TY - JOUR
T1 - Optically thick winds from degenerate dwarfs. I. Classical novae of populations I and II
AU - Kato, Mariko
PY - 1997/11
Y1 - 1997/11
N2 - Twenty-six sequences of optically thick wind solutions have been calculated that mimic time-dependent evolution of classical novae of Populations I and II. The peak of the new opacity around log T = 5.2 due to iron lines is found to be strong enough to accelerate the winds even when the iron abundance is very low such as Z = 0.001 for massive white dwarfs (≥0.8 M⊙). The old population novae show a slow light curve, a long X-ray turnoff time, a small expansion velocity, and a small wind mass-loss rate. The X-ray turnoff time is a good indicator of the white dwarf mass because of its strong dependence on the white dwarf mass and weak dependence on the populations. The white dwarf mass is estimated to be ∼0.6 M⊙ for GQ Mus and ∼1.0 M⊙ for V1974 Cyg. A systematic difference of the wind velocity is predicted between novae in globular clusters and in the galactic disk. Twenty-six tables are presented in computer-readable form on CD-ROM that consist of the optically thick wind solutions and the static solutions for the decay phase of classical novae with composition of X = 0.35, C = 0.1, and O = 0.2 and heavy element content Z = 0.001, 0.004, 0.02, 0.05, and 0.1 for white dwarf masses of 0.4, 0.6, 0.7, 0.8, 0.9, 1.0, 1.2, and 1.35 M⊙. These tables list characteristic values of the envelope such as the photospheric temperature, the velocity, the wind mass-loss rate, and fluxes of four wavelength bands. The updated OPAL opacity is used.
AB - Twenty-six sequences of optically thick wind solutions have been calculated that mimic time-dependent evolution of classical novae of Populations I and II. The peak of the new opacity around log T = 5.2 due to iron lines is found to be strong enough to accelerate the winds even when the iron abundance is very low such as Z = 0.001 for massive white dwarfs (≥0.8 M⊙). The old population novae show a slow light curve, a long X-ray turnoff time, a small expansion velocity, and a small wind mass-loss rate. The X-ray turnoff time is a good indicator of the white dwarf mass because of its strong dependence on the white dwarf mass and weak dependence on the populations. The white dwarf mass is estimated to be ∼0.6 M⊙ for GQ Mus and ∼1.0 M⊙ for V1974 Cyg. A systematic difference of the wind velocity is predicted between novae in globular clusters and in the galactic disk. Twenty-six tables are presented in computer-readable form on CD-ROM that consist of the optically thick wind solutions and the static solutions for the decay phase of classical novae with composition of X = 0.35, C = 0.1, and O = 0.2 and heavy element content Z = 0.001, 0.004, 0.02, 0.05, and 0.1 for white dwarf masses of 0.4, 0.6, 0.7, 0.8, 0.9, 1.0, 1.2, and 1.35 M⊙. These tables list characteristic values of the envelope such as the photospheric temperature, the velocity, the wind mass-loss rate, and fluxes of four wavelength bands. The updated OPAL opacity is used.
KW - Novae, cataclysmic variables
KW - Stars: Evolution
KW - Stars: Interiors
KW - Stars: Mass loss
KW - Stars: Population II
KW - White dwarfs
KW - X-rays: Stars
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U2 - 10.1086/313047
DO - 10.1086/313047
M3 - Article
AN - SCOPUS:0042597513
SN - 0067-0049
VL - 113
SP - 121
EP - 129
JO - Astrophysical Journal, Supplement Series
JF - Astrophysical Journal, Supplement Series
IS - 1
ER -