Brookhaven Science Associates U.S. Department of Energy 1 Simulation of High-Intensity Pulsed Beam Targeting Roman Samulyak (October 20, 2009) AMS Department,

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Brookhaven Science Associates U.S. Department of Energy 1 Simulation of High-Intensity Pulsed Beam Targeting Roman Samulyak (October 20, 2009) AMS Department, Stony Brook University and Computational Science Center Brookhaven National Laboratory Collaborators: Wurigen Bo, Shuqiang Wang (Stony Brook) Harold Kirk (BNL), Kirk McDonald (Princeton) Workshop on Applications of High Intensity Proton Accelerators October , 2009, FNAL

Brookhaven Science Associates U.S. Department of Energy Talk Overview n Simulation of mercury jet target: main goals n FronTier code for multiphase, multiphysics simulations Typical applications of the FronTier code related to energy research n Simulation of liquid mercury jet target for Neutrino Factory / Muon Collider and comparison with MERIT experiment

Brookhaven Science Associates U.S. Department of Energy 3 Motivation of the Present Study of the Mercury Target Understanding of the hydrodynamic response of the mercury target and explanation of all details of MERIT data is necessary for the future target design Using improved 3D FrontTier capabilities, perform new series of full 3D simulations of the mercury target with resolved all relevant physics processes Perform full benchmark of simulations with MERIT data and fine-tune FronTier models After the benchmark, FronTier can be used for reliable predictions of future targets.

Brookhaven Science Associates U.S. Department of Energy 4 Mercury Jet Target for Neutrino Factory / Muon Collider Jet disruptions Top: experiment Bottom: simulation Target schematic Target is a mercury jet interacting with a proton pulse in a magnetic field Target converts protons to pions that decay to muons and neutrinos or to neutrons (accelerator based neutron sources) Understanding of the target hydrodynamic response is critical for design Studies of surface instabilities, jet breakup, and cavitation MHD forces reduce both jet expansion, instabilities, and cavitation

Brookhaven Science Associates U.S. Department of Energy 5 Front Tracking: A hybrid of Eulerian and Lagrangian methods Advantages of explicit interface tracking: No numerical interfacial diffusion Real physics models for interface propagation Different physics / numerical approximations in domains separated by interfaces Two separate grids to describe the solution: 1.A volume filling rectangular mesh 2.An unstructured codimension-1 Lagrangian mesh to represent interface Main Ideas of Front Tracking Major components: 1.Front propagation and redistribution 2.Wave (smooth region) solution

Brookhaven Science Associates U.S. Department of Energy 6 FronTier is a parallel 3D multiphysics code based on front tracking Being developed within DOE SciDAC program Adaptive mesh refinement Physics models include Compressible and incompressible fluid dynamics, MHD Flows in porous media Phase transitions and turbulence models The FronTier Code Turbulent fluid mixing. Left: 2D Right: 3D (fragment of the interface)

Brookhaven Science Associates U.S. Department of Energy 7 ITER is a joint international research and development project that aims to demonstrate the scientific and technical feasibility of fusion power ITER will be constructed in Europe, at Cadarache in the South of France in ~10 years Fusion Energy. ITER project: fuel pellet ablation Models and simulations of tokamak fueling through the ablation of frozen D 2 pellets Collaboration with General Atomics Our contribution:

Brookhaven Science Associates U.S. Department of Energy 8 New Ideas in Nuclear Fusion: Palsma Jet Induced Magneto Inertial Fusion

Brookhaven Science Associates U.S. Department of Energy 9 FronTier Application: NERI Collaboration of RPI, SBU, Columbia, and BNL. Fuel Rod Failures in Sodium Coled Reactors NPHASE-CMFD code uses Reynolds-Averaged Navier Stokes (RANS, e.g. k-ε model) approach to multiphase modeling Flow of liquid sodium coolant and fission gas around l reactor fuel rods PHASTA uses direct numerical simulation (DNS) with Level Set method to track the interface between gas and liquid phases Jet of high pressure fission gas entering coolant channels FronTier is a front tracking code capable of simulating multiphase compressible fluid dynamics Fuel rod overheating and melting of cladding in case of coolant-blockage accident Molecular Dynamics approach analyses the irradiated fuel properties Prediction of fuel properties evolution NERI PROJECT NO

Brookhaven Science Associates U.S. Department of Energy 10 Simulations of the mercury jet entrance into the magnetic field

Brookhaven Science Associates U.S. Department of Energy 11 Distortion of the jet entering 15 T solenoid B = 15 T V0 = 25 m/s Top: Aspect ration of the jet entering 15 T solenoid

Brookhaven Science Associates U.S. Department of Energy 12 R. Samulyak et. al, Journal of Computational Physics, 226 (2007), Comparison with the theory and other experiments (Oshima et al) Obtained an excellent agreement with theory and experiments (Oshima at al) on the jet distortion MERIT target simulations by FronTier agreed well with HyperMAG simulations (Neal Morley)

Brookhaven Science Associates U.S. Department of Energy 13 Predicted jet distortion in three view ports (MERIT experiment) vp1 vp2 vp3 Our simulations underestimeted the jet distortion. Some other factors need to be resolved

Brookhaven Science Associates U.S. Department of Energy 14 Simulations only qualitatively explain the width of the jet in different view ports. Experimental data V = 15 m/s, B = 10TV = 20 m/s, B = 10T B = 15T

Brookhaven Science Associates U.S. Department of Energy 15 Simulations of the mercury jet interaction with proton pulses

Brookhaven Science Associates U.S. Department of Energy 3D Simuation of Jet Ejection from a Nozzle. High Speed Jet Cavitation, Breakup and Atomization We evaluated the influence of the initial jet turbulence on jet disruption due to the interaction with the proton pulse Initial turbulence is negligible compared to proton pulse induced instabilities As a result, most of runs are done with idealized initial jet

Brookhaven Science Associates U.S. Department of Energy 17 Simulation setup for proton-jet interaction Elliptic jet: Major radius = 0.8cm Minor radius = 0.3cm Striganov’s Energy deposition calculation for 14Gev, 10T proton beam is used. The peak pressure is 12,050 bar. Initial pressure distribution

Brookhaven Science Associates U.S. Department of Energy 18 Evolution of the jet surface and cavitation bubbles for B=5T

Brookhaven Science Associates U.S. Department of Energy 19 Positions for the filament length calculation To obtain the expansion velocity along the jet surface, we evaluate the expansion length in 4 typical positions.

Brookhaven Science Associates U.S. Department of Energy 20 MHD Stabilizing Effect Right: From top to bottom, the jet surface at 150 microsecond under longitudinal magnetic field. Both the interior velocity and the surface velocity of the jet are decreasing with the increasing magnetic field. The MHD stabilizing effect is weaker than in the corresponding 2D simulations where circular current exists in filaments. Image from the experiment, B=10T 5T 0T 10T 15T

Brookhaven Science Associates U.S. Department of Energy 21 No magnetic field

Brookhaven Science Associates U.S. Department of Energy 22 B=5T

Brookhaven Science Associates U.S. Department of Energy 23 B=10T

Brookhaven Science Associates U.S. Department of Energy 24 B=15T

Brookhaven Science Associates U.S. Department of Energy 25 Maximum length of expansion for B=15T under mesh refinement. Mesh refinement

Brookhaven Science Associates U.S. Department of Energy 26 The velocity of filaments in the major axis of the ellipse for different magnetic fields.

Brookhaven Science Associates U.S. Department of Energy 27 The velocity of filaments in the major axis of the ellipse for different magnetic fields: comparison of experiments and simulations

Brookhaven Science Associates U.S. Department of Energy 28 Large (~25 microsecond) delay in the formation of filaments was not observed in simulations. Currently the nature of this delay is not understood. Delay in the formation of filaments

Brookhaven Science Associates U.S. Department of Energy 29 Conclusions and Future Plan New robust algorithm for topological change of 3D surface, 3D bubble insertion method coupling with the MHD code enabled large scale 3D simulations with complex geometry. Performed simulations of mercury jets interacting with magnetic fields Observed good agreement with experiments on the filament velocity The delay of the filament formation was not observed in simulations. Need to clarify the physics of the observed delay of the jet disruption Further study of the jet entrance in the magnetic field will be performed and the contribution of several factors (velocity profile, turbulence etc) will be tested Comprehensive benchmark with MERIT experiments Simulations of mercury target at higher beam intensities Simulations of the mercury damp process Studies relevant to other target concepts (waterfall etc.)