2016
DOI: 10.1017/pasa.2016.45
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Grand Challenges in Protoplanetary Disc Modelling

Abstract: The Protoplanetary Discussions conference-held in Edinburgh, UK, from 2016 March 7th-11th-included several open sessions led by participants. This paper reports on the discussions collectively concerned with the multi-physics modelling of protoplanetary discs, including the self-consistent calculation of gas and dust dynamics, radiative transfer, and chemistry. After a short introduction to each of these disciplines in isolation, we identify a series of burning questions and grand challenges associated with th… Show more

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Cited by 69 publications
(34 citation statements)
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References 293 publications
(423 reference statements)
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“…There is now overwhelming evidence that planets form from discs of material around young stars (for reviews see e.g. Williams & Cieza 2011;Andrews 2015;Owen 2016;Sicilia-Aguilar et al 2016;Haworth et al 2016a;Ercolano & Pascucci 2017). The vast majority of studies of disc evolution and planet formation consider the young star-disc in isolation and such approaches are proving very effective at understanding the myriad physical processes that take place in planet-forming discs.…”
Section: Introductionmentioning
confidence: 99%
“…There is now overwhelming evidence that planets form from discs of material around young stars (for reviews see e.g. Williams & Cieza 2011;Andrews 2015;Owen 2016;Sicilia-Aguilar et al 2016;Haworth et al 2016a;Ercolano & Pascucci 2017). The vast majority of studies of disc evolution and planet formation consider the young star-disc in isolation and such approaches are proving very effective at understanding the myriad physical processes that take place in planet-forming discs.…”
Section: Introductionmentioning
confidence: 99%
“…The condition (2) is violated with our adopted grid computational method (h = 10c s t stop ), but it is possible to closely approach the exact solution by reducing the time step. Figure 2 presents the analogous results for the scheme (19)- (21) for various CF L values. The dot-dashed curves in the upper panels show the gas velocity that the medium would have if the dust exerted no influence on the gas dynamics.…”
Section: Numerical Solution Of the Dustywave Problemmentioning
confidence: 97%
“…The propagation of the sound wave is obtained with acceptable accuracy for both a stiffly coupled and weakly coupled medium. Thus, the condition (2) is not necessary for the piecewise-parabolic advection (PPA) method applied in conjunction with the scheme (19)- (21) or (23)- (24). It is clear that both of the approaches (19)-(21) and (23)-(24) enable the use of a time step determined from the Courant condition (37) for a two-phase medium without additional reduction (15) due to the appearance of the "short" time t stop .…”
Section: Numerical Solution Of the Dustywave Problemmentioning
confidence: 99%
“…where r 0 = 20 AU, St = 2 × 10 −3 . According to (7) under the conditions of a massive disk described in Section 2, this stopping time corresponds to an initial radius for the bodies of 2 − 3 mm. The migration of bodies in the inner region of the disk in a regime in which the stopping time remains constant implies that the radius of solid-phase particles grows in accordance with a law that depends on the surface density and radius.…”
Section: Migration Of a Ringmentioning
confidence: 99%