Air and fuel staged burner

Information

  • Patent Grant
  • 6685463
  • Patent Number
    6,685,463
  • Date Filed
    Friday, December 15, 2000
    23 years ago
  • Date Issued
    Tuesday, February 3, 2004
    20 years ago
Abstract
A burner (10) for reducing NOx emissions where supply fuel (16) and supply air (20) are supplied to a combustion tunnel (52) at high and low velocities and secondary air (26) is supplied to a secondary combustion zone (60), wherein products of combustion (59) exiting into the secondary combustion zone (60) from the combustion tunnel (52) are drawn back into the combustion tunnel (52) and back into the secondary air conduit (54).
Description




BACKGROUND OF THE INVENTION




1. Field of the Invention




The present invention relates to burners and, more particularly, to low NO


x


emission burners having staged air and staged fuel capabilities.




2. Brief Description of the Prior Art




Low NO


x


burners are known in the art. For example, U.S. Pat. Nos. 5,180,300 and 4,983,118 both disclose low NO


x


regenerative burners. Likewise, U.S. Pat. No. 4,732,093 to Hansen et al. discloses a method and apparatus for burning fuel in an annular nozzle burner. However, there exists a need for a burner that further reduces NO


x


generation.




SUMMARY OF THE INVENTION




The present invention provides an air and fuel staged burner that reduces NO


x


generation. One embodiment of a burner according the present invention generally includes a main burner body defining an internal cavity, an air connection fluidly connected to the internal cavity, and a combustion tunnel. A distribution tee may be fluidly connected to the internal cavity defined by the main burner body and a burner nozzle may be positioned in the interior cavity of the main burner body. The burner nozzle may define a primary air orifice, an annulus, and a fuel orifice. The air connection may be configured to receive supply air and divide the supply air into primary air and secondary air, where the ratio of primary air to secondary air is approximately in the range of 40/60 to 70/30 respectively, with a 50/50 ratio being preferred. The primary air preferably flows through the primary air orifice at a rate of approximately 300-400 feet/second (91-122 meters/second).




The main burner body generally extends longitudinally about an imaginary burner centerline, and the primary air orifice is preferably oriented to form a convergent angle as measured from the imaginary burner centerline, such as an angle of approximately 30-60° as measured from the imaginary burner centerline. Alternatively, the primary air orifice may be oriented to produce a swirl pattern of primary air in the combustion tunnel, where the swirl is approximately less than or equal to 0.7 times an internal diameter of the combustion tunnel.




The burner may also include a secondary air conduit fluidly connected to the distribution tee, the secondary air conduit having a secondary air jet fluidly connected to a secondary combustion zone. The main burner body generally extends longitudinally about an imaginary burner centerline and the secondary air jet is oriented substantially parallel to the imaginary burner centerline. Alternatively, the main burner body may extend longitudinally about the imaginary burner centerline with the secondary air jet oriented at an angle convergent with the imaginary burner centerline. The secondary air exits the secondary air jet at a velocity of approximately 150-400 feet/second (46-122 meters/second).




A fuel connector is configured to receive a supply fuel and divide the supply fuel into a primary fuel and a secondary fuel. The split ratio of primary fuel to secondary fuel split ratio is approximately in the range of 20/80 to 40/60 respectively, with a split ratio of 22/78 being preferred. A primary fuel path and a secondary fuel path may also be included, with the primary fuel path fluidly connected to the annulus, the secondary fuel path fluidly connected to the fuel orifice, and the primary fuel path and the secondary fuel path fluidly connected to each other. The primary fuel may exit the annulus defined by the burner nozzle at a velocity approximately less than 100 feet/second (30 meters/second). The secondary fuel may exit the fuel orifice defined by the burner nozzle at a velocity approximately greater than 350 feet/second. The fuel orifice and the fuel annulus may lie in the same plane, substantially perpendicular to an imaginary burner centerline and the distribution tee may be positioned adjacent to the internal cavity of the main burner body and opposite the combustion tunnel (


52


).




One method of decreasing NO


x


emissions in a burner having a main burner body defining a combustion tunnel may include the steps of flowing supply air into the main burner body, dividing the supply air into primary air and secondary air, flowing the primary air into the combustion tunnel at a given velocity, flowing primary fuel into the combustion tunnel at a velocity lower than the velocity of the primary air, flowing secondary fuel into the combustion tunnel at a velocity higher than the velocity of the primary fuel, flowing secondary air into a secondary combustion zone by a secondary air jet at a velocity higher than the velocity of the primary fuel, and igniting the primary fuel, the secondary fuel, and primary air in the combustion tunnel to form products of combustion. Additional steps may include exhausting products of combustion into the secondary combustion zone and drawing products of combustion into the combustion tunnel and into the secondary air jet.




The device and method according to the present invention helps to reduce burner NO


x


emissions.




These and other features and advantages of the present invention will be clarified in the description of the preferred embodiment taken together with the attached drawings in which like reference numerals represent like elements throughout.











BRIEF DESCRIPTION OF THE DRAWINGS





FIG. 1

is a partial cross-sectional side view of one embodiment of the present invention;





FIG. 2

is a full cross-sectional side view of the embodiment shown in

FIG. 1

excluding the secondary air jets for clarity and rotating the location of the primary air connection by 90 degrees; and





FIG. 3

is a front view of a burner nozzle shown in FIG.


2


.











DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT




The preferred embodiment of a burner


10


according to the present invention is shown in

FIGS. 1-3

.

FIG. 2

shows the burner


10


having a main burner body


22


defining an air connection


12


, an internal cavity


13


, and a combustion tunnel


52


. A fuel connector


14


is provided through which supply fuel


16


enters the burner


10


, except in the event a gas pilot (not shown) is used through a port


18


. An electrode (not shown) is used to ignite the burner


10


; however, a gaseous pilot could be used.




As best shown in

FIG. 2

, supply air


20


enters the air connection


12


, passes into the internal cavity


13


defined by the main burner body


22


, and is divided into primary air


24


and secondary air


26


. A secondary air orifice


28


permits the secondary air


26


to enter a secondary air distribution tee


30


while the primary air


24


passes through at least one primary air orifice


32


defined by a burner nozzle


46


, with the number of primary air orifices


32


preferably in the range of four to eight orifices


32


. The primary air


24


is accelerated through the primary air orifice or orifices


32


to a range of approximately 300 feet/second-400 feet/second (91-122 meters/second), depending on the air preheat available, nominal burner


10


ratio, and rated input. The primary air


24


is preferably directed in a convergent manner toward an imaginary burner centerline C; however, the primary air orifice or orifices


32


may also be slightly offset to induce a swirl pattern on the primary air


24


. A convergence angle α of the primary air orifice or orifices


32


can be approximately 30°-60°, as measured from the imaginary burner centerline C. The swirl or offset can be as much as 0.7 times the primary port, or combustion tunnel, diameter D.




The supply fuel


16


entering fuel connector


14


passes into a fuel sparger


34


which divides the supply fuel


16


via holes


36


into primary fuel


38


and secondary fuel


40


. The primary fuel


38


travels along one or more primary fuel paths


42


, preferably parallel to the secondary fuel


40


which travels through a secondary fuel path


44


. The primary fuel path


42


is preferably fluidly connected to an annulus


47


defined by the burner nozzle


46


positioned in the internal cavity


13


defined by the main burner body


22


. The secondary fuel path


44


is preferably fluidly connected to a fuel orifice


48


, also defined by the burner nozzle


46


. The primary fuel


38


exits the burner nozzle


46


through the annulus


47


into the combustion tunnel


52


at a low velocity, ideally less then 100 feet/second (30 meters/second), depending on rated input. The secondary fuel


40


passes down the secondary fuel path


44


and exits into the combustion tunnel


52


through fuel orifice


48


, preferably accelerated to a velocity approximately greater than 350 feet/second (107 meters/second), depending on rated input. As shown in

FIG. 3

, the fuel annulus


47


preferably has a first width W


1


and the fuel orifice


48


preferably has a second width W


2


, with the first width W


1


of the fuel annulus


47


being less than the second width W


2


of the fuel orifice


48


.




Referring again to

FIG. 2

, the velocities of the primary and the secondary fuels


38


,


40


exiting the annulus


47


and the fuel orifice


48


of the burner nozzle


46


will depend on the velocity of the primary air


24


exiting the primary air orifice or orifices


32


. The primary fuel


38


exiting the annulus


47


mixes in a highly turbulent region with the primary air


24


exiting the primary air orifice or orifices


32


, creating a highly reducing combustion region within the combustion tunnel


52


. The secondary fuel


40


exiting the fuel orifice


48


is accelerated to the point that there is only a partial mixing of the secondary fuel


40


with the primary air


24


and products of combustion


59


in a primary combustion zone


50


of the combustion tunnel


52


. Therefore, the profile of combustion exiting the combustion tunnel


52


is more oxidizing toward the perimeter of combustion tunnel


52


and more reducing along the imaginary burner centerline C.




As best shown in

FIG. 1

, the secondary air


26


passes through the distribution tee


30


and into a secondary air conduit


54


. The secondary air conduit


54


communicates the secondary air


26


to a secondary air jet


56


spaced apart from a combustion tunnel exit


62


of the combustion tunnel


52


and in fluid communication with a secondary combustion zone


60


. Secondary air


26


exits the secondary air jet


56


at a velocity in the range of 150 feet/second to 400 feet/second (46-122 meters/second), depending on the air preheat, nominal design ratio of the burner


10


, and rated input.




The burner


10


is capable of being operated with a single secondary air jet


56


or a plurality of secondary air jets


56


. The secondary air jets


56


may be oriented parallel or convergent to the imaginary burner centerline C, shown as angle β in FIG.


1


. The secondary air


26


exits the secondary air jets


56


at a furnace wall


58


and creates a negative pressure region pulling the products of combustion


59


from the second combustion zone


60


back into the secondary air orifice


56


, highly vitiating the secondary air


26


before the secondary air


26


reaches the sub-stoichiometric ratio mixture exiting the combustion tunnel


52


. The resultant combustion expansion in the primary combustion zone


50


of combustion tunnel


52


also creates a suction at the furnace wall


58


in the vicinity of the combustion tunnel exit


62


which also induces the furnace products of combustion


59


back to the combustion tunnel exit


62


.




The burner


10


configuration of the present invention provides vitiation in the primary and secondary combustion zones


50


,


60


such that the stoichiometry to the burner


10


must be on the oxidizing side to initiate stable combustion in the secondary combustion zone


60


when below 1200° F. furnace temperature. At approximately 1200° F. (649° C.), the stoichiometry can be brought to approximately 10% excess air with the resulting main flame stability and the secondary combustion reactions completing without the generation of free combustibles. Minor traces of CO will be apparent with furnace temperature between 1200° F. and 1400° F. (649° C.-760° C.). The primary fuel


38


to secondary fuel


40


split ratio can be approximately 20/80 to 40/60, respectively, while the primary air


24


to secondary air


26


split ratio can be 40/60 to 70/30, respectively. The optimum primary fuel


38


to secondary fuel


40


split ratio is approximately 22/78, respectively, and the optimum primary air


24


to secondary air


26


split is approximately 50/50.




The air and fuel staged burner


10


according to this first embodiment significantly improves NO


x


emission capabilities, as illustrated in the following table:












TABLE 1











COMPARISION OF PRESENT INVENTION WITH AN






AIR STAGED BURNER AT AN AIR TEMPERATURE OF






750° F. (399° C.) AND A FURNACE TEMPERATURE OF






1600° F. (871° C.)














AIR STAGED




FUEL & AIR STAGED

















NO


x


PPM @ 3%




44




22














The invention has been described with reference to the preferred embodiment. Obvious modifications and alterations will occur to others upon reading and understanding the preceding detailed description. It is intended that the invention be construed as including all such modifications and alterations.



Claims
  • 1. A method of decreasing NOx emissions in a burner (10) having a main burner body (22) that defines a combustion tunnel (52) and a source of secondary air (26) comprising the steps of:a) flowing supply air (20) into the main burner body (22); b) dividing the supply air (20) into primary air (24) and secondary air (26), wherein the ratio of primary air (24) to secondary air (26) is approximately in the range of 40/60 to 70/30, respectively; c) flowing the primary air (24) into the combustion tunnel (52) at a given velocity; d) flowing primary fuel (38) into the combustion tunnel (52) at a velocity lower than the velocity of the primary air (24); e) flowing secondary fuel (40) into the combustion tunnel (52) at a velocity higher that the velocity of the primary fuel (38); f) flowing the secondary air (26) into the secondary combustion zone (60) at a velocity higher than the velocity of the primary fuel (38); g) igniting the primary fuel (38), the secondary fuel (40), and primary air (24) in the combustion tunnel (52) to form products of combustion (59); h) exhausting the products of combustion (59) into a secondary combustion zone (60); and i) drawing the products of combustion (59) from the secondary combustion zone (60) to a combustion tunnel exit (62) and to the source of secondary air (26).
  • 2. The method as claimed in claim 1 further comprising the step of:j) vitiating the secondary air (26) before the secondary air (26) reaches a sub-stoichiometric ratio mixture exiting the combustion tunnel (52).
  • 3. A method of decreasing NOx emissions in a burner (10) having a main burner body (22) defining a combustion tunnel (52) and a source of secondary air (26) comprising the steps of:a) flowing supply air (20) into the main burner body (22); b) dividing the supply air (20) into primary air (24) and secondary air (26); c) flowing the primary air (24) into the combustion tunnel (52) at a given velocity; d) flowing primary fuel (38) into the combustion tunnel (52) at a velocity lower than the velocity of the primary air (24); e) flowing secondary fuel (40) into the combustion tunnel (52) at a velocity higher than the velocity of the primary fuel (38); f) flowing the secondary air (26) into the secondary combustion zone (60) at a velocity higher than the velocity of the primary fuel (38); and g) igniting the primary fuel (38), the secondary fuel (40), and primary air (24) in the combustion tunnel (52) to form products of combustion (59); h) exhausting products of combustion (59) into a secondary combustion zone (60); and i) drawing products of combustion (59) from the secondary combustion zone (6) to a combustion tunnel exit (62) and to the source of secondary air (26).
  • 4. The method as claimed in claim 3, wherein the primary air (24) flows into the combustion tunnel (52) at a rate of approximately 300-400 feet per second at rated input.
  • 5. The method as claimed in claim 3, wherein the secondary air (26) flows in the secondary combustion zone (60) at a velocity of approximately 150-400 feet/second at rated input.
  • 6. The method as claimed in claim 3, wherein the primary fuel (38) to secondary fuel (40) split ratio is in the range of approximately 20/80 to 40/60, respectively.
  • 7. The method as claimed in claim 3, wherein the primary fuel (38) flows into the combustion tunnel (52) at a velocity less than approximately 100 feet/second at rated input.
  • 8. The method as claimed in claim 3, wherein the secondary fuel (40) flows into the combustion tunnel (52) at a velocity approximately greater than 350 feet/second at rated input.
  • 9. The method as claimed in claim 3 further comprising the step of:j) vitiating the secondary air (26) before the secondary air (26) reaches a sub-stoichiometric ratio mixture exiting the combustion tunnel (52).
CROSS-REFERENCE TO RELATED APPLICATION

This application claims the benefit of earlier filed United States Provisional Patent Application Ser. No. 60/171,073, filed Dec. 16, 1999, entitled “Air and Fuel Staged Burner”.

US Referenced Citations (20)
Number Name Date Kind
3022815 Bloom et al. Feb 1962 A
4023921 Anson May 1977 A
4095929 McCartney Jun 1978 A
4351632 Nagai Sep 1982 A
4629413 Michelson et al. Dec 1986 A
4645449 Schwartz et al. Feb 1987 A
4732093 Hansen et al. Mar 1988 A
4859173 Davis, Jr. et al. Aug 1989 A
4878829 Anderson Nov 1989 A
4983118 Hovis et al. Jan 1991 A
4988285 Delano Jan 1991 A
5092761 Dinicolantonio Mar 1992 A
5180300 Hovis et al. Jan 1993 A
5209656 Kobayashi et al. May 1993 A
5295816 Kobayashi et al. Mar 1994 A
5431559 Taylor Jul 1995 A
5449286 Snyder et al. Sep 1995 A
5460512 Lifshits et al. Oct 1995 A
5944507 Feldermann Aug 1999 A
6068470 Zarzalis et al. May 2000 A
Foreign Referenced Citations (3)
Number Date Country
0 076 036 Apr 1983 EP
0430376 Jun 1991 EP
60-78208 May 1985 JP
Provisional Applications (1)
Number Date Country
60/171073 Dec 1999 US