The present disclosure concerns a gas turbine engine fan assembly, and a gas turbine engine comprising a fan assembly.
Turbofan engines comprise a fan and a core compressor. The fan is typically provided upstream of the compressor, and provides a portion of its exhaust air to the downstream compressor, with the remainder being bypassed around the compressor in a bypass duct. The fan comprises a plurality of blades attached to a hub. The compressor flow is drawn from the fan airflow adjacent the hub (also known as the “root” region). Air in this region comprises “clean” flow, which is substantially free from turbulence and travels in a generally axial direction, and “secondary flow”. Generally, secondary flow comprises flow which travels in a direction non-parallel with the main flow. For example, flow adjacent the fan root (so-called “boundary layer flow”) tends to be driven radially outwardly as it passes through the fan, before forming turbulent vortices. Compressors generally operate at higher efficiencies when ingesting clean air flow from an axial direction, rather than turbulent secondary flow.
Consequently, it is desirable to provide a fan assembly and a gas turbine engine configured to reduce delivery of secondary flow to downstream components.
According to a first aspect of the invention there is provided a fan assembly for a gas turbine engine, the assembly comprising:
a hub and a plurality of blades projecting from the hub;
wherein the hub comprises an inlet aperture located adjacent a blade root, the inlet aperture being in fluid communication with a passage extending along at least part of a span of the blade, wherein the passage communicates with an outlet provided on an exterior of the blade, radially outwardly of the inlet.
Advantageously, the inlet, passage and outlet provide a route for secondary air adjacent the hub, upstream of the blade root, thereby diverting the secondary flow away from the blade root. Since the passage extends through the interior of the blade, and extends in a radial direction, the blade acts as a centrifugal pump thereby energising the flow to draw in air flow, and increase its energy as it leaves the outlet.
The inlet may be provided adjacent one of a leading and a trailing edge of a blade root of one or more blades. A first inlet may be provided adjacent the leading edge of the blade root and a second inlet may be provided adjacent the trailing edge of the blade root.
The first inlet may be located axially forwardly of the leading edge of one or more blades at a circumferential position of the leading edge. Advantageously, secondary air is diverted from the leading edge of each fan blade. Alternatively or in addition, the first inlet may be provided circumferentially offset from the blade leading edges. The second inlet may be provided downstream of the first inlet. The second inlet may be provided in an inter-blade passage defined by opposing surfaces of adjacent blades. The second inlet may be provided downstream of a trailing edge of the blades.
The or each inlet may comprise one or more annular slots. Alternatively or in addition, the or each inlet may comprise a plurality of holes arranged in a generally circumferential extending row.
The outlet may be provided at a radial position such that, in use, air exiting from the outlet has a static pressure exceeding the static pressure of external air flow at the outlet.
The passage may extend in a generally radial direction, and the outlet may be provided adjacent a tip of the blade. Accordingly, the airflow from the passage may provide oppose tip leakage flows, thereby increasing the efficiency of the fan.
The outlet may be provided adjacent the leading edge of the respective blade, and may be provided at a pressure surface of the respective blade.
The outlet may comprise a slot, or may comprise a plurality of holes.
Alternatively, at least a portion of the passage may extend at least partially in an axial direction, and the outlet may be provided at a trailing edge of the respective blade.
Each respective blade may comprise a plurality of radially extending passages in fluid communication with the or each inlet. The radially extending passages may communicate with an axially extending outlet manifold.
The blades may comprise one or more of aluminium, titanium alloy and a composite material such as carbon fibre reinforced plastic (CFRP). Where the blades comprise titanium alloy, the blades may be formed by a superplastic diffusion bonding process (SPDFB).
The passage may extend within a hollow interior of the respective blade between the pressure and suction surfaces. Alternatively, the passage may comprise a blister located on a surface of the blade. The blister may extend from the pressure surface of the blade, or may extend from both the pressure and suction surface of the blade.
The blade may comprise a CFRP main body joined to a metallic leading edge. The passage may be located within one of the metallic leading edge, the CFRP main body, and the join between the leading edge and main body.
At least one of the inlets may comprise an inlet passage extending in a substantially axial direction. Consequently, the inlet passage ingests airflow into the inlet without significantly altering the flow direction of the secondary airflow. At least one of the inlets may comprise a vane which may project from the hub to guide air into the inlet.
The arrangement may comprise first and second inlets and an inlet manifold located within the blade hub, the inlet manifold being in fluid communication with the first and second inlets and at least one passage.
The outlet may be provided at a radial position of at least 30% of the span of the fan blade.
According to a second aspect of the present invention there is provided a gas turbine engine comprising a fan assembly in accordance with the first aspect of the invention.
The gas turbine engine may comprise a compressor having an air inlet located downstream of the fan assembly.
The gas turbine engine may comprise a bypass ratio greater than 10. At higher bypass ratios, a larger portion of the air entering the core will comprise secondary flow. Consequently, the compressor efficiency will be reduced, thereby negating some of the advantages of increased bypass ratio. The invention is therefore particularly beneficial at high bypass ratios, i.e. approximately 10 or greater.
The fan may have a pressure ratio in operation of between 1.2 and 1.6.
The outlet may be provided at a pressure surface of the blade, and may be configured to provide an outlet flow having a circumferential component directed toward an adjacent blade. Advantageously, flow from the outlet may oppose over-tip leakage flow, thereby reducing over-tip leakage, and enhancing fan efficiency, while also capturing secondary flow.
The skilled person will appreciate that except where mutually exclusive, a feature described in relation to any one of the above aspects of the invention may be applied mutatis mutandis to any other aspect of the invention.
Embodiments of the invention will now be described by way of example only, with reference to the Figures, in which:
With reference to
The gas turbine engine 10 works in the conventional manner so that air entering the intake 12 is accelerated by the fan 13 to produce two air flows; a first air flow A into the intermediate pressure compressor 14 and a second air flow B which passes through a bypass duct defined by an internal space between a radially inner side of the engine nacelle 49 and a radially outer side of a core nacelle 50 to provide propulsive thrust. The intermediate pressure compressor 14 compresses the air flow directed into it before delivering that air to the high pressure compressor 15 where further compression takes place. A ratio of air entering the engine core (i.e. the intermediate pressure compressor 14) to air bypassing the core defines an engine bypass ratio (i.e. mass flow of air flow B divided by mass flow of air flow A). In this example, the bypass ratio is approximately 10. It has been found that at bypass ratios of approximately 10 or greater, the invention is particularly effective, though it will be understood that the invention is also applicable to engines having lower bypass ratios.
The compressed air exhausted from the high-pressure compressor 15 is directed into the combustion equipment 16 where it is mixed with fuel and the mixture combusted. The resultant hot combustion products then expand through, and thereby drive the high, intermediate and low-pressure turbines 17, 18, 19 before being exhausted through the nozzle 20 to provide additional propulsive thrust. The high 17, intermediate 18 and low 19 pressure turbines drive respectively the high pressure compressor 15, intermediate pressure compressor 14 and fan 13, each by suitable interconnecting shafts. The compressors 14, 15, combustor 16 and turbines 17, 18, 19 are housed within the core nacelle 50. The core nacelle 50 defines a core inlet 38 at an axially forward end, and a core exhaust 23 at an axially rearward end.
The hub 22 is mounted to a low pressure shaft 28, which is in turn attached to the low pressure turbine 19. Consequently, the hub 22 is driven by the low pressure turbine 19. The blades 21 are each attached to a fan disc 28 by a fir tree mounting arrangement 29. The fan disc 28 is in turn attached to the hub 22, such that they rotate together.
The hub 22 comprises a first inlet aperture 30 provided on an external, radially outer surface thereon. The inlet aperture 30 extends through the external surface of the hub 22 into the hollow exterior therein. The inlet aperture 30 communicated with a passage 31 provided in the blade 21. The passage 31 extends from a radially inner end radially inwardly of the aerodynamic root 26, and radially outwardly of the fir tree mounting arrangement 29 within a hollow interior 53 of the blade 21.
The passage 31 extends generally radially outwardly from the inlet 30 part way along the span of the blade 21. In the embodiment shown in
For example, a propulsive fan 13 for a passenger airliner may have a diameter D of 2.5 m, a hub to tip ratio HTR of 0.3, and operate at a tip relative Mach number Mrel_tip of 1.3 with an axial Mach number Max of 0.6.
At operating altitude the static temperature T and pressure P may be 240K and 28150 Pa respectively, and the specific heat at constant pressure cp may be 1005 J/kg/K. The gas constant R for air is 287 J/kg/K, which gives the ratio of specific heats at constant pressure and volume γ as 1.4. Depending on the design requirements, the fan 13 would typically produce a pressure ratio of between 1.3 and 1.6.
The fan rotational speed ω is thus:
The total temperature rises as a result of the work input to the flow up the passage in the blade. A design choice must be made as to what radial position along the blade 21 the outlet 34 will be provided. Let the radial position of the outlet 34 as a fraction of the fan diameter D be denoted as X, with values between HTR and 1.0 being possible. The total temperature rise may then be determined as:
The maximum temperature rise occurs at X=1.0, and is 58K for the example presented here.
The total temperature is:
The total pressure is:
The pressure ratio imparted by this work input process can be determined by compressible flow relationships:
Consequently, in this example, the total pressure is 73197 Pa, so the total pressure rise is ˜37000 Pa.
Clearly, the above numbers describe the maximum achievable pressure rise within the fan blade passage. In practice, a smaller fraction of the pressure rise may be chosen and pressure losses will be generated at entrance, exit and within the fan blade passage 32.
Once the cross sectional area of the passage 32 within the fan blade and the desired mass flow are chosen, the pressure losses may be determined as follows.
A typical fan 13 may have twenty-two blades 21 with a maximum thickness of less than 20 mm. Let us assume a passage 32 with an area equivalent to a tube of half this diameter at d=10 mm or area ˜8×10−5 m2. Using a relationship for the pipe friction F such as that of Holbrook:
(With a representative roughness of 5×10−5 m and Reynolds number
The pressure drop due to friction in the pipe can be derived as:
Additional pressure losses can be anticipated at the entrance and exit of the flow passage 32. These may be accounted as a loss coefficient applied to the dynamic pressure:
ΔPloss=k(P0−P)
we will assume that all dynamic pressure at inlet is lost (kin=1.0) and a further 10% in the exit process (kex=0.1). For a representative flow of 0.03% of the full flow, these pressure losses would match the 37000 Pa pressure rise and allow a system capable of exhausting the flow at the tip 27 adjacent the leading edge 24. Increasing the available flow area within the fan blade 21 would increase the flow.
Taking a maximum possible area of the blade 21 as two triangles meeting at a maximum height at mid chord, a flow area increase of a factor of 20 and an associated flow increase up to 1.6% of the fan flow could be achievable.
Alternatively, using this maximum area, the 0.03% flow could be ejected at 30% of the blade height.
It will be understood that the invention could be applied to different diameter fans. For example, where the fan blades 13 have a diameter of 3 metres, then the flow would increase from 0.03% of full flow to 0.05% for the same diameter passages, in view of the increased pressure provided by the greater diameter. Similarly, for the maximum internal area case, the flow would increase from 1.65% of full flow to 2.1%. On the other hand, for a fan blade 21 having a diameter of 1 metre, 0.5% of the full flow could be provided using the whole internal area where the flow is ejected at the tip. Similarly, increasing the speed will also increase the available flow. For example, for the 2.5 metre fan blade diameter case, increasing the tip speed from Mach 1.3 to 1.5 will increase the flow from 0.03% to 0.05% for a single passage, or from 1.65% to 2.07% for the maximum available area case. On the other hand, reducing the tip speed to Mach 1.1 would reduce the flow from the single passage from 0.03% to 0.017% and would reduce the flow for the maximum area case from 1.65% to 1.25%.
The hub 22 further comprises a second inlet aperture 36 located adjacent the trailing edge 25 of the blade 21. The second inlet aperture 36 communicates with the first inlet aperture 30 via an inlet manifold 37 defined by a hollow region within the blade 21 between the aerodynamic root 26 and the fir tree mounting arrangement 29. Consequently, air is drawn from both the area adjacent the leading edge 24 of the blade 21, and the area adjacent the trailing edge 25 of the blade 21. Consequently, secondary flow adjacent the outer surface of the hub 22 is withdrawn, and so the aft ingested into the engine core has less turbulence, thereby improving core performance.
Each of the passages 331a-f terminates in a generally axially (i.e. chordally) extending outlet manifold 339 with which the passages 3311a-f are in fluid communication. The manifold 339 extends from substantially the leading edge 325 to the trailing edge 325 of the blade 321, and terminates in an outlet 335. The outlet 335 is located mid-way along the span of the blade 321, radially outwardly of the core inlet 38, adjacent the trailing edge 325. Consequently, the inlet apertures 330, 336 communicate with the outlet 335 via the inlet manifold 337, passages 331a-f and manifold 339 in flow sequence. Such an arrangement increases the internal space of the blade 21 used for the passages, and so increases the flow at the outlet 335. The passages 331a-f may be formed by spaces defined by an internal warren structure within the hollow blade 321. The warren structure comprises web members 354 which extend between the pressure and suction surfaces 323, 340 within the blade, to thereby providing internal bracing. The manifold 339 may comprise chordally extending apertures provided within the web members 354, to thereby interconnect the spaces.
Similarly, the second aperture 836 comprises a first lip 848 at an upstream end, which projects radially inwardly toward the inlet manifold 837. Again, the lip 848 reduces turning of the flow into the inlet manifold 837.
Consequently, this arrangement will oppose over-tip leakage, which otherwise tends to flow from the pressure side 1023 to the suction side 1040 of the blade 1021 at the tip 1024 in use. Such leakage will normally result in reduced fan efficiency. Consequently, by reducing over-tip leakage, fan efficiency can be increased. Alternatively or in addition, since fan leakage is related to the gap between the fan blade tip 1024 and the inner radius of the nacelle, this tip gap can be increased for a given fan tip leakage flow, leading to lower manufacturing costs.
It will be understood that the inlet apertures of any of
It will be understood that the invention is not limited to the embodiments above-described and various modifications and improvements can be made without departing from the concepts described herein. Except where mutually exclusive, any of the features may be employed separately or in combination with any other features and the disclosure extends to and includes all combinations and sub-combinations of one or more features described herein.
For example, the blade could be of carbon fibre construction, optionally comprising a metallic leading edge. In this case, the passage could be provided within a hollow metallic leading edge, or within a space defined by the join between the metallic leading edge and the main carbon fibre body.
It will be understood that the drawings are not to scale.
Number | Date | Country | Kind |
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1605323.3 | Mar 2016 | GB | national |