Abstract:The magnetic Rayleigh-Taylor instability is a fundamental instability of many astrophysical systems, and recent observations are consistent with this instability developing in solar prominences. Prominences are cool, dense clouds of plasma that form in the solar corona that display a wide range of dynamics of a multitude of spatial and temporal scales, and two different phenomena that have been discovered to occur in prominences can be understood as resulting from the Rayleigh-Taylor instability. The first is … Show more
“…We have discussed the role that mass plays in the global evolution and eruption of flux ropes, suggesting that it depends on four main parameters; the strength of the surface field generating the background potential field, how much mass is loaded into a flux rope, how much mass drains during its evolution, and when along a flux rope's equilibrium curve the mass drains. The effect of the local evolution of plasma within prominences is not discussed in this manuscript, i.e., the mass-draining that is studied here differs from the massloss due to the Rayleigh-Taylor instability (RTI) that has been studied extensively in both observations and simulations (e.g., Hillier et al 2012;Xia & Keppens 2016;Hillier 2018). In addition, Kaneko & Yokoyama (2018) pointed out that, in their case, the mass-loss from the prominence due to RTI was balanced by new condensations into the prominence.…”
Quiescent solar prominences are observed to exist within the solar atmosphere for up to several solar rotations. Their eruption is commonly preceded by a slow increase in height that can last from hours to days. This increase in the prominence height is believed to be due to their host magnetic flux rope transitioning through a series of neighbouring quasi-equilibria before the main loss-of-equilibrium that drives the eruption. Recent work suggests that the removal of prominence mass from a stable, quiescent flux rope is one possible cause for this change in height. However, these conclusions are drawn from observations and are subject to interpretation. Here we present a simple model to quantify the effect of "mass-draining" during the pre-eruptive height-evolution of a solar flux rope. The flux rope is modeled as a line current suspended within a background potential magnetic field. We first show that the inclusion of mass, up to 10 12 kg, can modify the height at which the line current experiences loss-of-equilibrium by up to 14%. Next, we show that the rapid removal of mass prior to the loss-of-equilibrium can allow the height of the flux rope to increase sharply and without upper bound as it approaches its loss-of-equilibrium point. This indicates that the critical height for the loss-of-equilibrium can occur at a range of heights depending explicitly on the amount and evolution of mass within the flux rope. Finally, we demonstrate that for the same amount of drained mass, the effect on the height of the flux rope is up to two order of magnitude larger for quiescent than for active region prominences.
“…We have discussed the role that mass plays in the global evolution and eruption of flux ropes, suggesting that it depends on four main parameters; the strength of the surface field generating the background potential field, how much mass is loaded into a flux rope, how much mass drains during its evolution, and when along a flux rope's equilibrium curve the mass drains. The effect of the local evolution of plasma within prominences is not discussed in this manuscript, i.e., the mass-draining that is studied here differs from the massloss due to the Rayleigh-Taylor instability (RTI) that has been studied extensively in both observations and simulations (e.g., Hillier et al 2012;Xia & Keppens 2016;Hillier 2018). In addition, Kaneko & Yokoyama (2018) pointed out that, in their case, the mass-loss from the prominence due to RTI was balanced by new condensations into the prominence.…”
Quiescent solar prominences are observed to exist within the solar atmosphere for up to several solar rotations. Their eruption is commonly preceded by a slow increase in height that can last from hours to days. This increase in the prominence height is believed to be due to their host magnetic flux rope transitioning through a series of neighbouring quasi-equilibria before the main loss-of-equilibrium that drives the eruption. Recent work suggests that the removal of prominence mass from a stable, quiescent flux rope is one possible cause for this change in height. However, these conclusions are drawn from observations and are subject to interpretation. Here we present a simple model to quantify the effect of "mass-draining" during the pre-eruptive height-evolution of a solar flux rope. The flux rope is modeled as a line current suspended within a background potential magnetic field. We first show that the inclusion of mass, up to 10 12 kg, can modify the height at which the line current experiences loss-of-equilibrium by up to 14%. Next, we show that the rapid removal of mass prior to the loss-of-equilibrium can allow the height of the flux rope to increase sharply and without upper bound as it approaches its loss-of-equilibrium point. This indicates that the critical height for the loss-of-equilibrium can occur at a range of heights depending explicitly on the amount and evolution of mass within the flux rope. Finally, we demonstrate that for the same amount of drained mass, the effect on the height of the flux rope is up to two order of magnitude larger for quiescent than for active region prominences.
“…2014). Further discussion of models of vertical flows in prominences, including a thorough review of prominence RT instability studies, can be found in Hillier (2018).…”
Section: Adding Flesh and Blood To The Skeleton: Incorporating Dynamimentioning
Magnetic fields suspend the relatively cool material of solar prominences in an otherwise hot corona. A comprehensive understanding of solar prominences ultimately requires complex and dynamic models, constrained and validated by observations spanning the solar atmosphere. We obtain the core of this understanding from observations that give us information about the structure of the “magnetic skeleton” that supports and surrounds the prominence. Energetically-sophisticated magnetohydrodynamic simulations then add flesh and blood to the skeleton, demonstrating how a thermally varying plasma may pulse through to form the prominence, and how the plasma and magnetic fields dynamically interact.
“…The Rayleigh-Taylor instability (RTI) is an important instability in many astrophysical and laboratory systems, such as supernova explosions (Hachisu et al 1992;Hester et al 1996;Porth et al 2014), solar prominences (Berger et al 2010;Ryutova et al 2010;Terradas et al 2015;Hillier 2018), and inertial confinement fusion (Takabe et al 1985;Betti et al 1998). RTI occurs when a heavy fluid is initially on top of a light fluid.…”
A hoop force driven magnetic Rayleigh-Taylor instability (MRTI) is observed in a laboratory experiment that simulates a solar coronal loop. Increase of the axial wavelength λ is observed when the axial magnetic field increases. This scaling is consistent with the theoretical MRTI growth rate (•) g m r = k B gk 2 2 0 2 0 , which implies that if k is parallel to B 0 (i.e., undular mode), the fastest-growing mode has l p p m r = = k B g 2 8 0 2 0. Unified Astronomy Thesaurus concepts: Magnetohydrodynamics (1964); Laboratory astrophysics (2004); Solar activity (1475); Solar corona (1483); Solar prominences (1519); Solar filaments (1495); Quiescent solar prominence (1321); Solar coronal plumes (2039); Solar coronal mass ejections (310); Space plasmas (1544)
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