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  • Online publication date: June 2016

9 - Laser Driven Turbulence in High Energy Density Physics and Inertial Confinement Fusion Experiments

from Part III - Complex Mixing Consequences

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[1]Welser-Sherrill, L., Fincke, J., Doss, F., Loomis, E., Flippo, K., Offermann, D., Keiter, P., Haines, B.M., and Grinstein, F.F.. “Two laser-driven mix experiments to study reshock and shear.” High Energy Density Physics Journal 9(3):496499, 2013.
[2]Haines, B.M., Grinstein, F.F., Welser–Sherrill, L., and Fincke, J. R.. “Simulations of material mixing in laser-driven reshock experiments.” Phys. Plasmas 20:022309, 2013.
[3]Haines, B.M., Grinstein, F.F., Welser–Sherrill, L., Fincke, J.R., and Doss, F. W.. “Simulation ensemble for a laser-driven shear experiment.” Phys. Plasmas 20:092301, 2013.
[4]Haines, B.M., Grinstein, F.F., and Fincke, J.R.. “Three-dimensional simulation strategy to determine the effects of turbulent mixing on inertial-confinement-fusion capsule performance.” Physical Review E, 89:053302, 2014.
[5]Ho, C.-M. and Huerre, P.. “Perturbed free shear layers.” Ann. Rev. Fluid Mech. 16:365424, 1984.
[6]Williamson, C.H.K.. “Vortex dynamics in the cylinder wake.” Annu. Rev. Fluid. Mech. 28:477539, 1996.
[7]Gutmark, E.J. and Grinstein, F.F.. “Flow control with noncircular jets.” Annu. Rev. Fluid Mech. 31:239272, 1999.
[8]Grinstein, F.F.. “Vortex dynamics and transition to turbulence in free shear flows,” in Implicit Large Eddy Simulation: Computing Turbulent Flow Dynamics, ed. by Grinstein, F. F., Margolin, L. G., and Rider, W. J.. Cambridge University Press, New York, 2nd printing, 2010.
[9]Sagaut, P.. Large Eddy Simulation for Incompressible Flows, 3rd ed. Springer, New York, 2006.
[10]Grinstein, F.F., Margolin, L.G., and Rider, W.J., eds. Implicit Large Eddy Simulation: Computing Turbulent Flow Dynamics. Cambridge University Press, New York, 2nd printing, 2010.
[11]George, W.K. and Davidson, L.. “Role of initial conditions in establishing asymptotic flow behavior.” AIAA Journal. 42:438446, 2004.
[12]Haines, B.M., Grinstein, F.F., and Schwarzkopf, J.D.. “Reynolds-averaged Navier-Stokes anitialization and benchmarking in shock-driven turbulent mixing.” Journal of Turbulence 14(2):4670, 2013.
[13]Gittings, M. et al.The RAGE radiation-hydrodynamic code.” Comput. Science & Discovery 1:015005, 2008.
[14]Lyon, S.P. and Johnson, J. D.. “SESAME: the Los Alamos National Laboratory Equation of State Database.” Los Alamos National Laboratory LA-UR-92-3407, 1992.
[15]Launder, B.E., Reese, G.J., and Rodi, W.. “Progress in the development of a Reynolds-stress turbulence closure.” J. Fluid Mech., 68:537, 1975.
[16]Besnard, D., Harlow, F.H., Rauenzahn, F.H., and Zemach, C.. “Turbulence transport equations for variable-density turbulence and their relationship to two-field models.” LA-UR-12303, Los Alamos National Laboratory, 1992.
[17]Grégoire, O., Souffland, D., and Gauthier, S.. “A second-order turbulence model for gaseous mixtures induced by Richtmyer-Meshkov instability.” J. Turbul. 6:1, 2005.
[18]Livescu, D., Ristorcelli, J.R., Gore, R.A., Dean, S.H., Cabot, W.H., and Cook, A.W.. “High-Reynolds number Rayleigh-Taylor turbulence.” J. Turbul. 10:1, 2009.
[19]Schwarzkopf, J.D., Livescu, D., Gore, R.A., Rauenzahn, R.M., and Ristorcelli, J.R.. “Application of a second-moment closure model to mixing processes involving multi-component miscible fluids.” J. Turbul. 12:135, 2011.
[20]Banerjee, A., Gore, R.A., and Andrews, M. J.. “Development and validation of a turbulent mix model for variable-density and compressible flows.” Phys. Rev. E 82:046309, 2010.
[21]Cook, A.W.. “Enthalpy diffusion in multicomponent flows.” Phys. Fluids 21:055109, 2009.
[22]George, W.K.. “The Self-preservation of turbulent flows and its relation to initial conditions and coherent structures,” in Advances in Turbulence, ed. by George, W.K. and Arndt, R.E.A., New York, 1989.
[23]Dimonte, G.. “Nonlinear evolution of the Rayleigh-Taylor and Richtmyer-Meshkov instabilities.” Phys. Plasma., 6:2009–15, 1999.
[24]Youngs, D.. “Rayleigh-Taylor and Richtmyer-Meshkov mixing,” in Implicit Large Eddy Simulation: Computing Turbulent Flow Dynamics, ed. by Grinstein, F.F., Margolin, L.G., and Rider, W.J.. Cambridge University Press, 2nd printing, 2010.
[25]Gowardhan, A.A. and Grinstein, F.F.. “Numerical simulation of Richtmyer–Meshkov instabilities in shocked gas curtains.” Journal of Turbulence 12(43):124, 2011.
[26]Jiménez, J., Wray, A.A., Saffman, P.G., and Rogallo, R.S.. “The structure of intense vorticity in isotropic turbulence.” J. Fluid Mech., 255:6590, 1993.
[27]Wachtor, A.J., Grinstein, F.F., DeVore, C.R., Ristorcelli, J.R., and Margolin, L.G.. “Mixing in implicit large-eddy simulation of statistically stationary isotropic turbulence.” Physics of Fluids, 25:025101, 2013.
[28]Fureby, C. and Grinstein, F.F.. “Monotonically integrated large eddy simulation of free shear flows.” AIAA J., 37:544, 1999.
[29]Dimotakis, P.E.. “The mixing transition in turbulent flows.” J. Fluid Mech., 409:69, 2000.
[30]Gowardhan, A.A., Ristorcelli, J.R., and Grinstein, F.F.. “The bipolar behavior of the Richtmyer–Meshkov instability.” Physics of Fluids 23:071701, 2011.
[31]Kolmogorov, A.N.. C. R. Acad. Sci. URSS 30:301, 1941.
[32]Falcovich, G., Gawedzki, K., and Vergassola, M.. “Particles and fields in fluid turbulence.” Reviews of Modern Physics, 73:913–75, 2001.
[33]Tennekes, H. and Lumley, J.L.. A First Course in Turbulence. MIT Press, Cambridge, MA, 1972.
[34]Zhou, Y.. “Unification and extension of the similarity scaling criteria and mixing transition for studying astrophysics using high energy density laboratory experiments or numerical simulations.” Physics of Plasmas, 14:082701, 2007.
[35]Zhou, Y., Grinstein, F.F., Wachtor, A.J., and Haines, B.M.. “Estimating the effective Reynolds number in implicit large eddy simulation.” Phys. Rev. E 89:013303, 2014.
[36]Kaneda, Y., et al.Energy dissipation rate and energy spectrum in high resolution direct numerical simulations of turbulence in a periodic box.” Phys. Fluids 15, L21. 2003.
[37]Grinstein, F.F., Gowardhan, A.A., and Wachtor, A.J.. “Simulations of Richtmyer-Meshkov instabilities in planar shock-tube experiments.” Physics of Fluids, 23:034106, 2011.
[38]Nuckolls, J., Wood, L., Thiessen, A., and Zimmerman, G.. “Laser compression of matter to super-high densities: Thermonuclear (CTR) applications.” Nature 239, 139, 1972.
[39]Thomas, V.A. and Kares, R.J.. “Drive asymmetry and the origin of turbulence in an ICF implosion.” Phys. Rev. Letters 109, 075004, 2012.
[40]Haan, S.W. et al.Design and modeling of ignition targets for the National Ignition Facility.” Phys. Plasma., 2:24802487, 1995.
[41]Callahan, D.A. et al.Optimization of the NIF ignition point design hohlraum.” J. Phy.s. Conf. Ser., 112:022021, 2008.
[42]Clark, D.S., Haan, S.W., Hammel, B.A., Salmonson, J.D., Callahan, D.A., and Town, R.P.J.. “Plastic ablator ignition capsule design for the National Ignition Facility.” Phys. Plasma. 17:052703, 2010.
[43]Haan, S.W. et al.Point design targets, specifications, and requirements for the 2010 ignition campaign on the National Ignition Facility.” Phys. Plasma. 18:051001, 2011.
[44]Radha, P.B. et al.Two-dimensional simulations of plastic-shell, direct-drive implosions on OMEGA.” Physics of Plasmas 12:032702, 2005.
[45]Radha, P.B. et al.Multidimensional analysis of direct-drive, plastic-shell implosions on OMEGA.” Physics of Plasmas 12:056307, 2005.
[46]Radha, P.B. et al.Triple-picket warm plastic shell implosions on OMEGA.” Physics of Plasmas 18:012705, 2011.
[47]Molvig, K., Hoffman, N.M., Albright, B.J., Nelson, E.M., and Webster, R.B.. “Knudsen layer reduction of fusion reactivity.” Phys. Rev. Lett., 109:095001, 2012.
[48]Amendt, P., Landen, O.L., Robey, H.F., Li, C.K., and Petrasso, R.D.. “Plasma barrodiffusion in inertial-confinement-fusion implosions: application to observed yield anomalies in thermonuclear fuel mixtures.” Phys. Rev. Lett., 105:115005, 2010.
[49]Dodd, E.S. et al.The effects of laser absorption on direct-drive capsule experiments at OMEGA.” Phys. Plasma. 19:042703, 2012.
[50]Scott, R.H.H. et al.Numerical modeling of the sensitivity of x-ray driven implosions to low-mode flux asymmetries.” Phys. Rev. Letters 110:075001, 2013.
[51]Clark, D.S. et al.Short-wavelength and three-dimensional instability evolution in National Ignition Facility ignition capsule designs.” Physics of Plasmas 18:082701, 2011.
[52]Grim, G.P. et al.Nuclear imaging of the fuel assembly in ignition experiments.” Physics of Plasmas 20:056320, 2013.
[53]Joggerst, C.C. et al.Cross-code comparison of mixing during the implosion of dense cylindrical and spherical shells.” J. Comput. Phys. 275:154173, 2014.
[54]Haines, B.M., Grinstein, F.F., Welser–Sherrill, L., Fincke, J.R., and Doss, F.W.. “Analysis of the effects of energy deposition on shock–driven turbulent mixing.” Physics of Plasmas 20:072306, 2013.
[55]Richtmyer, R.D.. “Taylor instability in shock acceleration of compressible fluids.” Comm. Pure Appl. Math 13:297319, 1960.
[56]Holmes, R.L. et al.Richtmyer–Meshkov instability growth: Experiment, simulation, and theory.” J. Fluid Mech. 389:5579, 1999.
[57]Ristorcelli, J.R., Gowardhan, A.A., and Grinstein, F.F.. “Two classes of Richtmyer-Meshkov instabilities: A detailed statistical look.” Physics of Fluids 25:044106, 2013.
[58]Marshall, F.J. et al.Direct-drive-implosion experiments with enhanced fluence balance on OMEGA.” Physics of Plasmas 11(1):251259, 2004.
[59]Drazin, P.G.. Introduction to Hydrodynamic Stability, Cambridge University Press, 2002.
[60]Epstein, R.. “On the Bell–Plesset effects: the effects of uniform compression and geometrical convergence on the classical Rayleigh–Taylor instability.” Physics of Plasmas 11(11):51145124, 2004.
[61]Park, H.S. et al.High-adiabat high-foot inertial confinement fusion implosion experiments on the National Ignition Facility.” Phys. Rev. Lett. 112:055001, 2014.
[62]Baumgaertel, J.A. et al.Observation of early shell-dopant mix in OMEGA direct-drive implosions and comparisons with radiation-hydrodynamic simulations.” Physics of Plasmas 21:052706, 2014.