REGULATION OF GAS COMBUSTION THROUGH FLAME POSITION

Abstract: Method for the regulation of a combustion system where the fuel-gas air mixture, which is from almost stoichiometric to strongly hyperstoichiometric, outflows from at least one flame opening of a premixed burner, with velocity and modalities such as to obtain a lamellar flame, substantially detached from the area of at least one flame opening; characterised by the fact that to maintain the flame around a prefixed optimum position, at least one of the three variable quantities of the mixture is varied: the value of premixture rate lambda , the outflow velocity, the temperature upstream the flame front.

Description: DESCRIPTION Regulation of gas combustion through flame position FIELD OF THE INVENTION The present invention relates to gaseous fuel combustion systems and in particular to a method and apparatuses in accomplishment of same, for controlling the combustion to obtain: flame stability, low emissions, in the most wide field of burner capacity modulation required in practice, even in feeding conditions with limit gases, in a so simple and practical way to be used also for apparatus with capacity of only few KW . The gas combustion system is the assembly of the burner with, the combustion chamber, the heat exchanger, the means for the circulation of air and exhausts, if existing, as well as the control apparatus with its sensors; more elements of the assembly can form a sole body therefore a distinction only possible for functions. The gas combustion systems are the main functional assembly of domestic and industrial appliances as central heating boilers, water heaters, of two main types: istantaneous and storage water heater, room heater and furnaces, gas cookers etc.. For burner it is understood the functional assembly of the parts which create the mixture of air and fuel-gas and make possible the outflowing of them in the combustion chamber through the flame openings. The invention applies in particular to fuel-gas combustion systems, where the mixture, formed by air, said primary air, and fuel gas (hereafter simply said mixture) is by approx. stoichiometric to strongly hyperstoichiometric (0.95 < λ < 1.6, where λ is the ratio between air actually present in the mixture and the air existing in the stoichiometric mixture of the same gas in the same conditions); flow in combustion chamber, out from the flame openings of the burners with substantially larninar flow, having an out flow velocity between 0.2 and 4.0 meter per second, and generates a lamellar flame, means of big surface and minimum thickness (magnitude order of a millimetre),this means that the ratio surface thickness is well over a value of ten, substancially detached from the area occupied by the flame openings; the flame front, that is the surface where the combustion starts, coincides with the flame itself being the combustion monostadium for the presence of all the necessary oxygen since the ignition and is from laminar to wrinkled. The invention applies to combustion systems with gas atmospheric burners but also with forced burners, where the air gas mixture is obtained, in the wanted flow and composition, with the help of auxiliary means (for example fans, or compressors) both types operate CONFIRMATION C0Pτ either with the presence of secondary air (called partially pre- ixed burners) or with only primary air (called totally pre-mixed burners). In all types of burners the mixture outflows from the flame openings with a velocity fairly higher to the flame speed so as to avoid that the flame adheres to the opening itself (flame substancially detached). In the combustion chamber the mixture ignited, at least initially, by suitable ignition devices, forms the flame which is kept in stability conditions from a sort of anchorage system, acting at least in some points. Opening configurations, in particular slots obtained in thin thickness sheet, so close to create an almost homogeneous sole jet of mixture are considered single flame opening. The front of flame is recognisable because it emits in the visible, even if the specific maximum emission due to OH and CH ions is respectively in the wavelength between 305 and 320 mm and around 431.5 and 438 mm. BACKGROUND OF THE INVENTION A problem of the apparatuses of the kind discloses in the preamble of claims 1 and 2 arises when instead of the standard fuel-gas for which the apparatus is set, a fuel-gas from the same family as said standard fuel-gas but prone on flame blow-off or prone to flash back are fed. Specifically, the burner flame openings surface may attain critical temperature value, and in some other occasion, the flame may become unstable, resulting in poor combustion of fuel-gas. A method, applicable to highly premixed but only atmospheric burners, to maintain stable the temperature of the flame openings and reduce the harmful emissions by the variation of - λ - in the mixture according to the temperature of the flame openings itself is described in the European patent of the author EP0606527A1 deposited on 16 August 1993, but don't take into consideration the flame, its position, shape or density, particularly is not considering a lamellar flame detached from the area of the flame openings. It is also known a method described in patent DE3630177 dated 4 September 1986 where thesignal of the ionisation current, inside the large volume of a turbulent flame, is used for the variation of - λ - nevertheless it is a signal relating to the combustion conditions inside the big volume of the turbulent flame itself, not of the ionisation conditions of the unburned mixture just upstream the flame front, so at conditions prior to the combustion. This signal is typical of the combustion conditions, specifically as to the limit of stability for the turbulent combustion, don't give any information about the position of the flame front or the flame distance. Furthermore the considered emission of UV, without description of how it is and how it can be used, would seem to determine the combustion condition as to the limit 85 of the stability for turbulent combustion. Control systems which vary the total quantity of air or of primary air basing itself on a temperature in combustion chamber, on the excess of air in fuels, either combined or not with air variation according to the flow rate of fuel-gas fed, are known. However none of these take into 90 account the influence of gases different from the standard one which can be distributed in sequence without notice and therefore feed the combustion system, nor can they maintain the stability of the flame in large ranges of capacity modulation, nor take into account the combustion of a hyperstoichiometric mixture in substantially laminar 95 flow, particularly with lamellar flames. These latter control systems and similar ones are complex, in particular for the type and positioning of the sensors, consequently, too expensive for gas appliances of flow limited to even few KW. None of the previously considered control systems are taking into 100 account the temperature as well the outflow velocity of the mixture. DISCLOSURE OF INVENTION The aim of this invention is to provide a method and apparatuses in fulfilment of same, for the control of the flame position driving the 105 value of at least one of the variable quantities characteristic of mixture outflowing from the flame openings into the combustion chamber: -λ, the velocity, the temperature; in eliminating the foresaid difficulties it makes possible the proper regulation also in very compact combustion systems, even forming a sole body. 110 This aim is reached by applying the method so that, having a method for the regulation of a combustion system where the fuel-gas air mixture, wich is from almost stoichiometric to strongly hyperstoichiometric, outflows from at least one flame opening of a premixed burner, with velocity and modalities such as to obtain a 1 15 lamellar flame, substantially detached from the area of at least one flame opening; characterised by the fact that to maintain the flame around a prefixed optimum position at least one of the three variable quantities of the mixture is varied: the value of premixture rate λ, the outflow velocity, the temperature upstream the flame front. 20 It is possible to define the position of the flame as the distance between the barycenter of the flame front and the surface of at least one flame opening which generates this front, hereafter said quantity will be called flame distance. The flame distance optimum value can generally be predetermined 125 arbitrary constant, but can have different values according to the fuel- gas flow rate; in any case, during the on periods on the combustion system, the istantaneous ratio, which is the detected flame distance/optimum flame distance, have the value -1- for the reached conditions considered as optimum, values over 1 show the tendency to 130 the flame blow-off increasing as the ratio increase, values under 1 show the tendency to overheat the burner head (means the flame openings zone) increasing as the ratio decrease. The istantaneous ratio: detected flame distance/optimum flame distance, will be hereafter called flame ratio. 135 Particularly convenient to obtain the regulation desired at least one of said variable quantities of the mixture is varied according to the flame ratio as per following modalities: - the λ premixture value is varied between a prefixed rninimum and maximum value according to the flame ratio, causing a flame ratio > 1 a 140 λ decrease and vice versa; - - the outflow mixture velocity is modified through the variation of the outflow cross section of at least one flame opening, between a minimum section and a maximum one, according to the flame ratio, causing a flame ratio > 1 an outflow section increase and vice versa. 145 - the temperature, of the mixture outflowed from at least one flame opening, between a prefixed minimum and maximum value, is varied, upstream the flame front, according to the flame ratio, causing a flame ratio > 1 a mixture temperature increase and vice versa. The regulation method of the invention can detect the quantity 150 indicative of the flame distance, through the position of the radiation source in the different frequencies of the flame itself, through the temperature detected at least upstream the flame front and in the immediate proximity of said front and through the ionisation current measured at least upstream the flame front and in the immediate 155 proximity of said front at least in average value. In a first variant, the value of the premixing rate - λ - is changed between prefixed minimum and maximum values according to the flame ratio, causing a flame ratio > 1 a λ decrease and vice versa, so as to maintain said flame distance around a given value, except for 160 different regulation during temporary periods, for example during the starting, when needed. In particular in case of use of a sole fuel-gas and with constant cross- section of the flame opening(s), the prefixed maximum and minimum values are corresponding respectively to the minimum flow and 165 maximum flow of the burner. It is also provided a simplified regulation, at steps, which varies - λ - between a minimum value and a maximum one if said flame distance either decreases or increases respectively. A modified regulation can provide, at ignition, to increase the flame 170 speed that otherwise would be too low, a mixture temperature increase obtained with heat transfer to the mixture brought to such a value to obtain the first and the cross-ignition, the heat transfer can remain as such for a determined period, for example for 10 seconds, or for wall temperatures of the flame opening below a given value. 175 By adopting the variation of the - λ - value in mixture, as described, if the composition of the fuel-gas feeding and/or the temperature of the mixture and also the cross-section of the flame opening(s) do not change, variation of outflow-velocity of the mixture remains in reduced limits, for the reasonable range of burner modulation, with small 180 movement of the flame front, even without any further regulation. In a second variant a basic value of - λ - is defined in linear relationship to the fuel-gas flow rate, detected through the fuel-gas injector pressure, corrected, between prefixed minimum and maximum deviation, according to the flame ratio, different regulation during 185 temporary periods, for example during the starting, is provided, when needed. In a third variant, to enlarge the capacity modulation field of the combustion system even to a modulation ratio 1/10, besides the - λ - variation as per above first variant, the outflow velocity of the mixture 190 is maintained almost constant by changing the cross section of at least one flame opening according to the instantaneous flow-rate of gas anyhow detected (for example by using the flame density) . Where the flame density is the specific concentration of the combustion and, if other parameters do not change, is index of the instantaneous gas flow 195 rate. In a fourth variant, together with the regulation as per first variant, it is also possible to vary the outflow velocity of the mixture from the flame openings, according to the temperature of the openings(s) by reducing the section at the increase of the temperature and vice versa. 200 In all the previous variants, changes of the conditions of the flame stability at constant fuel-gas flow rate, due to a modification of the flame speed for the change of the composition of the gas employed and/or of the temperature of the mixture (for example: for temperature changes of the inlet air), cause a deplacement of the flame front, and, 205 because the relation between λ and the flame position, a correction of the - λ - value is obtained such as to restore the stability conditions of the flame. At ignition, in order to improve the stability conditions, the λ value is the mimmum provided and can stay as such for a fixed period, for 210 example for at least ten seconds, or for wall temperatures of the flame openings below a certain value, for example around 200°C, then modifying itself according to the flame position . A fifth variant of the method provides that the outflow cross-section of the flame opening/s is varied according to the flame ratio, between a 215 minimum and a maximum cross-section, causing a flame ratio > 1 an outflow section increase and vice versa, so as to maintain the flame distance around a pre-fixed value, except for a different regulation during the transient periods, for example of starting, when needed. A simplified regulation which, according to the flame ratio, varies the 220 outflow cross-section of the flame openings between a minimum value and a maximum one, in one or more steps, opening or closing one or more flame openings if said flame ratio increases or decreases is also provided. By adopting the flame ratio, or any variable quantity which follows the 225 same variation law, as control-parameter for the variation of the outflow cross-section of the flame opening/s, it is possible to reduce at the minimum the variation of the outflow velocity at the change of the burner capacity by maintaining the flame stable and the emissions reduced. 230 If the composition of the feeding gas and/or the temperature of the mixture do not change, in particular in atmospheric burners, through the continuous variation of the mixture outflow velocity, as previously described, the value of λ in the mixture itself is maintained in reduced limits, in a range of burner capacities, favourably keeping almost fix the 235 flame front, without any fiirther regulation. Changes of the stability conditions of the flame at constant burner capacity, due to variation of the flame speed for the change of λ and/or of the composition of the feeding gas and/or of the mixture temperature, cause a correction of the outflow cross-section, such as to 240 favour the restoration of the stability conditions of the flame, that means increase of the outflow section in case of decrease of the flame speed and therefore tendency to the blow-off of the flame, the opposite if said speed increases that means a tendency to the overheating of the surface of the flame opening/s. 245 When the burner is in off condition the cross-section of the flame opening(s) can be the maximum possible and can remain as such for a pre-fixed period, for example for approximately ten seconds, during the ignition phase, then modifying according to the regulation law. Otherwise in order to improve the stability conditions in transient 250 periods, the modifications of the outflow cross-section can't happen for temperatures of flame openings below a pre-fixed value, usually around 200°C, to obtain an outflow velocity of the mixture lower than the one provided at steady state. Sixth variant: at the ignition, modifying the fifth variant, the flame 255 speed can be increased through the increase of the mixture temperature, obtained with heat transfer to the mixture, brought to such a value to obtain the first and the cross-ignition; after the ignition, the heat transfer can remain as such for a deteπriined period, for example for 10 seconds, or for wall temperatures of the flame opening below a given 260 value, then will change to drive the mixture temperature according to the variation of fuel-gas flow rate. Seventh variant: since it has been surprisingly noticed that, in a reasonable range of working conditions, the wall temperature of the flame opening/s or of a body in its immediate vicinity, varies with a law 265 comparable to that of the variation of the flame distance, also the temperature of these bodies compared to an optimum value, according to the invention, can be used as regulation parameter of the outflow cross-section of the flame opening/s variation, by detecting it with thermocouples, thermistors or other. 270 By increasing the temperature of the flame openings compared to a predetermined value, the method of the invention decreases the outflow cross-section tending to restore the lost equilibrium, by decreasing the temperature ratio it increases said cross-section, when the burner is in off condition the outflow cross-section is the maximum provided. 275 Controlling in this way the mixture outflow velocity, the temperature of the zone of the flame opening/s it maintains, within acceptable limits (even below 500°C), the flame stable the emission low, in a reasonable range of burner flow modulation and of kind of feeding gases. On the eighth variant: the value of the temperature of the mixture 280 upstream the flame front is varied according to the detected flame ratio, causing an increase of the flame ratio an increase of the temperature and vice versa, so as to maintain said flame distance around to a given value, except for different regulation during temporary periods, for example during the starting, when needed. 285 It is also possible a simplified regulation, on-off, wliich increases the temperature to a maximum one if said flame ratio increases over a predetermined value and during the starting periods. By adopting either the flame ratio, or any quantity which follows the same variation law of the flame position, as control-parameter for the 290 variation of the mixture temperature, if the composition of the fuel-gas, and/or λ in the mixture and also the cross-section of the flame opening(s) do not change, for the complete range of burner capacity modulation, small movement of the flame front are obtained, even without any further regulation because to a variation of outflow velocity 295 is opposed a flame speed variation in opposite direction. Changes of the stability conditions of the flame at steady state due to variation of the flame speed for the change of -λ- and/or of the composition of the feedgin fuel-gas cause a correction of the value of the temperature of the mixture, such as to favour the restoration of the 300 stability conditions of the flame, that means temperature increases in case of decrease of the flame speed and therefore tendency to the blow- off of the flame, the opposite if said speed increases that means a tendency to the overheating of the surface of the flame openig/s. Ninth variant : It is however possible to enlarge the flow modulation 305 field of the combustion system if, besides the regulation as above foreseen, either - λ - or the outflow velocity of the mixture are varied according to the instantaneous fuel-gas flow-rate, anyhow detected, almost constant - λ - slightly decreasing the outflow velocity by an increase of the gas flow rate and vice versa; acting so the capacity 310 modulation ratio can even go up to of 10/1, . Tenth variant the method of the invention carries out the temperature variation associated with the variation of the λ value in the mixture or its outflow velocity, all variating according to a quantity, index of the flame ratio as previously described. 315 Eleventh variant Associated with the temperature variation also it can be varied the outflow velocity of the mixture from the flame openings, according to temperature of the openings decreasing the section by increasing the temperature and vice versa. At ignition to increase the flame speed that otherwise would be 320 sometime too low, the heat transfer to the mixture can be brought to the maximum value provided to obtain the first ignition and cross-ignition, can remain as such for a determined period, for example for 10 seconds, or for wall temperatures of the flame opening below a given value, for example around 200°C, then be reduced to obtain the 325 temperature of the mixture according to the flame ratio. By using any variant of the described method, the temperature of the outflow zone of the mixture remains within acceptable limits (even below 400 °C), at any flow condition of the burner, type of feeding gas, temperature of the inlet air the flame remain stable, the harmful 330 emissions are reduced to nrinima values. BRIEF DESCRIPTION OF THE DRAWINGS In order to better understand the invention, its characteristic and the advantages it provides, few embodiments thereof are described 335 hereinafter, by way of non limitative example and with the assistance of the appended drawings, in which - Table 1/9 shows a combustion system with totally premixed atmospheric burner, forced draught, λ variation according to the flame distance, fig. 1 is a general scheme, fig. 2 detail of the by-pass, fig. 3 340 view of the flame openings. - Table 2/9 shows a combustion system with totally premixed forced burner, λ variation according to the flame ratio and to the instantaneous air flow rate. fig. 4 is a general scheme, fig. 5 view of the flame openings, fig. 6 detail of the air-gas regulation. 345 - Table 3/9 shows a combustion system with atmospheric burner partially premixed, natural draught, λ variation according to the flame ratio and variation of the outflow velocity according to the temperature of the flame opening, fig. 7 is a general scheme, fig. 8 detail of a flame opening, fig. 9 detail of the λ regulation system with a sliding sleeve 350 around the fuel-gas delivery nozzle . - Table 4/9 shows a combustion system with atmospheric burner, forced draught, λ variation according to the flame ratio and outflow velocity according to the fuel-gas flow rate, or vice versa, fig. 10 is a front view, fig. 11 a side view, fig. 12 a cross section of a flame 355 opening. - Table 5/9 shows two combustion systems with atmospheric burners, one with natural draught the second with forced draught, variation of the outflow velocity according to ihe the temperature of the flame opening fig. 13 shows a view in vertical cross section of a natural draft 360 combustion system with variation of the outflow cross section according to the temperature of the exit area of the flame openings using bimetallic strips, fig. 14 shows an enlargement of a flame opening of fig. 13; fig. 15 shows a view in vertical cross section of a forced draft combustion system where a bulb according to the reached temperature modifies the outflow cross section of flame openings fig. 16 shows an enlargement ofa flame opening of fig. 15. -.Tav 6/9 shows a burner of the extractible type with variation of the outflow cross section according to the temperature of the exit area of the flame openings using bimetallic strips fig 17 shows a burner in longitudinal view with a single flame opemng interrupted by bimetallic U formed bridges which by tightening the lips of the flame opening modify its cross section, fig 18 shows the same burner without the flame to a better comprension of the ecanism and fig. 19 shows a cross section ofa slightly different burner -.Table 7/9 shows in fig.20 a combustion system with variation of the mixture temperature according to the flame ratio; the mixture is heated by a wire heating element positioned in the combustion chamber, covering its plan with mesh, fig. 21 shows an enlarged plan view of the burner head. - Table 8/9 in fig. 22 shows a pressurised combustion system with variation of the mixture temperature according to the flame ratio and where λ is maintained steady at the changing of the instantaneous fuel- gas flow rate; the mixture is heated by a heating element inside the burner, in fig.23 shows a forced draught combustion system with variation of the mixture temperature and of λ according to the flame ratio, the mixture is heated by a heating element which acts also as fluids dynamics obstacle. - Table 9/9 shows a forced draught combustion system with variation of the temperature and of the outflow velocity of the mixture according to the flame ratio, the mixture is heated by a heating element downstream the flame openings which also acts as fluids dynamics obstacle. DETAILED DESCRIPTION OF THE INVENTION Fig. 1 shows, in vertical cross section A-A a combustion system operating in forced draught with the fan 4 working at constant spin velocity mounted downstream the heat exchanger 2 so the inside of the shell 5 is in depression compared to the outside. The burner 8B, the body of which is bottom part of the shell 5, is atmospheric, the air-fuel gas mixture is obtained in a Venturi type tube IOA from the fuel gas exiting the injector 23 and the air from outside the shell 5 entering the mouth 9A. Under the vacuum created by the fan in the combustion chamber 3 with respect to the region outside the shell 5 the mixture is drawn through the Venturi 10A and the mixing chamber 18 to the flame openings 7A,better described in fig. 3, obtained on the sheet metal, for example, of 0.4-0.6 mm thickness, of the burner head 6. The flame openings 7A, made of a row of slots each, are spaced centre to centre from 15 to 60 mm to obtain a flying carpet type lamellar flame 19 anchored to external obstacles 12A, visible in V shaped cross section with upstream vertex and centreline of the V, peφendicular to the surface and in centre of the flame openings, parallel to the rows and distant to the slot surface from few to some ten mm according to the cases. The lamellar flame covers the plan of the combustion chamber 3, lying at level of the optical sensor 14B. The process controller 15 varies the gas flow through the valve 11, according to the heat request and varies λ in the mixture, acting through the by-pass 24 better described in fig.2. The open cross section of the by-pass 24 varies with the rotation due to a step by step motor 25, the more is opened the by pass the lower value of λ is obtained. The process controller 15 act positioning first the by- pass 24,to obtain the minimum value of λ to facilitate the ignition, then, after some ten seconds, changing the by-pass position, according to the flame ratio, an increase of the flame ratio causing a decreasing of -λ - and vice versa, in order to maintain flame distance around a pre-fixed optimum value. Using a different process controll the process controller 15 can also act in a different way: first positioning the by-pass 24,to obtain the minimum value of λ to facilitate the ignition, then after some ten seconds positioning the by-pass 24 to obtain a predeteπnined value of λ related to the instantaneous fuel gas flow rate, but changing the by- pass position to obtain a λ deviation between a pre-fixed minimum and maximum, according to the flame ratio. The optical device 14B, based on photo sensor/s, transmits to the process controller 15 one signal corresponding to the detected position of the flame compared to a pre-fixed position, means the flame ratio, and another one proportional to the intensity of the flame radiation, in particular proportional in the radiation frequencies characteristic of OH, CH, C2 radicals. According to the heat request the controller 15 vary the instantaneous fuel-gas flow rate by a valve 11 with variable opening, and controlled using the radiation intensity measured by the optical device 14B; the λ value is varied by the by-pass position according to the fuel gas flow, verified by the radiation intensities of OH and C2 compared between them or with total radiation. The flame position can be detected with a single photosensitive element through the oscillation of the optical system with known frequency and amplitude. In fig. 2 is described the air flow through the by-pass 24, constituted by a cylinder with closed heads whose vertical rotation axis 24B lies on the surface of the shell 5 side wall where a window 24C is open, above the heat exchanger 2, with lips towards the inside 24D. 450 The cylinder side surface being removed for less than 180°; rotating the cylinder anticlockwise, from a nil passage position (wall closed 24E at the outside of the shell 5) we arrive with a rotation of about 120° to a maximum open passage (as in figure), the shape of the opening 24A is such to obtain an air flow into the shell 5, proportional to the rotation 455 angle, in order to simplify the λ variation; for maximum gas flow the passage is almost closed, for minimum gas flow open as in figure, in ignition phase the opening is greater than what requested at steady state for the corresponding gas flow, staying in this position for example from 10 to 30 seconds. 460 Fig. 3 is a top view B-B in two levels, of a part of the burner's head 6, two flame openings 7A are represented, made of two rows each of parallel slots having width from 0.5 to 0.75 mm and length from 5 to 15 mm, parallel adjacent on the long side, spaced centre to centre from 0.9 to 1.5 mm. 465 Fig. 4 shows, in vertical cross section, a combustion system 1 with a heat exchanger 2, a combustion chamber 3, a fan 4 for the air gas and exhausts circulation, put upstream the combustion chamber for which this is in over pressure compared to the outside of shell 5, whose inferior part together with the burner head 6 forms the burner 8B body; 470 flame openings 7 A better described in fig. 5, are lengthened, perpendicularly to the drawing surface, formed by two rows of slots each, punched on the sheet metal of the burner head 6 . The lamellar flame 19, ignited by a device not in the figure, generates and remains firmly anchored downstream of the flame openings 7A becoming alike 475 a wave shaped flying carpet. The fuel gas valves 11 and 11 A (better analysed in fig. 6)and the fan 4 speed are operated by the process controller 15 according to the signals transmitted by the ionisation current sensor 14A positioned in the volume just upstream flame 19. The sensor, in this case a two 480 electrodes one, but could have more if needed to enlarge the area under control and have a better definition, transmits the signals which the process controller 15 works out to obtain the average ionisation current values wliich define the flame distance according to a pre-fixed value, and to obtain amplitude and frequency of oscillation which together 485 with average current value define the flame density, indicator of fuel gas instantaneous flow rate which is used as feedback in the process control. Fig. 5 shows, from top view, a part of the head burner 6 with three flame openings 7A, obtained from slots pimched on thin sheet metal, 490 each made of two rows 7AI and 7AII of parallel slots having width from 0.5 to 0.75 mm length from 5 to 15 mm being adjacent on the long side, spaced centre to centre from 0.9 to 1.5 mm obtained from sheet metal of 0.4-0.6 mm thickness, which leave in between an unpunched strip 12C,as an example, the 12C width is between 2 and 6 mm.The 495 fluids dynamic obstacle 12C generating downstream a stagnation area, anchors the flame, the openings 7A being parallel double rows close enough, having centre to centre distance from 30 to 120 mm( according to the slots length), generate a wave shaped carpet lamellar flame (19 in fig. 4) with depression on the vertical of 12C peak half between two 500 adjacent openings 7A. Fig. 6 is an enlarged section of the air-gas regulation system of fig. 4 where I IA is the on-off valve which allows the fuel-gas to enter the membrane device 26. Inside the device the menbrane 26B balances the PA pressure upstream the diaphragm 27 of the air exiting the fan 4, 505 trasmitted through tlie connection pipe 26C, with the PG pressure of the fuel-gas exiting the device 26. The fuel-gas then goes through a variable flow valve 11 downstream wliich the fuel-gas pressure value becomes PGF<PG , the pressure value PGF determines the instantaneous fuel gas flow rate. 510 The variation of the heat request causes a variation of fan spin velocity, therefore a different air flow rate, a different PA1 pressure and a consequent PG1 pressure equal to PA1, without tlie valve 11 presence λ would remain steady during all the modulation range; the valve 11 intervenes to modify λ following the input formulated by 15 according 515 to tlie flame ratio detected by 14A, modifying in PGFl the pressure upstream injector 23 therefore the fuel gas flow rate and consequently λ in the mixture, between a fixed minimum and maximum deviation, causing a flame ratio increase a λ decrease and vice versa, in order to maintain said flame distance around a pre-fixed optimum value. 520 In the ignition phase the valve 11 is completely open to maintain a λ value lower for a certain time. The fig. 7 shows a natural draught combustion system which employs an atmospheric partially premixed burner 8A of the extractible type, lip shaped flame openings 7B (perpendicularly lengthened to the drawing) 525 on burner head 6 and internal fluids dynamic obstacles with V shaped cross section, made from bimetallic sheets. Being the centre distance among exits 7B big, the flame, ignited by a device not seen, divides itself in long separate V shaped lamellar flames 19A (perpendicularly lengthened to the drawing). The process controller 15, upon signal of 530 flame ratio from the temperature sensor 14C through step by step motor 25 varies the primary air flow as better described in fig. 9. Moreover a thermocouple 16 put on a flame opening lip 7B1 allows to maintain at the minimum the λ value in ignition until the lip temperature has not reached a value of let's say 150°C. 535 At the same time, as described in the enlarged section of a flame opening 7B of fig. 8 the internal bimetallic sheet V shaped obstacle, according to the temperature reached changes the cross section of the opening 7B therefore changing the outflow velocity so to favour the stability.For higher temperatures (continuous line) smaller cross 40 section, the contrary (dashed line) for lower temperatures. In fig. 9 is shown how the rotation of the eccentric axis 28 varies the pπmary air flow to the Venturi through 9A moving the sleeve sliding on the gas injector 23 to maintain steady the flame position with the λ variation as often described. Two positions of the sleeve regulating λ in 45 the mixture are displayed: continuous line for maximum λ, dashed line for minimum λ . In the combustion system of fig. 10 the fan 4 is downstream the exchanger 2, the burner, with a Venturi tube IOA, is atmospheric totally premixed, (nevertheless passages for secondary air among the 50 openings 7B can be provided). The flame openings 7B are lengthened, perpendicularly to the drawing surface, and made from lips obtained with the sheet of burner head 6. On the centre line axis of the flow from openings 7B, in combustion chamber 3, at a distance which can reach ten times the flame opening width are put V section fluids dynamics 55 obstacles 12A with vertexes upstream wliich cause stagnation downstream having the dimension peφendicular to the axis of the same magnitude of the flame openings 7B width which, in this case, can be between 2 and 4 mm, while the lips height can vary from 10 to 20 mm; the obstacles have the same length of the flame openings 60 peφendicularly to the drawing. The flame 19, ignited by a device not seen, stays steadily anchored downstream the obstacles 12A becoming wave shaped caφet as the flame openings are close enough to each other. A variation of the heat request causes a change of the valve 11 opening, the fuel-gas flow rate is controlled by the warm wire sensor 29 which sends a signal to 15 to modify the eccentric axis 28 position driven by the step by step motor 25 which moves the external obstacles 12A to modify the flame openings cross section 7B so as to maintain almost constant the velocity of tlie mixture outflow At the same time the fan 4 spin velocity is modified by the process controller 15 according to the signal of the flame ratio detected by the optical sensor 14B so that the λ variation in tlie mixture maintains the flame distance at the best position as already described. Fig. 11 is a view from A-A section of fig. 10, the obstacles 12A balanced on the springs 30 pressed at the centre by the eccentric axis 28 which can move them, each other parallely in a vertical way to modify the cross section of the flame openings 7B of fig. 10 as better seen in the section of fig. 12 where these obstacles are in intermediate position (continuous line) and in reduced passage position (dashed line) The same combustion system of fig. 10, 11, if the case with unimportant changes, but using a different controll process with a different controller device can be regulated in this new way: the signal of the fuel gas flow rate from the warm wire sensor 29 is worked out from the process controller to vary the value of λ according to the said flow rate by changing the fan spin velocity as well described previously. the signal of flame ratio transmitted from the optical sensor 14B is worked out from said controller to change the eccentric axis 28 position driven by the step by step motor 25 which moves the external obstacles 12A to vary the flame openings cross secion 7B so as to modify the mixture outflow velocity to maintain the flame at the best position according to the flame ration variation law. The movement of the external obstacles 12A is either upwards or downwards whether the flame ratio 19 rises or lowers itself, the movement can be gradual, or on-off, up to closing the flame openings according to the needs. In fig. 13 is shown a natural draft combustion system with partially premixed atmospheric burners of extractible type 8A; a spark ignition device 13 which at the start, ignite the mixture out flowing from flame opening of left burner to form a first V shaped lamellar flame 19A wliich cross-ignites the other burners 7B creating similar flames remaining sparate. It is also shown, but more detailed in fig. 14, how a temperature sensor 17A of the flame opening lips, which corresponds, in a reduced modulation range, to a flame distance sensor, can also be 605 the actuator of the movement, able of modifying the outflow cross section directly, as mobile part 7B2 of the flame opening which has fix lips 7B1; in fact the two bi-metallic sheets, which occupy longitudinally all the flame opening where they are mounted, are coupled together by longitudinal welding at the low edges so that, heating themselves the 610 upper edges, symmetrically spread as regards to the central axis of the flame opening itself, as per dashed line in fig. 14. These sheets at room temperature are pre-charged in order not to move away the upper edge until the temperature of same does not reach approx. 150°C. In fig. 15 is shown a forced draught combustion system with partially 615 premixed atmospheric burner; and in more details in fig.l 6 is shown the temperature sensor 17B of the flame opening 7B, which is, in a limited range, equivalent to a sensor of the flame distance, is also actuator of the movement able of modifying the outflow cross section directly, as mobile part 7B2 of the flame opening 7B, in this case is a sealed bulb 620 seensor 17B, filled with a fluid, which expand at the temperature increase and shrinking at its decreasing, its upper lips 7B2 which are part of the flame opening 7B with fix lips 7B1 , makes directly change the outflow cross section of said openings. In fact the expansion or contraction of the fluid in the bulb can modify 625 the transverse section of this to directly modify the outflow section. In fig. 17 is shown a burner 8A with a sole flame 19A in fig. 18 the same buner is shown without the flame, tlie opening 7B having only two mobile lips 7B2, wliich define the outflow cross section of it, moved by the deformation (temperature function of the flame opening 630 and therefore of tl e flame distance) of two bimetallic sensors-actuators 17 A. The lips 7B2 position full line drawn and the dashed drawn one correspond to two different conditions of the flame opening temperature obviously higher the one corresponding to the dashed line. An external fluids dynamics V shaped obstacle positioned with the 635 central axis on centeφlane of the burner at a distance from the flame opening edges of 3 to 10 times the width of the flame opening with a cross dimension of tlie same magnitude of said width, anchors the large V shaped flame.fig. 19 shows a cross section of a slightly different burner. 640 In fig.20 is shown a natural draught combustion system with atmospheric burner having a head 6 in perforated sheet metal the variation of the mixture temperature is realised according to the flame ratio, detected by a ionisation current sensor, capable to detect the average value of the ionisation current, in three different positions using 645 three electrodes on different levels and distance from the nearest flame opening, so that by any fuel gas flow rate, at least one electrode will detect the ionisation current upstream tlie flame front, a net made of parallel ceramic rods 22 in one direction and wires heating element peφendicularly, covering the combustion chamber plan said wires if 650 under a predeterminated electrical tension are heated to a temperature around 1000°C; therefore are capable to ignite the mixture. In case the wires are organised in more than one circuit, 20el and 20e2 acting also as part of the fluids dynamic obstacle, as shown in fig.21, after the ignition the variation of the mixture temperature, obtained upstream the 655 flame front,can vary by steps; fig. 21 shows an enlarged plan view of the burner head, slots parallel each other combined in groups of three and four, these said groups (the flame openings) are distributed in a check pattern to obtain a flyng caφet shape lamellar flame 19 of fig.20. In fig. 22 shows a pressurised combustion system 1 (the fan is 660 upstream the combustion chamber 3), the heat request produces a variation of tlie fan 4 spin velocity, consequently a variation of the air pressure Pa = Pg means fuel gas low rate, mantaϊning λ constant at the changing of the instantaneous fuel-gas flow rate; the variation of the mixture temperature up stream the flame front 19 according to the 665 flame ratio detected by the ionisation sensor 14A, which works as that of fig.20, worked out from the controller 15 changes the electric input to the heating element 20i which never reaches such temperatures to risk the ignition of the mixture inside the burner chamber 18; the wave caφet type flame pattern is obtained with a series of twings rows of 670 slots forming openings 7B having obstacles 12C, the ignition device is not shown. In fig.23 is shown a forced draught combustion system using an optical device to detect the flame ratio as to permit to the controller 15 the variation of the mixture temperature and of λ(as in fig 1,2,3) according 675 to said flame ratio; the mixture is heated by a heating element 20i which acts also as fluids dynamics obstacle, V shaped, made of special steel sheet metal, punched as shown in fig.27, supported by a ceramic rod; the slots punched on the sheet metal head 6, organised in rows near each other, together with the V shaped obstacle produce caφet 680 lamellar flame. In fig.24 and 25 is shown a forced draught combustion system 1 with variation of tl e temperature and of the outflow velocity of the mixture according to the flame ratio; the mixture is heated by a heating element downstream tlie flame openings which also acts as fluids dynamics 685 obstacle as in fig. 23 moved up and down to vary the outflow velocity of the mixture as in fig 10, 11, 12 but using as control parameter the flame ratio as the temperature variation. Although the foregoing invention has been described in some detail by way of illustration and example for puφoses of clarity of 690 understanding, it will be obvious to those skilled in the art that certain changes and modifications may be praticed without departing from the spirit and scope thereof as described in the specification and as defined in the appended claims.

Claims: CLAIMS 695 1. Method for the regulation of a combustion system where the fuel-gas air mixture, wich is from almost stoichiometric to strongly hyperstoichiometric, outflows from at least one flame opening of a premixed burner, with velocity and modalities such as to obtain a lamellar flame, substantially detached from the area of at least one 700 flame opening; characterised by the fact that to maintain the flame around a prefixed optimum position at least one of the three variable quantities of the mixture is varied: the value of premixture rate λ , the outflow velocity, the temperature upstream the flame front. 2. Regulation method as per claim 1 characterised by the fact that at 705 least one of said variable quantities of the mixture is varied according to the flame ratio as per following modalities: - the λ premixture value is varied between a prefixed minimum and maximum value according to the flame ratio, causing a flame ratio > 1 a λ decrease and vice versa; 710 - the outflow mixture velocity is modified through the variation of the outflow cross section of at least one flame opening, between a minimum section and a maximum one, according to the flame ratio, causing a flame ratio > 1 an outflow section increase and vice versa. - the temperature, of the mixture outflowed from at least one flame 715 opening, between a prefixed minimum and maximum value, is varied, upstream tlie flame front, according to the flame ratio, causing a flame ratio > 1 a mixture temperature increase and vice versa. 3. Regulation method according to either claim 1 or 2 characterised by the fact that the quantity detected, indicative of the flame distance, is 720 the position of the radiation source in the different frequencies of the flame itself. 4. Regulation method as per either claim 1 or 2 characterised by the fact that the quantity detected, indicative of the flame distance, is the temperature detected at least upstream the flame front and in the 725 immediate proximity of said front. 5. Regulation method as per either claim 1 or 2 characterised by the fact that the quantity detected,indicative of the flame distance, is the ionisation current measured at least upstream the flame front and in the immediate proximity of said front at least in average value. 730 6. Method as per either one or more of the above claims characterised by tl e fact instead that at least one of tlie above characteristic quantities of the mixture, is varied according to the instantaneous fuel gas flow rate instead of the flame distance. 7. Regulation method as per claim 6 characterised by the fact that the 735 indicative quantity of the instantaneous fuel gas flow rate used is the flame density. 8. Regulation method as per claim 7 characterised by the fact that the flame density is detected through the emission intensity in the different frequencies of the flame itself. 740 9. Regulation method as per either one or more of the previous claims characterised by the fact that a base regulation is made to have λ steady at the varying of the instantaneous air flow rate, subject then to modify this base λ value should the flame distance move from the prefixed value as per claim 2. 745 10. Method as per either one or more of the above claims characterised by the fact that the provided λ variation is combined with the outflow velocity variation of the mixture through the cross section variation of at least one flame opening, according to its wall temperature, by rising the temperature increases the velocity and vice versa. 750 11. Method as per claim 6 characterised by the fact that the λ variation at tlie varying of the flame distance is combined with the outflow velocity variation of the mixture from the flame opening/s according to the instantaneous fuel gas flow rate, so to increase the section for a flow rate increase and vice versa. 755 12. Regulation method as per one or more of the above claims characterised by the fact that the λ value variation is continue. 13. Regulation method as per one or more of the above claims, characterised by the fact that, at ignition, λ value is lower than that expected at steady state and modifies only after a predetermined period 760 of time. 14. Regulation method as per one or more of the above claims, characterised by the fact that, at ignition, λ value is lower than that expected at steady state and no λ value modification occurs for temperatures, of at least one flame opening, lower than a predetermined 765 value. 15. Regulation method as per claim 6 characterised by the fact that the outflow velocity variation of the mixture at the varying of the flame distance is combined with the temperature variation of tlie mixture upstream the flame front according to the instantaneous fuel gas flow 770 rate, so to increase the temperature for a flow rate increase and vice versa. 16. Regulation methods as per one or more of the above claims, characterised by the fact that the variation of the section of at least one flame opening, according to the flame distance, is continue . 775 17. Regulation method as per one or more of the above claims, characterised by tl e fact that when tl e burner is off, the flame opening/s section is the maximum provided and remains as such at ignition, for a predetermined time, then modifies. 18. Regulation method as per one or more of the above claims, 780 characterised by the fact that, at ignition, no change of the outflow section occurs for lower temperatures of at least one flame opening to a predetermined value, to obtain an outflow velocity of the mixture lower than the one provided at steady state. 19. Method as per one or more of the above claims, characterised by 785 the fact that, besides the mixture temperature variation upstream the flame front, according to the flame position, the λ is varied in the mixture. 20. Method as per claim 19 characterised by the fact that λ is varied according to the instantaneous fuel gas flow rate and reaches lower 790 value for higher flow rates and vice versa. 21. Method as per one or more of the above claims, characterised by the fact that besides tl e regulation obtained through the mixture temperature upstream the flame front, the section of at least one flame opening is varied. 795 22. Regulation method as per claim 21 characterised by the fact that the outflow cross section is varied according to the instantaneous fuel gas flow rate and becomes higher for higher flow rates and vice versa. 23. Method as per one or more of the above claims, characterised by the fact that the temperature variation of the mixture upstream the flame 800 front, is combined with the outflow velocity of the mixture variation through the cross section modification of the flame opening, according to its wall temperature, increasing the temperature increases the velocity and vice versa. 24. Regulation method according to one or more of the above claims, 805 characterised by the fact that the temperature variation of the mixture outflowed from one or more flame openings is continue. 25. Regulation method according to one or more of the above claims, characterised by the fact that, at ignition, the mixture temperature value is higher than the one provided at steady state and remains as such at 810 ignition, for a predetermined time, then modifies. 26. Regulation method according to one or more of the above claims, characterised by the fact that, at ignition, the mixture temperature value is higher than the one provided at steady state and does not change for temperatures of at least one flame opening lower than a predetermined 815 value. 27. Combustion system with gas burner, where the mixture outflowing from one or more flame openings in combustion chamber, made of primary air and fuel gas, is from almost stoichiometric to strongly hyperstoichiometric (0.95 < λ <1.6) and has an average outflow 820 velocity between 0.2 and 4.0 meters per second; has a lamellar flame, characterised by the fact of working following the method described in at least one of the claims from 1 to 26. 28. Regulation apparatus accomplishing the method as per one or more claims from 1 to 26 characterised by the fact of having an optical 825 sensor of the radiation emitted by the flame. 29. Apparatus as per claim 28 characterised by the fact that an optical sensor transmits a signal of the real flame position compared to a prefixed position. 30. Apparatus as per claim 28 and/or 29 characterised by the fact that 830 the optical sensor transmits a signal proportional to the emission intensity of the flame, in particular in radiation frequencies emitted from at least one of the OH, CH radicals. 31. Apparatus as per claims 28 and/or 29 and/or 30 characterised by the fact that the optical sensor transmits a signal proportional to the 835 emission intensity of the flame, in particular in the radiation frequencies emitted by at least one of the OH, C2 radicals. 32. Regulation apparatus accomplishing the method as per one or more of the claims from 1 to 26 characterised by the fact of having a sensor detecting the ionisation current, in at least a small volume, at least 840 upstream and close to the flame front in any of its possible position . 33. Apparatus as per claim 32 characterised by the fact that the ionisation current sensor transmits a signal of the real flame position compared to a prefixed position. 34. Apparatus as per claim 32 and or 33 characterised by the fact that 845 the ionistion sensor is connected to a device particularly suitable to the signal processing, able to provide the amplitude and frequency of the oscillation plus the average intensity of the ionisation current. 35. Regulation apparatus accomplishing the method as per one or more of the claims from 1 to 26 characterised by the fact that the flame 850 sensor is a temperature sensor, put at least upstream and very close to the flame front in any of its possible positions. 36. Apparatus as per claim 35 with a temperature sensor formed by at least two close thermocouples capable of measuring the local temperature gradient. 855 37. Combustion system as per claim 27 characterised by the fact that the temperature change of the mixture occurs in heating it upstream the flame front through a heating body. 38. Combustion system as per claim 37 where the heating body is formed by a shelled heating element 860 39. Combustion system as per claim 38 characterised by the fact that the heating element is made of material whose resistivity changes with the temperature so that it maintains steady the mixture temperature which laps it,maintaining same voltage at terminal. 40. Combustion system as per claim either 38 or 39 characterised by 865 the fact that the heating element has shape,dimensions and positioning such to be of fluid dynamics obstacle such to create downstream vortexes necessary and sufficient for the anchorage in that zone of the flame front. 41. Combustion system as per claim 37 and/or 38 characterised by the 870 fact that the heating body temperature never reaches values such to ignite the mixture so to be inserted upstream at least one flame opening. 42. Combustion system as per one or more of claims 38,39 40 characterised by the fact that the heating body temperatures reaches at least during the ignition period values such to ignite the mixture. 875 43. Combustion system as per claim 40 characterised by the fact that the heating body is distributed at least on a large part of the flame opening surface. 44. Combustion system as per claim 27 characterised by the fact that the temperature modification of the mixture occurs through the recircle 880 of exhausts at high temperature, joining the outflowing mixture before the flame front. 45 Combustion system as per claim 44 characterised by the fact that the exliausts recircle at high temperature occurs naturally for the distribution and shape of the flame openings,and the variation of exliausts back flow upstream the flame front is obtained through the movement of the fluid dynamics obstacle linked to the flame position. 46. Gas burner, where the outflowing mixture from one or more of the flame openings in combustion chamber, formed by primary air and fuel gas, is from almost stoichiometric to strongly hyperstoichiometric (0.95 < λ < 1.6) , and has average outflow velocity between 0.2 and 4.0 meters per second; produces a flame of big surface and minimum thickness, characterised by the fact of working following the regulation method provided by at least one of the claims from 1 to 26. 47. Gas burner as per claim 46 characterised by the fact that section modification of the mixture outflow occurs by either opening or closing one or more flame openings. 48. Gas burner as per claim 46 characterised by the fact that the regulation device of the outflow section of the flame opening/s can be advantageously mobile part of the flame opening itself. 49. Gas burner as per claim 48 characterised by the fact that the regulation device of the outflow section of the flame opening/s has gradual and continuous movement except during the start periods. 50. Burner as per claims 47 or 48 and or 49, characterised by the fact that the flame distance sensor is sensor of the flame opening temperature and acts with any actuator to modify the outflow section of at least one flame opening. 51. Burner as per claim 50 characterised by tl e fact that the temperature sensor of at least one flame opening can simultaneously be actuator of the movement able to modify directly the outflow section, being a mobile part of the flame opening. 52. Burner as per claim 50 characterised by the fact that the temperature sensor of the flame opening can simultaneously be actuator of the movement able to modify the outflow section of the flame opening acting on the mobile part of at least one flame opening either directly or indirectly. 53. Burner as per at least one of the claims from 47 to 52, characterised by the fact that the temperature-actuator sensor is realised with at least a bimetallic sheet of suitable shape, snapping if as per claim 47. 54. Burner as per claim 53, characterised by the fact that the bimetallic 920 sheet or sheets have a face limiting the distribution chamber flowed by the mixture so that the other face does not get in contact with the air- gas mixture, nevertheless able to freely move itself. 55. Burner as per claim 53 characterised by the fact that the bimetallic sheet/s have dented edges made to enter tl e slots which are the fix part 925 of the flame opening. 56. Burner as per claim 53 characterised by the fact that the bimetallic sheet/s are pre-charged at room temperature in order not to cause any variation of the outflow section of the flame opening till the flame opening temperature does not reach a predetermined value, 930 independently from the outflow mixture flow rate. 57. Burner as per claims either 51 or 52, characterised by the fact that the sensor-actuator is a bulb of suitable shape filled with fluid which expands itself with the temperature. 58. Burner as per claim 57, characterised by the fact that the expansion 935 of tl e fluid existing in at least one bulb modifies its transverse section for directly modifying the outflow section of at least one flame opening. 59. Burner as per claim 57, characterised by the fact that the expansion of the fluid existing in at least one bulb indirectly modifies the outflow section through the movement of the mobile part of at least one flame 940 opening. 60. Burner as per one or more of the claims from 46 to 59, characterised by the fact that a separate regulation is provided of the different flame openings ofa same burner. 61. Regulation apparatus acting the method as per one or more of the 945 claims from 1,2,10,11, 15, 16, 17, 18, 21, 22, 23 characterised by the fact that the flame distance sensor is an optical sensor of the flame radiation which works through a control unity and any actuator for modifying the outflow section of at least one flame opening, of at least one burner. 950 62. Regulation apparatus acting the method as per one or more of the claims 1, 2, 10, 11, 15, 16, 17,18, 21, 22, 23 characterised by the fact that the flame distance sensor is a sensor of the ionisation current which works through a control unity and any actuator for modifying the outflow section of at least one flame opening of at least one burner. 955

Inventors: SEBASTIANI ENRICO, SEBASTIANI, ENRICO
Applicants: SEBASTIANI ENRICO, SEBASTIANI, ENRICO
Application year: 1997
Main classification: F23N1
IPC codes: F23D14, F23N1, F23N5