2013
DOI: 10.1051/0004-6361/201321613
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Fluctuation dynamo amplified by intermittent shear bursts in convectively driven magnetohydrodynamic turbulence

Abstract: Intermittent large-scale high-shear flows are found to occur frequently and spontaneously in direct numerical simulations of statistically stationary turbulent Boussinesq magnetohydrodynamic (MHD) convection. The energetic steady state of the system is sustained by convective driving of the velocity field and small-scale dynamo action. The intermittent emergence of flow structures with strong velocity and magnetic shearing generates magnetic energy at an elevated rate on time scales that are longer than the ch… Show more

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Cited by 23 publications
(17 citation statements)
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“…Remarkably, we obtain from DNS the same scaling, γ(S) ∝ |S| 2/3 , for SSD growth rate as was theoretically predicted by Kolokolov et al (2011) for a given velocity field. Interestingly, the occurrences of intermittent shear bursts were found to amplify the growth of the SSD in turbulent magnetoconvection (Pratt et al 2013).…”
Section: Discussionmentioning
confidence: 99%
“…Remarkably, we obtain from DNS the same scaling, γ(S) ∝ |S| 2/3 , for SSD growth rate as was theoretically predicted by Kolokolov et al (2011) for a given velocity field. Interestingly, the occurrences of intermittent shear bursts were found to amplify the growth of the SSD in turbulent magnetoconvection (Pratt et al 2013).…”
Section: Discussionmentioning
confidence: 99%
“…We investigate three different types of turbulent systems: forced homogeneous isotropic Navier-Stokes turbulence (simulation NST) [43], Boussinesq convection in a neutral fluid (simulation HC), and Boussinesq convection in an electrically conducting fluid (simulation MC) [12,44]. These simulations are not designed for close comparison, but produced for a broad exploration of the convex hull analysis.…”
Section: Simulationsmentioning
confidence: 99%
“…However, in astrophysical environments where the effects of magnetic fields, rotation, or gravity are often significant, the more complex nature of statistically anisotropic or even inhomogenous nonlinear dynamics warrants additional examination. Dispersion in dynamically anisotropic systems such as vigorously convecting flows [12][13][14][15][16] where preferred directions exist and spatially coherent, persistent structures like convective plumes can form, motivates the present consideration of a complementary diagnostic based on a different Lagrangian concept: the convex hull [17] of a n-particle group (n 4  ). The convex hull is the smallest convex polygon that encloses a group of particles; two dimensional convex hulls are pictured in figure 1.…”
Section: Introductionmentioning
confidence: 99%
“…In this paper, we consider the following 2D incompressible Boussinesq equations for magnetohydrodynamics (MHD) convection with stratification effects [5,6,48]:              ∂ t θ + u · ∇θ − div(κ(θ)∇θ)) = −u 2 T ′ 0 (x 2 ), ∂ t u + u · ∇u − div(µ(θ)∇u) + ∇Π = θe 2 + J B ⊥ , ∂ t B + u · ∇B − ∇ ⊥ (σ(θ)J) = B · ∇u, divu = div B = 0.…”
Section: Introduction and Main Resultsmentioning
confidence: 99%