Download Electronic Circuits Handbook for Design and Application by Tietze U. PDF
By Tietze U.
This ebook is written for college students, practising engineers and scientists. It covers all very important elements of analog and electronic circuit layout. half I describes semiconductor units and their habit with admire to the types utilized in circuit simulation. uncomplicated circuits are analyzed in 4 steps: large-signal move attribute, small-signal reaction, noise and distortion. half II describes using operational amplifiers and A/D and D/A converters in low-frequency purposes. half III describes circuits for analog and electronic communique over instant channels. This contains the high-frequency habit of passive elements, amplifiers and mixers. Simulation courses are supplied: PSpice for analog circuit layout and ispLever for electronic circuit layout.
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Example text
29 shows the maximum power gains for transistor BFR93 at VCE,A = 5 V and IC,A = 30 mA. The maximum available power gain (MAG) is only defined for f > 500 MHz as only here does the stability factor k rise above one. It declines at a rate of 20 dB/decade and assumes the value 1 or 0 dB at the transit frequency fT = 5 GHz. For f < 500 MHz the maximum stable power gain (MSG) is obtained which, at lower frequencies, declines at a rate of 10 dB/decade. 5 dB and assumes the value 1 or 0 dB at fmax = 12 GHz.
40 on page 1227 from the S parameters while taking into account the condition S11 = S22 = 0. 4 Power Gain 1401 2 |S 21,match | = MAG S11 ,S12 ,S21 ,S22 , k >1 Rg= ZW vg Matching network S 11,match =0 Matching network rg,o rL ,o RL= Z W S22,match =0 Fig. 28. Maximum available power gain (MAG) of an amplifier matched at both sides Maximum Stable Power Gain At frequencies above approximately a quarter of the transit frequency, the conditions for impedance matching at both sides are usually met. e.
1390 27. High-Frequency Amplifiers R R ii io vi vi g m vi ri vo RL Rg vi a Gain and input resistance vi g m vi vo ro b Output resistance Fig. 22. 17) According to Fig. 20) The reflection factors S11 and S22 are identical and become zero for: 2 R = gm ZW This means that both sides are matched. 22) This is identical to the gain in a circuit which is matched at both ends. It can be influenced only by means of the transconductance gm as the feedback resistance is linked to the transconductance. A high transconductance results in a high gain.