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Lab manual for photo transistor, Cheat Sheet of Laboratory Practices and Management

Lab manual for photo transistor

Typology: Cheat Sheet

2023/2024

Uploaded on 07/11/2024

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COLLEGE OF ENGINEERING AND TECHNOLOGY
EC8252-ELECTRONIC DEVICES
5.9 PHOTO TRANSISTOR
Phototransistors are either tri-terminal (emitter, base and collector) or bi-terminal (emitter
and collector) semiconductor devices which have a light-sensitive base region. Although
all transistors exhibit light-sensitive nature, these are specially designed and optimized
for photo applications. These are made of diffusion or ion-implantation and have much
larger collector and base regions in comparison with the ordinary transistors. These
devices can be either homojunction structured or heterojunction structured, as shown by
Figure respectively.
Fig:5.9.1 Symbol of Photo Transistor
In the case of homojunction phototransistors, the entire device will be made of a single
material-type; either silicon or germanium. However to increase their efficiency, the
phototransistors can be made of non-identical materials (Group III-V materials like
GaAs) on either side of the pn junction leading to heterojunction devices. Nevertheless,
homojunction devices are more often used in comparison with the hetero junction devices
as they are economical.
Fig:5.9.2 Photo Transistor (a) Homo Junction (b) Hetero Junction
The circuit symbol for npn phototransistors is shown by Figure 2 which is nothing but a
transistor (with or without base lead) with two arrows pointing towards the base
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5.9 PHOTO TRANSISTOR

Phototransistors are either tri-terminal (emitter, base and collector) or bi-terminal (emitter and collector) semiconductor devices which have a light-sensitive base region. Although all transistors exhibit light-sensitive nature, these are specially designed and optimized for photo applications. These are made of diffusion or ion-implantation and have much larger collector and base regions in comparison with the ordinary transistors. These devices can be either homojunction structured or heterojunction structured, as shown by Figure respectively. Fig:5.9.1 Symbol of Photo Transistor In the case of homojunction phototransistors, the entire device will be made of a single material-type; either silicon or germanium. However to increase their efficiency, the phototransistors can be made of non-identical materials (Group III-V materials like GaAs) on either side of the pn junction leading to heterojunction devices. Nevertheless, homojunction devices are more often used in comparison with the hetero junction devices as they are economical. Fig:5.9.2 Photo Transistor (a) Homo Junction (b) Hetero Junction The circuit symbol for npn phototransistors is shown by Figure 2 which is nothing but a transistor (with or without base lead) with two arrows pointing towards the base

indicating its sensitivity to light. Similar symbolic representation holds well even in the case of pnp phototransistors with the only change being the arrow at emitter pointing in, instead of out. Fig:5.9.3 Characteristics of Photo Transistor The behavior of phototransistors is identical to that of normal transistors except the fact that here the effect brought-about by the base voltage will be experienced due to the incident light. This can be made clearer by analyzing the following points

  1. The characteristics of phototransistors are similar to those of normal transistors except that they have base current replaced by light intensity. This means that even these devices have three operating regions viz., cut-off, active and saturation. This further implies that the phototransistors can be used for either switching (cut-off and saturation mode dependent) applications or for amplification (active mode operation), just like ordinary transistors.
  2. The phototransistors can be configured in two different configurations viz., common collector and common emitter, depending on the terminal which is common between the input and output terminals, similar to normal transistors.

Advantages of Phototransistor

  1. Simple, compact and less expensive.
  2. Higher current, higher gain and faster response times in comparison with photodiodes.
  3. Results in output voltage unlike photo resistors.
  4. Sensitive to a wide range of wavelengths ranging from ultraviolet (UV) to infrared (IR) through visible radiation.
  5. Sensitive to large number of sources including incandescent bulbs, fluorescent bulbs, neon bulbs, lasers, flames and sunlight.
  6. Highly reliable and temporally stable.
  7. Less noisy when compared to avalanche photodiodes.
  8. Available in wide variety of package types including epoxy-coated, transfer- molded and surface mounted. Disadvantages of Phototransistor
  9. Cannot handle high voltages if made of silicon.
  10. Prone to electric spikes and surges.
  11. Affected by electromagnetic energy.
  12. Do not permit the easy flow of electrons unlike electron tubes.
  13. Poor high frequency response due to a large base-collector capacitance.
  14. Cannot detect low levels of light better than photodiodes. Applications of Phototransistor
  15. Object detection
  16. Encoder sensing
  17. Automatic electric control systems such as in light detectors
  18. Security systems
  19. Punch-card readers
  20. Relays
  21. Computer logic circuitry
  22. Counting systems
  23. Smoke detectors
  24. Laser-ranging finding devices
  1. Optical remote controls
  2. CD players
  3. Astronomy
  4. Night vision systems
  5. Infrared receivers
  6. Printers and copiers
  7. Cameras as shutter controllers
  8. Level comparators