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Under certain conditions, diodes can be made to produce microwave radio signals. There are three types of diodes that do this: Gunn diodes, IMPATT diodes, and tunnel diodes.

Downloaded from Digital Engineering Library @ McGraw-Hill (www.digitalengineeringlibrary.com) Copyright 2004 The McGraw-Hill Companies. All rights reserved. Any use is subject to the Terms of Use as given at the website.

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jBL = j[1/(6.28f L)] = j[1/(6.28 4.00 6.00)] = j0.00663 Next, calculate the susceptance of the capacitor (converting its value to microfarads) at 4.00 MHz, as follows: jBC = j(6.28f C ) = j(6.28 4.00 0.000150) = j0.00377 Finally, add the inductive and capacitive susceptances to obtain the net susceptance: jB = jBL + jBC = j0.00663 + j0.00377 = j0.00286 This is a pure inductive susceptance.

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A Gunn diode can produce up to 1 W of RF power output, but more commonly it works at levels of about 0.1 W. Gunn diodes are usually made from gallium arsenide. A Gunn diode oscillates because of the Gunn effect, named after J. Gunn of International Business Machines (IBM) who observed it in the sixties. A Gunn diode doesn t work anything like a rectifier, detector, or mixer; instead, the oscillation takes place as a result of a quirk called negative resistance. Gunn-diode oscillators are often tuned using varactor diodes. A Gunn-diode oscillator, connected directly to a microwave horn antenna, is known as a Gunnplexer. These devices are popular with amateur-radio experimenters at frequencies of 10 GHz and above.

Problem 16-12 What is the net susceptance of the above parallel-connected inductor and capacitor at a frequency of f = 5.31 MHz

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The acronym IMPATT comes from the words impact avalanche transit time. This, like negative resistance, is a phenomenon the details of which are rather esoteric. An IMPATT diode is a microwave oscillating device like a Gunn diode, except that it uses silicon rather than gallium arsenide. An IMPATT diode can be used as an amplifier for a microwave transmitter that employs a Gunn-diode oscillator. As an oscillator, an IMPATT diode produces about the same amount of output power, at comparable frequencies, as the Gunn diode.

First calculate the susceptance of the inductor at 5.31 MHz, as follows: jBL = j[1/(6.28f L)] = j[1/(6.28 5.31 6.00)] = j0.00500 Next calculate the susceptance of the capacitor (converting its value to microfarads) at 5.31 MHz, as follows: jBC = j(6.28f C ) = j(6.28 5.31 0.000150) = j0.00500 Finally, add the inductive and capacitive susceptances to obtain the net susceptance: jB = jBL + jBC = j0.00500 + j0.00500 = j0 This means that the circuit has no susceptance at 5.31 MHz. The situation in which there is no susceptance in an LC circuit is known as parallel resonance. It is discussed in the next chapter.

Another type of diode that will oscillate at microwave frequencies is the tunnel diode, also known as the Esaki diode. It produces only a very small amount of power, but it can be used as a local oscillator in a microwave radio receiver. Tunnel diodes work well as amplifiers in microwave receivers, because they generate very little unwanted noise. This is especially true of gallium arsenide devices. The behavior of Gunn, IMPATT, and tunnel diodes is a sophisticated topic and is beyond the scope of this book. College-level electrical-engineering texts are good sources of information on this subject. You will want to know about how these devices work if you plan to become a microwave engineer.

In reality, single-mode fiber is a stepped-index design, because the core s refractive index is slightly higher than that of the cladding. It has become the de facto standard for optical transmission systems and takes on many forms depending on the specific application within which it will be used. Most single-mode fiber has an extremely narrow core diameter on the order of seven to nine microns, and a cladding diameter of 125 microns. The advantage of this design is that it only enables a single mode to propagate. The downside, however, is the difficulty involved in working with it. The core must be coupled directly to the light source and the receiver in order to make the system as effective as possible. Given that the core is approximately one-sixth the diameter of a human hair, the mechanical process through which this coupling takes place becomes Herculean.

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