/15RRP HAPL Dec 6, 20021 Robert R. Peterson Los Alamos National Laboratory and University of Wisconsin Calculations of the Response of Inertial Fusion.

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Presentation transcript:

/15RRP HAPL Dec 6, Robert R. Peterson Los Alamos National Laboratory and University of Wisconsin Calculations of the Response of Inertial Fusion Energy Materials to X-ray and Ion Irradiation on Z and RHEPP High Average Power Laser Meeting Naval Research Laboratory Washington DC December 5 and 6, 2002 LA-UR With help from Igor E. Golovkin Prism Computational Sciences Timothy J. Renk, Tina J. Tanaka, Gregory A. Rochau and Craig L. Olson Sandia National Laboratories

/15RRP HAPL Dec 6, OUTLINE 1.Z X-ray Experiments: BUCKY Simulations 2.RHEPP Ion Experiments: BUCKY Simulations 3.Comparison with Experiments 4.Summary and Future Work

/15RRP HAPL Dec 6, BUCKY Melting and Vaporization Models (for Code Jocks only) BUCKY has separate 1-D meshes for the gas/vapor/plasma and for the liquid/solid. The gas/vapor/plasma mesh is Lagrangian radiation hydrodynamics. The liquid/solid mesh has no radiation transport or hydro. Vaporization and condensation moves cells between the two meshes. This phase change is calculated with thermodynamic and kinetic models. Latent Heat is included. Melting is calculated within the liquid/solid mesh. Material properties change as the temperature moves through the melting temperature. Latent heat is included through the temperature dependent EOS. Thermal conduction (diffusion) is calculated on the liquid/solid mesh using input temperature-dependent conductivities and heat capacities. External electron, ion and x-ray sources deposit volumetrically through out both meshes. Stopping powers are calculated for electrons and ions and are looked up on cold experimental data tables for x-rays. The x-ray deposition is adjusted to included bleaching. Radiation transport in the gas/vapor/plasma mesh is calculated with either gray diffusion, mult-group diffusion, Variable Eddington, or multi-angle method of characteristics. Radiation and thermal conduction from the gas/vapor/plasma mesh are surface sources on the liquid/solid mesh.

/15RRP HAPL Dec 6, Z-Machine Produces Intense X-rays for Many Uses: Including Study of Inertial Fusion Energy Target Chamber Materials W Wire Array X-ray Pin Hole Image of Imploded Wire Array Pinch in Slotted Current Return Can Collimators, Filters and Sample Holders

/15RRP HAPL Dec 6, Z Shot 783 Produced Significant X-Rays for IFE Vaporization Experiments 1.9 MJ W wire Array Z x-rays consist of direct z-pinch x-rays and those from walls ( i.e. see work of M. Cuneo and G.A. Rochau of SNL). In these simulations, x- ray spectrum is taken as a black-body peaking at about 160 eV. A high energy tail has been seen representing a few % of spectrum. This and details of filtering need to be included.

/15RRP HAPL Dec 6, Erosion Threshold for Pure Tungsten Irradiated by X-Rays on Z is Calculated by BUCKY to be J/cm 2, But Very Sensitive to Thermal Conductivity This effect is reduced by 3-D expansion of vapor (BUCKY is 1-D). “Vapor Shielding” has not been tested on Z. BUCKY Calculations done with Low and High Thermal Conductivity models for solid Tungsten; Conductivity of liquid = 2 W/cm-K. After threshold fluence is surpassed, melt depth is insensitive to x-ray fluence because of absorption of x- rays by vapor.

/15RRP HAPL Dec 6, RHEPP Uses a MAP Extraction Diode to Produce Intense Bursts of Ions for Many Uses, Including Study of Inertial Fusion Energy Target Chamber Materials Ions are generated by the magnetically-confined anode plasma (MAP) source RHEPP (Repetitive High-Energy Pulse Power) kV ≤ 250 A/cm 2 Beams from H, He, N 2, O 2, Ne, Ar, Xe, Kr, CH 4 Overall treatment area ~ 100 cm 2 Diode vacuum ~ Torr

/15RRP HAPL Dec 6, In the Most Recent Series of Experiments, RHEPP Nitrogen Beams are Used to Study Target Chamber Materials N +2 peaks at about 1.2 MeV in a pulse about 60 ns wide (FWHM). N + peaks at about 0.6 MeV in a pulse about 60 ns wide (FWHM). H + peaks at about 0.6 MeV in a pulse about 80 ns wide (FWHM). All are included in the BUCKY simulations.

/15RRP HAPL Dec 6, Erosion Threshold for Pure Tungsten Irradiated by Nitrogen Ions on RHEPP is Calculated by BUCKY to be ~6 J/cm 2 BUCKY simulations done for High and Low solid thermal conductivities and melt conductivities of 0.1 and 2.0 W/cm-K. Threshold is very sensitive to thermal conductivity of solid and melt. After threshold fluence is surpassed, melt depth is insensitive to ion fluence because of absorption of ions by vapor. This effect is reduced by 3- D expansion of vapor (BUCKY is 1-D).

/15RRP HAPL Dec 6, Example: High Thermal Conductivity T vap is the vaporization temperature, and is assumed to be constant in these simulations. For 12.5 J/cm 2 on RHEPP N ions deposited on Pure Tungsten, there is only a small amount of vaporization (0.177  m). When there is a large amount of vaporization or vaporization in the middle of a solid, the vapor density and suppress vaporization, increasing T vap (model in BUCKY)

/15RRP HAPL Dec 6, Two Orientations for Pyrolytic Graphite are Considered, Perpendicular (PERP) and Parallel (ASDEP), With Quite Different Thermal Conductivity Models The thermal conductivity of Pyrolytic Graphite is very an- isotropic. Conductivity in the direction parallel to the fibers (ASDEP) is 60 times that in the direction perpendicular to the fibers (PERP). Experiments on RHEPP and BUCKY simulations have been carried out for both orientations. From Tina Tanaka (SNL)

/15RRP HAPL Dec 6, Erosion Threshold for Pyrolytic Graphite Irradiated by Nitrogen Ions on RHEPP is Calculated by BUCKY For Parallel (ASDEP) and Perpendicular (PERP) Thermal Conductivity Models Threshold for Vaporization of PERP Pyrolytic Graphite is 1.6 J/cm 2. Threshold for Vaporization of ASDEP Pyrolytic Graphite is 2.5 J/cm 2.

/15RRP HAPL Dec 6, Self-shielding of Vaporizing Samples from X-rays and Ions is Important in BUCKY Simulations Fraction (%) of ion or x- ray energy that is stopped in the gas and vapor is plotted against the width of material vaporized. W is very successful at stopping Z x-rays. W and Graphite are about equally able to stop RHEPP N-beams. The points outside of the trend were high fluence (5 and 7 J/cm 2 ) where 8-10 % of the energy was re- radiated to the sample over a long time. Tungsten results for high Conductivity

/15RRP HAPL Dec 6, Comparison BUCKY Predicted Thresholds And Measured Data: BUCKY Slightly Over-Predicts Damage in Experiments BUCKYExperiments Tungsten with Ions6 J/cm 2 > 7 J/cm 2 Tungsten with X-rays3.5-4 J/cm J/cm 2 PERP Graphite with Ions 1.6 J/cm 2 (~2 for dx >.01  m) <3.0 J/cm 2 ASDEP Graphite with Ions 2.5 J/cm 2 (~2.75 for dx >.01  m) J/cm 2

/15RRP HAPL Dec 6, Summary and Future Work BUCKY Simulations have been performed for Graphite and Tungsten samples shot on RHEPP and Z. Initial Comparisons have been performed. Simulations and Experiments are consistent but there are still uncertainties in x-ray drive spectrum and material properties. Effects of variations in Z x-ray spectrum and RHEPP ion species should be studied. Other materials (Tungsten alloys, liquids) should be studied.