Flashback Avoidance in Swirling Flow Burners
Impedimento de reflujo de llama en quemadores de flujo giratorio
Vigueras-Zúñiga Marco Osvaldo
Universidad Veracruzana, México, Facultad de Ingeniería
Syred Nicholas**
Cardiff University School of Engineering, United Kingdom
Valera-Medina Agustín***
Cardiff University School of Engineering, United Kingdom
De la Rosa-Urbalejo Daniel****
Cardiff University School of Engineering, United Kingdom
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Edgar" "autores" => array:1 [ 0 => array:2 [ "nombre" => "Serna-M." "apellidos" => "Edgar" ] ] ] 1 => array:2 [ "autoresLista" => "Morales-V. David" "autores" => array:1 [ 0 => array:2 [ "nombre" => "Morales-V." 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del sistema robótico</p>" ] ] ] "autores" => array:2 [ 0 => array:2 [ "autoresLista" => "Bugarin-Carlos Eusebio" "autores" => array:1 [ 0 => array:2 [ "nombre" => "Bugarin-Carlos" "apellidos" => "Eusebio" ] ] ] 1 => array:2 [ "autoresLista" => "Aguilar-Bustos Ana Yaveni" "autores" => array:1 [ 0 => array:2 [ "nombre" => "Aguilar-Bustos" "apellidos" => "Ana Yaveni" ] ] ] ] ] "idiomaDefecto" => "es" "EPUB" => "https://multimedia.elsevier.es/PublicationsMultimediaV1/item/epub/S1405774314706572?idApp=UINPBA00004N" "url" => "/14057743/0000001500000004/v1_201412280017/S1405774314706572/v1_201412280017/es/main.assets" ] "en" => array:21 [ "idiomaDefecto" => true "titulo" => "Flashback Avoidance in Swirling Flow Burners" "tieneTextoCompleto" => true "paginas" => array:1 [ 0 => array:2 [ "paginaInicial" => "603" "paginaFinal" => "614" ] ] "autores" => array:4 [ 0 => array:3 [ "autoresLista" => "Vigueras-Zúñiga Marco Osvaldo" "autores" => array:1 [ 0 => array:4 [ "nombre" => "Vigueras-Zúñiga" "apellidos" => "Marco Osvaldo" "email" => array:1 [ 0 => "mvigueras@uv.mx" ] "referencia" => array:1 [ 0 => array:2 [ "etiqueta" => "<span class="elsevierStyleSup">*</span>" "identificador" => "fnr0005" ] ] ] ] "afiliaciones" => array:1 [ 0 => array:2 [ "entidad" => "Universidad Veracruzana, México, Facultad de Ingeniería" "identificador" => "aff0005" ] ] ] 1 => array:3 [ "autoresLista" => "Syred Nicholas" "autores" => array:1 [ 0 => array:4 [ "nombre" => "Syred" "apellidos" => "Nicholas" "email" => array:1 [ 0 => "nsyred@cf.ac.uk" ] "referencia" => array:1 [ 0 => array:2 [ "etiqueta" => "<span class="elsevierStyleSup">**</span>" "identificador" => "fnr0010" ] ] ] ] "afiliaciones" => array:1 [ 0 => array:2 [ "entidad" => "Cardiff University School of Engineering, United Kingdom" "identificador" => "aff0010" ] ] ] 2 => array:3 [ "autoresLista" => "Valera-Medina Agustín" "autores" => array:1 [ 0 => array:4 [ "nombre" => "Valera-Medina" "apellidos" => "Agustín" "email" => array:1 [ 0 => "Valeramedinaa1@cardiff.ac.uk" ] "referencia" => array:1 [ 0 => array:2 [ "etiqueta" => "<span class="elsevierStyleSup">***</span>" "identificador" => "fnr0015" ] ] ] ] "afiliaciones" => array:1 [ 0 => array:2 [ "entidad" => "Cardiff University School of Engineering, United Kingdom" "identificador" => "aff0015" ] ] ] 3 => array:3 [ "autoresLista" => "De la Rosa-Urbalejo Daniel" "autores" => array:1 [ 0 => array:4 [ "nombre" => "De la Rosa-Urbalejo" "apellidos" => "Daniel" "email" => array:1 [ 0 => "delarosaurbalejod@cardiff.ac.uk" ] "referencia" => array:1 [ 0 => array:2 [ "etiqueta" => "<span class="elsevierStyleSup">****</span>" "identificador" => "fnr0020" ] ] ] ] "afiliaciones" => array:1 [ 0 => array:2 [ "entidad" => "Cardiff University School of Engineering, United Kingdom" "identificador" => "aff0020" ] ] ] ] "titulosAlternativos" => array:1 [ "es" => array:1 [ "titulo" => "Impedimento de reflujo de llama en quemadores de flujo giratorio" ] ] "resumenGrafico" => array:2 [ "original" => 0 "multimedia" => array:7 [ "identificador" => "fig0025" "etiqueta" => "Figure 5" "tipo" => "MULTIMEDIAFIGURA" "mostrarFloat" => true "mostrarDisplay" => false "figura" => array:1 [ 0 => array:4 [ "imagen" => "gr5.jpeg" "Alto" => 1874 "Ancho" => 935 "Tamanyo" => 169011 ] ] "descripcion" => array:1 [ "en" => "<p id="spar0025" class="elsevierStyleSimplePara elsevierViewall">Flashback results with fuel injector. Confinement as in <a class="elsevierStyleCrossRef" href="#fig0015">Figure 3a</a>, a) no confinement-nozzle, b) confinement-nozzle, c) confinement-without nozzle</p>" ] ] ] "textoCompleto" => "<span class="elsevierStyleSections"><span id="sec0005" class="elsevierStyleSection elsevierViewall"><span class="elsevierStyleSectionTitle" id="sect0025"><a name="p604"></a>Introduction</span><p id="par0005" class="elsevierStylePara elsevierViewall">The crucial feature of swirl burners is the formation of a central recirculation zone (CRZ) which extends blow off limits by recycling heat and active chemical species to the root of the flame in the burner exit. However, unless its size and shape are properly controlled, problems can arise. The CRZ can, for instance, readily extend back into the burner, even surrounding the fuel injector and facilitating early flashback (<a class="elsevierStyleCrossRef" href="#bib0080">Subramanya and Choudhuri, 2007</a>; <a class="elsevierStyleCrossRef" href="#bib0095">Thornton <span class="elsevierStyleItalic">et al</span>., 2007</a>; <a class="elsevierStyleCrossRef" href="#bib0055">Lieuwen <span class="elsevierStyleItalic">et al</span>., 2008</a>).</p><p id="par0010" class="elsevierStylePara elsevierViewall">Flashback can occur when the gas velocity becomes lower than the flame speed, allowing the flame to propagate upstream, potentially causing damaging effects. The phenomenon can be caused by (i) boundary layer flame propagation, (ii) turbulent flame propagation in the core flow, (iii) combustion instabilities and (iv) upstream flame propagation of coherent vortical structures (<a class="elsevierStyleCrossRef" href="#bib0055">Lieuwen <span class="elsevierStyleItalic">et al</span>., 2008</a>, <a class="elsevierStyleCrossRef" href="#bib0050">Lefebvre, 1999</a>). For the latter, flow speed not necessarily can be lower than the flame velocity everywhere, though flashback is still observed. This refers to a highly complex phenomenon. This paper focuses on the two main causes of flashback:<ul class="elsevierStyleList" id="lis0005"><li class="elsevierStyleListItem" id="lsti0005"><span class="elsevierStyleLabel">•</span><p id="par0015" class="elsevierStylePara elsevierViewall">Flashback occurring through the low-velocity flow in the boundary layer along the walls of the burner close to the exit and governed by the critical boundary velocity gradient,</p></li><li class="elsevierStyleListItem" id="lsti0010"><span class="elsevierStyleLabel">•</span><p id="par0020" class="elsevierStylePara elsevierViewall">Flashback occurring due to coherent structures.</p></li></ul></p><p id="par0025" class="elsevierStylePara elsevierViewall">The mechanisms may involve the use of homogeneous and/or heterogeneous reactions. <a class="elsevierStyleCrossRef" href="#bib0055">Lieuwen <span class="elsevierStyleItalic">et al</span>. (2008)</a> reviewed flashback in the context of syngas fired combustors and noted that minimization of flashback requires that the flow field should not have strong local velocity deficits and the axial flow velocity must be substantially above the local turbulent flame speed, S<span class="elsevierStyleInf">t</span>. High turbulence levels, one of the very useful features of swirling flow because of their mixing potential, detrimentally affect flashback limits due to their effects on S<span class="elsevierStyleInf">t</span>, especially for hydrogen enriched syngases.</p><p id="par0030" class="elsevierStylePara elsevierViewall">Lean combustion tends to reduce flame velocity, but other factors associated with engine cycles, such as high temperatures, pressure, turbulence levels and preignition reactions in the gases due to appreciable residence times at high temperature cause increased flame speeds, encouraging flashback.</p><p id="par0035" class="elsevierStylePara elsevierViewall">With swirl burners, the swirl number, S (<a class="elsevierStyleCrossRef" href="#bib0090">Syred and Beer, 1974</a>) defined by the normalized ratio of axial flux of axial momentum and axial flux of angular momentum, is crucial as higher values (S<span class="elsevierStyleHsp" style=""></span>><span class="elsevierStyleHsp" style=""></span>1.2) tend to exacerbate the formation of excessively large CRZs which extend back into the burner. Moreover, higher swirl numbers tend to increase turbulence and consequently, the turbulent flame speed (<a class="elsevierStyleCrossRef" href="#bib0100">Valera <span class="elsevierStyleItalic">et al</span>., 2011</a>; <a class="elsevierStyleCrossRef" href="#bib0025">Huang and Yang, 2004</a>; <a class="elsevierStyleCrossRef" href="#bib0030">2005</a>) and propensity to flashback in low velocity regions. Combustion located downstream of the tangential inlets alters significantly the axial flux of axial momentum <a class="elsevierStyleCrossRef" href="#bib0090">Syred and Beer, 1974</a>) hence local swirl number is also affected. This effect depends strongly on the equivalence ratio, rate of heat release, location of flame front and mode of fuel injection. Such changes in swirl number due to combustion can subsequently alter the resistance to flashback. Off-design condition operations that impact on the swirl number and flame stability can produce oscillations associated with unsteady flashback (<a class="elsevierStyleCrossRef" href="#bib0015">Dhanuka <span class="elsevierStyleItalic">et al</span>., 2009</a>).</p><p id="par0040" class="elsevierStylePara elsevierViewall">These factors can explain the anomalous behavior of many swirl burners under various conditions, including flashback. Premixed combustion can especially change a highly swirling flow from a situation with a large stable CRZ to one where the CRZ is eliminated, the effect being a maximum at an equivalence ratio, φ, ~ 1 where heat release is at its highest point. Varying the equivalence ratio can substantially affect the occurrence, strength and size of any CRZ formed. Therefore, the evidence suggests that flashback is very dependent on several parameters, making very difficult to generalize any pattern that directly influence this phenomenon.</p><p id="par0045" class="elsevierStylePara elsevierViewall">Flame flashback from the combustion chamber into the mixing zone can limit the reliability of swirl stabilized lean premixed combustion in gas turbines. A phenomenon labelled combustion induced vortex breakdown (CIVB) has been identified as an initial flashback mechanism in some swirl burners (<a class="elsevierStyleCrossRef" href="#bib0035">Kröner <span class="elsevierStyleItalic">et al</span>., 2003</a>; <a class="elsevierStyleCrossRef" href="#bib0040">Kiesewetter <span class="elsevierStyleItalic">et al</span>., 2007</a>; <a class="elsevierStyleCrossRef" href="#bib0045">Kröner <span class="elsevierStyleItalic">et al</span>., 2007</a>). It occurs with values of S between 0.5 and 0.9 when vortex breakdown is about to, or has just occurred (<a class="elsevierStyleCrossRef" href="#bib0020">Gupta <span class="elsevierStyleItalic">et al</span>., 1984</a>), without the presence of a central fuel injector. The phenomenon occurs as a sudden transition driven by the interaction of chemical reactions and vortex dynamics. First, a CRZ forms downstream of the burner exit that holds the flame. Then, the chemical reactions in the vortex core lead to the propagation of the CRZ into the burner. A closed recirculation bubble forms and the drop of density leads to the extinction of the downstream CRZ (<a class="elsevierStyleCrossRef" href="#bib0045">Kröner <span class="elsevierStyleItalic">et al</span>., 2007</a>). <a class="elsevierStyleCrossRef" href="#bib0055">Lieuwen <span class="elsevierStyleItalic">et al</span>. (2008)</a> also indicated that the CIVB phenomenon is primarily determined by density gradients and other combustion aerodynamic phenomena. <a class="elsevierStyleCrossRef" href="#bib0090">Syred and Beer (1974)</a><a class="elsevierStyleCrossRef" href="#bib0020">and Gupta <span class="elsevierStyleItalic">et al</span>. (1984)</a> showed that these effects can be caused by swirl number reduction <a name="p605"></a>effects as combustion effects increase the axial flux of axial momentum, but generally not that of angular momentum. For instance with the burner used in this study and for equivalence ratios ~1 the CRZ can completely disappear, whilst an equivalence ratio reduction to about ~0.75 leads to vortex breakdown and the formation of a CRZ in the burner exit region (<a class="elsevierStyleCrossRef" href="#bib0100">Valera <span class="elsevierStyleItalic">et al</span>., 2011</a>).</p><p id="par0050" class="elsevierStylePara elsevierViewall">Flashback depends on parameters such as heating values, reaction rate, etc., making more difficult the use of potential alternative fuels (<a class="elsevierStyleCrossRef" href="#bib0010">Chiesa <span class="elsevierStyleItalic">et al</span>., 2005</a>; <a class="elsevierStyleCrossRef" href="#bib0005">Bagdanavicius <span class="elsevierStyleItalic">et al</span>., 2009</a>). Some authors (<a class="elsevierStyleCrossRef" href="#bib0025">Huang and Yang, 2004</a>; <a class="elsevierStyleCrossRef" href="#bib0015">Dhanuka <span class="elsevierStyleItalic">et al</span>., 2009</a>) have experimented with CO2 and N2 diluents to control flame propagation for these fuels.</p><p id="par0055" class="elsevierStylePara elsevierViewall">Another important parameter in flashback propagation is the geometry of the system (<a class="elsevierStyleCrossRef" href="#bib0070">Plee and Mellor, 1978</a>). Small changes in the details of the geometry of the premixing tube such as steps, diverging sections, surface discontinuities, or method of fuel injection such as counterflow injection, diffusive penetration, etc., can cause significant changes in flashback behaviour.</p><p id="par0060" class="elsevierStylePara elsevierViewall">At values of S<span class="elsevierStyleHsp" style=""></span>><span class="elsevierStyleHsp" style=""></span>1 the flame and at least part of the CRZ will extend naturally and attach to the burner baseplate as a long columnar tulip shaped structure <a class="elsevierStyleCrossRef" href="#bib0090">Syred and Beer, 1974</a>; <a class="elsevierStyleCrossRef" href="#bib0060">Lucca and O’Doherty, 2001</a>), the bulbous end of the tulip being located in the burner exit. When a fuel injector is fitted, the columnar CRZ (and flame burning on its boundary) may surround the injector, unless the injector is of large diameter (<a class="elsevierStyleCrossRef" href="#bib0040">Kiesewetter <span class="elsevierStyleItalic">et al</span>., 2007</a>) or S is reduced. The CRZ size and position can become variable in the region of the injector as equivalence ratio is reduced and the aerodynamics tend more to that of the isothermal state, remembering that combustion can reduce S to such an extent that the CRZ disappears <a class="elsevierStyleCrossRef" href="#bib0090">Syred and Beer, 1974</a>); <a class="elsevierStyleCrossRef" href="#bib0100">Valera <span class="elsevierStyleItalic">et al</span>., 2011</a>) due to the effects of varying density ratios.</p><p id="par0065" class="elsevierStylePara elsevierViewall">The effect of Reynolds number (Re, normally based on isothermal conditions and the average throat axial velocity) on vortex breakdown and the formation of CRZs must also be considered. <a class="elsevierStyleCrossRef" href="#bib0075">Sarpkaya (1971)</a> showed the effect of Re on the location of vortex breakdown, the precursor to the formation of CRZs. Essentially it was only for S<span class="elsevierStyleHsp" style=""></span>><span class="elsevierStyleHsp" style=""></span>1 that the CRZ would firmly locate to the baseplate of the swirl generator; otherwise it was freely located. The effect was also complicated by the transition between different types of vortex breakdown (<a class="elsevierStyleCrossRef" href="#bib0060">Lucca and O’Doherty, 2001</a>). <a class="elsevierStyleCrossRef" href="#bib0060">Lucca-Negro and O’Doherty (2001)</a> showed that although other workers identified other forms and occurrences of vortex breakdown, the dependence of its location upon Reynolds numbers was still very similar to Sarpkaya’s. Of relevance to swirl combustion is that for 0.6<span class="elsevierStyleHsp" style=""></span><<span class="elsevierStyleHsp" style=""></span>S<span class="elsevierStyleHsp" style=""></span><<span class="elsevierStyleHsp" style=""></span>1.1 where the vortex breakdown, hence any CRZ, was not attached to the baseplate of the swirl generator for any Reynolds number.</p><p id="par0070" class="elsevierStylePara elsevierViewall">From the above the main effects on swirl combustion and especially flashback are:<ul class="elsevierStyleList" id="lis0010"><li class="elsevierStyleListItem" id="lsti0015"><span class="elsevierStyleLabel">•</span><p id="par0075" class="elsevierStylePara elsevierViewall">CRZs generated by values of S between 0.5 and 1.0 are desirable as associated flames are located away from vulnerable surfaces, whilst pressure drop is minimized. However the CRZs are likely to be easily perturbed by coupling with acoustic or combustion induced disturbances due to their ‘free’ axial location.</p></li><li class="elsevierStyleListItem" id="lsti0020"><span class="elsevierStyleLabel">•</span><p id="par0080" class="elsevierStylePara elsevierViewall">Devices operating at higher Reynolds numbers may behave differently close to flashback as the onset of vortex breakdown may well subtly alter. Although chemical reactions rate dependency on pressure is important with CIVB propagation (and especially any hydrogen containing fuel), the strength of the initial vortex breakdown and CRZ is highly related to Re (<a class="elsevierStyleCrossRef" href="#bib0075">Sarpkaya, 1971</a>) especially with natural gas where flashback can occur at low exit velocities, as discussed later. Reynolds number effects on vortex breakdown, CRZ formation, flame stability and hence flashback especially for smaller burners or those operating at high turndown, are important as the isothermal Reynolds number readily reduces with combustion by up to a factor ~8 (at 1000K) to 16 (at 1500K) (<a class="elsevierStyleCrossRef" href="#bib0075">Sarpkaya, 1971</a>).</p></li><li class="elsevierStyleListItem" id="lsti0025"><span class="elsevierStyleLabel">•</span><p id="par0085" class="elsevierStylePara elsevierViewall">Central fuel injectors, widely employed especially with liquid fuels, will interact and interfere with the above processes, although it is recognized that CRZs can easily surround smaller injectors and promote early flashback, especially at lean values of φ and values of S<span class="elsevierStyleHsp" style=""></span>><span class="elsevierStyleHsp" style=""></span>1 (<a class="elsevierStyleCrossRef" href="#bib0060">Lucca and O’Doherty, 2001</a>; <a class="elsevierStyleCrossRef" href="#bib0085">Syred, 2006</a>).</p></li></ul></p><p id="par0090" class="elsevierStylePara elsevierViewall">This paper is thus aimed at analyzing the mechanisms of flashback taking place in a natural gas fired swirl burner with and without a central fuel injector so as to understand the physical processes and how they can be alleviated using different passive mechanisms.</p></span><span id="sec0010" class="elsevierStyleSection elsevierViewall"><span class="elsevierStyleSectionTitle" id="sect0030">Experimental setup</span><p id="par0095" class="elsevierStylePara elsevierViewall">Experiments were performed in a 100kW steel scaled version of a 2MW commercial swirl burner under combustion conditions, <a class="elsevierStyleCrossRef" href="#fig0005">Figure 1</a>.</p><elsevierMultimedia ident="fig0005"></elsevierMultimedia><p id="par0100" class="elsevierStylePara elsevierViewall">Two tangential inlets were used together with inserts blocking 25% of their transversal area, giving a swirl number of 1.08 (0.86 with the nozzle, <a class="elsevierStyleCrossRef" href="#fig0010">Figure 2</a> fitted) (<a class="elsevierStyleCrossRef" href="#bib0105">Valera <span class="elsevierStyleItalic">et al</span>., 2009</a>; <a class="elsevierStyleCrossRef" href="#bib0110">Valera, 2009</a>).</p><elsevierMultimedia ident="fig0010"></elsevierMultimedia><p id="par0105" class="elsevierStylePara elsevierViewall"><a name="p606"></a>Flow straighteners consisting of a honeycomb matrix were fitted upstream of each inlet. The system was fed by a centrifugal fan providing air flow via flexible hoses and two banks of rotameters for the control of the air flow and injection of the natural gas respectively. The inclusion of two stainless steel mirrors at the exit and bottom of the rig (and rotated by 45°) allowed the visualization of flashback. A quartz plate replaced the burner baseplate to enable visualization of flashback that occurred inside of the swirl chamber when using high speed photography. The plate was mounted via an extension to the base of the burner to remove the quartz plate from the flashback region. This was observed not to affect the flashback process.</p><p id="par0110" class="elsevierStylePara elsevierViewall">Two different modes of natural gas injection were possible, a diffusive mode with fuel injected along the central axis from the burner baseplate and a premixed mode with entry in one or both tangential inlets, located before the inserts used to regulate the Swirl number. Premixed gas injectors, extending across the inlet ducts, were located just before the inlets. Turbulence is generated by the ducts which cross the inlet area and increase the mixing previous to the entrance of the mixture into the swirl chamber. Overall equivalence ratio, φ, with 5% uncertainty due to the variations in the air and gas flows is reported, as well as the fuel proportion injected diffusively by the fuel injectors mounted along the axis followed by that injected as premixed in the tangential inlets. The following nomenclature was used to describe the relative quantities of fuel injected diffusively either through the center of the baseplate or via the fuel injector and premixed through injectors upstream of the tangential inlets: i.e., {25-40} means that 25_l/min was injected diffusively, 40_l/min premixed. To modify φ, the air supply was kept constant during the test whilst varying the gas supply until flashback was observed. The experimental conditions are at 288K and sea level atmospheric pressure.</p><p id="par0115" class="elsevierStylePara elsevierViewall">A Photron Fastcam high speed camera model APX RS of 250,000frames/s maximum speed was used for flashback visualization with a 105mm, 1:2.8 Nikon Lens. The camera was setup at only 500frames/s to avoid resolution problems and increase the visual field, since the frequency of the expected events and of the large coherent structures known to be present in the system has been observed to lie in the range of 100-200Hz (<a class="elsevierStyleCrossRef" href="#bib0110">Valera, 2009</a>; <a class="elsevierStyleCrossRef" href="#bib0065">Nauert <span class="elsevierStyleItalic">et al</span>., 2007</a>). The resulting images were analyzed using the PFV version 2.4.1.1 software. It is recognized that the use of these technique gives insight of the mechanism of propagation of the flame, but not a full picture of the intensity of the combustion process. The appearance of soot particles can degrade the unfiltered images, whilst the view of reaction occurring in the boundary layers near the walls is attenuated due to the presence of dark walls in the field of view.</p><p id="par0120" class="elsevierStylePara elsevierViewall">Equivalence ratios were investigated from lean conditions at 0.600 to rich values at ~2.000. A wide variation in the airflow and gas flow rates was also made to visualize the progressive development of flames and coherent structures.</p><p id="par0125" class="elsevierStylePara elsevierViewall">The burner exit was varied from an open case with no nozzle to that with a quarl nozzle (<a class="elsevierStyleCrossRef" href="#fig0010">Figure 2</a>). Corresponding swirl numbers are 1.08 and 0.86 respectively (<a class="elsevierStyleCrossRef" href="#bib0100">Valera <span class="elsevierStyleItalic">et al</span>., 2011</a>).</p><p id="par0130" class="elsevierStylePara elsevierViewall">The central fuel injector extended from the burner baseplate to near the nozzle (<a class="elsevierStyleCrossRef" href="#fig0010">Figure 2</a>). This was 35mm outer and 23.4mm inner diameters, whilst its end was located 47.5mm upstream from the burner exit. The nozzle extending into the swirl chamber is designed to reduce flashback by increasing the radial velocity. It was originally developed for a larger scale 2MW version <a name="p607"></a>of this unit (<a class="elsevierStyleCrossRef" href="#bib0085">Syred, 2006</a>). All reported flashback curves were measured with a steel baseplate fitted and the cage and quartz plate removed. For the cases with partially premixed combustion and no injector, fuel was simply fed at low velocity through a nozzle in the center of the baseplate.</p><p id="par0135" class="elsevierStylePara elsevierViewall">First experiments were made with no confinement attached to the combustion chamber. However, as most practical flames do not discharge into free air, for much of the work, confinements from previous experiments (<a class="elsevierStyleCrossRef" href="#bib0085">Syred, 2006</a>; <a class="elsevierStyleCrossRef" href="#bib0105">Valera <span class="elsevierStyleItalic">et al</span>., 2009</a>) were used, with open and conical exit nozzles, the latter being the most representative of industrial burners (<a class="elsevierStyleCrossRef" href="#fig0015">Figure 3</a>).</p><elsevierMultimedia ident="fig0015"></elsevierMultimedia><p id="par0140" class="elsevierStylePara elsevierViewall">The objective was to recognize the position and evolution of flashback, as a function of different geometries and parameters which are known to be influential (<a class="elsevierStyleCrossRef" href="#bib0100">Valera <span class="elsevierStyleItalic">et al</span>., 2011</a>; <a class="elsevierStyleCrossRef" href="#bib0105">2009</a>). Geometrical variables included the effect of a fuel injector, nozzle, two different confinements, with both premixed and partial premixed combustion being also investigated.</p></span><span id="sec0015" class="elsevierStyleSection elsevierViewall"><span class="elsevierStyleSectionTitle" id="sect0035">Results and discussion</span><p id="par0145" class="elsevierStylePara elsevierViewall">The phenomena of flashback was investigated as a function of a wide range of variables for natural gas combustion including equivalence ratio, velocity levels, geometrical parameters including nozzles, confinements and fuel injectors. Comparison between cases was performed using both the averaged (isothermal) axial velocities in the burner exit and the tangential inlet velocity as follows:<ul class="elsevierStyleList" id="lis0015"><li class="elsevierStyleListItem" id="lsti0030"><span class="elsevierStyleLabel">•</span><p id="par0150" class="elsevierStylePara elsevierViewall">V<span class="elsevierStyleInf">ex</span><span class="elsevierStyleHsp" style=""></span>=<span class="elsevierStyleHsp" style=""></span>1.219W</p></li><li class="elsevierStyleListItem" id="lsti0035"><span class="elsevierStyleLabel">•</span><p id="par0155" class="elsevierStylePara elsevierViewall">V<span class="elsevierStyleInf">exqua</span><span class="elsevierStyleHsp" style=""></span>=<span class="elsevierStyleHsp" style=""></span>1.9W</p></li><li class="elsevierStyleListItem" id="lsti0040"><span class="elsevierStyleLabel">•</span><p id="par0160" class="elsevierStylePara elsevierViewall">W<span class="elsevierStyleHsp" style=""></span>=<span class="elsevierStyleHsp" style=""></span>inlet flow rate/tangential inlet area</p></li></ul></p><span id="sec0020" class="elsevierStyleSection elsevierViewall"><span class="elsevierStyleSectionTitle" id="sect0040">Characterization process</span><p id="par0165" class="elsevierStylePara elsevierViewall">A wide range of flashback conditions were investigated for cases with and without confinement, injector and nozzle. Either 100% premixed combustion or partially premixed combustion was used. For each run stable conditions were established for a given air flow and then the equivalence ratio was varied until flashback occurred. The flashback condition was established when the flame moved upstream towards the mixing chamber, accessing the latter. This was monitored using the high speed camera. The burner was then cooled at high airflow before proceeding with the next test. To trigger the high speed camera whilst obtaining flashback conditions, the system was set up at conditions close to flashback with premixed combustion with extra small quantities of diffusive fuel. To initiate flashback the diffusive fuel was then switched off (not being redirected to the premixed inlets), providing consistency for the visualization process.</p></span><span id="sec0025" class="elsevierStyleSection elsevierViewall"><span class="elsevierStyleSectionTitle" id="sect0045">Flashback with no fuel injector, premixed combustion</span><p id="par0170" class="elsevierStylePara elsevierViewall"><a class="elsevierStyleCrossRef" href="#fig0020">Figure 4</a> shows a comparison of flashback conditions for the burner with various geometrical configurations, but no central fuel injector. Best flashback limits are obtained with no confinement or nozzle for most equivalence ratios (<a class="elsevierStyleCrossRef" href="#fig0020">Figure 4a</a>). Comparing <a class="elsevierStyleCrossRef" href="#fig0020">Figures 4b and 4a</a> the nozzle only shows flashback benefit for values of φ<span class="elsevierStyleHsp" style=""></span>≤<span class="elsevierStyleHsp" style=""></span>0.7. However, flashback resistance seems to be worsened by the increased strength of the CRZ, as observed by <a class="elsevierStyleCrossRef" href="#bib0110">Valera-Medina (2009)</a>. The use of the nozzle increases the CRZ, which seems to be affecting the flashback resistance limit. Moreover, <a class="elsevierStyleCrossRef" href="#fig0020">Figures 4c</a> and <a class="elsevierStyleCrossRef" href="#fig0020">4d</a> show that the confinement with or without the nozzle increases susceptibility to flashback for all values of φ (<a class="elsevierStyleCrossRef" href="#bib0005">Bagdanavicius <span class="elsevierStyleItalic">et al</span>., 2009</a>).</p><elsevierMultimedia ident="fig0020"></elsevierMultimedia><p id="par0175" class="elsevierStylePara elsevierViewall">In the case of the confinement, the change in flashback limits is due to reduced external air entrainment and its cylindrical shape which produces changes in axial and radial pressure gradients, thus modifying aerodynamic characteristics. Such aerodynamic changes have been observed under both isothermal and combustion conditions (<a class="elsevierStyleCrossRef" href="#bib0085">Syred, 2006</a>; <a class="elsevierStyleCrossRef" href="#bib0105">Valera <span class="elsevierStyleItalic">et al</span>., 2009</a>). The flashback line is also steeper with confinement, (compare <a class="elsevierStyleCrossRef" href="#fig0020">Figure 4b to 4c</a>) and extends to higher velocities for φ<span class="elsevierStyleHsp" style=""></span>≥<span class="elsevierStyleHsp" style=""></span>0.75. Results were only obtainable up to φ<span class="elsevierStyleHsp" style=""></span>=<span class="elsevierStyleHsp" style=""></span>0.8 with the confinement due to rig limitations, although the trends are clear.</p><p id="par0180" class="elsevierStylePara elsevierViewall"><a name="p608"></a>Comparison of <a class="elsevierStyleCrossRef" href="#fig0020">Figures 4c and 4d</a> shows the dominant effect of the confinement upon flashback as there appears to be little effect of the nozzle. Due to the changes in the aerodynamics that affect the CRZ, the use of confinement alters the strength of the recirculation zone, changing the flashback trend. Other studies (<a class="elsevierStyleCrossRef" href="#bib0110">Valera, 2009</a>; <a class="elsevierStyleCrossRef" href="#bib0065">Nauert <span class="elsevierStyleItalic">et al</span>., 2007</a>) show that confinement augments the CRZ strength, thus confirming that flashback resistance decrement is related to alterations of this structure.</p><p id="par0185" class="elsevierStylePara elsevierViewall">Observations of flashback with the open flame and no confinement showed that just before flashback initiation the flame front was of thin annular form and was located on the burner lip, whilst the resulting flame coalesced a couple of diameters downstream, then being of long lazy form. The flame could be observed to be trying to move down the outer wall boundary layer and was attempting to propagate in this mode. This led to the conclusion that boundary layer flame propagation was part of the way in which the flame flashed back.</p></span><span id="sec0030" class="elsevierStyleSection elsevierViewall"><span class="elsevierStyleSectionTitle" id="sect0050">Flashback with the fuel injector, premixed combustion</span><p id="par0190" class="elsevierStylePara elsevierViewall"><a class="elsevierStyleCrossRef" href="#fig0025">Figure 5</a> shows three flashback curves with the fuel injector. The improvements in flashback occurrence are very clear and emphasize the advantages of the use of the injector for all cases.</p><elsevierMultimedia ident="fig0025"></elsevierMultimedia><p id="par0195" class="elsevierStylePara elsevierViewall">Differences between two sets of curves, <a class="elsevierStyleCrossRef" href="#fig0025">Figures 5a and 5b</a>, are small with the nozzle, with or without the confinement. <a class="elsevierStyleCrossRef" href="#fig0025">Figure 5c</a> with the confinement and no nozzle shows flashback limits that are somewhat worsened, occurring at velocities about 10% higher. Nevertheless, the trend is consistent. The increase in flashback resistance is produced by the presence of the injector, which avoids the direct influence of the CRZ, probably with the avoidance of the formation of the CIVB. Comparing <a class="elsevierStyleCrossRef" href="#fig0020">Figures 4</a> and <a class="elsevierStyleCrossRef" href="#fig0025">5</a>, the changes in aerodynamics above the injector are no longer a determinant factor in the flashback limit. This leaves the entire phenomenon to the boundary layer propagation. Moreover, a core <a name="p609"></a>flow acceleration induced by the injector increases flow velocities in the annular flow surrounding the latter, hence boundary layer velocity gradients in the outer wall boundary layer are augmented with flashback resistance.</p><p id="par0200" class="elsevierStylePara elsevierViewall">The flame with the injector would also re-attach to the nozzle for rich equivalent ratios, an effect of the changes in flame front location, occurrence and form of any CRZ. There appears to be a transition from the state with flashback for equivalence ratios less than about 1.05 to that with the flame attached to the lip of the nozzle. Flashback always occurred soon after two flame fronts formed, one located in the core flow, the other on the outer burner lip</p><p id="par0205" class="elsevierStylePara elsevierViewall">As discussed earlier, flashback was more intense with the injector for all cases tested. This occurs because velocity levels at flashback are lower in the system by up to a factor of 2 for a given equivalence ratio, compare <a class="elsevierStyleCrossRef" href="#fig0020">Figures 4</a> and <a class="elsevierStyleCrossRef" href="#fig0025">5</a>. The fitting of the fuel injector has thus substantially improved flashback limits.</p><p id="par0210" class="elsevierStylePara elsevierViewall">An interesting phenomenon developed from low to intermediate Re (~15,000 to 26,000) around values of φ ~ 1.1 to 1.2. The flame would attach to the nozzle, then move in, down the boundary layer, and then out of the nozzle around the injector. At this point the flame was incapable of flashback through the boundary layer or indeed stabilizing in the shear flow between the nozzle and fuel injector as velocity gradients were too high. When an equivalence ratio of 1.1 was reached, the flame located inside of the sleeve in the boundary layer around the injector. There was no reaction in the annulus between the outer flame at the wall and the inner flame stabilized close to the swirl chamber. Under these conditions the flame would not flashback into the swirl chamber. At an equivalence ratio of 1.19 the flame moved back out of the burner and located on the lip of the nozzle. Boundary layer propagation seems to be the leading mechanism of flashback with the injector for lean equivalence ratios. However, the phenomenon of boundary layer propagation towards the swirling flow is also altered by the stoichiometry of the flame and the velocity of reaction. Since the natural gas has a relatively slow burning velocity, the increase of mass flow rate (air and gas) produced a faster flow than the boundary layer propagation at high equivalence ratios, thus pushing back the flame towards the tip of the injector. This phenomenon was observed with both the open and the quarl nozzle (<a class="elsevierStyleCrossRef" href="#fig0010">Figure 2</a>). A summary of all premixed combustion cases is shown in <a class="elsevierStyleCrossRef" href="#tbl0005">Table 1</a>.</p><elsevierMultimedia ident="tbl0005"></elsevierMultimedia></span><span id="sec0035" class="elsevierStyleSection elsevierViewall"><span class="elsevierStyleSectionTitle" id="sect0055">Visualization of the flow</span><p id="par0215" class="elsevierStylePara elsevierViewall">The process of flashback was visualized with high speed photography and results from the two cases with and without the injector are shown from <a class="elsevierStyleCrossRef" href="#fig0030">Figures 6a to 6l</a>. <a class="elsevierStyleCrossRef" href="#fig0030">Figures 6b to 6f</a> show a sequence of images from the camera via a top view and the 45° mirror with no fuel injector. The camera focuses only on the nozzle. <a class="elsevierStyleCrossRef" href="#fig0030">Figure 6a</a> is a photo of the flame just before flashback and shows how the flame is attached to the burner lip with no combustion in the mid - section, φ<span class="elsevierStyleHsp" style=""></span>=<span class="elsevierStyleHsp" style=""></span>0.54, the main <a name="p610"></a>flame developing well downstream. At higher flow rates the flame was lifted and only reattaches to the burner lip close to flashback.</p><elsevierMultimedia ident="fig0030"></elsevierMultimedia><p id="par0220" class="elsevierStylePara elsevierViewall">A sequence of flame images, from <a class="elsevierStyleCrossRef" href="#fig0030">Figure 6b to 6f</a>, shows how flashback is initiated. <a class="elsevierStyleCrossRef" href="#fig0030">Figure 6b</a>, besides illustrating the onset of combustion, shows the quartz baseplate with the dark blue image of the (not used) feed for the injector. Combustion is initiated in two regions in the outer wall region and boundary layer (<a class="elsevierStyleCrossRef" href="#fig0030">Figure 6b</a>). Combustion quickly propagates upstream and across the section of the nozzle, such that after 10 milliseconds it has spread to almost all the section of the nozzle, <a class="elsevierStyleCrossRef" href="#fig0030">Figures 6b to 6f</a>. With this configuration the flashback process is intermittent with flames darting up and down the wall boundary layer, often being stretched to extinction, not quite reaching the main swirl chamber and causing complete flashback. Interesting behavior occurred in the swirl chamber as the flame propagated radially outwards from the end of the nozzle to the tangential inlets (not shown). The process has a complex 2D propagation with the flames apparently following the inlet flow back to the inlets; simultaneously PVCs and small CRZs developed in the central region of flow, this is discussed in more detail elsewhere (<a class="elsevierStyleCrossRef" href="#bib0110">Valera, 2009</a>; <a class="elsevierStyleCrossRef" href="#bib0115">Vigueras <span class="elsevierStyleItalic">et al</span>., 2012</a>).</p><p id="par0225" class="elsevierStylePara elsevierViewall">The process is quite different when the fuel injector is present, from <a class="elsevierStyleCrossRef" href="#fig0030">Figures 6g to 6l</a>. <a class="elsevierStyleCrossRef" href="#fig0030">Figure 6g</a> shows the flame just before flashback, φ<span class="elsevierStyleHsp" style=""></span>=<span class="elsevierStyleHsp" style=""></span>0.95. Two flame fronts are formed, one as before on the outer burner lip, the other in the center being stabilized by the fuel injector. Because of the higher value of φ and the presence of two flames it was not possible to visualize processes from the top view. The sequence of images shows flashback development via a bottom view through the quartz baseplate. The feed to the fuel injector obscures part of the view. In <a class="elsevierStyleCrossRef" href="#fig0030">Figure 6h</a> the quite uniform flame radiation from the burner exit is evident with combustion occurring in the wall boundary layers (green). Moving through the images flame propagation occurs radially outwards from the nozzle into the swirl chamber developing over a sector extending from ~70° to 150°. This process was not as intermittent as in the previous case and was much more violent owing to the higher values of φ and lower velocities due to the lower air flows. The flames rapidly and completely filled the swirl chamber to the tangential inlets in contrast to the case without the injector.</p><p id="par0230" class="elsevierStylePara elsevierViewall">At low air flow rates boundary layer propagation is the leading mechanism of flashback. However, if the air-gas flow rate is high enough to overcome the propagation in the boundary layers of the sleeve and injector, flashback will not occur and the flame will be pushed back to the nozzle with a phenomenon of reattachment to the lip of the burner. This was corroborated using the high speed photography (<a class="elsevierStyleCrossRef" href="#fig0035">Figure 7</a>).</p><elsevierMultimedia ident="fig0035"></elsevierMultimedia></span></span><span id="sec0040" class="elsevierStyleSection elsevierViewall"><span class="elsevierStyleSectionTitle" id="sect0060">Conclusions</span><p id="par0235" class="elsevierStylePara elsevierViewall">This paper describes a series of experiments for the analysis of flashback in a pilot scale swirl burner fired on natural gas. Several conclusions emerge:<ul class="elsevierStyleList" id="lis0020"><li class="elsevierStyleListItem" id="lsti0045"><span class="elsevierStyleLabel">1.</span><p id="par0240" class="elsevierStylePara elsevierViewall">When firing premixed natural gas the presence of a central fuel injector substantially improves resistance to flashback for the given swirl number range. This seems to be caused by flow acceleration in the central core flow affecting the outer wall boundary layer and the velocity gradients, added to the avoidance of the formation of any coherent structure through the burner passages. When no injector is present, the <a name="p611"></a><a name="p612"></a>flow is generally of lower velocity across the flow section, coherent structures can propagate and hence the system is less able to resist flashback.</p></li><li class="elsevierStyleListItem" id="lsti0050"><span class="elsevierStyleLabel">2.</span><p id="par0245" class="elsevierStylePara elsevierViewall">When no fuel injector was present, the nozzle and the confinements of <a class="elsevierStyleCrossRef" href="#fig0015">Figure 3</a> worsened flashback. This is caused by changes in decay of tangential velocity profiles in the axial direction and elimination of external flow entrainment, which in turn alter the pressure gradients which govern CRZ formation/strength and flame front location.</p></li><li class="elsevierStyleListItem" id="lsti0055"><span class="elsevierStyleLabel">3.</span><p id="par0250" class="elsevierStylePara elsevierViewall">Flow visualization, flame characteristics and CFD indicate that no CRZs are present just before flashback without the injector. However, other experiments demonstrate the existence of a strong CRZ that influence the flame movement upstream, whilst others give details of coherent structures formed in the passages of the burner. Thus, the lack of CRZ just before flashback seems to be a point of transition that needs further research.</p></li><li class="elsevierStyleListItem" id="lsti0060"><span class="elsevierStyleLabel">4.</span><p id="par0255" class="elsevierStylePara elsevierViewall">High speed photography showed that flashback started in a small area of the wall boundary of the burner exit and then rapidly spread across the nozzle as the flame propagated upstream.</p></li><li class="elsevierStyleListItem" id="lsti0065"><span class="elsevierStyleLabel">5.</span><p id="par0260" class="elsevierStylePara elsevierViewall">The nozzle improved the flashback behavior by moving the flames further away from the injector and downstream of the burner exit with partially premixed injection. Different flow rates and equivalence ratios changed the position of the flame from being lifted to being attached prior to flashback; the CRZ that anchors the flame also moves axially in this process.</p></li></ul></p></span><span id="s2560" class="elsevierStyleSection elsevierViewall"><span class="elsevierStyleSectionTitle" id="st0000">Nomenclature</span><p id="par0275" class="elsevierStylePara elsevierViewall"><span class="elsevierStyleDefList"><span class="elsevierStyleDefTerm">Ae</span><span class="elsevierStyleDefDescription"><p id="p9900" class="elsevierStylePara elsevierViewall">Inlet area [m<span class="elsevierStyleSup">2</span>]</p></span><span class="elsevierStyleDefTerm">CRZ</span><span class="elsevierStyleDefDescription"><p id="par9900" class="elsevierStylePara elsevierViewall">Central Recirculation Zone</p></span><span class="elsevierStyleDefTerm">PVC</span><span class="elsevierStyleDefDescription"><p id="par9980" class="elsevierStylePara elsevierViewall">Precessing Vortex Core</p></span><span class="elsevierStyleDefTerm">R<span class="elsevierStyleInf">e</span></span><span class="elsevierStyleDefDescription"><p id="p8950" class="elsevierStylePara elsevierViewall">Reynolds number [-]. Here is defined using average exit velocity and gas kinematic viscosity from the burner under isothermal conditions</p></span><span class="elsevierStyleDefTerm">r<span class="elsevierStyleInf">e</span></span><span class="elsevierStyleDefDescription"><p id="p6580" class="elsevierStylePara elsevierViewall">Exit radius of the burner [m]</p></span><span class="elsevierStyleDefTerm">r<span class="elsevierStyleInf">i</span></span><span class="elsevierStyleDefDescription"><p id="p2000" class="elsevierStylePara elsevierViewall">Radius upon which the tangential inlet jets fire [m]</p></span><span class="elsevierStyleDefTerm">S</span><span class="elsevierStyleDefDescription"><p id="p3000" class="elsevierStylePara elsevierViewall">Geometrical Swirl number defined in the text [-]</p></span><span class="elsevierStyleDefTerm">S<span class="elsevierStyleInf">t</span></span><span class="elsevierStyleDefDescription"><p id="p4000" class="elsevierStylePara elsevierViewall">Turbulent Flame Speed [m/s]</p></span><span class="elsevierStyleDefTerm">V<span class="elsevierStyleInf">ex</span></span><span class="elsevierStyleDefDescription"><p id="p5000" class="elsevierStylePara elsevierViewall">Exit velocity (axial), no nozzle [m/s]</p></span><span class="elsevierStyleDefTerm">V<span class="elsevierStyleInf">exqua</span></span><span class="elsevierStyleDefDescription"><p id="p6000" class="elsevierStylePara elsevierViewall">Exit velocity (axial), with/without injector, nozzle fitted [m/s]</p></span><span class="elsevierStyleDefTerm">W</span><span class="elsevierStyleDefDescription"><p id="p7000" class="elsevierStylePara elsevierViewall">Tangential inlet velocity [m/s]</p></span><span class="elsevierStyleDefTerm">φ</span><span class="elsevierStyleDefDescription"><p id="par8000" class="elsevierStylePara elsevierViewall">Equivalence ratio [-]</p></span></span></p></span></span>" "textoCompletoSecciones" => array:1 [ "secciones" => array:12 [ 0 => array:2 [ "identificador" => "xres405040" "titulo" => "Abstract" ] 1 => array:2 [ "identificador" => "xpalclavsec381416" "titulo" => "Keywords" ] 2 => array:2 [ "identificador" => "xres405039" "titulo" => "Resumen" ] 3 => array:2 [ "identificador" => "xpalclavsec381417" "titulo" => "Descriptores" ] 4 => array:2 [ "identificador" => "sec0005" "titulo" => "Introduction" ] 5 => array:2 [ "identificador" => "sec0010" "titulo" => "Experimental setup" ] 6 => array:3 [ "identificador" => "sec0015" "titulo" => "Results and discussion" "secciones" => array:4 [ 0 => array:2 [ "identificador" => "sec0020" "titulo" => "Characterization process" ] 1 => array:2 [ "identificador" => "sec0025" "titulo" => "Flashback with no fuel injector, premixed combustion" ] 2 => array:2 [ "identificador" => "sec0030" "titulo" => "Flashback with the fuel injector, premixed combustion" ] 3 => array:2 [ "identificador" => "sec0035" "titulo" => "Visualization of the flow" ] ] ] 7 => array:2 [ "identificador" => "sec0040" "titulo" => "Conclusions" ] 8 => array:2 [ "identificador" => "s2560" "titulo" => "Nomenclature" ] 9 => array:2 [ "identificador" => "xack117830" "titulo" => "Acknowledgements" ] 10 => array:1 [ "titulo" => "<span class="elsevierStyleSectionTitle" id="sect0125">Citation for this article:</span>" ] 11 => array:1 [ "titulo" => "References" ] ] ] "pdfFichero" => "main.pdf" "tienePdf" => true "fechaRecibido" => "2013-04-30" "fechaAceptado" => "2013-07-31" "PalabrasClave" => array:2 [ "en" => array:1 [ 0 => array:4 [ "clase" => "keyword" "titulo" => "Keywords" "identificador" => "xpalclavsec381416" "palabras" => array:3 [ 0 => "flashback" 1 => "swirling flows" 2 => "high speed photography" ] ] ] "es" => array:1 [ 0 => array:4 [ "clase" => "keyword" "titulo" => "Descriptores" "identificador" => "xpalclavsec381417" "palabras" => array:3 [ 0 => "reflujo de llama" 1 => "flujos giratorios" 2 => "fotografía de rápida velocidad" ] ] ] ] "tieneResumen" => true "resumen" => array:2 [ "en" => array:2 [ "titulo" => "Abstract" "resumen" => "<p id="spar0045" class="elsevierStyleSimplePara elsevierViewall">Lean premixed combustion using swirling flows is widely used in gas turbines and combustion. Although flashback is not generally a problem with natural gas combustion, there are some reports of flashback damage with existing gas turbines, whilst hydrogen enriched fuel blends cause concerns in this area. Thus, this paper describes a practical approach to study and avoid flashback in a pilot scale 100<span class="elsevierStyleHsp" style=""></span>kW tangential swirl burner. The flashback phenomenon is studied experimentally via the derivation of flashback limits for a variety of different geometrical conditions. A high speed camera is used to visualize the process and distinguish new patterns of avoidance. The use of a central fuel injector is shown to give substantial benefits in terms of flashback resistance. Conclusions are drawn as to mitigation technologies.</p>" ] "es" => array:2 [ "titulo" => "Resumen" "resumen" => "<p id="spar0050" class="elsevierStyleSimplePara elsevierViewall">El uso de flujos giratorios en condiciones pobres premezcladas se utiliza ampliamente en turbinas de gas y en combustión en general. A pesar de que el reflujo de llama no suele ser un problema durante la combustión de gas natural, existen muchos reportes sobre el daño que el reflujo puede producir en turbinas de gas actuales, especialmente cuando se utilizan mezclas de combustible con hidrógeno enriquecido. Por ende, este artículo describe una aproximación práctica al estudio y eliminación del reflujo de llama en un quemador de flujo giratorio tangencial de 100kW. El fenómeno de reflujo de llama se estudia experimentalmente mediante la derivación de los límites de reflujo para una gran variedad de geometrías diferentes. Se utilizó una cámara de fotografía rápida para visualizar el proceso y distinguir algunos parámetros para evitar el fenómeno. El uso de un inyector de combustible central produjo beneficios substanciales en términos de resistencia al reflujo de llama. Se presentan conclusiones sobre cómo mitigar el fenómeno.</p>" ] ] "NotaPie" => array:4 [ 0 => array:2 [ "etiqueta" => "*" "nota" => "<p class="elsevierStyleNotepara" id="np1520"><span class="elsevierStyleItalic">Marco Osvaldo Vigueras-Zúñiga.</span> Mechanical engineer from UNAM, obtained his MSc in project management and his PhD in thermofluids for turbomachinery at Cranfield University, England. He is responsible for the energy-thermofluid research group at the Universidad Veracruzana and has the role of leader in numerical simulation in combustion technologies. He is also consultant for research projects in the fields of oil and gas, energy and aerospace. He has various publications with national and international journals, as well as several research thesis.</p>" ] 1 => array:2 [ "etiqueta" => "**" "nota" => "<p class="elsevierStyleNotepara" id="np4710"><span class="elsevierStyleItalic">Agustín Valera-Medina</span>. Mechanical engineer from the UNAM, obtained his MSc in geoenvironmental engineering and a PhD in combustion dyanmics at Cardiff University, Wales. After working for a research centre in Mexico, CIATEQ, he moved back to the UK to continue his research in combustion dynamics and thermofluids for gas turbines. Now, he is a lecturer at Cardiff University, involved in the topics of propulsion, combustion, alternative fuels and thermoacoustics. He has participated in several international conferences, with more than 30 publications. Some of the latter have been written for journals such as Combustion and Flame, Experiments in Fluids, ASME, AIAA, etc.</p>" ] 2 => array:2 [ "etiqueta" => "***" "nota" => "<p class="elsevierStyleNotepara" id="np7410"><span class="elsevierStyleItalic">Nicholas Syred.</span> Mechanical engineer from Sheffield, he obtained his doctoral degree in 1969 in power fluids, getting a position as associate researcher in the department of swirling flows under the tutelage of Prof. Chigier and Prof. Beer. He moved to Cardiff in 1974, where he has conducted a great variety of projects with BP, Air Products, SERC, UKAEA, etc. In 2002, he was awarded the NATO prize for innovation in cooling systems for gas turbine blades. Currently, he is a fellow of the IMechE. He has published more than 300 papers, giving supervision to more than 30 students at PhD level.</p>" ] 3 => array:2 [ "etiqueta" => "****" "nota" => "<p class="elsevierStyleNotepara" id="np1500"><span class="elsevierStyleItalic">Daniel de la Rosa-Urbalejo.</span> Industrial engineer from the UNAM, he worked for 4 years in the aerospace industry. He was awarded a scholarship for his MSc in mechanical engineering at the Faculty of Engineering, UNAM. After completing his degree, he was awarded another scholarship to continue his studies at Cardiff University, obtaining a PhD in flame stretch and combustion fundamentals using alternative fuels. He has participated in 9 conferences across Europe and the United States, presenting 2 papers in the European combustion meeting and the turbo expo ASME.</p>" ] ] "multimedia" => array:8 [ 0 => array:7 [ "identificador" => "fig0005" "etiqueta" => "Figure 1" "tipo" => "MULTIMEDIAFIGURA" "mostrarFloat" => true "mostrarDisplay" => false "figura" => array:1 [ 0 => array:4 [ "imagen" => "gr1.jpeg" "Alto" => 700 "Ancho" => 946 "Tamanyo" => 125600 ] ] "descripcion" => array:1 [ "en" => "<p id="spar0005" class="elsevierStyleSimplePara elsevierViewall">Details of swirl burner</p>" ] ] 1 => array:7 [ "identificador" => "fig0010" "etiqueta" => "Figure 2" "tipo" => "MULTIMEDIAFIGURA" "mostrarFloat" => true "mostrarDisplay" => false "figura" => array:1 [ 0 => array:4 [ "imagen" => "gr2.jpeg" "Alto" => 674 "Ancho" => 963 "Tamanyo" => 74867 ] ] "descripcion" => array:1 [ "en" => "<p id="spar0010" class="elsevierStyleSimplePara elsevierViewall">Quarl nozzle</p>" ] ] 2 => array:7 [ "identificador" => "fig0015" "etiqueta" => "Figure 3" "tipo" => "MULTIMEDIAFIGURA" "mostrarFloat" => true "mostrarDisplay" => false "figura" => array:1 [ 0 => array:4 [ "imagen" => "gr3.jpeg" "Alto" => 587 "Ancho" => 963 "Tamanyo" => 65249 ] ] "descripcion" => array:1 [ "en" => "<p id="spar0015" class="elsevierStyleSimplePara elsevierViewall">Burner confinements a) open and b) conical exit geometries</p>" ] ] 3 => array:7 [ "identificador" => "fig0020" "etiqueta" => "Figure 4" "tipo" => "MULTIMEDIAFIGURA" "mostrarFloat" => true "mostrarDisplay" => false "figura" => array:1 [ 0 => array:4 [ "imagen" => "gr4.jpeg" "Alto" => 1184 "Ancho" => 2002 "Tamanyo" => 204757 ] ] "descripcion" => array:1 [ "en" => "<p id="spar0020" class="elsevierStyleSimplePara elsevierViewall">Flashback comparison without fuel injector. Confinement as in <a class="elsevierStyleCrossRef" href="#fig0015">Figure 3a</a>, a) no confinement-without nozzle, b) no confinementnozzle, c) confinement-nozzle, d) confinement-without nozzle</p>" ] ] 4 => array:7 [ "identificador" => "fig0025" "etiqueta" => "Figure 5" "tipo" => "MULTIMEDIAFIGURA" "mostrarFloat" => true "mostrarDisplay" => false "figura" => array:1 [ 0 => array:4 [ "imagen" => "gr5.jpeg" "Alto" => 1874 "Ancho" => 935 "Tamanyo" => 169011 ] ] "descripcion" => array:1 [ "en" => "<p id="spar0025" class="elsevierStyleSimplePara elsevierViewall">Flashback results with fuel injector. Confinement as in <a class="elsevierStyleCrossRef" href="#fig0015">Figure 3a</a>, a) no confinement-nozzle, b) confinement-nozzle, c) confinement-without nozzle</p>" ] ] 5 => array:7 [ "identificador" => "fig0030" "etiqueta" => "Figure 6" "tipo" => "MULTIMEDIAFIGURA" "mostrarFloat" => true "mostrarDisplay" => false "figura" => array:1 [ 0 => array:4 [ "imagen" => "gr6.jpeg" "Alto" => 2393 "Ancho" => 1714 "Tamanyo" => 592767 ] ] "descripcion" => array:1 [ "en" => "<p id="spar0030" class="elsevierStyleSimplePara elsevierViewall">Flame and high speed camera images, a) top view, no injector with nozzle, 700_l/min air, φ<span class="elsevierStyleHsp" style=""></span>=<span class="elsevierStyleHsp" style=""></span>0.54, flame just before flashback, b to f) high speed camera images separated by 2 milliseconds showing flashback development, g) bottom view with injector and nozzle, φ<span class="elsevierStyleHsp" style=""></span>=<span class="elsevierStyleHsp" style=""></span>0.95, S<span class="elsevierStyleHsp" style=""></span>=<span class="elsevierStyleHsp" style=""></span>0.86, h to l) high speed camera images separated 2 milliseconds showing flashback expanding into the swirl chamber</p>" ] ] 6 => array:7 [ "identificador" => "fig0035" "etiqueta" => "Figure 7" "tipo" => "MULTIMEDIAFIGURA" "mostrarFloat" => true "mostrarDisplay" => false "figura" => array:1 [ 0 => array:4 [ "imagen" => "gr7.jpeg" "Alto" => 566 "Ancho" => 1833 "Tamanyo" => 107753 ] ] "descripcion" => array:1 [ "en" => "<p id="spar0035" class="elsevierStyleSimplePara elsevierViewall">Case at 100<span class="elsevierStyleHsp" style=""></span>l/min gas, 100% premixed, a) the airflow is at 1,000<span class="elsevierStyleHsp" style=""></span>l/min. The flame is attached to the nozzle, b) the airflow is at 900<span class="elsevierStyleHsp" style=""></span>l/min. The flame is inside of the sleeve, close to flashback into the swirl chamber, c) the airflow is at 800<span class="elsevierStyleHsp" style=""></span>l/min. The flame is reattached to the nozzle again, out of the sleeve</p>" ] ] 7 => array:7 [ "identificador" => "tbl0005" "etiqueta" => "Table 1" "tipo" => "MULTIMEDIATABLA" "mostrarFloat" => true "mostrarDisplay" => false "tabla" => array:1 [ "tablatextoimagen" => array:1 [ 0 => array:2 [ "tabla" => array:1 [ 0 => """ <table border="0" frame="\n \t\t\t\t\tvoid\n \t\t\t\t" class=""><thead title="thead"><tr title="table-row"><td class="td" title="\n \t\t\t\t\ttable-head\n \t\t\t\t " align="center" valign="top" style="border-bottom: 2px solid black">Confinement \t\t\t\t\t\t\n \t\t\t\t</td><td class="td" title="\n \t\t\t\t\ttable-head\n \t\t\t\t " align="center" valign="top" style="border-bottom: 2px solid black">Injector \t\t\t\t\t\t\n \t\t\t\t</td><td class="td" title="\n \t\t\t\t\ttable-head\n \t\t\t\t " align="center" valign="top" style="border-bottom: 2px solid black">Nozzle \t\t\t\t\t\t\n \t\t\t\t</td><td class="td" title="\n \t\t\t\t\ttable-head\n \t\t\t\t " align="center" valign="top" style="border-bottom: 2px solid black">Swirl Number S \t\t\t\t\t\t\n \t\t\t\t</td><td class="td" title="\n \t\t\t\t\ttable-head\n \t\t\t\t " align="center" valign="top" style="border-bottom: 2px solid black">Observations \t\t\t\t\t\t\n \t\t\t\t</td></tr></thead><tbody title="tbody"><tr title="table-row"><td class="td" title="\n \t\t\t\t\ttable-entry\n \t\t\t\t " align="" valign="\n \t\t\t\t\ttop\n \t\t\t\t"> \t\t\t\t\t\t\n \t\t\t\t</td><td class="td" title="\n \t\t\t\t\ttable-entry\n \t\t\t\t " align="" valign="\n \t\t\t\t\ttop\n \t\t\t\t"> \t\t\t\t\t\t\n \t\t\t\t</td><td class="td" title="\n \t\t\t\t\ttable-entry\n \t\t\t\t " align="" valign="\n \t\t\t\t\ttop\n \t\t\t\t"> \t\t\t\t\t\t\n \t\t\t\t</td><td class="td" title="\n \t\t\t\t\ttable-entry\n \t\t\t\t " align="center" valign="top">1.08 \t\t\t\t\t\t\n \t\t\t\t</td><td class="td" title="\n \t\t\t\t\ttable-entry\n \t\t\t\t " align="left" valign="top"><a class="elsevierStyleCrossRef" href="#fig0020">Figura 4a</a>. Typical flashback curve with a near stoichiometric peak \t\t\t\t\t\t\n \t\t\t\t</td></tr><tr title="table-row"><td class="td" title="\n \t\t\t\t\ttable-entry\n \t\t\t\t " align="" valign="\n \t\t\t\t\ttop\n \t\t\t\t"> \t\t\t\t\t\t\n \t\t\t\t</td><td class="td" title="\n \t\t\t\t\ttable-entry\n \t\t\t\t " align="" valign="\n \t\t\t\t\ttop\n \t\t\t\t"> \t\t\t\t\t\t\n \t\t\t\t</td><td class="td" title="\n \t\t\t\t\ttable-entry\n \t\t\t\t " align="center" valign="top">✓ \t\t\t\t\t\t\n \t\t\t\t</td><td class="td" title="\n \t\t\t\t\ttable-entry\n \t\t\t\t " align="center" valign="top">0.86 \t\t\t\t\t\t\n \t\t\t\t</td><td class="td" title="\n \t\t\t\t\ttable-entry\n \t\t\t\t " align="left" valign="top"><a class="elsevierStyleCrossRef" href="#fig0020">Figura 4b</a>. Nozzle decreases flashback resistance. Stronger CRZ visualized, possible responsible \t\t\t\t\t\t\n \t\t\t\t</td></tr><tr title="table-row"><td class="td" title="\n \t\t\t\t\ttable-entry\n \t\t\t\t " align="center" valign="top">✓ \t\t\t\t\t\t\n \t\t\t\t</td><td class="td" title="\n \t\t\t\t\ttable-entry\n \t\t\t\t " align="" valign="\n \t\t\t\t\ttop\n \t\t\t\t"> \t\t\t\t\t\t\n \t\t\t\t</td><td class="td" title="\n \t\t\t\t\ttable-entry\n \t\t\t\t " align="center" valign="top">✓ \t\t\t\t\t\t\n \t\t\t\t</td><td class="td" title="\n \t\t\t\t\ttable-entry\n \t\t\t\t " align="center" valign="top">0.86 \t\t\t\t\t\t\n \t\t\t\t</td><td class="td" title="\n \t\t\t\t\ttable-entry\n \t\t\t\t " align="left" valign="top"><a class="elsevierStyleCrossRef" href="#fig0020">Figura 4c</a>. Confinement and nozzle decrease flashback resistance substantially \t\t\t\t\t\t\n \t\t\t\t</td></tr><tr title="table-row"><td class="td" title="\n \t\t\t\t\ttable-entry\n \t\t\t\t " align="center" valign="top">✓ \t\t\t\t\t\t\n \t\t\t\t</td><td class="td" title="\n \t\t\t\t\ttable-entry\n \t\t\t\t " align="" valign="\n \t\t\t\t\ttop\n \t\t\t\t"> \t\t\t\t\t\t\n \t\t\t\t</td><td class="td" title="\n \t\t\t\t\ttable-entry\n \t\t\t\t " align="" valign="\n \t\t\t\t\ttop\n \t\t\t\t"> \t\t\t\t\t\t\n \t\t\t\t</td><td class="td" title="\n \t\t\t\t\ttable-entry\n \t\t\t\t " align="center" valign="top">1.08 \t\t\t\t\t\t\n \t\t\t\t</td><td class="td" title="\n \t\t\t\t\ttable-entry\n \t\t\t\t " align="left" valign="top"><a class="elsevierStyleCrossRef" href="#fig0020">Figura 4d</a>. Very similar to previous case, despite removal of nozzle \t\t\t\t\t\t\n \t\t\t\t</td></tr><tr title="table-row"><td class="td" title="\n \t\t\t\t\ttable-entry\n \t\t\t\t " align="" valign="\n \t\t\t\t\ttop\n \t\t\t\t"> \t\t\t\t\t\t\n \t\t\t\t</td><td class="td" title="\n \t\t\t\t\ttable-entry\n \t\t\t\t " align="center" valign="top">✓ \t\t\t\t\t\t\n \t\t\t\t</td><td class="td" title="\n \t\t\t\t\ttable-entry\n \t\t\t\t " align="center" valign="top">✓ \t\t\t\t\t\t\n \t\t\t\t</td><td class="td" title="\n \t\t\t\t\ttable-entry\n \t\t\t\t " align="center" valign="top">0.86 \t\t\t\t\t\t\n \t\t\t\t</td><td class="td" title="\n \t\t\t\t\ttable-entry\n \t\t\t\t " align="left" valign="top"><a class="elsevierStyleCrossRef" href="#fig0025">Figura 5a</a>. Typical flashback curve, with a near stoichiometric peak, limits much improved due to Injector use \t\t\t\t\t\t\n \t\t\t\t</td></tr><tr title="table-row"><td class="td" title="\n \t\t\t\t\ttable-entry\n \t\t\t\t " align="center" valign="top">✓ \t\t\t\t\t\t\n \t\t\t\t</td><td class="td" title="\n \t\t\t\t\ttable-entry\n \t\t\t\t " align="center" valign="top">✓ \t\t\t\t\t\t\n \t\t\t\t</td><td class="td" title="\n \t\t\t\t\ttable-entry\n \t\t\t\t " align="center" valign="top">✓ \t\t\t\t\t\t\n \t\t\t\t</td><td class="td" title="\n \t\t\t\t\ttable-entry\n \t\t\t\t " align="center" valign="top">0.86 \t\t\t\t\t\t\n \t\t\t\t</td><td class="td" title="\n \t\t\t\t\ttable-entry\n \t\t\t\t " align="left" valign="top"><a class="elsevierStyleCrossRef" href="#fig0025">Figura 5b</a>. Flashback curve similar to previous case. Confinement has little effect here on flashback \t\t\t\t\t\t\n \t\t\t\t</td></tr><tr title="table-row"><td class="td" title="\n \t\t\t\t\ttable-entry\n \t\t\t\t " align="center" valign="top">✓ \t\t\t\t\t\t\n \t\t\t\t</td><td class="td" title="\n \t\t\t\t\ttable-entry\n \t\t\t\t " align="center" valign="top">✓ \t\t\t\t\t\t\n \t\t\t\t</td><td class="td" title="\n \t\t\t\t\ttable-entry\n \t\t\t\t " align="" valign="\n \t\t\t\t\ttop\n \t\t\t\t"> \t\t\t\t\t\t\n \t\t\t\t</td><td class="td" title="\n \t\t\t\t\ttable-entry\n \t\t\t\t " align="center" valign="top">1.08 \t\t\t\t\t\t\n \t\t\t\t</td><td class="td" title="\n \t\t\t\t\ttable-entry\n \t\t\t\t " align="left" valign="top"><a class="elsevierStyleCrossRef" href="#fig0025">Figura 5c</a>. Flashback curve somewhat worse than previous 2 cases due to absence of nozzle \t\t\t\t\t\t\n \t\t\t\t</td></tr></tbody></table> """ ] "imagenFichero" => array:1 [ 0 => "xTab630076.png" ] ] ] ] "descripcion" => array:1 [ "en" => "<p id="spar0040" class="elsevierStyleSimplePara elsevierViewall">Summary of all cases with premixed combustion</p>" ] ] ] "bibliografia" => array:2 [ "titulo" => "References" "seccion" => array:1 [ 0 => array:2 [ "identificador" => "bibs0005" "bibliografiaReferencia" => array:23 [ 0 => array:3 [ "identificador" => "bib0005" "etiqueta" => "Bagdanavicius et al., 2009" "referencia" => array:1 [ 0 => array:2 [ "contribucion" => array:1 [ 0 => array:1 [ "autores" => array:1 [ 0 => array:2 [ "etal" => false "autores" => array:6 [ 0 => "A. Bagdanavicius" 1 => "P. Bowen" 2 => "N. Syred" 3 => "P. Kay" 4 => "A. Crayford" 5 => "Wood J. 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