JPH11190203A - Axial flow turbine blade cascade - Google Patents
Axial flow turbine blade cascadeInfo
- Publication number
- JPH11190203A JPH11190203A JP35756597A JP35756597A JPH11190203A JP H11190203 A JPH11190203 A JP H11190203A JP 35756597 A JP35756597 A JP 35756597A JP 35756597 A JP35756597 A JP 35756597A JP H11190203 A JPH11190203 A JP H11190203A
- Authority
- JP
- Japan
- Prior art keywords
- blade
- flow
- turbine
- end wall
- cascade
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
- 230000003187 abdominal effect Effects 0.000 claims description 22
- 239000011295 pitch Substances 0.000 claims 1
- 230000003313 weakening effect Effects 0.000 abstract description 2
- 230000000452 restraining effect Effects 0.000 abstract 1
- 239000012530 fluid Substances 0.000 description 37
- 230000003068 static effect Effects 0.000 description 12
- 230000007423 decrease Effects 0.000 description 5
- 238000011144 upstream manufacturing Methods 0.000 description 5
- 238000010586 diagram Methods 0.000 description 4
- 230000003111 delayed effect Effects 0.000 description 2
- 210000001015 abdomen Anatomy 0.000 description 1
- 230000015556 catabolic process Effects 0.000 description 1
- 239000000567 combustion gas Substances 0.000 description 1
- 238000006731 degradation reaction Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 239000000284 extract Substances 0.000 description 1
- 239000007789 gas Substances 0.000 description 1
Landscapes
- Turbine Rotor Nozzle Sealing (AREA)
Abstract
Description
【0001】[0001]
【発明の属する技術分野】本発明は、蒸気タービン及び
ガスタービン等に利用され、翼列を構成する3次元翼型
の翼端壁近傍に発生する2次流れで発生する2次流れ渦
によるエネルギー損失をそれぞれ低減し、性能を大幅に
向上できる軸流タービン翼に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention is used in a steam turbine, a gas turbine, and the like, and uses a secondary flow vortex generated in a secondary flow generated near a tip wall of a three-dimensional airfoil constituting a cascade. The present invention relates to an axial flow turbine blade capable of reducing loss and greatly improving performance.
【0002】[0002]
【従来の技術】翼列を形成する3次元翼型の翼根、若し
くは翼端近傍の翼端壁に発生する、2次流れにより発達
する2次流れ渦で生じるエネルギー損失によって、大き
な翼列損失が発生する軸流タービン翼においては、これ
らの翼列損失を低減することが性能向上上重要である。2. Description of the Related Art A large cascade loss is caused by energy loss caused by a secondary flow vortex developed by a secondary flow generated on a root of a three-dimensional airfoil forming a cascade or on a tip wall near a blade tip. In an axial flow turbine blade in which turbulence occurs, it is important to reduce these cascade losses in order to improve performance.
【0003】図3は、翼列を形成するように、翼端壁2
にタービン翼1を周方向に立設して設けられた軸流ター
ビン翼の翼列内部の流れの様子を示す模式図である。図
に示すように、翼列上流の翼端壁2付近を流れる蒸気又
は燃焼ガス等の作動流体Fの流れは、タービン翼1の前
縁に衝突すると、翼端壁2側へ潜り込み、通路渦を形成
する。FIG. 3 shows a blade tip wall 2 so as to form a cascade.
FIG. 3 is a schematic diagram showing a state of a flow inside a cascade of axial flow turbine blades provided with a turbine blade 1 erected in a circumferential direction. As shown in the figure, the flow of the working fluid F such as steam or combustion gas flowing near the blade tip wall 2 upstream of the cascade collides with the leading edge of the turbine blade 1 and sinks into the blade tip wall 2 to form a passage vortex. To form
【0004】この通路渦の渦管は、翼端壁2付近の翼前
縁を取り巻くように形成され、1点鎖線で示すように、
その形状が馬蹄形状をしていることから、通常馬蹄渦3
と呼ばれている。一方、隣接して配設されたタービン翼
1の、一方のタービン翼1の翼腹面4と他方のタービン
翼1の翼背面5とで挟まれて、形成される翼列内部に形
成される翼間流路8内における翼端壁2付近では、翼腹
面4と翼背面5とにそれぞれ作用する作動流体Fによっ
て生じる圧力差によって、翼腹面4側から翼背面5側に
向けて流れる2次流れ6が形成される。[0004] The vortex tube of this passage vortex is formed so as to surround the leading edge of the wing near the wing tip wall 2, and as shown by a dashed line,
Since the shape is a horseshoe shape, the normal horseshoe vortex 3
It is called. On the other hand, of the turbine blades 1 disposed adjacent to each other, the blades formed in the cascade formed by being sandwiched between the blade abdominal surface 4 of one turbine blade 1 and the blade back surface 5 of the other turbine blade 1. In the vicinity of the wing tip wall 2 in the interflow path 8, a secondary flow flowing from the wing apex face 4 side to the wing back face 5 due to a pressure difference generated by the working fluid F acting on the wing apex face 4 and the wing back face 5, respectively. 6 are formed.
【0005】このため、特に、作動流体Fがタービン翼
1の前縁に衝突して生じる馬蹄渦3のうち、翼腹面4側
へ流れる馬蹄渦3は、作動流体Fによって翼間流路8内
を下流側へ流されるとともに、翼腹面4側から翼背面5
側に向けて流れ、この2次流れ6により、翼間流路8内
を翼背面5側へと流されながら、2次流れ渦7と呼ばれ
る大きな渦に発達する。[0005] Therefore, among the horseshoe vortices 3 generated when the working fluid F collides with the leading edge of the turbine blade 1, the horseshoe vortex 3 flowing toward the blade abdominal surface 4 is caused by the working fluid F in the inter-blade flow path 8. From the wing abdominal surface 4 side to the wing back surface 5
The secondary flow 6 develops into a large vortex called a secondary flow vortex 7 while flowing in the inter-blade flow path 8 toward the blade back surface 5 by the secondary flow 6.
【0006】この2次流れ渦7は、その中心にエネルギ
ー損失の大きい流体、いわゆる圧損流体を含んでいるう
えに、それ自体が相互に摩擦してエネルギー損失を発生
するとともに、翼背面5等の壁面との摩擦によって大き
なエネルギー損失を発生する、いわゆる粘性散逸作用を
もっており、翼間流路8内を流れる作動流体Fのエネル
ギー損失を大きくするため、作動流体Fの運動エネルギ
ーを仕事として取り出すタービン翼列においては、この
2次流れ渦7の発達によって、性能低下につながること
になる。The secondary flow vortex 7 contains a fluid having a large energy loss at the center thereof, that is, a so-called pressure-loss fluid. A turbine blade that has a so-called viscous dissipation action that generates a large energy loss due to friction with a wall surface, and extracts kinetic energy of the working fluid F as work in order to increase the energy loss of the working fluid F flowing in the inter-blade flow path 8. In a row, the development of this secondary flow vortex 7 will lead to a performance degradation.
【0007】一般に、翼腹面4と翼背面5とにそれぞれ
作用する作動流体Fによって生じる圧力差が大きい程、
前述した2次流れ6の強さは強くなり、また、翼間流路
8内を翼腹面4から翼背面5へ流されながら発達する2
次流れ渦7は、翼端壁2近傍の2次流れ6の強さが強い
ほど大きく発達し、これに伴い粘性散逸作用も大きくな
り、2次流れ渦7によるタービン翼列の性能低下が著し
くなる。In general, the larger the pressure difference caused by the working fluid F acting on the blade flank 4 and the blade back 5, the greater
The strength of the secondary flow 6 described above increases, and the secondary flow 6 develops while flowing in the interblade flow path 8 from the blade abdominal surface 4 to the blade back surface 5.
The secondary flow vortex 7 develops more as the strength of the secondary flow 6 near the blade tip wall 2 increases, and the viscous dissipation action also increases, and the secondary flow vortex 7 significantly reduces the performance of the turbine cascade. Become.
【0008】[0008]
【発明が解決しようとする課題】本発明は、2次流れ渦
で生じるエネルギー損失によって、大きな翼列損失が生
じ性能低下をきたしている、従来の軸流タービン翼列の
不具合を解消するため、翼腹面と翼背面とにそれぞれ作
用する作動流体によって生じる、翼腹面側と翼背面側と
の間に生じる圧力差が小さくするにつれて、この圧力差
によって生じる2次流れの強さ、特に、翼端壁近傍の圧
力差を小さくして、翼端壁近傍に発生する2次流れの強
さを弱くして、2次流れ渦の発達を抑制して、又はでき
るだけ遅らせ、翼間流路内を流れる作動流体のエネルギ
ー損失を小さくして、タービン翼列の性能を向上させる
ようにした、軸流タービン翼列を提供することを課題と
する。SUMMARY OF THE INVENTION The present invention solves the problem of the conventional axial flow turbine cascade, in which a large cascade loss is caused by the energy loss generated by the secondary flow vortex, and the performance is deteriorated. As the pressure difference between the abdominal surface and the back surface of the blade caused by the working fluid acting on the abdominal surface and the back surface of the blade decreases, the strength of the secondary flow caused by the pressure difference, in particular, the blade tip By reducing the pressure difference near the wall, weakening the intensity of the secondary flow generated near the blade tip wall, suppressing or delaying the development of the secondary flow vortex, and flowing in the inter-blade flow path An object of the present invention is to provide an axial turbine cascade in which the energy loss of a working fluid is reduced and the performance of the turbine cascade is improved.
【0009】[0009]
【課題を解決するための手段】このため、本発明の軸流
タービン翼列は次の手段とした。For this reason, the axial flow turbine cascade of the present invention has the following means.
【0010】(1)周方向に翼列を形成するように、翼
端壁に立設されたタービン翼の翼腹面近傍の流れ方向の
断面形状が、流れ方向の中央部ほど翼端壁を内方に向け
て突出量を大きくした凸面形状にされ、(2)タービン
翼の翼背面近傍の流れ方向の断面形状が、流れ方向の中
央部ほど翼端壁を外方に向けて突出量を大きくした凹面
形状にされ、(3)流れ方向の断面形状が凸面形状にさ
れた翼腹面近傍の翼端壁と、流れ方向の断面形状が凹面
形状にされた翼背面近傍の翼端壁とが、周方向には滑ら
かに接続されて、翼端壁の周方向には、等ピッチの凹凸
面が形成されるようにした横断面形状が、流れ方向に形
成された翼間流路を、隣接するタービン翼とともに形成
するものとした。(1) The cross-sectional shape in the flow direction near the blade abdominal surface of the turbine blade erected on the blade tip wall so as to form a blade row in the circumferential direction is such that the more the center in the flow direction, the deeper the blade tip wall becomes. (2) The cross-sectional shape in the flow direction near the blade back surface of the turbine blade increases toward the center of the flow direction with the blade end wall outwardly increasing toward the center. (3) A wing tip wall near the wing apex surface having a convex cross-sectional shape in the flow direction, and a wing tip wall near the wing back surface having a concave cross-sectional shape in the flow direction, In the circumferential direction of the blade tip wall, the cross-sectional shape that is smoothly connected in the circumferential direction and the uneven pitch surface is formed at an equal pitch adjoins the inter-blade flow path formed in the flow direction. It was formed together with the turbine blade.
【0011】なお、流れ方向の中央部ほど翼端壁を内方
に向く突出量を大きくして、翼腹面近傍の流れの方向に
設けられる凸面形状の断面形状にされた翼端壁の上流、
および下流端側は、凹凸面を設けずに、タービン翼を設
置するようにした通常の翼端壁面より外方に向けて突出
させるとともに、流れ方向の中央部ほど翼端壁を外方に
向く突出量を大きくして、翼背面近傍の流れの方向に設
けられる凹面形状の断面形状にされた翼端壁の上流、お
よび下流端側は、通常の翼端壁面より内方に向けて突出
させるようにした断面形状することが好ましい。It is to be noted that, by increasing the amount of inward projection of the wing tip wall toward the center in the flow direction, the upstream of the wing tip wall having a convex cross-sectional shape provided in the flow direction near the wing abdominal surface,
And the downstream end side, without providing the uneven surface, project outward from the normal blade end wall where the turbine blade is installed, and the blade end wall faces outward toward the center in the flow direction By increasing the amount of protrusion, the upstream and downstream end sides of the blade end wall having a concave cross-sectional shape provided in the flow direction near the blade rear surface are made to project inward from the normal blade end wall surface. It is preferable that the cross section be shaped as described above.
【0012】本発明の軸流タービン翼列は、上述の手段
により、タービン翼が立設される翼端壁が凸面形状にさ
れた翼腹面近傍の、しかも、翼端壁に近い部分の翼間流
路を流れる作動流体ほど、翼端壁の凸面形状により加速
され、これに伴い、この部分の静圧が低下する。また、
凹面形状にされた翼背面近傍の、しかも、翼端壁に近い
部分の翼間流路を流れる作動流体ほど、翼端壁の凹面形
状により減速され、これに伴い、この部分の静圧が上昇
する。According to the axial flow turbine cascade of the present invention, by the means described above, the inter-blade between the blade apex and the portion close to the blade end wall where the blade end wall on which the turbine blade is erected is made convex is provided. The working fluid flowing through the flow path is accelerated by the convex shape of the blade tip wall, and accordingly, the static pressure in this portion decreases. Also,
The working fluid flowing through the inter-blade flow path in the vicinity of the back surface of the wing and in the vicinity of the wing tip wall is decelerated by the concave shape of the wing tip wall, and the static pressure in this part increases accordingly. I do.
【0013】これにより、翼腹面と翼背面とにそれぞれ
作用する作動流体Fによって生じる圧力差、すなわち翼
背面近傍の静圧より翼腹面近傍の静圧が高くなる圧力
差、しかも、2次流れ渦が発生し、発達していく翼端壁
近傍における圧力差ほど緩和され、翼腹面側から翼背面
側へ向けて流れる2次流れの強さは弱められる。As a result, a pressure difference generated by the working fluid F acting on each of the blade abdominal surface and the blade back surface, that is, a pressure difference in which the static pressure near the blade abdominal surface is higher than the static pressure near the blade back surface, and a secondary flow vortex Is generated and the pressure difference in the vicinity of the developing blade tip wall is alleviated, and the strength of the secondary flow flowing from the blade abdominal surface toward the blade rear surface is reduced.
【0014】このため、翼間流路内を翼腹面側から翼背
面側へ流されながら下流側へ流れる2次流れ渦は、この
翼端壁近傍の2次流れの強さが弱められることにより発
達が抑制され、さらには、発達の速度が遅らされ、翼間
流路を流れているときに作動流体に含まれる圧損流体の
量が低減するとともに、粘性散逸作用も小さくなり、翼
間流路内を流れる作動流体の2次流れ渦によるエネルギ
ー損失を小さくして、タービン翼列の性能を向上させる
ことができ、タービン効率の良い軸流タービン翼列とす
ることができる。For this reason, the secondary flow vortex flowing downstream from the blade apex side to the blade back side in the blade-to-blade flow path is weakened by reducing the strength of the secondary flow near the blade tip wall. The development is suppressed, and furthermore, the speed of development is slowed down, the amount of pressure loss fluid contained in the working fluid when flowing in the inter-blade flow path is reduced, and the viscous dissipation action is also reduced, and the inter-blade flow Energy loss due to the secondary flow vortex of the working fluid flowing in the path can be reduced, the performance of the turbine cascade can be improved, and an axial turbine cascade with high turbine efficiency can be obtained.
【0015】[0015]
【発明の実施の形態】以下、本発明の軸流タービン翼列
の実施の一形態を図面にもとづき説明する。図1は、本
発明の軸タービン翼列の実施の第1形態としての軸流タ
ービン翼列の一部分を示す模式図、図2は、図1に示す
軸流タービン翼列の流れ方向翼端壁形状の概念図であ
る。なお、図において図3に示す部材と同一部材には、
同一符番を付して説明は省略する。DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of an axial turbine cascade according to the present invention will be described below with reference to the drawings. FIG. 1 is a schematic view showing a part of an axial turbine cascade as a first embodiment of the axial turbine cascade of the present invention. FIG. 2 is a flow direction blade end wall of the axial turbine cascade shown in FIG. It is a conceptual diagram of a shape. In the figure, the same members as those shown in FIG.
The same reference numerals are given and the description is omitted.
【0016】図において、9は翼端壁2上において翼腹
面4近傍を流れる作動流体Fの流れ方向に設けられた腹
面側切断線、10は同様に翼端壁2上において翼背面近
傍を流れる作動流体の流れ方向に設けられた背面側切断
線である。この翼腹面4付近、翼背面5付近の流れ方向
に設けられた、腹面側切断線9および背面側切断線10
に沿って切断された、作動流体8の流れ方向の翼端壁2
の断面形状は、図2に示すように、翼腹面4近傍におけ
る切断線9部分の断面形状は、流れの中央部ほど、翼端
壁2が内方(上方)に向けて突出量を大きくした凸面形
状11にされ、翼背面5近傍における切断線10部分の
断面形状は、流れの中央部ほど、翼端壁2が外方に向け
て突出量を大きくした凹面形状12にされている。In the drawing, reference numeral 9 denotes a ventral cut line provided in the flow direction of the working fluid F flowing near the wing apex surface 4 on the wing tip wall 2, and 10 similarly flows near the wing back surface on the wing tip wall 2. It is a back side cutting line provided in the flow direction of the working fluid. Ventral-side cutting line 9 and back-side cutting line 10 provided in the flow direction near the wing abdominal surface 4 and near the wing back surface 5
End wall 2 cut in the direction of flow of working fluid 8
As shown in FIG. 2, the cross-sectional shape of the cutting line 9 in the vicinity of the blade abdominal surface 4 is such that the blade end wall 2 has a larger amount of inward (upward) projection toward the center of the flow. The cross-sectional shape of the portion along the cutting line 10 near the blade back surface 5 is a concave shape 12 in which the blade end wall 2 has a larger outward projection toward the center of the flow.
【0017】また、流れ方向の断面形状が凸面形状11
にされた翼腹面4近傍の翼端壁2と、流れ方向の断面形
状が凸面形状12にされた翼背面5近傍の翼端壁2と
は、周方向には滑らかな曲線、もしくは直線で接続され
て、タービン翼1が立設された翼端壁2の周方向には、
等ピッチの凹凸面が形成された横断面形状の翼端壁2に
され、隣接するタービン翼1とで、タービン翼1の前縁
側から後縁側方向に作動流体Fを流す翼間流路8を形成
するようにしている。The sectional shape in the flow direction is a convex shape 11
The wing tip wall 2 in the vicinity of the wing abdominal surface 4 and the wing tip wall 2 in the vicinity of the wing back surface 5 having a convex sectional shape 12 in the flow direction are connected by a smooth curve or straight line in the circumferential direction. Then, in the circumferential direction of the blade end wall 2 on which the turbine blade 1 is erected,
A blade end wall 2 having a transverse cross-sectional shape having a uniform pitch uneven surface is formed, and an inter-blade flow path 8 for flowing a working fluid F from the leading edge side to the trailing edge side of the turbine blade 1 with the adjacent turbine blade 1. It is formed.
【0018】また、翼腹面4近傍の流れの方向に設けら
れる凸面形状11の上流および下流端側は、凹凸面を設
けずにタービン翼を立設するようにした、通常の翼端壁
2面2より外方に向けて突出させて配置されるととも
に、翼背面5近傍の流れの方向に設けられる凹面形状1
2の上流および下流端側は、通常の翼端壁2面より内方
に向けて突出させて配置されるようにしている。The upstream and downstream ends of the convex shape 11 provided in the flow direction near the blade abdominal surface 4 are provided with two normal blade tip walls on which turbine blades are erected without providing any uneven surface. 2 and a concave shape 1 provided in the flow direction near the blade back surface 5.
The upstream and downstream ends of the blade 2 are arranged so as to protrude inward from the normal surface of the wing tip wall 2.
【0019】本実施の形態の軸流タービン翼列において
は、このように、翼端壁2が翼腹面4近傍では凸面形状
11、翼背面5近傍では凹面形状12をなすように、流
れ方向断面形状を翼列ピッチに合わせて、変化させるこ
とにより、2次流れ渦7による作動流体Fのエネルギー
損失を低減して、タービン効率を向上させることができ
る。In the axial flow turbine cascade according to the present embodiment, the blade tip wall 2 has a convex shape 11 near the blade abdominal surface 4 and a concave shape 12 near the blade back surface 5. By changing the shape in accordance with the cascade pitch, energy loss of the working fluid F due to the secondary flow vortex 7 can be reduced, and turbine efficiency can be improved.
【0020】すなわち、翼腹面4近傍では、翼端壁2は
作動流体Fの流れ方向に凸面形状11にされていること
から、これに沿って流れる作動流体Fの流速は上昇し、
流速の2乗に比例して変化する静圧は低下する。このた
め、タービン翼1の翼端部の翼腹面4側では、翼高さ中
央部分の翼腹面4側に比べて静圧が低下する。That is, in the vicinity of the wing apex surface 4, the wing tip wall 2 has a convex shape 11 in the flow direction of the working fluid F, so that the flow velocity of the working fluid F flowing along the wing tip wall 2 increases,
The static pressure, which varies in proportion to the square of the flow rate, decreases. For this reason, the static pressure is lower at the blade tip surface 4 at the blade tip of the turbine blade 1 than at the blade tip surface 4 at the center of the blade height.
【0021】一方、翼背面5近傍では、翼端壁2は作動
流体Fの流れ方向に凹面形状12となっていることか
ら、これに沿って流れる流体の流速は低下し、これに伴
い静圧は上昇する。このため、翼端部の翼背面5側で
は、翼高さ中央部分の翼背面5側に比べて静圧が上昇す
る。On the other hand, in the vicinity of the blade back surface 5, the blade end wall 2 has a concave shape 12 in the flow direction of the working fluid F, so that the flow velocity of the fluid flowing therethrough decreases, and the static pressure is accordingly reduced. Rises. For this reason, the static pressure is higher at the blade back 5 at the blade tip than at the blade back 5 at the center of the blade height.
【0022】その結果、タービン翼1の翼端部では翼腹
面4と翼背面5との圧力差が、翼高さ中央部分の翼腹面
4と翼背面5との圧力差に比べて小さくなり、翼腹面4
側から翼背面5に向けて流れる2次流れ6の強さが弱く
なり、特に、タービン翼1の前縁部の翼端壁2の近傍で
発生し、翼端壁2近傍の2次流れ6によって発達する2
次流れ渦7の発達が抑制され、さらには、翼間流路8を
流れている間に発達する2次流れ渦7の発達が遅らさ
れ、翼間流路8を流れているときに作動流体Fに含まれ
る圧損流体が低減するとともに、粘性散逸作用も小さく
なり、翼間流路8内を流れる作動流体Fの2次流れ渦に
よるエネルギー損失を小さくして、タービン翼列の性能
を向上させることができ、タービン効率の良い軸流ター
ビン翼列とすることができる。As a result, at the blade tip of the turbine blade 1, the pressure difference between the blade abdominal surface 4 and the blade back surface 5 becomes smaller than the pressure difference between the blade abdominal surface 4 and the blade back surface 5 at the center of the blade height. Wing vent surface 4
The strength of the secondary flow 6 flowing from the side toward the blade back surface 5 is weakened, and particularly the secondary flow 6 generated near the blade tip wall 2 at the leading edge of the turbine blade 1 and near the blade tip wall 2. Developed by 2
The development of the secondary flow vortex 7 is suppressed, and the development of the secondary flow vortex 7 that develops while flowing in the inter-blade flow path 8 is delayed. The pressure loss fluid contained in the fluid F is reduced, and the viscous dissipation action is also reduced. The energy loss due to the secondary flow vortex of the working fluid F flowing in the interblade flow path 8 is reduced, thereby improving the performance of the turbine cascade. And an axial turbine cascade with high turbine efficiency can be obtained.
【0023】[0023]
【発明の効果】以上説明したように、本発明の軸流ター
ビン翼列によれば、周方向に翼列を形成するように、翼
端壁に立設されたタービン翼の翼腹面近傍の流れ方向の
断面形状が、流れ方向の中央部ほど翼端壁を内方に向け
て突出量を大きくした凸面形状にされ、タービン翼の翼
背面近傍の流れ方向の断面形状が、流れ方向の中央部ほ
ど翼端壁を外方に向けて突出量を大きくした凹面形状に
され、翼腹面近傍の翼端壁と翼背面近傍の翼端壁とが、
周方向には滑らかに接続されて、翼端壁の周方向に等ピ
ッチの凹凸面をするようにした横断面形状が、流れ方向
に形成された翼間流路を隣接するタービン翼とともに形
成するものとした。As described above, according to the axial turbine cascade of the present invention, the flow near the blade abdominal surface of the turbine blade erected on the blade end wall so as to form the blade cascade in the circumferential direction. The cross-sectional shape in the direction is a convex shape with the blade tip wall inwardly projecting inward toward the center in the flow direction and the amount of protrusion is increased.The cross-sectional shape in the flow direction near the back of the blade of the turbine blade is the center in the flow direction. The wing tip wall has a concave shape with the projection amount increased toward the outside, and the wing tip wall near the wing abdominal surface and the wing tip wall near the wing back face,
The cross-sectional shape, which is smoothly connected in the circumferential direction and has an uneven pitch at the same pitch in the circumferential direction of the blade tip wall, forms an inter-blade flow path formed in the flow direction together with the adjacent turbine blade. It was taken.
【0024】本発明の軸流タービン翼列は、これによ
り、タービン翼が立設される翼端壁が凸面形状にされた
翼腹面近傍で、しかも翼端壁に近い部分の翼間流路を流
れる作動流体ほど、凸面形状によって加速され、これに
伴い、この部分の静圧が低下するとともに、凹面形状に
された翼背面近傍で、しかも翼端壁に近い部分の翼間流
路を流れる作動流体ほど、凹面形状により減速され、こ
れに伴い、この部分の静圧が上昇する。In the axial flow turbine cascade according to the present invention, the inter-blade flow path in the vicinity of the blade tip surface where the blade tip wall on which the turbine blade is erected is formed in a convex shape and near the blade tip wall is thereby formed. The flowing working fluid is accelerated by the convex shape, and the static pressure in this portion decreases accordingly, and the working fluid flows through the inter-blade flow passage near the concave back surface of the blade and near the blade tip wall. The more the fluid, the more the speed is reduced by the concave shape, and the static pressure in this portion increases accordingly.
【0025】従って、翼腹面と翼背面とにそれぞれ作用
する作動流体Fによって生じる圧力差、すなわち、翼背
面近傍の静圧により翼腹面近傍の静圧が高くなる圧力
差、しかも2次流れ渦が発生し、発達していく翼端壁近
傍における圧力差ほど緩和され、翼腹面側から翼背面側
へ向けて流れる2次流れの強さは弱められる。Therefore, the pressure difference generated by the working fluid F acting on the blade apex surface and the blade back surface, that is, the pressure difference in which the static pressure near the blade aft surface is increased by the static pressure near the blade back surface, and the secondary flow vortex The pressure difference in the vicinity of the generated and developed blade tip wall is alleviated, and the intensity of the secondary flow flowing from the blade abdominal surface toward the blade back surface is reduced.
【0026】このため、タービン翼の前縁部の翼端壁近
傍で発生し、翼間流路内を翼腹面側から翼背面側へ流さ
れながら発達していく2次流れ渦は、この翼端壁近傍の
2次流れの強さが弱められることにより発達が抑制さ
れ、さらには発達が遅らされ、翼間流路を流れていると
きに作動流体に含まれる圧損流体が低減するとともに、
粘性散逸作用も小さくなり、翼間流路内を流れる作動流
体の2次流れ渦によるエネルギー損失も小さくなり、タ
ービン翼列の性能を向上させることができ、タービン効
率の良い軸流タービン翼列とすることができる。Therefore, the secondary flow vortex generated near the blade tip wall at the leading edge of the turbine blade and developing while flowing from the blade abdomen side to the blade back side in the blade-to-blade flow path is generated by the blade. The development is suppressed by the strength of the secondary flow near the end wall being weakened, the development is further delayed, and the pressure drop fluid contained in the working fluid when flowing in the inter-blade flow path is reduced,
The viscous dissipation effect is also reduced, the energy loss due to the secondary flow vortex of the working fluid flowing in the inter-blade flow path is also reduced, and the performance of the turbine cascade can be improved. can do.
【図1】本発明の軸流タービン翼列の実施の第1形態と
しての軸流タービン翼列の一部分を示す模式図、FIG. 1 is a schematic view showing a part of an axial flow turbine cascade as a first embodiment of an axial flow turbine cascade according to the present invention;
【図2】図1に示す軸流タービン翼列の流れ方向翼端壁
の断面形状の概念図、2 is a conceptual diagram of a cross-sectional shape of a flow direction blade end wall of the axial flow turbine cascade shown in FIG.
【図3】従来の軸流タービン翼列内部の流れの様子を示
す模式図である。FIG. 3 is a schematic diagram showing a state of a flow inside a conventional axial flow turbine cascade.
1 タービン翼 2 翼端壁 3 馬蹄渦 4 翼腹面 5 翼背面 6 2次流れ 7 2次流れ渦 8 翼間流路 9 腹面側切断線 10 背面側切断線 11 凸面形状 12 凹面形状 F 作動流体 DESCRIPTION OF SYMBOLS 1 Turbine blade 2 Blade end wall 3 Horseshoe vortex 4 Blade surface 5 Blade back surface 6 Secondary flow 7 Secondary flow vortex 8 Blade flow path 9 Ventral cut line 10 Back cut line 11 Convex shape 12 Concave shape F Working fluid
Claims (1)
にタービン翼を立設して設けられた軸流タービン翼列に
おいて、前記タービン翼の翼腹面近傍の前記翼端壁の流
れ方向の断面形状が流れ方向の中央部ほど内方に向けて
突出する凸面形状にされ、前記タービン翼の翼背面近傍
の前記翼端壁の流れ方向の断面形状が流れ方向の中央部
ほど外方に向けて突出する凹面形状にされるとともに、
前記凸面形状と前記凹面形状とが周方向に滑らかに接続
されて、前記翼端壁上に等ピッチの凹凸面を周方向に形
成した断面形状の翼間流路を設けたことを特徴とする軸
流タービン翼列。1. An axial flow turbine cascade provided with turbine blades erected on a blade tip wall so as to form a blade cascade in a circumferential direction, wherein the blade tip wall near a blade abdominal surface of the turbine blade is provided. The cross-sectional shape in the flow direction has a convex shape protruding inward toward the center in the flow direction, and the cross-sectional shape in the flow direction of the blade end wall near the blade back surface of the turbine blade is more outward toward the center in the flow direction. The concave shape that protrudes toward
The convex shape and the concave shape are smoothly connected to each other in the circumferential direction, and an inter-blade flow path having a cross-sectional shape in which uneven surfaces having equal pitches are formed in the circumferential direction on the blade tip wall is provided. Axial turbine cascade.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP35756597A JPH11190203A (en) | 1997-12-25 | 1997-12-25 | Axial flow turbine blade cascade |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP35756597A JPH11190203A (en) | 1997-12-25 | 1997-12-25 | Axial flow turbine blade cascade |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH11190203A true JPH11190203A (en) | 1999-07-13 |
Family
ID=18454780
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP35756597A Pending JPH11190203A (en) | 1997-12-25 | 1997-12-25 | Axial flow turbine blade cascade |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH11190203A (en) |
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US7164854B2 (en) | 2002-08-27 | 2007-01-16 | Pentax Corporation | Cam mechanism of a photographing lens |
| US7289725B2 (en) | 2002-08-27 | 2007-10-30 | Pentax Corporation | Retractable lens barrel |
| KR101258049B1 (en) * | 2008-01-21 | 2013-04-24 | 미츠비시 쥬고교 가부시키가이샤 | Turbine blade-cascade end wall |
-
1997
- 1997-12-25 JP JP35756597A patent/JPH11190203A/en active Pending
Cited By (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US7164854B2 (en) | 2002-08-27 | 2007-01-16 | Pentax Corporation | Cam mechanism of a photographing lens |
| US7289725B2 (en) | 2002-08-27 | 2007-10-30 | Pentax Corporation | Retractable lens barrel |
| KR101258049B1 (en) * | 2008-01-21 | 2013-04-24 | 미츠비시 쥬고교 가부시키가이샤 | Turbine blade-cascade end wall |
| KR101257984B1 (en) * | 2008-01-21 | 2013-04-24 | 미츠비시 쥬고교 가부시키가이샤 | Turbine blade-cascade end wall |
| US8469659B2 (en) | 2008-01-21 | 2013-06-25 | Mitsubishi Heavy Industries, Ltd. | Turbine blade cascade endwall |
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