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                       FIGURE 11.34  Representation of nonlinear element in
                       a linear circuit.


                       There exists, in fact, a circuit element (the semiconductor diode) that very nearly satisfies this simple
                       relationship. The difficulty in the i-v relationship of Eq. (11.27) is that it is not possible, in general, to
                       obtain a closed-form analytical solution, even for a very simple circuit.
                         One approach to analyzing a circuit containing a nonlinear element might be to treat the nonlinear
                       element as a load, and to compute the Thévenin equivalent of the remaining circuit, as shown in Fig. 11.34.
                       Applying KVL, the following equation may then be obtained:

                                                        v T =  R T i x +  v x                   (11.28)


                       To obtain the second equation needed to solve for both the unknown voltage, v x , and the unknown
                       current, i x , it is necessary to resort to the i-v description of the nonlinear element, namely, Eq. (11.27).
                       If, for the moment, only positive voltages are considered, the circuit is completely described by the
                       following system:


                                                      i x =  I 0 e an x , v >  0
                                                                                                (11.29)
                                                      v T =  R T i x +  v x


                       The two parts of Eq. (11.29) represent a system of two equations in two unknowns. Any numerical
                       method of choice may now be applied to solve the system of Eqs. (11.29).



                       11.4 AC Network Analysis

                       In this section we introduce energy-storage elements, dynamic circuits, and the analysis of circuits excited
                       by sinusoidal voltages and currents. Sinusoidal (or AC) signals constitute the most important class of
                       signals in the analysis of electrical circuits. The simplest reason is that virtually all of the electric power
                       used in households and industries comes in the form of sinusoidal voltages and currents.

                       Energy-Storage (Dynamic) Circuit Elements

                       The ideal resistor was introduced through Ohm’s law in Section 11.2 as a useful idealization of many
                       practical electrical devices. However, in addition to resistance to the flow of electric current, which is purely
                       a dissipative (i.e., an energy-loss) phenomenon, electric devices may also exhibit energy-storage properties,
                       much in the same way a spring or a flywheel can store mechanical energy. Two distinct mechanisms for
                       energy storage exist in electric circuits: capacitance and inductance, both of which lead to the storage of
                       energy in an electromagnetic field.
                       The Ideal Capacitor
                       A physical capacitor is a device that can store energy in the form of a charge separation when appropriately
                       polarized by an electric field (i.e., a voltage). The simplest capacitor configuration consists of two parallel


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