Reaction Zone of Steady-State Detonation Waves in Dinitrodiazapentane and RDX

Author(s):  
Sergey A. Kolesnikov

Measurements are described of the reflexion and transmission of 3 cm wavelength microwaves b y detonation waves in stoichiometric oxyhydrogen seeded with nitrogen, and oxyacetylene mixtures. Conductivity measurementsare also obtained by means of two types of d.c. probe, termed ‘axial’ and ‘gap ’ probe respectively. The observed reflexion coefficient in the oxyhydrogen waves is approximately tenfold greater than the calculated value assuming a step profile and equilibrium ionization at the detonation front. The character of the gap probe records indicates that regions of higher ionization occur along the detonation tube axis at locations which correspond to the intersection points o f the oblique shock waves generated b y the wavefront and the w all boundary layer. It is shown that the enhanced power reflexion can be explained in terms of these regions. Microwave absorption and d.c. axial probe measurements give values of conductivity in reasonable agreement with theory, assuming the absence of OH ions. The measured values o f reflected pow er and conductivity in oxyacetylene waves show no anomaly for initial gas pressures in the range 760 to roughly 300 m m H g. A t lower pressures the reflexion coefficient is w ell in excess o f the calculated value and both m icrow ave and d.c. probes exhibit a frontal ionization peak. This is in accord with the observation, by other investigators, o f chemiluminescence in the reaction zone of waves in organic fuel mixtures and chemi-ionization process in the reaction zone of flames. A value for the ionelectron recombination rate constant is derived which is in agreement with that observed in flames.


Detonation performance is defined in terms of the steady state wave structure of the detonation front, and the initiation behaviour of the explosive. Some common techniques for modelling detonation performance are described, based on semi-analytic hydrodynamic and computational fluid dynamic reactive flow models. Accurate modelling of detonation performance is shown to require resolution of the reaction zone in the explosive, for non-ideal and for intrinsically unreactive systems. The ability of detonation models to predict steady state and initiation performance is discussed. Examples of resolve reaction zone models of explosives of varying degrees of ideality are presented. The sensitivity of predictions to primary data is examined for steady state reaction zone modelling of the insensitive explosive PBX W115, and Composition B3. Future directions for development of reactive flow models are examined. Particular emphasis is drawn to the need for more detailed temperature dependent kinetic schemes, and the inclusion of more detailed reaction geometries in such flow models.


2007 ◽  
Vol 580 ◽  
pp. 31-81 ◽  
Author(s):  
MATEI I. RADULESCU ◽  
GARY J. SHARPE ◽  
CHUNG K. LAW ◽  
JOHN H. S. LEE

The study analyses the cellular reaction zone structure of unstable methane–oxygen detonations, which are characterized by large hydrodynamic fluctuations and unreacted pockets with a fine structure. Complementary series of experiments and numerical simulations are presented, which illustrate the important role of hydrodynamic instabilities and diffusive phenomena in dictating the global reaction rate in detonations. The quantitative comparison between experiment and numerics also permits identification of the current limitations of numerical simulations in capturing these effects. Simulations are also performed for parameters corresponding to weakly unstable cellular detonations, which are used for comparison and validation. The numerical and experimental results are used to guide the formulation of a stochastic steady one-dimensional representation for such detonation waves. The numerically obtained flow fields were Favre-averaged in time and space. The resulting one-dimensional profiles for the mean values and fluctuations reveal the two important length scales, the first being associated with the chemical exothermicity and the second (the ‘hydrodynamic thickness’) with the slower dissipation of the hydrodynamic fluctuations, which govern the location of the average sonic surface. This second length scale is found to be much longer than that predicted by one-dimensional reaction zone calculations.


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