Adam Cooman

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Linearized active circuits:
transfer functions and stability

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6. Illustrative example: a time-delayed Chua’s circuit

The time-delayed Chua’s circuit represented on Figure 6.1 is composed of a realistic model of a linearized diode (see Figure 5.1) and a block made of an ideal line with a resistor in series [33]. Using (4.4) with γ(s)=st\gamma(s)\ell=st, where tt is a time constant, the impedance of this block is computed as:

Zlin(s)=Z01ke2st1+ke2st,with  k=Z0RSZ0+RS<1.Z_{\rm lin}(s)=Z_0 \frac{1-k e^{-2st}}{1+k e^{-2st}}, {\rm with} ~~k=\frac{Z_0-R_S}{Z_0+R_S} <1.

Both the numerator and the denominator of Zlin(s)Z_{\rm lin}(s) are quasi-polynomials of neutral type and since k<1|k|<1, it is easily checked that their roots lie on the vertical axis lnk/2t\ln k/2t. Thus, this block is realistic. This provides us with an alternative model of a realistic line: an ideal line in series with a resistor.

Since this linearized circuit is made of realistic components, by Proposition 1 and Lemma 1, the impedance Z(s)Z(s) measured at the red dot on Figure 6.1 is well-defined, meromorphic and for (s)0\Re(s) \geq 0, it is bounded outside a compact set. From Theorem 1, it has at most a finite number of unstable poles. Checking stability to small current perturbations at this node, amounts to determine whether Z(s)Z(s) has or not unstable poles. For this purpose, the method proposed in [23] and numerically implemented in [34], based on the stable/unstable decomposition (2.9), can be used. In the present example, Z(jω)Z(j\omega) was determined on 1500 points between 0 and 9 GHz. The results are shown on Figure 6.2 and the circuit is clearly unstable. In addition, 44 poles in the right half-plane have been identified using the Principal Hankel Components algorithm (PHC) [35]: two expected poles at 2 GHz and two positive real poles (at DC). Details can be found in the conference paper [24].

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Figure 6.1 Time-delayed Chua’s circuit made of realistic linearized electronic components.

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Figure 6.2 Stability analysis tractable: the impedance determined at the location of the red dot has a finite number of unstable poles.

Beyond the simplicity of this illustrative example, the method apply to any time-delayed system of this type, as soon as it is obtained from realistic linearized electronic components.

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