  We calculate the jet power of the classical Blandford-Znajek(BZ) model and
hybrid model developed by Meier based on the global solutions of advection
dominated accretion flows (ADAFs) surrounding Kerr black holes. We find that
the jet power of the hybrid model is larger than that of the pure BZ model. The
jet power will dominate over the accretion power, and the objects will enter
into "jet-power-dominated advective systems", when the accretion rate is less
than a critical value mdot_c=Mdot_c/Mdot_Edd, where 3*10^-4 < mdot_c < 5*10^-3
is a function of black hole spin parameter. The accretion power will be
dominant when mdot<mdot_c and the objects will enter into
"accretion-power-dominated advective systems." This is roughly consistent with
that constrained from the low/hard-state black hole X-ray binaries (e.g.,
Fender et al.). We calculate the maximal jet power as a function of black hole
mass with the hybrid jet formation model, and find it can roughly reproduce the
dividing line of the Ledlow-Owen relation for FR I/FR II dichotomy in the jet
power-black hole(BH) mass plane (Q_jet-M_BH) if the dimensionless accretion
rate mdot~0.01 and BH spin parameter j~0.9-0.99 are adopted. This accretion
rate mdot~0.01 is consistent with that of the critical accretion rate for the
accretion mode transition of a standard disk to an ADAF constrained from the
state transition of X-ray binaries. Our results imply that most FR I galaxies
may be in the ADAF accretion mode similar to the low/hard-state XRBs.
