Numerical simulation of flame propagation and localized preflame autoignition in enclosures

被引:15
作者
Frolov, S. M. [1 ]
Ivanov, V. S. [1 ]
Basara, B. [2 ]
Suffa, M. [2 ]
机构
[1] NN Semenov Chem Phys Inst, Dept Combust & Explos, Moscow 119991, Russia
[2] AVL LIST GmbH, Adv Simulat Technol, Graz, Austria
基金
俄罗斯基础研究基金会;
关键词
Frontal and volumetric combustion; Enclosure; Numerical simulation; TURBULENT; COMBUSTION; MIXTURE;
D O I
10.1016/j.jlp.2011.09.007
中图分类号
TQ [化学工业];
学科分类号
0817 ;
摘要
A novel computational approach based on the coupled 3D Flame-Tracking-Particle (FTP) method is used for numerical simulation of confined explosions caused by preflame autoignition. The Flame-Tracking (FT) technique implies continuous tracing of the mean flame surface and application of the laminar/turbulent flame velocity concepts. The Particle method is based on the joint velocity-scalar probability density function approach for simulating reactive mixture autoignition in the preflame zone. The coupled algorithm is supplemented with the database of tabulated laminar flame velocities as well as with reaction rates of hydrocarbon fuel oxidation in wide ranges of initial temperature, pressure, and equivalence ratio. The main advantage of the FTP method is that it covers both possible modes of premixed combustion, namely, frontal and volumetric. As examples, combustion of premixed hydrogen-air, propane-air, and n-heptane-air mixtures in enclosures of different geometry is considered. At certain conditions, volumetric hot spots ahead of the propagating flame are identified. These hot spots transform to localized exothermic centers giving birth to spontaneous ignition waves traversing the preflame zone at very high apparent velocities, i.e., nearly homogeneous preflame explosion occurs. The abrupt pressure rise results in the formation of shock waves producing high overpressure peaks after reflections from enclosure walls. (c) 2011 Elsevier Ltd. All rights reserved.
引用
收藏
页码:302 / 309
页数:8
相关论文
共 19 条
[1]  
Basevich VYa., 2007, Russ Chem Rev (Engl Transl), V76, P867
[2]  
Belyaev A. A., 2010, COMBUST EXPLO SHOCK, P30
[3]  
Bradley D, 1992, Symposium (International) on Combustion, V24, P247
[4]  
Damkhler G., 1940, Z. Elektrochem. Angew. Phys. Chem., V46, P601, DOI [10.1002/bbpc.19400461102, DOI 10.1002/BBPC.19400461102]
[5]   Turbulent premixed combustion: Flamelet structure and its effect on turbulent burning velocities [J].
Driscoll, James F. .
PROGRESS IN ENERGY AND COMBUSTION SCIENCE, 2008, 34 (01) :91-134
[6]  
Frolov S. M., 2006, RUSSIAN J CHEM PHYS, V25, P54
[7]  
Frolov S.M., 2010, DEFLAGRATIVE DETONAT, P133
[8]  
Gulder O.L., 1990, P COMBUST INST, V23, P743, DOI [10.1016/S0082-0784(06)80325-5, DOI 10.1016/S0082-0784(06)80325-5]
[9]  
Ivanov V. S., 2010, J FIRE EXPLOSION SAF, V19, P14
[10]   Experimental study of flame propagation in propane-air mixture near rich flammability limits in microgravity [J].
Jarosinski, J ;
Podfilipski, J ;
Gorczakowski, A ;
Veyssiere, B .
COMBUSTION SCIENCE AND TECHNOLOGY, 2002, 174 (09) :21-48