1989
DOI: 10.1086/132551
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Non-LTE effects in streams, and mass-transfer rates in three eclipsing binaries

Abstract: A mass-transferring stream in an eclipsing binary is seen in projection against the hot star in roughly the quarter-period before primary eclipse. At this time a small fraction of the light of the hot star is blocked by the stream, depressing light curves slightly. We discuss five-color observations of such light curves in AQ Cas, RZ Set, and U Sge. We compare non-LTE and LTE predictions of stream-produced light losses with these observations, discuss the validity of this mechanism, and estimate mass-transfer … Show more

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Cited by 9 publications
(14 citation statements)
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“…If this amount of gas is accreted each orbital cycle, then the mass transfer rate needed to maintain this disk is yr~1. M 0^9 ] 10~10 M _ This mass transfer rate is D44 times lower than the value calculated by Olson & Bell (1989) from the photometric absorption attributed to the gas stream between phases 0.80È0.95. Alternatively, if we assumed that most of the gas is accreted before it makes one orbit around the primary star and measure the average tangential velocity of the emission peaks (D325 km s~1), then the maximum lifetime of the gas in the disk is D16 hours and the median lifetime is D8 hours.…”
Section: Disk Geometrymentioning
confidence: 66%
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“…If this amount of gas is accreted each orbital cycle, then the mass transfer rate needed to maintain this disk is yr~1. M 0^9 ] 10~10 M _ This mass transfer rate is D44 times lower than the value calculated by Olson & Bell (1989) from the photometric absorption attributed to the gas stream between phases 0.80È0.95. Alternatively, if we assumed that most of the gas is accreted before it makes one orbit around the primary star and measure the average tangential velocity of the emission peaks (D325 km s~1), then the maximum lifetime of the gas in the disk is D16 hours and the median lifetime is D8 hours.…”
Section: Disk Geometrymentioning
confidence: 66%
“…Alternatively, if we assumed that most of the gas is accreted before it makes one orbit around the primary star and measure the average tangential velocity of the emission peaks (D325 km s~1), then the maximum lifetime of the gas in the disk is D16 hours and the median lifetime is D8 hours. The mass transfer rate needed to produce this disk every 8 hours increases to yr~1, M 0 \ 9 ] 10~9 M _ still only 23% of the value calculated by Olson & Bell (1989). Possibly, only a small percentage of the gas in the stream is fed into the disk, and the rest is immediately accreted by the star.…”
Section: Disk Geometrymentioning
confidence: 83%
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“…6. It can be seen that the expected course of the period change foṙ m determined by Olson & Bell (1989) is too small to be unambiguously present in the available data. It is interesting to note that although the parameters and position of AQ Cas in the r−q and P −q diagrams in Fig.…”
Section: Aq Casmentioning
confidence: 86%
“…The mass transfer rateṁ ≈ 5 10 −7 M yr −1 was determined from the photometric manifestations of the mass stream by Olson & Bell (1989). In order to assess how largė m for the conservative transfer (Huang 1963) can be hidden in the scatter of the data parabolic courses for a set ofṁ were computed and are included in Fig.…”
Section: Aq Casmentioning
confidence: 99%