	1.12	1.25	4.13	176.70	0.69	20.22	2.557	38.24
`b0vl-dh-q125`	3.33	3.70	1.25	4.51	176.66	0.75	20.40	2.525	33.73
`b0vl-dvh-q125`	3.33	11.2	1.25	3.51	176.53	0.69	17.90	2.491	29.54
`b0l-dvl-q125`	11.1	0.112	1.25	3.88	176.31	0.69	21.15	2.303	47.16
`b0l-dl-q125`	11.1	0.370	1.25	3.38	176.19	0.69	19.16	2.276	42.54
`b0l-dm-q125`	11.1	1.12	1.25	3.38	176.19	0.64	20.44	2.252	38.59
`b0l-dh-q125`	11.1	3.70	1.25	3.88	176.13	0.74	20.72	2.216	33.57
`b0l-dvh-q125`	11.1	11.2	1.25	3.01	175.95	0.68	18.28	2.183	29.48
`b0m-dvl-q125`	33.3	0.112	1.25	2.76	175.58	0.67	18.62	2.026	47.45
`b0m-dl-q125`	33.3	0.370	1.25	2.88	175.53	0.69	18.91	1.999	42.67
`b0m-dm-q125`	33.3	1.12	1.25	3.01	175.47	0.72	19.27	1.973	38.51
`b0m-dh-q125`	33.3	3.70	1.25	3.14	175.43	0.73	19.98	1.941	34.11
`b0m-dvh-q125`	33.3	112	1.25	2.38	175.19	0.65	17.93	1.906	29.60
`b0h-dvl-q125`	111	0.112	1.25	2.26	174.61	0.66	18.89	1.720	47.66
`b0h-dl-q125`	111	0.370	1.25	2.39	174.59	0.66	19.93	1.695	43.21
`b0h-dm-q125`	111	1.12	1.25	2.39	174.59	0.62	21.16	1.673	39.59
`b0h-dh-q125`	111	3.70	1.25	2.64	174.29	0.80	19.19	1.639	34.65
`b0h-dvh-q125`	111	112	1.25	2.01	173.94	0.70	17.60	1.600	29.72
`b0vh-dvl-q125`	333	0.112	1.25	2.27	173.35	0.76	20.15	1.438	47.25
`b0vh-dl-q125`	333	0.370	1.25	2.27	173.35	0.71	21.59	1.413	42.81
`b0vh-dm-q125`	333	1.12	1.25	2.02	172.88	0.76	19.14	1.385	38.40
`b0vh-dh-q125`	333	3.70	1.25	2.02	172.88	0.70	20.88	1.352	33.71
`b0vh-dvh-q125`	333	11.2	1.25	2.14	172.63	0.78	20.71	1.321	29.77

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