GASFLOW-MPI analysis on deflagration in full-scale hydrogen refueling station experiments: H2-air premixed cloud and high-pressure H2 jet

被引:16
作者
Wang, Fangnian [1 ]
Xiao, Jianjun [1 ]
Jordan, Thomas [1 ]
机构
[1] Germany Karlsruhe Inst Technol KIT, Inst Thermal Energy Technol & Safety ITES, Karlsruhe, Germany
关键词
Hydrogen deflagration; Premixed cloud; High-pressure jet; GASFLOW-MPI; Hydrogen refueling station; SPEED CFD CODE; TURBULENT DISPERSION; COMBUSTION; SIMULATION; AIR;
D O I
10.1016/j.ijhydene.2022.02.215
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
Safety of the hydrogen refueling station under a postulated accident (e.g. leakage) is of great importance in hydrogen energy. The predictive CFD tool GASFLOW-MPI is utilized to simulate the full-scale hydrogen refueling station deflagration experiments with premixed H-2-air cloud and high-pressure H-2 jet. The overpressures are predicted for an ignition between two dispensers in the premixed trial and a spark in the engine bay in the jet trial, which agree with the experimental data and validate the GASFLOW-MPI as well. Five turbulent burning velocity models are involved to investigate the explosion of the premixed H-2-air cloud. The Zimont correlation is recommended for the combustion simulation of engineering full-scale H-2 refueling station. The turbulent flame speed is predicted after an ignition resulting in 50-200 m/s, and the flame acceleration happens due to the turbulence effect by obstacles. The developments of the pressure, temperature and H-2 concentration of premixed H-2-air deflagration, indicate the pressure wave propagates with the reflections on obstacles, and the flammable H-2 cloud is enlarged by the push of combustion product Moreover, the standard k - epsilon and DES model are adopted on the jet dispersion analysis. The local flow variables show some differences, but the global properties of average hydrogen concentration, the shape and size of the burnable cloud are similar, which indicates the hydrogen dispersion transient computed by k - epsilon turbulence model provides a reliable basis for estimating the combustion process. The evolutions of the jet resulting burnable H-2-air mixture in the domain in terms of H-2 velocity field, concentration and mass are evaluated. The velocity field in jet trial explains that the momentum dominates hydrogen dispersion and result in a corresponding hydrogen concentration, however a large zone with high turbulence forms after combustion. The analysis of H-2 dispersed in the engine bay shows the growth and decay of the hydrogen concentration above some specified value of interest (4 and 10 vol% H-2). Most dispersed H-2 cloud is burnable, and half of the mass distributed in the cloud above 10 vol% may accelerate the flame to sonic. The comparison of the overpressure in k - epsilon and DES turbulence models with real and ideal gas release sources, shows in general no significant difference. The hydrogen release jet with higher turbulence generates the hydrogen cloud that can result in a large overpressure. (c) 2022 Hydrogen Energy Publications LLC. Published by Elsevier Ltd. All rights reserved.& nbsp;& nbsp;
引用
收藏
页码:14725 / 14739
页数:15
相关论文
共 34 条
[1]   SARNET hydrogen deflagration benchmarks: Main outcomes and conclusions [J].
Bentaib, A. ;
Bleyer, A. ;
Meynet, N. ;
Chaumeix, N. ;
Schramm, B. ;
Hoehne, M. ;
Kostka, P. ;
Movahed, M. ;
Worapittayaporn, S. ;
Braehler, T. ;
Seok-Kang, H. ;
Povilaitis, M. ;
Kljenak, I. ;
Sathiah, P. .
ANNALS OF NUCLEAR ENERGY, 2014, 74 :143-152
[2]  
Bentaib A, 2012, SARNET H2 COMBUSTION
[3]   Analysis of transient supersonic hydrogen release, dispersion and combustion [J].
Breitung, Wolfgang ;
Halmer, Gerold ;
Kuznetsou, Mike ;
Xiao, Jianjun .
INTERNATIONAL JOURNAL OF HYDROGEN ENERGY, 2019, 44 (17) :9089-9099
[4]  
Burke Eoin M., 2016, UNSP V04BT04A043, V4B
[5]  
Cheng Z, 2005, PAPER 110090, P8
[6]   Three-dimensional computational fluid dynamics simulation of hydrogen engines using a turbulent flame speed closure combustion model [J].
Gerke, Udo ;
Boulouchos, Konstantinos .
INTERNATIONAL JOURNAL OF ENGINE RESEARCH, 2012, 13 (05) :464-481
[7]   CFD simulations of premixed hydrogen combustion using the Eddy Dissipation and the Turbulent Flame Closure models [J].
Halouane, Y. ;
Dehbi, A. .
INTERNATIONAL JOURNAL OF HYDROGEN ENERGY, 2017, 42 (34) :21990-22004
[8]   THE TURBULENT WALL JET - MEASUREMENTS AND MODELING [J].
LAUNDER, BE ;
RODI, W .
ANNUAL REVIEW OF FLUID MECHANICS, 1983, 15 :429-459
[9]  
Magnussen B.F., 1976, Symp (Int) Combust, V16, P719, DOI [DOI 10.1016/S0082-0784(77)80366-4, 10.1016/S0082-0784(77)80366-4]
[10]   An inter-comparison exercise on CFD model capabilities to predict a hydrogen explosion in a simulated vehicle refuelling environment [J].
Makarov, D. ;
Verbecke, F. ;
Molkov, V. ;
Roe, O. ;
Skotenne, M. ;
Kotchourko, A. ;
Lelyakin, A. ;
Yanez, J. ;
Hansen, O. ;
Middha, P. ;
Ledin, S. ;
Baraldi, D. ;
Heitsch, M. ;
Efimenko, A. ;
Gavrikov, A. .
INTERNATIONAL JOURNAL OF HYDROGEN ENERGY, 2009, 34 (06) :2800-2814