The Size, Structure, and Variability of Late-Type Stars Measured ...
The Size, Structure, and Variability of Late-Type Stars Measured ...
The Size, Structure, and Variability of Late-Type Stars Measured ...
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34<br />
Mira.<br />
Finally, variations in time <strong>of</strong> stellar features have been seen in several stars from<br />
repeated measurements using a single instrument. Gray (2000) [35] reports non-regular<br />
changes occuring in the spectrum <strong>of</strong> α Ori on time scales ranging from days to years.<br />
Changes in the brightness distribution <strong>of</strong> α Ori over a period <strong>of</strong> 22 months have been observed<br />
by Wilson et al. (1992) [111]. Karovska et al. (1991) [56] have seen changes in the size<br />
<strong>and</strong> asymmetry in o Cet over the course <strong>of</strong> a year. A phase-related change in size by 35% <strong>of</strong><br />
some <strong>of</strong> the atmospheric layers <strong>of</strong> R Leo was reported by Burns et al. (1998) [19]. In contrast,<br />
radio measurements <strong>of</strong> flux density for o Cet <strong>and</strong> R Leo by Reid <strong>and</strong> Menten (1997) [84]<br />
show no variability in the “radio photospheres” <strong>of</strong> these stars (around 2R ∗ ) indicating that<br />
outwardly propagating pulsational disturbances must be damped by some mechanism before<br />
reaching 2R ∗ .<br />
3.2 Dust<br />
<strong>The</strong> cool temperatures <strong>and</strong> relatively high densities in the circumstellar environment<br />
<strong>of</strong> these AGB stars can lead to the precipitation <strong>of</strong> small solids. <strong>The</strong>se sub-micron<br />
sized particles made up <strong>of</strong> carbon or oxides are collectively known as dust. <strong>The</strong> carbon<br />
monoxide molecule, having a strong binding energy, is readily formed in the atmospheres<br />
<strong>of</strong> stars. <strong>The</strong> formation <strong>of</strong> this molecule occurs until almost all <strong>of</strong> the limiting reactant,<br />
carbon or oxygen, is bound. <strong>The</strong> result is that stars with a slight carbon overabundance<br />
end up with no free oxygen in the cool regions <strong>of</strong> its atmosphere, <strong>and</strong> its dust is made up<br />
entirely <strong>of</strong> amorphous carbon particles <strong>and</strong> graphites. Conversely, O-rich stars, such as all<br />
<strong>of</strong> the stars we’re considering, are surrounded by dust shells made up <strong>of</strong> oxides <strong>of</strong> Si, Mg,<br />
Ti, Al, S, Fe, etc.<br />
<strong>The</strong> optical properties <strong>of</strong> the dust are somewhat dependent on the chemistry <strong>and</strong><br />
distribution <strong>of</strong> grain sizes. Measurements <strong>of</strong> laboratory-formed dust have been performed<br />
<strong>and</strong> compared with astronomical data. Martin <strong>and</strong> Rogers (1987) [67] describe some models<br />
for carbon dust compared with spectral observations <strong>of</strong> the carbon star IRC+10216.<br />
Suh (1999) [96] presents the optical properties <strong>of</strong> silicate dust <strong>and</strong> data supporting the<br />
conclusion that silicates are the dominant form <strong>of</strong> dust in O-rich AGB stars. <strong>The</strong> same conclusion<br />
is reached in Danchi et al. (1994) [22] for the five stars considered here. Figure 3.1<br />
reproduces Figure 1 from Suh (1999) [96] comparing the absorptivity <strong>of</strong> 0.1 µm silicate dust