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For binary systems, phased-locked variations can be used to determine some of the basic orbital characteristics such as a value for the inclination, this being very important for resolving the mass function The distribution of scattering material around any system may be established with estimates for the rate of mass loss Schulte-Ladbeck (1989) discussed the importance of knowing the masses of Wolf Rayet binaries in respect of their evolution, and she emphasized the role that polarimetry plays in helping to establish a catalogue of values The appendix of her work provides a summary of 10 such systems For single stars, polarization variability provides information on asymmetries and inhomogeneities (blobs) in the stellar wind As early as 1946, Kopal & Shapley (1946) suggested that the eclipsing Wolf Rayet, V 444 Cyg, was an ideal system for investigation by polarimetry From the light curve, they concluded that the main cause of extinction in the semi-transparent envelope surrounding the WR component is scattering by free electrons, and, in turn, this would produce a small polarized ux best seen several hours before and after primary minimum Monitoring the variation of p should provide an estimate of the proportion of the light scattered, and allow determination of the longitude of the node of the binary system Early polarimetric observations of a WR star were those of McLean, Coyne, Frecker, et al (1979) using a spectral resolution of 50 , revealing that the prominent emission lines of HD 50896 = WR 6 = EZ CMa, a WN5-type star, exhibited ecreases of polarization relative to the continuum The behaviour suggested strati cation of ionization and excitation in the extended atmosphere, with the recombination lines of He II being formed deeper than those of He I, so that the ionization is decreasing outwards The continuum polarization is typical of almost pure electron scattering, suggesting that the envelope must be highly ionized and attened to some degree, or localized Later, McLean (1980) showed that the system had a polarimetric period of 1d 88, this being the second harmonic of the 3d 76 value associated with photometric and spectroscopic modulations Determination of i was made dif cult because of aperiodic instabilities, but a value of 71 was suggested, implying a 13 M companion for the 10 M primary star As a result of a photometric and polarimetric campaign, Drissen, Robert, Lamontagne, et al (1989) found that the shapes of both the light curve and the polarimetric curve changed over 2 months, but maintained the periodicity From high spectral resolution measurements, Schulte-Ladbeck, Nordsieck, Nook, et al (1990) revealed that the position angle of the polarization changed across the emission lines such that loops were executed in the q u-plane Such behaviour may be explained in terms of there being a rotating, expanding disc in the system The behaviour of the emission lines was explored further by Moffat & Piirola (1993) who found their polarization variation 03% was very much less than that of the continuum 16% For two other non-eclipsing WC7 + O binaries, they found no variation in the emission complex of C III/IV 4650 + He II 4685 , in.

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