DDT and detonation propagation limits in an obstacle filled tube

作者：Cross Mitchell^*; Ciccarelli Gaby

来源：Journal of Loss Prevention in the Process Industries, 2015, 36: 382-388.

DOI：10.1016/j.jlp.2014.11.020

• Quasi-detonation
• DDT
• Choked-flame
• Explosions

Experiments with hydrogen-air and ethylene-air mixtures at atmospheric pressure were carried out in a 6.1 m long, 0.1 m diameter tube with different obstacle configurations and ignition types. Classical DDT experiments were performed with the first part of the tube filled with equally spaced 75 mm (44% area blockage ratio) orifice-plates. The DDT limits, defining the so-called quasi-detonation regime, where the wave propagates at a velocity above the speed of sound in the products, were found to be well correlated with d/lambda = 1, where d is orifice-plate diameter and lambda is the detonation cell size. The only exception was the rich ethylene limit where d/lambda = 1.9 was found. In a second experiment detonation propagation limits were measured by transmitting a CJ detonation wave into an obstacle filled (same equally spaced 44% orifice plates) section of the tube. An oxy-acetylene driver promptly initiated a detonation wave at one end. In this experiment the quasi-detonation propagation limits were found to agree very well with the d/lambda = 1 correlation. This indicates that the d/lambda = 1 represents a propagation limit. In general, One can conclude that the classical DDT limits measured in an orifice-plate filled tube are governed by the wave propagation mechanism, independent of detonation initiation (DDT process) that can occur locally in the obstacles outside these limits. For rich mixtures, transmission of the quasi-detonation into the smooth tube resulted in CJ detonation wave. However, in a narrow range of mixtures on the lean side, the detonation failed to transmit in the smooth tube. This highlights the critical role that shock reflection plays in the propagation of quasi-detonation waves.

• 出版日期2015-7