US20210062829A1 - Fan nose cone and dynamic tuning of aircrafts - Google Patents
Fan nose cone and dynamic tuning of aircrafts Download PDFInfo
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- US20210062829A1 US20210062829A1 US16/583,995 US201916583995A US2021062829A1 US 20210062829 A1 US20210062829 A1 US 20210062829A1 US 201916583995 A US201916583995 A US 201916583995A US 2021062829 A1 US2021062829 A1 US 2021062829A1
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Images
Classifications
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- B—PERFORMING OPERATIONS; TRANSPORTING
- B64—AIRCRAFT; AVIATION; COSMONAUTICS
- B64D—EQUIPMENT FOR FITTING IN OR TO AIRCRAFT; FLIGHT SUITS; PARACHUTES; ARRANGEMENT OR MOUNTING OF POWER PLANTS OR PROPULSION TRANSMISSIONS IN AIRCRAFT
- B64D27/00—Arrangement or mounting of power plants in aircraft; Aircraft characterised by the type or position of power plants
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F04—POSITIVE - DISPLACEMENT MACHINES FOR LIQUIDS; PUMPS FOR LIQUIDS OR ELASTIC FLUIDS
- F04D—NON-POSITIVE-DISPLACEMENT PUMPS
- F04D29/00—Details, component parts, or accessories
- F04D29/66—Combating cavitation, whirls, noise, vibration or the like; Balancing
- F04D29/661—Combating cavitation, whirls, noise, vibration or the like; Balancing especially adapted for elastic fluid pumps
- F04D29/668—Combating cavitation, whirls, noise, vibration or the like; Balancing especially adapted for elastic fluid pumps damping or preventing mechanical vibrations
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B64—AIRCRAFT; AVIATION; COSMONAUTICS
- B64C—AEROPLANES; HELICOPTERS
- B64C11/00—Propellers, e.g. of ducted type; Features common to propellers and rotors for rotorcraft
- B64C11/02—Hub construction
- B64C11/14—Spinners
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B64—AIRCRAFT; AVIATION; COSMONAUTICS
- B64D—EQUIPMENT FOR FITTING IN OR TO AIRCRAFT; FLIGHT SUITS; PARACHUTES; ARRANGEMENT OR MOUNTING OF POWER PLANTS OR PROPULSION TRANSMISSIONS IN AIRCRAFT
- B64D27/00—Arrangement or mounting of power plants in aircraft; Aircraft characterised by the type or position of power plants
- B64D27/40—Arrangements for mounting power plants in aircraft
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F01—MACHINES OR ENGINES IN GENERAL; ENGINE PLANTS IN GENERAL; STEAM ENGINES
- F01D—NON-POSITIVE DISPLACEMENT MACHINES OR ENGINES, e.g. STEAM TURBINES
- F01D25/00—Component parts, details, or accessories, not provided for in, or of interest apart from, other groups
- F01D25/04—Antivibration arrangements
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F01—MACHINES OR ENGINES IN GENERAL; ENGINE PLANTS IN GENERAL; STEAM ENGINES
- F01D—NON-POSITIVE DISPLACEMENT MACHINES OR ENGINES, e.g. STEAM TURBINES
- F01D5/00—Blades; Blade-carrying members; Heating, heat-insulating, cooling or antivibration means on the blades or the members
- F01D5/02—Blade-carrying members, e.g. rotors
- F01D5/027—Arrangements for balancing
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F05—INDEXING SCHEMES RELATING TO ENGINES OR PUMPS IN VARIOUS SUBCLASSES OF CLASSES F01-F04
- F05D—INDEXING SCHEME FOR ASPECTS RELATING TO NON-POSITIVE-DISPLACEMENT MACHINES OR ENGINES, GAS-TURBINES OR JET-PROPULSION PLANTS
- F05D2260/00—Function
- F05D2260/96—Preventing, counteracting or reducing vibration or noise
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F16—ENGINEERING ELEMENTS AND UNITS; GENERAL MEASURES FOR PRODUCING AND MAINTAINING EFFECTIVE FUNCTIONING OF MACHINES OR INSTALLATIONS; THERMAL INSULATION IN GENERAL
- F16F—SPRINGS; SHOCK-ABSORBERS; MEANS FOR DAMPING VIBRATION
- F16F15/00—Suppression of vibrations in systems; Means or arrangements for avoiding or reducing out-of-balance forces, e.g. due to motion
- F16F15/32—Correcting- or balancing-weights or equivalent means for balancing rotating bodies, e.g. vehicle wheels
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02T—CLIMATE CHANGE MITIGATION TECHNOLOGIES RELATED TO TRANSPORTATION
- Y02T50/00—Aeronautics or air transport
- Y02T50/60—Efficient propulsion technologies, e.g. for aircraft
Definitions
- the application relates generally to optimization of vibration behaviour of aircrafts and, more particularly, to methods for tuning dynamic coupling of turbofan engines and aircrafts.
- a method of tuning dynamic coupling of an aircraft system comprising an airframe and a turbofan engine mounted thereto, the turbofan engine having an engine rotor including a nose cone, the method comprising: obtaining operational frequencies of the aircraft system, including at least one dominant frequencies range; determining a target resonant frequency of the turbofan engine different from that of the at least one dominant frequencies range of the aircraft system; and modifying a mass of the nose cone to achieve said target resonant frequency of the turbofan engine.
- a method for tuning a dynamic coupling of an airframe and a turbofan engine of an aircraft system the turbofan engine mounted to the airframe, the turbofan engine having at least one resonant frequency
- the method comprising: obtaining an aircraft system vibratory response, the aircraft system vibratory response defining a range of operational frequencies of the aircraft system, the turbofan engine having an fan and a baseline nose cone removably attached thereto; removing the baseline nose cone from the fan of the turbofan engine; and mounting a tuned nose cone to the fan of the turbofan engine in place of the baseline nose cone, the tuned nose cone having a mass greater than that of the baseline nose cone or a mass distribution different from that of the baseline nose cone to modify the at least one resonant frequency.
- FIG. 2 is a cross-sectional perspective view of an exemplary nose cone as used in the turbofan engine of FIG. 1 ;
- FIG. 3 is a block diagram illustrating an exemplary method for tuning engine/aircraft resonances, involving turbofan engines such as shown in FIG. 1 ;
- FIG. 4 is a block diagram illustrating another exemplary method for tuning dynamic coupling of an aircraft system, involving turbofan engines such as shown in FIG. 1 ;
- FIG. 5 is a cross-sectional perspective view of an exemplary nose cone as used for tuning engine/aircraft resonances of turbofan engines such as shown in FIG. 1 ;
- FIG. 6 is a cross-sectional perspective view of another exemplary nose cone as used for tuning engine/aircraft resonances of turbofan engines such as shown in FIG. 1 .
- FIG. 1 illustrates a gas turbine engine 10 of a type preferably provided for use in subsonic flight, generally comprising in serial flow communication a fan 12 through which ambient air is propelled, a multistage compressor section 14 for pressurizing the air, a combustor 16 in which the compressed air is mixed with fuel and ignited for generating an annular stream of hot combustion gases, and a turbine section 18 comprising one or more turbines for extracting energy from the combustion gases.
- the gas turbine engine 10 may be suitable for use in aircraft applications. More particularly, as illustrated, the gas turbine engine 10 is a turbofan engine.
- the gas turbine engine 10 comprises a central axis of rotation RA about which one or more spools of the gas turbine engine 10 may rotate.
- central axis of rotation RA may also correspond to (i.e., be coaxial with) a rotation axis of the fan 12 .
- the gas turbine engine 10 is schematically shown as part of an aircraft system 1 , which includes an airframe and which may include one or more of the engine(s) 10 dynamically coupled, as will be described later.
- the turbofan engine 10 includes an engine rotor 11 , in one or more sections, and/or a plurality of engine rotors 11 .
- the fan 12 may be considered part of the engine rotor 11 .
- the fan 12 is driven by an engine shaft (or simply the “engine rotor 11 ”) for rotation therewith about the rotation axis RA.
- the fan 12 comprises a plurality of circumferentially distributed fan blades 12 A, which may extend from a fan hub (not shown).
- the fan 12 may be disposed at or near an inlet of the gas turbine engine 10 and may be considered an inlet fan.
- the fan 12 may be considered as part of the compressor section 14 .
- the fan blades 12 A may be arranged as a circular array of radially extending fan blades 12 A in driving engagement with the engine rotor 11 , such as by being secured to the fan hub.
- the gas turbine engine 10 comprises a nose cone 20 .
- the nose cone 20 is mounted to the fan 12 , such as to be located upstream of the fan hub, for instance, and coaxial therewith.
- the nose cone 20 projects axially beyond the fan blades 12 A. In other words, the nose cone 20 extends axially upstream of the fan blades 12 A.
- the nose cone 20 may be secured to the fan hub for common rotation therewith.
- the nose cone 20 may also be referred to as “inlet cone” or “fan spinner” of the gas turbine engine 10 .
- the nose cone 20 may be integrally formed with the hub 12 B as a unitary construction, or the nose cone 20 may comprise a separately formed component or components (e.g., removably) secured individually or as an assembly to the fan hub according to any suitable method such as by a plurality of circumferentially-distributed fasteners (not shown).
- FIG. 2 illustrates an exemplary nose cone 20 according to an embodiment.
- the nose cone 20 has a conical body 21 including an outer wall 22 defining an outer surface 23 of the nose cone 20 for interfacing with a free stream of ambient air AMB (e.g., ram air) entering the gas turbine engine 10 during flight or other mode(s) of operation of the gas turbine engine 10 .
- AMB ambient air
- the outer surface 23 circumscribes (or defines a periphery of) a volume V of the nose cone 20 .
- the nose cone 20 defines an interior (i.e., an internal volume/space), which may also be referred to as a nose cone cavity 24 , at least partially enclosed by the outer wall 21 .
- the outer wall 21 is thin over a substantial portion of the outer wall 21 , and therefore it could be referred to as a nose cone shell.
- the nose cone volume may maximize an internal space (or simply stated, the nose cone cavity 24 ), which may in turn minimize the overall nose cone 20 weight. While it may be advantageous to minimize the nose cone weight, as is the normal trend for aviation applications, adding mass within the volume of the nose cone 20 may be desirable to place the engine rotor 11 resonance in an optimal frequency range. In other words, adding mass within the volume of the nose cone 20 may allow to adjust the natural frequencies (at least one, or more) of the gas turbine engine 10 . These and other aspects resulting from adding mass in the nose cone 20 are further discussed later.
- the depicted nose cone cavity 24 is in fluid communication with the free stream of ambient air AMB entering the gas turbine engine 10 , such as by one or more air inlet(s) 25 defined at the apex 26 of the nose cone 20 , as one possibility.
- Other configurations of the nose cone 20 may be contemplated, whether or not allowing fluid communication between the nose cone cavity 24 and the ambient air AMB upstream of the nose cone 20 and entering the gas turbine engine 10 , though fluid communication between the nose cone cavity 24 and the ambient air AMB upstream of the nose cone 20 may be desirable in most cases.
- the nose cone 20 is made of at least two separate components, which defines a base section 30 and a tip section 40 of the nose cone 20 .
- the nose cone body 21 may be formed of a single part, from the apex 26 to the fan hub (or equivalent) junction end 27 of the nose cone 20 .
- the tip section 40 defines the tip or apex 26 of the nose cone 20 .
- the base section 30 includes a connection interface at a junction end 27 (or simply the axial end) of the nose cone 20 , which may be configured for connection with the fan hub (or equivalent) or other component(s) of the engine rotor 11 .
- the base section 30 and the tip section 40 have interfacing flanges 31 , 41 located about their respective circumference and configured to interconnect the base section 30 and the tip section 40 to each other, via fasteners (not shown), or otherwise.
- the tip section 40 extends from the apex 26 to an axial distance X 1 from the apex 26 .
- Such axial distance X 1 is defined between the apex 26 and the junction end 27 of the nose cone 20 .
- the axial distance X 1 corresponds to the interfacing flange 41 .
- the base section 30 and the tip section 40 may thus be removably connected to each other, as opposed to forming a single rigid part. When assembled together the base section 30 and the tip section 40 may form a continuous outer surface 23 of the nose cone 20 , defining the nose cone “jacket” or periphery, which circumscribes the nose cone volume.
- Aircraft certification typically involves characterizing the dynamic behaviour of the aircraft, or stated differently the aircraft system 1 vibration response, including an airframe 2 with engines, such as gas turbine engines 10 , mounted thereon.
- the dynamic behaviour of an aircraft system 1 comprising one or more turbofan engine 10 can be determined using any suitable techniques, such as, without limitation, via ground vibration testing (GVT), which generally consist in defining the elastic and inertial characteristics of the aircraft system 1 .
- GVT ground vibration testing
- an analytical model may be conceived. Determining the aircraft system 1 vibration response may allow to identify the aircraft system 1 critical resonances, which are associated with dominant frequencies (or dominant frequencies ranges) of the aircraft system.
- the airframe 2 and engines 10 may be considered as an aircraft system 1 and the dynamic response of such aircraft system 1 may be optimized. In other words, during certification or post-certification, tuning of the dynamic coupling of the turbofan engine(s) 10 and aircraft (or together simply the “aircraft system 1 ”) may be desirable.
- frequencies are generated, due for instance to the rotation of the engine rotor 11 , aeroelastic effects, reciprocal motions of moving parts of the turbofan engine 10 , engine balance imperfections or slight misalignments of parts within the turbofan engine 10 , as a few examples.
- These frequencies hereinafter referred to as excitation frequencies of the turbofan engine 10 , may propagate in the whole aircraft system 1 , for instance through mounting supports of the engines on the airframe 2 , such as through the engine casing/housing to the wings (or aircraft tail) via engine supports.
- This frequency propagation may be impaired in many suitable ways, such as by adding dampers or other devices for reducing/damping vibrations in the engine supports, and/or by modifying engine components stiffness, such as the engine housing, for examples.
- Such excitation frequencies are typically evaluated during the engine design and certification process. However, such excitation frequencies may be unsuited to proper dynamic coupling of the engine(s) 10 with the airframe 2 .
- operational frequencies of the aircraft system 1 are obtained. This may allow aircraft systems manufacturers to determine the vibration behaviour of the aircraft system 1 . Operational frequencies of the aircraft system 1 may be obtained using any suitable vibration testing techniques, such as, without limitations, GVT as discussed above. With such operational frequencies of the aircraft system 1 obtained, intrinsic vibration characteristics of the aircraft system 1 may be determined. In other words, one may draw a portrait of the aircraft system 1 in the frequency domain, which may be used to validate analytical models of the aircraft systems. Obtaining the operational frequencies of the aircraft system 1 includes identifying one or more dominant frequencies (or dominant frequencies ranges) within the operational frequencies of the aircraft system 1 .
- the dominant frequencies (or dominant frequencies ranges) of the aircraft system 1 may often be associated with one or more main resonance modes of the engine 10 . These main resonance modes may correspond to the rotor critical speeds, which include compressor and turbine bounce modes.
- the one or more dominant frequencies are associated with first order resonance modes of the engine 10 . Such one or more dominant frequencies may be visualized on a Campbell diagram, which may also be commonly referred to as “Whirl Maps” diagram.
- the one or more dominant frequencies (or dominant frequencies ranges) may be considered as low frequencies (frequencies ranges), for instance lower than 60 Hz. Depending on the dynamic system, the one or more dominant frequencies may however be greater than 60 Hz, in some cases. This may be function of modal characteristics of the dynamic system.
- the main resonance modes of the engine 10 may be established (obtained) during engine 10 certification and their association with the modes of the aircraft system 1 may be evaluated through a ground vibration test of the aircraft system 1 .
- Aircraft systems 1 including at least an airframe 2 and at least one turbofan engine 10 may not be readily compatible dynamically once assembled together right off the manufacture.
- dynamic coupling of a specific turbofan engine 10 mounted to a specific airframe 2 may be optimized, which can in turn enhance the performance of the aircraft system 1 as a whole, and/or simply allow the aircraft system 1 to pass the certification processes and meet certification requirements.
- modifying engine components to selectively place the engine excitation frequencies in a most desirable place within the aircraft system 1 operational frequencies range may substantially affect design time and expenses.
- adjusting the natural frequencies of the turbofan engine(s) 10 may involve re-design of major parts or components of the aircraft and/or the turbofan engine(s) 10 , which may result in a major impact on design, testing, certification time and costs. Such re-design may require re-certification of the aircraft system 1 , for instance, which may be undesirable.
- adding mass in the nose cone 20 will affect (displace or attenuate) the natural frequencies of the engine(s) 10 .
- Adding mass in the nose cone 20 may provide an amplified ability to affect the natural frequencies of the turbofan engine(s) 10 and/or dynamic response of the aircraft system 1 as a whole, due for instance to that location of the added mass within the engine(s) 10 , without having to re-design other components of the engine(s) 10 , such as the engine housing, as a possibility.
- This specific area of the turbofan engine 10 is more easily accessible by an aircraft professional than other parts of the turbofan engine 10 , such as other portions of the turbofan engine 10 enclosed in a casing and/or parts of the turbofan engine 10 interfacing with the airframe 2 .
- Tuning the dynamic coupling of the turbofan engine(s) 10 and aircraft as described herein may advantageously be made without having to re-design major parts or components of the aircraft or engine(s) 10 . Accordingly, this may optimize a dynamic coupling of an aircraft system 1 without requiring re-certification of the aircraft system 1 .
- One purpose of tuning the dynamic coupling of the turbofan engine(s) 10 is to adjust the natural frequency of the rotor 11 , so that natural frequencies may be outside of a predetermined range frequencies. This may reduce, for instance, the likelihood that the rotor 11 will resonate, thereby reducing the vibratory stress experienced by the rotor 11 . Such purpose is different than when the objective is to balance the rotor 11 .
- One objective in balancing a rotor 11 is to align the actual axis of rotation with the desired axis of rotation, whereas the goal of tuning a rotor 11 is to adjust its natural frequency. Rotor balancing is about removing or reducing rotor eccentricities.
- a method for tuning a vibratory response of an aircraft system 1 is represented. As shown, the method is applied to an aircraft system 1 that includes an airframe 2 and at least one turbofan engine 10 mounted thereto.
- the turbofan engine 10 has an engine rotor 11 which includes a nose cone 20 .
- a range of frequencies (or a frequency) associated with at least one resonance mode of the aircraft system 1 is obtained.
- Mass is added in the nose cone to offset at least one dominant excitation frequency of the turbofan engine 10 outside the range of frequencies associated with the at least one resonance mode of the aircraft system 1 .
- FIG. 4 a method of tuning dynamic coupling of an aircraft system 1 comprising an airframe 2 and a turbofan engine 10 mounted thereto.
- the method is applied, similarly to what is represented in FIG. 3 , to an aircraft system 1 comprising an airframe 2 and a turbofan engine 10 mounted thereto, the turbofan engine 10 having an engine rotor 11 including a nose cone.
- the method includes obtaining operational frequencies of the aircraft system 1 , including one or more dominant frequencies ranges; determining a target resonant frequency of the turbofan engine 10 different from that of the one or more dominant frequencies ranges of the aircraft system 1 ; and modifying a mass of the nose cone to achieve said target resonant frequency of the turbofan engine 10 .
- adding mass may include obtaining an axially decreasing weight distribution of the nose cone such that weight of the nose cone is greater from the nose cone apex to an axial plane PA of the nose cone between the nose cone apex and the axial end of the nose cone than from said axial plane PA to the axial end.
- said axial plane PA is located at an axial distance X 1 from the apex corresponding to at least 1 ⁇ 3 but less than 2 ⁇ 3 of an overall length of the nose cone extending from the apex to the axial end of the nose cone, and obtaining the axially decreasing weight distribution of the nose cone includes distributing the weight of the nose cone such that the weight of the nose cone between the apex and the axial plane PA accounts for a majority of the weight of the nose cone. In some cases, obtaining the axially decreasing weight distribution of the nose cone includes distributing the weight of the nose cone such that the weight of the nose cone between the apex and the axial plane PA accounts for between about 50% to about 80% of the weight of the nose cone.
- obtaining the axially decreasing weight distribution of the nose cone includes distributing the weight of the nose cone such that the weight of the nose cone between the apex and the axial plane PA accounts is more than two times but less than three times the weight of the nose cone between the axial plane PA and the axial end of the nose cone.
- Other weight distributions may be contemplated in other embodiments, so long as the weight distribution of the nose cone allows for having the most weight at the most forward location relative to the fan 12 (or fan blades 12 A).
- the filling material MF may be of the same material than that of the outer wall 22 of the nose cone 20 .
- the filling material MF is integral with the outer wall 22 of the nose cone 20 .
- the outer wall 22 rather than being thin over a substantial portion of the tip section 40 such as to define a nose cone shell, forms a solid or thick structure having an irregular cross-sectional shape.
- Other configurations of the nose cone 20 may be contemplated, where, for instance, the outer wall 22 circumscribing the volume V of the nose cone 20 may be made of a different material than the filling material MF located within the volume V of the nose cone 20 , radially inwardly from the outer surface 23 of the nose cone 20 .
- a first portion 24 A of the nose cone cavity 24 may be circumscribed by the outer wall 22 portion forming the tip section 40 of the nose cone 20
- a second portion 24 B of the nose cone cavity 24 may be circumscribed by the outer wall 22 portion forming the base section 30 of the nose cone 20
- a portion 24 A of the nose cone cavity 24 may be within the volume of the tip section 40
- another portion 24 B of the nose cone cavity 24 may be within the volume of the base section 30 of the nose cone 20
- the portion 24 B of the nose cone cavity 24 of FIG. 5 is substantially similar to the one shown in FIG. 2 , differences are visible with respect to the portion 24 A of the nose cone cavity 20 .
- the portion 24 A of the nose cone cavity 20 in the tip section 40 defines a bullet-shaped feature.
- the portion 24 A of the nose cone cavity 24 is surrounded by the filling material MF in the tip section 40 , where the filling material MF defines the portion 24 A of the nose cone cavity 24 .
- the portion 24 A when viewed in a cross-section taken along the central axis AX of the nose cone 20 (see FIG. 5 ), the portion 24 A has a bullet-like shape. Other shapes may be contemplated in other embodiments.
- forming the annular mass within the nose cone may include defining an internal dome surface 42 in a foremost volume of the nose cone 20 , extending towards and merging into a tubular surface 43 such as to form a continuous surface therebetween, with the tubular surface 43 extending about the central axis AX of the nose cone 20 , where the central axis AX coincides with the rotation axis RA of the engine rotor 11 .
- forming the annular mass may include forming a second tubular surface extending about the central axis of the nose cone, the first and second tubular surfaces being concentric with one another.
- the first tubular section 44 and the second tubular section 47 merge into one another, thereby forming the shoulder 45 as a consequence of the difference in diameters D 1 , D 2 .
- the shoulder 45 extends radially normal to the central axis AX of the nose cone 20
- the shoulder 45 may be configured differently in other embodiments.
- Other geometries may be contemplated for the portion 24 A of the nose cone cavity 24 . For instance, there may be more or less tubular section(s) and/or cross-section(s) of the tubular section(s) may be different, such as square, hexagonal, or other geometrical shapes.
- the tip section 40 has an annular channel 48 defined therein, about at least part of the portion 24 A of the nose cone cavity 20 , shown herein about the second tubular section 47 at a radial distance R thereof.
- part of the filling material M is defined between the second tubular section 47 and the annular channel 48 .
- the portion 24 A of the nose cone cavity defines a bullet-shaped feature, with a first and a second tubular section 44 ′, 47 ′ extending along the central axis AX and coaxial with one another.
- the domed surface 42 ′ extends towards and merges into the first tubular surface 43 ′, with the first tubular surface 43 ′ defining the first tubular section 44 ′ having a diameter D 3 .
- the second tubular surface 46 ′ defines the second tubular section 47 ′.
- the first tubular section 44 ′ extends toward the shoulder 45 ′.
- the shoulder 45 ′ defines the junction between the first tubular section 44 ′ and the second tubular section 47 ′.
- the shoulder 45 ′ extends at an angle relative to the central axis AX of the nose cone 20 .
- the shoulder 45 ′ has a flared shape, such that the diameter of the shoulder 45 ′ increases toward the second tubular section 47 ′.
- the second tubular section 47 ′ has a diameter D 4 greater than the diameter D 3 of the first tubular section 44 ′.
- the shoulder 45 ′ does not transition directly from the first tubular surface 43 ′ to the second tubular surface 46 ′, or stated differently, from the diameter D 3 to the diameter D 4 .
- the filling material M providing added mass to the nose cone 20 may be obtained by manufacturing the tip section 40 from a plain block of material, by any suitable material removal techniques, such as machining, for example.
- the tip section 40 of the nose cone 20 may be manufactured using any suitable material additive manufacturing techniques, such as 3 D-printing, for instance.
- a method for tuning a dynamic coupling of an airframe 2 and turbofan engine 10 of an aircraft system 1 may be drawn from the above, according to another possibility. Said method may be implemented using the various embodiments discussed above.
- the turbofan engine 10 has an engine rotor 11 including a shaft and a baseline nose cone removably attached to the fan.
- the nose cone 20 is such as the one discussed above with respect to FIG. 2 .
- An aircraft system 1 vibration response is obtained, the aircraft system 1 vibratory response defining a range of operational frequencies of the aircraft system 1 .
- the baseline nose cone is then removed (removed or disassembled) from the fan of the turbofan engine 10 and a tuned nose cone is mounted to the fan in place of the baseline nose cone.
- Said tuned nose cone 20 may be in accordance with the embodiments discussed with respect to FIGS. 5 and 6 .
- the tuned nose cone thus have a greater weight than that of the baseline nose cone or a mass distribution different from that of the baseline nose cone.
- the tip section 40 instead of removing the whole baseline nose cone and replacing the baseline nose cone with a tuned nose cone, only one portion of the nose cone 20 may be removed, such as the tip section 40 , which for consistency with the present disclosure may be referred to as a baseline tip section, and replaced by a tuned tip section 40 having a mass greater than that of the baseline tip section 40 or a mass distribution different from that of the baseline tip section 40 .
- adding mass in the nose cone may include providing a tuned tip portion having a weight greater than that of the tip portion, the tuned tip portion adapted to replace the tip portion in place and connect to the remainder of the nose cone.
- the nose cone is formed of at least two separate parts removably connected to one another, a first one of the separate parts defining a tip portion (or section 40 ) of the nose cone and a second one of the separate parts defining a base portion (or section 30 ), the tip portion defining an apex of the nose cone, the base portion extending from the tip portion to an axial end of the nose cone
- adding mass in the nose cone includes providing a tuned tip portion having a weight greater than that of the tip portion in place, or a tuned tip portion having a different weight distribution than the tip portion in place.
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- Structures Of Non-Positive Displacement Pumps (AREA)
Abstract
A method for tuning a vibration response of an aircraft system is disclosed, where the aircraft system comprises an airframe and at least one engine dynamically coupled, the at least one engine having an engine rotor including a nose cone. The method comprises obtaining a range of frequencies associated with at least one resonance mode of the aircraft system and adding mass within the nose cone to offset at least one dominant excitation frequency of the turbofan engine outside the range of frequencies associated with the at least one resonance mode of the aircraft system. A method of tuning dynamic coupling of an aircraft system comprising an airframe and an engine mounted thereto is also disclosed.
Description
- The present application claims priority on U.S. Patent Application No. 62/892,156 filed Aug. 27, 2019, the entire content of which is incorporated herein by reference.
- The application relates generally to optimization of vibration behaviour of aircrafts and, more particularly, to methods for tuning dynamic coupling of turbofan engines and aircrafts.
- During normal operating conditions of an aircraft, vibratory phenomenon are generated, for instance via relative movements between moving and/or assembled components of the aircraft, such as rotating components of engines, and/or via aeroelastic effects on the aircraft. During certification of an aircraft, the dynamic behaviour of aircrafts including the airframe and engines, such as turbofan engines, is typically characterized. Incompatibilities in dynamic coupling between an aircraft and engine(s) may affect the overall performance, stability and/or durability of aircraft components(s) or the aircraft as a whole, and/or affect the comfort of occupants of the aircraft during normal operating conditions of the aircraft, such as during flight.
- In one aspect, there is provided a method for tuning a vibratory response of an aircraft system comprising an airframe and at least one turbofan engine dynamically coupled, the at least one turbofan engine having an engine rotor including a nose cone, the method comprising: obtaining a range of frequencies associated with at least one resonance mode of the aircraft system; and adding mass within the nose cone to offset at least one dominant excitation frequency of the turbofan engine outside the range of frequencies associated with the at least one resonance mode of the aircraft system.
- In another aspect, there is provided a method of tuning dynamic coupling of an aircraft system comprising an airframe and a turbofan engine mounted thereto, the turbofan engine having an engine rotor including a nose cone, the method comprising: obtaining operational frequencies of the aircraft system, including at least one dominant frequencies range; determining a target resonant frequency of the turbofan engine different from that of the at least one dominant frequencies range of the aircraft system; and modifying a mass of the nose cone to achieve said target resonant frequency of the turbofan engine.
- In a further aspect, there is provided a method for tuning a dynamic coupling of an airframe and a turbofan engine of an aircraft system, the turbofan engine mounted to the airframe, the turbofan engine having at least one resonant frequency, the method comprising: obtaining an aircraft system vibratory response, the aircraft system vibratory response defining a range of operational frequencies of the aircraft system, the turbofan engine having an fan and a baseline nose cone removably attached thereto; removing the baseline nose cone from the fan of the turbofan engine; and mounting a tuned nose cone to the fan of the turbofan engine in place of the baseline nose cone, the tuned nose cone having a mass greater than that of the baseline nose cone or a mass distribution different from that of the baseline nose cone to modify the at least one resonant frequency.
- Reference is now made to the accompanying figures in which:
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FIG. 1 is a schematic cross-sectional view of a turbofan engine; -
FIG. 2 is a cross-sectional perspective view of an exemplary nose cone as used in the turbofan engine ofFIG. 1 ; -
FIG. 3 is a block diagram illustrating an exemplary method for tuning engine/aircraft resonances, involving turbofan engines such as shown inFIG. 1 ; -
FIG. 4 is a block diagram illustrating another exemplary method for tuning dynamic coupling of an aircraft system, involving turbofan engines such as shown inFIG. 1 ; -
FIG. 5 is a cross-sectional perspective view of an exemplary nose cone as used for tuning engine/aircraft resonances of turbofan engines such as shown inFIG. 1 ; and -
FIG. 6 is a cross-sectional perspective view of another exemplary nose cone as used for tuning engine/aircraft resonances of turbofan engines such as shown inFIG. 1 . -
FIG. 1 illustrates agas turbine engine 10 of a type preferably provided for use in subsonic flight, generally comprising in serial flow communication afan 12 through which ambient air is propelled, amultistage compressor section 14 for pressurizing the air, acombustor 16 in which the compressed air is mixed with fuel and ignited for generating an annular stream of hot combustion gases, and aturbine section 18 comprising one or more turbines for extracting energy from the combustion gases. Thegas turbine engine 10 may be suitable for use in aircraft applications. More particularly, as illustrated, thegas turbine engine 10 is a turbofan engine. Thegas turbine engine 10 comprises a central axis of rotation RA about which one or more spools of thegas turbine engine 10 may rotate. In some embodiments, central axis of rotation RA may also correspond to (i.e., be coaxial with) a rotation axis of thefan 12. Thegas turbine engine 10 is schematically shown as part of anaircraft system 1, which includes an airframe and which may include one or more of the engine(s) 10 dynamically coupled, as will be described later. - The
turbofan engine 10 includes anengine rotor 11, in one or more sections, and/or a plurality ofengine rotors 11. Thefan 12 may be considered part of theengine rotor 11. Thefan 12 is driven by an engine shaft (or simply the “engine rotor 11”) for rotation therewith about the rotation axis RA. Thefan 12 comprises a plurality of circumferentially distributedfan blades 12A, which may extend from a fan hub (not shown). Thefan 12 may be disposed at or near an inlet of thegas turbine engine 10 and may be considered an inlet fan. Thefan 12 may be considered as part of thecompressor section 14. Thefan blades 12A may be arranged as a circular array of radially extendingfan blades 12A in driving engagement with theengine rotor 11, such as by being secured to the fan hub. As shown inFIG. 1 , thegas turbine engine 10 comprises anose cone 20. Thenose cone 20 is mounted to thefan 12, such as to be located upstream of the fan hub, for instance, and coaxial therewith. The nose cone 20 projects axially beyond thefan blades 12A. In other words, thenose cone 20 extends axially upstream of thefan blades 12A. In some embodiments, thenose cone 20 may be secured to the fan hub for common rotation therewith. Thenose cone 20 may also be referred to as “inlet cone” or “fan spinner” of thegas turbine engine 10. Thenose cone 20 may be integrally formed with the hub 12B as a unitary construction, or thenose cone 20 may comprise a separately formed component or components (e.g., removably) secured individually or as an assembly to the fan hub according to any suitable method such as by a plurality of circumferentially-distributed fasteners (not shown). -
FIG. 2 illustrates anexemplary nose cone 20 according to an embodiment. There is shown a cross-section of thenose cone 20 taken along a central axis AX of thenose cone 20. Thenose cone 20 has aconical body 21 including anouter wall 22 defining anouter surface 23 of thenose cone 20 for interfacing with a free stream of ambient air AMB (e.g., ram air) entering thegas turbine engine 10 during flight or other mode(s) of operation of thegas turbine engine 10. Theouter surface 23 circumscribes (or defines a periphery of) a volume V of thenose cone 20. - The
nose cone 20 defines an interior (i.e., an internal volume/space), which may also be referred to as anose cone cavity 24, at least partially enclosed by theouter wall 21. In the depicted embodiment, theouter wall 21 is thin over a substantial portion of theouter wall 21, and therefore it could be referred to as a nose cone shell. As such, the nose cone volume may maximize an internal space (or simply stated, the nose cone cavity 24), which may in turn minimize theoverall nose cone 20 weight. While it may be advantageous to minimize the nose cone weight, as is the normal trend for aviation applications, adding mass within the volume of thenose cone 20 may be desirable to place theengine rotor 11 resonance in an optimal frequency range. In other words, adding mass within the volume of thenose cone 20 may allow to adjust the natural frequencies (at least one, or more) of thegas turbine engine 10. These and other aspects resulting from adding mass in thenose cone 20 are further discussed later. - With continued reference to
FIG. 2 , the depictednose cone cavity 24 is in fluid communication with the free stream of ambient air AMB entering thegas turbine engine 10, such as by one or more air inlet(s) 25 defined at theapex 26 of thenose cone 20, as one possibility. Other configurations of thenose cone 20 may be contemplated, whether or not allowing fluid communication between thenose cone cavity 24 and the ambient air AMB upstream of thenose cone 20 and entering thegas turbine engine 10, though fluid communication between thenose cone cavity 24 and the ambient air AMB upstream of thenose cone 20 may be desirable in most cases. - In the depicted embodiment, the
nose cone 20, more specifically thenose cone body 21, is made of at least two separate components, which defines abase section 30 and atip section 40 of thenose cone 20. This is only one possibility, as thenose cone body 21 may be formed of a single part, from theapex 26 to the fan hub (or equivalent)junction end 27 of thenose cone 20. Thetip section 40 defines the tip orapex 26 of thenose cone 20. As shown, thebase section 30 includes a connection interface at a junction end 27 (or simply the axial end) of thenose cone 20, which may be configured for connection with the fan hub (or equivalent) or other component(s) of theengine rotor 11. As shown, thebase section 30 and thetip section 40 have interfacingflanges base section 30 and thetip section 40 to each other, via fasteners (not shown), or otherwise. Thetip section 40 extends from theapex 26 to an axial distance X1 from theapex 26. Such axial distance X1 is defined between theapex 26 and thejunction end 27 of thenose cone 20. In the depicted embodiment, the axial distance X1 corresponds to theinterfacing flange 41. Thebase section 30 and thetip section 40 may thus be removably connected to each other, as opposed to forming a single rigid part. When assembled together thebase section 30 and thetip section 40 may form a continuousouter surface 23 of thenose cone 20, defining the nose cone “jacket” or periphery, which circumscribes the nose cone volume. - Aircraft certification typically involves characterizing the dynamic behaviour of the aircraft, or stated differently the
aircraft system 1 vibration response, including anairframe 2 with engines, such asgas turbine engines 10, mounted thereon. The dynamic behaviour of anaircraft system 1 comprising one ormore turbofan engine 10 can be determined using any suitable techniques, such as, without limitation, via ground vibration testing (GVT), which generally consist in defining the elastic and inertial characteristics of theaircraft system 1. Prior of after performing such testings, an analytical model may be conceived. Determining theaircraft system 1 vibration response may allow to identify theaircraft system 1 critical resonances, which are associated with dominant frequencies (or dominant frequencies ranges) of the aircraft system. Theairframe 2 andengines 10 may be considered as anaircraft system 1 and the dynamic response ofsuch aircraft system 1 may be optimized. In other words, during certification or post-certification, tuning of the dynamic coupling of the turbofan engine(s) 10 and aircraft (or together simply the “aircraft system 1”) may be desirable. - During operation of the
turbofan engine 10, frequencies are generated, due for instance to the rotation of theengine rotor 11, aeroelastic effects, reciprocal motions of moving parts of theturbofan engine 10, engine balance imperfections or slight misalignments of parts within theturbofan engine 10, as a few examples. These frequencies, hereinafter referred to as excitation frequencies of theturbofan engine 10, may propagate in thewhole aircraft system 1, for instance through mounting supports of the engines on theairframe 2, such as through the engine casing/housing to the wings (or aircraft tail) via engine supports. This frequency propagation may be impaired in many suitable ways, such as by adding dampers or other devices for reducing/damping vibrations in the engine supports, and/or by modifying engine components stiffness, such as the engine housing, for examples. Such excitation frequencies are typically evaluated during the engine design and certification process. However, such excitation frequencies may be unsuited to proper dynamic coupling of the engine(s) 10 with theairframe 2. - During or in association with the
engine 10 and aircraft certification process, operational frequencies of theaircraft system 1 are obtained. This may allow aircraft systems manufacturers to determine the vibration behaviour of theaircraft system 1. Operational frequencies of theaircraft system 1 may be obtained using any suitable vibration testing techniques, such as, without limitations, GVT as discussed above. With such operational frequencies of theaircraft system 1 obtained, intrinsic vibration characteristics of theaircraft system 1 may be determined. In other words, one may draw a portrait of theaircraft system 1 in the frequency domain, which may be used to validate analytical models of the aircraft systems. Obtaining the operational frequencies of theaircraft system 1 includes identifying one or more dominant frequencies (or dominant frequencies ranges) within the operational frequencies of theaircraft system 1. The dominant frequencies (or dominant frequencies ranges) of theaircraft system 1 may often be associated with one or more main resonance modes of theengine 10. These main resonance modes may correspond to the rotor critical speeds, which include compressor and turbine bounce modes. The one or more dominant frequencies are associated with first order resonance modes of theengine 10. Such one or more dominant frequencies may be visualized on a Campbell diagram, which may also be commonly referred to as “Whirl Maps” diagram. In some embodiments, the one or more dominant frequencies (or dominant frequencies ranges) may be considered as low frequencies (frequencies ranges), for instance lower than 60 Hz. Depending on the dynamic system, the one or more dominant frequencies may however be greater than 60 Hz, in some cases. This may be function of modal characteristics of the dynamic system. The main resonance modes of theengine 10 may be established (obtained) duringengine 10 certification and their association with the modes of theaircraft system 1 may be evaluated through a ground vibration test of theaircraft system 1. - It may be desirable to have at least one or more dominant ones of the engine excitation frequencies offset (offset in the frequency domain) or dissociated from at least the one or more main resonance modes of the
aircraft system 1. This may prevent or otherwise limitaircraft system 1 dynamic instabilities and/or durability, for instance due to vibrations or portions of the aircraft entering into resonance (e.g. entering momentarily into one or more modes of resonance). -
Aircraft systems 1 including at least anairframe 2 and at least oneturbofan engine 10 may not be readily compatible dynamically once assembled together right off the manufacture. In other words, dynamic coupling of aspecific turbofan engine 10 mounted to aspecific airframe 2 may be optimized, which can in turn enhance the performance of theaircraft system 1 as a whole, and/or simply allow theaircraft system 1 to pass the certification processes and meet certification requirements. - Due to engine and aircraft certification process and requirements, modifying engine components to selectively place the engine excitation frequencies in a most desirable place within the
aircraft system 1 operational frequencies range, which may be referred to as the vibratory response of the aircraft, may substantially affect design time and expenses. In other words, adjusting the natural frequencies of the turbofan engine(s) 10 may involve re-design of major parts or components of the aircraft and/or the turbofan engine(s) 10, which may result in a major impact on design, testing, certification time and costs. Such re-design may require re-certification of theaircraft system 1, for instance, which may be undesirable. As mentioned above, adding mass in thenose cone 20 will affect (displace or attenuate) the natural frequencies of the engine(s) 10. Adding mass in thenose cone 20 may provide an amplified ability to affect the natural frequencies of the turbofan engine(s) 10 and/or dynamic response of theaircraft system 1 as a whole, due for instance to that location of the added mass within the engine(s) 10, without having to re-design other components of the engine(s) 10, such as the engine housing, as a possibility. This specific area of theturbofan engine 10 is more easily accessible by an aircraft professional than other parts of theturbofan engine 10, such as other portions of theturbofan engine 10 enclosed in a casing and/or parts of theturbofan engine 10 interfacing with theairframe 2. - Tuning the dynamic coupling of the turbofan engine(s) 10 and aircraft as described herein may advantageously be made without having to re-design major parts or components of the aircraft or engine(s) 10. Accordingly, this may optimize a dynamic coupling of an
aircraft system 1 without requiring re-certification of theaircraft system 1. - One purpose of tuning the dynamic coupling of the turbofan engine(s) 10 is to adjust the natural frequency of the
rotor 11, so that natural frequencies may be outside of a predetermined range frequencies. This may reduce, for instance, the likelihood that therotor 11 will resonate, thereby reducing the vibratory stress experienced by therotor 11. Such purpose is different than when the objective is to balance therotor 11. One objective in balancing arotor 11 is to align the actual axis of rotation with the desired axis of rotation, whereas the goal of tuning arotor 11 is to adjust its natural frequency. Rotor balancing is about removing or reducing rotor eccentricities. These eccentricities cause vibration in theengine 10 as a whole, but have little to no effect on the natural frequency(ies) of therotor 11. The purpose of weight balancing arotor 11 is to align the actual rotor axis (i.e. its inertial axis) to the physical centerline of therotor 11. The misalignment in the actual versus desired axis causes an imbalance. This imbalance manifests itself as a vibration which occurs with each revolution of therotor 11. Reducing these vibrations is not considered, by those skilled in the art, to be the same as tuning therotor 11. - Referring to
FIG. 3 , a method for tuning a vibratory response of anaircraft system 1 is represented. As shown, the method is applied to anaircraft system 1 that includes anairframe 2 and at least oneturbofan engine 10 mounted thereto. Theturbofan engine 10 has anengine rotor 11 which includes anose cone 20. A range of frequencies (or a frequency) associated with at least one resonance mode of theaircraft system 1 is obtained. Mass is added in the nose cone to offset at least one dominant excitation frequency of theturbofan engine 10 outside the range of frequencies associated with the at least one resonance mode of theaircraft system 1. - Referring to
FIG. 4 , a method of tuning dynamic coupling of anaircraft system 1 comprising anairframe 2 and aturbofan engine 10 mounted thereto. As shown, the method is applied, similarly to what is represented inFIG. 3 , to anaircraft system 1 comprising anairframe 2 and aturbofan engine 10 mounted thereto, theturbofan engine 10 having anengine rotor 11 including a nose cone. The method includes obtaining operational frequencies of theaircraft system 1, including one or more dominant frequencies ranges; determining a target resonant frequency of theturbofan engine 10 different from that of the one or more dominant frequencies ranges of theaircraft system 1; and modifying a mass of the nose cone to achieve said target resonant frequency of theturbofan engine 10. - Depending on the embodiments, adding mass in the nose cone may include different
nose cone cavity 24 shapes, volumes, and/or geometries and/or weight distribution. Various embodiments of the nose cone with added mass are discussed later below. As will become apparent from the description of these various embodiments, in some cases adding mass includes evenly distributing said added mass about the rotation axis of theengine rotor 11 within a volume of the nose cone. - In some embodiments, adding mass may include obtaining an axially decreasing weight distribution of the nose cone such that weight of the nose cone is greater from the nose cone apex to an axial plane PA of the nose cone between the nose cone apex and the axial end of the nose cone than from said axial plane PA to the axial end. In a particular embodiment, said axial plane PA is located at an axial distance X1 from the apex corresponding to at least ⅓ but less than ⅔ of an overall length of the nose cone extending from the apex to the axial end of the nose cone, and obtaining the axially decreasing weight distribution of the nose cone includes distributing the weight of the nose cone such that the weight of the nose cone between the apex and the axial plane PA accounts for a majority of the weight of the nose cone. In some cases, obtaining the axially decreasing weight distribution of the nose cone includes distributing the weight of the nose cone such that the weight of the nose cone between the apex and the axial plane PA accounts for between about 50% to about 80% of the weight of the nose cone. In some cases, obtaining the axially decreasing weight distribution of the nose cone includes distributing the weight of the nose cone such that the weight of the nose cone between the apex and the axial plane PA accounts is more than two times but less than three times the weight of the nose cone between the axial plane PA and the axial end of the nose cone. Other weight distributions may be contemplated in other embodiments, so long as the weight distribution of the nose cone allows for having the most weight at the most forward location relative to the fan 12 (or
fan blades 12A). - Referring to
FIG. 5 , anexemplary nose cone 20 with added mass is shown. In the depicted embodiment, thenose cone 20 shares similar features as those discussed above and therefore such features will not be described again. - In the depicted embodiment, the
nose cone 20 has an added mass defined at a frontmost portion thereof. The volume of thenose cone cavity 24 is reduced when compared to the embodiment shown inFIG. 2 . As such, in such embodiment, adding mass includes forming an annular mass within a volume of the nose cone, the annular mass defining aninternal cavity 24 of the nose cone. More particularly, in the depicted embodiment, a substantial portion of the overall volume V1 of thetip section 40 of thenose cone 20 is filled with material MF. Such material MF may be foam, such as a metallic foam as one possibility, titanium, aluminium as other possibilities. Other materials, including other types of materials, may be contemplated in other embodiments. - In the depicted embodiment, the filling material MF may be of the same material than that of the
outer wall 22 of thenose cone 20. In the embodiment shown, the filling material MF is integral with theouter wall 22 of thenose cone 20. In other words, theouter wall 22, rather than being thin over a substantial portion of thetip section 40 such as to define a nose cone shell, forms a solid or thick structure having an irregular cross-sectional shape. Other configurations of thenose cone 20 may be contemplated, where, for instance, theouter wall 22 circumscribing the volume V of thenose cone 20 may be made of a different material than the filling material MF located within the volume V of thenose cone 20, radially inwardly from theouter surface 23 of thenose cone 20. - A
first portion 24A of thenose cone cavity 24 may be circumscribed by theouter wall 22 portion forming thetip section 40 of thenose cone 20, whereas asecond portion 24B of thenose cone cavity 24 may be circumscribed by theouter wall 22 portion forming thebase section 30 of thenose cone 20. In other words, aportion 24A of thenose cone cavity 24 may be within the volume of thetip section 40, and anotherportion 24B of thenose cone cavity 24 may be within the volume of thebase section 30 of thenose cone 20. While theportion 24B of thenose cone cavity 24 ofFIG. 5 is substantially similar to the one shown inFIG. 2 , differences are visible with respect to theportion 24A of thenose cone cavity 20. With continued reference toFIG. 5 , theportion 24A of thenose cone cavity 20 in thetip section 40 defines a bullet-shaped feature. In other words, theportion 24A of thenose cone cavity 24 is surrounded by the filling material MF in thetip section 40, where the filling material MF defines theportion 24A of thenose cone cavity 24. In the embodiment shown, when viewed in a cross-section taken along the central axis AX of the nose cone 20 (seeFIG. 5 ), theportion 24A has a bullet-like shape. Other shapes may be contemplated in other embodiments. - More particularly, in the embodiment shown, a foremost area of the
portion 24A defines aninternal dome surface 42, which may also be referred to as an hemispherical surface. Theinternal dome surface 42 extends towards and merges into a firsttubular surface 43, here a cylindrical surface, such as to form a continuous surface therebetween, with such firsttubular surface 43 extending about the central axis AX of thenose cone 20. As such, forming the annular mass within the nose cone may include defining aninternal dome surface 42 in a foremost volume of thenose cone 20, extending towards and merging into atubular surface 43 such as to form a continuous surface therebetween, with thetubular surface 43 extending about the central axis AX of thenose cone 20, where the central axis AX coincides with the rotation axis RA of theengine rotor 11. - The first
tubular surface 43 defines atubular section 44, here in the form of a cylinder having a diameter D1. The firsttubular surface 43 extends axially from thedome surface 42 to ashoulder 45, theshoulder 45 defining an axial junction between the firsttubular surface 43 and a secondtubular surface 46. Thetubular section 44 may be referred to as a first tubular section, with the secondtubular surface 46 defining a secondtubular section 47, here in the form of a cylinder having a diameter D2 greater than the diameter D1. In other words, the firsttubular section 44 and the secondtubular section 47 are concentric with one another, both extending along the central axis AX of thenose cone 20. As such, forming the annular mass may include forming a second tubular surface extending about the central axis of the nose cone, the first and second tubular surfaces being concentric with one another. The firsttubular section 44 and the secondtubular section 47 merge into one another, thereby forming theshoulder 45 as a consequence of the difference in diameters D1, D2. While in the embodiment shown theshoulder 45 extends radially normal to the central axis AX of thenose cone 20, theshoulder 45 may be configured differently in other embodiments. Other geometries may be contemplated for theportion 24A of thenose cone cavity 24. For instance, there may be more or less tubular section(s) and/or cross-section(s) of the tubular section(s) may be different, such as square, hexagonal, or other geometrical shapes. - In the embodiment shown, the
tip section 40 has anannular channel 48 defined therein, about at least part of theportion 24A of thenose cone cavity 20, shown herein about the secondtubular section 47 at a radial distance R thereof. In other words, part of the filling material M is defined between the secondtubular section 47 and theannular channel 48. - Referring to
FIG. 6 , there is shown anotherexemplary nose cone 20, with similar features to those discussed above with respect to other embodiments, and therefore similar features will not be described again hereinafter. In the depicted embodiment ofFIG. 6 , theportion 24A of the nose cone cavity defines a bullet-shaped feature, with a first and a secondtubular section 44′, 47′ extending along the central axis AX and coaxial with one another. Thedomed surface 42′ extends towards and merges into the firsttubular surface 43′, with the firsttubular surface 43′ defining the firsttubular section 44′ having a diameter D3. The secondtubular surface 46′ defines the secondtubular section 47′. - In the depicted embodiment, the first
tubular section 44′ extends toward theshoulder 45′. As shown, theshoulder 45′ defines the junction between the firsttubular section 44′ and the secondtubular section 47′. Theshoulder 45′ extends at an angle relative to the central axis AX of thenose cone 20. Theshoulder 45′ has a flared shape, such that the diameter of theshoulder 45′ increases toward the secondtubular section 47′. The secondtubular section 47′ has a diameter D4 greater than the diameter D3 of the firsttubular section 44′. In the embodiment shown, theshoulder 45′ does not transition directly from the firsttubular surface 43′ to the secondtubular surface 46′, or stated differently, from the diameter D3 to the diameter D4. As shown, a diameter D5 of theshoulder 45′ at the junction with the secondtubular section 47′ is smaller than the diameter D4, where the diameter D4 is taken at the largest diameter of the secondtubular section 47′. Anaxial surface 46A′ extending circumferentially at an end of the secondtubular section 47′ extends between theshoulder 45′ and the secondtubular surface 46′. Theaxial surface 46A′ may thus allow the transition between theshoulder 45′ and the secondtubular surface 46′. Theaxial surface 46A′ defines arib 49′ extending about the central axis AX of thenose cone 20. In the depicted embodiment, therib 49′ is an annular rib extending along the full circumference of theaxial surface 46A′. Therib 49′ may be absent in other embodiments (such as in the embodiment shown inFIG. 5 ). - The bullet-shaped features described above may vary in shape in other embodiments. For instance, the diameters D1, D2, D3, D4 and/or D5 may vary in other embodiments, and/or more or less filling material M may be included within the volume V of the
nose cone 20. In other words, the filling material MF may fill a greater or lesser volume V of thenose cone 20/a greater or lesser volume V1 of thetip section 40 of thenose cone 20. In some embodiments, the bullet-shaped features may advantageously be easier to manufacture than other geometries, and/or they may allow optimization of the weight distribution within thenose cone 20. While the embodiments ofFIGS. 3-4 have similar bullet-shapedportion 24A of thenose cone cavity 24, alternative designs and various geometrical shapes may be contemplated in other embodiments. - In some embodiments, the filling material M providing added mass to the
nose cone 20 may be obtained by manufacturing thetip section 40 from a plain block of material, by any suitable material removal techniques, such as machining, for example. Thetip section 40 of thenose cone 20 may be manufactured using any suitable material additive manufacturing techniques, such as 3D-printing, for instance. - Adding mass to the
nose cone 20 includes distributing a weight of thenose cone 20 with a weight of thetip section 40 accounting for a majority of the weight of thenose cone 20. This may be obtained by forming thenose cone 20, and/or more particularly thetip section 40 thereof as described above with respect to various embodiments of thenose cone 20. In an embodiment, a weight distribution of thenose cone 20 is such that thetip section 40 is heavier than the base section. - A method for tuning a dynamic coupling of an
airframe 2 andturbofan engine 10 of anaircraft system 1 may be drawn from the above, according to another possibility. Said method may be implemented using the various embodiments discussed above. Theturbofan engine 10 has anengine rotor 11 including a shaft and a baseline nose cone removably attached to the fan. In some embodiments, thenose cone 20 is such as the one discussed above with respect toFIG. 2 . Anaircraft system 1 vibration response is obtained, theaircraft system 1 vibratory response defining a range of operational frequencies of theaircraft system 1. The baseline nose cone is then removed (removed or disassembled) from the fan of theturbofan engine 10 and a tuned nose cone is mounted to the fan in place of the baseline nose cone. Said tunednose cone 20 may be in accordance with the embodiments discussed with respect toFIGS. 5 and 6 . The tuned nose cone thus have a greater weight than that of the baseline nose cone or a mass distribution different from that of the baseline nose cone. In some cases, for instance in embodiments where thenose cone 20 is made of atip section 30 and abase section 40 as discussed above, instead of removing the whole baseline nose cone and replacing the baseline nose cone with a tuned nose cone, only one portion of thenose cone 20 may be removed, such as thetip section 40, which for consistency with the present disclosure may be referred to as a baseline tip section, and replaced by atuned tip section 40 having a mass greater than that of thebaseline tip section 40 or a mass distribution different from that of thebaseline tip section 40. As such, in some embodiments, adding mass in the nose cone may include providing a tuned tip portion having a weight greater than that of the tip portion, the tuned tip portion adapted to replace the tip portion in place and connect to the remainder of the nose cone. In some embodiments, where the nose cone is formed of at least two separate parts removably connected to one another, a first one of the separate parts defining a tip portion (or section 40) of the nose cone and a second one of the separate parts defining a base portion (or section 30), the tip portion defining an apex of the nose cone, the base portion extending from the tip portion to an axial end of the nose cone, adding mass in the nose cone includes providing a tuned tip portion having a weight greater than that of the tip portion in place, or a tuned tip portion having a different weight distribution than the tip portion in place. - The above description is meant to be exemplary only, and one skilled in the art will recognize that changes may be made to the embodiments described without departing from the scope of the invention disclosed. Still other modifications which fall within the scope of the present invention will be apparent to those skilled in the art, in light of a review of this disclosure, and such modifications are intended to fall within the appended claims.
Claims (20)
1. A method for tuning a vibratory response of an aircraft system comprising an airframe and at least one turbofan engine dynamically coupled, the at least one turbofan engine having an engine rotor including a nose cone, the method comprising:
obtaining a range of frequencies associated with at least one resonance mode of the aircraft system; and
adding mass within the nose cone to offset at least one dominant excitation frequency of the turbofan engine outside the range of frequencies associated with the at least one resonance mode of the aircraft system.
2. The method as defined in claim 1 , further comprising determining a range of excitation frequencies of the turbofan engine prior to adding mass in the nose cone.
3. The method as defined in claim 1 , further comprising evaluating the vibratory response of the aircraft system after adding the mass in the nose cone.
4. The method as defined in claim 1 , wherein the engine rotor is mounted for rotation about a rotation axis, wherein adding mass includes evenly distributing said added mass about the rotation axis of the engine rotor within a volume of the nose cone, the volume circumscribed by an outer surface of the nose cone.
5. The method as defined in claim 1 , wherein the nose cone defines an apex and an axial end of the nose cone, wherein adding mass includes obtaining an axially decreasing weight distribution of the nose cone such that a weight of the nose cone is greater from the apex to an axial plane of the nose cone between the apex and the axial end of the nose cone than from said axial plane to the axial end of the nose cone.
6. The method as defined in claim 5 , wherein the axial plane is located at an axial distance from the apex corresponding to at least ⅓ but less than ⅔ of an overall length of the nose cone extending from the apex to the axial end of the nose cone, wherein obtaining the axially decreasing weight distribution of the nose cone includes distributing the weight of the nose cone such that the weight of the nose cone between the apex and the axial plane accounts for a majority of the weight of the nose cone.
7. The method as defined in claim 5 , wherein the axial plane is located at an axial distance from the apex corresponding to at least ⅓ but less than ⅔ of an overall length of the nose cone extending from the apex to the axial end of the nose cone, wherein obtaining the axially decreasing weight distribution of the nose cone includes distributing the weight of the nose cone such that the weight of the nose cone between the apex and the axial plane accounts for between about 50% to about 80% of the weight of the nose cone.
8. The method as defined in claim 5 , wherein the axial plane is located at an axial distance from the apex corresponding to at least ⅓ but less than ⅔ of an overall length of the nose cone extending from the apex to the axial end of the nose cone, wherein obtaining the axially decreasing weight distribution of the nose cone includes distributing the weight of the nose cone such that the weight of the nose cone between the apex and the axial plane accounts is more than two times but less than three times the weight of the nose cone between the axial plane and the axial end of the nose cone.
9. The method as defined in claim 1 , wherein adding mass includes forming an annular mass within a volume of the nose cone, the annular mass defining an internal cavity of the nose cone.
10. The method as defined in claim 9 , wherein forming the annular mass includes defining an internal dome surface at a foremost area of the nose cone, extending towards and merging into a tubular surface such as to form a continuous surface therebetween, the tubular surface extending about a central axis of the nose cone, the central axis coinciding with the rotation axis of the engine rotor.
11. The method as defined in claim 10 , wherein the tubular surface is a first tubular surface, wherein forming the annular mass includes forming a second tubular surface extending about the central axis of the nose cone, the first and second tubular surfaces being concentric with one another.
12. The method as defined in claim 1 , wherein the nose cone has a tip portion defining an apex of the nose cone and extending axially along a central axis of the nose cone over at least one third of a total length of the nose cone, the tip portion removably connected to a remainder of the nose cone, wherein adding mass in the nose cone includes providing a tuned tip portion having a weight greater than that of the tip portion, the tuned tip portion adapted to replace the tip portion in place and connect to the remainder of the nose cone.
13. The method as defined in claim 1 , wherein the nose cone is formed of at least two separate parts removably connected to one another, a first one of the separate parts defining a tip portion of the nose cone and a second one of the separate parts defining a base portion, the tip portion defining an apex of the nose cone, the base portion extending from the tip portion to an axial end of the nose cone, wherein adding mass in the nose cone includes providing a tuned tip portion having a weight greater than that of the tip portion in place, the tuned tip portion adapted to connect to the base portion of the nose cone.
14. A method of tuning dynamic coupling of an aircraft system comprising an airframe and a turbofan engine mounted thereto, the turbofan engine having an engine rotor including a nose cone, the method comprising:
obtaining operational frequencies of the aircraft system, including at least one dominant frequencies range;
determining a target resonant frequency of the turbofan engine different from that of the at least one dominant frequencies range of the aircraft system; and
modifying a mass of the nose cone to achieve said target resonant frequency of the turbofan engine.
15. The method as defined in claim 14 , wherein tuning the mass of the nose cone includes forming an annular mass within a volume of the nose cone, the annular mass defining an internal cavity of the nose cone.
16. The method as defined in claim 15 , wherein forming the annular mass includes defining an internal dome surface at a foremost area of the nose cone, extending towards and merging into a tubular surface such as to form a continuous surface therebetween, the tubular surface extending about a central axis of the nose cone, the central axis coinciding with the rotation axis of the engine rotor.
17. The method as defined in claim 14 , wherein the engine rotor is mounted for rotation about a rotation axis, wherein tuning the mass includes adding the mass such as to evenly distribute said added mass about the rotation axis of the engine rotor within a volume of the nose cone, the volume circumscribed by an outer surface of the nose cone.
18. The method as defined in claim 14 , wherein the nose cone defines an apex and an axial end of the nose cone, wherein tuning the mass includes obtaining an axially decreasing weight distribution of the nose cone such that a weight of the nose cone is greater from the apex to an axial plane of the nose cone between the apex and the axial end of the nose cone than from said axial plane to the axial end of the nose cone.
19. The method as defined in claim 18 , wherein the axial plane is located at an axial distance from the apex corresponding to at least ⅓ but less than ⅔ of an overall length of the nose cone extending from the apex to the axial end of the nose cone, wherein obtaining the axially decreasing weight distribution of the nose cone includes distributing the weight of the nose cone such that the weight of the nose cone between the apex and the axial plane accounts for between about 50% to about 80% of the weight of the nose cone.
20. A method for tuning a dynamic coupling of an airframe and a turbofan engine of an aircraft system, the turbofan engine mounted to the airframe, the turbofan engine having at least one resonant frequency, the method comprising:
obtaining an aircraft system vibratory response, the aircraft system vibratory response defining a range of operational frequencies of the aircraft system, the turbofan engine having a fan and a baseline nose cone removably attached thereto;
removing the baseline nose cone from the fan of the turbofan engine; and
mounting a tuned nose cone to the fan of the turbofan engine in place of the baseline nose cone, the tuned nose cone having a mass greater than that of the baseline nose cone or a mass distribution different from that of the baseline nose cone to modify the at least one resonant frequency.
Priority Applications (4)
Application Number | Priority Date | Filing Date | Title |
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US16/583,995 US10947995B1 (en) | 2019-08-27 | 2019-09-26 | Fan nose cone and dynamic tuning of aircrafts |
CA3083311A CA3083311A1 (en) | 2019-08-27 | 2020-06-11 | Fan nose cone and dynamic tuning of aircrafts |
PL20192242.4T PL3786066T3 (en) | 2019-08-27 | 2020-08-21 | Dynamic tuning of aircrafts |
EP20192242.4A EP3786066B1 (en) | 2019-08-27 | 2020-08-21 | Dynamic tuning of aircrafts |
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US201962892156P | 2019-08-27 | 2019-08-27 | |
US16/583,995 US10947995B1 (en) | 2019-08-27 | 2019-09-26 | Fan nose cone and dynamic tuning of aircrafts |
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US20210062829A1 true US20210062829A1 (en) | 2021-03-04 |
US10947995B1 US10947995B1 (en) | 2021-03-16 |
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EP (1) | EP3786066B1 (en) |
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Also Published As
Publication number | Publication date |
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EP3786066B1 (en) | 2022-03-23 |
US10947995B1 (en) | 2021-03-16 |
PL3786066T3 (en) | 2022-08-16 |
CA3083311A1 (en) | 2021-02-27 |
EP3786066A1 (en) | 2021-03-03 |
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