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Dive into the research topics where Aaron L. Brundage is active.

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Featured researches published by Aaron L. Brundage.


Journal of Fire Sciences | 2011

Thermocouple Response in Fires, Part 1: Considerations in Flame Temperature Measurements by a Thermocouple

Aaron L. Brundage; A. Burl Donaldson; Walter Gill; Sean P. Kearney; Vern F. Nicolette; Nadir Yilmaz

This PIRT exercise identifies a number of factors which can influence thermocouple readings made in fires. Identified factors are: (a) the fuel/oxidizer equivalence ratio and its effect on readings, (b) the influence of the state of oxidation and variation with time for the thermocouple sheath, (c) the convection coefficient models and how experimental readings are influenced by thermocouple diameter and yaw angle, (d) response time of a MIMS thermocouple, and (e) thermocouple end effects.


Journal of Materials Research | 2010

Characterization of pore morphology in molecular crystal explosives by focused ion-beam nanotomography

Ryan R. Wixom; Alexander S. Tappan; Aaron L. Brundage; Robert Knepper; M. Barry Ritchey; Joseph R. Michael; Michael J. Rye

The initiation and detonation properties of explosives are often empirically correlated to density, surface area, and particle size. Although these correlations are sometimes used successfully to predict the performance of bulk samples, the data are spatially averaged, which unfortunately muddles information critical to understanding fundamental processes. Density and surface area are essentially an indirect measure of porosity, which is arguably a more appropriate metric in many applications. We report the direct characterization of porosity in polycrystalline molecular crystal explosives by focused ion beam nanotomography, a technique that is typically reserved for robust materials such as ceramics and metals. The resulting three-dimensional microstructural data are incredibly rich, promising a substantial advance in our ability to unravel the processes governing initiation and detonation of molecular crystal explosives. In a larger context, this work demonstrates that focused ion beam nanotomography may be successfully extended to the investigation of nanoscale porosity in other molecular crystal or polymer materials.


Archive | 2005

A joint computational and experimental study to evaluate Inconel-sheathed thermocouple performance in flames.

Aaron L. Brundage; Vernon F. Nicolette; A. Burl Donaldson; Sean P. Kearney; Walter Gill

A joint experimental and computational study was performed to evaluate the capability of the Sandia Fire Code VULCAN to predict thermocouple response temperature. Thermocouple temperatures recorded by an Inconel-sheathed thermocouple inserted into a near-adiabatic flat flame were predicted by companion VULCAN simulations. The predicted thermocouple temperatures were within 6% of the measured values, with the error primarily attributable to uncertainty in Inconel 600 emissivity and axial conduction losses along the length of the thermocouple assembly. Hence, it is recommended that future thermocouple models (for Inconel-sheathed designs) include a correction for axial conduction. Given the remarkable agreement between experiment and simulation, it is recommended that the analysis be repeated for thermocouples in flames with pollutants such as soot.


SHOCK COMPRESSION OF CONDENSED MATTER 2009: Proceedings of the American Physical Society Topical Group on Shock Compression of Condensed Matter | 2009

MESOSCALE SIMULATIONS OF SHOCK INITIATION IN ENERGETIC MATERIALS CHARACTERIZED BY THREE‐DIMENSIONAL NANOTOMOGRAPHY

Aaron L. Brundage; Ryan R. Wixom; Alexander S. Tappan; Gregory T. Long

Three‐dimensional shock simulations of energetic materials have been conducted to improve our understanding of initiation at the mesoscale. Vapor‐deposited films of PETN and pressed powders of HNS were characterized with a novel three‐dimensional nanotomographic technique. Detailed microstructures were constructed experimentally from a stack of serial electron micrographs obtained by successive milling and imaging in a dual‐beam FIB/SEM. These microstructures were digitized and imported into a multidimensional, multimaterial Eulerian shock physics code. The simulations provided insight into the mechanisms of pore collapse in PETN and HNS samples with distinctly different three‐dimensional pore morphology and distribution. This modeling effort supports investigations of microscale explosive phenomenology and elucidates mechanisms governing initiation of secondary explosives.


Journal of Fire Sciences | 2011

Thermocouple Response in Fires, Part 2: Validation of Virtual Thermocouple Model for Fire Codes

Aaron L. Brundage; A. Burl Donaldson; Walter Gill; Sean P. Kearney; Vern F. Nicolette; Nadir Yilmaz

A virtual thermocouple model for high fidelity multiphysics computer simulation is introduced in this article. Detailed thermocouple and gas temperature (Coherent Anti-Stokes Raman Scattering) measurements were performed using a well-controlled, adiabatic, flat-flame Hencken burner, which provided data for validating the thermocouple model in a Sandia National Laboratories fire code. Comparison of simulation results to test data indicated a mean error of 6% between the thermocouple reading and predicted temperature.


ASME 2015 International Mechanical Engineering Congress and Exposition | 2015

Virtual Simulation of the Effects of Intracranial Fluid Cavitation in Blast-Induced Traumatic Brain Injury

Shivonne Haniff; Paul A. Taylor; Aaron L. Brundage; Damon J. Burnett; Candice Frances Cooper; Arne S. Gullerud; Ryan John Terpsma

A microscale model of the brain was developed in order to understand the details of intracranial fluid cavitation and the damage mechanisms associated with cavitation bubble collapse due to blast-induced traumatic brain injury (TBI). Our macroscale model predicted cavitation in regions of high concentration of cerebrospinal fluid (CSF) and blood. The results from this macroscale simulation directed the development of the microscale model of the superior sagittal sinus (SSS) region. The microscale model includes layers of scalp, skull, dura, superior sagittal sinus, falx, arachnoid, subarachnoid spacing, pia, and gray matter. We conducted numerical simulations to understand the effects of a blast load applied to the scalp with the pressure wave propagating through the layers and eventually causing the cavitation bubbles to collapse. Collapse of these bubbles creates spikes in pressure and von Mises stress downstream from the bubble locations. We investigate the influence of cavitation bubble size, compressive wave amplitude, and internal bubble pressure. The results indicate that these factors may contribute to a greater downstream pressure and von Mises stress which could lead to significant tissue damage.Copyright


SHOCK COMPRESSION OF CONDENSED MATTER - 2011: Proceedings of the Conference of the American Physical Society Topical Group on Shock Compression of Condensed Matter | 2012

Modeling compressive reaction and estimating model uncertainty in shock loaded porous samples of hexanitrostilbene (HNS)

Aaron L. Brundage; Jared C. Gump

Neat pressings of HNS powders have been used in many explosive applications for over 50 years. However, characterization of its crystalline properties has lagged that of other explosives, and the solid stress has been inferred from impact experiments or estimated from mercury porosimetry. This lack of knowledge of the precise crystalline isotherm can contribute to large model uncertainty in the reacted response of pellets to shock impact. At high impact stresses, deflagration-to-detonation transition (DDT) processes initiated by compressive reaction have been interpreted from velocity interferometry at the surface of distended HNS-FP pellets. In particular, the Baer-Nunziato multiphase model in CTH, Sandias Eulerian, finite volume shock propagation code, was used to predict compressive waves in pellets having approximately a 60% theoretical maximum density (TMD). These calculations were repeated with newly acquired isothermal compression measurements of fineparticle HNS using diamond anvil cells to compr...


Bulletin of the American Physical Society | 2009

STATIC AND DYNAMIC COMPACTION OF CL‐20 POWDERS

Marcia A. Cooper; Aaron L. Brundage; Evan C. Dudley

Hexanitrohexaazaisowurtzitane (CL‐20) powders were compacted under quasi‐static and dynamic loading conditions. A uniaxial compression apparatus quasi‐statically compressed the powders to 90% theoretical maximum density with applied stresses up to 0.4 GPa. Dynamic compaction measurements using low‐density pressings approximately 64% theoretical maximum density (TMD) were obtained in a single‐stage gas gun at impact velocities between 0.17–0.95 km/s. Experiments were conducted in a reverse ballistic arrangement in which the projectile contained the CL‐20 powder bed and impacted a target consisting of an aluminized window. VISAR‐measured particle velocities at the explosive‐window interface determined the shock Hugoniot states for pressures up to 1.3 GPa. Approved for public release, SAND2009‐4810C.


Bulletin of the American Physical Society | 2009

MICROENERGETIC SHOCK INITIATION STUDIES ON DEPOSITED FILMS OF PETN

Alexander S. Tappan; Ryan R. Wixom; Wayne M. Trott; Gregory T. Long; Robert Knepper; Aaron L. Brundage; David Alexander Jones

Films of the high explosive PETN (pentaerythritol tetranitrate) up to 500‐μm thick have been deposited through physical vapor deposition, with the intent of creating well‐defined samples for shock‐initiation studies. PETN films were characterized with microscopy, x‐ray diffraction, and focused ion beam nanotomography. These high‐density films were subjected to strong shocks in both the out‐of‐plane and in‐plane orientations. Initiation behavior was monitored with high‐speed framing and streak camera photography. Direct initiation with a donor explosive (either RDX with binder, or CL‐20 with binder) was possible in both orientations, but with the addition of a thin aluminum buffer plate (in‐plane configuration only), initiation proved to be difficult. Initiation was possible with an explosively‐driven 0.13‐mm thick Kapton flyer and direct observation of initiation behavior was examined using streak camera photography at different flyer velocities. Models of this configuration were created using the shock p...


ASME/JSME 2011 8th Thermal Engineering Joint Conference | 2011

Modeling Compressive Reaction in Shock-Driven Secondary Granular Explosives

Aaron L. Brundage

Hexanitrostilbene (HNS) is a secondary, granular explosive with a wide usage in commercial and governmental sectors. For example, HNS is used in the aerospace industry as boosters in rockets, in the oil and gas industry in linear shaped charge designs in wellbore perforating guns, and in a number of applications in the US Department of Energy (DOE) and Department of Defense (DoD). In many of these applications, neat granules of HNS are pressed without binder and device performance is achieved with shock initiation of the powdered bed. Previous studies have demonstrated that powdered explosives do not transmit sharp shocks, but produce dispersive compaction waves. These compaction waves can induce combustion in the material, leading to a phenomenon termed Deflagration-to-Detonation Transition (DDT). The Baer-Nunziato (B-N) multiphase model was developed to predict compressive reaction in granular energetic materials due to shock and non-shock inputs using non-equilibrium multiphase mixture theory. The B-N model was fit to historical data of HNS, and this model was used to predict recent impact experiments where samples pressed to approximately 60% of theoretical maximum density (TMD) were shock loaded by high-velocity flyers [1]. Shock wave computations were performed using CTH, an Eulerian, multimaterial, multidimensional, finite-volume shock physics code developed at Sandia National Laboratories [2]. Predicted interface velocities using the B-N model were shown to be in good agreement with the measurements. Furthermore, an uncertainty quantification study was performed and the computational results are presented with best estimates of uncertainty.Copyright

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Alexander S. Tappan

Sandia National Laboratories

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A. Burl Donaldson

New Mexico State University

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Gregory T. Long

Sandia National Laboratories

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Marcia A. Cooper

Sandia National Laboratories

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Ryan R. Wixom

Sandia National Laboratories

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Sean P. Kearney

Sandia National Laboratories

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Walter Gill

Sandia National Laboratories

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David W. Peterson

United States Forest Service

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Evan C. Dudley

Sandia National Laboratories

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Nadir Yilmaz

New Mexico Institute of Mining and Technology

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