Density of RDX Crystals Grown During High Acceleration in an Ultracentrifuge

2005 ◽  
Vol 896 ◽  
Author(s):  
Mary Y. D. Lanzerotti ◽  
Richard Z. Squillace ◽  
Alexander Gandzelko ◽  
Jagadish Sharma

AbstractRDX (cyclotrimethylene-trinitramine) crystals were grown during high acceleration (high g) in an ultracentrifuge. These crystals are found to have a density ∼0.6% greater than 1 g crystals and to have a greatly reduced defect content. The high g crystals should therefore have significantly reduced shock sensitivity as compared to commercial grade RDX. When a RDX saturated acetone solution is accelerated at 200,000 g, the RDX solute molecules move individually through the acetone solvent molecules to form a RDX crystal because the density of the RDX (Theoretical Maximum Density 1.806 g/cc) solute is more dense than the acetone (0.79 g/cc)solvent. Crystal growth is controlled by the g-force. Crystal defects including voids and solution inclusions caused by temperature variation or evaporation at 1 g are minimized and the RDX crystal density increases. A nitrogen pycnometer was used to measure the density of the RDX crystals grown at 1 g and at 200,000 g. The density of the RDX crystals grown at 200,000 g (1.7980±0.0003 g/cc) is found to be greater than the density of RDX crystals grown at 1 g (1.7881±0.0003 g/cc) by 0.0099 g/cc. The density of the high g crystal is 99.6% of the Theoretical Maximum Density of RDX.

1995 ◽  
Vol 418 ◽  
Author(s):  
M. Y. D. Lanzerotti ◽  
J. Autera ◽  
L. Borne ◽  
J. Sharma

AbstractStudies of the growth of crystals of energetic materials under conditions of high acceleration in an ultracentrifuge are reported. When a saturated solution is accelerated in an ultracentrifuge, the solute molecules move individually through the solvent molecules to form a crystal at the outer edge of the tube if the solute is more dense than the solvent. Since there is no evaporation or temperature variation, convection currents caused by simultaneous movement of solvent and solute are minimized and crystal defects are potentially minimized. Crystal growth is controlled by the g-level of the acceleration. In addition, solution inclusions and bubbles migrate out of the saturated solution as a result of the pressure gradient induced by the g-force. We present results of TNT, RDX, and TNAZ grown at high g from various solutions.


Author(s):  
M. Y. D. Lanzerotti ◽  
J. Autera ◽  
J. Pinto ◽  
J. Sharma

1994 ◽  
Vol 362 ◽  
Author(s):  
M. Yvonne D. Lanzerotti ◽  
J. Sharma

AbstractThe mechanical behavior of explosives subjected to high acceleration (high g) has been studied in an ultracentrifuge. The experiments reported here reveal new information on the mechanical behavior of such materials and the influence of grain size on the fracture process. Through measurement and analysis of fracture surfaces, we have found that predominately intergranular failure occurs when the shear or tensile strength of the explosive is exceeded. We have found that the mechanical strength of melt-cast polycrystalline TNT varies inversely with crystal size. That is, if the sample consists of large, homogeneous crystals, these are found to separate from the sample at lower g-levels due to the larger mass-to-binding surface area ratio of the crystals. Conversely, smaller original crystallites are found to separate at higher g-levets due to the smaller mass-to-binding surface area ratio. Our results show that single crystals of TNT fracture under a higher g-level at crystal defects. We have also found that the fracture acceleration of Octol decreases with increasing percent TNT and decreasing percent HMX. Hexanitrostilbene (HNS) has been shown by other investigators to be an effective additive to prevent growth of large TNT grains. We have found that the fracture acceleration increases when HNS is added to Octol.


2015 ◽  
Vol 179 ◽  
pp. 475-488 ◽  
Author(s):  
Baptiste Fours ◽  
Yohann Cartigny ◽  
Samuel Petit ◽  
Gérard Coquerel

Rimonabant monohydrate can be dehydrated at 100 °C or above with complete loss of structural information; in this case the amorphous material can lead to nucleation and crystal growth. The water molecules can also be removed by a smooth process below Tg (78 °C) of the anhydrous phase. In that latter process there is a structural filiation between the mother phase and the daughter phase. The solvent molecules escape from the mother structure by using a network of specific channels; the new non-solvated material undergoes a relaxation process similar to a directional crystallization. By this soft mode of desolvation inside a material which has a very limited mobility, the nucleation of a non-solvated material can be avoided. The structural information contained in the mother phase is not used as a template for crystal growth but it is more a progressive rearrangement of the new desolvated material towards the nearest well in energy. Thus, a metastable new polymorph of a non-solvated component can be obtained by: (i) the crystallization of the component as a solvate and (ii) a smooth desolvation at T < Tg. Other parameters liable to interfere with that transmission of structural information are discussed.


1997 ◽  
pp. 213-219
Author(s):  
M. Y. D. Lanzerotti ◽  
J. Autera ◽  
L. Borne ◽  
J. Sharma

1968 ◽  
Vol 23 (7) ◽  
pp. 997-1000 ◽  
Author(s):  
Erich W. Labouvie

It is shown by an etching method joined with microscopical observations that the structure of Rochelle salt crystals is not very much disturbed by dislocations and sudares. The correlation between the distributions of dislocations and sudares is obviously determined by the process of crystal growth. Measurements of the upper Curie-point and the dielectric constant are made in order to reveal some influence of these crystal defects on the dielectric properties.


1994 ◽  
Author(s):  
M. Y. D. Lanzerotti ◽  
J. Autera ◽  
J. Pinto ◽  
J. Sharma

1992 ◽  
Vol 119 (1-2) ◽  
pp. 79-93 ◽  
Author(s):  
H. Wiedemeier ◽  
L.L. Regel ◽  
W. Palosz

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