BURNER FOR A FLARE
20190195491 ยท 2019-06-27
Assignee
Inventors
Cpc classification
F23G7/08
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F23D14/02
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F23D2210/00
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F23D14/24
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F23D14/58
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F23D2212/105
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
International classification
F23G7/08
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
Abstract
A tip burner for a flare comprises a diffuser (7) which is sealingly connected downstream to a shroud (9) comprising a tightly packed bed of granular material (13). The stream of fuel and oxidizer flows to a diffuser where is mixed and tangentially swirled by a swirler (8) located either in the diffuser or in a closed proximity to the diffuser inlet. The mixture flows next to the shroud where the granular material provides a tortious flow path for the stream, restructuring it aerodynamically and reducing its velocity, preferably to sub sonic level. A combustible mixture exits the shroud as multiple of jet, at low velocity and low turbulence. The mixture is ignited by a pilot burner installed above but in close proximity of the shroud, resulting in a stable flame which generates a low noise level.
Claims
1. A burner [for a flare stack] comprising in co-operating arrangement: i) an open upwardly expanding truncated conical mixing diffuser having an inlet receiving a gaseous feed comprising at least one fuel and an oxidant in a ratio to provide for the substantially complete combustion of the fuel at the burner exit; ii) above and co-operating with the outlet of said mixing diffuser an upper shroud, which can be in a shape of an open upwardly expanding truncated cone or a cylinder; iii) two perforated plates which constitute the inlet and the outlet of the said shroud; iv) within the shroud, a bed of inert, solid or hollow rigid tightly packed granules, said bed having the height at least equivalent to one inlet radius of the said shroud, and having a total cross sectional area of interstitial voids among the granules at the shroud inlet of not less than 2 times the cross sectional area of the inlet of the said diffuser; and iv) one or more pilot burners above and proximate to the surface of the upper perforated plate which constitutes the shroud exit.
2. The burner according to claim 1 further comprising one or more arrays of swirling vanes either: i) inside the said diffuser, the said array comprising a set of vanes forming a series of radially enclosed channels to swirl, mix and discharge said streams of fuel and oxidizer, in a radially outward and tangential manner wherein the sum of the cross section areas of said channels is not less than 95% of the total cross section area of the diffuser inlet; or ii) inside the passages or tubing which deliver fuel and oxidizer to the said diffuser, and in proximity to the diffuser inlet, said arrays comprising a set of vanes forming a series of radially enclosed channels to swirl and discharge said respective streams of fuel and oxidizer in a radially outward and tangential manner into the mixing diffuser, wherein the sum of the cross section areas of said channels is not less than 95% of the total cross section area of the diffuser inlet.
3. The burner according to claim 2, wherein said perforated plates which constitute the inlet and outlet of the said shroud are selected from the group consisting of a wire mesh, a perforated plate and a grid of parallel metal bars defining openings there through, having a maximum size opening not more than 70% of the characteristic smallest dimension of the inert granular packing.
4. The burner according to claim 3, wherein the inert granular packing comprises the particles of the same size and the same regular shape selected from the group consisting of solid spheres, rods, pellets, prills, saddles, and rings, and mixtures thereof made of the material selected from the group consisting of metal, ceramic and polymeric materials, having a melting temperature not less than 50 C. greater than the combustion temperature of the mixture of said at least one fuel and said oxidant.
5. The burner according to claim 4, wherein the inert granular packing comprises a mixture of irregularly shaped or differently shaped particles, with size distribution within 25% of the average mean dimension.
6. The burner according to claim 5, wherein the inert granular packing is cleaned and sieved gravel having a size distribution within 25% of average sieve size.
7. The burner according to claim 5, wherein the shroud containing the granular material, has a diameter substantially the same size as the outlet of said diffuser and has a length to radius ratio of not less than 1:2.
8. The burner according to claim 5, wherein the shroud has an exit diameter from 2 to 15 times the diameter the said diffuser outlet and has a length to radius ratio of not less than 1:1.
9. The burner according to claim 5, wherein in the mixing diffuser the angle of the side wall is from 10 to 50 off vertical.
10. The burner according to claim 9, wherein said closed diffuser is an upward opening truncated cone.
11. The burner according to claim 10, wherein in said r diffuser contains swirling vanes, which are uniformly radially spaced.
12. The burner according to claim 13, wherein said vanes have a tangential deflective angle greater than 5.
13. The burner according to claim 12, wherein said vanes have straight parallel deflective edges.
14. The burner according to claim 13, wherein said vanes are wedged shaped.
15. The burner according to claim 12, wherein said vanes are curved.
16. The burner according to claim 10, wherein upstream and proximate to the inlet to the diffuser, separate arrays of swirling vanes are in the oxidant passage and in the fuel passage, so the gas and the oxidant are separately swirled, before they tangentially enter the diffuser inlet.
17. The burner according to claim 10, wherein the swirling vanes are mounted upstream and proximate to the inlet of the diffuser in the oxidant passage(s) so only oxidant is swirled, before it tangentially enters the diffuser.
18. The burner according to claim 10, wherein the swirling vanes are mounted upstream and proximate to the inlet of the diffuser in the fuel passage(s) so only fuel stream is swirled, before it tangentially enters the diffuser.
Description
BRIEF DESCRIPTION OF DRAWINGS
[0031]
[0032]
[0033]
BEST MODE FOR CARRYING OUT THE INVENTION
[0034] The present invention is directed to a silencing burner for a flare. The silencing burner has low noise level (generally less than 95 dBA, preferably less than 85 dBA) and has a stable flame.
[0035] In
[0036] In
[0037] In
[0038] In
[0039] In
[0040] In
[0041] In the preceding embodiments the side wall of the mixing diffuser is open (hollow) upwardly opening truncated cone and the side wall of the shroud is open (hollow) upwardly opening truncated cone or cylinder. Other shapes could be used for example hollow upwardly opening parabolas or hemisphere, as is shown in
[0042] The granular material in the bed is selected so that the total cross sectional area of the interstitial voids between the particles at the bed or shroud inlet is of not less than 2, in some embodiments not less than 2.25, in other embodiments not less than 2.5, in further embodiments not less than 3, times the cross sectional areas of the inlet to the diffuser.
[0043] For regularly shaped particles, such as spheres, the cross sectional area of the interstitial voids may be calculated using the methods known to estimate close-packing of particles in a granular bed, [see, for example, Aste T., Weaire D., (2000), The Pursuit of Perfect Packing, London, Institute of Physics Publishing, ISBN 0-7503-0648-3, Section 2 (Loose change and hard packing) & Section 3 (Hard Problem with Hard Spheres); Conway J. H., Sloane N. J., Bannai E. Sphere Packings, Lattices and Groups, Springer 1999, Sec. 6.3; and Sloane N. J. H., (1984), The Packing of Spheres, Scientific American 250, pgs. 116-125]. Assuming that the spheres are tightly packed, the interstitial area will depend on diameter of the spheres.
[0044] In some instances, for example, where the packing is irregularly shaped (e.g. gravel), it may be simpler to experimentally determine the cross sectional area of the interstitial voids between granules by filling a representative bed with a liquid, such as, water, measuring the volume and determining the change in volume with the change in the level of liquid in the bed to approximate the volume between particles, and then to determine the cross sectional area at different heights of the packing.
[0045] In one embodiment of the present invention, the bed of granular material is tightly packed. That is, the granular material is not simply poured into the bed. Rather, the granular material is placed in the bed/shroud and the shroud is subject to vibration (shaking) to pack the bed to achieve a tight and uniform packing.
[0046] One factor to ensure the efficient operation of some embodiments of the present invention is the adequate pressure drop as the gas flows through tortuous passages between granular material contained in the bed. The pressure drop should be sufficient to reduce the gas velocity to sub-sonic level, while the gas exits the perforated cap on the shroud at a pressure equal to the ambient pressure level.
[0047] The granular packing in the shroud creates the tortuous path for the flow of the stream of oxidant and fuel, which results in an aerodynamic restructuring of the stream which has pressure and velocity further reduced. The achieved reduction depends on the thickness of the granular layer and on the angle of the wall of the conical shroud or on the diameter of the cylindrical shroud which is, in turn, determined by the exit diameter of the upstream diffuser. The diameter or size of the opening at the exit of the shroud is such that there is no substantial constraint on the mass flow rate of the fluid out of the shroud, but the velocity of fluid is substantially reduced, in case of sonic jetspreferably to subsonic velocity. The depth of packing to obtain a desired pressure drop to substantially atmospheric pressure may be calculated based on principles for fluid (gas) flow through a tightly packed granular bed. Once the bed depth is determined and the size of the exit from the diffuser is calculated, the angle of the wall of the diffuser may be determined as a function of the exit opening and the bed depth.
[0048] As noted above there are pilot burners proximate and external to the perforated upper plate of the shroud. Also in some cases the wall may extent up above the particulate bed to provide protection for the flame from destabilizing wind effects.
[0049] The operation of the burner will now be described.
[0050] A gaseous stream comprising fuel and oxidant, in some instances under high pressure, enters the inlet of the burner, and flows into the diffuser containing the swirling vanes. The fluid is there divided among the swirler channels into the smaller streams, which are discharged radially outwardly from the channel exits into the dissipative shroud, at tangential directions consistent with the shape of the swirling vanes.
[0051] Alternatively, fuel and oxidant flowing through their respective passages in the stack, are entering the swirling vanes which are located in the passage exits, in close proximity to the diffuser inlet. Thus, both streams are already swirled when they enter tangentially the diffuser.
[0052] The swirling streams, after impinging and mixing inside the diffuser, enter the shroud through the bottom perforated plate and flow upwards, through the circular cross section of the shroud. The gas flows through the constant or increasingly large cross section of the granular bed, which creates the tortuous path for the flow. As a result, the stream is aerodynamically restructured into multitude of smaller streams, which are of low turbulence, low velocity, and they experience further mixing and pressure losses combined with the simultaneous velocity reduction. The flow exits the diffuser through the top perforated plate, at atmospheric pressure and with a subsonic velocity. Accordingly, noise generated by the jet is significantly reduced.
[0053] The exiting jet is ignited by one or more pilot burners and because of the good mixing of fuel and oxidant as they pass through the burner, and because of low and uniform velocity of the jet, the flame is very stable.
INDUSTRIAL APPLICABILITY
[0054] A burner for a flare comprises swirler up stream of a packed bed to initially mix oxidant and fuel which then passes through the packed bed to reduce the velocity of the gases to sub sonic levels to reduce the noise of the flare.