This application is the US National Stage of International Application No. PCT/EP2015/069232 filed Aug. 21, 2015, and claims the benefit thereof. The International Application claims the benefit of European Application No. EP14182277 filed Aug. 26, 2014. All of the applications are incorporated by reference herein in their entirety.
The invention relates to a turbine blade for a turbomachine.
Turbomachines, especially gas turbines (in the broader sense), have a gas turbine (in the narrower sense) in which a hot gas, which beforehand has been compressed in a compressor and heated in a combustion chamber, is expanded to produce work. For high mass flows of the hot gas, and therefore high power ranges, gas turbines are constructed in an axial structural design, wherein the gas turbine is formed from a plurality of blade rings which are in series in the throughflow direction. The blade rings have impeller blades and diffuser blades which are arranged over their circumference, wherein the impeller blades are fastened on a rotor of the gas turbine and the diffuser blades are fastened on the casing of the gas turbine.
Such turbine blades are known from JP 206 307 842 A.
The higher the inlet temperature of the hot gas in the gas turbine is, the higher is the thermodynamic efficiency of gas turbines. However, limits are set upon the level of the inlet temperature by the thermal loadability of the turbine blades. Consequently, an aim is to create turbine blades which even in the case of high thermal loads have an adequate mechanical strength for operation of the gas turbine. To this end, turbine blades are provided with costly coating systems. For further increase of the permissible turbine inlet temperature turbine blades are cooled during operation of the gas turbine. In this case, film cooling constitutes a very effective and reliable method for cooling highly stressed turbine blades. In this, cool air is tapped from the compressor and guided into the turbine blades which are provided with internal cooling passages. After convective cooling of the materials from the inner side of the turbine blades, the air is directed onto the outer surface of the turbine blades by means of fluid passages. There, it forms a film which flows along the outer surface of the turbine blade and cools these and also protects them from the hot flow at the same time.
An ideal film cooling could be achieved with the aid of a slot blow-out system. Since this cannot be realized on turbine blades from the structural-mechanical point of view, cylindrical fluid passages or even fluid passages with an oval cross section are used in the first instance on account of manufacturability. Close to the principle of slot cooling, it is furthermore known to widen the cross section of the flow passages at their outlet, i.e. in the manner of a diffuser in their outflow passage section. In this case, the outlet cross section is increased by a determined factor. This leads to a fanning-out of the cooling air jet which, independently of the flow situation, involves a lowering of the jet impulse, lower mixing losses and a larger lateral covering. It is generally considered that contoured holes lead to an increase of effectiveness in the region of the fluid-passage longitudinal axis and overall to a better lateral covering.
Trials have shown that the cooling air in the fluid passages or cooling passages separates from their wall. As shown in
Annular vortices Ω1: The cooling air jet acts like an inclined cylinder upon the main flow and accelerates this. Pressure differences are formed between the side facing upstream and downstream and the upper side of the cooling air jet, which lead to a compensating flow. As a result, annular vortices Ω1 are formed. The rotation of the discharging boundary layer of the cooling air supports this effect.
Reniform vortices Ω2: The reniform vortices are a result of a vortex pair which occurs in the fluid passage. Friction forces in the free shear layer between the discharging cooling fluid jet and the main flow additionally intensify the rotation.
Horseshoe vortices Ω3: Horseshoe vortices Ω3 occur in the stagnant zone of a cylinder which is vertical in a boundary layer flow. Close to the wall, the pressure in the boundary layer is minimal. In contrast to this, in the outer layer of the main-flow boundary layer a positive pressure gradient is formed. The boundary layer separates and rolls against the wall against the main flow in the direction of the pressure minimum. The ensuing vortex is located on both sides around the cylinder. The direction of rotation of the horseshoe vortices Ω3 is opposite to that of the adjacent reniform vortices Ω2, and the horseshoe vortices Ω3 extend laterally beneath the cooling air jet during individual-hole blow-out.
Unsteady vortices Ω4: The unsteady vortices are comparable to Kármán vortices in the wake of a cylinder. The cause of the vortex formation is the boundary layer separation on the suction side of the cylinder. The unsteady vortices Ω4 occur vertically on the cooled surface.
If, therefore, hot gas from a combustion chamber of the turbomachine on the outer surface of the turbine blade meets a jet of cooling fluid discharging from the fluid passage, then the flow of hot gas is distributed around the cooling fluid jet, and a chimney vortex, with two vortex arms Ω2, is formed as a result of the action of the hot gas on the jet edge. Each of the two vortex arms Ω2 is formed by one vortex, wherein the velocity vectors of the hot gas on the two inner sides of the vortex arms point away from the outer wall.
In order to influence the vortex formation, it is known to provide turbolators in the form of fins or pins in the fluid passages (see WO 2013/089255 A1 and US 2009/0304499 A1).
The aims are to further increase the film cooling capacity. Accordingly, it is an object of the present invention to create a turbine blade for a turbomachine which can be effectively cooled using film cooling.
This object is achieved according to the invention in a turbine blade of the type referred to in the introduction by means of the characterizing features as claimed.
According to the invention, it is therefore provided that the central passage section adjoins the intermediate passage section, forming a shoulder face which lies between them and lies perpendicularly to the longitudinal axis of the fluid passage. Alternatively, a shoulder face, which lies in a plane which is inclined to the longitudinal axis of the fluid passage at an angle of α≠90°, for example about 45°, can be formed in the transition region between the intermediate passage section and the central passage section. In this case, the shoulder face is formed on a wall region of the fluid passage, whereas on the opposite wall region the intermediate passage section and the central passage section merge into each other in a straight line, i.e. without a shoulder being formed. The wall of the fluid passage can especially extend in a straight line over its entire length in this case. Alternatively, a shoulder with a low shoulder height can also be formed here, however.
The shoulder face advantageously lies on the wall region of the fluid passage which faces the hot gas side or the cold gas side.
According to one embodiment of the invention, provision is made between the central passage section and the inflow passage section for an intermediate passage section which has a constant, advantageously circular or oval, cross section over its length, wherein the longitudinal axis of the intermediate passage section is offset in relation to the longitudinal axis of the central fluid passage section and especially extends parallel to this.
It has been shown that as a result of the change of geometry which is undertaken according to the invention the flow of cooling fluid in the fluid passage can be influenced in a way that the local flow velocities in the fluid passage are adjusted in such a way that on the one hand vortex pairs Ω2, which are shown in
It has been shown that particularly good results are achieved if the central passage section has a cross-sectional area which is smaller by at least 30%, especially by at least 40% and advantageously by at least by 60%, in relation to the intermediate passage section.
If the central passage section and the intermediate passage section each have a circular cross section, the diameter D of the intermediate passage section and the diameter d of the central passage section are advantageously in the ratio of D/d=1.3 to 1.7, especially D/d=1.5.
The outflow passage section can be designed in a known way with a widening cross section in the manner of a diffuser. In this case, the wall of the fluid passage on its wall region which faces the cold gas side extends in the direction of the longitudinal axis of the fluid passage and adjoins the central passage section in a straight line. Alternatively, it can be provided that the outflow passage section has a constant, especially round, cross section over its entire length. In this case, the outflow passage section advantageously extends concentrically to the central passage section and has the same cross section as this.
With regard to advantageous embodiments of the invention, reference is made to the following description of an exemplary embodiment. In the drawing
Shown in
The transition region between the intermediate passage section 2d and the central passage section 2c is of sharp-edged design, wherein the wall of the fluid passage 2 on that side of the fluid passage 2 which faces the cold gas side extends in a straight line, and on the opposite wall region which faces the hot gas side a shoulder face 5 is formed between the intermediate passage section 2d and the central passage section 2c and lies perpendicularly to the longitudinal axis X of the fluid passage 2. Alternatively, it is also possible, however, as shown in
In
In the embodiment according to
If during operation the fluid passage 2 is exposed to a throughflow of cooling fluid, such as cooling air, the sharp-edged constriction in the transition region between the intermediate passage section 2d and the central passage section 2c leads to the cooling fluid flow—as shown in
Shown in
Shown in
Alternatively to the embodiment shown in
In the embodiment shown in
As a result of the embodiment of the fluid passage 2 according to
Although the invention has been fully illustrated and described in detail by means of the preferred exemplary embodiment, the invention is not then limited by the disclosed examples and other variations can be derived by the person skilled in the art without departing from the extent of protection of the patent.
Number | Date | Country | Kind |
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14182277 | Aug 2014 | EP | regional |
Filing Document | Filing Date | Country | Kind |
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PCT/EP2015/069232 | 8/21/2015 | WO | 00 |
Publishing Document | Publishing Date | Country | Kind |
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WO2106/030289 | 3/3/2016 | WO | A |
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