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Session R4 - Shock Synthesis.
ORAL session, Friday morning, July 02
Superior Room, Cliff Lodge Convention Center

[R4.01] Analytical Modeling of Shear-Induced Chemical Reactions in Mixed Powders

Yasuyuki Horie (North Caolina State University, Raleigh, NC 27695-7908)

A theoretical model is formulated to describe a complex interplay of mechanical, thermal, chemical processes associated with intense shear in mixed powders. The model is an outgrowth of a recent numerical study of chemical reactions in Nb-Si and Ni-Al mixtures. In the analytical model, mass mixing of constituents is represented effectively by a mixing characteristic time, which is assumed to be a function of strain rate. The overall governing equations resemble a theory of continuously stirred chemical reactors. Using a dimensionless system of equations, we show a variety of flow regimes in terms of the mixing time, whcih is found to be equivalent to residence time in the reactor theory. Solutions include oscillatory as well as discontious behavior. The conditions of spontaneous ignition and extinction are evaluated in terms of dimensionnless groups that are functions of process parameters such as surface heat transfer coefficient, heat of reaction, and the width of shear bands. The ignition conditions are also examined in the context of shock-wave processing.

[R4.02] Shock Induced Reaction to Refractory Metal Di-Silicides from MA Precursor

Tatsuhiko Aizawa (Department of metallurgy, University of Tokyo), Ken-ichi Ichige (Department of Metallurgy,University of Tokyo), Yasuhiko Syono (Institute of materials Research, Tohoku Univerisity), Silicide Collaboration

In general, when using the elemental powder mixes, little or no reactions occurred; since full reactivity can be realized when starting from the MA precursors or the pretretaed element constituent mixes by mechanical miling, variation of shock loading conditions leads to direct investigation of shock reaction mechanism in terms of post-shock analyses. In this paper, Mo-Si and Ti-Si systems are employed to discuss the fundamental shock induced reaction process intrinsic to each system. The feature common to these systems is that the shock induced reaction should be composed of two or more steps. In Mo-2Si system, the amorphous phase might be first synthesized during shock loading and followed by the regularization process into MoSi2. Through microstructure observation of post-shock samples, volume fraction of amorphous phase, with the local chemical compositions varying from Mo60Si40 to Mo40Si60, increases with decreasing the shock pressure. On the other hand, no intermediate phase can be seen in the microstructure in Ti-Si system; regularization process into TiSi2 in the same shock loading condition is activated by increasing the milling time. Local fine mixture of Ti and Si or solid-solution-like phase can be seen through precise microstructure observation. TEM analysis is further performed to describe these pre-regularization processes and to discuss the effect of shock loading condition on the transient reaction path to synthesize the refractory metal di-silides with consideration on the role of Si.

[R4.03] An Analysis of Shock-Compression in Mo-Si Powder Mixtures Using Recovery and Time-Resolved Measurements

Kevin S. Vandersall, Naresh N. Thadhani (Georgia Institute of Technology)

The densification and reaction characteristics in the Mo-Si system were investigated utilizing recovery experiments as well as time resolved measurements with in-situ stress gages. The starting sample in all cases consisted of statically pressed Mo + 2 Si powder mixtures (\sim55% TMD). The recovery experiments were performed using the Sandia Momma Bear and Momma Bear A fixtures with baratol and composition B explosives respectively. The instrumented experiments were performed in a capsule design similar to that of the Momma Bear, but modified to incorporate poly-vinyl di-flouride (PVDF) stress gages at the front and rear surfaces of the powder. These experiments were performed using a single stage gas gun in the velocity range of 500 m/s to 1 km/s. The instrumented experiments allow the crush strength, densification history, and reaction threshold to be mapped at increasing pressure to correlate with reaction observed in the recovery experiments.

[R4.04] Possibility of making polycrystalline diamond using high-temperature shock consolidation technique

Kazuyuki Hokamoto, Masahiro Fujita (Dept. of Mech. Eng. amp; Mater. Sci.,Kumamoto University, Japan), Sei-ichiro Tanaka (Kumamoto Prefectural College of Technology, Japan), Makoto Ayabe (Graduate Student, Kumamoto University), Shigeru Itoh (Dept. of Mech. Eng. amp; Mater. Sci., Kumamoto University, Japan)

The making of polycrystalline diamond using shock compaction technique has been pursued by many researchers, but the difficulty is due to cracking by the propagation of strong shock wave and the lack of interparticle bonding through an intensive surface deformation. The authors tried to develop high-temperature shock compression apparatus using converging underwater shock wave. Some of the samples are successfully recovered up to 1373 K though the samples are cracked. One of the polycrystalline diamond recovered shows high Vickers hardness above 90 GPa, which corresponds with the value of natural diamond, based on the strong interparticle bonding between particles by the help of heating. High fracture toughness is measured for the sample which depends on the isotropic property.

[R4.05] Shock and impact initiation of a porous incendiary material

Jeffery Davis (Naval Air Warfare Center, China Lake CA 93555), Phil Miller, Diana Woody

A series of gas gun tests has been performed on an energetic composition containing KClO4 and Al/Mg. These materials are currently being developed for an initiation system in medium caliber bullets. Initiation begins upon impact of the bullet with the target through the interaction of the compaction wave with an incendiary charge. In order to better understand the deformation - initiation process, experiments have been performed in which the incendiary charge was impact tested via gas gun at velocities ranging from 0.33 - 0.98 mm/ms at two densities: 84 and 70

[R4.06] Attempts to initiate detonations in metal-sulfur mixtures

Samuel Goroshin, Junping Jiang, John H.S. Lee, Massimiliano Romano (McGill University, Canada)

Deflagration waves, which convert solid reactants into solid products, have been observed in certain inorganic mixtures. The possibility of self-sustained "gasless" detonation waves has yet to be experimentally demonstrated. The present study attempts to initiate detonation in metal-sulfur mixtures. Specifically, manganese-sulfur mixtures are used because they are extremely energetic with flame temperature as high as 4000 K and all their detonation products exist in a condensed phase. The charges were 50 mm in diameter and 250 mm long, and were confined with a heavy walled steel pipe. At one end, a short length of bare Mn-S charge was wrapped with sheet explosive. Upon initiation of the sheet explosive, a strong Mach disk was driven into the Mn-S charge. Contact gauges and ion probes were used to monitor the shock and reaction front in the charge. The results indicate that the speed of the reaction front in the part of the charge surrounded by explosive was 6-7 km/sec, but quickly decelerated to below 2.5 km/s as it propagated into steel-confined charge. The results indicate that self-sustained "gasless" detonation is not observed even using an overdriven Mach disk for initiation. Rapid reactions can be initiated by shock wave, but the shock wave apparently cannot be maintained without significant volume expansion in the products.

[R4.07] Three-dimensional modeling of impact of capsule with Ti-C powder mixture on target

Vassili A. Gorelski, Vadim V. Kim, Aleksei Yu. Smolin (Tomsk Branch of the Institute of Structural Macrokinetics and Materials Science RAS)

A problem of oblique high-velocity interaction of a steel capsule containing stoichiometric porous mixture of titanium and carbon with a rigid wall is considered. The angle of impact is 15^\circ, the impact velocity is varied in the range of 500--1200~m/s. The diameter of the capsule is 7.62~mm, the height is 26~mm. Three values of the initial porosity of the mixture are used: 0%, 50% and 70%. The set of equations describing adiabatic motion of a compressible chemically active medium consists of the equations of continuity, motion, energy, chemical kinetics and the equation describing generation and growth of the specific volume of pores. The finite-element method is used for solving the problem. The time-dependencies for specific volume of pores, pressure and interaction force as well as configurations of the capsule at different times are analyzed. The influence of initial velocity and porosity on chemical reaction is revealed. The results of simulation allows to subdivide the process into three stages: 1)~when only compaction process occurs, 2)~the chemical reaction of synthesis takes place in porousless mixture near the contact surface, 3)~the chemical reaction takes place in mixture at the upper side of the capsule.

[R4.08] Investigation of Role of Cocentration Ingomogeneity of Powder Mixture in the Initiation of "Shock-Induced" Chemical Reaction

V.N. Leitsin, V.A. Skripnyak (Tomsk State University, Russia)

The main aim of the work is development of thermo-mechanical initiation model of chemical reactions under deformation of powders mixtures as Ti-Al. Computer simulation of processes, occurring in reacting laier at shock compression showed: 1. The rection of synthesis of intermetallic compounds in systems Ti-Al can be "self-assisted"; 2. The speed of propagation of front of chemical transformations is defined by a degree and papameters of spatial concentration inhomogeneity of powders mixture; 3. Necessery conditions for initiation of "shock-induced" chemical reactions includes the presence of non-zero porosity and certain initial temperature of a mixture. It is essential, that reduction of porosity and degree of concentration ingomogeneity of powder mixture can lead to changing of a mode of reaction and down to complete its prohibition.

Part R of program listing