1973
DOI: 10.1086/151862
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A Linear Nonadiabatic Analysis of Radial Oscillations in Models for Beta Cephei Stars

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Cited by 15 publications
(7 citation statements)
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“…With M * = 14.2 ± 0.4 M⊙, R * = 7.9 ± 0.6 R⊙, and the theoretical value Q = 0.035 (Davey 1973;Stothers 1976), this yields P fun = 0.18 ± 0.02 d, very close to the true pulsation period P ∼ 0.21 d. If the actual pulsation period is used to calculate Q, we obtain Q = P fun √ ρ = 0.041 ± 0.003.…”
Section: Fig 8 Shows ξmentioning
confidence: 91%
“…With M * = 14.2 ± 0.4 M⊙, R * = 7.9 ± 0.6 R⊙, and the theoretical value Q = 0.035 (Davey 1973;Stothers 1976), this yields P fun = 0.18 ± 0.02 d, very close to the true pulsation period P ∼ 0.21 d. If the actual pulsation period is used to calculate Q, we obtain Q = P fun √ ρ = 0.041 ± 0.003.…”
Section: Fig 8 Shows ξmentioning
confidence: 91%
“…However, regarding heat-driven pulsations, the matter of whether a given period P might be due to pressure or gravity modes can even be more quantitatively evaluated with the associated value of the pulsation constant Q = P (M/M )/(R/R ) 3 . The pulsation constant is of the order of 0.033 − 0.042 d for the radial fundamental mode (Davey 1973;Lesh & Aizenman 1974;Fitch 1981;Stankov & Handler 2005), such that any value above this is indicative of gravity modes, while values below this correspond to pressure modes. For a (45M , 36R ) star, Q 0.03P, meaning that heat-driven p modes are expected to have periods shorter than ∼1 d for such stars, whereas periods longer than ∼1 d are likely to be those of g modes.…”
Section: Origin Of the Light Variationsmentioning
confidence: 99%
“…The results for P and its mass dependence are in good agreement with the estimates of Eggleton and Percy (1973). The periods of the 15 My model are the same as those found by Davey (1973).…”
Section: -32 4-30 Logtementioning
confidence: 57%