BIOFLAM PROJECT: APPLICATION OF LIQUID BIOFUELS IN NEW HEATING TECHNOLOGIES FOR DOMESTIC APPLIANCES BASED ON COOL FLAME VAPORIZATION AND POROUS MEDIUM COMBUSTION T. Brehmer1, F. Heger1, K. Lucka2, J. von Schloss2, Y. Abu-Sharekh3, D. Trimis3, A. Heeb4, G. Köb4, T. Hayashi5, J.C.F. Pereira5, M. Founti6, D. Kolaitis6, M. Molinari7, A. Ortona7, J.-B. Michel8, P. Theurillat8 1 OMV AG, Vienna, Austria, 2 EST, RWTH-Aachen, Aachen, Germany, 3 LSTM, University of Erlangen-Nuremberg, Erlangen, Germany, 4 Hovalwerk AG, Vaduz, Liechtenstein, 5 LASEF, Instituto Superior Tecnico (IST), Lisbon, Portugal, 6 Thermal Section, National Technical University of Athens (NTUA), Athens, Greece, 7 PTC SA, Novazzano, Switzerland, 8 CSEM SA, Neuchâtel, Switzerland. Abstract The BIOFLAM project intends to provide solutions to the problem of environmental impact of combustion of liquid fuels for heating purposes. Oil burners show up to date a very poor power modulation especially at low power outputs, as usually needed in domestic appliances. Liquid biofuels like FAME are also not compatible with conventional oil burner technologies. Furthermore, the integration of oil burners in wall-hung systems requires further burner size reductions. Within the EC-funded BIOFLAM project new liquid fuel fired condensing boilers are being developed showing such major features as a power modulation of at least 10:1, ultra low CO and NOx emissions over the entire power modulation range, significantly more compactness than conventional liquid fuel fired boilers and compatibility with renewable liquid fuels like FAME. In order to reach these goals new ceramic premixed liquid fuel burners were developed based on the combination of the innovative cool flame vaporization process and the novel porous medium burner concept. High temperature ceramics, condensing boiler technology with condense water neutralization and innovative burner controls with a power modulation were utilized, in order to realize all the principal advantages of the employed technologies. Keywords Cool flame vaporizer, Porous media combustion, Oil burners, Condensing boilers 1. Introduction The BIOFLAM project intends to provide solutions to the problem of environmental impact of combustion of liquid fuels for heating purposes. Oil burners show up to date a very poor power modulation especially at low power outputs, as usually needed in domestic appliances. Liquid biofuels like FAME are also not compatible with conventional oil burner technologies. Furthermore, the integration of oil burners in wall-hung systems requires further burner size reductions. Within the EC funded BIOFLAM project new liquid fuel fired condensing boilers are being developed showing the following major features: • power modulation of at least 10:1 • ultra low CO and NOx emissions over the entire power modulation range • significantly more compact than conventional liquid fuel fired boilers • compatible with renewable liquid fuels like FAME (based on rape-seed RME, sunflower SFME and used fried oil UFO) [13-14]. 47 In order to reach these goals new ceramic premixed liquid fuel burners were developed based on the combination of the innovative cool flame vaporization process and the novel porous medium burner concept. High temperature ceramics, condensing boiler technology with condense water neutralization and innovative burner controls with a power modulation of at least 10:1 were utilized, in order to realize all the principal advantages of the employed technologies. Combustion in porous, inert media offers exceptional advantages compared to techniques of free flame burners. The relatively new technology of porous medium burners is characterized by higher burning rates, increased flame stability with low noise emissions and lower combustion zone temperatures which lead to a reduction in NOx formation. Porous medium burners also show low emissions of CO and very small scale sizes. Additionally, complex combustion chamber geometries, which are not feasible with conventional state of the art combustion techniques, are possible. Research and development activities on stationary combustion in inert porous media started in the first decades of the 20th century [1, 2] and are still continuing up to the present time (see for example [3, 4, 5]). A novel combustion technique based on the combustion in porous media has been developed in the last years at the Department of Fluid Mechanics at the university of Erlangen [6, 7, 8]. The major novelty of this work is the combustion stabilization principle, which allows an extremely stable operation of the premixed combustion process in the porous matrix. The flame stabilization layer is placed inside of the porous matrix and is well defined by the matrix design. The most important criterion, which determines whether or not a combustion process can take place inside a porous structure, is its critical pore size. If the size of the pores is smaller than this critical dimension, flame propagation is prohibited; the flame is always quenched. On the other hand, if the pore size exceeds the critical dimension, flame propagation inside the porous structure is possible. Waste gas Heat transfer in the axial direction by radiation, conduction, dispersion and convection Heat transport for the stabilization of the combustion process Heat removal by radiation and conduction of the solid, conductive heat transfer of the gas phase and dispersion Large pores region (region C) Small pores region (region A) Region C Combustion zone Ignition temperature Region A Preheating zone Gas mixture (fuel and oxidant) Figure 1: Schematic setup of a porous burner Figure 1 shows the schematic setup of a porous burner with the preheating region A and the actual combustion region C. The critical pore size may be determined by a modified Péclet number. In the porous burner, the combustion process is stabilized with a sudden change of the pore size, corresponding to a change of the Péclet number inside the combustion reactor. In region A of the porous burner, the porous body properties are chosen in such a way that flame propagation is not possible. In region C, the pores are large enough so that flame propagation is possible. Combustion of liquid fuels like Industrial Gas Oil (IGO) is taking place after the evaporation procedure of the liquid fuel. In most cases the liquid fuel is atomized with a spray nozzle and mixed with the combustion air. In the resulting two-phase flow the evaporation/gasification of 48 the atomized liquid fuel is the first step before combustion takes place. The combustion heat release and the heat transport properties influence significantly the evaporation process. Because of these reasons the evaporation and the combustion process cannot be separated clearly. Because of insufficient spray quality and flame stabilization, commercial liquid fuel burners normally show a power modulation less than 1,4:1. The vaporizing and combustion zone are not clearly separated, so the system is sensitive to changes in temperature and flow field, which are arising with power rate modulation. A porous burner for liquid fuels like IGO should be operated with a clear separation between the combustion and the evaporation process. The concept of the cool flame vaporizer, which was developed at the Institute for Heat and Mass Transfer of the University of Aachen (ESTAachen), offers the possibility for a clear separation between the evaporation and the combustion process [9, 10, 11]. g a s te m p e ra tu re a fte r fu e l a d d itio n The main problem in producing a homogeneous mixture of air and liquid fuel is the tendency of autoignition during the vaporization due to the heat flux necessary to provide the vaporizing enthalpy. The cool flame vaporizer uses the internal heat production to vaporize the fuel. The slightly exothermic cool flame reactions cause an energy conversion of about 5% to 10%, so that it can be described as autothermal. 800 tR > 1 s 0 .6 s 0 .2 s 700 600 no re a c tio n c o o l fla m e a u to ig n itio n off gas 500 fuel 400 gas analysis 300 200 200 oxidizer 300 400 500 600 700 800 g a s te m p e ra tu re b e fo re fu e l a d d itio n in ° C Figure 2: Temperature evolution of IGO in a cool flame (p = 1bar) Figure 2 shows the temperatures before and after the fuel addition. Cool flames start at a temperature of 300° C and stabilize, virtually independently of the air ratio, at a temperature of 480 °C at 1 bar conditions. The final temperature is also independent of the initial temperature, which is the temperature at the start of fuel injection. The activation energy to reach autoignition is too high at 1 bar. This is due to reaction inhibition which leads to a constant temperature. 49 550 gas temperature ϑ in °C 500 450 final temperature n-heptane IGO n-oktane FAME 400 350 300 initial temperature 250 0 0,00 0,6 0,8 1,0 1,2 1,4 1,6 1,8 2,0 air ratio λ Figure 3: Start and end temperatures of cool flames for different fuel types The mechanism works for most hydrocarbons and their mixtures as demonstrated in figure 3, so that also renewable fuels like FAME can be applied. Because no heat exchanger is in direct contact with the liquid fuel there are no problems with crack processes. Soot will also not be formed. A combination of the cool flame vaporizer with the porous medium burner concept has already been realized in the past [12]. However the proposed concept in [12] proved to be very sensitive on the adjustment of the heat balance between cool flame vaporizer and porous burner. In contrast to the proposed concept of [12] in the BIOFLAM project a complete decoupling of the porous burner from the cool flame vaporizer was realized, resulting in a very robust operational behavior over the entire power modulation range. In the following paragraphs the concept of the BIOFLAM boiler and operational characteristics are presented. The research and development efforts are still in progress in the framework of a combined research and demonstration project financed by the European Commission. The heterogeneous consortium of the project partners includes all different necessary expertise for such a system development like fuel properties (OMV), boiler design (Hovalwerk), electronic controls (CSEM), ceramics (PTC), CFD (IST and NTUA), cool flame process (EST) and porous burners (LSTM). 2. Concept of the bioflam boiler unit Porous burner In the case of the combination of a porous burner with a cool flame vaporizer one has to face the increased temperatures of the incoming fuel/air mixture which should be maintained even in the flame stabilization region in order to prevent condensation and coking of the oil vapor. Thus, the stabilization principle and the applied materials of the porous medium burner had to be adapted and improved in order to fulfill the requirements of the cool flame vaporizer products. The design of the porous burner flame trap (Region A) was adapted corresponding to the expected conditions of the cool flame products. Materials with extremely low conductivity (ceramic matrix composites based on alumina fibers, < 0,2 W/mK) were applied. The flame trap faces temperature gradients up to 1000 °C/cm and has to show a very low effective 50 conductivity in the upstream direction, in order to prevent overheating and flashback. The flame trap was realized as a hole plate with holes of 1mm diameter. Flame detection sensor Zone A Zone C Ignition electrode Gas/gas heat exchanger Figure 4: Porous burner design and burner in operation The combustion region consisted of a silicon carbide (SiC) foam, developed by PTC, able to withstand temperatures up to 1650 °C and extreme heating and cooling rates. A special production process starting from a PU-foam precursor, coatings and with a final silicon infiltration and conversion of carbon particles to SiC in vacuum was applied. Cool flame vaporizer Although the cool flame process is an exothermal one, due to heat losses and due to the starting temperature level of the cool flame process at 300 °C, it was not possible to realize a cool flame vaporizer operating with the complete combustion air, without external preheating. In the development of the cool flame vaporizer mainly two aspects were significant. First the heat production of the cool flame reaction had to be maximized in order to achieve an autothermal operation mode. This can be accomplished, if the recirculation ratio increases by taking a higher pressure drop into account. On the other hand a marketable fan should be used for the BIOFLAM unit (pressure drop < 2500 Pa). Use marketable fan Maximize vaporizer heat production Reduce pressure loss Maximize recirculation ratio Figure 5: Contradiction between minimal pressure loss and autothermal operation mode Since one main objective for the vaporizer design was an autothermal operation, the air ratio at the vaporizer had to be sub–stoichiometric due to the recirculation ratio limits imposed by the available marketable fans. Thus a staged process was applied with a sub–stoichiometric operation of the vaporizer and subsequently mixing of the secondary air before entering the porous burner. The primary air ratio should not be too low, otherwise mixing with secondary air is difficult and possibly inhomogeneous. To avoid condensation in the mixing process the mixing temperature had to be higher than 250°C. For this purpose the cool flame heat production had to be be maximized. Figure 6 shows the heat balance for the cool flame 51 vaporizer. It can be seen that for a burner inlet temperature of 250°C a fuel conversion of minimal 11.8% for maximum burner power is needed. Heat losses app. 50 W Cool Flame product 250°C Oil 35°C Vaporizer Burner Flue gas Air 20°C Cool Flame Conversion: 2.3 kW burner power -> 13.8% 23 kW burner power -> 11.8% Figure 6: Heat balance of the cool flame vaporizer The maximal fuel conversion of the cool flame vaporizer was determined experimentally. Therefore temperatures at- in and outlet of the vaporizer were measured for the maximal possible air ratio with a stable cool flame. fuel conversion Cool Flame 16% 14% 12% 10% 8% 6% 4% conversion needed 2% conversion staging 2 0% 0 5 10 15 20 25 burner power in kW Figure 7: Fuel conversion of Cool Flame vaporizer As indicated in Figure 7 the fuel conversion was not high enough, in order to reach the desired temperature of 250 °C after mixing with the secondary air. To avoid condensation of the cool flame products the missing heat amount had to be introduced with the secondary air. For this purpose a heat exchanger for the secondary air was combined with the porous burner construction (see Figure 5). The overall vaporization and premixing process is shown schematically in Figure 8. λ prim = 0,4 primary air, 20°C cold flame products 400°C vaporizer Mix burner secondary air, 20°C λ sek = 0,8 preheater 270°C 200°C Figure 8: Staging concept of the cool flame vaporizer and premixing unit 52 3. Design of the BIOFLAM boiler unit In figure 9 the schematic diagram of the BIOFLAM unit is shown. The liquid fuel is entering the vaporizer through a spray nozzle. A fan is used for pressurizing the combustion air, which is split between primary and secondary air. The primary air enters the vaporizer through an annular gap around the injection nozzle, which was designed in order to maximize the internal recirculation rate in the cool flame vaporizer section. Recirculation is realized through the internal cylinder in the vaporizer section. The secondary air enters the burner section, is preheated and subsequently enters the mixing chamber and is mixed with the cool flame products. The complete mixture enters the porous burner at a temperature level of ca. 270 °C. The exhaust gases enter after the porous burner the condensing boiler, which utilizes the Hovalwerk multi-jet technology. Automotive high pressure injection nozzles were used in the BIOFLAM unit, in order to realize the high power modulation range with a good spray quality. The fuel oil flow was controlled by changing the opening time and frequency of the nozzle needle without a change of the oil pressure. A minimal opening time of 2 ms or a maximal frequency of 150 Hz was possible. Such nozzles are developed for operation with gasoline at a pressure of 10 MPa. For the BIOFLAM unit they were used with IGO and a pressure of 1 MPa. Due to that reason no data about the operation regime for this nozzle under these conditions was available and an experimental characterization of different nozzles was performed. Oil nozzle Bosch HDEV 67 ° Ignition electrode Flame detection Primary air vaporizer porous burner Cool flame Vaporizer condensing boiler Cool Flame Product Mixing chamber Secondary air Preheated secondary air Zone A Zone C Porous burner Gas/gas heat exchanger Exhaust Figure 9: Design of the BIOFLAM boiler unit Special attention was given on the starting procedure and the control aspects. During the burner start the vaporizer is used as a burner, until the unit reaches the proper operating conditions. New control strategies were necessary, in order to control the vaporizer and the 53 burner operation, especially during startup. Ignition electrodes were used in the vaporizer and in the burner section. Based on a control of the temperatures in the different sections of the unit, the conditions for switching from the starting mode to the stationary porous burner combustion mode were evaluated. In Figure 10 a schematic diagram indicates the major sensors and controls applied in the BIOFLAM unit. At the current development stage the control is realized with PC based modules. A robust microprocessor based control is under preparation for the next evolution stage of the unit. Figure 10: Schematic of the major BIOFLAM unit controls 4. Preliminary results and discussion The previously described concept was realized in 5 identical prototypes and first tests were performed with the BIOFLAM boiler prototypes. Photographs of the realized units can de seen in Figure 11. An important aspect during the preliminary tests was the temperature distribution inside the vaporizer over the entire power modulation range. The burner power was changed from 2.6 kW to 23.5 kW. The secondary air preheating was approx. 200°C. 54 Figure 11: Photographs of the BIOFLAM boiler prototype in operation In Figure 12 the temperature measuring positions in the vaporizer and the variation of the different temperatures over the power modulation range are shown. From high to low powers the temperature at T(rec2) increases while T(rec1) decreases. So it can be assumed that cool flame reaction in case of low power is finished locally earlier inside the recirculation gap or even before entering the recirculation gap. Nevertheless the cool flame reaction is stable for the whole modulation range. Consequently, the mixing temperature was above 250°C at any time. Thus, re-condensation of cool flame products before entering the porous burner section can be certainly excluded. 55 temperature in °C 500 450 400 350 300 250 200 150 100 50 0 0 2 4 6 8 10 12 14 16 18 20 22 24 burner power in kW T (air1) T (rec2) T (air2,heater) T (premix) T (air2) T (mix) T (rec1) T (wall) Figure 12: Temperature distribution over the power modulation of staged vaporizer In Figure 13 the emission characteristics of the first prototypes over the entire power modulation range are shown. In the diagram also emissions with a non-staged operation of the cool flame vaporizer with preheated air at 350 °C are shown (version 1) for comparison purposes. The non staged operation of the cool flame vaporizer needs a substantial air preheating, in order to avoid extinction of the cool flame. It is obvious, that the staged vaporizer concept (version 2) requires much less air preheating (only the secondary air is preheated at a much lower level of 200 °C) and results in significantly less nitrogen oxide emissions, due to the resulting reduced combustion temperatures, although a lower excess air ratio was adjusted. 56 Emissions [mg/kWh] 140 1st version: CO 2nd version NOx 2nd Version 120 preheating of the entire air T air,total = 350 °C Pvaporizer = 3.5 - 18 kW ; λ = 1,35 100 2nd version: CO 1st version NOx 1st Version preheating of the secondary air T air,sec = 200 °C Pvaporizer = 2.6 - 23 kW ; λ = 1,25 80 60 40 20 0 0 5 10 15 20 25 Power [kW] Figure 13: Emission characteristics of the BIOFLAM unit over the power modulation range The excellent emissions characteristic of the BIOFLAM boiler unit operating with a staged cool flame vaporizer is comparable to the emission levels of low emission gas burners, which represents a breakthrough for oil burners. 5. Conclusions and future work The developed burner and boiler unit for liquid fuels in the framework of the BIOFLAM project allows a high power modulation combined with a condensing operation mode at low emission levels. The good operational characteristics result from the combination of the cool flame vaporizer with the porous burner. Besides the low emission levels, the developed boiler also shows a higher overall efficiency, in comparison to conventional oil burners, because of the high power modulation and the condensing heat exchanger. The obtained results are very promising and further optimization work is undergoing, basically towards long term stability issues of the applied components, control strategy and safety issues. Extensive laboratory tests especially with different fuel qualities and mixtures with renewable fuels of the FAME type are already running and results are expected in the near future. A CE certification and a field test of 2 units under real conditions in selected households and of additional 5 units under laboratory conditions is under preparation. 57 Acknowledgments The contribution and financial support of the European Commission and the Swiss Federal Office of Education and Science under the contract No. ENK6-CT-2000-00317 are gratefully acknowledged. References [1] [2] [3] [4] [5] [6] [7] [8] [9] [10] [11] [12] [13] [14] Bone, W. A. Surface Combustion. The Journal of the Franklin Institute 173, No. 2: 101131, 1912. Lucke, C. E., Design of Surface Combustion Appliances. The Journal of Industrial and Engineering Chemistry 5, No. 10: 801-824, 1912. Martin, R. J., Stilger, D., and Holst, M. R. Method and Apparatus for Controlled Reaction in a Reaction Matrix, US Patent No. 5165884, 1991. Hsu, P. F., Howell, J. R., and Matthews, R. D. A numerical investigation of pre-mixed combustion within porous inert media, J. Heat Transfer, 115:744-750, 1993. Hackert, C. 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