INLET CONE FOR AN AIRCRAFT TURBOMACHINE

Abstract

An inlet cone for an aircraft turbomachine, having at least one first portion made of a first material, referred to as rigid material, and at least one second portion made of a second material which has a hardness less than that of said first material and which is referred to as flexible material, these second portions being configured to deform elastically in the radial direction with respect to the axis when the cone is being driven to rotate.

Claims

1. An inlet cone for an aircraft turbomachine, this inlet cone being configured so as to be driven in rotation about an axis and comprising a body of conical or elliptical shape and on which ice is capable of forming, said body having at least one first portion made of a first material referred to as rigid material, and at least one second portion made of a second material which has a hardness less than that of said first material and which is referred to as flexible material, wherein said first portion is monobloc and formed by a plurality of axial sections connected together by partitions extending in a longitudinal direction relative to the axis, said sections and said partitions defining between them housings, and in that said body comprises a plurality of second portions located in said housings, these second portions being configured to deform elastically in the radial direction with respect to the axis when the cone is driven in rotation.

2. The inlet cone as claimed in claim 1, wherein said body comprises an end forming a tip made of said second material.

3. The inlet cone as claimed in claim 1, wherein each of the housings has a generally arcuate shape about the axis, and the second portions are configured to fill these housings completely.

4. The inlet cone according to claim 1, wherein each of the second portions has a Young's modulus of between 1 and 10 MPa, and preferably from 1 to 4 MPa.

5. The inlet cone according to claim 1, wherein each of the second portions has a maximum thickness of 4 mm, the thickness being measured in a longitudinal direction with respect to the axis.

6. The inlet cone according to claim 1, wherein each of the second portions comprises an external surface with a maximum radius (r) of 40 mm, the radius (r) being measured with respect to the axis.

7. The inlet cone according to claim 1, wherein each of the second portions has a density of between 500 and 1500 Kg/m.sup.3, and preferably 1200 Kg/m.sup.3.

8. The inlet cone according to claim 1, wherein each axial section is an angular sector of between 10 and 90?.

9. The inlet cone according to claim 1, wherein each second portion is made of elastomer, silicone, rubber or polytetrafluoroethylene.

10. The inlet cone according to claim 1, wherein said first portion is made of composite or metallic material, for example aluminium.

11. An aircraft turbomachine comprising an inlet cone according to claim 1.

12. A method for using a turbomachine according to claim 11, wherein said cone is rotated either at a first speed which is at least greater than 5000 rpm, or at a second speed which is lower than said first speed, and in that: when said cone rotates at the first speed, the second portions are configured to fragment ice (G) deposited on the cone, moving radially with respect to the axis, and when said cone is rotating at the second speed or at a standstill, the second portions are immobile.

13. The method according to claim 12, wherein the radial displacement of said flexible portions is greater than 0.02 mm, and preferably between 0.02 and 0.20 mm.

Description

BRIEF DESCRIPTION OF THE FIGURES

[0035] The invention will be better understood and other details, characteristics and advantages of the present invention will become clearer from the following description made by way of non-limiting example and with reference to the attached drawings, in which:

[0036] FIG. 1 is a schematic half-view of an aircraft turbomachine in axial cross-section, according to one of the embodiments of the invention,

[0037] FIG. 2a shows schematically a half-view in axial cross-section of an ice accretion on a prior art inlet cone,

[0038] FIG. 2b shows schematically a half-view in axial cross-section of a fragmentation of the ice from the inlet cone in FIG. 2a,

[0039] FIG. 2c shows schematically a half-view in axial cross-section of a detachment of randomly large pieces of ice from the inlet cone of FIG. 2a,

[0040] FIG. 3 is a schematic front perspective view of a prior art inlet cone,

[0041] FIG. 4 is a schematic front perspective view of an inlet cone according to a first embodiment of the invention,

[0042] FIG. 5a shows schematically a half-view in axial cross-section of an ice accretion on the entrance cone of FIG. 4,

[0043] FIG. 5b shows schematically a half-view in axial cross-section of a fragmentation of the ice from the inlet cone in FIG. 5,

[0044] FIG. 5c shows schematically a half-view in axial cross-section of a detachment of pieces of ice of controlled and reduced size from the inlet cone of FIG. 4,

[0045] FIG. 6 illustrates a graph showing a radial displacement of the second portions of the cone of the invention as a function of the rotation speeds of the cone.

DETAILED DESCRIPTION OF THE INVENTION

[0046] By convention in the present application, the terms inner and outer, and internal and external are defined radially with respect to a longitudinal axis X of the aircraft engine of the turbomachine. For example, a cylinder extending along the axis X comprises an inner face facing the axis of the engine and an outer surface opposite its inner surface. By Axial or axially is meant any direction parallel to the axis X, and transversely or transversal is meant any direction perpendicular to the axis X. Similarly, the terms upstream and downstream are defined in relation to the flow orientation of the air in the turbomachine.

[0047] FIG. 1 shows a turbomachine 1 of double flow, in particular for an aircraft. However, this is not a limit and the turbomachine may be of another type, such as a turboprop.

[0048] The turbomachine 1 extends along a longitudinal axis X and comprises from upstream to downstream, in the flow orientation of the gases, a fan 2, one or more compressor stages (for example a low-pressure compressor 3 and a high-pressure compressor 4), a combustion chamber 5, one or more turbine stages (for example a high-pressure turbine 6 and a low-pressure turbine 7), and an exhaust nozzle 8 for the gases. The fan 2, low-pressure compressor 3 and low-pressure turbine 7 are connected to a low-pressure shaft extending along a longitudinal axis. The high-pressure compressor 4 and high-pressure turbine 6 are connected to a high-pressure shaft arranged around the low-pressure shaft. The low-pressure turbine 7 drives the low-pressure shaft in rotation, while the high-pressure turbine 6 drives the high-pressure shaft in rotation.

[0049] The turbomachine 1 also comprises, upstream of the fan 2, an air inlet cone 10, 10 which is mounted on the fan 2 by means of a shell (not shown), preferably by bolt-type attachments. The shell is located downstream of the inlet cone 10, 10 and this shell is also connected to the low-pressure shaft.

[0050] The inlet cone 10, 10 together with the shell are connected to the rotor, in other words to the rotating parts of the turbomachine 1. The inlet cone 10, 10 therefore rotates around the longitudinal axis X.

[0051] FIGS. 2a, 2b, 2c and 3 illustrate the inlet cone 10 of the prior art, as described above, in the technical background of the present application.

[0052] FIG. 4 shows an inlet cone 10 according to the invention. This cone 10 is configured, on the one hand, to be driven in rotation about the axis X and, on the other hand, to fragment the ice accreted on the cone 10 into several pieces of calibrated size so as not to damage, in particular, the vanes of the fan 2.

[0053] To this end, the cone 10 comprises a cone-shaped body extending around an axis of revolution. This axis of revolution of the cone 10 corresponds to the axis X of the turbomachine.

[0054] The body of the cone 10 comprises a first portion 20 made of a first material referred to as rigid material.

[0055] The first portion 20 is in the form of a single, monobloc piece. The first portion 20 is formed by a plurality of axial sections 22 which are connected together by partitions 24. The partitions 24 extend in a longitudinal direction with respect to the axis X. The plurality of axial sections 22 may be formed by at least one upstream section 22a and one downstream section 22b. The upstream section 22a has a smaller diameter than the downstream section 22b. The plurality of sections 22 may also comprise one or more intermediate sections 22c interposed between the upstream 22a and downstream 22b sections. Each intermediate section 22c has a smaller diameter than the downstream section 22b and a larger diameter than the upstream section 22a.

[0056] In the example shown in FIG. 4, each section 22 comprises as many sectors as there are partitions 26 to which it is connected. Each sector of the section extends between two adjacent partitions.

[0057] The plurality of axial sections 22 and the partitions 24 define housings 26 between them. Each housing 26 can be an opening. In the example, each housing 26 may have a generally arcuate shape with respect to the axis X.

[0058] The first material can be a metallic material (such as aluminium) or a composite material.

[0059] The body of the cone 10 also comprises a number of second portions 30, each made from a second material referred to as flexible material. The second material has a lower hardness than the first material. For example, the hardness of the materials is defined by the Young's modulus.

[0060] Each second portion 30 may have a Young's modulus of between 1 and 10 MPa. Preferably, the Young's modulus of the second portions 30 is between 1 and 4 MPa.

[0061] Each second portion 30 may have a density of between 500 and 1500 Kg/m.sup.3. Preferably, the density is 1200 Kg/m.sup.3.

[0062] The second material can be an elastomer, silicone, rubber or polytetrafluoroethylene (PTFE).

[0063] The cone 10 can have a maximum radius of 50 cm.

[0064] In the example shown in FIG. 4, each second portion 30 is an angular sector. Each angular sector can be between 5 and 345?. The angular sector is preferably between 5 and 180?. Even more preferably, the angular sector is between 10 and 90?. The second portions 30 are located in the housings 26 in the first portion 20. In the example, the second portions 30 are spaced apart and separated from each other by at least one of the sections 22 and/or partitions 26. This gives the body of the cone 10 an alternating pattern, in particular between the sections 22 of the first portion 20 and the second portions 30 (in a longitudinal direction with respect to the axis X).

[0065] Each second portion 30 has a complementary shape to that of the corresponding housing 26. In this way, the second portions 30 are configured to completely fill the housings.

[0066] Each of the second portions 30 can have a maximum thickness E of 2 to 10 mm, preferably the thickness is 4 mm. The thickness E is measured in a longitudinal direction with respect to the axis X (FIG. 5a). The radial direction is substantially perpendicular to the axis X.

[0067] Each of the second portions 30 comprises an external surface 32 which can have a maximum radius r of 20 to 100 mm, preferably a radius of 40 mm. The radius r is measured in a radial direction with respect to the axis X (FIG. 5a).

[0068] The body of the cone 10 may comprise an end forming a tip 12. In the example, the tip 12 is made from the second material. Alternatively, the tip 12 is made from the first material, in which the tip 12 and the first portion 20 are monobloc.

[0069] The alternating pattern between the first and second materials according to the invention can be applied to any type of air inlet cone of a turbomachine, while adapting the angles and lengths of the tip according to the dimensions of the inlet cone. In addition, the hardness of the second material is a parameter that can vary according to the speed of rotation, the angle of attack and the dimensions of the inlet cone.

[0070] According to other variants not illustrated, the housings 26 can be a helical groove and the second portions 30 can have a spiral configuration, or longitudinal grooves and the second portions 30 can have a rectilinear shape. These variants also allow other patterns to be produced so that the first and second materials alternate on the body of the cone.

[0071] Generally speaking, the second portions 30 are capable of elastic deformation in the radial direction when the cone 10 is driven in rotation. This allows to generate stresses in the ice formed at the interface of the rigid and flexible materials, so as to fragment the ice into several pieces of calibrated size acceptable for an impact to the fan vanes 2. With reference to FIGS. 5a to 5c, the present application describes the ice fragmentation conferred by the specific configuration of the cone 10 of the invention.

[0072] When the turbomachine is running at steady state (i.e. at a speed of 3000 rpm or less), as shown in FIG. 2a, the ice G forms on the external surface of the inlet cone 10. When the cone 10 is rotated at a second speed V2 by the turbomachine, there is no relative movement between the rigid and flexible materials. The second portions 30 are therefore immobile.

[0073] When the cone 10 is rotated at a first speed V1 by the turbomachine, as shown in FIG. 5b, there is a deviation in deformation D (or displacement) under centrifugal force of the second portions 30 with respect to the first portion 20 in a radial direction with respect to the axis X. This deviation generates cracks which fragment the ice G at the interface between the rigid and flexible materials. This allows to fragment the ice G into several small pieces.

[0074] FIG. 5c illustrates the detachment of the pieces of ice, which are reduced in size so as not to damage the components downstream of the cone 10.

[0075] The first speed V1 may be at least 5000 rpm and the second speed V2 may be less than 5000 rpm.

[0076] The deformation deviation D (or the radial displacement) of the second portions is greater than 0.02 mm. Preferably, the deviation is between 0.02 and 0.20 mm.

[0077] The dimensions (shape, thickness, size, hardness, etc.) and the position on the body of the cone 10 of the housings 26 in the first portion 20 and in the second portions 30 can vary according to the desired size of the pieces of ice to be fragmented and the type of inlet cone.

[0078] When the cone 10 rotates at the second speed V2, the turbomachine can be accelerated to achieve the desired radial displacement of the second portions and achieve a fragmentation of the ice.

[0079] Advantageously, the radial displacement D of the second portions 30 of the cone 10 is proportional to at least one of the following dimensioning parameters: [0080] to the square of the speed of rotation of the cone 10, [0081] to the square of the thickness of the second portions 30, [0082] to the hardness of the second material, and at the distance of the second portions 30 from the axis X.

[0083] Thus, at least one of the aforementioned dimensioning parameters is modified to obtain a radial displacement of at least 0.02 mm on each of the second portions 30 and to break a maximum radial ice thickness of 15 mm on the cone 10, as summarised in the following table (Table 1) by way of example.

TABLE-US-00001 TABLE 1 Greater Greater Lower radius r radius r speed and and and Young's modified Young's Lower modulus thickness modulus Refer- speed and of the E of the of the ence modified second second second config- thickness modified flexible modified uration E material portion material Turbomachine 5000 37500 37500 5000 5000 speed (rpm) Young's 2.8 2.8 1.6 2.8 1.4 modulus of the second material (Mpa) Radial 4.0 5.3 4.0 2.8 4.0 thickness E second flexible portion (mm) Radius r of 40 40 40 80 80 the second flexible portion (mm) Density of the 1200 1200 1200 1200 1200 second flexible portion (Kg/m.sup.3)

[0084] By way of example, the radial displacement of the second portions 30 of the cone 10 of the invention is measured as a function of the speed of the turbomachine.

[0085] For this purpose, the cone 10 with a maximum radius of 40 mm comprises a first portion 20 made of metal (such as aluminium) and second portions 30 made of elastomer with a Shore hardness A of 50 (at a temperature of 23? C.). The radial displacements of the second portions were measured under centrifugal force and according to the presence or absence of ice at 5000 and 7500 rpm. For example, the radial thickness of the ice formed on the cone is around 10 mm.

[0086] These measurements of the radial displacement of the second portions 30 are summarised in the following table (Table 2).

TABLE-US-00002 TABLE 2 Radial displacements measured at the Maximum radial Turbomachine Ice presence interface of the rigid displacements speed on the and flexible materials measured (rpm) inlet cone (mm) (mm) 5000 Without ice 0.02 0.06 With ice 0.08 0.15 7500 Without ice 0.06 0.14 With ice 0.14 0.34

[0087] By way of example, FIG. 6 illustrates the effect of the radial displacement of the second portions 30 of the cone 10 of the invention on the fragmentation of ice accreted on the cone 10 (in particular, at the interface between the rigid and flexible materials), is determined as a function of the different rotational speeds of the cone 10 (and consequently of the turbomachine).

[0088] To achieve this, the cone 10 comprises a first portion 20 made of metal (such as aluminium) and second portions 30 made of elastomer. The elastomer has a Shore hardness A of 50 (at a temperature of 23? C.) and a density of 1200 Kg/m.sup.3. The second portions 30 are 4 mm thick. The second portion 30 of the body of the cone, which has an external surface with a larger diameter, has a radius of 40 mm.

[0089] The null speed correspond to the cone at a standstill, the stability speed correspond to approximately 3,000 rpm and the maximum speed (corresponding to an acceleration phase) are approximately 7,500 rpm.

[0090] In FIG. 6, the area Z1 corresponds to the radial displacements of the second portions of the cone, in which a fragmentation and a detachment of the pieces of ice with a reduced and acceptable size can be observed. This area Z1 extends between 0.02 and 0.06 mm. A clear fragmentation of the ice is therefore observed at the interface between the rigid and flexible materials, from a radial displacement of 0.02 mm.

[0091] In FIG. 6, the area Z2 corresponds to minimal displacement or no radial displacement of the second portions of the cone, in which a fragmentation and a detachment of the ice pieces are not observed.