scholarly journals Experimental Study of Microwave Streamer Discharge Ignition of Premixed Air/Fuel Mixtures

2019 ◽  
Vol 47 (1) ◽  
pp. 57-61
Author(s):  
Mikhail Bulat ◽  
Pavel Bulat ◽  
Petr Denissenko ◽  
Igor Esakov ◽  
Lev Grachev ◽  
...  
2000 ◽  
Vol 73 (2) ◽  
pp. 293-298
Author(s):  
O. V. Achasov ◽  
T. Kageyama ◽  
S. A. Labuda ◽  
T. Taillefet ◽  
F. Fisson

2021 ◽  
Author(s):  
Mario Ditaranto ◽  
Inge Saanum ◽  
Jenny Larfeldt

Abstract Hydrogen, a carbon-free fuel, is a challenging gas to transport and store, but that can be solved by producing ammonia, a worldwide commonly distributed chemical. Ideally, ammonia should be used directly on site as a fuel, but it has many combustion shortcomings, with a very low reactivity and a high propensity to generate NOx. Alternatively, ammonia could be decomposed back to a mixture of hydrogen and nitrogen which has better combustion properties, but at the expense of an endothermal reaction. Between these two options, a trade off could be a partial decomposition where the end use fuel is a mixture of ammonia, hydrogen, and nitrogen. We present an experimental study aiming at finding optimal NH3-H2-N2 fuel blends to be used in gas turbines and provide manufacturers with guidelines for their use in retrofit and new combustion applications. The industrial burner considered in this study is a small-scale Siemens burner used in the SGT-750 gas turbine, tested in the SINTEF high pressure combustion facility. The overall behaviour of the burner in terms of stability and emissions is characterized as a function of fuel mixtures corresponding to partial and full decomposition of ammonia. It is found that when ammonia is present in the fuel, the NOx emissions although high can be limited if the primary flame zone is operated fuel rich. Increasing pressure has shown to have a strong and favourable effect on NOx formation. When ammonia is fully decomposed to 75% H2 and 25% N2, the opposite behaviour is observed. In conclusion, either low rate or full decomposition are found to be the better options.


2015 ◽  
Vol 2015.21 (0) ◽  
pp. _10901-1_-_10901-2_
Author(s):  
Masanori YAMADA ◽  
Naoya ITO ◽  
Takashi SHIMADA ◽  
Akira IIJIMA ◽  
Hideo SHOJI

2018 ◽  
Vol 25 (9) ◽  
pp. 093512 ◽  
Author(s):  
Le Cheng ◽  
Yanan Wang ◽  
Weidong Ding ◽  
Chongjian Ge ◽  
Jiaqi Yan ◽  
...  

1988 ◽  
Vol 5 (4) ◽  
pp. 177-180 ◽  
Author(s):  
Li Zhongzhen ◽  
Tang Xiaowei

2019 ◽  
Vol 47 (1) ◽  
pp. 62-68
Author(s):  
Mikhail Bulat ◽  
Pavel Bulat ◽  
Petr Denissenko ◽  
Igor Esakov ◽  
Lev Grachev ◽  
...  

2019 ◽  
Vol 141 (8) ◽  
Author(s):  
Kwonse Kim ◽  
Omid Askari

This work is an experimental and computational study to investigate the effect of capacitive discharge ignition (CDI) on plasma kernel formation and flame propagation of air–propane mixture. This paper is mainly focused on the plasma formation and flame propagation characteristics, pressure rise, propagation time, velocity field, and species concentrations. A conventional ignition system is used for comparison purpose. A constant volume combustion chamber with volume of 400 cm3 is designed for experimental study. This chamber is utilized to visualize the plasma formation as well as the flame propagation induced from two ignition sources. The experiments are performed in a wide range of operating conditions, i.e., initial pressure of 2–4 bar, temperature of 300 K, chamber wall temperature of 350 K, spark plug gaps of 1.0–1.5 mm, discharge duration of 1 ms, discharge energy of 500 mJ, and equivalence ratio of 0.5–1.0. The computational study is performed by ANSYS fluent using the partially premixed combustion (PPC) model having the same conditions as experimental study. It is shown that the average peak pressure in CDI increased by 5.79%, 4.84% and 4.36% at initial pressures of 2, 3, and 4 bar, respectively, comparing with conventional ignition. It could be determined that the impact of combustion pressure in CDI system is more significant than conventional ignition particularly in lean mixtures. Consequently, the flame propagation rate in CDI system, due to the large ionized kernel around the spark plug, can be significantly enhanced.


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