6533b7d5fe1ef96bd126460f

RESEARCH PRODUCT

On the deceleration of Fanaroff–Riley Class I jets: mass loading by stellar winds

Robert LaingManel PeruchoJosé-maría MartíPhilip E. Hardee

subject

PhysicsStellar mass010308 nuclear & particles physicsRadio galaxyAstrophysics::High Energy Astrophysical PhenomenaMolecular cloudAstronomyAstronomy and AstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicsKinetic energy01 natural sciencesSpace and Planetary ScienceStellar mass loss0103 physical sciencesElliptical galaxyEntrainment (chronobiology)010303 astronomy & astrophysicsAstrophysics::Galaxy AstrophysicsRelativistic speed

description

Jets in low-luminosity radio galaxies are known to decelerate from relativistic speeds on parsec scales to mildly or sub-relativistic speeds on kiloparsec scales. Several mechanisms have been proposed to explain this effect, including strong reconfinement shocks and the growth of instabilities (both leading to boundary-layer entrainment) and mass loading from stellar winds or molecular clouds. We have performed a series of axisymmetric simulations of the early evolution of jets in a realistic ambient medium to probe the effects of mass loading from stellar winds using the code Ratpenat. We study the evolution of Fanaroff-Riley Class I (FRI) jets, with kinetic powers L_j \sim 1.e41-1.e44 erg/s, within the first 2 kpc of their evolution, where deceleration by stellar mass loading should be most effective. Mass entrainment rates consistent with present models of stellar mass loss in elliptical galaxies produce deceleration and effective decollimation of weak FRI jets within the first kiloparsec. However, powerful FRI jets are not decelerated significantly. In those cases where the mass loading is important, the jets show larger opening angles and decollimate at smaller distances, but the overall structure and dynamics of the bow-shock are similar to those of unloaded jets with the same power and thrust. According to our results, the flaring observed on kpc scales is initiated by mass loading in the weaker FRI jets and by reconfinement shocks or the growth of instabilities in the more powerful jets. The final mechanism of decollimation and deceleration is always the development of disruptive pinching modes.

https://doi.org/10.1093/mnras/stu676