1998
DOI: 10.1086/305099
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Instabilities in Three‐dimensional Simulations of Astrophysical Jets Crossing Tilted Interfaces

Abstract: Three-dimensional numerical simulations of light supersonic hydrodynamic jets have been performed to quantify the crucial roles of the interstellar medium (ISM) and intracluster medium (ICM) in deÐning the gross morphologies of powerful radio galaxies. Such a jet emerges through a power-law atmosphere (ISM) of its host galaxy and then crosses into a hotter, but less dense, ICM. Our eight mediumresolution simulations are followed to lengths of 45 initial jet radii. Simulations with di †erent jet velocities, jet… Show more

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Cited by 17 publications
(9 citation statements)
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“…The substantial difference between the two estimates was taken by Scheuer as evidence for a rapid 'backflow' of the relativistic plasma within the lobes, which is indeed expected if the jet material is much less dense than the ambient plasma. Such strong backflows are clearly observed in many numerical simulations of jet propagation (e.g., Norman 1996;Hooda & Wiita 1998).…”
Section: Further Constraining the Hot-spot Speeds By The Jet-sidednessmentioning
confidence: 80%
“…The substantial difference between the two estimates was taken by Scheuer as evidence for a rapid 'backflow' of the relativistic plasma within the lobes, which is indeed expected if the jet material is much less dense than the ambient plasma. Such strong backflows are clearly observed in many numerical simulations of jet propagation (e.g., Norman 1996;Hooda & Wiita 1998).…”
Section: Further Constraining the Hot-spot Speeds By The Jet-sidednessmentioning
confidence: 80%
“…For our calculations we choose θ = 0.1 rad, which is certainly justified as appropriate for the inner jet regions, particularly since it is now recognized that the jet's thrust acts on a larger area than the instantaneous hot spot (e.g., Scheuer's 1982 'dentist-drill', as supported by many threedimensional numerical simulations: Norman 1996; Clarke 1996; Hooda & Wiita 1998). Following Bicknell (1995), we further assume that the X-ray emitting ISM gas temperature is tied to the central stellar velocity dispersion, σ, via, kT = 2.2µm p σ 2 /δ, which is Fall's (1987) relation between circular velocity and σ.…”
Section: The Modelmentioning
confidence: 99%
“…The most novel assumption is the transition from low to high density across a contact interface (across which the pressure is necessarily constant), which is different from the work done by Hooda & Wiita (1998) where they used a classical code with a density decrease across the contact, and also different from the study by Loken et al (1993), where they used a classical code to look into jet propagation through a pressure wall. We explored the influence of a sudden density jump in ISM on jet propagation, stability, and formation of the bow shock.…”
Section: Introductionmentioning
confidence: 99%