Download Analog Integrated Circuits for Communication by Donald O. Pederson PDF

By Donald O. Pederson

Analog built-in Circuits for conversation: rules, Simulation and layout, moment version covers the research and layout of nonlinear analog built-in circuits that shape the foundation of present-day conversation platforms. either bipolar and MOS transistor circuits are analyzed and a number of other numerical examples are used to demonstrate the research and layout concepts constructed during this e-book.

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38) We next introduce a sinusoidal input voltage and include it in the power series. 303D-04 TOTAL HARMONIC DISTORTION = V1A = 0. 2 V, Tstep = 0. 680 PERCENT V1A = 2. 0 V, Tstep = 0. 786271 PERCENT Fig. 24. Fourier components of the output voltage for two input amplitudes. 2 V and V(16) for an input of 2 V. 39) where V1A is the zero-to-peak value of the input sinusoidal tone. 38) can be converted to harmonic terms using trigonometric identities. 40) 3 cos 3ω1 t − . . where compression and expansion terms from higher-order terms are neglected.

4. 5 mA -10 V 2 k' = 30 µA/V , VT = 0. 5 V, W = 10 L Fig. 29. 5. 1 General Power Series Description In the previous chapter, a power-series expansion of the transfer characteristics of a stage is obtained from the circuit analysis of the stage using simplified circuit models for the transistors. In order to use a truncated set of first few terms of the power series, a restriction must be made to relatively small 1. , for the ECP stage, V1 /Vt In general, the transfer characteristic of an amplifier can be described by a power series.

295%, using RELTOL = 1 × 10−6 . Notice that HD3 goes up as the square of V1A , the input amplitude, although the compression term in b1 ultimately comes into the scene. From the developments above, all even-order harmonics should be zero. In a Spice output, these even-order harmonics are small, but not zero. The nonzero values are due to ‘numerical noise’ in the Fourier calculations. The same results for HD3 are obtained for the other two output possibilities, Vo1 and Vo = Vo1 − Vo2 . The only change occurs in the sign (phase) of the components of the Fourier expansion of the outputs.

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