Table 3: M₁, R₁, the factor $\phi$ = (R₁/M₁)/(R_1o/M_1o), the post-1967 mass accretion rate $\dot{M}$ (for $L_{\rm disk}$ = 70 $L_{\odot }$ ), the ignition mass, and the recurrence time $\tau$ = $M_{\rm ign}$ / $\dot{M}$ (see Sect. 8).
M₁ R₁ $\phi$ $\dot{M}$ $M_{\rm ign}$ $\tau$

( $M_{\odot }$ ) (10^-3 $R_{\odot}$ ) (10^-8 $M_{\odot }$ yr^-1) (10^-7 $M_{\odot }$ ) (yrs)

1.00 8.10 1.000 3.66 108.78 297.2

1.05 7.63 0.897 3.28 92.88 283.2

1.10 7.10 0.797 2.92 77.75 266.3

1.15 6.51 0.699 2.56 63.32 247.3

1.20 5.85 0.602 2.20 49.19 223.6

1.25 5.14 0.508 1.86 35.21 189.3

1.30 4.35 0.413 1.51 22.22 147.1

1.33 3.85 0.357 1.31 14.78 112.8

1.35 3.51 0.321 1.17 10.35 88.5

1.36 3.33 0.302 1.11 8.26 74.4

1.37 3.15 0.284 1.04 6.35 61.1

1.38 2.96 0.265 0.97 4.61 47.5

1.39 2.78 0.247 0.90 3.06 34.0

1.40 2.60 0.229 0.84 1.78 21.2

**Table 3:** M₁, R₁, the factor $\phi$ = (R₁/M₁)/(R_1o/M_1o), the post-1967 mass accretion rate $\dot{M}$ (for $L_{\rm disk}$ = 70 $L_{\odot }$ ), the ignition mass, and the recurrence time $\tau$ = $M_{\rm ign}$ / $\dot{M}$ (see Sect. 8).
M₁	R₁	$\phi$	$\dot{M}$	$M_{\rm ign}$	$\tau$
( $M_{\odot }$ )	(10^-3 $R_{\odot}$ )		(10^-8 $M_{\odot }$ yr^-1)	(10^-7 $M_{\odot }$ )	(yrs)
1.00	8.10	1.000	3.66	108.78	297.2
1.05	7.63	0.897	3.28	92.88	283.2
1.10	7.10	0.797	2.92	77.75	266.3
1.15	6.51	0.699	2.56	63.32	247.3
1.20	5.85	0.602	2.20	49.19	223.6
1.25	5.14	0.508	1.86	35.21	189.3
1.30	4.35	0.413	1.51	22.22	147.1
1.33	3.85	0.357	1.31	14.78	112.8
1.35	3.51	0.321	1.17	10.35	88.5
1.36	3.33	0.302	1.11	8.26	74.4
1.37	3.15	0.284	1.04	6.35	61.1
1.38	2.96	0.265	0.97	4.61	47.5
1.39	2.78	0.247	0.90	3.06	34.0
1.40	2.60	0.229	0.84	1.78	21.2

Source LaTeX | All tables | In the text