
resistors in series this becomes V = I(R
1
⫹R
2
). The power dissipated in the re-
sistor is given by P = IV. For AC signals, RMS voltages are used so that the
same model can be applied. Reactive components need the frequency of the
signal to be included, so V = IX is used, where X is the reactance. For a capac-
itor, the magnitude of the reactance is 1/ωC, for an inductor ωL, where C is the
capacitance and L the inductance. We then need to model the phase relation-
ship between voltage and current, using complex numbers, and so on.
Digital circuits are in principle easier, since they are modelled using simple
logical relationships, such as A = B.C, w