TY - JOUR
T1 - Efficient acceleration of relativistic magnetohydrodynamic jets
AU - Toma, Kenji
AU - Takahara, Fumio
PY - 2013/8
Y1 - 2013/8
N2 - Relativistic jets in active galactic nuclei, galactic microquasars, and gamma-ray bursts are widely considered to be magnetohydrodynamically driven by black hole accretion systems, although the conversion mechanism from the Poynting into the particle kinetic energy flux is still open. Recent detailed numerical and analytical studies of global structures of steady, axisymmetric magnetohydrodynamic (MHD) flows with specific boundary conditions have not reproduced as rapid an energy conversion as required by observations. In order to find more suitable boundary conditions, we focus on the flow along a poloidal magnetic field line just inside the external boundary, without treating the transfield force balance in detail. We find some examples of the poloidal field structure and corresponding external pressure profile for an efficient and rapid energy conversion as required by observations, and that the rapid acceleration requires a rapid decrease of the external pressure above the accretion disk.We also clarify the differences between the fast magnetosonic point of the MHD flow and the sonic point of the de Laval nozzle.
AB - Relativistic jets in active galactic nuclei, galactic microquasars, and gamma-ray bursts are widely considered to be magnetohydrodynamically driven by black hole accretion systems, although the conversion mechanism from the Poynting into the particle kinetic energy flux is still open. Recent detailed numerical and analytical studies of global structures of steady, axisymmetric magnetohydrodynamic (MHD) flows with specific boundary conditions have not reproduced as rapid an energy conversion as required by observations. In order to find more suitable boundary conditions, we focus on the flow along a poloidal magnetic field line just inside the external boundary, without treating the transfield force balance in detail. We find some examples of the poloidal field structure and corresponding external pressure profile for an efficient and rapid energy conversion as required by observations, and that the rapid acceleration requires a rapid decrease of the external pressure above the accretion disk.We also clarify the differences between the fast magnetosonic point of the MHD flow and the sonic point of the de Laval nozzle.
UR - http://www.scopus.com/inward/record.url?scp=84884515618&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=84884515618&partnerID=8YFLogxK
U2 - 10.1093/ptep/ptt058
DO - 10.1093/ptep/ptt058
M3 - Article
AN - SCOPUS:84884515618
SN - 2050-3911
VL - 2013
JO - Progress of Theoretical and Experimental Physics
JF - Progress of Theoretical and Experimental Physics
IS - 8
M1 - 083E02
ER -