Network


Latest external collaboration on country level. Dive into details by clicking on the dots.

Hotspot


Dive into the research topics where T. Cardenas is active.

Publication


Featured researches published by T. Cardenas.


Fusion Science and Technology | 2016

Additive Manufacturing Capabilities Applied to Inertial Confinement Fusion at Los Alamos National Laboratory

T. Cardenas; D. W. Schmidt; Dominic S. Peterson

Abstract We describe the use at Los Alamos National Laboratory of additive manufacturing (AM) for a variety of jigs and coating, assembly, and radiography fixtures. Additive manufacturing has also been used to produce shipping containers of complex design that would be too costly to have fabricated using traditional techniques. The current goal for AM use in target fabrication is to increase target accuracy and rigidity. This has been realized by implementing AM into target stalk fabrication, allowing increased complexity to address target strength and the addition of features for alignment at facilities. We will describe the fabrication of these components and our plans to utilize AM in the future.


Fusion Science and Technology | 2016

Development of Indirectly Driven Shock Tube Targets for Counter-Propagating Shear-Driven Kelvin-Helmholtz Experiments on the National Ignition Facility

Deanna Capelli; D. W. Schmidt; T. Cardenas; Gerald Rivera; Randall B. Randolph; Franklin Fierro; E. C. Merritt; K. A. Flippo; F. W. Doss; J. L. Kline

Abstract The shear experiments are designed to investigate the transition to turbulence of the Kelvin-Helmholtz instability driven by counter-propagating shear flows. The shear targets for the National Ignition Facility (NIF) shear experiments consist of two hohlraums connected to both ends of a shock tube. The cylindrical shock tube is filled with two hemi-cylindrical CH foams separated by a metal tracer foil. On both ends, a thick gold half-moon–shaped D-plug is placed on opposite halves of the tube to create counter-propagating shock waves. The design is based on a smaller Omega shear target. While the basic NIF design has remained the same, details of the design have undergone several changes over the last 2 years and continue to evolve to improve the quality of the experimental results. Design changes include shock tube designs, tracer foil variations, transitioning to beryllium spool machining, and groove features inside of the tube. Details of how the targets are built including design, machining the parts, target assembly, and metrology are presented, as well as recent target developmental work to meet the needs of future experiments and to improve target assembly efficiency and accuracy.


Fusion Science and Technology | 2018

Design and Fabrication of Opacity Targets for the National Ignition Facility

T. Cardenas; D. W. Schmidt; E.S. Dodd; Theodore Sonne Perry; Deanna Capelli; Theresa E. Quintana; John A. Oertel; Dominic S. Peterson; E. Giraldez; R. F. Heeter

Abstract Accurate models for opacity of partially ionized atoms are important for modeling and understanding stellar interiors and other high-energy-density phenomena such as inertial confinement fusion. Lawrence Livermore National Laboratory is leading a multilaboratory effort to conduct experiments on the National Ignition Facility (NIF) to try to reproduce recent opacity tests at the Sandia National Laboratory Z-facility. Since 2015, the NIF effort has evolved several hohlraum designs that consist of multiple pieces joined together. The target also has three components attached to the main stalk over a long distance with high tolerances that have resulted in several design iterations. The target has made use of rapid prototyped features to attach a capsule and collimator under the hohlraum while avoiding interference with the beams. This paper discusses the evolution of the hohlraum and overall target design and the challenges involved with fabricating and assembling these targets.


Physics of Plasmas | 2018

Hohlraum modeling for opacity experiments on the National Ignition Facility

E.S. Dodd; B. G. DeVolder; M. E. Martin; Natalia S. Krasheninnikova; I.L. Tregillis; T. S. Perry; R. F. Heeter; Y. P. Opachich; A. Moore; J. L. Kline; Heather Marie Johns; Duane A. Liedahl; T. Cardenas; R. E. Olson; Bernhard H. Wilde; T.J. Urbatsch

This paper discusses the modeling of experiments that measure iron opacity in local thermodynamic equilibrium (LTE) using laser-driven hohlraums at the National Ignition Facility (NIF). A previous set of experiments fielded at Sandias Z facility [Bailey et al., Nature 517, 56 (2015)] have shown up to factors of two discrepancies between the theory and experiment, casting doubt on the validity of the opacity models. The purpose of the new experiments is to make corroborating measurements at the same densities and temperatures, with the initial measurements made at a temperature of 160 eV and an electron density of 0.7 × 1022 cm−3. The X-ray hot spots of a laser-driven hohlraum are not in LTE, and the iron must be shielded from a direct line-of-sight to obtain the data [Perry et al., Phys. Rev. B 54, 5617 (1996)]. This shielding is provided either with the internal structure (e.g., baffles) or external wall shapes that divide the hohlraum into a laser-heated portion and an LTE portion. In contrast, most inertial confinement fusion hohlraums are simple cylinders lacking complex gold walls, and the design codes are not typically applied to targets like those for the opacity experiments. We will discuss the initial basis for the modeling using LASNEX, and the subsequent modeling of five different hohlraum geometries that have been fielded on the NIF to date. This includes a comparison of calculated and measured radiation temperatures.This paper discusses the modeling of experiments that measure iron opacity in local thermodynamic equilibrium (LTE) using laser-driven hohlraums at the National Ignition Facility (NIF). A previous set of experiments fielded at Sandias Z facility [Bailey et al., Nature 517, 56 (2015)] have shown up to factors of two discrepancies between the theory and experiment, casting doubt on the validity of the opacity models. The purpose of the new experiments is to make corroborating measurements at the same densities and temperatures, with the initial measurements made at a temperature of 160 eV and an electron density of 0.7 × 1022 cm−3. The X-ray hot spots of a laser-driven hohlraum are not in LTE, and the iron must be shielded from a direct line-of-sight to obtain the data [Perry et al., Phys. Rev. B 54, 5617 (1996)]. This shielding is provided either with the internal structure (e.g., baffles) or external wall shapes that divide the hohlraum into a laser-heated portion and an LTE portion. In contrast, most in...


Fusion Science and Technology | 2018

Progress in Developing Novel Double-Shell Metal Targets Via Magnetron Sputtering

H. Xu; H. Huang; J. Walker; C. Kong; N. Rice; M. P. Mauldin; J. D. Vocke; J. H. Bae; W. Sweet; F. H. Elsner; M. Farrell; Yinmin Wang; C. Alford; T. Cardenas; E. N. Loomis

Abstract Double-shell inertial confinement fusion targets represent a unique platform for achieving ignition. They consist of a low-Z outer ablator, a high-Z inner pusher layer, and a low-density foam layer sandwiched in between. There is the possibility that double-shell targets may achieve ignition at lower ion temperatures due to the containment of radiation and conduction losses as well as requiring smaller convergence ratios. We have explored using magnetron sputtering to make the inner high-Z pusher layers and have demonstrated a W-Cr bilayer inner-shell design. An Al-Be mixture was explored as one of the outer ablator materials. This material takes advantage of Al X-ray M-band absorption to reduce preheating and still retain Be high-ablation speeds. Typical commercial Al-Be materials suffer from phase separation. However, by using magnetron sputtering we have been able to demonstrate homogeneous Al-Be ablator coatings. The sputtered material forms with nanosized grains and has demonstrated excellent machinability. As a second type of shell explored, pushered single shells can exploit large density gradients to stabilize Rayleigh-Taylor instabilities during compression. Sharp gradients will have higher ignition yields and larger grading lengths will be more stable. We were able to demonstrate pushered single shells made from W-Be gradient layers with various grading slopes and provide simulated results showing that the grading profiles can be influenced by the coating rates of two components.


Fusion Science and Technology | 2018

Dry-Machining of Aerogel Foams, CH Foams, and Specially Engineered Foams Using Turn-Milling Techniques

Randall B. Randolph; John A. Oertel; T. Cardenas; Christopher E. Hamilton; D. W. Schmidt; Brian M. Patterson; Franklin Fierro; Deanna Capelli

Abstract A new method has been developed to dry-machine foams. Most of these foams are at the lower end of what is considered machineable because of their density or foam composition. Excluding aerogel foams, the foams traditionally required a wax-fill process before surviving any machining forces. This new dry-machining method uses a technique called turn-milling and replaces the old wax-fill method that added several weeks to the fabrication schedule and uncertainty in the quality of the final part. The new method utilizes a computer numerical control gang-tool–style lathe that is set up with electric live-tooling spindles. The foams are dry-machined with the lathe main spindle turning in the opposite direction of the live-tooling spindle. This turn-milling technique reduces tool pressure and can accommodate heavier roughing cuts that produce much faster cycle times. With this new dry-machining method we are able to machine the entire foam target component in one operation, eliminating the need for another machining operation for finishing the backside.


Journal of Physics: Conference Series | 2016

Increasing shot and data collection rates of the Shock/Shear experiment at the National Ignition Facility

F.W. Doss; K. A. Flippo; D. Capelli; T. Cardenas; B. G. DeVolder; J. L. Kline; L. Kot; S. Kurien; E. N. Loomis; E. C. Merritt; T. S. Perry; D. W. Schmidt; C. Di Stefano

Updates to the Los Alamos laser-driven high-energy-density Shock/Shear mixing- layer experiment are reported, which have collectively increased the platforms shot and data acquisition rates. The strategies employed have included a move from two-strip to four-strip imagers (allowing four times to be recorded per shot instead of two), the implementation of physics-informed rules of engagements allowing for the maximum flexibility in a shots total energy and symmetry performance, and splitting the lasers main drive pulse from a monolithic single pulse equal to all beams into a triply-segmented pulse which minimizes optics damage.


Physics of Plasmas | 2018

Shock-driven discrete vortex evolution on a high-Atwood number oblique interface

A.M. Rasmus; C. A. Di Stefano; K. A. Flippo; F. W. Doss; J. L. Kline; Jonathan Hager; E. C. Merritt; T. R. Desjardins; Weigang Wan; T. Cardenas; D. W. Schmidt; P. M. Donovan; Frank Fierro; J. I. Martinez; J. S. Zingale; C. C. Kuranz

We derive a model describing vorticity deposition on a high-Atwood number interface with a sinusoidal perturbation by an oblique shock propagating from a heavy into a light material. Limiting cases of the model result in vorticity distributions that lead to Richtmyer-Meshkov and Kelvin-Helmholtz instability growth. For certain combinations of perturbation amplitude, wavelength, and tilt of the shock, a regime is found in which discrete, co-aligned, vortices are deposited on the interface. The subsequent interface evolution is described by a discrete vortex model, which is found to agree well with both RAGE simulations and experiments at early times.


Physics of Plasmas | 2018

Late-time mixing and turbulent behavior in high-energy-density shear experiments at high Atwood numbers

K. A. Flippo; F. W. Doss; E. C. Merritt; B. G. DeVolder; C. A. Di Stefano; P. A. Bradley; D. Capelli; T. Cardenas; T. R. Desjardins; Frank Fierro; C. M. Huntington; J. L. Kline; L. Kot; S. Kurien; E. N. Loomis; S. A. MacLaren; T. J. Murphy; S. R. Nagel; T. S. Perry; R. B. Randolph; A.M. Rasmus; D. W. Schmidt

The LANL Shear Campaign uses millimeter-scale initially solid shock tubes on the National Ignition Facility to conduct high-energy-density hydrodynamic plasma experiments, capable of reaching energy densities exceeding 100 kJ/cm3. These shock-tube experiments have for the first time reproduced spontaneously emergent coherent structures due to shear-based fluid instabilities [i.e., Kelvin-Helmholtz (KH)], demonstrating hydrodynamic scaling over 8 orders of magnitude in time and velocity. The KH vortices, referred to as “rollers,” and the secondary instabilities, referred to as “ribs,” are used to understand the turbulent kinetic energy contained in the system. Their evolution is used to understand the transition to turbulence and that transitions dependence on initial conditions. Experimental results from these studies are well modeled by the RAGE (Radiation Adaptive Grid Eulerian) hydro-code using the Besnard-Harlow-Rauenzahn turbulent mix model. Information inferred from both the experimental data and the mix model allows us to demonstrate that the specific Turbulent Kinetic Energy (sTKE) in the layer, as calculated from the plan-view structure data, is consistent with the mixing width growth and the RAGE simulations of sTKE.The LANL Shear Campaign uses millimeter-scale initially solid shock tubes on the National Ignition Facility to conduct high-energy-density hydrodynamic plasma experiments, capable of reaching energy densities exceeding 100 kJ/cm3. These shock-tube experiments have for the first time reproduced spontaneously emergent coherent structures due to shear-based fluid instabilities [i.e., Kelvin-Helmholtz (KH)], demonstrating hydrodynamic scaling over 8 orders of magnitude in time and velocity. The KH vortices, referred to as “rollers,” and the secondary instabilities, referred to as “ribs,” are used to understand the turbulent kinetic energy contained in the system. Their evolution is used to understand the transition to turbulence and that transitions dependence on initial conditions. Experimental results from these studies are well modeled by the RAGE (Radiation Adaptive Grid Eulerian) hydro-code using the Besnard-Harlow-Rauenzahn turbulent mix model. Information inferred from both the experimental data and t...


Physics of Plasmas | 2018

Design considerations for indirectly driven double shell capsules

D. S. Montgomery; William Daughton; B. J. Albright; Andrei N. Simakov; D. C. Wilson; E.S. Dodd; R. C. Kirkpatrick; Robert G. Watt; Mark Gunderson; E. N. Loomis; E. C. Merritt; T. Cardenas; Peter A. Amendt; J. L. Milovich; H. F. Robey; Robert Tipton; M. D. Rosen

Double shell capsules are predicted to ignite and burn at relatively low temperature (∼3 keV) via volume ignition and are a potential low-convergence path to substantial α-heating and possibly ignition at the National Ignition Facility. Double shells consist of a dense, high-Z pusher, which first shock heats and then performs work due to changes in pressure and volume (PdV work) on deuterium-tritium gas, bringing the entire fuel volume to high pressure thermonuclear conditions near implosion stagnation. The high-Z pusher is accelerated via a shock and subsequent compression of an intervening foam cushion by an ablatively driven low-Z outer shell. A broad capsule design parameter space exists due to the inherent flexibility of potential materials for the outer and inner shells and foam cushion. This is narrowed down by design physics choices and the ability to fabricate and assemble the separate pieces forming a double shell capsule. We describe the key physics for good double shell performance, the trade-offs in various design choices, and the challenges for capsule fabrication. Both 1D and 2D calculations from radiation-hydrodynamic simulations are presented.Double shell capsules are predicted to ignite and burn at relatively low temperature (∼3 keV) via volume ignition and are a potential low-convergence path to substantial α-heating and possibly ignition at the National Ignition Facility. Double shells consist of a dense, high-Z pusher, which first shock heats and then performs work due to changes in pressure and volume (PdV work) on deuterium-tritium gas, bringing the entire fuel volume to high pressure thermonuclear conditions near implosion stagnation. The high-Z pusher is accelerated via a shock and subsequent compression of an intervening foam cushion by an ablatively driven low-Z outer shell. A broad capsule design parameter space exists due to the inherent flexibility of potential materials for the outer and inner shells and foam cushion. This is narrowed down by design physics choices and the ability to fabricate and assemble the separate pieces forming a double shell capsule. We describe the key physics for good double shell performance, the trade-...

Collaboration


Dive into the T. Cardenas's collaboration.

Top Co-Authors

Avatar

D. W. Schmidt

Los Alamos National Laboratory

View shared research outputs
Top Co-Authors

Avatar

J. L. Kline

Los Alamos National Laboratory

View shared research outputs
Top Co-Authors

Avatar

E. C. Merritt

Los Alamos National Laboratory

View shared research outputs
Top Co-Authors

Avatar

E.S. Dodd

Los Alamos National Laboratory

View shared research outputs
Top Co-Authors

Avatar

K. A. Flippo

Los Alamos National Laboratory

View shared research outputs
Top Co-Authors

Avatar

D. C. Wilson

Los Alamos National Laboratory

View shared research outputs
Top Co-Authors

Avatar

D. S. Montgomery

Los Alamos National Laboratory

View shared research outputs
Top Co-Authors

Avatar

William Daughton

Los Alamos National Laboratory

View shared research outputs
Top Co-Authors

Avatar

B. G. DeVolder

Los Alamos National Laboratory

View shared research outputs
Top Co-Authors

Avatar

Christopher E. Hamilton

Los Alamos National Laboratory

View shared research outputs
Researchain Logo
Decentralizing Knowledge