Navy Electricity and Electronics Training Series (NEETS)
7—Introduction to Solid-State Devices and Power Supplies
3: Pages 3-51 through 3-55
Module 7—Introduction to Solid-State Devices and Power Supplies
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1-11 to 1-20
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1-31 to 1-40
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2-1 to 2-10
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2-21 to 2-30
2-31 to 2-40
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2-51 to 2-54
, 3-1 to 3-10
3-11 to 3-20
, 3-21 to 3-30
3-31 to 3-40
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3-51 to 3-54
4-1 to 4-10
, 4-11 to 4-20
4-21 to 4-30
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4-41 to 4-50
, 4-51 to 4-62
This chapter introduced you to a representative selection of solid-state devices that have special
properties. The basic operating principles of the devices discussed in this chapter are summarized in the
following paragraphs for you to use as a review and a future reference.
The ZENER DIODE
is a PN junction that is designed to operate in the reverse-bias breakdown mode. When the applied voltage reaches
the breakdown point, the Zener diode, for all practical purposes, becomes a short circuit. The reverse bias and
breakdown mode of operation cause the Zener diode to conduct with (in the direction of) the arrow in the symbol as
Two theories are used to explain the breakdown action of Zener diodes. The ZENER EFFECT
explains the breakdown of diodes below 5 volts. The heavy doping used in these diodes allows the valence band of
one material to overlap the energy level of the conduction band of the other material. This situation allows
electrons to tunnel across the PN junction at the point where the two energy bands overlap. Zener diodes that
operate above 5 volts are explained by the AVALANCHE EFFECT in which free electrons colliding with bound electrons
cause an ever-increasing number of free current carriers in a multiplying action. The Zener diode is used
primarily as a voltage regulator in electronic circuits.
The TUNNEL DIODE is a heavily
doped PN junction that exhibits negative resistance over part of its range of operation, as can be seen in the
curve in the illustration. The heavy doping causes the tunnel diode to have a very narrow depletion region and
also causes the valence band of one of the semiconductor materials to overlap the energy level of the conduction
band of the other semiconductor material. At the energy overlap point, electrons can cross from the valence band
of one material to the conduction band of the other material without acquiring any additional energy. This action
is called tunneling. Tunnel diodes are used as amplifiers, oscillators, and high-speed switching devices.
The VARACTOR is a diode that exhibits the characteristics of a variable capacitor. The
depletion region at the PN junction acts as the dielectric of a capacitor and is caused to expand and contract by
the voltage applied to the diode. This action increases and decreases the capacitance. The schematic symbol for
the varactor is shown below. Varactors are used in tuning circuits and can be used as high-frequency amplifiers.
The SILICON CONTROLLED RECTIFIER (SCR) is a four-element, solid-state device that
combines characteristics of both diodes and transistors. The symbol for the SCR is shown below. A signal must be
applied to the gate to cause the SCR to conduct. When the proper gate signal is applied, the SCR conducts or
"fires" until the bias potential across the device drops below the minimum required to sustain current flow.
Removal of the gate signal does not shut off the SCR. In fact, the gate signal is often a very narrow voltage
pulse or trigger. The SCR is ideal for use in situations where a small, low-power gate can be used to turn on
larger currents, such as those found in rectifier and switching circuits. SCRs are used extensively in power
supply circuits as rectifiers.
OPTOELECTRONIC DEVICES are of two basic types: light producers or light users. The LED
is the most widely used light-producing device. When the LED is forward biased it emits energy in the form of
light. LEDs are used in several configurations as digital equipment readout displays. The PHOTODIODE, the
PHOTOTRANSISTOR, and the PHOTOCELL are all devices that use light to modify conduction through them. The SOLAR
CELL uses light to produce voltage.
The UNIJUNCTION TRANSISTOR (UJT) is a three-terminal,
solid-state device with only one PN junction. The block diagram below shows the difference in construction between
normal transistors and the UJT. The area between base 1 and base 2 of the UJT acts as a variable resister. The
emitter of the UJT acts as the wiper arm. The sequential rise in voltage between the bases is called a voltage
gradient. The UJT conducts when the emitter is more positive than the voltage gradient at the emitter/base contact
point. There are many variations of the UJT which are used in switching circuits, oscillators, and wave- shaping
The FIELD-EFFECT TRANSISTOR combines the high input impedance of the vacuum tube with all the other
advantages of the transistor. The elements of the FET are the gate, source, and drain, which are comparable to the
base, emitter, and collector of a standard transistor. The JFET or "junction FET" is made of a solid bar of either
P- or N-semiconductor material, and the gate is made of the opposite type material, as illustrated below. The FET
is called P-channel or N-channel depending upon the type of material used to make the bar between the source and
drain. Voltage applied to the gate controls the width of the channel and consequently controls the current flow
from the source to the drain. The JFET is normally operated with reverse bias that controls the channel width by
increasing or decreasing the depletion region.
The MOSFET is an FET that has even higher input impedances than the JFET because the
gate of the MOSFET is completely insulated from the rest of the device. The MOSFET operates in either the
depletion mode or the forward-bias enhancement mode and can be either N-channel or P-channel. The induced-channel
and the dual-gate MOSFETs are variations of the basic MOSFET.
ANSWERS TO QUESTIONS Q1. THROUGH Q44.
A1. The minority carriers.
A2. Zener effect and avalanche effect
A4. The doping level of an avalanche effect diode is lower.
A5. An external
A6. Because Zener diodes are operated in the reverse bias mode.
The amount of doping.
A8. Negative resistance.
A9. The tunnel diode has a very narrow depletion region.
A11. Variable capacitance.
A12. The depletion region decreases.
A14. The SCR is primarily used for switching power on or off.
A16. The forward bias must be reduced below the minimum conduction level.
A18. During both alternations.
A19. Forward bias.
A20. Very low.
A21. The cathode.
A22. Very high.
A23. Reverse bias.
A25. Photovoltaic cell.
A27. Variable resistor.
A28. A voltage gradient.
A29. From base 1 to the emitter.
A30. High input impedance.
A31. Voltage controls
A33. N-channel and P-channel.
A34. N-type material.
A35. Effective cross-sectional area of the channel.
A36. From source to drain.
A37. Source-to-drain resistance increases.
A38. They are 180 degrees out of phase.
A39. The MOSFET has a higher input impedance.
A40. Gate, source, drain, and substrate.
A41. P-type material.
A42. The gate terminal.
A43. The dual-gate MOSFET.
A44. To prevent damage from static electricity.
Introduction to Matter, Energy,
and Direct Current, Introduction to Alternating Current and Transformers,
Introduction to Circuit Protection,
Control, and Measurement, Introduction to
Electrical Conductors, Wiring Techniques, and Schematic Reading,
Introduction to Generators and Motors,
Introduction to Electronic Emission, Tubes, and
Power Supplies, Introduction to Solid-State
Devices and Power Supplies, Introduction
to Amplifiers, Introduction to Wave-Generation
and Wave-Shaping Circuits, Introduction to
Wave Propagation, Transmission Lines, and Antennas,
Modulation Principles, Introduction to Number
Systems and Logic Circuits, Introduction to Microelectronics,
Principles of Synchros, Servos, and Gyros,
Introduction to Test Equipment,
Radio-Frequency Communications Principles,
Radar Principles, The Technician's Handbook,
Master Glossary, Test Methods and Practices,
Introduction to Digital Computers, Magnetic Recording, Introduction to Fiber Optics
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