Investigation of the detonation regimes in gaseous mixtures with suspendedstarch particles

Citation
B. Veyssiere et al., Investigation of the detonation regimes in gaseous mixtures with suspendedstarch particles, SHOCK WAVES, 9(3), 1999, pp. 165-172
Citations number
10
Categorie Soggetti
Mechanical Engineering
Journal title
SHOCK WAVES
ISSN journal
09381287 → ACNP
Volume
9
Issue
3
Year of publication
1999
Pages
165 - 172
Database
ISI
SICI code
0938-1287(199906)9:3<165:IOTDRI>2.0.ZU;2-9
Abstract
The existence of a secondary discontinuity at the rear of a detonation fron t shown in experiments by Peraldi and Veyssiere (1986) in stoichiometric hy drogen-oxygen mixtures with suspended 20-mu m starch particles has not been explained satisfactorily. Recently Veyssiere et al. (1997) analyzed these results using a one-dimensional (1-D) numerical model, and concluded that t he heat release rate provided by the burning of starch particles in gaseous detonation products is too weak to support a double-front detonation (DFD) ; in contrast to the case of hybrid mixtures of hydrogen-air with suspended aluminium particles in which a double-front detonation structure was obser ved by Veyssiere (1986). A two-dimensional (2-D) numerical model was used i n the present work to investigate abovementioned experimental results for h ybrid mixtures with starch particles. The formation and propagation of the detonation has been examined in the geometry similar to the experimental tu be of Peraldi and Veyssiere (1986); which has an area change after 2 m of p ropagation from the ignition point from a 69 mm dia. section to a 53 mm x 5 3 mm square cross section corresponding to a 33% area contraction. It is sh own that the detonation propagation regime in these experiments has a diffe rent nature from the double-front detonation observed in hybrid mixtures wi th aluminium particles. The detonation propagates as a pseudo-gas detonatio n (PGD) because starch particles release their heat downstream of the CJ pl ane giving rise to a non-stationary compression wave. The discontinuity wav e at the rear of the detonation front is due to the interaction of the lead ing detonation front with the tube contraction, and is detected at the fart hest pressure gauge location because the tube length is insufficient for th e perturbation generated by the tube contraction to decay. Thus, numerical simulations explain experimental observations made by Peraldi and Veyssiere (1986).