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Table 2
Results of a nonadiabatic study to match predicted mode instability with the observed frequencies.
Opacity | X | Z | Mass [M⊙] | log Teff | log L/L⊙ | Frequency range [d-1] | Frequency [d-1] |
with η > 0 | of ηmax | ||||||
|
|||||||
OPAL | 0.76 | 0.0134 | – | – | – | – | – |
OPAL | 0.74 | 0.0134 | 1.576 | 3.874 | 0.757 | 16.8–55.3 | 23.3 |
OPAL | 0.72 | 0.0134 | 1.604 | 3.894 | 0.844 | 24.6–54.4 | 37.8 |
OPAL | 0.70 | 0.0134 | 1.623 | 3.911 | 0.915 | 38.2–61.0 | 52.5 |
OPAL | 0.68 | 0.0134 | 1.615 | 3.921 | 0.951 | 42.5–68.0 | 56.3 |
OPAL | 0.65 | 0.0134 | 1.599 | 3.928 | 0.979 | 45.3–72.9 | 60.1 |
OPAL | 0.74 | 0.0160 | – | – | – | – | – |
OPAL | 0.74 | 0.0140 | 1.683 | 3.897 | 0.868 | 30.4–54.8 | 41.8 |
OPAL | 0.74 | 0.0120 | 1.646 | 3.902 | 0.880 | 34.3–55.7 | 45.2 |
OPAL | 0.74 | 0.0100 | 1.698 | 3.927 | 0.991 | – | 60.0 |
OPAL | 0.74 | 0.0008 | 1.718 | 3.945 | 1.069 | – | 67.4 |
OPAL | 0.70 | 0.0160 | – | – | – | – | – |
OPAL | 0.70 | 0.0140 | 1.604 | 3.903 | 0.878 | 30.5–57.3 | 45.2 |
OPAL | 0.70 | 0.0120 | 1.647 | 3.925 | 0.974 | 47.6–68.3 | 60.1 |
OPAL | 0.70 | 0.0100 | 1.662 | 3.941 | 1.039 | 56.8–74.4 | 67.4 |
OPAL | 0.70 | 0.0008 | 1.670 | 3.956 | 1.102 | 69.3–75.4 | 71.2 |
OP | 0.74 | 0.0134 | 1.631 | 3.889 | 0.827 | 21.7–54.8 | 35.4 |
OP | 0.74 | 0.010 | 1.741 | 3.936 | 1.034 | – | 63.8 |
OP | 0.70 | 0.010 | 1.695 | 3.947 | 1.071 | 60.8–75.1 | 67.4 |
OP | 0.70 | 0.011 | 1.694 | 3.941 | 1.045 | 56.3–73.4 | 67.4 |
|
|||||||
observed | 59.9–71.1 | 67.6 |
Notes. All models fit the four frequency groups following hypothesis 2 and were obtained with the A09 element mixture adopting Vrot = 15.0 km s-1.
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