Flame structure and fuel reaction on a non-premixed shuttlecock-like conical burner
Introduction
A traditional shuttlecock that serves as a missile between players of badminton has a conical shape and gap structures, formed by feathers inserted into a cork base. Those special structures, the conical shape and gaps, induce interesting aerodynamic phenomena in the wake region when an air current passes through a shuttlecock. The effects of the conical shape and gaps on the aerodynamic characteristics of a shuttlecock have been widely investigated [[1], [2], [3], [4]]. Cooke [1] examined the aerodynamics of a shuttlecock when an air current passed through it; the air jet through the gap structure interacted with the outer flow, forming an unsteady and irregular wake pattern. The outer flow tended to curl inward, while the inner air jet tended to curl outward. Those curl structures impacted each other in the wake; the air jet dissipated downstream behind the wake. Lin et al. [2] investigated the effects of gaps on the flow properties of a conical structure; the gaps caused the introduction of an air jet that diminished the wake of recirculation type behind the bluff body. The effect of a bluff body hence decreases with a larger gap structure. Kitta et al. [3] and Hasegawa et al. [4] visualized the flow pattern of the wake region of a shuttlecock; they found that the flow passed the gaps and proceeded downstream along the axis of a shuttlecock when it had gaps; the flow through the gaps suppressed the roll-up vortex in the near region of the trailing edge of a shuttlecock. The strong voticies were maintained, however, even far downstream because of the entrainment of the fluid. A large vortex exists near the leeside of a shuttlecock with gaps, and typically sheds downstream, but a roll-up vortex is not observed when a shuttlecock lacks gaps. As the gap structures on a conical body maintain the strong vortices in the wake and allow an introduction of the co-flow into the interior of the cone, the mixing of fuel and air might be thereby enhanced when this structure is applied to the design of a combustor.
Non-premixed combustion is widely used in many practical combustion systems, such as gas turbines, boilers and furnaces. In a non-premixed flame, the reactants remain separated from the oxidant; both mixing and reaction occur only at the interface between the fuel and oxidant [5]. Flash-back phenomena hence do not occur during a non-premixed combustion process, but its combustion efficiency is less than that of premixed or partially premixed combustion because of a lack of oxidant or an insufficient mixing of fuel and oxidant. A recirculating flow is beneficial for the mixing of fuel and oxidant; a combustor is thus generally designed to form a recirculation zone [[6], [7], [8]]. According to the aerodynamic principle, a zone of low pressure induced by a bluff body or a swirl generator causes a reverse flow and a recirculation zone at the burner exit, which increases the mixing and extends the residence period of fuel and oxidant [[6], [7], [8], [9], [10], [11], [12], [13], [14], [15]]. The efficiency and stability of non-premixed combustion are thereby improved.
Other useful designs to form a recirculation flow include the diffuser [6,14,16], the conical burner [[17], [18], [19], [20], [21], [22], [23]], the double-concentric-pipe burner [24], and a new method using a circular transverse jet [25]. The cone shape of a conical burner is similar to a shuttlecock; the major difference between a conical burner and a shuttlecock is the gap structure. Domkundwar et al. [14] reported that the strength and size of the recirculation zone increase with an increasing angle of divergence; the swirl required to form the recirculation can be significantly decreased at a large angle of divergence. The pressure loss in the flow field hence was kept small. The strength and size of the reversal zone, however, decrease with a secondary mass flow passing through the walls of the diffuser and with combustion. Mansour designed a concentric-flow conical-nozzle burner (CFCN) [17] and concentric flow slot burner (CFSB) [18] in which the non-premixed fuel achieved a partially premixed condition through the spatial structure of the burner. For a CFCN burner, the flame stability was greatly affected by the cone angle because an increasing cone angle caused a large entrainment of air, breaking the core of stabilization and then impeding the flame stability [19]. Li et al. [20] experimentally and numerically studied a partially premixed flame in a conical burner; they found that the flame is stabilized inside the cone above the nozzle exit because of the propagation of the premixed flame front. The flow reverses near the wall of the cone, and depends on the cone angle. Mansour et al. [21] employed a fused-silica conical nozzle to undertake the measurement with particle-image velocimetry (PIV); they reported that a recirculation zone was produced at the near region inside the cone, heating the entrained air from the surroundings. The increasing reverse velocity increased the rate of spread, but decreased the intensity of turbulence inside the cone, and decreased the thickness of the boundary layer. When an air co-flow was applied to the CFCN burner [22], the added co-flow caused the formation of two vortices at the cone exit, resulting in the stabilization of the flame anchored to the nozzle tip; the reaction shifted toward a decreased turbulent intensity at the side of the cone. The stability of a flame is improved on adding a co-flow of air. The modified CFCN swirl burner improves flam stability and extends the blowout limits over a wide range of partial premixing levels [23]. As a conical burner with a simple flow geometry makes feasible the formation of a reversal flow structure, it is suitable to serve as a reference for the design of a burner for non-premixed combustion.
Accordingly, the aim of this work was to apply slot structures to an ordinary conical burner. We designed a shuttlecock-like conical burner that had slot structures on a conical body; those slots introduced a co-flow of air into the cone of the designed burner. The mixing condition of the fuel and the air co-flow thereby transformed naturally from a non-premixed to partically premixed. The simple geometry of the designed burner is adaptable for industrial applications to improve the efficiency of non-premixed combustion. The flame structure, flow structure, chemiluminescence of OH radical and distribution of flame temperature were experimentally examined and are discussed in what follows.
Section snippets
Burner design
The design of a shuttlecock-like conical burner is inspired from the geometry of a shuttlecock; the side of a traditional shuttlecock is composed of feathers and is similar to a conical shape with a slot structure. This slot structure allows a co-flow of air to be naturally introduced to pass through the cone of the shuttlecock. For non-premixed combustion, the introduced air co-flow provides additional oxidant for the fuel through a simple geometry. Fig. 1 shows a schematic of the design of a
Nomenclature
- D
inner diameter of the conical body, mm
- d
inner diameter of the fuel tube, mm
- ua
flow velocity of the air co-flow, m/s
- uf
flow velocity at the exit of the fuel tube, m/s
- Qf
volume flow rate of fuel, L/min
- Pideal
ideal power of fuel
Flame patterns
Fig. 4 shows the distribution of flame patterns of a shuttlecock-like conical burner and of an ordinary conical burner observed with varied velocity of the central fuel jet and the air co-flow. The velocity of the central fuel jet was varied from 0.1 to 1.5 m/s; the velocity of the air co-flow was varied from 0 to 6.3 m/s. Fig. 5 shows typical flame photographs of a shuttlecock-like conical burner and of an ordinary conical burner. Whether a shuttlecock-like conical burner or an ordinary
Conclusions
In this work, a novel design inspired from the structure of a shuttlecock was applied to a non-premixed burner. We designed the slot structure to introduce naturally a co-flow of air into a non-premixed burner, which is named a shuttlecock-like conical burner. The mixing condition of the fuel in the cone therefore transformed from non-premixed to partically premixed. The flame patterns, structure of the isothermal flow field, reaction characteristics and flame temperature of a shuttlecock-like
Credit author statement
Chih-Pin Chiu: Writing-original draft & Project administration.
Yueh Lu: Conceptulization & Data curation.
Yu-Tai Sheng: Data curation.
Szu-I Yeh: Formal analysis & Writing-review and editing.
Jing-Tang Yang: Supervision & Writing-review and editing.
Declaration of Competing Interest
The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.
Acknowledgements
This research did not receive any specific grant from funding agencies in the public, commercial, or not-for-profit sectors.
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