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posted:
11/3/2011
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Lead Name - Dean Townsley



Institutions - DOE NNSA/ASC Flash Center at the University of Chicago and Argonne

National Laboratory ALCF (project supported under the 2008 INCITE award program)



Contributors (in alphabetical order) - Ray Bair, Anshu Dubey Robert Fisher, Nathan

Hearn, Don Lamb, Katherine Riley



Title - Buoyancy-Driven Turbulent Nuclear Combustion



Abstract :



A fundamental challenge in our understanding of reactive flows is the process by which

turbulence wrinkles a combustive flame front, thereby increasing its surface area and

effective flame speed. In particular, the mechanism of buoyancy-driven turbulent

combustion is central to our understanding of the explosion mechanism of Type Ia

supernovae, which in turn play a key role in our understanding of the expansion of the

universe and the nature of dark energy.



We will present a visualization which demonstrates that turbulence develops behind the

surface of the flame, but the flame surface itself is effectively ``polished" by the action of

the flame, and is smooth beneath a certain critical scale. In addition, the turbulence

behind the flame front is inhomogeneous and non-steady, in contrast to the assumptions

made by many theoretical models of turbulent burning. This visualization clearly

demonstrates this complex result, which has significant ramifications for the modeling of

turbulence nuclear flames in Type Ia supernovae.



Caption:



These four frames represent three different ways of visualizing the same snapshot of a

simulation of buoyancy-driven turbulent reactive flow; each is complementary to the rest

and distinctively insightful. In this 3-D simulation, an initially planar flame surface

perturbed with a multimode perturbation burns its way upward through a stratified

medium under conditions characteristic of the nuclear-degenerate material at the central

density of a near-Chandrasekhar mass C/O white dwarf. Gravity is directed downward.



The leftmost frame visualizes the flame surface itself. The simulation tracks the surface

of the flame through the evolution of a scalar advection diffusion reaction equation; this

frame depicts an isocontour of this scalar at the flame surface. The next two frames to the

right present volume renderings of the velocity field, and the enstrophy. Here the

baroclinic mechanism leads to the generation of vorticity at the flame surface. The

magnitude of the turbulent velocities drop off behind the flame front over an integral

length scale. The rightmost frame shows the progression of the flame through the

computational domain.



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