COMMISSION 27 OF THE I. A. U. INFORMATION BULLETIN ON VARIABLE STARS Number 1141 Konkoly Observatory Budapest 1976 June 14 PHOTOELECTRIC MAXIMA OF VZ CANCRI Between December 1973 and April 1976, 1800 photoelectric observations of the short-period variable VZ Cancri were carried out at the Astronomical Observatory of the University of Cluj- Napoca. The observations were made in V light with a 50 cm Newton reflector, a photometer employing an unrefrigerated 1P21 photomultiplier tube and a Corning 3384 filter. The comparison star was HD 73938 (BD+11d1894). From the observed light-curves, by Pogson's method, 17 heliocentric maxima and the corresponding magnitudes V_max. were determined. Table 1 contains the observed times of maxima, where the differences O-C's and the phase psi_b (for the beat period) refer to the following elements Max.hel.= JD 2433631.8655+ 0.17836367d E for the principal period, and Max.hel.= JD 2433631.8605+ 0.716292d E_b for the beat period, respectively. In order to have a general picture of period variation we have constructed the diagram O-C=f(psi_b) for heliocentric maxima. With this end in view we have used the corresponding observations made by Fitch (Ap.J. 121, 690, 1955), Spinrad (Ap.J. 131, 134, 1960), Oosterhoff (BAN 18, 459, 1966), and the determined maxima published by Guman (Mitt.d.Sternw.Budapest-Szabadsaghegy, no. 36, 1955), and Popovici (IBVS 508, 1971). The results are presented in Figure 1. The diagram V_max=f(psi_b) is plotted in Figure 2, but here we have used only Fitch's, Spinrad's, Oosterhoff's and Todoran's observations. IOAN TODORAN Astronomical Observatory Cluj-Napoca, Rumania Table 1 Observed maxima Max. hel. 2442000+ V_max. E O-C E_b psi_b 128.3910 7.37m 47636 -0.0063d 11861 0.8252d 132.3295 7.37 47658 + .0082 11867 .3236 161.3885 7.43 47821 - .0061 11867 .8929 453.5485 7.35 49459 - .0058 12315 .7706 474.4160 7.44 49576 - .0068 12344 .9034 476.3790 7.20 49587 - .0058 12347 .6439 485.4855 7.38 49638 + .0041 12360 .3573 487.4465 7.50 49649 + .0031 12363 .0949 508.3195 7.49 49766 + .0076 12392 .2352 531.3285 7.33 49895 + .0077 12424 .3577 756.4113 7.17 51157 - .0045 12738 .5910 771.3955 7.24 51241 - .0028 12759 .5101 785.4980 7.41 51320 + .0090 12779 .1982 837.3865 - 51611 - .0064 12851 .6387 867.3600 7.22 51779 + .0020 12893 .4840 871.2775 7.38 51801 - .0045 12898 .9532 873.4160 7.36 51813 - .0063 12901 0.9387 [FIGURE 1] [FIGURE 2]