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Published byChristine Chambers Modified over 9 years ago
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Type Ia Supernova: Turbulent Combustion on the Grandest Scale Deep inside a dying star in a galaxy far, far away, a carbon fusion flame ignites. Ignition may happen in the middle or displaced slightly to one side, but this simulation explores the consequences of central ignition. In a localized hot spot, represented here by a deformed sphere with an average radius of 100 km, carbon is assumed to have already fused to iron, producing hot ash (~ten billion K) with a density about 20% less than its surroundings. As the burning progresses, this hot buoyant ash rises up and interacts with cold fuel. Rayleigh-Taylor fingers give rise to shear and turbulence, which act back on the flame, causing it to move faster. In about two seconds, the energy released blows the entire white dwarf star up, leaving nothing behind but a rapidly expanding cloud of radioactive nickel, iron, and other heavy elements. A Type Ia supernova is born.
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Visualizing Coolant Flow in Sodium Fast Reactor Subassemblies Interchannel cross-flow is the principal cross-assembly energy transport mechanism for sodium fast reactors. For this design, uniformity temperatures enable peak power output. This Nek5000 simulation modeled the coolant for a 217 pin reactor, using an unstructured mesh with over one billion degrees of freedom per time slice. The visualization, done with VisIt, aimed to better understand the flow distribution, which is required for improving future designs.
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Turbulent Flow of Coolant in an Advanced Recycling Nuclear Reactor Here we see the turbulent flow of coolant into a mock- up of an advanced recycling nuclear reactor. The colors indicate the speed of the fluid, with red representing regions of high velocity and blue representing regions of low velocity. The simulation used 23 million grid points and represents 60 seconds of flow time.
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