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Astron. Astrophys. 317, 121-124 (1997) 1. IntroductionAn important property of red giants and AGB stars is that they have
strong stellar winds. The rates of mass loss due to stellar winds have
the values of
(i) AGB stars may go through a phase of large amplitude radial pulsations, which may strongly enhance the mass loss rate (Wilson and Hill 1979; Wood 1979,1981; Wood et al.1983). (ii) Pulsational models of AGB stars suggest that superwind might be caused by switching of pulsation from the first overtone to the fundamental mode, perhaps giving rise to sporadic episodes of mass ejection (Wood 1974;Tuchman et al.1979). (iii) Pulsation-radiation pressure can induce envelope ejection (Wannier 1984; Wilson and Kowalsky 1987; de Jager and Nieuwenhuijzen 1988; Wood and Vassiliadis 1992; Feast 1992; Vassiliadis and Wood 1992). Furthermore, superwind can be caused by large-scale instabilities occurring on dynamical time scales(Lucy 1967; Paczynski and Ziolkowski 1968; Han et al.1994). In all the above investigations the contribution of turbulent pressure is neglected. However, if the turbulent pressure becomes important in the convective envelopes of red giants and AGB stars, the effect of turbulent pressure can cause not only a change in the internal structure, but also dynamical instabilities in the regions close to the surfaces which may affect mass ejection outwards. The purpose of this paper is to investigate the mechanism driving strong stellar winds from the red giants and the AGB stars. In order to understand the occurrence of dynamical instabilities in the convective envelopes,we present at first a criterion for the dynamical instability. Using this criterion we discuss whether dynamical instabilities can occur or not in the regions close to the surfaces of these stars, which finally affect the mass ejection outwards. © European Southern Observatory (ESO) 1997 |