This invention relates to a vortex generator and particularly but not exclusively relates to a boundary layer energiser for energising a boundary layer flow over a surface.
Typically, active flow control involves injecting an energetic flow into a boundary layer to increase the momentum of the boundary layer flow thereby delaying separation of the boundary layer from the surface. In particular, active flow control on the intake lips of a jet engine has been proposed previously.
It has been suggested previously that active flow control could be provided by the use of perforations on the intake surface. A flow may be introduced through these perforations to re-energise the intake near wall boundary layer. These perforations may take the form of holes either perpendicular to the surface contour or angled in a uniform orientation. However, as shown in
By contrast, U.S. Pat. No. 4,749,150 discloses a “Turbofan duct with noise suppression and boundary layer control” and describes the use of suction through the acoustic liner of an engine intake for boundary layer control. However, this invention also uses a lot of power to suck sufficient air from the boundary layer. Furthermore, it is also subject to blockage with debris such as dust and insects. For these reasons blowing, as opposed to suction, is preferred.
The present invention therefore seeks to address these issues.
According to a first aspect of the present invention there is provided a boundary layer energiser for energising a boundary layer flow over a surface, the boundary layer energiser comprising a plurality of passages, each passage terminating in a respective hole provided on the surface, the holes being arranged in a cluster on the surface, wherein the plurality of passages are angled with respect to one another at the surface is such that, when in use, a vortex is formed by a fluid flowing through the plurality of passages.
The vortex may be a helical vortex. The cluster of holes may comprise two holes. Alternatively, the cluster of holes may comprise three or more holes and the holes may be arranged on the surface such that each hole may be at the vertex of a first polygon. The first polygon may comprise between three and ten vertices. The first polygon may be a regular polygon and may be a triangle, square, pentagon, hexagon etc.
The boundary layer energiser may comprise a plurality of clusters, each with a plurality of passages and respective holes arranged on the surface. A centre of each cluster may be arranged on the surface at the vertex of a second polygon. The second polygon may comprise one of a triangle, square, pentagon, hexagon etc. The second polygon may be a regular polygon. The second polygon may comprise an even number of vertices.
The boundary layer energiser may comprise a plurality of clusters, each with a plurality of passages and respective holes arranged on the surface, wherein a centre of each cluster may be arranged on the surface in a linear arrangement. The passages may be arranged such that neighbouring clusters generate a vortex in opposite directions.
The direction of each passage at the surface may have a vector component parallel to the surface. The vector defined by the sum of the directions of the plurality of passages at the surface may be perpendicular to the surface. The vector defined by the sum of the directions of the plurality of passages at the surface may have a component parallel to the surface.
The flow may be provided by a flow source. The flow may be provided from an opening in a second surface.
A turbomachine may comprise a boundary layer energiser as described above. A gas turbine may comprise a boundary layer energiser as described above.
According to a second aspect of the present invention there is provided a boundary layer energiser for energising a boundary layer flow over a surface, the boundary layer energiser comprising one or more passages terminating in one or more respective holes provided on the surface, wherein the one or more passages are configured such that, when in use, a fluid emanating from the one or more passages flows in a vortex.
According to a third aspect of the present invention there is provided a method of energising a boundary layer flowing over a surface, the method comprising: providing a plurality of passages, each passage terminating in a respective hole provided on the surface, the holes being arranged in a cluster on the surface, wherein the plurality of passages are angled with respect to one another at the surface; allowing a fluid to flow through the plurality of passages; and forming a helical vortex with the fluid by virtue of the angles between the passages.
According to a fourth aspect of the present invention there is provided a method of energising a boundary layer flowing over a surface, the method comprising: providing one or more passages terminating in one or more respective holes provided on the surface; allowing a fluid to flow through the plurality of passages; and forming a vortex with the fluid by virtue of the one or more passages which are configured such that the fluid emanating from the one or more passages flows in a vortex.
For a better understanding of the present invention, and to show more clearly how it may be carried into effect, reference will now be made, by way of example, to the accompanying drawings, in which:
a and 2b shows a boundary layer energiser according to an example of the present invention;
With reference to
Each cluster 23 may comprise between 2 and 10 passages and respective holes. In the case of the cluster of holes comprising three or more holes, the holes may be arranged on the surface such that each hole is at the vertex of a first polygon comprising between three and ten vertices. In the particular embodiment shown in
With reference to
The vector defined by the sum of the direction vectors 28 of the plurality of passages 24 at the surface 22 may be perpendicular to the surface. In other words the net flow and the vortex 21 emanating from the plurality of passages may be perpendicular to the surface. Alternatively, the vector defined by the sum of the direction vectors 28 of the plurality of passages at the surface may have a component parallel to the surface 22.
In other words the vortex generated by the plurality of passages and holes may, in the absence of a mainstream flow, either be perpendicular to the surface or have a component parallel to the surface.
With reference to
With the linear arrangement of individual clusters (as shown in
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Number | Date | Country | Kind |
---|---|---|---|
0919107.3 | Nov 2009 | GB | national |
Number | Name | Date | Kind |
---|---|---|---|
2041793 | Stalker | May 1936 | A |
2248308 | Rice | Jul 1941 | A |
2565720 | Collison et al. | Aug 1951 | A |
2650781 | Taylor | Sep 1953 | A |
2836463 | Wilson | May 1958 | A |
3421577 | Valyi | Jan 1969 | A |
3508561 | Cornish, III | Apr 1970 | A |
3525486 | Wimpenny | Aug 1970 | A |
3556444 | Kopp | Jan 1971 | A |
3776363 | Kuethe | Dec 1973 | A |
4163366 | Kent | Aug 1979 | A |
4478380 | Frakes | Oct 1984 | A |
4529358 | Papell | Jul 1985 | A |
4749150 | Rose et al. | Jun 1988 | A |
4955565 | Coplin | Sep 1990 | A |
5080303 | Hutton | Jan 1992 | A |
5104069 | Reising | Apr 1992 | A |
5148989 | Skinner | Sep 1992 | A |
5552576 | Giamati | Sep 1996 | A |
5655732 | Frank | Aug 1997 | A |
5778676 | Joshi et al. | Jul 1998 | A |
5803409 | Keefe | Sep 1998 | A |
5988522 | Glezer et al. | Nov 1999 | A |
6116015 | Taylor et al. | Sep 2000 | A |
6425554 | Moreland | Jul 2002 | B1 |
6837465 | Lisy et al. | Jan 2005 | B2 |
7111809 | Tai et al. | Sep 2006 | B1 |
7143983 | McClure | Dec 2006 | B2 |
7510149 | Miller et al. | Mar 2009 | B2 |
7597288 | Kwok et al. | Oct 2009 | B2 |
7832689 | Prince et al. | Nov 2010 | B2 |
8038102 | Miller et al. | Oct 2011 | B2 |
8348199 | Sheaf et al. | Jan 2013 | B2 |
20050147497 | Doerffer et al. | Jul 2005 | A1 |
20060078417 | Benton | Apr 2006 | A1 |
20060249628 | Turner et al. | Nov 2006 | A1 |
20070227153 | Truax | Oct 2007 | A1 |
20080149205 | Gupta et al. | Jun 2008 | A1 |
20100293917 | Handley et al. | Nov 2010 | A1 |
Number | Date | Country |
---|---|---|
0 439 923 | Aug 1991 | EP |
0 940 338 | Sep 1999 | EP |
2 065 303 | Jun 2009 | EP |
2 446 147 | Aug 2008 | GB |
WO 2008045074 | Apr 2008 | WO |
WO 2009025549 | Feb 2009 | WO |
Entry |
---|
Jun. 8, 2012 Office Action issued in U.S. Appl. No. 12/883,566. |
Search Report issued in British Patent Application No. 0919110.7, on Feb. 17, 2010. |
Search Report issued in British Patent Application No. 0919107.3, on Feb. 17, 2010. |
Search Report issued in British Patent Application No. 0919115.6, on Feb. 15, 2010. |
Search Report issued in British Patent Application No. 0908540.8, on Sep. 7, 2009. |
Search Report issued in British Patent Application No. 0919118.0, on Feb. 15, 2010. |
U.S. Appl. No. 12/883,566 in the name of Christopher T.J. Sheaf, filed Sep. 16, 2010. |
U.S. Appl. No. 12/767,989 in the name of Christopher T.J. Sheaf, filed Apr. 27, 2010. |
U.S. Appl. No. 12/883,400 in the name of Christopher T.J. Sheaf, filed Sep. 16, 2010. |
Jun. 20, 2013 Office Action issued in U.S. Appl. No. 12/883,400. |
Search Report issued in corresponding European Application No. 10 16 1151.5 dated Mar. 4, 2011. |
Apr. 3, 2014 European Search Report issued in European Patent Application No. EP 10 17 7121. |
Number | Date | Country | |
---|---|---|---|
20110103969 A1 | May 2011 | US |