Low-temperature zone in a hydrocarbon-flame front VII. Structure of the flame front in hexane with aerosol fuel injection

1982 ◽  
Vol 18 (6) ◽  
pp. 637-639
Author(s):  
V. K. Manzhos ◽  
B. Ya. Kolesnikov ◽  
A. K. Murzagaliev ◽  
G. I. Ksandopulo
1976 ◽  
Vol 11 (1) ◽  
pp. 114-117
Author(s):  
G. I. Ksandopulo ◽  
B. Ya. Kolesnikov ◽  
D. S. Odnorog

1976 ◽  
Vol 11 (3) ◽  
pp. 350-354
Author(s):  
G. I. Ksandopulo ◽  
B. Ya. Kolesnikov ◽  
D. S. Odnorog ◽  
V. V. Dubinin

1978 ◽  
Vol 13 (4) ◽  
pp. 547-549
Author(s):  
G. I. Ksandopulo ◽  
B. Ya. Kolesnikov ◽  
V. V. Dubinin ◽  
D. S. Odnorog

1975 ◽  
Vol 11 (6) ◽  
pp. 714-719
Author(s):  
G. I. Ksandopulo ◽  
A. A. Sagindykov ◽  
S. E. Kudaibergenov ◽  
Z. A. Mansurov

2021 ◽  
pp. 83-90
Author(s):  
Alyona Shilova ◽  
◽  
Nikolay Bachev ◽  
Roman Bulbovich ◽  
◽  
...  

For a stable position of the flame front in the combustion chambers of gas turbine power plants, the fresh gas-air mixture must be heated to the ignition temperature during the entire operation process. With air excess coefficients in the interval between the upper and lower concentration limits, reverse currents from the zone of developed combustion successfully cope with this task. When organizing low-temperature combustion near the lean limit, the contribution of reverse currents to heating the fresh gas-air mixture turns out to be insufficient and additional external heating of the components in special heaters with exhaust gases from the turbine is required. The temperature characteristics of the fresh gas-air mixture at the inlet to the chamber and in the zone of return currents, as well as combustion products in the developed flame zone, were obtained from the solution of the energy balance equations. The modes of low-temperature lean combustion with excess air coefficients exceeding the lower concentration limit α = 2 are considered. The calculations were carried out for two values of the ejection coefficient in the zone of reverse currents K = 0.14 and K = 0.30. A K value of 0.14 was obtained using empirical relationships. The value K = 0.30 was obtained from the condition that during stoichiometric combustion, the gas-air mixture is heated completely by reverse currents. It is shown that with an increase in the excess air ratio to ensure a stable position of the flame front, the role of external heating of components increases.


Author(s):  
Hongsheng Guo ◽  
W. Stuart Neill ◽  
Wally Chippior ◽  
Hailin Li ◽  
Joshua D. Taylor

Homogeneous charge compression ignition (HCCI) is an advanced low-temperature combustion technology being considered for internal combustion engines due to its potential for high fuel conversion efficiency and extremely low emissions of particulate matter and oxides of nitrogen (NOx). In its simplest form, HCCI combustion involves the auto-ignition of a homogeneous mixture of fuel, air, and diluents at low to moderate temperatures and high pressure. Previous research has indicated that fuel chemistry has a strong impact on HCCI combustion. This paper reports the preliminary results of an experimental and modeling study of HCCI combustion using n-heptane, a volatile hydrocarbon with well known fuel chemistry. A Co-operative Fuel Research (CFR) engine was modified by the addition of a port fuel injection system to produce a homogeneous fuel-air mixture in the intake manifold, which contributed to a stable and repeatable HCCI combustion process. Detailed experiments were performed to explore the effects of critical engine parameters such as intake temperature, compression ratio, air/fuel ratio, engine speed, turbocharging, and intake mixture throttling on HCCI combustion. The influence of these parameters on the phasing of the low-temperature reaction, main combustion stage, and negative temperature coefficient delay period are presented and discussed. A single-zone numerical simulation with detailed fuel chemistry was developed and validated. The simulations show good agreement with the experimental data and capture important combustion phase trends as engine parameters are varied.


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