Analysis of Solid Explosion Products of Mixtures Based on HMX and Peroxide Benzoyl with Aluminum

The explosive transformation of mixtures of HMX and benzoyl peroxide with aluminum was studied. Aluminum oxides formed during initiation of an impact explosion were investigated. An x-ray analysis showed that aluminum is not oxidized during explosion of its mixtures with benzoyl peroxide. An analysis was made of aluminum oxides formed during explosion of HMX mixtures with aluminum hydride and ternary mixtures of aluminum, HMX, and benzoyl peroxide. It was found that the state of aluminum introduced into the composition and the explosion temperature influence the structure of aluminum oxide (Al8/3O4), whose lattice is a derivative of the spinel lattice.     

On the interpretation of vapor pressure measurements on oxide fuel at very-high temperatures for fast reactor safety analysis

Safety analysis of fast reactors requires knowledge of the evaporation behavior and the total vapor pressure of oxide fuel materials in the temperature region from 3000 K upwards. Dynamic vapor pressure measurements on liquid oxide fuels performed in open-evaporation experiments with laser heating techniques imply strong alterations in the composition of the incongruently evaporating fuel surface, since, during evaporation, the depletion in the preferentially evaporating components cannot be resupplied by diffusion from the bulk material. After a short transient evaporation period stationary surface-evaporation is reached with a surface composition which differs greatly from the given fuel composition and depends on the actual evaporation temperature. When this stationary forced-congruent evaporation mode is reached, the gross vapor composition is well-defined and is identical to the bulk composition of the fuel but is quite different from the actual surface composition. In consequence, the total vapor pressure developing in open surface-evaporation of a liquid oxide fuel can substantially deviate from its thermodynamic equation-of-state, in the case of (U_0.80Pu_0.20) mixed oxide by a factor of 2 to 7 depending on the $\text{O}\text{M}$-ratio. Following these thermodynamic calculations direct measurement of the equation-of-state in open-evaporation experiments is practically impossible. Theoretically fitted expressions applicable in reactor safety analysis are presented for the equations-of-state and the vapor pressure equations for open surface-evaporation and also for the heats of evaporation of liquid (U_0.80Pu_0.20)O_1.95…2.00 mixed oxides.     

Corrosion resistance of silicon-infiltrated silicon carbide (SiSiC)

Silicon carbide ceramics have found widespread use due to their high corrosion stability. Both solid state-sintered silicon carbide, which has an extremely high corrosion resistance, and silicon-infiltrated silicon carbide are used for various applications. The latter material contains SiC as well as free silicon, which is less stable. Hence, in the present work, the corrosion behavior of silicon-infiltrated silicon carbide ceramics was investigated in NaOH solutions. Long-term corrosion experiments were conducted, and a method for analyzing the corrosion behavior in short-term experiments was developed. The short-term method is based on the accurate measurement of the corrosion depth by laser scanning microscopy on polished surfaces. The results of both methods were in good agreement. The advantage of the short-term method is that it provides information on changes in corrosion mechanisms and corrosion rates in the initial period and as a function of the impurities present. Preferential corrosion of Si at the interface to SiC was observed. TEM investigations revealed that this enhanced corrosion was caused by the segregation of impurities.     

X-ray tomographic microscopy of fibre-reinforced materials

Aluminium composites containing Al₂O₃ fibres and precipitates of various intermetallic phases are investigated by high-resolution computerized microtomography. Individual fibres 15 μm in diameter and intermetallic phases forming a network with about 15 μm mesh size have been imaged. The capabilities of the method and its further development down 1 μm and less spatial resolution are discussed.