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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).