1. Field of the Invention
The present invention relates to a turbine moving blade applied to a steam turbine.
2. Description of the Related Art
In general, a steam turbine includes a plurality of stages each composed of a moving blade and a stator vane axially provided on a turbine rotor. In addition, the steam turbine is provided, on an outer circumferential portion of an outlet of its final stage, with a flow guide portion adapted to lead steam into an exhaust hood. Such a steam turbine is operated such that the stator vane formed as a restrictive passage accelerates steam to increase its kinetic energy and the moving blade converts the kinetic energy into rotational energy to generate power. Then, some of the steam is turned in an extraction channel in a rotor-radial direction and rest of the steam is discharged into the exhaust hood. See JP-2003-27901-A.
Since shortening the length of a turbine shaft in such a steam turbine can reduce a difference in an axial thermal extension of the turbine rotor, the effects of reducing loss resulting from leakage flow and improving reliability in turbine shaft vibration can be expected.
The axial length of a low-pressure turbine depends on a position at which the radial turning of a flow guide provided at the downstream end of an external stationary wall of a final stage terminates. Therefore, if the curvature of the flow guide portion is increased, the radial turning of the flow guide portion can be terminated on the more upstream side in a steam flow direction (hereinafter, simply described as the upstream side). Thus, the length of the turbine shaft can be reduced. However, the exhaust chamber is formed as a diffuser path, which has an inverse pressure gradient. Because of this, if the curvature of the flow guide portion is increased to increase a flare angle of the flow guide portion, separation of a steam flow from the flow guide portion is likely to occur, which may probably cause a flow loss. Incidentally, the above-mentioned flare angle means an angle formed between a steam passage outer circumferential wall and a turbine central axis.
In addition, it is necessary to radially turn the stream flow in a shorter shaft length by reducing the turbine shaft length. Therefore, in an extraction stage provided on the upstream side of the low-pressure turbine, a deviation is increased between a flare angle of a shroud inner circumferential surface of a blade constituting the extraction stage and a flare angle of an outer circumferential side stationary wall inner circumferential surface adjacently provided on the moving blade downstream side. In addition, a distance between the moving blade outlet and the extraction path is reduced and the steam flow is radially turned in a shorter distance between the moving blade outlet and the extraction path inlet. Thus, a separation swirl is likely to occur at the extraction path inlet, which may probably cause a flow loss.
Accordingly, it is an object of the present invention to provide a steam turbine moving blade that can reduce the length of a turbine shaft while suppressing occurrence of a loss resulting from flow separation and from a secondary flow to suppress a decrease in turbine efficiency.
To solve the above object, according to an aspect of the present invention, there is provided a moving blade for a steam turbine, the moving blade having a shroud formed at an outer circumferential side distal end, wherein the shroud has an inner circumferential surface so formed that a moving blade outlet flare angle is greater than a moving blade inlet flare angle, the moving blade inlet flare angle is generally equal to a moving blade upstream side flare angle of an outer circumferential side stationary wall adjacently provided on an upstream side of the shroud; and the moving blade outlet flare angle is generally equal to a moving blade downstream side flare angle of the outer circumferential side stationary wall adjacently provided on a downstream side of the shroud. More specifically, the moving blade and the steam turbine are each configured as recited in corresponding claims.
The present invention can reduce the length of a turbine shaft while suppressing occurrence of a loss resulting from flow separation and from a secondary flow to suppress a decrease in turbine efficiency.
Preferred embodiments of the present invention will hereinafter be described in detail with reference to the drawings. Incidentally, like or corresponding elements are denoted with like reference numerals over the drawings.
A description is given of a first embodiment of the present invention.
Arrow 51 in
A casing 9 for covering the outer circumferential side stationary wall 4 is provided on a turbine-radially outer circumferential side (hereinafter, simply described as the outer circumferential side) of the outer circumferential side stationary wall 4. An exhaust hood 12 is defined between the outer circumferential side stationary wall 4 and the casing 9. A flow guide portion 11 adapted to lead steam leaving the moving blade 1 to the exhaust hood 12 is formed at the downstream side end portion of the outer circumferential side stationary wall 4. A bearing cone 10 is provided on a turbine-radially inner circumferential side (hereinafter, simply called the inner circumferential side) of the flow guide portion 11. In this way, an annular diffuser path 18 is defined between the bearing cone 10 and the flow guide portion 11.
The flow guide portion 11 and the bearing cone 10 are each bent in the turbine-radial direction. The diffuser path 18 communicates with the exhaust hood 12. Thus, the steam having passed through the final stage moving blade 1 passes through the diffuser path 18. While the flowing direction is turned from the axial direction to the radial direction, the steam decelerates so that energy according to the deceleration is converted to pressure to recover pressure. Then, the steam is led to the exhaust hood. After having led to the exhaust hood 12, the steam is introduced into a condenser (not illustrated) communicating with the exhaust hood.
A description is next given of a structure of the shroud 3. Hereinafter, a flare angle is defined as an angle formed between an outer circumferential wall of a steam path 19 and a turbine central axis 50. The outer circumferential wall of the steam path 19 means e.g. an inner circumferential wall surface 13 of the outer circumferential side stationary wall 4, an inner circumferential surface 14 of the shroud 3 or an inner circumferential surface 15 of the flow guide portion 11.
Referring to
An angle formed between the inner circumferential surface 13 of the outer circumferential side stationary wall 4 constituting the final stage and the turbine central axis 50 is referred to as a moving blade upstream side flare angle α1. The flow guide portion 11 is formed to be radially smoothly bent so that the flare angle is gradually increased from the upstream side toward the downstream side. An angle formed between the turbine central axis 50 and a tangential line (indicated with a broken line) extending from a curvature start point C of the inner circumferential surface 15 of the flow guide portion 50 is referred to as a moving blade downstream side flare angle α4. In the present embodiment, the inner circumferential surface 14 of the shroud 3 is formed as below. The moving blade inlet flare angle α2 is generally equal to the moving blade upstream side flare angle α1 of the outer circumferential side stationary wall 4 adjacently provided on the moving blade upstream side. In addition, the moving blade outlet flare angle α3 is generally equal to the moving blade downstream side flare angle α4 of the floor guide portion 11 of the outer circumferential side stationary wall adjacently provided on the moving blade downstream side.
On the other hand, the outer circumferential surface of the shroud 3 has an inclination surface 16 on the upstream side and a parallel surface 17 parallel to the turbine central axis 50 on the downstream side. A shroud upstream side outer diameter is made smaller than a shroud downstream side outer diameter. The shroud upstream side outer diameter is a distance from the turbine central axis 50 to the upstream side end of the outer circumferential surface of the shroud 3. The shroud downstream side outer diameter is a distance from the turbine central axis 50 to the downstream side end of the outer circumferential surface of the shroud 3. Incidentally, the inclination angle of the inclination surface 16 is set such that the shroud 3 has a thickness generally uniform from the upstream side to the downstream side.
Seal fins 6 are provided on the outer circumferential side stationary wall 4 opposite the parallel surface 17 of the outer circumferential surface of the shroud 3. This narrows a gap between the outer circumferential side stationary wall 4 and the shroud 3 to suppress leakage of a steam flow getting around the moving blade 1. Incidentally, in the turbine final stage, a leakage passage area defined between the seal fins and the shroud is smaller than the passage area of the moving blade. Therefore, the seal fins 6 may be provided only on the moving blade outlet side.
A description is given of a function and effect of the present embodiment. The inner circumferential surface 14 of the shroud 3 is formed such that the moving blade inlet flare angle α2 is generally equal to the moving blade upstream side flare angle α1 and the moving blade outlet flare angle α3 is generally equal to the moving blade downstream side flare angle α4. Therefore, steam flows parallel to the inner circumferential surface from the outer circumferential side stationary wall 4 to the shroud 3. The steam flows parallel to the inner circumferential surface from the shroud 3 to the flow guide portion 11. The flow of steam is radially smoothly turned between the stator vane and the moving blade and between the moving blade and the flow guide portion. Thus, occurrence of a loss resulting from flow separation and from a secondary flow can be suppressed, which can suppress the lowering of turbine efficiency.
In the present invention, it is preferred that the moving blade inlet flare angle α2 be equal to the moving blade upstream side flare angle α1 and the moving blade outlet flare angle α3 be equal to the moving blade downstream side flare angle α4. However, if respective deviations of the flare angles are generally equal to each other, i.e., if each of the deviations falls within 5°, achievement of the effect of the present invention can be expected.
The internal circumferential surface 14 of the shroud 3 is formed such that the moving blade outlet flare angle α3 is greater than the moving blade inlet flare angle α2 so as to allow also the moving blade 1 to take on a share of the radial turning of steam. The steam on the moving blade shroud side of the low-pressure turbine final stage has high-speed and large kinetic energy. Conventionally, this high-speed steam has radially been turned mainly by the diffuser path 18 and the exhaust hood 12 having an inverse pressure gradient. In the present invention, the radial turning of steam is shared by the inside of the moving blade at which steam speed is slower and the kinetic energy is smaller than at the outlet of the moving blade. Therefore, a radially turning amount of steam flow in the exhaust hood 12 can be made smaller than ever before. Consequently, if the radius of curvature of the inner circumferential surface 15 of the flow guide portion 11 is equal to the traditional one, i.e., if separation occurrence potential of the passage shape is generally equal to the traditional one, the shaft length to a position where steam is radially turned can be reduced.
The increase in flare angle due to the reduced length of the turbine shaft increases the curvature of the shroud 3, i.e., increases the difference between the moving blade outlet flare angle α3 and the moving blade inlet flare angle α2. However, the inclination surface 16 is formed on the upstream side of the outer circumferential surface of the shroud 3 and the parallel surface 17 is formed on the downstream side in parallel to the central axis. This makes the upstream side outer diameter smaller than the downstream side outer diameter. The above-mentioned upstream side outer diameter corresponds to the distance from the turbine central axis 50 to the upstream side distal end of the outer circumferential surface of the shroud 3. In addition, the above-mentioned downstream side outer diameter corresponds to the distance from the turbine central axis 50 to the downstream side distal end of the outer circumferential surface of the shroud 3. Thus, the weight increase of the shroud per se can be suppressed. As a result, it is possible to prevent the strength reliability of the turbine blade from lowering.
A description is next given of a second embodiment of the present invention.
In the present embodiment, an inner circumferential surface downstream side end portion of an outer circumferential side stationary wall 4 supporting a stator vane 2 of a final stage is formed parallel to a turbine central axis 50. In addition, a moving blade upstream side flare angle α1 is formed at an approximately 0 degree at an outlet of the outer circumferential side stationary wall 4. On the other hand, an inner circumferential surface of a shroud 3 is composed of an upstream side parallel surface 21 parallel to the turbine central axis 50 and a downstream side inclination surface 22. Incidentally, the upstream side end portion of the inner circumferential surface is included in the parallel surface 21 and the downstream side end portion is included in the inclination surface 22.
A moving blade inlet flare angle and a moving blade outlet flare angle are defined as below. If the upstream side end portion of the inner circumferential surface is included in a plane (precisely, curve-shaped in a circumferential direction and straight line-shaped in an axial direction, hereinafter, simply described as the plane), an angle formed between the plane including the upstream side end portion and the central axis, i.e., an angle formed between a cross-line which the plane including the upstream side end portion crosses with a turbine meridian plane and the central axis, is referred to as the moving blade inlet flare angle. If the downstream side end portion of the inner circumferential surface is included in the plane, an angle formed between the plane including the downstream side end portion and the central axis i.e., an angle formed between a cross-line which the plane including the downstream side end portion crosses with a turbine meridian plane and the central axis, is referred to as the moving blade outlet flare angle. Thus, in the present embodiment, an angle formed between the parallel surface 21 and the turbine central axis 50 is defined as a moving blade inlet flare angle α2. An angle formed between the inclination surface 22 and the turbine central axis 50 is defined as a moving blade outlet flare angle α3.
In the present embodiment, the inner circumferential surface of the shroud 3 is such that the moving blade inlet flare angle α2 is generally equal to a moving blade upstream side flare angle α1 and the moving blade outlet flare angle α3 is generally equal to a moving blade downstream side flare angle α4 of a floor guide portion 11. In addition, the moving blade outlet flare angle α3 is formed to be greater than the moving blade inlet flare angle α2. Incidentally, as shown in
The outer circumferential surface of the shroud 3 has an upper stream side parallel surface 23 being parallel to the turbine central axis 50 and including an upstream side end, a downstream side parallel surface 25 being parallel to the turbine central axis 50 and including a downstream side end, and an inclination surface 24 inclined relative to the turbine central axis 50 and connecting the upstream side parallel surface with the downstream side parallel surface. The shroud 3 is formed such that its upstream side outer diameter is smaller than its downstream side outer diameter. The upstream side outer diameter is a distance from the turbine central axis 50 to the upstream side distal end of the outer circumferential surface of the shroud 3. The downstream side outer diameter is a distance from the turbine central axis 50 to the downstream side distal end of the outer circumferential surface of the shroud 3. In addition, the shroud 3 is formed to have a generally constant thickness from the upstream side to the downstream side.
In the present embodiment, the inner circumferential surface 14 of the shroud 3 is formed as below. The moving blade inlet flare angle α2 is generally equal to the moving blade upstream side flare angle α1. The moving blade outlet flare angle α3 is generally equal to the moving blade downstream side flare angle α4. Further, the moving blade outlet flare angle α3 is greater than the moving blade inlet flare angle α2. Therefore, steam 20 flows between the inner circumferential surface 14 of the shroud 3 and the inner circumferential surface 13 of the outer circumferential side stationary wall 4 and between the inner circumferential surface 14 of the shroud 3 and the inner circumferential surface 15 of the flow guide portion 11, in general parallel to the inner circumferential surfaces. Thus, occurrence of a loss resulting from steam flow separation and from a secondary flow can be suppressed, which can suppress the lowering of turbine efficiency.
Incidentally, also in the present embodiment, it is preferred that the moving blade inlet flare angle α2 be equal to the moving blade upstream side flare angle α1 and the moving blade outlet flare angle α3 be equal to the moving blade downstream side flare angle α4. However, if respective deviations of the flare angles are generally equal to each other, i.e., if each of the deviations falls within 5°, achievement of the effect of the present invention can be expected.
It is possible to turn the steam flow in the radial direction between the inlet and outlet of the moving blade 2. It is possible to make the amount of radially turning steam flow smaller than ever before in the exhaust hood 12 including the flow guide portion 11 having high separation potential due to inverse pressure gradient. As a result, if the curvature radius of the inner circumferential surface 15 of the flow guide portion 11 is equal to the traditional one, i.e., if the separation occurrence potential of the passage shape is general equal to the traditional one, it is possible to reduce the shaft length to the radial turn.
The upstream side outer diameter which is the distance from the turbine central axis 50 to the upstream side distal end of the outer circumferential surface of the shroud 3 is made smaller than the downstream side outer diameter which is the distance from the turbine central axis 50 to the downstream side distal end of the outer circumferential surface of the shroud 3. Therefore, even if the tilted angle of the inclination surface 22 is increased, it is possible to suppress the increase in the weight of the shroud per se. Consequently, it is possible to prevent the strength reliability of the turbine blade from lowering.
A description is given of a third embodiment of the present invention.
Referring to
A plurality of moving blades 31 are secured to a turbine rotor 7 between the stator vanes 26 and the extraction port 29. The moving blades 31, along with the stator vanes 26, constitute an extraction stage. A shroud 32 is mounted on the outer circumferential ends of the moving blades 31. An internal circumferential surface 33 of the shroud 32 is radially smoothly bent to gradually increase a flare angle from the upstream toward the downstream. In addition, the internal circumferential surface 33 is formed such that a moving blade outlet flare angle α3 is greater than a moving blade inlet flare angle α2. The moving blade outlet flare angle α3 is an angle formed between a tangential line F (indicated with a broken line) at a downstream side distal end of the shroud inner circumferential surface 33 and a turbine central axis 50. The moving blade inlet flare angle α2 is an angle formed between a tangential line E (indicated with a broken line) at an upstream side distal end of the shroud inner circumferential surface 33 and the turbine central axis 50.
An angle formed between an inner circumferential surface 34 of the outer circumferential side stator blade wall 27 and the turbine central axis 50 is defined as a moving blade upstream side flare angle α1. An angle formed between an upstream side lateral wall of the extraction port 29 and the turbine central axis 50 is defined as a moving blade downstream side flare angle α4. The inner circumferential surface 33 of the shroud 32 in the present embodiment is formed such that the moving blade inlet flare angle α2 is generally equal to the moving blade upstream side flare angle α1. In addition, the moving blade outlet flare angle α3 is generally equal to the moving blade downstream side flare angle α4.
An outer circumferential surface of the shroud 32 is composed of an upstream side parallel surface 37 being parallel to the turbine central axis 50 and including an upstream side end; a downstream side parallel surface 38 being parallel to the turbine central axis 50 and including a downstream side parallel surface 38; and a curved surface 39 radially bent relative to the turbine central axis 50 so as to connect the upstream side parallel surface 37 with the downstream side parallel surface 38. Also in the present embodiment, the shroud upstream side outer diameter is made smaller than the shroud downstream side outer diameter. This intends to reduce the weight of the shroud.
The low-pressure turbine upstream stage may suffer from a significant influence on performance degradation caused by steam leakage. Therefore, seal fins 6 are arranged on the inner circumferential surface of the outer circumferential side stationary wall 27 opposite the upstream side parallel surface 37 and the downstream side parallel surface 38 so as to be circumferentially extended. A step is provided on a seal fin installation portion of the outer circumferential side stationary wall in order to make a distance between the seal fins and the parallel surfaces constant. The positional relationship between the seal fins 6 and the shroud 32 is axially shifted due to thermal extension difference resulting from high temperature during the operation. However, even in such a case, since the seal fins are arranged on the parallel surfaces of the shroud outer circumferential surface, a gap between the seal fins 6 and the shroud 32 can be allowed to remain unchanged during operation to maintain sealing performance.
As shown in
Returning to
Incidentally, also in the present embodiment, it is preferred that the moving blade inlet flare angle α2 be equal to the moving blade upstream side flare angle α1 and the moving blade outlet flare angle α3 be equal to the moving blade downstream side flare angle α4. However, if respective deviations of the flare angles are generally equal to each other, i.e., if each of the deviations falls within 5°, achievement of the effect of the present invention can be expected.
The shroud shown in
A description is given of a fourth embodiment of the present invention.
The present embodiment has a structure different from the third embodiment in a shroud. An inner circumferential surface of the shroud 43 of the present embodiment is composed of an upstream side inner circumferential surface 45 including an upstream end and a downstream side inner circumferential surface 46 including a downstream end. Also in the present embodiment, the inner circumferential surface of the shroud 43 is formed as below. A moving blade inlet flare angle α2 is generally equal to a moving blade upstream side flare α1. The moving blade inlet flare angle α2 is an angle formed between the upstream side inner circumferential surface 45 and the turbine central axis 50. The moving blade upstream side flare angle α1 is an angle formed between the inner circumferential surface 33 of the outer circumferential side stationary wall 27 and the turbine central axis 50. In addition, a moving blade outlet flare angle α3 is generally equal to a moving blade downstream side flare angle α4. The moving blade outlet flare angle α3 is an angle formed between the downstream side inner circumferential surface 46 and the turbine central axis 50. The moving blade downstream side flare angle α4 is an angle formed between an inner circumferential surface 36 of an outer circumferential side stationary wall 28 adjacently provided on the downstream side. Further, the moving blade outlet flare angle α3 is formed greater than the moving blade inlet flare angle α2.
In contrast, the outer circumferential surface 47 of the shroud 43 is composed of a parallel surface parallel to the turbine central axis 50 from the upstream end to the downstream end. In addition, seal fins 6 are provided on the outer circumferential side stationary wall 27 opposite the parallel surface.
The present embodiment provides the same effect as that of the third embodiment shown in
A description is given of a fifth embodiment of the present invention.
Number | Date | Country | Kind |
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2009-062229 | Mar 2009 | JP | national |