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Oscillator uses dual-output current-controlled conveyors

Varying the bias current of dual-output current-controlled conveyors controls the frequency of oscillation of the circuits.

Abhirup Lahiri, Netaji Subhas Institute of Technology, New Delhi, India; Edited by Martin Rowe and Fran Granville -- EDN, November 13, 2008

In the last decade, engineers have done much work in designing and implementing current-mode circuits using second-generation current conveyors, which have higher signal bandwidth, greater linearity, larger dynamic range, simpler circuitry, and lower power consumption than their predecessors. Recently, a second-generation dual-output, current-controlled conveyor has emerged. The device is an active building block (Figure 1), and the following equations characterize it: IY=0, VX=VY+IXRX, and IZ+=IX; IZ–=–IX.The parasitic resistance at terminal X is RX=(VT/2IB), where VT is the thermal voltage and IB is the bias current of the conveyor that is tunable over several decades.

Figure 2 shows current-controlled oscillators with few components, employing only two dual-output current-controlled conveyors and two grounded capacitors. The devices use no external resistors, and the parasitic resistance at terminal X realizes resistance. The proposed design for the circuit provides electronic controllability of frequency of oscillation.

The characteristic equation for both of the circuits in Figure 2 is s2C1C2RX1RX2+sC2RX1–sC1RX1+1=0. Satisfying Barkhausen’s criteria—that the loop gain is unity or greater and that the feedback signal arriving back at the input is phase-shifted 360°—the required condition for oscillation is C1=C2, and the frequency of oscillation is f=1/(2π).

Assuming that C1=C2=C and taking RX1=RX2=VT/2IB yield a frequency of oscillation: f=(IB/πCVT). Clearly, the dc-bias current, IB, can vary the frequency of the current conveyors, and the frequency is, therefore, electronically controllable.

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