AERODYNAMIC BODY PROVIDED WITH SURFACE CAVITIES

Abstract: An airfoil is provided with a surface cavity (1) having an aperture (2), towards the external surface of the airfoil, and defined by a front edge (7) and rear edge (6) positioned transversally to the direction of movement of the profile, in which the front edge (7) is reentrant with respect to the rear edge (6) by a distance (H). The area (5) located upstream of the front edge (7) slopes gradually downwards from the outer surface of the profile towards the cavity (1) in order to divert part of the flow of the fluid F, which skims the outer surface, into the cavity (1).

Description: AERODYNAMIC BODY PROVIDED WITH SURFACE CAVITIES Field of the invention The present invention concerns an aerodynamic body with an aerodynamically shaped outer surface which, due to its shape, can vary both the lift and the drag of the body itself. In practice the body can take the form of ailerons, air brakes, stabilizers or control elements and aerodynamic appendixes in general. Previous technology One of the main problems of racing cars, and in particular of formula racing cars, with exposed wheels, consists in the creation of a braking system that combines the requirements of lightness, reliability, easy access and high power. Some of these requirements are obviously contradictory: for this reason, considerable resources are dedicated every year to the design and production of new or renewed braking systems. On the other hand, the outer shape of the vehicle bodywork must comply with stringent aerodynamic specifications, which entail a low Cx, a high lateral stability and an attitude generally with negative lift, all devices that increase the driveability of the vehicle. Regulations permit the addition of wing-shaped aerodynamic appendixes, known as spoilers, which can be adjusted according to the characteristics of the track, to optimise the combination of good manoeuvrability with high negative lift, low top speed, good behaviour on mixed courses and good top speed with low negative lift, high top speed and poor stability on mixed courses. An idea already tested out in Formula 1 car racing is to construct the aerodynamic appendix of the vehicle so that it can also perform a braking and negative lift function as required by the driver (mobile aileron). Following serious accidents caused by detachment of the aileron, this solution was subsequently prohibited: the 2000/2001 regulations permit the use of aerodynamic appendixes on the outside of the vehicle body only if said surfaces are fixed, i.e. they cannot be adjusted unless the vehicle is at a standstill. The "adjustment" to which the regulations refer is the inclination: a variation in the setting angle of the stabiliser with respect to the roadway produces a variation in the angle of attack and a consequent variation in the lift. One aim of the present invention is to provide a device to vary the lift and if necessary the braking capacity of a stabiliser, aileron or aerodynamic appendix, with fixed setting angle. Said problem is solved by an aerodynamic body defining an external surface designed to be skimmed by a fluid in relative movement with it in a predetermined direction, and comprising at least one cavity provided with an aperture in correspondence of said external surface, said aperture being defined by a first edge upstream of said cavity, in the direction of the fluid flow with respect to the external surface, and a second edge downstream of said cavity, said first and second edges being arranged substantially transversally to said predetermined direction of relative movement, characterised in that said first edge is in a reentrant position with respect to said second edge by a pre-determined distance with reference to said external surface. In this way, part of the fluid skimming the surface outside the cavity is diverted inside the cavity, sets up a vortex and flows out of it in a substantially intermittent manner, in such a way that it is not possible to describe the phenomenon with steady-state methods and models. The air flows out in a jet transversally to the cavity inflow and to the incoming external flow that skims the outer surface; said jet introduces additional turbulence in said flow. By making a number of cavities defined as above on the pressure side of a airfoil profile or any aerodynamic element of an aircraft, vehicle or vessel, the turbulence of the various cavities increases the drag on the aerodynamic element. The area of the airfoil where the cavities are provided according to the invention will depend on the required effects on the dynamic behaviour of the vehicle or aircraft. With very simple forms and a limited number of components, it is possible to create cavities with varying shapes and therefore with varying braking capacity; they can therefore be applied to obtain a variation in the drag and lift on larger aerodynamic elements such as wings and ailerons, the latter remaining with fixed setting angle, and thus being structurally stronger, with all consequent benefits in terms of economy, reliability and maintenance. In a particular embodiment of the invention, the cavities are closed by partitions or shutters, thus permitting elimination of the drag whenever deemed necessary. A further embodiment of the invention provides for a mechanism driven by electrical, hydraulic or mechanical devices that reduces or increases the difference in level between the two edges, front and rear, of the cavity/cavities according to the movement requirements of the vehicle or aircraft on which the airfoil is applied in accordance with the invention. List of figures Further advantages that can be obtained with the present invention will become more apparent to a person skilled in the art, from the following detailed description by way of example of a particular non-limiting embodiment, with reference to the following figures, in which: Figure 1 shows schematically the distribution of the pressure exerted on a cross section of a airfoil profile of known type and immersed in a flowing fluid; Figure 2 shows schematically the conventional physical-geometrical quantities in the study of forces acting on a airfoil profile of the known art; Figure 3 shows schematically in cross section the detail of a preferred embodiment of an airfoil according to the invention; Figure 4 shows schematically a distribution of the speed vectors at some points and near the cavity of the airfoil of Figure 3; Figures 5a, 5b show schematically a second preferred embodiment of an airfoil according to the present invention; Figure 6 shows a third preferred embodiment of an airfoil according to the present invention. Detailed description With reference to Figures 1 and 2, certain basic concepts and conventions of aerodynamics are summarised: when a wing section is immersed in a fluid F and moves in relation to it, a lift is generated on the wing section due to the different variation in the momentum of the fluid particles on the side PS with positive pressure with respect to those on the side SS with negative pressure. The air stream near the surface SS with negative pressure has a greater speed than the one flowing on PS, and the relative pressures acting locally on each area of the surface will be consequently higher on the side PS with positive pressure and lower on the side SS with negative pressure. The integral of the pressure distribution on the surface of the wing section provides a force that can be split into two component forces: the lift L, providing the wing supporting action, and the drag D, which produces resistance to the forward movement of the wing and corresponds to the power dissipated in viscous effects. Both the lift L and the drag D, with the same airfoil profile, depend on the angle of attack α, defined as the angle between the tangent to the chord C of the wing section at the leading edge and the direction of the mean relative speed of the fluid F, measured with respect to a system of reference co-ordinates integral with the wing: when the angle α is varied, the values of the lift L and the drag D vary, and this is what happens in the current technical solution using mobile ailerons, which are basically wings with variable angle of attack and lift exerted downwards, i.e. with the side PS with positive pressure facing upwards. The operating range of a mobile aileron is generally established so that as the lift L increases, the drag D also increases. Figure 3 shows the details of a first preferred embodiment of an airfoil according to the present invention, the operating principle of which is the following: the arrow V indicates the direction of the relative movement of the airfoil, near the cavity 1 , with respect to a fluid F which is, for example but not necessarily, air, in which the airfoil and the airfoil profile to which it belongs are immersed. V can also indicate the direction of the fluid stream velocity not disturbed by the movement of the supporting surface. It is assumed that the fluid F flows from left to right with reference to the arrangement of Fig. 3; 3 and 4 indicate respectively the area upstream and the area downstream of the aperture of the cavity 1. Figure 3 shows a cross section of an airfoil according to the present invention, according to a section plane vertical and substantially parallel to the direction of the relative movement between the uniform flow F and the airfoil itself; the cavity 1 extends towards the inside of the airfoil profile or body, defines an internal space 1 preferably, but not necessarily, rounded with relatively long radii of curvature in order not to obstruct the flow of as large as possible a vortex inside it, and is provided with an aperture 2 which faces the outside and towards the fluid F. The aperture 2 has edges 6, 7, preferably sharp or, taking account of the inevitable machining tolerances, with chamfers or radii sufficiently small and negligible with respect, for example, to the curves of the inside of the cavity 1 , as a specialist technician will be able to determine on a time by time basis. According to an aspect of the present invention, the edge upstream 7 of the aperture 2 is not at the same level as the edge 6 downstream of the aperture, but lays lower of a predetermined distance H. In addition, upstream of the edge 7 positioned upstream of the aperture is a gradually downward-sloping area 5, for example in the shape of a sloping flat surface, designed to gently deflect inside the cavity 1 a part of the fluid stream F that flows on the external surface 8. Alternatively, the sloping surface 5 can be a curved surface with progressively increasing angle as it nears the edge 7, creating an inlet with as dull a shape as possible, to divert part of the air flow that flows along the supporting surface, inside the cavity 1. The gradually downward-sloping surface 5 terminates at one end with the edge upstream 7. Owing to the difference in the distance H between the edges upstream 7 and downstream 6, airstream VA, or other fluid, enters the cavity 1 , sets up a vortex, shown in Figure 3 in clockwise direction, and flows out of the cavity 1 again through the aperture 2 with a jet of air VU transversal to the external fluid stream which arrives from upstream of the cavity 1 and skims the aileron. The numerical simulation schematised in Figure 4 shows how, according to the present solution, in cavity 1 we have a voluminous flow of incoming and outgoing air, where the component of the outgoing jet VU, transversal to the flow VA which runs over the cavity 1 , is fairly large; this intermittent outgoing jet VU periodically interfers with the boundary layer of the fluid F which flows along the pressurised surface PS generating additional turbulence and thus increasing the drag of the stabiliser and its drag. The surface 9 of the cavity 1 immediately downstream of the edge upstream 7 forms with the sloping surface 5 an angle β - preferably between 75° and 135° - in order not to obstruct the flow of the vortex inside cavity 1 and setting up of the outgoing jet of air VU transversally to the air stream VA flowing over the cavity 1. The jet of air VU flowing out of the cavity 1 pulsates at the approximate frequency resulting from the following formula f = v/p where f is the frequency, v the relative velocity between airfoil and the uniform flow, and p is the effective perimeter of the cavity. The section of cavity 1 shown schematically in Figures 3, 4 can be made in different embodiments, for example to produce one or more elongated slots that extend transversally to the fluid streams flowing on the airfoil according to the design direction, or to produce one or more cavities with squat and/or round, spherical, oval volume etc. According to a further aspect of the present invention, one or more cavities 1 are arranged preferably on the side PS with positive pressure of a airfoil profile, aileron or other aerodynamic appendix, for example more than 5-10 cavities spaced in the direction of the relative movement. This, for example in the case of a negative lift stabiliser for Formula 1 cars, increases both the lift P and the drag D. According to a further preferred embodiment of the present invention, illustrated in Figures 5a, 5b, the apertures 2 of the cavities 1 are opened and closed by a partition or sliding or concealed strip 11 moved by appropriate drive devices: in an automotive application, for example when the driver operates the brake, the partition 11 gradually uncovers a number of cavities 1 for example proportional to the pressure on the brake pedal, or according to the commands of the vehicle control computer, permitting progressive and adjustable increase in the negative lift and drag D of the stabilisers, or other aerodynamic appendixes, even though they have a fixed setting angle. This increased braking and negative lift action increases the stability of the vehicle during braking. Figure 6 shows a further form of preferred embodiment of a device for varying the braking action of a cavity according to the present invention: according to said form of embodiment, the extent of the jet VU, and therefore of the braking action, is adjusted by varying the angle of the gradually retracting surface 5, obtained on a horizontally pivoting element 12 appropriately hinged on an axis 13. By rotating the element 12 clockwise by an angle δ, the distance H increases and with it the braking action of the cavities, while by rotating the element 12 anticlockwise, the distance H can be reduced to zero: in this case the braking action of the cavity 1 becomes negligible, and the situation is similar, in certain aspects, to that of the "captive vortex cavities" previously discussed. Another particular application concerns the wings of aircraft: by creating an appropriate number of cavities 1 on the lower surface, with positive pressure, of the wing of an aircraft, the gradual uncovering of said cavities 1 generates additional lift P and drag D, in the same way as the mobile ailerons currently used. These can therefore be replaced by a system of progressively operated cavities 1 , safer, with fewer mobile parts and therefore more reliable, less expensive and easier to install, adjust and maintain, for example in appropriate areas of aircraft wings. The embodiments described above are intended to be illustrative and not restrictive and are therefore subject to numerous other modifications, variations and applications that will be apparent to a man skilled in the art, while remaining within the scope of the present invention, which for example can be applied to all cases, not only automotive or aeronautical, in which it is desirable to improve the braking and lift capacity of an airfoil profile: for example the internal cavity 1 can have various shapes, not necessarily rounded, and its internal volume can be varied for example by means of a piston, cam or gear system.

Claims: CLAIMS 1) Airfoil section defining an external surface adapted to be skimmed by a fluid (F) in relative movement with it in a predetermined direction, and comprising at least one cavity (1 ) provided with an aperture (2) corresponding to said external surface, said aperture being defined by a first edge (7) upstream of said cavity (1 ), in the direction of the fluid flow (F) with respect to the external surface, and a second edge (6) downstream of said cavity (1 ), said first and second edges being arranged substantially transversally to said predetermined direction of relative movement, characterised in that said first edge (7) is in a reentrant position with respect to said second edge (6) by a pre-defined distance (H) with reference to said external surface. 2) Airfoil section according to claim 1 wherein, in correspondence of at least one cavity (1 ), there is provided an area (5) located upstream of said first edge (7), which is gradually reentrant from said external surface towards the respective cavity (1 ) in order to divert part of the flow of the fluid F, which skims the outer surface, into the respective cavity (1 ). 3) Airfoil section according to claim 2, wherein the gradually reentrant area (5) has a flat surface. 4) Airfoil section according to claim 2, wherein said first edge (7) corresponds to the edge of the angle (β), of value between 75° and 135°, formed by said reentrant area (5) of the outer surface and by the internal wall of the respective cavity (1 ). 5) Airfoil section according to one of the previous claims, wherein the cavity (1) consists substantially of a slot that extends transversally to the direction of the fluid (F). 6) Airfoil section according to claim 1 , in which said cavity (1 ) features a section, on a plane parallel to the direction of the fluid (F), with substantially squat and/or rounded shape. 7) Airfoil section according to one of the previous claims, provided with devices (11 ) for closing the aperture (2) of at least one cavity (1 ). 8) Airfoil section according to claim 7, in which the closing devices (11) comprise a mobile partition or strip. 9) Airfoil section according to claim 2, in which said pre-defined distance (H) can be varied by operating mechanisms over a range with minimum value near to zero and a predetermined maximum value. 10) Airfoil section according to claim 9, characterised in that the distance (H) can be varied by varying the angle of said reentrant area (5) upstream of the first edge (7). 11) Airfoil adapted to move in a fluid in relative movement with respect to it, provided with a side (SS) with negative pressure and a side (PS) with positive pressure, characterised in that it comprises in an area of the external surface with features according to one or more of the previous claims.

Inventors: GAMMA FAUSTO, SCIUBBA ENRICO, ZINGARO DOMENICO, GAMMA, FAUSTO, SCIUBBA, ENRICO, ZINGARO, DOMENICO
Applicants: GAMMA FAUSTO, SCIUBBA ENRICO, UNIV ROMA, ZINGARO DOMENICO, GAMMA, FAUSTO, SCIUBBA, ENRICO, UNIVERSITA DEGLI STUDI DI ROMA "LA SAPIENZA", ZINGARO, DOMENICO
Application year: 2001
Main classification: B64C23
IPC codes: B64C23