None.
None.
The present invention relates generally to a gas turbine engine, and more specifically to an air cooled airfoil in the engine.
Description of the Related Art including information disclosed under 37 CFR 1.97 and 1.98
Airfoils used in a gas turbine engine, such as rotor blades and stator vanes (guide nozzles), require film cooling of the external surface where the hottest gas flow temperatures are found. The airfoil leading edge region is exposed to the highest gas flow temperature and therefore film cooling holes are used here. Film cooling holes discharge pressurized cooling air onto the airfoil surface as a layer that forms a blanket to protect the metal surface from the hot gas flow. The prior art is full of complex film hole shapes that are designed to maximize the film coverage on the airfoil surface while minimizing loses.
Standard film holes pass straight through the airfoil wall at a constant diameter and exit at an angle to the airfoil surface. This is shown in
An improvement of the straight film hole is the diffusion hole shown in FIGS. 8 through 10 which is disclosed in U.S. Pat. No. 4,653,983 issued to Vehr on Mar. 31, 1987 and entitled CROSS-FLOW FILM COOLING PASSAGES, which discloses a film hole with 10×10×10 streamwise three dimension diffusion hole. This type of film cooling hole includes a constant cross section flow area at the entrance region for the cooling flow metering purpose. Downstream from the constant diameter section, is a diffusion section with diffusion in three sides that include the two side walls and the downstream wall in which each of these three walls have a diffusion angle of 10 degrees from the hole axis. However, in the Vehr hole there is no diffusion in the upstream side wall (the top wall in
It is an object of the present invention to provide for a film cooling hole that will produce less turbulence than the citer prior art film holes.
It is another object of the present invention to provide for a film cooling hole that will produce less dilution of the film cooling air than the film holes of the cited prior art.
It is another object of the present invention to provide for a film cooling hole that will have a higher downstream film effectiveness than the film holes of the cited prior art.
It is another object of the present invention to provide for a film cooling hole that will produce less internal flow separation within the diffusion hole than the film hales of the cited prior art.
The film cooling hole of the present invention includes a metering section and a diffusion section that includes flow guides to form separate diffusion passages in order to minimize shear mixing between the cooling layers versus the hot gas stream. In one embodiment, three flow guides form four separate diffusion passages each having an expansion in both sideways and downstream walls of the passage. The two inner passages have the same flow area and the two outer passages have the same flow area at the exits. The middle flow guide is shorter than the two outer flow guides so that three inlets for the four passages are formed where all three inlets have the same flow area.
In a second embodiment used in a compound angled bell-mouth shaped film hole, four flow guides form five diffusion passages with an inner passage, two middle passages and two outer passages. Two inner flow guides are shorter than the two outer flow guides and form three inlets to the five passages. Each passage expands in both side wall directions and the downstream side wall direction. No expansion is formed in the upstream side wall.
The film cooling holes of the present invention are shown in
The inlet section 11 has a constant diameter along the length to provide for metering of the pressurized cooling air through the film hole 10. The downstream wall is shown in
The diffusion passages 13-16 all have expansions in the two sideways directions and the downstream side wall as seen in
The outlets of the outer diffusion passages 13 and 14 have the same flow area. The outlets of the two inner diffusion passages 15 and 16 have the same flow area. The three ribs in
In the
In the stream-wise direction, the straight wall at the upstream side of the film cooling hole has an infinite radius (straight) of curvature while the downstream side wall has a positive radius of curvature, which creates diffusion in the stream-wise flow direction. Also, the straight wall in the upstream flow direction has a built-in tapered flow guide that eliminates the hot gas entrainment problem of the prior art. The end product from the tapered flow guide in the upstream corner yields a diffusion film cooling hole at a much lower cooling injection angle. Thus, shear mixing between the cooling layers versus the hot gas stream is minimized which results in a better film layer at a higher effective level than in the prior art. The curved surfaces on the downstream wall are formed with a continuous arc connecting the point at the end of the metering section and the intersection between the expansion surfaces to the airfoil external wall. The radius of curvature for the lower surface is determined with the continuous arc tangent to the points A and cut through points B. the downstream surface for the film hole has an expansion of between 15 to 25 degrees toward the airfoil trailing edge.
The position of the exit flow guides is dependent on the film flow distribution requirement. It can be positioned at equal inlet area to obtain the same amount of film flow or one can position the flow guide at the large flow area for the corner channel than the middle channels. This allows for a higher film flow in the corner channels for the elimination of vortices formation underneath the film injection location.
In the spanwise direction, the radial outward and radial inward film cooling hole walls can be curved at the same radius of curvature. This increases the film cooling hole breakout and yields a better film coverage in the spanwise direction. This film cooling hole expansion, between 15 to 25 degrees, is valid only if the hole is oriented in the stream-wise direction or at a small compound angle at less than 20 degrees. However, if the cooling hole is used in a highly radial direction oriented application (greater than 40 degrees from the axial flow direction) then the radial outward surface for the film cooling hole has to be at a different radius of curvature than the radial inward surface. The radial outward surface will be at an expansion of less than 7 degrees. For this particular application, the radius of curvature for the inward wall can be much smaller than the outward surface and the expansion angle will from 20 to 30 degrees which is larger than the 15 to 25 degree expansion used for the stream-wise angled film hole.
Number | Name | Date | Kind |
---|---|---|---|
4684323 | Field | Aug 1987 | A |
7300242 | Liang | Nov 2007 | B2 |
7374401 | Lee | May 2008 | B2 |