1998
DOI: 10.1086/306117
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The Dynamics of Heavy Gaseous Disks

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Cited by 76 publications
(93 citation statements)
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References 27 publications
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“…spiral activity can be easily recognized at t ≈ 1.5t0, t ≈ 4t0 and t ≈ 6t0. A similar cyclic behaviour, with a modulation of the amplitude of the dominant m = 2 mode, has been found in previous simulations of self-gravitating discs (Sellwood & Carlberg 1984;Laughlin & Bodenheimer 1994;Laughlin et al 1998). Laughlin et al (1998) have attributed this behaviour to the effect of non-linear coupling between different modes.…”
Section: The M Disc = 1m⋆ Casesupporting
confidence: 84%
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“…spiral activity can be easily recognized at t ≈ 1.5t0, t ≈ 4t0 and t ≈ 6t0. A similar cyclic behaviour, with a modulation of the amplitude of the dominant m = 2 mode, has been found in previous simulations of self-gravitating discs (Sellwood & Carlberg 1984;Laughlin & Bodenheimer 1994;Laughlin et al 1998). Laughlin et al (1998) have attributed this behaviour to the effect of non-linear coupling between different modes.…”
Section: The M Disc = 1m⋆ Casesupporting
confidence: 84%
“…In particular, here we describe the results of two new simulations, in which the disc mass is of the same order of the central object mass, namely M disc = 0.5M⋆ and M disc = 1M⋆. Given the specific region of the parameter space that we explore, our simulations have two previous analogues: the N -body simulations by Sellwood & Carlberg (1984), who mimicked the cooling of the stellar component of a galaxy disc through continuous accretion of stars, and a series of simulations by Laughlin et al (Laughlin & Bodenheimer 1994;Laughlin et al 1997Laughlin et al , 1998, who simulated massive gaseous disc, adopting simple equations of state (mostly isothermal) without any spe-cific cooling. The main difference between the latter simulations and those presented here lies in the way we handle the disc thermodynamics.…”
Section: Discussionmentioning
confidence: 99%
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“…In the disc region 10 −2 AU x 1AU Toomre's Q value is Q ∼ 2 − 3. As pointed out in previous studies, the disc becomes unstable against non-axisymmetric perturbations when Q ∼ 1.5 and the spiral arms develop (Laughlin, Korchagin & Adams 1998). The spiral arms invoke an angular momentum transfer.…”
Section: Rotationally Supported Disc Around Protostarsupporting
confidence: 56%
“…Thus, amplitude is naturally spread from lower order to higher order as the available m-values increase. Indeed, even if the disk is dominated by a few low-order modes at the time of outburst, this power spreads to all m-values in the nonlinear regime (for example Laughlin et al 1997Laughlin et al , 1998Laughlin & Rozyczka 1996).…”
Section: Non-axisymmetric Structurementioning
confidence: 99%