COMMISSION 27 OF THE I. A. U. INFORMATION BULLETIN ON VARIABLE STARS Number 2119 Konkoly Observatory Budapest 1982 March 29 HU ISSN 0374-0676 PHOTOELECTRIC TIMINGS OF PRIMARY MINIMUM OF TV Cas AND THE METHOD In this paper 4 new timings of primary minimum of the eclipsing binary TV Cas are presented. Essentially the same procedure was used as in De Landtsheer (1981), i.e. the timings are mean values of 4 separate determinations made in 4 different color- bands. However, a small improvement in the method of determination was implemented, which led to a slightly different value (+0.0003 day) for the time of primary minimum published in that paper. This calls for an explanation of our "folding-method". In principle the folding-method is a midpoint-method. The observations of the one side of the minimum are folded on a trial time of minimum upon the other side. The time, which yields the narrowest band of points is the timing we look for. To measure the width of the band we formerly calculated the distances of the individual points to a second order polynomial through the whole set of observations. But since the exact shape of the minimum is not known it is better to assume as little as possible in its representation. To this purpose an approximating cubic spline function gives preference to a polynomial. So at present we draw a spline through the branch with the largest number of observations, fold the other on the trial time and compute the distances of the folded points to the spline. The time which yields the least sum of absolute values of the deviations, in the time direction, from the spline, is the one. This procedure is similar to the approach of Kwee and Van Woerden (1956). But since the observations are folded in the time direction, we look for deviations in the time direction rather than in the magnitude direction. Since we are in search of the narrowest band, we sum absolute values rather than squares. Not every observation can be used. Points in the bottom and the shoulders of the minimum when folded, do not add meaningful information about the time of minimum. In the case of TV Cas only points in the phase intervals 0.925-0.990 and 0.010-0.075 were used. The folding-method may be applied to all selected points in one go. But of course they may be first divided into several subsets. Thus information may be gained about a possible asymmetry of the minimum, or, if no systematic trend is found, about the accuracy of the determination. In the case of TV Cas no asymmetry was found. Table I Heliocentric times of minimum of TV Cas Hel. J.D.- 2,444,000.0 E O-C Number of Obs. 602.4537+- .0003 1659 +.0014 109 843.5296+- .0003 1792 +.0022 63 910.5965+- .0003 1829 +.0031 118 912.4089+- .0003 1830 +.0029 174 990.3503+- .0005 1873 +.0028 48 The 4 new timings and the earlier published, but revised one are shown in Table I. The ephemeris 2441595.3582 + 1.8124944 E of Margrave (1980) was used to calculate the O-C values. A.C. DE LANDTSHEER The Astronomical Institute at Utrecht Zonnenburg 2 3512 NL Utrecht The Netherlands References: De Landtsheer, A.C., 1981, IBVS No. 1985. Kwee, K.K. and Van Woerden, H., 1956, B.A.N., 12, 327. [BIBCODE 1956BAN....12..327K ] Margrave, T.E., 1980, IBVS 1869.