2004
DOI: 10.1017/s0252921100011131
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Non-adiabatic Asteroseismology of Near-Main Sequence Variable Stars

Abstract: Abstract. We present in this talk a new linear non-adiabatic pulsation code: MAD 1 . We detail all the possible applications of it in the frame of asteroseismology. By using it, photospheric observables such as multi-color photometric amplitude ratios, phase differences and line profile variations can be determined accurately and confronted with observations. Moreover, MAD enables the precisely analysis of the excitation mechanisms of pulsating stars. Non-adiabatic asteroseismologyIn the superficial layers of… Show more

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Cited by 3 publications
(3 citation statements)
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“…As a first step to understand the theoretical pulsational spectrum of δ Scuti stars, we show the evolution of pulsational frequencies of l = 0, 1, 2 modes of a 1.8M ⊙ star from Zero Age Main Sequence (ZAMS) to post-MS phases in Figures 14 and 15. A similar diagram can be found in Dupret (2002). These modes suffer from less cancellation effect in broadband photometry like Kepler and thus are most likely to be observed.…”
Section: Interpretation Of Pulsationssupporting
confidence: 66%
“…As a first step to understand the theoretical pulsational spectrum of δ Scuti stars, we show the evolution of pulsational frequencies of l = 0, 1, 2 modes of a 1.8M ⊙ star from Zero Age Main Sequence (ZAMS) to post-MS phases in Figures 14 and 15. A similar diagram can be found in Dupret (2002). These modes suffer from less cancellation effect in broadband photometry like Kepler and thus are most likely to be observed.…”
Section: Interpretation Of Pulsationssupporting
confidence: 66%
“…The modal surface effect stems from the fact that oscillation frequencies of stars are computed under the assumption of adiabaticity, which does not hold true in the near-surface layers (e.g. Dupret 2004;Christensen-Dalsgaard 2008;Townsend & Teitler 2013;Grosjean et al 2014). Moreover, the contribution from turbulent pressure, i.e.…”
mentioning
confidence: 99%
“…We adopted the AGS05 metal mixture (Asplund et al 2005), the corresponding OP opacity tables (Badnell et al 2005), X = 0.070 and Z = 0.014 and a convective core overshooting of 0.1. Non-adiabatic computations have been performed with MAD (Dupret 2002), in which the traditional approximation for rotation has been implemented (Bouabid et al 2013) to perform modes for 1 l 4. The efficiency of wave leakage (given by the integral over the surface of the wave kinetic energy) should increase with the rotation as the critical frequency increases.…”
Section: Stellar and Pulsational Modelsmentioning
confidence: 99%