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Swirling flame

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EXPERIMENTAL STUDY OF THE FUEL COMBUSTION AND SWIRLING FLAME DYNAMICS UNDER THE PREMIXED AND NON-PREMIXED COMBUSTION CONDITIONS

The general objective of the research is development and optimization of the swirling combustion by providing the control of the swirling flame flow formation and recirculation of products inside the swirling flame flow and so providing control of the mixing rates of the axial fuel flow with the swirling airflow, formation of the temperature field downstream of the swirling flame flow, as well as control of the formation of polluting emissions. The electric field effect on the swirling flame dynamics is used to provide the control of the swirling flame dynamics and the formation of the polluting emissions. It is established that the electric force largely (F=qE) affects the axial velocity component of the swirling flame flow with a direct influence on the recirculation and swirling flame flow formation by varying the visible flame shape and length, depending on the field strength and configuration (Fig.1).

Fig.1. The electric field effect on the swirling flame shape and length by varying the bias voltage and polarity of the electrode. 1. U=0; 2. U=+0.3 kV; 3. U=+1.8 kV; 4. U=-1.8 kV.

The experimental set-up is presented in Fig.2. The experimental apparatus consists of a gas burner, sectioned water-cooled channel and central wire electrode. The fuel is injected axially into the burner through a single-hole nozzle of 20mm inner diameter, while the airflow - tangentially, through the annular duct using the air swirler with 8 peepholes of 3mm inner diameter. The swirled airflow is supplied through the radially displaced annular duct up to the burner outlet and then gradually mixes with the coaxial fuel flow, providing the axial symmetry of the velocity field. The rate of air injection into the burner can be varied ranging within 10- 20 l/min, while the propane rate - from 0.4 to 1 l/min, providing the variation of axial flow rate in a range of 0,6-1,26 m/s and the variation of the tangential flow rate in a range of 3,5-7 m/s at nearly constant and relatively high swirl number of the swirling flow at the burner outlet- S≈5,6. The equivalence rate of the air supply in these experiments can be varied from α=0.7 to α=1.44.

The electric field to the swirling flame flow is applied in a space between the axially inserted electrode, surface of the burner and water-cooled channel walls. The bias voltage and polarity of the axially arranged central electrode in the recent investigations are varied in the range from –3.0 kV up to +3.0 kV, while the ion current in the flame in this study is limited to 200 mkA.

Fig.2. Digital image of the experimental set-up (a), schematic of the experimental facility (b): 1- axially arranged central electrode, 2- water-cooled sections of the channel, 3- peepholes for the diagnostic tools, 4- tangential air entry, 5-axial propane entry, 6-swirling burner, 7- recirculation zone; and schematic of the flow field formation (c).


The investigations of the electric field effect on the premixed propane/air flame flow include:

  • The experimental study of the electric field effect on the processes of heat and mass transfer;
  • The experimental study of the electric field effect on the local flame composition;
  • The experimental study of the electric field effect on the local temperature and rate of fuel combustion;
  • The experimental study of the electric field effect on the levels of greenhouse emissions (CO2, NOx);
  • The experimental study of the electric field effect on the soot formation, carbon capture and sequestration from the flame flow;
  • The experimental study of the electric field effect on pre-combustion fuel decarbonisation.
Main publications:

  1. I. Barmina, A. Desnickis, A. Meijere, M. Zake, Active Electric Control of Emissions From the Swirling Combustion, In: Advanced Combustion and Aerothermal Technologies: The Biomass and Alternative Fuels, Ed. Nick Syred, WB/Nato Publishing Unit, P.O.Box 17,3300 AA Dordrecht, The Netherlands, Springer, 2007, pp. 405-412.
  2. M. Zaķe, I. Barmina, D. Turlajs, M. Lubāne, A. Krūmiņa. Swirling Flame. Part 2. Electric Field Effect on the Soot Formation and Greenhouse Emissions. Magnetohydrodynamics, 2004, Vol. 40, No 2, p.183-202.
  3. M. Zaķe, I. Barmina, M. Lubāne. Swirling flame. Part 1. Experimental Study of the Effect of Stage Combustion on Soot Formation and Carbon Sequestration from the Nonpremixed Swirling Flame. Magnetohydrodynamics, 2004, Vol. 40, No 2, p.161-181.

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