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Unit 2. Transistors and Voltage<br />

Amplification<br />

Radio transmitters and receivers have existed since before the end of the nineteenth century.<br />

A practical form of wireless telegraph, attributed to G. Marconi, appeared in 1895, and<br />

successful transmission across the Atlantic Ocean was achieved in 1901. However, in the early<br />

part of the twentieth century, systems were limited by the lack of a means of voltage<br />

amplification. The appearance of a voltage amplification device, the vacuum tube, dramatically<br />

improved the concept, as microvolt signals could be boosted for receiving and transmitting.<br />

In the middle of the twentieth century, the transistor appeared. The idea of transistors based<br />

on a sandwich of pn junctions (BJT) and a field-effect transistor based on pn junctions (JFET)<br />

and on a metal – oxide – semiconductor (MOS) structure (basically, a capacitor) were all<br />

understood at the time. However, pn-junction devices became a practical realization much<br />

sooner than the MOS structure, due to fabrication complications in producing the MOS device<br />

as well as perhaps a perceived lack of need. The JFET served as an interim field-effect<br />

transistor until the MOS technology evolved. It provided for a transistor with very high input<br />

resistance and was used extensively as the input transistors for BJT opamps.<br />

A textbook on radio, Elements of Radio, published in 1948 (Marcus and Marcus, 1948), makes<br />

no mention of transistors. A 1958 text, (Millman, 1958), Vacuum-Tube and Semiconductor<br />

Electronics, gives equal weight to vacuum tubes and BJTs in electronic circuits but makes no<br />

mention of the field-effect transistor. Slightly later (Nanavati, 1963), in An Introduction to<br />

Semiconductor Electronics, as the title suggests, vacuum tubes are dropped completely and<br />

the only reference to a field-effect transistor is in one section of the last chapter and this refers<br />

to a junction field-effect transistor. In 1965, in his textbook Analysis and Design of Electronic<br />

<strong>Circuit</strong>s, Chirlian devotes a small portion of the book to vacuum tubes, but most of the<br />

emphasis is on circuits based on the BJT (Chirlian, 1965). No mention is made of the fieldeffect-transistor.<br />

An example of a book in which BJTs and field-effect transistors of both types<br />

were finally given balanced treatment was published in 1979 (Millman, 1979). Textbooks tend<br />

to lag the industry a bit, and during the 1970s, MOSFET circuits were emerging rapidly, driven<br />

by the simultaneous development of integrated circuits. The four editions of a text on analog<br />

circuits by Gray and Meyer, (1977, 1984, 1993) and Gray, et al. (2001) serve well as a series<br />

through which we observe a transition from mostly BJT to, in the last two editions, more-orless<br />

equal treatment of BJT and MOSFET devices. A recent textbook on the subject of analog<br />

integrated circuits (Johns and Martin, 1997) takes the approach that such circuits are now<br />

totally dominated by MOSFETS but includes some BJT applications. BiCMOS, a combination of<br />

MOSFET and BJT devices on the same integrated circuit, is growing in popularity as more ways<br />

of taking advantage of the superior properties of the two transistor types are developed.<br />

Since the earliest transistors, there has been persistent competition between BJT and MOS<br />

transistors. It has been, to a large extent (along with many other considerations), a matter of<br />

power consumption versus speed; the BJT has been faster but is associated with high power<br />

consumption. The MOSFET has gradually taken over as the most important transistor, with<br />

increased emphasis on integrated circuits and improved speeds.

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