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Fundamentals of hydrogen storage in nanoporous materials

Progress in Energy

Zhang, Linda; Allendorf, Mark D.; Balderas-Xicohtencatl, Rafael; Broom, Darren P.; Fanourgakis, George S.; Froudakis, George E.; Gennett, Thomas; Hurst, Katherine E.; Ling, Sanliang; Milanese, Chiara; Parilla, Philip A.; Pontiroli, Daniele; Ricco, Mauro; Shulda, Sarah; Stavila, Vitalie; Steriotis, Theodore A.; Webb, Colin J.; Witman, Matthew D.; Hirscher, Michael

Physisorption of hydrogen in nanoporous materials offers an efficient and competitive alternative for hydrogen storage. At low temperatures (e.g. 77 K) and moderate pressures (below 100 bar) molecular H2 adsorbs reversibly, with very fast kinetics, at high density on the inner surfaces of materials such as zeolites, activated carbons and metal-organic frameworks (MOFs). This review, by experts of Task 40 ‘Energy Storage and Conversion based on Hydrogen’ of the Hydrogen Technology Collaboration Programme of the International Energy Agency, covers the fundamentals of H2 adsorption in nanoporous materials and assessment of their storage performance. The discussion includes recent work on H2 adsorption at both low temperature and high pressure, new findings on the assessment of the hydrogen storage performance of materials, the correlation of volumetric and gravimetric H2 storage capacities, usable capacity, and optimum operating temperature. The application of neutron scattering as an ideal tool for characterising H2 adsorption is summarised and state-of-the-art computational methods, such as machine learning, are considered for the discovery of new MOFs for H2 storage applications, as well as the modelling of flexible porous networks for optimised H2 delivery. The discussion focuses moreover on additional important issues, such as sustainable materials synthesis and improved reproducibility of experimental H2 adsorption isotherm data by interlaboratory exercises and reference materials.

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Comparison of exponential integrators and traditional time integration schemes for the shallow water equations

Applied Numerical Mathematics

Eldred, Christopher; Brachet, Matthieu; Debreu, Laurent

The time integration scheme is probably one of the most fundamental choices in the development of an ocean model. In this paper, we investigate several time integration schemes when applied to the shallow water equations. This set of equations is accurate enough for the modeling of a shallow ocean and is also relevant to study as it is the one solved for the barotropic (i.e. vertically averaged) component of a three dimensional ocean model. We analyze different time stepping algorithms for the linearized shallow water equations. High order explicit schemes are accurate but the time step is constrained by the Courant-Friedrichs-Lewy stability condition. Implicit schemes can be unconditionally stable but, in practice lack accuracy when used with large time steps. In this paper we propose a detailed comparison of such classical schemes with exponential integrators. The accuracy and the computational costs are analyzed in different configurations.

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A model for K-shell x-ray yield from magnetic implosions at Sandia's Z machine

Physics of Plasmas

Schwarz, Jens; Vesey, Roger A.; Ampleford, David; Schaeuble, Marc-Andre; Giuliani, J.L.; Esaulov, A.; Dasgupta, A.; Jones, Brent M.

A zero-dimensional magnetic implosion model with a coupled equivalent circuit for the description of an imploding nested wire array or gas puff is presented. Circuit model results have been compared with data from imploding stainless steel wire arrays, and good agreement has been found. The total energy coupled to the load, E j × B, has been applied to a simple semi-analytic K-shell yield model, and excellent agreement with previously reported K-shell yields across all wire array and gas puff platforms is seen. Trade space studies in implosion radius and mass have found that most platforms operate near the predicted maximum yield. In some cases, the K-shell yield may be increased by increasing the mass or radius of the imploding array or gas puff.

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Rachel Wood Consulting - Viga Span Tables

Bosiljevac, Thomas B.

The purpose and scope of the viga span tables project for Rachel Wood Consulting (RWC) is focused on producing tabulated beam span tables for three species of wood vigas commonly used in New Mexico to allow producers, designers and builders to incorporate vigas into their building designs in a prescriptive manner similar to the span tables for sawn lumber incorporated into the International Residential Code (IRC) or the International Log Builders Association (ILBA) publication. The information provided in this report and the associated viga span tables also attempts to address and clarify questions raised by RWC during their review of the 2018 Los Alamos National Laboratory (LANL) New Mexico Small Business Assistance (NMSBA) program report by August Mosimann pertaining to span lengths, loading, deflection calculations, and log grading certification prior to submitting the span tables to the Construction Industries Division (CID) of New Mexico.

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Exploring the Basic Physical Mechanisms of Cathode- and Anode-Initiated High-Voltage Surface Flashover

IEEE Transactions on Plasma Science

Brooks, William; Clark, Raimi; Young, Jacob; Hopkins, Matthew M.; Dickens, James; Neuber, Andreas

Surface flashover in vacuum imposes a substantial physical limit on modern, large-scale pulsed power. One of the ramifications is a minimum size requirement for new machines, which in itself becomes a hard barrier to the modernization and improvement of existing infrastructure. Pulsed power topologies require the physical mechanisms of both anode- and cathode-initiated flashover to be considered. Originally, the geometrical implications of field emission at the cathode triple junction (CTJ) motivated the usage of configurations that avoid electrons impinging on the insulating material. This will largely suppress the cathode-initiated flashover, which is best described by the secondary electron avalanche mechanism, gas desorption, and final breakdown in the desorbed gas. It depends on the cascade growth of a conducting plasma along the length of the insulator from the cathode. Mitigating the cathode-initiated flashover typically comes at the cost of a significant field enhancement at the anode triple junction (ATJ). In a typical implementation, the anode field may be three times higher than the cathode field for a given voltage, making the corresponding anode-initiated flashover much more common than otherwise. In the case of pulsed, anode-initiated flashover, experimental evidence suggests that charge is directly extracted from the insulator resulting in the insulator taking on a net positive charge advancing the anode potential. Along with accompanying gas desorption from the surface, the potential will then propagate from the anode toward the cathode until the effective length of the gap is sufficiently reduced to support flashover. The underlying physical mechanisms of cathode- and anode-directed flashover are discussed in light of previously gathered experimental data and recent experiments with pulsed, high-gradient, anode-initiated flashover.

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A Liquid Stratification Model to Predict Failure in Thermally Damaged EBW Detonators

Propellants, Explosives, Pyrotechnics

Hobbs, Michael L.; Coronel, Stephanie A.

In previous work, commercially available downward facing exploding bridgewire detonators (EBWs) were exposed to elevated temperatures. These detonators were then initiated using a firing set which discharged a high amplitude short duration electrical pulse into a thin gold bridgewire. Responses of the detonators were measured using photonic doppler velocimetry (PDV) and high-speed photography. A time delay of 2 μs between EBW initiation and first movement of an output flyer separated operable detonators from inoperable detonators or duds. In the current work, we propose a simple method to determine detonator operability from the calculated state of the detonator at the time the firing set is initiated. The failure criterion is based on the gap distance between the exploding bridgewire (EBW) and the adjacent initiating explosive within the detonator which is low-density pentaerythritol tetranitrate (PETN) that melts between 413–415 K (140–142 °C). The gap forms as PETN melts and flows to the bottom of the input pellet. Melting of PETN is modeled thermodynamically as an energy sink using a normal distribution spread over a temperature range between the onset temperature of 413 K and the ending temperature of 415 K. The extent of the melt is determined from the average temperature of the PETN. The PETN liquid is assumed to occupy the interstitial gas volume in the lower part of the input pellet. The vacated volume from the relocated liquid forms the gap between the EBW and the PETN. The remaining sandwiched layer consists of solid PETN particles and gas filling interstitial volume. We predict that a threshold gap between 17–27 μm separates properly functioning detonators from duds.

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Results 6651–6675 of 100,993
Results 6651–6675 of 100,993
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