55 research outputs found
Relativistic parsec-scale jets: I. Particle acceleration
We develop a theory of particle acceleration inside relativistic rotating
electron-positron force-free jets with spiral magnetic fields. We considered
perturbation of the stationary magnetic field structure and found that
acceleration takes place in the regions where the Alfven resonant condition
with the eigenmodes in the jet is fulfilled, i.e. where the local Alfven speed
is equal to the phase speed of an eigenmode. The acceleration mechanism is
regular acceleration by the electric field of the electromagnetic wave, which
is the eigenmode of the force-free cylindrical jet: particles drift out of the
region of the large wave amplitude near the Alfven resonant surface and gain
energy. Acceleration in the strong electric field near the Alfven resonance and
synchrotron losses combine to form a power-law energy spectrum of
ultra-relativistic electrons and positrons with index between 2 and 3 depending
upon the initial energy of the injected particles. The power law distribution
ranges from 10 MeV to 1000 MeV.Comment: 14 pages, 4 figures; Astron. Astrophys. in pres
Magnetorotational Instability in Liquid Metal Couette Flow
Despite the importance of the magnetorotational instability (MRI) as a
fundamental mechanism for angular momentum transport in magnetized accretion
disks, it has yet to be demonstrated in the laboratory. A liquid sodium
alpha-omega dynamo experiment at the New Mexico Institute of Mining and
Technology provides an ideal environment to study the MRI in a rotating metal
annulus (Couette flow). A local stability analysis is performed as a function
of shear, magnetic field strength, magnetic Reynolds number, and turbulent
Prandtl number. The later takes into account the minimum turbulence induced by
the formation of an Ekman layer against the rigidly rotating end walls of a
cylindrical vessel. Stability conditions are presented and unstable conditions
for the sodium experiment are compared with another proposed MRI experiment
with liquid gallium. Due to the relatively large magnetic Reynolds number
achievable in the sodium experiment, it should be possible to observe the
excitation of the MRI for a wide range of wavenumbers and further to observe
the transition to the turbulent state.Comment: 12 pages, 22 figures, 1 table. To appear in the Astrophysical Journa
Magnetized Ekman Layer and Stewartson Layer in a Magnetized Taylor-Couette Flow
In this paper we present axisymmetric nonlinear simulations of magnetized
Ekman and Stewartson layers in a magnetized Taylor-Couette flow with a
centrifugally stable angular-momemtum profile and with a magnetic Reynolds
number below the threshold of magnetorotational instability. The magnetic field
is found to inhibit the Ekman suction. The width of the Ekman layer is reduced
with increased magnetic field normal to the end plate. A uniformly-rotating
region forms near the outer cylinder. A strong magnetic field leads to a steady
Stewartson layer emanating from the junction between differentially rotating
rings at the endcaps. The Stewartson layer becomes thinner with larger Reynolds
number and penetrates deeper into the bulk flow with stronger magnetic field
and larger Reynolds number. However, at Reynolds number larger than a critical
value , axisymmetric, and perhaps also nonaxisymmetric, instabilities
occur and result in a less prominent Stewartson layer that extends less far
from the boundary.Comment: 24 pages, 12 figures, accepted by PRE, revision according to referee
A Magnetic Alpha-Omega Dynamo in Active Galactic Nuclei Disks: I. The Hydrodynamics of Star-Disk Collisions and Keplerian Flow
A magnetic field dynamo in the inner regions of the accretion disk
surrounding the supermassive black holes in AGNs may be the mechanism for the
generation of magnetic fields in galaxies and in extragalactic space. We argue
that the two coherent motions produced by 1) the Keplerian motion and 2)
star-disk collisions, numerous in the inner region of AGN accretion disks, are
both basic to the formation of a robust, coherent dynamo and consequently the
generation of large scale magnetic fields. They are frequent enough to account
for an integrated dynamo gain, e^{10^{9}} at 100 gravitational radii of a
central black hole, many orders of magnitude greater than required to amplify
any seed field no matter how small. The existence of extra-galactic, coherent,
large scale magnetic fields whose energies greatly exceed all but massive black
hole energies is recognized. In paper II (Pariev, Colgate, and Finn 2006) we
argue that in order to produce a dynamo that can access the free energy of
black hole formation and produce all the magnetic flux in a coherent fashion
the existence of these two coherent motions in a conducting fluid is required.
The differential winding of Keplerian motion is obvious, but the disk structure
depends upon the model of "alpha", the transport coefficient of angular
momentum chosen. The counter rotation of driven plumes in a rotating frame is
less well known, but fortunately the magnetic effect is independent of the disk
model. Both motions are discussed in this paper, paper I. The description of
the two motions are preliminary to two theoretical derivations and one
numerical simulation of the alpha-omega dynamo in paper II. (Abridged)Comment: 34 pages, 1 figure, accepted by Ap
Relativistic parsec-scale jets: II. Synchrotron emission
We calculate the optically thin synchrotron emission of fast electrons and
positrons in a spiral stationary magnetic field and a radial electric field of
a rotating relativistic strongly magnetized force-free jet consisting of
electron-positron pair plasma. The magnetic field has a helical structure with
a uniform axial component and a toroidal component that is maximal inside the
jet and decreasing to zero towards the boundary of the jet. Doppler boosting
and swing of the polarization angle of synchrotron emission due to the
relativistic motion of the emitting volume are calculated. The distribution of
the plasma velocity in the jet is consistent with the electromagnetic field
structure. Two spatial distributions of fast particles are considered: uniform,
and concentrated in the vicinity of the Alfven resonance surface. The latter
distribution corresponds to the regular acceleration by an electromagnetic wave
in the vicinity of its Alfven resonance surface inside the jet. The
polarization properties of the radiation have been obtained and compared with
the existing VLBI polarization measurements of parsec-scale jets in BL Lac
sources and quasars. Our results give a natural explanation of the observed
bimodality in the alignment between the electric field vector of the polarized
radiation and the projection of the jet axis on the plane of the sky. We
interpret the motion of bright knots as a phase velocity of standing spiral
eigenmodes of electromagnetic perturbations in a cylindrical jet. The degree of
polarization and the velocity of the observed proper motion of bright knots
depend upon the angular rotational velocity of the jet. The observed
polarizations and velocities of knots indicate that the magnetic field lines
are bent in the direction opposite to the direction of the jet rotation.Comment: 14 pages, 5 figures, Astron. Astroph. in pres
Line Emission from an Accretion Disk around a Black hole: Effects of Disk Structure
The observed iron K-alpha fluorescence lines in Seyfert-1 galaxies provide
strong evidence for an accretion disk near a supermassive black hole as a
source of the line emission. These lines serve as powerful probes for examining
the structure of inner regions of accretion disks. Previous studies of line
emission have considered geometrically thin disks only, where the gas moves
along geodesics in the equatorial plane of a black hole. Here we extend this
work to consider effects on line profiles from finite disk thickness, radial
accretion flow and turbulence. We adopt the Novikov and Thorne (1973) solution,
and find that within this framework, turbulent broadening is the dominant new
effect. The most prominent change in the skewed, double-horned line profiles is
a substantial reduction in the maximum flux at both red and blue peaks. The
effect is most pronounced when the inclination angle is large, and when the
accretion rate is high. Thus, the effects discussed here may be important for
future detailed modeling of high quality observational data.Comment: 21 pages including 8 figures; LaTeX; ApJ format; accepted by ApJ;
short results of this paper appeared before as a conference proceedings
(astro-ph/9711214
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