Publications

Tappan, Alexander S.; Ball, James P.; Miller, Jill C.

Abstract not provided.

Tappan, Alexander S.; Ball, James P.; Miller, Jill C.

Abstract not provided.

AIP Conference Proceedings

Tappan, Alexander S.; Knepper, Robert; Wixom, Ryan R.; Marquez, Michael P.; Ball, J.P.; Miller, Jill C.

The use of physical vapor deposition is an attractive technique to produce microenergetic samples to study sub-millimeter explosive behavior. Films of the high explosive PETN (pentaerythritol tetranitrate) were deposited through vacuum thermal sublimation. Deposition conditions were varied to understand the effect of substrate cooling capacity and substrate temperature during deposition. PETN films were characterized with surface profilometry and scanning electron microscopy. Detonation velocity versus PETN film thickness was analyzed using a variation of the standard form for analysis of the diameter effect. Results were compared with previous work conducted on PETN films deposited with lower substrate cooling capacity. Seemingly subtle variations in PETN deposition conditions led to differences in detonation behaviors such as critical thickness for detonation, detonation velocity at "infinite" thickness, and the shape of the critical thickness curves. © 2012 American Institute of Physics.

Tappan, Alexander S.; Knepper, Robert; Wixom, Ryan R.; Marquez, Michael P.; Ball, James P.; Miller, Jill C.

Abstract not provided.

Proceedings - 14th International Detonation Symposium, IDS 2010

Tappan, Alexander S.; Knepper, Robert; Wixom, Ryan R.; Miller, Jill C.; Marquez, Michael P.; Ball, J.P.

Abstract not provided.

Tappan, Alexander S.; Knepper, Robert; Wixom, Ryan R.; Baer, Melvin B.; Marquez, Michael P.; Ball, James P.; Miller, Jill C.

Abstract not provided.

Tappan, Alexander S.; Knepper, Robert; Wixom, Ryan R.; Miller, Jill C.; Marquez, Michael P.; Ball, James P.

Abstract not provided.

Bickes, Robert W.; Smith, Stuart A.; Rivera, Wayne G.; Renlund, Anita M.; Miller, Jill C.

Abstract not provided.

Ulibarri, Tamara A.; Erickson, Kenneth L.; Wiemann, Dora K.; Erickson, Kenneth L.; Castaneda, Jaime N.; Borek, Theodore T.; Renlund, Anita M.; Miller, Jill C.

Preliminary thermal decomposition experiments with Ablefoam and EF-AR20 foam (Ablefoam replacement) were done to determine the important chemical and associated physical phenomena that should be investigated to develop the foam decomposition chemistry sub-models that are required in numerical simulations of the fire-induced response of foam-filled engineered systems for nuclear safety applications. Although the two epoxy foams are physically and chemically similar, the thermal decomposition of each foam involves different chemical mechanisms, and the associated physical behavior of the foams, particularly ''foaming'' and ''liquefaction,'' have significant implications for modeling. A simplified decomposition chemistry sub-model is suggested that, subject to certain caveats, may be appropriate for ''scoping-type'' calculations.

Tappan, Alexander S.; Renlund, Anita M.; Miller, Jill C.

The HMX {beta}-{delta} solid-solid phase transition, which occurs as HMX is heated near 170 C, is linked to increased reactivity and sensitivity to initiation. Thermally damaged energetic materials (EMs) containing HMX therefore may present a safety concern. Information about the phase transition is vital to predictive safety models for HMX and HMX-containing EMs. We report work on monitoring the phase transition with real-time Raman spectroscopy aimed towards obtaining a better understanding of physical properties of HMX through the phase transition. HMX samples were confined in a cell of minimal free volume in a displacement-controlled or load-controlled arrangement. The cell was heated and then cooled at controlled rates while real-time Raman spectroscopic measurements were performed. Raman spectroscopy provides a clear distinction between the phases of HMX because the vibrational transitions of the molecule change with conformational changes associated with the phase transition. Temperature of phase transition versus load data are presented for both the heating and cooling cycles in the load-controlled apparatus, and general trends are discussed. A weak dependence of the temperature of phase transition on load was discovered during the heating cycle, with higher loads causing the phase transition to occur at a higher temperature. This was especially true in the temperature of completion of phase transition data as opposed to the temperature of onset of phase transition data. A stronger dependence on load was observed in the cooling cycle, with higher loads causing the reverse phase transitions to occur at a higher cooling temperature. Also, higher loads tended to cause the phase transition to occur over a longer period of time in the heating cycle and over a shorter period of time in the cooling cycle. All three of the pure HMX phases ({alpha}, {beta} and {delta}) were detected on cooling of the heated samples, either in pure form or as a mixture.