Electrophotography is the science of document copying by selective dissipation of charge of corona charged layers. The recent trend in this field is to develop binder-layer type xerographic plates [1, 2]. Copper-phthalocyanine (CuPh) is a well studied photosensitive material and some work on its electrophotographic use has been' done using silicone resin as a binder [3, 4]. In the present paper, electrophotographic characteristics of copper-phthalocyanine (CuPh) in polyvinyl cinnamate (PVCn) binder are described. PVCn is also a photosensitive polymer. CuPh and PVCn used in the present study were obtained from Fluk: A. Chemische Fabrik CH-9470 BUCTIS and Polysciences Inc (USA), respectively. The desired weight ratios of these materials were milled in a mechanical grinder using benzene as a thinner. The films were made by pouring this mixture on an aluminium substrate. The layers were dried in atmospheric benzene and later in an oven maintained at 60°C for 48 h to remove all traces of benzene. The films were positively charged by a d.c. corona unit for 15 sec and then the surface potential decay was measured in the dark as well as in the light. The various samples studied during the present investigation were 20 : 80, 30: 70, 40:60, 50:50 and 60:40 weight ratio of CuPh and PVCn. The film thickness was 100 pro. The light from a 60 W tungsten lamp of intensity 1200 lux was used for photodischarge studies. The room temperature (30 ° C) and relative humidity (55%) were maintained constant during the course of investigations. The grid voltage and charging time were optimized to 1.5 kV and 15 sec, respectively, which were maintained constant throughout the experiments. The corona voltage was 6 kV. The effect of charging time and grid potential on the initial surface potential of 50:50 CuPh: PVCn samples are shown in Figs. 1 and 2, respectively. It has been observed that initially the surface potential increases both with charging time and grid potential and finally attains a saturation value. These results are expected. The number of charge carriers becoming trapped during corona charging increases with charging time and grid potential and hence the surface potential increases with the increase in time and grid potential. But the detrapping and recombination of charge carriers takes place simultaneously along with trapping. When these two, i.e. trapping and detrapping and recombination become equal, further charging of the film stops and we observed a saturation effect [5, 6]. The difference in surface potential decay in the dark and the light determines the use of a material in electrophotography. A good electro