Bulletin of the American Physical Society
60th Annual Meeting of the APS Division of Plasma Physics
Volume 63, Number 11
Monday–Friday, November 5–9, 2018; Portland, Oregon
Session GO6: Compression and Burn II |
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Chair: Art Pak, Lawrence Livermore National Laboratory Room: OCC B115-116 |
Tuesday, November 6, 2018 9:30AM - 9:42AM |
GO6.00001: Thermonuclear Ignition and the Onset of Propagating Burn in Inertial Fusion Alison Christopherson, Riccardo Betti Defining ignition in inertial confinement fusion (ICF) is an unresolved problem. In ICF, a distinction must be made between the ignition of the hot spot and the propagation of the burn wave in the surrounding dense fuel since most of the energy gain comes from burning the dense shell. In this work, we used a large 1-D simulation ensemble to show that it is possible to identify the onset of ignition through a unique value of the yield amplification defined as the ratio of the fusion yield including alpha-particle deposition to the fusion yield without alphas. Since the yield amplification is a function of the fractional alpha energy (total alpha energy/hot-spot energy, a measurable quantity), it appears possible not only to define ignition but also to measure the onset of ignition by the experimental inference of the fractional alpha energy and yield amplification. We also investigate the impacts of low- and mid-mode asymmetries on this ignition curve and how the definition of ignition is modified by these perturbations. |
Tuesday, November 6, 2018 9:42AM - 9:54AM |
GO6.00002: Modification of Transport in Burning Plasmas due to alpha-electron Collisions Brian Appelbe, Mark Sherlock, Daniel E Ruiz, Jon Tong, Jeremy Chittenden Ignition in ICF requires alpha particles to transfer energy to the deuterium-tritium plasma via Coulomb collisions. For plasma temperatures < ~25 keV, the alphas transfer energy predominantly to the plasma electrons. The electron-electron collision time is much shorter than the alpha-electron collision time since the alpha number density is a small fraction of the electron number density. Therefore, it is usually assumed that the electron distribution function remains Maxwellian when alpha particles are present. In this work it is shown that a net flux of alpha particles can perturb the electron distribution function from Maxwellian. The electron kinetic equation is solved in the presence of arbitrary populations of alpha particles to quantify this perturbation. The perturbation results in the transport of energy and momentum by the plasma electrons. In particular, it is shown that heat flow from hot to cooler regions of an igniting plasma can be increased by the flux of alpha particles that results from differences in reactivity between the regions. Burn propagation into cold fuel is also modified by this effect. |
Tuesday, November 6, 2018 9:54AM - 10:06AM |
GO6.00003: Development of a 3D Generalized Lawson ignition threshold metric and application to high yield NIF implosion data Paul T Springer, Omar A Hurricane, James Henry Hammer, Riccardo Betti, Michael J Edwards The self-heating condition for an imploding hotspot require understanding the balance between mechanical work, heating via fusion reactions, and the radiative and conduction losses. A 3D generalized Lawson ignition threshold criterion is achieved when hotspot rho-r and temperature exceed critical values. In the presence of 3D shell rho-R asymmetry, loss of confinement in “thin” regions of the stagnated fuel increases expansion phase PdV work leading to loss of pressure, temperature, and alpha heating. Compared to conventional ignition metrics, the proper 3D metric requires both increased pressure and temperature for ignition to offset 3D loss in confinement, and places requirements on rho-r asymmetry and minimum rho-r. A potential flow solution to the 3D flows that develop near peak compression is derived and fit to observed hotspot and shell asymmetry data, to account for the expected thinning due to the evolution of the Rayleigh Taylor instability. This technique is applied to high yield implosion data from NIF, which exhibit significant 3D rho-r asymmetry, and is used to predict required improvements needed to achieve ignition. |
Tuesday, November 6, 2018 10:06AM - 10:18AM |
GO6.00004: Stagnation conditions achieved in DT implosions on the NIF Pravesh K Patel Recent cryogenic deuterium-tritium (DT) spherical implosion experiments on the National Ignition Facility (NIF) have exceed 50 kJ in fusion yield—several times that of the energy delivered to the fuel through compressive work of the implosion. More than 10 kJ of alpha-particle energy is created, of which most is deposited within the hot-spot, producing significant self-heating and an amplification of ~3x in the fusion yield. This talk will summarize the performance of the campaigns in terms of stagnation conditions achieved and examine the scaling of the key parameters including pressure, temperature, areal density, and the Lawson parameter, which determine the proximity to ignition. |
Tuesday, November 6, 2018 10:18AM - 10:30AM |
GO6.00005: Sensitivity of yield and compression to velocity, shock timing, coast time and asymmetry in indirect-drive NIF implosions* Otto L Landen, Paul T Springer, Cliff A Thomas, Pravesh K Patel, John D Lindl, Dov Shvarts The yield and fuel compression sensitivity to various drive parameters for the >100 NIF indirect-drive cryogenic DT implosions performed to date is empirically examined across all scales, ablators and in-flight adiabats. Low mix yields normalized by fuel mass increase with velocity, and increase with fuel compression after normalizing out velocity, but only up to a point. Compression remains sensitive to shock merge depths and coast times [1] even at higher adiabats. Mass and velocity normalized yields and compressions drop by factors 1.5-3x in the presence of measured large mode 1 and 2 asymmetries. The trends will be compared to analytic expressions [2,3] and the hypotheses for some notable outliers will be discussed. [1] O. Hurricane et. al. Phys. Plasmas 24, 092706 (2017) [2] J. Lindl et. al, submitted to Physics Plasmas [3] R. Kishony and D. Shvarts, Phys. Plasmas 8, 4925 (2001) |
Tuesday, November 6, 2018 10:30AM - 10:42AM |
GO6.00006: Novel double-spike pulse shape for OMEGA cryogenic implosions Dhrumir P Patel, Riccardo Betti, Varchas Gopalaswamy, Ka Ming Woo Models obtained through statistical analysis have demonstrated good predictive capability for the fusion yields of OMEGA cryogenic implosions. These models produced accurate correlations between the experimental fusion yields and several output variables from the 1-D radiation–hydrodynamic code LILAC. These statistical relations were used to design new implosion experiments, leading to tripling of the fusion yield on OMEGA. Here we describe how these statistical methods can be applied to predict other experimental observables including the areal density and hot-spot radius. These predictive correlations are then used to design new pulse shapes to increase the convergence ratio and the areal density for a new implosion campaign. Once an accurate predictive capability is established for both fusion yields and areal densities, it will be possible to design and field the optimum implosion compatible with the capabilities of the OMEGA laser. |
Tuesday, November 6, 2018 10:42AM - 10:54AM |
GO6.00007: Using neutron and X-ray images of layered HDC implosion on the NIF to reconstruct hotspot conditions during burn Laurent Divol, Arthur Pak, Petr L Volegov, Carl Wilde, Laura Berzak Hopkins, Sebastien Le Pape, Eduard L. Dewald, David Neal Fittinghoff, Chris Weber The time-integrated neutron image(s) of a layered implosion on the NIF, under an isobaric assumption, allows the reconstruction of the density and temperature profile of the central hotspot. The measured neutron yield and spectral width constrain the stagnation pressure. One can then look for signatures of various degradation mechanisms. For instance, one can compare a co-registered X-ray image to a synthetic reconstruction and assess the impact of Carbon penetrating the hot spot through mix and the fill-tube jet. The method will be validated using simulated images and applied to a series of recent high-performing HDC implosions [1]. [1] “Fusion energy output greater than the kinetic energy of an imploding shell at the National Ignition Facility”, S. LePape et al., Phys. Rev. Lett. 120, 245003 (2018) |
Tuesday, November 6, 2018 10:54AM - 11:06AM |
GO6.00008: Survey of Neutron Spectrum Signatures in 3D Simulations of ICF Implosions John Field, Ryan Nora, B. K. Spears, D. H. Munro, J. L. Peterson, S. Brandon At LLNL, we have recently started to do large 3D HYDRA simulation surveys of perturbed ICF implosions. In 3D, the fluid flow constraints are greatly relaxed from those in 2D and therefore the likelihood of particular flow patterns in simulation is likely to be much more representative of the real experimental situation. This talk will concentrate on histograms of the combined velocity and temperature distribution of the burning plasma and the resulting signature in neutron time of flight measurements. In particular, we will discuss the flow pattern effects on the magnitude and shape of the spectrum. |
Tuesday, November 6, 2018 11:06AM - 11:18AM |
GO6.00009: Three-dimensional modeling and hydrodynamic scaling of high density carbon ablator implosions on the National Ignition Facility Daniel Clark, Jose L Milovich, Christopher Weber, Andrea Kritcher, Pravesh K Patel, Bruce A Hammel, Joseph M Koning, Michael M Marinak, Laurent Pierre Masse, Arthur Pak, Mehul V Patel, Christopher R Schroeder, Scott Sepke, Petr L Volegov Recent implosion experiments using high density carbon ablators on the National Ignition Facility have achieved neutron yields exceeding 1016. Three-dimensional, high-resolution modeling of these cryogenic implosions shows encouraging agreement with experiment in many respects. This includes x-ray and neutron imaging data from the implosions, flange nuclear activation detector (fNAD) maps, and directional neutron spectral measurements, as well as scalar observables such as total neutron yield. This talk reviews the status of these high-resolution simulations, their comparison to experiment, and where discrepancies still remain. Preliminary results using these simulations to assess hydrodynamic scaling to higher energy will also be discussed. |
Tuesday, November 6, 2018 11:18AM - 11:30AM |
GO6.00010: Large-scale Implosions Using HDC Ablators for the Frustraum Darwin Ho, Peter Andrew Amendt, John D Lindl A diamond-shaped hohlraum (“frustraum”) proposed by Amendt† may provide adequate radiation symmetry for large capsules (1500 m radius) and Tradin the range 290-300 eV while only requiring < 1.8 MJ of laser energy. The implosion physics and designs for these large capsules are presented here and compared to nominal scale (1100 m radius) HDC implosions. The fuel adiabat for the large-scale capsules ranges from 2.5 to 4.5. Larger scale has higher 1D margin or GLC, e.g., the adiabat 4 design gives a 2D yield of 20 MJ while the nominal-scale adiabat 4 design has a 2D yield of only about 0.5 MJ. Lower hard x-ray fraction (14%) from the frustraum with a DU wall results in neutral Atwood number at peak velocity. This reduces mix and gives a high clean fuel fraction of 95%. Large-scale capsules are also robust to fuel preheat, hotspot contamination, and tent and fill-tube perturbations. The methods used for the large-scale designs are the same for the postshot modeling of N170601, which give close agreement with the data. †Amendtet al., this conference. |
Tuesday, November 6, 2018 11:30AM - 11:42AM |
GO6.00011: Beryllium-ablator DT implosion performance at high case-to-capsule ratio on the National Ignition Facility Alex Zylstra, S. Austin Yi, John L Kline, George A Kyrala, Stephan A MacLaren, Joseph E Ralph, Benjamin Bachmann, Shahab Khan, Debra Ann Callahan, Omar A Hurricane Using beryllium as an ablator material has several potential advantages for inertial fusion because of its low opacity and thus higher ablation rate. This could enable novel designs taking advantage of the reduced ablation-front growth rate or operating at lower radiation temperature. We report on a series of DT layered experiments using subscale beryllium implosions at high case-to-capsule ratio to isolate the implosion physics from hohlraum uncertainties. We find that the DT performance degrades substantially relative to 1-D clean predictions as the velocity increases by increased mass ablation. The performance trends are investigated with mix models, especially between the fuel and ablator. |
Tuesday, November 6, 2018 11:42AM - 11:54AM |
GO6.00012: Taking beryllium ablator implosions to larger scale on the NIF S.A. MacLaren, S.A. Yi, A.B. Zylstra, J.E. Ralph, G.A. Kyrala, B. Bachmann, L.P. Masse, J.L. Kline, D.A. Callahan, O.A. Hurricane A series of 4 cryo-layered implosion experiments with 900 µm outer radius Be ablators has been performed at the NIF. The first three used similar Cu-doped Be capsules, and the fourth used a thicker layer of Cu dopant to move off the “rocket curve” of the first three and maintain velocity while preserving remaining mass; this fourth implosion produced the highest yield of the set. A model of the hydrodynamic instability-driven mixing between ablator and fuel was developed that reduced the compressibility of the fuel and reproduced the stagnation observables the first three implosions. This model was then used to successfully predict the performance of the fourth. This model can now be used to explore the performance of Cu-doped Be capsule implosions at larger (+20% and +30%) scale on the NIF. The phenomena that establish the seeds and growth of instabilities that mix ablator and fuel do not necessarily scale with the capsule size and velocity. As a result, the model predicts the performance at larger scales should be factors of several better than what one obtains from the simply scaling capsule radius and fuel velocity. |
Tuesday, November 6, 2018 11:54AM - 12:06PM |
GO6.00013: Achieving high hot-spot pressures with 0.9scale CH capsule implosions at the National Ignition Facility* Tilo Doeppner, Denise E Hinkel, Leonard C Jarrott, Laura Robin Benedetti, Andrea Kritcher, Laurent Pierre Masse, Jose L Milovich, Jaebum Park, Joseph E Ralph, Benjamin Bachmann, Daniel T Casey, Alastair Moore, Petr L Volegov, Debra Ann Callahan, Omar A Hurricane We are reporting on a series of indirect-drive 0.9scale CH capsule implosions (inner radius = 840 μm) fielded in low gas-fill (0.6 mg/cm3) hohlraums of 6.72 mm diameter. Thanks to the increase in case-to-capsule ratio we achieved good hot spot symmetry control near 33% cone-fraction and zero wavelength separation. As a result, we demonstrated hot spot pressures approaching 300 Gbar in fully-integrated layered DT implosions. However, pushing this design to higher velocity resulted in a reduction of neutron yield. Highly-resolved capsule simulations suggest that higher Au M-shell preheat due to a reduced Si-dopant fraction resulted in an increase in Atwood number at the ablator-ice interface. These results provide important scaling information for next-generation CH designs. |
Tuesday, November 6, 2018 12:06PM - 12:18PM |
GO6.00014: Capsule symmetry and hydrodynamic stability of high density carbon and plastic ablator implosion designs on the National Ignition Facility Marion Lafon, Max Bonnefille, Marc Vandenboomgaerde Achieving areal density and temperature conditions necessary for hot spot ignition at the National Ignition Facility (NIF) requires careful control of capsule performance (implosion velocity, fuel adiabat) and hot spot shape. Capsules using high density carbon (HDC) and plastic ablators driven by adiabat-shaped X-ray profiles are designed to reach the alpha heating regime. A comparison of the relative stability of these designs was made using TROLL radiation hydrodynamics simulations of single-mode perturbation linear growth at the ablation front and fuel-ablator interface. Performing designs have to associate both hohlraum performance and capsule stability. Two-dimensional integrated simulations have been performed to evaluate how changes to the hohlraum (size, gas fill density, shape, beam balance) and to the laser pulse (picket, foot drive, pulse length) impact the HDC and plastic capsule performance and implosion symmetry. The combination of all these effects is used to help guide future designs for NIF and the Laser Mega Joule facility. |
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