The invention relates to the field of aero-acoustic management of a fixed vane in an aircraft turbomachine or in an aircraft turbomachine test bed.
This type of fixed vane is found for example in OGV (outlet guide vanes), or straighteners disposed downstream of a rotating body, for straightening the flow of air. The term stator vane will be used to designate a fixed vane.
An example will be given for a turbofan with a fan and a straightener disposed in the secondary flow path.
The interaction between the flow rotated by the fan and the straightener in the secondary flow path is the origin of a noise source that is predominant in the total noise generated by the engine, or even by the airplane depending on the operating regime.
Several approaches are considered for controlling and/or reducing noise of aerodynamic origin, either by modification of the incident aerodynamic field (aerodynamic excitation), or by modification of the geometry of the stators (aero-acoustic response).
In the second case, a modification of the geometry of the leading edge of the stator vanes has been proposed in the form of undulated leading edges commonly called “wavy leading edge,” “serrated leading edge,” or “leading edge serrations.”
The principal of reducing noise emission generated by the OGV cascade resides in the fact of spatially dephasing the noise sources distributed along the leading edge by means of undulations, identical or not. In order for the principle to apply, the size, (depth, width, thickness) of the undulations must be adapted to the content of the incident aerodynamic field (thickness and deficit of average wakes, size of vortices for turbulence) which varies depending on the operating regime of the engine.
As presented in the references listed below, the geometric variation function along the chord is given by the following equation:
c(r)=c0+h·sin(2πr/λ)
where c0 is the reference chord, h the amplitude and λ the wavelength of the undulations and r the radius.
The angle θ expressed below is a key parameter in noise reduction. Its value is determined by the following formula, illustrated in
θ=a tan(4h/λ)
The value of λ is selected based on the wavelength of the turbulence of the fluid arriving at the leading edge of the vane.
However, the presence of teeths 112 at the leading edge 108 reduces considerably the mechanical status of the OGV, with strong stress concentrations in the troughs of the teeth.
In fact, under aerodynamic forces the blade bends tangentially, which induces a transverse shear effect from one tooth to another. Thus the longer the teeth, the smaller the radius of the troughs of the teeth, the greater the stress in the troughs of the teeth will be.
However, this observation is the inverse of the desired acoustic gain because the latter is maximized for teeth that are thin and long.
There exists therefore a need for solutions allowing vanes with serrated profiles to be protected.
To this end, the invention proposes a stator vane comprising:
The invention can comprise the following features, taken alone or in combination:
Where c0 is the reference chord, h the amplitude and λ the wavelength of the undulations and r the radius
The invention also relates to a straightener ring comprising a plurality of vanes as described previously, the vanes being distributed circumferentially around a hub.
The invention also relates to a turbomachine or a test bed comprising a vane or a ring as previously described.
This consists of a turbomachine or for example a test bed of a partial turbomachine, this assembly being for example a single entry straightener of the partial turbomachine by constituting a flow path which would correspond to a secondary flow path considering the case of a complete turbomachine.
Other features, aims and advantages of the invention will be revealed by the description that follows, which is purely illustrative and not limiting, and which must be read with reference to the appended drawings, in which:
Placing the following within the scope of a portion of a turbomachine, typically a flow path which could be equivalent to a secondary flow path of a turbofan with a straightener (OGV) disposed at the fan outlet. It can therefore be the scope of a test bed, for example for single-entry straighteners or any other type of test bed in which a fixed vane is used. Such a test bed is for example a partial engine allowing for example the validation of the data on phenomena representative of those occurring customarily in the secondary flow path of a complete engine.
At another, radially external, end, the vane 100 is attached to a casing 250 by a vane tip 115.
To form the flow path V, an interior platform 220 can be provided radially beyond the hub 200, which has no aerodynamic function.
The vane 100 has a profiled shape to straighten the flow, with in particular a pressure side and a suction side. The vane 100 root 110 can have a shape continuing the pressure side and the suction side.
The vane 100 comprises a serrated leading edge 120, that is one which has undulations in the form of an alternation of teeth 122 and of troughs 124, with for example a sinusoidal pattern as described in the introduction.
The vane 100 can be made of metal or of composite material (resin matrix with reinforcements, typically of carbon).
In order to protect the serrated profile, one objective of the invention is to relieve mechanically the teeth and troughs where stresses are the highest.
To this end, as illustrated in
In this series, the amplitude of the teeth 122 and of the troughs 124 decreases when approaching the vane root 110 or the vane tip 115. Alternately or in addition, it is the thickness of the leading edge 120 that increases when approaching the vane root 110 or the vane tip 115.
This series 300 can be located at the vane tip 115 and/or and the vane root 110.
The amplitude is defined as the distance between the peaks (of the tooth or of the trough) with respect to a straight profile. It therefore corresponds to the “h sin(2πr/λ)” of the formula given in the introduction.
The thickness is defined at the straight profile for a zero tooth or trough amplitude). In fact, the thickness of the vane 100 is variable between upstream and downstream of the vane: it is for example thinner at the peaks of the teeth 122 than at the peaks of the troughs 124.
Such a vane 100 allows distributing the load by smoothing the stress over several serrations.
Hereafter in the application, only “reduction in amplitude” will be discussed, which can be replaced with “increase in thickness.”
To ensure this continuity, the reduction in amplitude can be governed by formulas.
Recall the placement in the scope of a vane 100 of which the serrated profile is defined by the following shape:
c(r)=c0+h·sin(2πr/λ)
Where c0 is the reference chord, h the amplitude and λ the wavelength of the undulations and r the radius. By radius is meant the positioning along the leading edge 120 (which extends radially from the longitudinal axis, hence the term radius). It is assumed that r=0 signifies that the location is against the edge of the flow path V, either at the vane tip 115 or at the vane root 110.
The equation is conceptually simplified by considering that λ is an arbitrarily fixed constant.
This regular sinusoidal profile Ps is illustrated in
Several embodiments allow the serrations in the series 300 to be modulated.
In one embodiment illustrated in
c(r)=c0+h·sin(2πr/λ)·K·r
In one embodiment illustrated in
c(r)=c0+h·sin(2πr/λ)·L·r2
In one embodiment illustrated in
c(r)=c0+h·sin(2πr/λ)·sin(Mπ/2·r)
In one embodiment illustrated in
c(r)=c0+h·sin(2πr/λ)·exp(N·r)
Any continuous function strictly decreasing in the direction of the root 110 or of the tip 115 of the vane is usable in practice.
Preferably, the first tooth 122 or the first trough 124 is prevented from having zero amplitude, because that would only carry the load over to the next tooth or trough. To this end, it is sufficient to integrate a slight offset, of the type r-r0, into the equations given above.
In one embodiment, the series 300 comprises four, or even five troughs and five successive teeth.
In one embodiment, the series 300 extends between 20 and 50% of the length of the vane 100 into the flow path.
It is possible to combine the variations of amplitude and thickness, so as to create a vane 100 profile that is three-dimensionally variable.
In addition to a turbomachine, this vane 100 can be mounted within the scope of a test bed or of a test turbomachine.
Number | Date | Country | Kind |
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1760212 | Oct 2017 | FR | national |
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Entry |
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Search Report and Written Opinion dated Jul. 24, 2018 in corresponding French Patent Application No. FR1760212 (with English Translation of Category of Cited Documents), citing documents AA, AO-AQ therein, 7 pages. |
Number | Date | Country | |
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20190170003 A1 | Jun 2019 | US |