Large Eddy Simulation on the Effects of Pressure on Syngas/Air Turbulent Nonpremixed Jet Flames

被引:7
|
作者
Ciottoli, Pietro P. [1 ]
Lee, Bok Jik [2 ]
Lapenna, Pasquale E. [1 ]
Galassi, Riccardo Malpica [1 ]
Hernandez-Perez, Francisco E. [3 ]
Martelli, Emanuele [4 ]
Valorani, Mauro [1 ]
Im, Hong G. [3 ]
机构
[1] Sapienza Univ Rome, Dept Mech & Aerosp Engn, Rome, Italy
[2] Seoul Natl Univ, Dept Mech & Aerosp Engn, Seoul, South Korea
[3] KAUST, Clean Combust Res Ctr, Thuwal, Saudi Arabia
[4] Campania Univ L Vanvitelli, Dept Engn, Aversa, Italy
基金
新加坡国家研究基金会;
关键词
Large eddy simulation; turbulent jet flames; pressure effects; high-pressure combustion; CONDITIONAL MOMENT CLOSURE; NON-PREMIXED COMBUSTION; DIFFUSION FLAMES; CHEMICAL-KINETICS; SOOT FORMATION; NOX FORMATION; A-PRIORI; METHANE; SIMPLIFICATION; MODEL;
D O I
10.1080/00102202.2019.1632300
中图分类号
O414.1 [热力学];
学科分类号
摘要
The influence of increasing pressure on nonpremixed syngas/air turbulent jet flames is numerically investigated using large eddy simulations in conjunction with a steady laminar flamelet approach. The applicability of the steady flamelet approach is assessed through an extensive parametric study of laminar counterflow flames and tangential stretching rate analysis on target flame structures at different pressures. Two sets of large eddy simulations, exploring pressure values up to atm, are carried out. The first one (series A) is characterized by a constant jet Reynolds number, while the second one (series B) is characterized by a constant jet inlet velocity. Both campaigns show narrower flame brushes and reduced radical concentrations with increasing pressure. While for series A the flame length is not sensitive to pressure, a longer flame brush is noticed for series B, being mainly caused by the increased mass flow rate. The sensitivity of the local flame behavior to pressure, such as the OH layer thickness and position, is compared to the available experimental results, showing similar trends with a satisfactory agreement.
引用
收藏
页码:1963 / 1996
页数:34
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