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26  Complementarity and Variational Inequalities in Electronics



























                           FIGURE 2.16 Zener diode model.


                           diode (see Fig. 2.16) is a good voltage regulator to maintain a constant voltage
                           regardless of minor variations in load current or input voltage. There is a current
                           point I Z , called the Zener knee current, which is the minimum value of the Zener
                           current required to maintain voltage regulation and a maximum allowable value
                           of Zener current I M . Currents above this value damage or destroy the system.
                              The graph corresponding to the ampere–volt characteristic (i,V ) is maximal
                           monotone, and there exists a proper convex continuous electrical superpotential
                           ϕ Z : R → R such that
                                                 (∀i ∈ R) : V ∈ ∂ϕ Z (i).
                           The ideal Zener diode model (see Fig. 2.17) is given by the practical diode
                           model (see Fig. 2.14) with appropriate values for V 1 and V 2 . This means that
                           the voltage across the diode is constant over a wide range of device current
                           values.
                              The practical Zener diode model (see Fig. 2.18) is a piecewise linear model
                           that includes the effects of the Zener impedance.
                              Let us use the notation of Fig. 2.18. Here it is implicitly assumed that
                                           I 1 < 0 <I 2 ,V 1 <V 3 < 0 <V 4 <V 2 .
                           The electrical superpotential of the Zener diode is

                                                ⎧
                                                ⎨ (V 1 −V 3 ) 2   if x< 0
                                                         x + V 3 x
                                                     2I 1
                                         ϕ Z (x) =
                                                ⎩ (V 2 −V 4 ) 2
                                                         x + V 4 x  if x ≥ 0.
                                                     2I 2
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