Endwall component for a turbine stage of a gas turbine engine

0001The present invention relates to a component of a turbine stage of a gas turbine engine, the component forming an endwall for the working gas annulus of the stage.

0002With reference to <figref idref="f0001">Figure 1</figref>, a ducted fan gas turbine engine generally indicated at 10 has a principal and rotational axis X-X. The engine comprises, in axial flow series, an air intake 11, a propulsive fan 12, an intermediate pressure compressor 13, a high-pressure compressor 14, combustion equipment 15, a high-pressure turbine 16, and intermediate-pressure turbine 17, a low-pressure turbine 18 and a core engine exhaust nozzle 19. A nacelle 21 generally surrounds the engine 10 and defines the intake 11, a bypass duct 22 and a bypass exhaust nozzle 23.

0003The gas turbine engine 10 works in a conventional manner so that air entering the intake 11 is accelerated by the fan 12 to produce two air flows: a first air flow A into the intermediate pressure compressor 14 and a second air flow B which passes through the bypass duct 22 to provide propulsive thrust. The intermediate pressure compressor 13 compresses the air flow A directed into it before delivering that air to the high pressure compressor 14 where further compression takes place.

0004The compressed air exhausted from the high-pressure compressor 14 is directed into the combustion equipment 15 where it is mixed with fuel and the mixture combusted. The resultant hot combustion products then expand through, and thereby drive the high, intermediate and low-pressure turbines 16, 17, 18 before being exhausted through the nozzle 19 to provide additional propulsive thrust. The high, intermediate and low-pressure turbines respectively drive the high and intermediate pressure compressors 14, 13 and the fan 12 by suitable interconnecting shafts.

0005The performance of gas turbine engines, whether measured in terms of efficiency or specific output, is improved by increasing the turbine gas temperature. It is therefore desirable to operate the turbines at the highest possible temperatures. For any engine cycle compression ratio or bypass ratio, increasing the turbine entry gas temperature produces more specific thrust (e.g. engine thrust per unit of air mass flow). However as turbine entry temperatures increase, the life of an un-cooled turbine falls, necessitating the development of better materials and the introduction of internal air cooling.

0006In modern engines, the high-pressure turbine gas temperatures are hotter than the melting point of the material of the blades and vanes, necessitating internal air cooling of these airfoil components. During its passage through the engine, the mean temperature of the gas stream decreases as power is extracted. Therefore, the need to cool the static and rotary parts of the engine structure decreases as the gas moves from the high-pressure stage(s), through the intermediate-pressure and low-pressure stages, and towards the exit nozzle.

0007<figref idref="f0002">Figure 2</figref> shows an isometric view of a typical single stage cooled turbine. Cooling air flows are indicated by arrows.

0008Internal convection and external films are the prime methods of cooling the gas path components - airfoils, platforms, shrouds and shroud segments etc. High-pressure turbine nozzle guide vanes 31 (NGVs) consume the greatest amount of cooling air on high temperature engines. High-pressure blades 32 typically use about half of the NGV flow. The intermediate-pressure and low-pressure stages downstream of the HP turbine use progressively less cooling air.

0009The high-pressure turbine airfoils are cooled by using high pressure air from the compressor that has by-passed the combustor and is therefore relatively cool compared to the gas temperature. Typical cooling air temperatures are between 800 and 1000 Kelvin (K), while gas temperatures can be in excess of 2100 K.

0010The cooling air from the compressor that is used to cool the hot turbine components is not used fully to extract work from the turbine. Therefore, as extracting coolant flow has an adverse effect on the engine operating efficiency, it is important to use the cooling air effectively.

0011Ever increasing gas temperature levels combined with a drive towards flatter combustion radial profiles, in the interests of reduced combustor emissions, have resulted in an increase in local gas temperature experienced by the working gas annulus endwalls, which include NGV platforms 33, blade platforms 34 and shroud segments 35 (also known as shroud liners). However, the flow of air that is used to cool these endwalls can be highly detrimental to the turbine efficiency. This is due to the high mixing losses attributed to these cooling flows when they are returned to the mainstream working gas path flow, in particular when the air exhausts behind turbine blades.

0012<figref idref="f0003">Figure 3</figref> shows an isometric view of a typical high-pressure turbine shroud segment. The segment, which is mounted to an external casing by legs 36, provides an endwall 37 for the working gas annulus, an abradable coating being formed on the gas-washed surface of the endwall. A plurality of effusion exhaust holes 38 are formed in the endwall, cooling air passing from an internal plenum or plena through the holes to form a cooling film on the gas-washed surface. In <patcit id="pcit0001" dnum="US5993150A"><text>US 5 993 150</text></patcit>, a turbine shroud includes a panel having a forward hook and an aft hook spaced therefrom. A primary cooling circuit extends through the panel adjacent the forward hook, and has a primary inlet for receiving primary air at a first pressure, and a primary outlet for discharging the primary air. A secondary cooling circuit extends through the panel adjacent the aft hook independently of the primary circuit. The secondary circuit includes a secondary inlet for receiving secondary air at a second pressure different than the first pressure, and a secondary outlet for discharging the secondary air. <patcit id="pcit0002" dnum="WO9417285A"><text>WO 94/17285</text></patcit> discloses a turbine vane for a gas turbine engine core adaptable to be operated in a variety of thrust regimes. Various construction details are developed which provide means to provide cooling of an inner platform of the turbine vane. <patcit id="pcit0003" dnum="US2010129196A"><text>US 2010/129196</text></patcit> discloses a gas turbine vane. A cooling circuit to the trailing edge of a vane airfoil is fed from the outer diameter platform, which prevents failure due to an oxidized and eroded airfoil trailing edge. The pressure of the cooling air in the plenum or plena must be kept above the hot gas annulus pressure to prevent ingestion. In the case of a shroudless turbine blade there is a pulse of high pressure as the blade passes over the shroud segment. The plenum pressure must be kept above the peak of the pulse if ingestion of hot gas is to be avoided. However, between peaks, the excess plenum pressure can lead to excessive cooling air flow and hence can reduce engine operating efficiency.

0013An aim of the present invention is to provide a turbine stage endwall component which can operate at lower plenum pressures while avoiding the detrimental effects of hot gas ingestion.

0014Accordingly, the present invention provides a component of a turbine stage of a gas turbine engine, the component forming an endwall for the working gas annulus of the stage, and the component having: <ul id="ul0001" list-style="none" compact="compact"><li>one or more internal plena behind the endwall which, in use, contain a flow of cooling air, and a plurality of exhaust holes in the endwall, each exhaust hole extending between the plena and a gas-washed surface of the endwall such that the cooling air effuses through the holes to form a cooling film over the gas-washed surface;</li><li>wherein each exhaust hole has a flow cross-sectional area which is greater at an intermediate position between the entrance of the hole from the respective plenum and the exit of the hole to the gas-washed surface than it is at the exit.</li></ul>

0015Conventionally, exhaust holes are formed as straight cylinders having a constant flow cross-sectional area from entrance to exit. However, advantageously, by having an increased flow cross-sectional area away from their exits, the exhaust holes can have an increased fill volume, leading to expansion and pressure loss of any ingested hot gas. In this way, the time taken for the hot gas to penetrate the endwall after a pressure pulse can be increased, which in turn allows the pressure of cooling air in the plenum or plena to be reduced so that component can be operated at a lower average cooing air feed to exhaust pressure ratio.

0016The component may have any one or, to the extent that they are compatible, any combination of the following optional features.

0017The flow cross-sectional area may be greater at the intermediate position than it is at the exit by a factor of at least 1.5, and preferably by a factor of at least 2 or 4.

0018Preferably, the flow cross-sectional area is also greater at the intermediate position than it is at the entrance. In this way, any ingested hot gas can be better contained in the holes. The flow cross-sectional area may be greater at the intermediate position than it is at the entrance by a factor of at least 1.5, and preferably by a factor of at least 2 or 4.

0019The component may be a shroud segment providing a close clearance to the tips of a row of turbine blades which sweep across the segment. Such segments experience pressure pulses as they are swept over by the blades, and thus can benefit from such exhaust holes.

0020However, other turbine stage components can also experience hot gas pressure variations, e.g. due to vortex shedding from upstream structures. Thus the component may be a turbine blade, an inner platform of the blade forming the endwall. Alternatively, the component may be a static guide vane, an inner and/or an outer platform of the vane forming the endwall.

0021Embodiments of the invention will now be described by way of example with reference to the accompanying drawings in which: <ul id="ul0002" list-style="none" compact="compact"><li><figref idref="f0001">Figure 1</figref> shows a schematic longitudinal cross-section through a ducted fan gas turbine engine;</li><li><figref idref="f0002">Figure 2</figref> shows an isometric view of a typical single stage cooled turbine;</li><li><figref idref="f0003">Figure 3</figref> shows an isometric view of a typical high-pressure turbine shroud segment;</li><li><figref idref="f0003">Figure 4</figref> shows a schematic cross-sectional view through a high-pressure turbine shroud segment according to a first embodiment;</li><li><figref idref="f0004">Figure 5</figref> shows a schematic cross-sectional view through a high-pressure turbine shroud segment according to a second embodiment; and</li><li><figref idref="f0004">Figure 6</figref> shows a schematic cross-sectional view through a further high-pressure turbine shroud segment according to a third embodiment.</li><li><figref idref="f0003">Figure 4</figref> shows a schematic cross-sectional view through a high-pressure turbine shroud segment according to a first embodiment. The shroud segment has an endwall 40 which forms a gas-washed surface for the working gas annulus of an engine. Internal plena 41 are formed behind the endwall, the plena containing a flow of cooling air introduced into the plena through feed holes 42. In <figref idref="f0003">Figure 4</figref> two plena are shown, but the number could be as low as one or perhaps as high as five or six. A plurality of exhaust holes 43 traverse the endwall, each hole has an entrance 44 which receives cooling air from the plena and an exit 45 at the gas-washed surface from which the cooling air effuses to form a cooling layer over the gas-washed surface.</li></ul>

0022Each exhaust hole 43 expands in flow cross-sectional area from its entrance 44 to a maximum area at an intermediate position 46, and then contracts in flow cross-sectional area to its exit 45. The flow cross-sectional area at the intermediate position can be greater than the flow cross-sectional area at the entrance and/or the exit by a factor of at least 1.5, and preferably by a factor of at least 2 or 4.

0023There is a pulse of high pressure in the hot working gas as each turbine blade passes over the shroud segment. Due to their increased flow cross-sectional area at the intermediate position 46, the exhaust holes 43 have high internal volumes relative to conventional straight exhaust holes. Accordingly, flow of ingested hot gas through each exhaust hole 43 has to expand at the intermediate position. This in turn produces an increased pressure loss when the hot gas enters the exhaust hole. This pressure loss helps to retain the ingested hot gas in the exhaust holes for a given pressure of the cooling air in the plena. That is, the cooling air in the plena is maintained at a pressure which prevents hot gas ingestion into the plena at the peak of each pressure pulse, but by adopting exhaust holes of the type shown in <figref idref="f0003">Figure 4</figref> that pressure can be reduced, leading to consequent improvements in engine efficiency. Some hot gas ingestion into the exhaust holes occurs, but as long as the hot gas is prevented from mixing with the cooling gas in the plena, that hot gas is simply ejected from the holes after the peak of the pressure pulse is passed.

0024<figref idref="f0004">Figure 5</figref> shows a schematic cross-sectional view through a high-pressure turbine shroud segment according to a second embodiment. Corresponding features in <figref idref="f0003">Figures 4</figref> and <figref idref="f0004">5</figref> have the same reference numbers. In the second embodiment, as in the first, each exhaust hole 43 expands in flow cross-sectional area from its entrance 44 to a maximum area at an intermediate position 46, and then contracting in flow cross-sectional area to its exit 45. However, in the first embodiment, the expansion and contraction is caused by the cavity of each exhaust hole being formed as a pair of base-to-base frustocones. In contrast, in the second embodiment, the expansion and contraction is caused by the cavity being formed by two short cylindrical sections joined together by a large diameter sphere. Other shapes for the cavity can also be adopted, e.g. depending on manufacturing convenience.

0025In the first and second embodiments, the expansion in flow cross-sectional area from the entrance 44 to the intermediate position 46 helps to retain the hot gas within the exhaust holes 43. However, such an expansion is not always necessary. <figref idref="f0004">Figure 6</figref> shows a schematic cross-sectional view through a high-pressure turbine shroud segment according to a third embodiment. Corresponding features in <figref idref="f0003 f0004">Figures 4 to 6</figref> have the same reference numbers. In the third embodiment, the cavity of each exhaust hole 43 is formed by two end-to end cylinders, the interior cylinder having a greater diameter than the exterior cylinder. In this way, the hole contracts in flow cross-sectional area from its intermediate position 46 to its exit 45, but has a constant flow cross-sectional area from its entrance 44 to its intermediate position. Ingested hot gas experiences an expansion and pressure loss, and can thus still be detained in the holes.

0026While the invention has been described in conjunction with the exemplary embodiments described above, many equivalent modifications and variations will be apparent to those skilled in the art when given this disclosure. Accordingly, the exemplary embodiments of the invention set forth above are considered to be illustrative and not limiting.