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36  Complementarity and Variational Inequalities in Electronics


                              The approach using variational inequalities of the second kind so as to study
                           electrical networks involving devices like diodes and transistors has been devel-
                           oped in [5] and [40]. The mathematical approach studied in [5] uses recession
                           tools so as to define a new class of problems that is called “semicomplementarity
                           problems” (see also [43]). It is first shown that the study of semicomplementar-
                           ity problems can be used to prove qualitative results applicable to the study of
                           linear variational inequalities of the second kind. By using variational inequali-
                           ties of the second kind the authors study diode circuits like amplitude selectors,
                           which are used to transmit the part of a given waveform that lies above or be-
                           low some given reference level, double-diode clippers that are used to limit the
                           input amplitude at two independent levels, sampling gates that are transmission
                           circuits in which the output is a reproduction of an input waveform during a
                           selected time interval and is zero otherwise, and other circuits involving diodes,
                           transistors, and operational amplifiers. Further theoretical results, applications
                           in electronics, and numerical simulations can be found in [7], [32], and [38].


                           3.3 A GENERAL CLIPPING CIRCUIT
                           Let us again consider the circuit of Fig. 1.2. We discuss here the case of a diode
                           with electrical superpotential ϕ. The Kirchhoff voltage law gives

                                                   u = U R + V + E,

                           where U R = Ri denotes the difference of potential across the resistor, and V ∈
                           ∂ϕ(i) is the difference of potential across diode. Thus

                                                 E + Ri − u ∈−∂ϕ(i),                  (3.7)

                           which is equivalent to the variational inequality

                                       (Ri + E − u)(v − i) + ϕ(v) − ϕ(i) ≥ 0,∀v ∈ R.

                           Moreover,

                                   E      u     1           E    u      1
                                     + i −  ∈− ∂ϕ(i) ⇐⇒ −      +   ∈ i +  ∂ϕ(i)
                                   R      R     R           R    R      R
                                                                    1    −1  u − E
                                                      ⇐⇒ i = (id R +  ∂ϕ)  (     ).
                                                                    R        R
                           Let us now consider a driven time-dependent input t  ø  u(t) and define the
                           output-signal t  ø  V o (t) as
                                             V o (t) = E + V(t) = u(t) − Ri(t).
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