**Table 1:** Basic model properties: sequence number, $M_{\rm init}$ : initial mass, Z: metallicity, $\dot M_{{\rm WR}}$ : option for the WR wind mass loss rate, $f_{\rm K}$ : initial rotational velocity in units of the Keplerian value, $V_{\rm init}/V_{\rm crit}$ : the ratio of the initial rotational velocity to the critical velocity at the equator (Eq. (4)), $Y_{\rm s, H-end}$ : surface helium abundance at core hydrogen exhaustion, $M_{\rm final}$ : final mass, $M_{\rm CO}$ : CO core mass at core carbon exhaustion, $J_{\rm init}$ : initial angular momentum, $J_{\rm final}$ : final angular momentum, $j_{3~M_\odot}$ : mean specific angular momentum in the innermost $3~{M}_\odot$ , $X_{\rm N, max}$ : maximum nitrogen surface mass fraction during the evolution.
No.	$M_{\rm init}$	Z	$\dot M_{{\rm WR}}$	$V_{\rm init}$	$f_{\rm K}$	$V_{\rm init}/V_{\rm crit}$	$Y_{\rm s, H-end}$	$M_{\rm final}$	$M_{\rm CO}$	$J_{\rm init}$	$J_{\rm final}$	$j_{3~M_\odot}$	$X_{\rm N, max}$
	[ ${M_\odot}$ ]			[ ${\rm km~s^{-1}}$ ]				[ ${M_\odot}$ ]	[ ${M_\odot}$ ]	[10⁵¹	[10⁵¹	[10¹⁵
										erg s]	erg s]	${\rm cm^2~s^{-1}}$ ]
A1	20	10^-5	WR1	479	0.5	0.56	0.94	16.40	9.48	46.92	3.79	2.50	$2.6\times 10^{-6}$
A2	30	10^-5	WR1	501	0.5	0.58	0.94	24.13	18.80	98.80	8.40	10.57	$1.3\times 10^{-2}$
A3	40	10^-5	WR1	230	0.2	0.25	0.27	39.84	7.08	73.58	65.36	0.90	$4.2\times 10^{-6}$
A4	40	10^-5	WR1	555	0.5	0.60	0.94	31.77	25.23	166.21	12.57	12.57	$1.4\times 10^{-2}$
A5	50	10^-5	WR1	583	0.5	0.64	0.94	39.21	33.68	247.54	19.03	13.75	$3.2\times 10^{-2}$
A6	60	10^-5	WR1	605	0.5	0.63	0.94	46.50	40.25	341.70	23.55	13.41	$2.8\times 10^{-2}$
B1	40	0.001	WR1	479	0.5	0.63	0.90	13.52	10.70	183.97	0.21	0.82	$6.7\times 10^{-4}$
B2^*	40	0.02	WR1	408	0.5	0.69	0.69	20.25	-	166.40	1.505	3.30	$1.3\times 10^{-2}$
C1	40	0.001	WR2	479	0.5	0.63	0.96	25.71	21.23	183.97	8.94	12.92	$3.3\times 10^{-3}$
C2	60	0.001	WR2	522	0.5	0.67	0.96	34.59	30.18	378.32	10.12	9.88	$6.7\times 10^{-4}$

^* sequence ends at core hydrogen exhaustion.

Source LaTeX | All tables | In the text