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Our next plan is to formulate the most general model for accretion powered
relativistic MHD jet formation. We would like to start by
writing the relativistic energy momentum tensor
for compressible fluid with shear and bulk
viscosity, with mutual energy exchange in between internal fluid
elements and radiative energy exchange in between the fluid
and the surrounding. Practically, such an energy momentum tensor
should be the combination of the individual energy momentum tensors representing the matter field and
the Maxwell stress-energy tensor associated with the
field. We plan to use the
Boyar Lindquist co-ordinate with an azimuthally
Lorentz boosted orthonormal tetrad basis co-rotating with the
accreting fluid, and consider gravo-magneto-viscous
non-alignment between the specific flow angular momentum of accreting matter and
the black hole spin angular momentum (the Kerr parameter
)
to include the Bardeen Paterson Effect as well.
Solution of the above equation will lead to the equations governing the
energy, mass, and the linear and angular momentum of the accretion flow.
The next step would be to construct the representative equations for general
relativistic MHD shocks. Such set of
equations, which fully governs the flow,
will be highly non-linearly coupled and
non-exactly solvable. At this stage, numerical
techniques will be employed to simultaneously solve the set of equations
governing the accretion flow along with the relativistic MHD shock
conditions. Initially our work will concentrate on axisymmetric stationary
solutions to investigate the formation of standing shocks and to study
how such shock solutions produces outflow. Subsequently,
we will introduce time dependence in our solution scheme to study how
such shock oscillates (depending on the relative magnitude of the post-shock
cooling and advection time scale) to produce the quasi periodic
oscillation (QPO) in galactic
sources harbouring stellar mass black holes.
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Tapas Kumar Das
2009-01-17