Photoconductive cells

The photoconductive cell is a two terminal semiconductor device whose terminal resistance will vary (linearly) with the intensity of the inci­dent light. For obvious reasons, it is frequently called a photoresistive device.

The photoconductive materials most frequently used include cadmium sulphide (CdS) and cadmium selenide (CdSe). Both materials respond rather slowly to changes in light intensity. The peak spectral response time of CdS units is about 100 ms and 10 ms for CdSe cells. Another im­portant difference between the two materials is their temperature sensitivity. There is large change in the resistance of a cadmium selenide cell with changes in ambient temperature, but the re­sistance of cadmium sulphide remains relatively stable. The spectral response of a cadmium sulphide cell closely matches thatof the human eye, and the cell is therefore often used in applications where human vision is a factor, such as street light control or automatic iris control for cameras.

The essential elements of a photoconductive cell are the ceramic substrate, a layer of photo­conductive material, metallic electrodes to connect the device into a circuit and a moisture re­sistant enclosure.

The circuit symbol and construction of a typical photoconductive cell are shown.

Light sensitive material is arranged in the form of a long strip, zigzagged across a disc shaped base with protective sides. For added protection, a glass or plastic cover may be included. The two ends of the strip are brought out to connecting pins below the base.

Photoconductive cell circuit:

Characteristics of a Photoconductive cell:

The illumination characteristics of a typi­cal photoconductive cell are shown from which it is obvious that when the cell is not illuminated its resistance may be more than 1 00 kilo ohms. This resistance is called the dark resistance. When the cell is illumi­nated, the resistance may fall to a few hun­dred ohms. Note that the scales on the illu­mination characteristic are logarithmic to cover a wide ranges of resistance and illu­mination that are possible. Cell sensitivity may be expressed in terms of the cell cur­rent for a given voltage and given level of illumination.

The major drawback of the photoconduc­tive cells is that temperature variations cause substantial variations in resistance for a substantial variations in resistance for a particular light intensity. Therefore such a cell is unsuitable for analog applications.

The photoconductive cell used for relay control is shown as circuit above When the cell is il­luminated, its resist­ance is low and the relay current is at its maximum. When the cell is dark, its high resistance re­duces the current down to a level too low to energize the relay. Resistance R is included to limit the relay current to the desired level when the resistance of the cell is low. Photoconductive cells are used to switch transistors on and off, as illustrated in figure. When the cell shown in figure is dark, the transistor base is biased above its emitter level, and the device is turned on. When the cell is illuminated, the lower resist­ance of the cell in series with R biases the transistor base voltage below its emitter level. Thus, the device is turned off.