Abstract

Any gravitating mass traversing a relatively sparse gas experiences a retarding force created by its disturbance of the surrounding medium. In a previous contribution (Lee & Stahler 2011), we determined this dynamical friction force when the object's velocity was subsonic. We now extend our analysis to the supersonic regime. As before, we consider small perturbations created in the gas far from the gravitating object, and thereby obtain the net influx of linear momentum over a large, bounding surface. Various terms in the perturbation series formally diverge, necessitating an approximate treatment of the flow streamlines. Nevertheless, we are able to derive exactly the force itself. As in the subsonic case, we find that F=Mdot*V, where Mdot is the rate of mass accretion onto the object and V its instantaneous velocity with respect to distant background gas. Our force law holds even when the object is porous (e.g., a galaxy) or is actually expelling mass in a wind. Quantitatively, the force in the supersonic regime is less than that derived analytically by previous researchers, and is also less than was found in numerical simulations through the mid 1990s. We urge simulators to revisit the problem using modern numerical techniques. Assuming our result to be correct, it is applicable to many fields of astrophysics, ranging from exoplanet studies to galactic dynamics.

Highlights

  • Whenever a massive object passes through a rarefied medium, it draws surrounding matter toward it. This material creates an overdense wake behind the object that exerts its own gravitational pull, retarding the original motion. Such dynamical friction arises whether the medium consists of non-interacting point particles, e.g., a stellar cluster, or a continuum fluid, e.g., an interstellar cloud

  • Those found a greater force than we derive in the supersonic regime; we indicate possible causes for this discrepancy

  • Stahler: Dynamical friction in a gas uniform density, which we denote as ρ0

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Summary

Introduction

Whenever a massive object passes through a rarefied medium, it draws surrounding matter toward it. Ostriker (1999) calculated the force by integrating directly over the wake, whose density she obtained through a linear perturbation analysis These researchers focused principally on the supersonic case, which is often the most interesting one astrophysically. Any determination of the force by an asymptotic surface integration cannot tease apart these two contributions The true flow around the gravitating mass is, well-defined everywhere, and the divergences indicate that the adopted series expansions fail at certain locations Despite this mathematical inconvenience, we are able once again to derive the dynamical friction force through spatial integration of the linear momentum influx.

Physical assumptions
Mathematical formulation
Upstream and downstream regions
Intermediate region
Vorticity
Dynamical equations
Near-cone divergence
Mass accretion
Enforcing smoothness
Sample results
Integration of the momentum flux
Comparison with simulations
F M V cd 2 racc reff
Applications of the new force law
Discussion

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