1994A&AS..105..447H


Query : 1994A&AS..105..447H

1994A&AS..105..447H - Astron. Astrophys., Suppl. Ser., 105, 447-480 (1994/June-2)

A photometric study of β Cephei stars. II. Determination of the degrees l of pulsation modes.

HEYNDERICKX D., WAELKENS C. and SMEYERS P.

Abstract (from CDS):

The wavelength dependence of photometric amplitudes is used as a means of identifying the degrees l of pulsation modes of β Cephei stars studied in an earlier paper. To this end, an expression for the photometric amplitude of a non-rotating pulsating star is derived in terms of the wavelength of the radiation received and the degree of the pulsation mode involved. The derivation differs from earlier derivations in that the specific radiation intensity is considered instead of the outward normal radiation flux. Furthermore, the effects of the non-radial components of the Lagrangian displacement on the local surface element of the star are taken into account. The angular dependence of the specific radiation intensity is determined by a limb-darkening function. The relative Lagrangian perturbation of the specific radiation intensity is set equal to the relative Lagrangian perturbation of the outward normal radiation flux. The physical parameters of the β Cephei stars are estimated by means of calibrations of photometric systems. From a comparison of the calibrations of the Walraven, the Geneva, and the Stroemgren system for early-type stars, it appears that the most reliable values are obtained by means of the Walraven system. The influence of the uncertainties on the physical parameters on the determination of the degrees l of pulsation modes in β Cephei stars is examined. The expression for the photometric amplitude of a pulsating star is used for the determination of the degree l of a pulsation mode by fitting curves of the wavelength dependences of theoretical photometric amplitudes for various degrees l to the wavelength dependence of observationally determined photometric amplitudes. In this way, values for the degrees l of most of the pulsation modes of the β Cephei stars considered are found. It appears that not all β Cephei stars pulsate in at least one radial mode and that multiperiodic β Cephei stars pulsate in a variety of combinations of pulsation modes.

Abstract Copyright:

Journal keyword(s): stars: early-type - stars: fundamental parameters - Hertzsprung-Russell (HR) diagram - stars: oscillations - stars: variables: other

Simbad objects: 62

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Number of rows : 62
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 * gam Peg bC* 00 13 14.1523490172 +15 11 00.954346538 1.75 2.61 2.84 2.94 3.13 B2IV 693 0
2 * del Cet bC* 02 39 28.9568473856 +00 19 42.631195332 2.97 3.85 4.07     B2IV 380 0
3 V* KP Per bC* 03 32 38.9776919424 +44 51 20.734775568 5.7 6.44 6.41     B2IV 129 0
4 * nu. Eri bC* 04 36 19.1419185396 -03 21 08.857744927 2.82 3.737 3.928     B2III 390 0
5 * bet CMa bC* 06 22 41.9853527 -17 57 21.307352 0.77 1.73 1.97 2.11 2.35 B1II-III 715 0
6 * ksi01 CMa bC* 06 31 51.3662820799 -23 25 06.319934859 3.10 4.09 4.33 4.45 4.72 B0.7IV 322 0
7 * 15 CMa bC* 06 53 32.9069226414 -20 13 27.309395177 3.66 4.62 4.83 4.95 5.17 B1IV 209 0
8 * 19 Mon bC* 07 02 54.7772531316 -04 14 21.235613879 3.87 4.80 5.00 5.06 5.25 B2Vn(e) 197 0
9 V* V350 Pup bC* 07 30 34.0740522576 -34 05 26.146528476 6.7 7.55 7.62     B1/2Ib/II 44 0
10 V* PT Pup bC* 07 36 41.0352383592 -19 42 08.425020168 4.65 5.524 5.699     B2III 147 0
11 V* QS Pup bC* 07 49 12.8625152304 -46 51 27.787514724 4.82 5.662 5.805     B2III 72 0
12 V* QU Pup bC* 07 51 40.3580164320 -42 53 17.533822092 4.98 5.847 6.032     B2III 58 0
13 V* V372 Car bC* 07 52 29.7416381280 -54 22 01.788879000 4.64 5.529 5.680     B2IV 78 0
14 V* IS Vel bC* 08 09 43.1541985440 -47 56 13.890437304 4.12 5.017 5.217     B2V 87 1
15 V* KK Vel bC* 09 07 42.5207085395 -44 37 56.750000545 6.03 6.76 6.80     B2II/III 65 0
16 V* IL Vel bC* 09 17 31.1516725008 -52 50 19.476373704 8.51 9.13 9.16     B2III 39 0
17 HD 90288 bC* 10 23 56.9130221208 -57 27 52.421282964 7.05 8.02 8.17     B2III/IV 39 0
18 V* V400 Car bC* 10 34 48.6840712008 -58 09 01.177020288 8.93 9.75 9.66 10.02 11.681 OB 55 0
19 V* V401 Car bC* 10 35 30.0530262192 -58 12 08.180867304 8.83 9.57 9.50 9.89 9.36 B5 59 0
20 V* V403 Car bC* 10 35 40.7035044864 -58 12 44.280907776 7.93 8.75 8.73 9.48 8.65 B1III 55 1
21 CD-57 3347 bC* 10 35 43.2986203224 -58 13 33.642743412 9.13 9.88 9.85 9.76 9.67 B1.5III 38 0
22 V* V405 Car s*b 10 35 48.2142075456 -58 12 33.202086660 8.35 9.234 9.242 9.772 9.19 B0Iab 60 0
23 MCW 1182 bC* 10 35 48.2508447536 -58 14 16.579582539 8.36 9.37 9.23 9.26 9.21 B2.5V 34 0
24 NGC 3293 OpC 10 35 52.8 -58 13 52           ~ 312 0
25 CPD-57 3517 Pu* 10 35 53.6409550056 -58 14 47.852298744 8.44 9.26 9.22 9.13 9.05 B1V 40 0
26 V* V406 Car bC* 10 35 57.8106305760 -58 12 21.308777280 8.39 9.22 9.26 9.24 9.20 B1V 42 0
27 V* V379 Car bC* 10 35 58.4856856776 -58 14 15.020184408 7.46 8.45 8.30 9.27 8.34 B1III 45 1
28 HD 92007 Pu* 10 36 01.5932715912 -58 15 09.587110032 8.26 9.00 8.92 9.57 8.74 B1III 70 0
29 HD 92024 Pu* 10 36 08.3339354160 -58 13 04.358647920 8.11 8.90 9.00 9.63 8.94 B1III 67 0
30 * bet Cru bC* 12 47 43.26877 -59 41 19.5792 0.03 1.02 1.25 1.38 1.64 B1IV 342 1
31 NGC 4755 OpC 12 53 39.6 -60 22 16           ~ 289 0
32 CPD-59 4564 bC* 12 53 57.5386794336 -60 24 58.092625152 8.45 9.12 9.06 9.64   B2III 62 0
33 V* V856 Cen bC* 12 57 36.2574706704 -49 46 50.094145848 7.66 8.36 8.33     B2II/III 44 0
34 * alf Vir bC* 13 25 11.57937 -11 09 40.7501 -0.20 0.74 0.97 1.06 1.30 B1V 855 2
35 * eps Cen bC* 13 39 53.25774 -53 27 59.0081 1.16 2.08 2.30 2.45 2.70 B1III 250 0
36 * bet Cen bC* 14 03 49.40535 -60 22 22.9266     0.58     B1III 361 0
37 * tau01 Lup bC* 14 26 08.2244287979 -45 13 17.123883210 3.68 4.393 4.553     B2IV 152 0
38 * alf Lup bC* 14 41 55.7557866 -47 23 17.515486 1.22 2.126 2.286     B1.5III 237 0
39 V* BU Cir bC* 14 45 10.9595976864 -55 36 05.906309508 5.23 6.016 6.089     B2III 97 0
40 V* V836 Cen bC* 14 46 25.7601403800 -37 13 20.082887904 7.04 7.88 8.05     B2 114 0
41 * del Lup bC* 15 21 22.3138254072 -40 38 51.109328940 2.12 2.995 3.190     B1.5IV 220 0
42 V* V349 Nor bC* 16 15 26.4194409792 -52 55 14.518386840 8.34 8.921 8.770     B2II/III 34 0
43 * sig Sco bC* 16 21 11.3157134 -25 35 34.051476 2.32 3.02 2.89 1.69 1.58 B1III+B1:V 870 0
44 HD 147985 bC? 16 26 56.7425350368 -43 47 57.155390448 7.45 8.03 7.92     B1/2II/III 33 0
45 V* V945 Sco bC* 16 53 54.5203569984 -41 52 14.960561412 9.090 9.745 9.575 9.618 9.260 B1V 43 0
46 V* V1032 Sco bC* 16 53 58.6055666592 -41 48 41.790648132 9.327 9.920 9.767 9.811 9.445 B2V 41 0
47 V* V946 Sco bC* 16 54 01.7631666120 -41 51 11.868345252 9.890 10.471 10.281 10.327 9.927 B2IV-V 47 0
48 NGC 6231 OpC 16 54 10.8 -41 48 43           ~ 538 0
49 V* V964 Sco bC* 16 54 18.3200772432 -41 51 35.651104416 9.126 9.776 9.603 9.61 9.290 B0.5V 59 0
50 V* V947 Sco bC* 16 54 36.0500878224 -41 53 38.119259292 9.45 10.06 9.78 10.06   B1V 52 0
51 CPD-41 7755 Y*? 16 54 39.8785805856 -41 53 38.480359596 9.675 10.273 10.068 11.4 9.705 B1V 38 0
52 V* V920 Sco bC* 16 54 43.1657949576 -41 49 35.456774916 9.153 9.795 9.601 9.95 9.256 B1V 65 0
53 HD 156662 bC? 17 21 06.0895034592 -45 58 55.615119960 7.35 9.15 9.13 8.70   B2III 36 0
54 * tet Oph bC* 17 22 00.5793468 -24 59 58.366974 2.18 3.03 3.26 3.38 3.58 OB 332 0
55 * lam Sco bC* 17 33 36.52012 -37 06 13.7648 0.52 1.49 1.63     B2IV+DA7.9 391 0
56 * kap Sco bC* 17 42 29.27520 -39 01 47.9391 1.32 2.211 2.386     B1.5III 241 0
57 V* V2052 Oph bC* 17 56 18.4001168880 +00 40 13.273317228 5.28 5.874 5.820     B3III 214 0
58 V* BW Vul bC* 20 54 22.3947588600 +28 31 19.190976132 5.47 6.40 6.54     B2IIIv 295 0
59 * bet Cep bC* 21 28 39.5968513 +70 33 38.574681 2.05 3.01 3.23 3.33 3.55 B0.5IIIs 725 0
60 V* HN Aqr bC* 22 37 38.2846689672 -18 39 51.268772880   11.293 11.426 11.813   B 67 0
61 * 12 Lac bC* 22 41 28.6495065456 +40 13 31.609736580 4.24 5.080 5.229     B2III 357 0
62 * 16 Lac bC* 22 56 23.6299283136 +41 36 13.948480440 4.61 5.436 5.587     B2IV 314 0

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