Simulation of liquid fuel combustion start-up dynamical behavior

被引:3
|
作者
Hussain, Mukkarum [1 ]
Ahmed, Iftikhar [2 ]
Khan, Ilyas [3 ]
My, Chu Anh [4 ]
Baig, Mirza Mehmood [5 ]
Khan, Afrasyab [6 ]
Makhanov, Stanislav S. [7 ]
机构
[1] Inst Space Technol Pakistan, Islamabad, Pakistan
[2] Sukkur IBA Univ, Sukkur, Pakistan
[3] Majmaah Univ, Coll Sci Al Zulfi, Dept Math, POB 66, Majmaah 11952, Saudi Arabia
[4] Le Quy Don Tech Univ LQDTU, Inst Simulat Technol, 236 Hoang Quoc Viet, Hanoi, Vietnam
[5] NED Univ Engn & Technol, Karachi, Pakistan
[6] South Ural State Univ, Dept Hydraul & Hydraul & Pneumat Syst, Inst Engn & Technol, Lenin Prospect 76, Chelyabinsk 454080, Russia
[7] Thammasat Univ, Sirindhorn Int Inst Technol, Sch Informat & Comp Technol, Tiwanont Rd, A Muang 12000, Pathum Thani, Thailand
关键词
CFD; Supercritical combustion; Ignition transients; Real gas; Kerosene/oxygen combustion; DESIGN; ENERGY; PLANT;
D O I
10.1016/j.csite.2021.101025
中图分类号
O414.1 [热力学];
学科分类号
摘要
A successful ignition is the consequence of corresponding conditions of fuel mass flow rates, mixture ratio, as well as initiation energy in time and space. If ignition does not take place accurately, serious damages can take place within or outside the engine. The dynamical behavior of the combustion chamber was investigated during ignition. Single shear coaxial injector combustion chamber test case is used in the present study. At the time of propellant injection, mostly the pressure and temperature remain subcritical. When injected these increases promptly and convert into supercritical conditions. The thermodynamic state usually changes from subcritical to supercritical during ignition. Navier Stokes equations along with Soave Redlich Kwong equation model has been applied during steady-state, while transient simulations with ideal gas assumptions are performed to analyze the dynamical behavior of the combustor. All the simulations were performed in the present study using the ANSYS Fluent 16.2 code. The computational findings have strong analytical consistency with the experimental data. Due to inappropriate modeling of the equation of state and limited information about initial and boundary conditions for ignition transient results have some differences with experimental data. The difference between the observed chamber pressure during the experiment and numerical computation using 0.4 RFL value is only 2 bar (approximately 7% difference).
引用
收藏
页数:14
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