It follows from Eq. (5.15) that for an open-loop stable
system, that is
and
, then
. Therefore the Nyquist criterion can be
reformulated as follows:
If the open loop is asymptotically stable, then the closed loop is only asymptotically stable, if the frequency response locus of the open loop does neither revolve around or pass through the critical point (-1,j0).
Another form of the simplified Nyquist criterion for
with
poles at
is the so called 'left-hand
rule':
The open loop has only poles in the left-halfThis form of the Nyquist criterion is sufficient for most cases. The part of the locus that is significant is that closest to the critical point. For very complicated curves one should go back to the general case. The left-hand rule can be graphically derived from the generalised locus according to section A.2. The orthogonal (plane with the exception of a single or double pole at
(P, I or
behaviour). In this case the closed loop is only stable, if the critical point (-1,j0) is on the left hand-side of the locus
in the direction of increasing values of
.