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Download RF and Microwave Transmitter Design by Andrei Grebennikov PDF

By Andrei Grebennikov

RF and Microwave Transmitter Design is exclusive in its insurance of either historic transmitter layout and cutting area technologies. This textual content explores the results of famous and new theoretical analyses, whereas informing readers of modern radio transmitters' pracitcal designs and their elements. full of details, this e-book announces and streamlines the author's considerable adventure in RF and microwave layout and improvement

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Example text

These capacitors are used to achieve higher capacitance values in small areas (10 pF and greater), with typical tolerances from 10% to 15%. The capacitance can be calculated according to Eq. 116). 7 TRANSMISSION LINE Transmission lines are widely used in matching circuits in power amplifiers, in resonant and feedback circuits in the oscillators, filters, directional couplers, power combiners, and dividers. When the propagated signal wavelength is compared to its physical dimension, the transmission line can be considered as a two-port network with distributed parameters, where the voltages and currents vary in magnitude and phase over length.

If all these elements are distributed uniformly along the transmission line, and their values do not depend on the chosen position of x, this transmission line is called the uniform transmission line. Any finite length of the uniform transmission line can be viewed as a cascade of section length x. To define the distribution of the voltages and currents along the uniform transmission line, it is necessary to write the differential equations using Kirchhoff’s voltage law for instantaneous values of the voltages and currents in the line section of length x, distant x from its beginning.

At frequencies well below the inductor self-resonant frequency ωSRF , the coupling capacitance Cc between metal segments due to fringing fields in both the dielectric and air regions can also be neglected since the relative dielectric constant of the oxide is small enough [13]. In this case, if one side of the inductor is grounded, the self-resonant frequency of the spiral inductor can approximately be calculated from ωSRF = √ 1 L s Cox L s − Rs2 Cox . 113) At frequencies higher than self-resonant frequency ωSRF , the inductor exhibits a capacitive behavior.

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