# MHD simulations of the formation and propagation of protostellar jets to observational length scales

## TL;DR

This paper presents detailed 2.5-D MHD simulations of protostellar jets, revealing their structure, dynamics, and scaling laws, and demonstrating how magnetic fields influence jet formation and propagation to observable scales.

## Contribution

It introduces a comprehensive simulation framework that models the formation and evolution of protostellar jets, highlighting the roles of magnetic fields and launching mechanisms in reproducing observed jet properties.

## Key findings

- Jet structure includes a core, sheath, and ambient medium.
- Power-law relationships between magnetic field strength and jet speed.
- Jets are launched by magnetic tower and bead-on-a-wire mechanisms.

## Abstract

We present 2.5-D global, ideal MHD simulations of magnetically and rotationally driven protostellar jets from Keplerian accretion discs, wherein only the initial magnetic field strength at the inner radius of the disc, $B_{\rm i}$, is varied. Using the AMR-MHD code AZEUS, we self-consistently follow the jet evolution into the observational regime ($>10^3\,\mathrm{AU}$) with a spatial dynamic range of $\sim6.5\times10^5$. The simulations reveal a three-component outflow: 1) A hot, dense, super-fast and highly magnetised 'jet core'; 2) a cold, rarefied, trans-fast and highly magnetised 'sheath' surrounding the jet core and extending to a tangential discontinuity; and 3) a warm, dense, trans-slow and weakly magnetised shocked ambient medium entrained by the advancing bow shock. The simulations reveal power-law relationships between $B_{\rm i}$ and the jet advance speed, $v_{\rm jet}$, the average jet rotation speed, $\langle v_\varphi\rangle$, as well as fluxes of mass, momentum, and kinetic energy. Quantities that do not depend on $B_{\rm i}$ include the plasma-$\beta$ of the transported material which, in all cases, seems to asymptote to order unity. Jets are launched by a combination of the 'magnetic tower' and 'bead-on-a-wire' mechanisms, with the former accounting for most of the jet acceleration---even for strong fields---and continuing well beyond the fast magnetosonic point. At no time does the leading bow shock leave the domain and, as such, these simulations generate large-scale jets that reproduce many of the observed properties of protostellar jets including their characteristic speeds and transported fluxes.