Download e-book for iPad: Sinusoidal Oscillators and Waveform Generators using Modern by Raj Senani, D. R. Bhaskar, V. K. Singh, R. K. Sharma

By Raj Senani, D. R. Bhaskar, V. K. Singh, R. K. Sharma

ISBN-10: 331923711X

ISBN-13: 9783319237114

ISBN-10: 3319237128

ISBN-13: 9783319237121

This ebook serves as a single-source connection with sinusoidal oscillators and waveform turbines, utilizing classical in addition to quite a few smooth digital circuit development blocks. It offers a state of the art evaluation of a big number of sinusoidal oscillators and waveform turbines and features a catalogue of over six hundred configurations of oscillators and waveform turbines, describing their suitable layout info and salient functionality features/limitations.
The authors talk about a couple of attention-grabbing, open learn difficulties and contain a entire choice of over 1500 references on oscillators and non-sinusoidal waveform generators/relaxation oscillators.

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Extra info for Sinusoidal Oscillators and Waveform Generators using Modern Electronic Circuit Building Blocks

Example text

Furthermore, even this gain requirement can be distributed over all the op-amps to reduce distortion. Thus, this oscillator is the one which gives the least distortion coupled with good frequency stability (which is to be elaborated further subsequently), though this improved performance comes at the cost of more number of op-amps than the classical single-op-ampbased RC phase-shift oscillators. 3 Colpitts and Hartley Oscillators While active RC oscillators are suitable for low to medium frequencies, for generating high-frequency signals, usually LC oscillators are preferred.

25, it may be observed that since the last part of the circuit using an op-amp and three resistors, in fact, simulates a negative resistance of value À(R02Ra/Rb), it follows that the circuit turns out to be exactly the same as the RLC shunt resonator of Fig. 26. We now show that the model shown in Fig. 26 can lead to many practical op-amp circuits in a number of ways. For example, one way of implementing this model could be to realize the inductor L0 by a generalized impedance converter (GIC) circuit and realizing the negative resistance by a single-op-amp circuit configured as negative-impedance converter (NIC).

The time 38 1 Basic Sinusoidal Oscillators and Waveform Generators Using IC Building Blocks Fig. 2 kΩ, R3 ¼ R4 ¼ 9 kΩ, R5 ¼ R6 ¼ 1 kΩ) −߱ R1 C R X1 R3 R5 −߱ R2 1 R4 C 2 R X2 R6 needed for the signal x1 to reach to zero value from its peak value V is T/4, where T is the period of the triangular wave. 2 V. The resulting final circuit is shown in Fig. 34. In this case, the time needed by the signal x2 to reach the zero value from its maximum positive value V is T/2, where T is the period of oscillation.

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Sinusoidal Oscillators and Waveform Generators using Modern Electronic Circuit Building Blocks by Raj Senani, D. R. Bhaskar, V. K. Singh, R. K. Sharma


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