Patent Publication Number: US-3879939-A

Title: Combustion inlet diffuser employing boundary layer flow straightening vanes

Description:
United States Patent Markowski Apr. 29, 1975 [5 COMBUSTION INLET DIFFUSER 2.570.155 10/1951 Redding 138/39 EMPLOYING BOUNDARY LAYER FLOW 2.795.373 6/1957 Hewson 138/39 STRAIGHTENING VANES 230L790 8/1957 Doll 415/217 2,844,001 7/1958 Alford 60139.5 X [75] Inventor; Stanley J. Markowski, East 3.l85,l8l 5/1965 Demyan 138/37 Hartford, Conn.  
 [73] Asslgnee: ggl g s gfz Cmponmon&#39; East Primary E.\&#39;aminerC. J. Husar Assistant Examiner-Robert E. Garrett Filed: Jan. 17, 1974 vfiuorney, Agent, or Firm-Vernon F. Hauschilcl 21 Appl. No.: 434,152  
  Related US. Application Data [62] Division of Sen l o. 5 2 l36. April i8. [973. 57 BST AC abandoned. which is a dlvislon of Ser. No. 84.086. 7 Oct. 26, I970. Pat. No. 3.786.065. The boundary layer along a combustor inlet diffuser is 52 u.s. c1 60/39.65; 60/39.?2 R; 138/39; emblilized by removing the Swirl from the nermally 4 5 1; 415/210; 415 217 swirling air flow along the walls, thereby increasing 51 Int. Cl. F02c 3/14 the axial component of the flew veleeity along the 5s 1 Field of Search 60139.65. 39.69; 137/151; fuser walls The invention is applied to an annular 4i5/DlG. l. 2l6. 2l0, 217, 191; [38/37, 39 burner of swirl flow configuration, and permits the utilization of a very wnjfi and short cone angle diffuser to 5 References Cited reduce burner length.  
  UNITED STATES PATENTS 2,558.8!6 7/l95l Bruyncs 138/37 3 Claims, 49 Drawing Figures PATENIEBmzsms 3.879.939  
 sum [:2 ar 11 FIG-6 F|G 7 010/ Sitd/VDAWV [j Pmmmmzsms 3.979.999  
 SHEET 0 3 OF H FIGJI 007E Jw A 29 f PATENTEDAPRZS 197s SHEET CEUF 11 PATENTEUAFRZSMS SHEET 070? 11 871111! III 1111111111 IIIIIIIIIIIIIIIIIIIIIIIIIII Illll IIIIIIII COMBUSTION INLET DIFFUSER EMPLOYING BOUNDARY LAYER FLOW STRAIGHTENING VANES This is a division, of application Ser. No. 352,136, filed Apr. 18, 1973, now abandoned, which is a divisional of Ser. No. 84,086, filed Oct. 26, 1970, now U.S. Pat. No. 3,786,065.  
 CROSS-REFERENCES TO RELATED APPLICATIONS This application contains subject matter related to the following two applications assigned to the same assignee:  
  1. Application Ser. No. 34,087, and now U.S. Pat. No. 3,701,255, filed concurrently herewith for Shortened Afterburner Construction for Turbine Engine&#34; and 2. Application Ser. No. 34,088, and now U.S. Pat. No. 3,675,419, filed concurrently herewith for &#34;Combustion Chamber Having Swirling Flow.  
 BACKGROUND OF THE lNVENTlON 1. Field of Invention This invention relates to the controlled mixing of two thermodynamically and aerodynamically dissimilar fluids and particularly to the use of swirling flow between two dissimilar fluids in annular combustion chambers, such as the burners and afterburners of turbine engines, to accelerate both the combustion process and the temperature reduction process of the products of combustion in the dilution zone of the burner.  
 2. Description of the Prior Art In the combustion chamber and burner art, it has been conventional to burn in a cylindrical chamber by discharging an atomized fuel spray into the center thereof with air being discharged therearound through a vaned cascade at tangential velocity V, so as to form a recirculation zone of the atomized fuel and swirling air so mixing. This recirculation zone is formed because the angular momentum of the air is proportional to the tangential velocity V, thereof times the radius of the air particle involved from the burner central axis, accordingly, any air which is at or near the burner axis is of minimal or zero radius so that the tangential velocity attempts -to go to infinity with the result that nonswirling secondary air is brought in around the recirculation zone for mixing with the stagnated fuel-air mixture downstream of the recirculation zone and for cooling the walls of the combustion chamber, as typically shown in U.S. Pat. No. 3,498,055.  
  These prior art burners are called can burners,&#34; because of their cylindrical shape, or can-annular burners,&#34; because they have a series of can-shaped inlet sections opening into an annular main section. The momentum-velocity system of establishing a recirculation zone is used in the can portion of both.  
  The momentum-velocity system of establishing a recirculation zone does not work in an annular combustion chamber because all combustion stations are of substantial radius and therefore 1 utilize the interdigitation of the swirling sheets of dissimilar fluids to perform this function.  
  The patents to Johnson U.S. Pat. No. 3,030,773 and Sanborn 2,473,347 utilize swirling flow in combustion chambers but it will be noted that these are cylindrical or can type combustion chambers and that none of this prior art teaches the use of establishing an unstable interface between two swirling dissimilar fluids for the purpose of accelerating mixing and combustion therebetween by the establishing and/or control of the fluid density and tangential velocity V, to produce dissimilar product parameters pV, between the two fluids. The conventional can or cylindrical burner is shown in afterburner form in U.S. Pat. No. 2,934,894.  
  Other than the aforementioned type of swirling flow to assist in establishing a recirculation zone in a cylindrical or can burner or in an annular burner having a plurality of substantially cylindrical, circumferentially extending can burner spray nozzles positioned circumferentially thereabout as in U.S. Pat. No. 3,000,183, swirling flow is generally discouraged in conventional combustion chambers and straightening vanes are provided for this purpose.  
  Swirling flow has been suggested for combustion chambers in certain patents, however, including Ferri, et al., U.S. Pat. No. 2,755,623 which teaches the concept of causing the fuel-air mixture passing through a combustion chamber to flow in swirling motion so as to improve combustion, however, it should be noted that in the Ferri, et al., patent there is but a single swirling stream and he therefore does not achieve the mixing and accelerated combustion advantages of my invention. The patent to Meurer U.S. Pat. No. 3,078,672 causes swirling air to be passed through a can-type burner and causes a solid sheet or film of fuel to be passed along the inner surface of the burner outer wall to be vaporized and to burn with the swirling air at the outer wall. Combustion takes place at the interface between the air and the fuel at the outer wall of the combustion chamber and the products of combustion move inwardly to be gathered and recycled through duct 22. Meurer clearly does not teach the concept of mixing and combusting two dissimilar fluids by control of the parameter products taught herein. My U.S. Pat. No. 3,393,516 illustrates curved flow in an exhaust gas deflector of a turbo-fan engine but it should be noted that there is no mixing and combustion in connection with the curved flow, in fact, such would be undesirable.  
 SUMMARY OF THE INVENTION A primary object of the&#39;present invention is to provide a mixer configuration which can be used to increase mixing between dissimilar swirling flow fluids in the combustion zone of an annular combustion chamber to accelerate combustion by increasing the mixing rate between the cool fuel-air mixture and the hot gases and which can also be used to accelerate mixing in the dilution zone of an annular combustion chamber between the products of combustion and the cooling air to accelerate temperature reduction. Combustion is mixing limited. The time or burner length required to obtain complete combustion can be limited by that necessary to mix together the hot gases and the cool fuel-air mixture. Accelerated mixing in both the combustion and dilution zones will shorten the length of the combustion chamber and hence shorten the length and weight of the engine.  
  A primary object of the present invention is to provide an improved annular combustion chamber by establishing, controlling and/or varying the product parameter pVf, where p is fluid density and V, is fluid tangential velocity, between two dissimilar swirling fluids to establish an unstable interface therebetween to accelerate mixing and hence combustion in the combustion zone and mixing and hence cooling in the dilution zone of the combustion chamber.  
  In accordance with the present invention, this product parameter is established, controlled and/or varied so that the product parameter of the fluid which is flowing at the lesser radius about the combustion chamber axis is greater than the product parameter of the fluid which is flowing at the greater radius, so that the mixing ratio in the combustion chamber is determined by the ratio pV, (inner flow) pV, (outer flow).  
  In accordance with a further aspect of the present invention, the interface between two dissimilar swirling combustion chamber fluids are established or controlled so that outside-inside burning occurs in the combustion chamber.  
  The invention permits accelerated mixing and combustion or accelerated mixing and dilution to occur in several annular combustion chamber configurations, for example, in the concentric flow mixer configuration, the barberpole mixer configuration, and the bent tube or folded combustion chamber mixer configuration.  
  In accordance with a further aspect of the present invention, a combustion chamber can be fabricated so as to consist of a combustion zone and a dilution zone with either or both of these zones utilizing a concentric mixer, a barberpole mixer, or a bent tube mixer and any of these mixers can be used with a conventional combustion zone or dilution zone.  
  It is a further aspect of the present invention that utilizing any of these mixing constructions, combustion can take place utilizing either the premixed or diffusion principlev It accordance with a further aspect of this invention, hardware is provided to establish, control or vary the orientation of two concentric fluid streams of different thermodynamic and aerodynamic states in such a way that the product parameter density, p, of the inner stream times the tangential velocity V, of the inner stream is greater than the corresponding product parameter of the outer stream.  
  In accordance with still a further feature of the present invention, compound mixing in radial, parallel staging occurs both in the combustion zone and the dilution zone of an annular combustion chamber in which the combustion zone and the dilution zone are axially staged in series so as to reduce the overall length of the combustion chamber and hence the engine length and weight.  
  In accordance with still a further feature of this invention, several modifications of the pilot combustion zone in a concentric mixer for a primary combustion zone are usable and of advantage depending upon the particular requirements of the combustion chamber configuration involved.  
  In accordance with still a further aspect of the present invention, triggers are used to disturb the unstable interface between two swirling streams to accelerate mixing and either combustion or cooling therebetween.  
  In accordance with still a further aspect of this invention, a combination flameholder and/or trigger can be used in a swirling flow annular combustion chamber to accelerate mixing and burning of the products of combustion from the recirculation zone established downstream of the flameholder and the fuel-air mixture passing around the flameholder.  
  In accordance with still a further feature of this invention, swirling fluid interface trigger mechanisms are provided in the form of a corrugated and tapered rings, which may have holes or scoops therein for noise deadening and trigger mechanism cooling purposes.  
  In accordance with still a further feature of this invention, combustion apparatus is provided in which combustion or dilution zones are located in series in which mixing occurs in both zones at parallel radial stations.  
  In accordance with a further teaching of this invention, the unstable interface between two swirling streams of fluid which are established by the product parameter criterion taught herein can be physically interrupted or disturbed by a variety of trigger mechanisms.  
  It is a further teaching of this application to establish a stable interface criteria between the cooling air for a combustion chamber liner and the products of com bustion.  
  In accordance with still a further feature of my invention, swirling flow in an annular combustion chamber invites the use of flameholders therein and the use of a substantial variety of fuel injecting devices to be used therewith.  
 BRIEF DESCRIPTION OF THE DRAWINGS FIG. I is a schematic representation of two dissimilar fluids flowing in swirling relationship in separated coannular passages and then joining and mixing in a single annular passage.  
  FIG. 2 is a schematic showing in cross-section of the FIG. 1 flow representation.  
  FIG. 3 is a vector diagram of the fluid flowing in swirling fashion in the FIG. I and 2 environment and the other environments disclosed herein.  
  FIG. 4 is a showing of the static pressure distribution across the outer and inner swirling fluid flows of the FIG. 1 and 2 environment.  
  FIG. 5 is a schematic representation of mixing occuring in two fluid streams flowing in side-by-side relationship and which are caused to swirl in passing through a bent tube.  
  FIG. 6 is a schematic cross-sectional showing of a barberpole&#34; swirl mixer.  
  FIG. 7 is an end view taken along line 7-7 of FIG. 6.  
  FIG. 8 is a showing of an annular combustion chamber concentric mixer utilizing the premixed burning principle.  
  FIG. 9 is similar to FIG. 8 but utilizing the diffusion burning principle.  
  FIG. 10 is a cross-sectional showing of an annular combustion chamber barberpole mixer used in the combustion zone and utilizing the premixed burning principle.  
  FIG. I] is similar to FIG. 10 but utilizing the diffusion burning principle.  
  FIG. 12 is a showing of a premixed combustor employing bent tube mixing in a folded combustion chamber which is preferably of the annular type.  
  FIG. 13 is a showing of a modern turbine engine of the type used in the modern aircraft and shown utilizing my invention.  
  FIG. I4 is a cross-sectional showing of an annular combustion chamber using a concentric mixer in both the combustion zone and the dilution zones.  
  FIG. is a showing of a vane of an annular vane cascade and its actuating mechanism to make the cascade variable angle so as to vary the angle at which the gases passing therethrough are discharged.  
  FIG. 16 is a cross-sectional showing of an annular combustion chamber using a barberpole mixer in both the combustion zone and dilution zones thereof.  
 FIG. 17 is taken along lines I7-l7 of FIG. l6.  
  FIG. 18 is an enlarged, unrolled showing of the combustion chamber outer liner of FIG. 16 to illustrate the orientation of the outer liner helical slots in the barberpole mixer of the dilution zone.  
  FIG. I9 is a cross-sectional showing of the varied, helical slots used in the inner wall of the dilution zone mixer of FIG. 16 and is taken along line 19-19 of FIG. 16.  
  FIG. 20 is a modification of the helical slots shown in FIG. 18 and can be used in the barberpole mixer either in the combustion zone or the dilution zone of an annular combustion chamber.  
  FIG. 21 is a cross-sectional showing of an annular combustion chamber having axially staged combustion and dilution zones and utilizing a concentric mixer in the combustion zone and a barberpole mixer in the dilution zone.  
  FIG. 22 is a cross-sectional showing of an annular combustion chamber having a conventional combustion zone and dilution zone of the folder burner or bent tube variety utilizing my invention.  
  FIG. 23 is a modification of the primary combustor portion of the combustion zone mixer shown in FIG. 14.  
  FIG. 24 is a modification of the concentric mixer used in the combustion zone of an annular combustion chamber which may be substituted for the type shown in FIG. 14.  
  FIG. 25 is an enlarged, partial. cross-sectional showing of the flameholder member taken along line 25-25 of FIG. 24.  
  FIG. 26 is a showing of a modification of the combustor shown in FIG. 25.  
  FIG. 27 is an enlarged showing of the FIG. 26 con struction taken along line 27 of FIG. 26.  
  FIG. 28 corresponds to FIG. 27 and shows the secondary flow patterns between the helical guide vanes.  
  FIG. 29 is still another modification for the primary combustion chamber shown in FIG. I4.  
  FIG. 30 is a schematic representation of two swirling fluids flowing through annular passages with a splitter duct therebetween and with a trigger mechanism attached to the downstream end of the splitter duct.  
 FIG. 3! is an end view of the FIG. 30 construction.  
  FIG. 32 is a cross-sectional showing of a trigger mechanism which may be substituted for the trigger mechanism shown in the splitter duct of FIG. 14.  
  FIG. 33 is a showing of the trigger mechanism of FIG. 32 shown with the splitter duct unrolled for purposes of better illustration. 7  
  FIG. 34 shows another modification of trigger mechanism of FIG. 14.  
  FIG. 35 is a showing of a further trigger mechanism modification utilizing plural rows or patterns of helical slots in or near the trailing edge of a splitter duct.  
  FIGS. 36 and 37 are plan and end views of still another trigger mechanism modification of the variety which utilizes both a helically slotted and helically corrugated downstream end on a splitter duct to perform their swirling fluid interface triggering functions.  
  FIG. 38 is a showing of still another trigger mechanism modification utilizing a combination of helical slots and scooped projections cooperating therewith at the downstream end of a splitter duct to accelerate mixing.  
  FIG. 39 is a representation of irregular trigger corrugation utilized for the purpose of noise suppression.  
  FIGS. 40 and 41 depict annular combustion chamber flow passage modifications which can be used because of the swirling flow therethrough to retard or prevent flow separation of the boundary layers along the diffuser walls.  
  FIGS. 42a and 42b are showings or an annular com bustion chamber utilizing swirl flow and further utilizing a compound vane cascade at the inlet thereof to control the amount of swirling at the various radial stations across the cascade so as to discourage boundary layer flow separation and permit the utilization of shortened diffuser section in the combustion chamber, thereby reducing the length of the combustion chamber.  
  FIGS. 43 and 44 are showings of the axial velocity profile and tangential velocity profile of the air immediately downstream of the cascade of compound vanes of FIG. 42.  
  FIG. 45 is a cross-sectional showing of a scoopedaperture which may be used with trigger mechanisms, such as those shown in FIG. 14.  
  FIGS. 46 thru 48 are showings of annular combustion chambers utilizing radially staged combustion for reduced combustion chamber and engine length and having provisions for engine power performance control.  
 DESCRIPTION OF THE PREFERRED EMBODIMENT To fully explain the subject matter of this application, it is deemed desirable to first describe the theory involved.  
  My observation of the dynamic behavior of concentric dissimilar swirling flows leads to the discovery of a fluid interface instability phenomenon that can be used to increase the mixing rate between the dissimilar fluids and which therefore is of particular interest in combustion chambers to accelerate combustion by increasing the mixing rate and hence the effective flame speed and also to accelerate the mixing which takes place in the combustor dilution zone wherein the products of combustion are cooled by mixing with cooling air before being passed through the turbine. As used herein the term dissimilar fluids means fluids which are thermodynamically and aerodynamically dissimilar. This phenomenon of interest and its characteristics will now be described by referring to FIGS. 1 and 2. In these figures, two dissimilar fluids are flowing in concentric swirling flow patterns and are isolated initially by a cylindrical separator wall 10, which is positioned between cylindrical ducts l2 and 14 so that walls l0, l2 and 14 are concentric about centerline or axis 16 and cooperate to define concentric annular passages 18 and 20. While the outer fluid will be described as the hot fluid and the inner fluid the cold fluid, this does not have to be the case.&#39;As the-swirling fluids pass downstream of the separator termination point 22, interface 24 is established therebetween. As best shown in FIG. 3, the velocity of each fluid may be represented by the flow vector diagram shown where V, is axial velocity, V, is tangential velocity and V is actual velocity in the indicated direction. Fluid flowing in such a manner comes under the primary influence of two forces of significant magnitude, namely, centrifugal forces and forces due to the pressure gradient which exists in the duct through which the fluid is flowing. At a given radius, the centrifugal force, F is proportional to the mass of the fluid, and consequently the density, p, of the fluid, and the square of the tangential velocity or tangential velocity component V,, ofthe fluid. The pressure gradient force, F,,, is proportional to the radial pressure gradient and results from the radial difference in static pressure across the radially projected area of the fluid element. During the passage of the two fluids through annular passages and 18, these forces are in equilibrium, as best shown in FIG. 1 with respect to simulated fluid particles 26 and 28, and the fluid flows in its helical path.  
  Downstream of separator 10, where both fluids enter common annular passage 30, the two fluids are in direct contact with each other and therefore are capable of influencing one another.  
  By viewing FlGS. l and 4 it should be noted that the static pressure distribution profile 32 for the outer swirling, usually hot fluid is considerable less steep than the static pressure distribution profile 34 of the inner swirling cold fluid, and this is reflected in the magnitude of the pressure gradient force, F,,, indicated to be acting upon the outer stream element 28 and the inner stream element 26 in FIG. 1. These pressure gradient forces acting on elements 28 and 26 are balanced by the centrifugal force, F action thereon because of the radial equilibrium of each individual stream.  
  My study and observations have lead me to the discovery that interface 24 between these two dissimilar fluids is unstable if the product parameter pV,, i.e., the product of the fluid density p and the square of the tangential velocity V, of the fluid, of the outer radial fluid is less than that of inner radial fluid. This instability is demonstrated by introducing a disturbance into the interface 24 such that a local interface convolution 36 projects radially outwardly into the outer radius fluid region. The element of fluid 26&#39; in this projection 36 is exposed to the relatively small radial pressure gradient, F,,,, of the outer radius fluid region but still retains its high centrifugal force, F This establishes an unbalance of forces on element 26&#39; and results in an acceleration of the disturbance radially outward to cause the convolution size and penetration into the outer radius fluid to increase, thereby increasing the rate of mixing between the two fluids. In similar fashion, a convolution 38 of the interface 24 projecting radially inward will result in a force unbalance on fluid element 28&#39; which remains under the relatively small centrifugal force, F and comes under the influence of the substantially larger pressure gradient force, F and is consequently accelerated radially inward to result in rapid inward growth of convolution 38 and accelerated mixing between the two streams.  
  The relative magnitude of the unbalanced forces just described may be assessed by considering the outer fluid as a combusted gas from a combustion chamber which typically would lower the density by a factor of perhaps four relative to the unvitiated innerstream. Since the tangential velocity of the gas in a typical combustor pilot will change relatively to a smaller magnitude, the unbalanced force is seen to be three-quarters or more of the maximum centrifugal force on the two fluids. This magnitude of the unbalanced force is decidedly first order and represents a large acceleration potential available to expedite the radial movement of the two concentric fluids into a helical sheet mode of flow.  
  My invention is the utilization of this phenomenon in accelerating mixing between two dissimilar swirling fluids in annular combustion chambers of the type used in turbine engines to both accelerate combustion and accelerate the dilution of the hot products of combustion with cooling air before passage through the turbine.  
  While I have described this mixing phenomenon in FIGS. 1 and 2 in the context of coannular, dissimilar, swirling streams, it should be borne in mind that the same mixing acceleration can be achieved in other environments such as the bent tube environment shown in FIG. 5 wherein both dissimilar streams flow through duct 66 which includes a straight portion 68 and bent portion 70, which has center of curvature 79, and which has splitter or separation member 72 at its upstream end cooperating with duct 66 to define two passages 74 and 76 through which the two dissimilar streams flow with the fluid in the outer passage 74 having lower pV, than the fluid in the inner passage 76 so that when the two fluids join in passage 78 they establish the unstable interface and accelerate mixing described in connection with FIGS. 1 and 2 as they become concentric swirling streams upon entering bent tube section 70, in view of the fact that the product parameter relationship p, V pc VJ, where pa and pe are the density of the hot outer, swirling stream and the cold, inner, swirling stream respectively, and V and V are their respective tangential velocities, which are actually their through-flow velocities in the bent tube construction.  
  This accelerated mixing can also be established by use of the barberpole swirl mixer 80 shown in FIGS. 6 and 7. The term barberpole is selected to describe this mixer because it causes the two dissimilar fluids to form into a series of interdigitated, swirling sheets or fingers. This mixer consists of outer wall 82 and inner wall 84 which preferably diverge to form diverging passage 86 through which the swirling main fluids flow and which have selectively oriented helical slots 88 and 90 extending therethrough, respectively, through which the secondary fluids flow and are caused to enter parallel to the main stream flow. As best shown in FIG. 7 the direction of helical slots 88 and 90 are such that they are locally parallel to the direction of the swirling main flow. By use of appropriate guide vanes and inlet conditions for the secondary flows the product parameter flow criterian: pV, inner secondary pV, main flow and pV, outer secondary pV, main flow are attained. With this flow criteria the sheets of secondary flow will penetrate rapidly across the main flow because the same mixing phenomenon previously de scribed in connection with the FlGS. 1 and 2 construction occurs here between each swirling fluid sheet and the two swirling sheets of dissimilar fluids adjacent thereto. Accordingly, total required mixing will occur more rapidly. In certain situations, it may be desirable to use a barberpole mixer of the type shown in FIGS. 6 and 7 in which the helical slots are used in one of the walls, 82, or 84 only. In the FIGS. 6 and 7 barberpole construction, the main flow is preferably hot air and the secondary flows are cooler air and the slots 88 and 90 are oriented to bring about not only helical flow but helical flow substantially parallel to the main flow direction.  
  Any of these mixers, that is, the concentric mixer, barberpole mixer and the bent tube mixer can be effectively utilized in the combustion zone of a combustor or burner to increase the rate of mixing and hence rate of combustion and effective flame speed so as to reduce overall burner length as illustrated in FIGS. 8-12. To emphasize similarity of function the reference numerals of FIGS. 1, 2, 6 and 7 will be repeated in describing the FlGS. 8-12 constructions.  
  In practice when using these mixers in the combustion zone of a combustor, one of the swirling streams is used as a hot pilot to initiate combustion in the other swirling stream, which is a fuel-air mixture. Burning occurs when the two streams mix.  
  We will now consider which stream to select as the pilot stream.  
  In the case of the concentric mixers and combustion chambers shown in FIGS. 8 and 9 and the bent tube combustion chamber shown in H6. 12, it is apparent that the pilot stream should be the outer stream because the density depression caused by heating helps in achieving the desired interfaced instability criteria pVf&#34; inner pV, outer. In the barberpole mixers and combustors shown in FIGS. 10 and 11, the choice of which stream will act as the heated pilot is not as obvious. in view of the density depression associated with fluid heating, it is apparent that the pilot stream should be one of the streams requiring a low pV, product parameter and hence the pilot stream should not be the secondary flow in inner passage 114. The main stream 112 should be chosen as the pilot stream to avoid the severe wall cooling problems which would be caused by injecting a hot gas secondary stream from passage 112 along outer walls 82. In view of the low density of the pilot stream, the product parameter pV, for the outer secondary fluid can be made smaller than the product parameter pV, of the pilot to obtain the desired rapid mixing by permitting little or no tangential velocity V, as it passes through slots 88. The desired interface instability criteria between the pilot flow from passage &#34;2 and inner secondary flow from passage 114 is satisfied by the use of the required turning vanes or the like to adjust the tangential velocity (V,) level to satisfy the required criteria pV, inner pV, pilot. Of course, the combustion process in the pilot decreases the density of this stream thereby assisting in satisfying this criteria.  
  FIG. 8 depicts a concentric mixer in a combustion chamber combustion zone where concentric passages 18 and 20 are formed between concentric ducts l2, l and 14 and wherein splitter duct terminates short of the outer ducts so that the outer ducts form combustion zone 30 downstream thereof. Appropriately positioned inlet guide vanes or other mechanisms cause swirling fluid to pass through each of passages 18 and 20. The flow in passage 20 serves as the pilot combustion stream in that pilot fuel is injected thereinto through pilot fuel nozzle mechanism 92 which sprays atomized fuel into the fluid passing therethrough just upstream of flameholder 94 to form pilot combustion zone 96 downstream thereof wherein the fuel-:ur mixture is burned and vitiated after appropriate ignition in combustion zone 96 so that the swirling fluid discharging from passage 20 becomes a pilot to ignite and sustain combustion in the swirling fluid passing through passage 18. This fluid in passage 18 has fuel added thereto by secondary fuel injector 98 to form a fuel-air mixture of the characteristics that the product of its density and tangential velocity squared pV, is greater than the cor responding product parameter for the outer swirling pilot stream of passage 20 so that accelerated mixing and subsequent combustion takes place between the two fluids in combustion zone 30. The burner shown in FIG. 8 utilizes the premixed burning principle in that fuel is sprayed into the secondary stream 18 prior to entering the mixing and combustion zone 30 and this stream becomes a combustible fuel-air mixture that is subsequently ignited and vitiated when it is mixed with the hot pilot gases or flame from stream 20.  
  Such a concentric mixer used as a combustor utilizing the diffusion burning principle is shown in FIG. 9. The diffusion burning technique works on a different principle than the premixed burning technique. In the diffusion burning technique, the pilot fuel from nozzle 92 is fully combusted and fully vitiated in pilot combustion zone 96 such that little or no oxygen remains therein and, accordingly, any fuel added thereto down stream of fully vitiated interface 100 can be vaporized only by the hot products of combustion from pilot zone 96. This phenomenon is taken advantage of in the dif fusion burning principle and secondary fuel is discharged into stream 20 by secondary fuel nozzles 101 but this secondary fuel cannot burn until it is mixed with the secondary air being passed in swirl fashion through in stream 18. In this case it will be seen that no fuel whatsoever is directed into stream l8 and that the pilot stream 20 carries not only the heat necessary to initiate combustion and mixing in mixing and combustion zone 20 but also carries the fuel to support this combustion process, when mixed with the air from passage 18.  
  FIGS. 10 and 11 depict barberpole mixers of the type shown in FIGS. 6 and 7 utilized to form combustion chambers of the premixed burning and diffusion burning variety. In the H0. lflconstruction, ducts I02, 104, I06 and 108 are positioned concentrically about center line 16 to form coannular passages 110, 112 and H4 therebetween. Guide vanes or the like are used to produce swirling flow in passages 110, 112, and 114 to achieve the desired tangential velocity V, or, as in all other configurations disclosed, this flow may be accepted directly from a compressor which does not have straightening vanes at its outlet. Ducts 104 and 106 join walls 82 and 84 which define passage 86, which is preferably divergent and is the main combustion zone 60. Fuel is sprayed through pilot nozzles 92 into annular passage 112 to be combusted in pilot combustion zone 96 downstream of flameholder 94 to serve as the pilot stream. Secondary fuel is injected into passages 110 and 1 14 through secondary fuel nozzles 98 in atomized form to be mixed with the air passing therethrough and to pass therefrom through opposed helical slots 88 and 90, respectively. to be discharged as a fuel-air mixture flow substantially parallel to the swirling pilot stream being directed from pilot combustion chamber 96 for accelerated mixing and subsequent combustion with the pilot stream in mixing and combustion zone 60. As in the case of the barberpole mixer, the direction of flow of the secondary fuel-air mixture through slots 88 and 90 are adjusted by suitable guide vanes to satisfy the instability criteria pV, outer secondary pV, pilot and pV, inner secondary pV, pilot.  
  In the FIG. -11 construction, all air entering passage 96 enters with a selectively established tangential velocity V,. This spinning of the air will lower the static pressure in the pilot combustion chamber 96. The premixed fuel-air mixture passing at a larger radius through passage 110 does not necessarily have swirl added thereto. In passage 110 air enters the combustion zone 60 through slots or helical hole pattern 88 in wall 82, such holes 88 are helical in nature or holes or slots designed in helical pattern. This air will accelerate radially through the holes 88 due to the static pressure drop across the holes or slots and once inside primary or pilot combustion zone 60, this air will continue to be accelerated radially inward because of the radial pressure gradient established by the swirling pilot fluid from passage 96 in combustion chamber 86. By admitting this fuel-air mixture through helical slots or holes or slots in a helical pattern, 88, a very rapid combustion pattern of helical layers will be established in the main combustion zone 60. The fuel-air mixture layers thus formed are burned as interdigitated mixing with the swirling air from the pilot proceeds. As the fuel-air mixture through slot 88 is burned, its radial inward motion is locally further accelerated because the consequent decrease in the density lowers its pV, product parame ter even further and the radial pressure gradient will accelerate a small portion of burned gas faster than unburned gas. The portion of the fuel-air mixture which passed through helical slots or hole pattern 90 has a tangnetial velocity V, imparted thereto that is sufficiently high for pV,&#34;&#39; pV, of the vitiated pilot gases. Therefore the admitted fuel-air mixture will form helical sheets which will interdigitate with the hot spinning air entering zone 60 from the pilot region and 96 and be accelerated radially outward. While the density, p, of the locally burned surface layer of the swirling fuelair mixture streams will decrease substantially during burning, it will retain the same tangential velocity, V,, since its angular momentum is unaffected by the change of thermodynamic state. Consequently, the local pV, product parameter of the sheets entering through the slots 90 will be substantially reduced and its acceleration due to the radial pressure gradient will also be reduced as the sheet burns. However, the unburned portion of the helical layer will continue to be accelerated radially outward, thus continuing to stir the flame front until it is completely burned.  
  Viewing FIG. 11 we see the barberpole mixer used as a combustion chamber utilizing diffusion burning in which concentric, preferably cylindrical ducts 102, 104, I06 and 108 are positioned concentrically about center liner axis 16 to form coannular passages 110, H2, and 114 therebetween, with ducts 104, 106 extending into preferably divergent walls 82 and 84 to form section 86 which defines the main combustion zone 60. Pilot fuel from nozzles 92 is admitted in atomized form to passage 112 upstream flameholder 94 to be fully combusted and vitiated in pilot combustion chamber 96 so that the products of combustion are fully vitiated upstream at interface 100. Secondary fuel is admitted to annular passage 112 downstream of interface 100 through secondary fuel nozzle 101 to be heated and carried with swirling combustion products of the pilot combustion chamber 96 into combustion zone 60, secondary air is passed through annular ducts I10 and 114 and through opposed helical slots 88 and 90, respectively, into mixing and combustion chamber 60 to be mixed with, the hot, fuel rich, flow from pilot stream duct 112. As the mixing process proceeds the excess fuel in the pilot stream comes into contact with the sheets of secondary air entering through slots 88 and and combustion occurs at the multiplicity of interface between these flows.  
  FIG. 12 depicts a bent tube mixer in the form of a folded burner or combustor of the premixed burning variety. In the FIG. 12 premixed burning configuration, the first fluid is passed through passage 74 to have atomized fuel added thereto from pilot fuel nozzle 92 and so that a pilot combustion zone is established at 96 so as to provide an outer pilot stream entering the curved section 70 of curved duct 66 to serve as a pilot to institute mixing with and subsequent combustion of the fuelair mixture being introduced through passage 76 into mixing and combustion chamber 30. The fuel-air mixture in passage 76 is generated by the passage of fluid therethrough and the introduction of atomized fuel thereinto through secondary fuel spray nozzles 98. It will accordingly be seen in the FIG. 12 construction that a hot pilot stream is established as the outer swirling stream with respect to the inner colder fuel-air mixture stream, both of which are concentric about center of curvature 79 to cause accelerated mixing and combustion therein in view of the flow criteria pV, inner pV, It will be evident to those skilled in the art that the construction shown in FIG. 12 could be made of the diffusion variety by moving pilot fuel nozzle 92 and flameholders 94 farther upstream so that combustion in the pilot combustion zone 96 is completed and a fully vitiated interface corresponding to 100 of FIG. 9 is established sufficiently far upstream of the termination of splitter member 72 that secondary fuel can be injected into passage 74 upstream into combustion chamber 30 in uncombusted form for mixing and combusting with secondary air which would flow through passage 76.  
  To assist in accelerating mixing between the two swirling flows in the concentric and bent tube mixers, it is sometimes desirable to use trigger mechanisms at the end of ducts which serve as splitter ducts between the swirling flow of two different fluids, such as triggers 164 and 166 shown in FIG. 14, to physically disturb the interface between the swirling fluids. A discussion of the theory of operation of these trigger mechanisms is believed to be helpful at this point and reference is first made to FIGS. 30 and 31 in this regard. In FIG. 30 we see trigger mechanism 166 positioned at the downstream end of splitter duct 246 which is of circular cross section and positioned concentrically about axis 16 and cooperates with outer cylindrical duct 248 and inner cylindrical duct 250 to define outer annular gas passage 252 and inner annular gas passage 254. For purposes of illustration, it should be considered that a hot fluid, which is to be the pilot fluid, is passed through passage 252. This hot outer fluid has a density p,, and a tangential velocity V,,,. A second fluid, which is preferably a cold (high density) combustible mixture, is passed through inner annular passage 254 and has a density of p and a tangential velocity V To effect accelerated mixing between these two fluids of passage 252 and 256, it is essential that the mixing criteria p V p V exists to establish an unstable interface between two swirling fluids. Above and beyond this, the use of trigger 166, which is shown to be a convoluted sheet metal ring member attached to the downstream end of splitter duct 246 further serves to accelcrate mixing and combustion. Trigger 166 defines convolutions which follow helical paths growing in amplitude in a downstream direction and as the fluids of passage 252 and 254 pass thereover. a regular pattern of radial fluid motion will be initiated outwardly and inwardly due to the change of flow direction imparted to the fluids by trigger mechanism 166. The motion thus initiated will grow because of the instability of the interface. Such a trigger mixer has been successfully demonstrated using air at 200 and 800F as working media.  
  The amount of tangential mixing induced by fluid shearing at the helical sheet interface will depend upon the difference between the circulation per radian of the fluids in ducts 252 and 254.  
  The use of trigger mechanisms provides the advantage of controlling the location, size and shape of the disturbance at the interface between the two fluids and it will be appreciated that in constructions where trigger mechanisms are not used the disturbance of the interface is caused by turbulence only and is therefore random in nature.  
  Of particular interest is a piloted combustion application of such a triggered inside-out mixing configuration as shown in FIGS. 30 and 31. Here, the hot vitiated pilot flow would be the outer radius fluid having a low pV, product parameter, while the cold combustible mixture would be the inner radius fluid having a high pV, product parameter. FIG. 31 is a showing of the combustion-pilot primary combustion zone down stream of trigger I66. The flame front where active combustion occurs is located at the interface 255 and 253, respectively, of the triggered helical sheets of hot pilot flow from duct 252 and cold combustible mixture flow from duct 254. As shown in FIG. 31, the flame speed, F/S, moves against the trigger helical current of the combustible mixture flowing radially outward and into the hot mass of pilot flow. As the combustion occurs at the flame front, elements of air undergo an abrupt density change in a high centrifugal field with resultant release of the acceleration potential to magnify the local turbulence and effective flame speed. This local stirring action, i.e., increased turbulence, is superimposed upon the interface of the triggered mixing of the initial hot pilot and cold combustible mixture flows. The triggered hot pilot gas from passage 252, which comprises a radially inward directed current, has an interface flame speed that moves with the current, as well as laterally into the unburned mixture. Again, the local magnitude of turbulence is increased at the flame front by the abrupt fluid density changes in a strong centrifugal field which increases the effective flame speed. The difference in circulation per radian for the initial hot pilot flow and cold combustible mixture provides a superimposed tangential mixing through tangential shearing action.  
  Another trigger mechanism. which could be used as a substitute for trigger I66 in the FIGS. 14 and 30 construction, is shown in FIGS. 32 and 33. As shown in FIG. 32, splitter duct 246 and ducts 248 and 250 are used in the same fashion as in the FIG. 30 construction. Hot products of combustion flow between ducts 246 and 248, while the cooler fluid, such as a fuel-air mixiture, flows in the passage between ducts 246 and 250. Trigger mechanism 258 is located at the downstream end of splitter duct I40 and consists of a series of oppositely oriented vane 260 and 262 pairs forming vortex generators which are spaced circumferentially about splitter duct and extending radially outwardly from the splitter duct and in any desired number of axially spaced rows. Once again, it is the object of trigger mechanism 258 to convolute the interface between the hot products of combustion flowing on one side of splitter duct and the cooling air or fuel-air mixture flowing in passage on the other side of the splitter duct so as to take advanatge of the mixing criteria in that the pV, product parameter of the hot gases flowing at the greater radius is less than the pV, product parameter of the cold air or fuel-air mixture flowing at a lesser radian at the interface therebetween and any convolution will react with the respective pressure gradients in the hot and cold regions to cause radial mixing currents with cold air current moving into the hot flow in helical sheets and the hot fluid currents moving into the cold region in helical sheets. The flow at the interface downstream of the trigger plane is unstable and the trigger configuration establishes the helical sheet mixing patterns. This mixing occurs from the inside (minimum radial station) to the outside (maximum radial station) and shortens the length of the combustion chamber and engine by accelerating the mixing process.  
  Referring to FIG. 34 we see still another modification of a splitter duct trigger which could be used in place of trigger 166 of FIG. I4. The trigger of FIG. 34 con&#39; sists of a series of helically oriented and circumferentially positioned slots 260 at the downstream end of splitter duct 140. The slots are preferably oriented to be parallel to the direction of flow, V, of either the hot or cold gas streams and serves to trigger or disturb the unstable interface which exists between the swirling hot gas flow from the combustion chamber flowing outside splitter duct and the swirling colder air of the cooling gas stream. flowing inside of the splitter duct 140 so as to accelerate intermixing.  
  An additional trigger embodiment is shown in FIG. 35 wherein a plurality of helically extending and circumferentially positioned slots 262 are positioned forward or upstream of slots 260 of the type shown in FIG. 34. Thereby adding to the mixing advantage of the trigger device by utilizing plural slot rows and/or patterns.  
  Still a further trigger configuration is shown in FIGS. 36 and 37 wherein slots comparable to slot 260 of FIG. 34 are fabricated so as to be elongated and are circumferentially positioned helical slots 264. In this configuration, the after end of splitter duct 140 is fabricated, as shown in FIG. 37, to be corrugated in shape so that the FIG. 36 and 37 trigger is a combination of the slotted trigger of FIG. 34 and the convoluted trigger of FIG. 30.  
  Still another form of trigger is shown in FIG. 38 wherein scoops 266 are added to helical slots 268, which are comparable to slots 260 of FIGS. 34 and 35 and which serve to scoop the cold spinning air from a construction comparable to the FIG. 14 construction flowing on the outside of splitter 140 into the hot region radially inward of the splitter duct I40 where the products of combustion from combustion chamber 60 flow, thus triggering the mixing pattern downstream of the splitter duct plane. This FIG. 38 construction will set up helical spinning layers of hot and cold air to mix downstream&#39;of the splitter duct. While but a single row of such scooped slots are shown in FIG. 38, it should be realized that more than one row or a pattern thereof could be used, as is shown in FIG. 35 without scoops.  
  For improved acoustic properties and for improves combustion of the trigger 166, it is recommended that trigger 166 be made of sheet metal with a series of small holes 257 therein and preferably, scoop member 259 (see FIG. 53) to be associated with holes 257 to force small jets from the cold side of the trigger to flow to the hot side to cool the trigger and to also introduce a fine scale of disturbance or turbulence to improve combustion.  
  As mentioned previously, acoustic benefit can be gained by utilizing perforations in the corrugated trigger of the type shown in FIG. 50 and this is important because large amplitude noise has been shown to affect combustion efficiency adversely. Additional noise suppression can be achieved by varying the height and width (distance between) of the trigger corrugations or other trigger mechanisms, and also varying the cycle of the trigger pattern peripherally to achieve noise sup pression, thus producing spiraling or helical sheets of hot and cold gases having different frequency response. Such a configuration is depicted in FIG. 39 wherein h represents height or amplitude of the convolutions and I and m represents different corrugation widths.  
  An engine of the type in which may invention may be used is shown in FIG. 13 as turbine engine 40, which consists of a compressor section 42, a burner or combustion section 44, a turbine section 46, and may have an afterburner section 48, which terminates in a variable area nozzle 50. Engine 40 is preferably of circular cross-section and concentric about axis 52. Combustion section 44 includes outer casing 54 and and annular combustor combustion chamber or burner 56, which consists of diffuser inlet section 58, combustion zone 60 and dilution zone 62. As used herein, the term annular combustion chamber&#34; means a combustion chamber having an annular passage extending from the inlet, or upstream end, to the outlet, or downstream end thereof. Fuel is supplied to combustor 56 by variable output fuel pump 64 which is either under pilot manual or pilot set automatic control, and is fed into the inlet of combustor 56 in a fashion to be described hereinafter, to be mixed therewith with a portion of the pressurized gas from compressor section 42 to form a combustible fuel-air mixture to be burned in combustion zone 60, from which the products of combustion pass into dilution zone 62 for mixing with dilutant cooling air also from the compressor to lower the temperature thereof prior to entry into turbine section 46. Engine 40 may be of the type more fully described in US. Pat. Nos. 2,747,367; 2,711,631 and 2,846,841.  
  A typical combustor system or section 44 of a turbine engine of the type shown in FIG. 13 may be considered to be composed of two components in series, namely, a combustion zone 60 in which fuel is burned in a portion of the total engine air flow from the compressor and a dilution zone 62 in which the balance of the air flow is mixed with the hot products of combustion from the combustion zone so that a substantially cooler mixture then the products of combustion is passed through the turbine 46. Any combination of concentric mixtures. barberpole mixers, and bent tube mixers, can be used to perform the combustion zone region mixing and combustion function and the dilution zone region mixing and cooling functions of such a combustion section 44.  
  Referring to FIG. 14 we see annular combustion chamber 56 which comprises outer case 54 and inner case 113, which are preferably of circular cross-section and mounted concentrically about axis or center line 16. The air from the compressor section 42 of FIG. 13 enters annular inlet 114 in either swirling flow or nonswirling flow depending upon the discharge conditions from the compressor section 42, and portions thereof pass through pilot passage 124, main combustion zone fuel preparation passage 126 and the dilutant air passage 130. Further quantities of air flow through passages 122 and 132 to provide for cooling the walls of the combustor chamber. Vanes 116, 118, and 128 are employed as required to swirl or straighten the flow in the respectivie passage so as to satisfy the previously defined mixing instability criteria. Each of the passages 122, 124, 126, 130 and 132 are of annular shape since the outer burner liner 134, the inner burner liner 136 and splitter ducts 138 and 140 are of circular crosssection and concentric about axis 16. Turning vanes 116 and 118, 120 and 128 may be fixed or any or all vanes could be of the variable angle type as shown, for example, in FIG. 15 wherein each of vanes 116 is pivotally connected to duct 134 and outerhousing 54 by pivot pins 144 and 146, respectively. Pivot pin 146 extends through outer case 54 and carries ring gear 148 at its outer end, which engages circumferentially rotatable ring or annular gear 150, which is pilot operated to rotate circumferentially about axis 16 by motion of pilot actuated lever 152 into and out of the plane of the paper, thereby causing vanes 116 to rotate in unison and thereby vary the tangential velocity V, of the gas or fluid passing thereby. The swirling air which entered passage 124 has atomized fuel added thereto by fuel injection device 156 to form a fuel-air mixture which is ignited by ingitor 158 and vitiated in pilot combustion chamber 160 which is located downstream of aperturetype flameholder 161, which is a tilted and aperture plate extending between ducts 134 and 138. The hot swirling stream emerging from passage 124 serves as a pilot stream for combustion chamber 60. The swirling air entering passage 126 has atomized fuel added thereto by injection member 162 and the amount of fule to be discharged into passage 124 and 126 can be regulated by the size and number of fuel nozzles, such as 162 located therein and by pilot controlled valves 163 and 165 located in the fuel line thereto. The atomized fuel entering passage 126 mixes with the swirling gas passing therethrough to provide a combustible fuelair mixture to combustion chamber 60 for accelerated mixing pilot stream emerging from passage 124 and subsequent combustion of this flow. It will accordingly be seen that hot swirling pilot stream emerging from passageway 124 to mix with and sustain combustion in the fuel-air mixture emerging from passageway 126 and the thermodynamic and aerodynamic characteristics of these two streams are established so as to satisfy the rapid mixing criteria pV, pv, outer. This may be attained by adjusting the tangential velocity v, in each stream through a suitable selection of the discharge angle of the vanes 118 and 120. It should be noted that the combustion process in the pilot duct 124 depresses the density p of this stream relative to that in duct 126 which assists in satisfying the desired rapid mixing criteria. The products of combustion from combustion zone 60 then pass into dilution chamber 62 in swirling, concentric flow relationship to the cooling air being passed into dilution zone 62 through cooling air passage 130 to again satisfy the aforement unstable inter-