We consider stationary, axisymmetric hydrodynamic accretion flows in Kerr
geometry. As a plausible means of efficiently separating a small population of
nonthermal particles from the bulk accretion flows, we investigate the
formation of standing dissipative shocks, i.e. shocks at which fraction of the
energy, angular momentum and mass fluxes do not participate in the shock
transition of the flow that accretes onto the compact object but are lost into
collimated (jets) or uncollimated (winds) outflows. The mass loss fraction (at
a shock front) is found to vary over a wide range (0 - 95%) depending on flow's
angular momentum and energy. On the other hand, the associated energy loss
fraction appears to be relatively low (<1%) for a flow onto a non-rotating
black hole case, whereas the fraction could be an order of magnitude higher
(<10%) for a flow onto a rapidly-rotating black hole. By estimating the escape
velocity of the outflowing particles with a mass-accretion rate relevant for
typical active galactic nuclei, we find that nearly 10% of the accreting mass
could escape to form an outflow in a disk around a non-rotating black hole,
while as much as 50% of the matter may contribute to outflows in a disk around
a rapidly-rotating black hole. In the context of disk-jet paradigm, our model
suggests that shock-driven outflows from accretion can occur in regions not too
far from a central engine. Our results imply that a shock front under some
conditions could serve as a plausible site where (nonthermal) seed particles of
the outflows (jets/winds) are efficiently decoupled from bulk accretion.Comment: 25 pages, 10 black&white figures, Accepted to Ap