The invention will now be described, by way of example only, with reference to the following figures in which:
The fuel injector 32 disclosed in
The fuel injector system 32 utilizes a pilot fuel injector 36 of the type commonly referred to as a simplex pressure atomizer fuel injector. As will be understood by those skilled in the art, the simplex pressure atomizer fuel injector 36 atomizes fuel based upon a pressure differential placed across the fuel, rather than atomizing fuel with a rapidly moving air stream as do airblast atomizers.
The fuel injector system 32 further includes a main airblast fuel injector 40 which is concentrically located about the simplex pressure atomizer pilot fuel injector 36. Inner and outer main swirlers 42 and 44 are located concentrically inward and outward of the main airblast fuel injector 40. The simplex pressure atomizer pilot fuel injector 36 and main fuel injector 40 may also be described as a primary fuel injector and a secondary fuel injector, respectively.
As it will be appreciated by those skilled in the art, the main airblast fuel injector 40 provides liquid fuel to an annular aft end 46 which allows the fuel to flow in an annular film. The annular film of liquid fuel is then entrained in the much more rapidly moving and swirling air streams passing through inner main swirler 42 and outer main swirler 44, which air streams cause the annular film of liquid fuel to be atomized into small droplets. Preferably, the design of the airblast main fuel injector 40 is such that the main fuel is entrained approximately mid-stream between the air streams exiting the inner main swirler 42 and the outer main swirler 44.
All three swirlers 38, 42 and 44 are fed from a common air supply system, and the relative volumes of air which flow through each of the swirlers are dependent upon the sizing and geometry of the swirlers and their associated air passages, and the fluid flow restriction to flow through those passages which is provided by the swirlers and the associated geometry of the air passages. In one exemplary embodiment, the swirlers and passage heights are constructed such that from 5 to 20 percent of total swirler air flow is through the pilot swirler 38, from 30 to 70 percent of total air flow is through the inner main swirler 42 and the balance of total air flow is through the outer main swirler 44.
Each of the inner and outer main swirlers 42 and 44 have a vane configuration, the vane angles of the outer main swirler 44 may be either counter-swirl or co-swirl with reference to the vane angles of the inner main swirler 42. The swirl vanes are typically straight, though they may be curved. The curved axial swirl vanes are provided to reduce the Sauter Mean Diameter of the main fuel spray from the main airblast injector 110 as compared to the Sauter Mean Diameter that would be created when utilizing straight vanes.
In a conventional fuel injector the vanes extend radially as depicted in
The vane configuration of the inner main swirler is depicted in more detail with reference to
Each of the vanes 50a . . . 50j comprises a leading edge 52, a trailing edge 54, a pressure flank 56 extending from the leading edge to the trailing edge and a suction flank (not shown) also extending from the leading edge to the trailing edge, and opposed to the pressure flank.
The vane follows a helix as the vane extends axially, the rotation of the helix occurring along a line that coincides with the radius of the swirler. Each of the leading edges 52 and trailing edges 54 extend along a radius of the injector between a hub 58 and a tip 60.
A velocity contour diagram at the plane of exit of the fuel passages to the pre-filmer 46 is depicted in
The Sauter Mean Diameter is inversely proportional to the velocity and therefore can be used to represent the atomisation performance. Where the velocity is lower the atomisation performance is reduced. The reduced atomisation can lead to increased levels of smoke or NOx being emitted from the engine.
With reference to
This divergence is caused by a strong circumferential drift of the low kinetic energy fluid from the pressure side to the suction side of the vane passage. Across the vane passage 62 a pressure gradient exists between the suction surface and the pressure surface. As depicted in
As well as drifting circumferentially towards the suction surface, the flow also experiences radial drift of the boundary layer from the tip of the vane passage towards the hub of the vane passage. The radial drift affects the quality and consistency of the flow over the surface of the prefilmer where the fuel is injected. Deviated and detached flow on the prefilmer leads to poor atomisation performance and high losses and higher than desired NOx results.
The vane configuration of the inner main swirler of the invention is depicted in more detail with reference to
Each of the vanes 50a . . . 50l comprises a leading edge 52, a trailing edge 54, a pressure flank 56 extending from the leading edge to the trailing edge and a suction flank (not shown) also extending from the leading edge to the trailing edge, and opposed to the pressure flank.
The vane follows a helix as the vane extends axially, the rotation of the helix occurring along a line that coincides with the radius of the swirler. Each of the leading edges 52 and trailing edges 54 is leant at an angle, with respect to the radius of the injector, between a hub 58 and a tip 60.
Leaning the vanes without adjusting the axial exit angle alleviates the radial pressure gradient without adjusting the permeability of the vanes. One of the effects of leaning the vanes is that radial lift is generated that balances the cross flow pressure gradients in the vane passage.
Cross-flow is generated within the boundary layer and at a ¼ of the vane length a cross-flow pressure gradient is evident. The cross-flow gradient at the tip is greater than the cross-flow gradient at the hub. By leaning the vanes towards the suction surface of an adjacent vane the relative static pressure is reduced and a less steep pressure curve is exhibited. The weaker pressure gradient diminishes the crossflow
The effect of introducing lean to the vane on the velocity of the air to the prefilmer is depicted in
It will be appreciated that the vane lean may be varied along its radial height. Such that the angle of lean near the hub is less than the angle of lean on portions of the vane further along the radius. Beneficially, the effect of adverse lean near the hub, where an increase in the pressure gradient is observed, is reduced.
Number | Date | Country | Kind |
---|---|---|---|
0611841.8 | Jun 2006 | GB | national |