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ring number A locally assigned, catenet-unique value identifying each ring in a source-routed catenet. RMON probe A node capable of passively monitoring network traf c, gathering statistics related to that traf c, and reporting it to a network management node using SNMP. root bridge In the Spanning Tree Protocol, the bridge in the catenet with the numerically lowest value for its bridge identi er. root port In the Spanning Tree Protocol, the port through which a designated bridge forwards traf c in the direction of the root bridge. route descriptor A catenation of a ring number and a bridge number within the routing information eld of a source-routed frame. route discovery The process of determining the available route(s) between a pair of nodes in a source-routed catenet. router An intermediate node operating as a Network layer relay node.

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For convenience we can de ne B = [I hA] 1 . Super cially, (10.103) seems to have the same form as (10.97). We might be lead therefore to believe (falsely) that the implicit method can be unstable, too. However, we may assume that there exists a nonsingular matrix V such that (if A RN N ) V 1 AV = , (10.104)

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Correspondingly, the value of an electrical quantity in the circuit may be plotted as a function of the parameter; for instance, let us assume that the amplitude of the oscillation saturates to a nite value because of the nonlinearities of the circuit, so far neglected for stability analysis Therefore, a plot of the amplitude of the oscillating voltage in the parallel resonant circuit after the oscillations have reached the equilibrium amplitude (see Section 53) looks as shown in Figure 87 For Gtot > 0, eq (824) has only one solution, which is the stable DC solution with vosc (t) = 0 For Gtot < 0, eq (824) has two solutions, of which the DC one with vosc (t) = 0 is only mathematical because it is unstable, while the other with vosc (t) > 0 is stable The point Gtot = 0 is a bifurcation point.

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In this case, the generation of a new branch is caused by the sign change of the real part of the complex roots of the perturbation equation (824), or in other words by the onset of an autonomous oscillation; this is called a Hopf bifurcation Other types of bifurcation are described below The circuit in Figure 85 becomes closer to real life if we consider it as the linearisation of a circuit including an active device, exhibiting a negative differential (small-signal) conductance in a given bias point range By changing the bias, the total conductance may change sign and quench the oscillations Therefore, the parameter that controls the bifurcation may be the bias voltage of the active device, for example, a tunnel diode Another example of control parameter is the gate bias voltage of an FET oscillator as described in Section 54, and shown in Figure 8.