EP2412941A1 - Exhaust diffuser for a gas turbine, and method thereof - Google Patents
Exhaust diffuser for a gas turbine, and method thereof Download PDFInfo
- Publication number
- EP2412941A1 EP2412941A1 EP10007757A EP10007757A EP2412941A1 EP 2412941 A1 EP2412941 A1 EP 2412941A1 EP 10007757 A EP10007757 A EP 10007757A EP 10007757 A EP10007757 A EP 10007757A EP 2412941 A1 EP2412941 A1 EP 2412941A1
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- EP
- European Patent Office
- Prior art keywords
- diffuser
- gas
- flow
- diffuser wall
- wall
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- 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.)
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Classifications
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F01—MACHINES OR ENGINES IN GENERAL; ENGINE PLANTS IN GENERAL; STEAM ENGINES
- F01D—NON-POSITIVE DISPLACEMENT MACHINES OR ENGINES, e.g. STEAM TURBINES
- F01D25/00—Component parts, details, or accessories, not provided for in, or of interest apart from, other groups
- F01D25/30—Exhaust heads, chambers, or the like
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F05—INDEXING SCHEMES RELATING TO ENGINES OR PUMPS IN VARIOUS SUBCLASSES OF CLASSES F01-F04
- F05D—INDEXING SCHEME FOR ASPECTS RELATING TO NON-POSITIVE-DISPLACEMENT MACHINES OR ENGINES, GAS-TURBINES OR JET-PROPULSION PLANTS
- F05D2220/00—Application
- F05D2220/30—Application in turbines
- F05D2220/32—Application in turbines in gas turbines
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F05—INDEXING SCHEMES RELATING TO ENGINES OR PUMPS IN VARIOUS SUBCLASSES OF CLASSES F01-F04
- F05D—INDEXING SCHEME FOR ASPECTS RELATING TO NON-POSITIVE-DISPLACEMENT MACHINES OR ENGINES, GAS-TURBINES OR JET-PROPULSION PLANTS
- F05D2250/00—Geometry
- F05D2250/20—Three-dimensional
- F05D2250/23—Three-dimensional prismatic
- F05D2250/232—Three-dimensional prismatic conical
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F05—INDEXING SCHEMES RELATING TO ENGINES OR PUMPS IN VARIOUS SUBCLASSES OF CLASSES F01-F04
- F05D—INDEXING SCHEME FOR ASPECTS RELATING TO NON-POSITIVE-DISPLACEMENT MACHINES OR ENGINES, GAS-TURBINES OR JET-PROPULSION PLANTS
- F05D2270/00—Control
- F05D2270/01—Purpose of the control system
- F05D2270/17—Purpose of the control system to control boundary layer
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F05—INDEXING SCHEMES RELATING TO ENGINES OR PUMPS IN VARIOUS SUBCLASSES OF CLASSES F01-F04
- F05D—INDEXING SCHEME FOR ASPECTS RELATING TO NON-POSITIVE-DISPLACEMENT MACHINES OR ENGINES, GAS-TURBINES OR JET-PROPULSION PLANTS
- F05D2270/00—Control
- F05D2270/30—Control parameters, e.g. input parameters
- F05D2270/301—Pressure
Definitions
- the present invention relates to exhaust diffusers for gas turbines, particularly for gas turbines in stationary or land based applications.
- exhaust diffusers serve to reduce the speed of the exhaust flow in a gas turbine and to thus recover pressure from the exhaust gas coming from the last stage of the turbine.
- the reduction in gas speed reduces the stress associated with the fluid flow on the exhaust equipment and enhances the performance levels of the turbine by recovering pressure from the exhaust gas, thus limiting head loss of the flow.
- the pressure recovery from the exhaust gas is directly proportional to the outlet to inlet area ratio of the diffuser, which controls amount of effective flow diffusion following the last turbine stage.
- a high outlet to inlet area ratio for a given axial length of the diffuser i.e., large diffuser angle
- causes rapid expansion of the gas leading to a separation of flow of the gas from the diffuser wall which, in turn, causes a reduction in the pressure recovery by the diffuser.
- Past attempts to solve the issue of flow separation from the diffuser wall involve the use of boundary layer control, for example, by suction or blowing, turbulators, among others.
- exhaust diffusers are designed to have area ratios that provide a maximum pressure recovery at full load, taking into account the flow separation at full load. In such a case, the pressure recovery, and hence the work extracted by the turbine, is substantially reduced when the gas turbine operates at part-load.
- the object of the present invention is to provide an exhaust diffuser assembly for a stationary gas turbine, and a method thereof, for achieving higher pressure recovery at different operating loads by reducing or eliminating excessive flow separation.
- the underlying idea of the present invention is to provide a mechanism of controlling pressure recovery in an exhaust diffuser by controlling the geometry of the diffuser.
- the proposed exhaust diffuser assembly has a variable geometry diffuser wall, which allows the divergence angle of the diffuser wall with respect to the longitudinal diffuser axis to be adjusted, so as to cause a resultant flow field of the gas that is attached to the diffuser wall.
- the variability of diffuser wall geometry allows adaptability of the proposed diffuser assembly for adjustments in mass flows, i.e., operating loads.
- said diffuser geometry control means comprises one or more actuators disposed on a surface said diffuser wall, said one or more actuators being adapted to exert an adjustable pressure said diffuser wall to resultantly adjust said divergence angle ' ⁇ ' of said diffuser wall.
- said one or more actuators are controllable for increasing said divergence angle ' ⁇ ' to cause a resultant flow field beyond a point of flow separation of said gas from said diffuser wall and subsequently reducing said divergence angle ' ⁇ ' to re-attach the flow of said gas to said diffuser wall, so as to cause a resultant flow of said gas through said diffuser wall that is substantially proximate and prior to said point of flow separation. Since pressure recovery increases with increase in the rate of expansion (i.e., divergence angle) for attached flow, maintaining the flow field just before separation point for any given mass-flow rate would maximize the pressure recovery at that mass -flow rate
- the proposed diffuser assembly further comprises a pressure probe disposed in a flow path of said gas through flowing said diffuser wall, wherein said point of flow separation is detected based on a decrease in sensed pressure between two progressively increasing settings of the divergence angle ' ⁇ '.
- the proposed diffuser assembly further comprises a sonic probe disposed in a flow path of said gas inside said diffuser wall to detect said point of flow separation.
- said point of flow separation is determined by flow visualization means adapted for detecting local direction of flow.
- said diffuser wall is made of a piece of sheet metal wound to spiral form. Such a diffuser wall provides increased elasticity for adjustment of divergence angle.
- said diffuser wall is made from a piece of sheet metal wound into a conical shape, wherein the edges of said piece of sheet metal are slidable against each other.
- said diffuser wall comprises an adjustable portion having a rectangular cross-section, wherein the diffuser wall at said adjustable portion is flexible attached to a fixed portion by a hinge.
- said diffuser wall has a rectangular cross-sectional geometry formed by angular plates forming corners of the rectangle, said angular plates being interspaced by and flat plates over which said angular plates are slidable such that said rectangular cross-sectional shape is adjustable along diagonal directions.
- This allows the rectangular geometry of the diffuser wall to be uniformly varied (maintaining the same aspect ratio) along the direction of the diagonals of the rectangle by placing actuators at the corner of the rectangle.
- an exhaust diffuser assembly 1 (also referred to as "diffuser 1") for a stationary gas turbine, for example, used in power generation and mechanical drives in land based applications.
- the diffuser 1 has an inlet 3 having a first cross-sectional area A 1 for receiving a mainflow gas from a last stage of a turbine section 60.
- the gas 5 flows along a longitudinal axis 2 through a conduit defined by a diverging diffuser wall 7 extending from the diffuser inlet 3 to a diffuser outlet 4 having a second cross-sectional area A 2 .
- the diffuser outlet 4 directs the gas 5 to an exhaust duct 80.
- the diffuser wall 7 serves to recover pressure from the gas by expanding the gas between the inlet 3 and the outlet 4. This reduces the total head loss of the gas, thereby increasing the work extracted from the gas 5.
- the diffuser wall 7 makes an angle of divergence ' ⁇ ' with respect to the longitudinal axis 2. In conventional diffusers, the divergence angle is normally fixed at about 5-6°.
- the area ratio 'R' increases with increase in divergence angle ' ⁇ '.
- the pressure recovery increases with increase in divergence angle ' ⁇ ' or area ratio R, till the flow of the gas 5 is separated from the diffuser wall 7. Separation of flow reduces the pressure recovery from the gas 5.
- the divergence angle ' ⁇ ' is adjusted to cause a resultant flow of the gas 5 that is attached to the diffuser wall 7.
- the diffuser wall 7 has an adjustable geometry wherein the angle ' ⁇ ' may be varied. Exemplary embodiments of an adjustable geometry diffuser wall are discussed below referring to FIGS 3-7 .
- variable seals 12 are provided at the connection of the diffuser wall 7 to the exhaust duct 80.
- one or more actuators 9 are disposed on a surface (inner or outer) of the diffuser wall 7.
- the actuators 9 are disposed on the outer surface of the diffuser wall 7.
- the actuators 9 may comprise, for example, hydraulically or pneumatically operated actuators that are controlled by a controller 10 to exert an adjustable pressure on the diffuser wall 7 to resultantly adjust the divergence angle ' ⁇ ' of the diffuser wall 7.
- the pressure recovery increases with increase in divergence angle ' ⁇ ' or area ratio 'R'.
- the pressure recovery is maximized by maintaining a flow field of the gas 5 within the diffuser wall 7 that is just before the point of flow separation.
- the actuators 9 are controlled to first increase the divergence angle ' ⁇ ' or area ratio 'R' to cause a resultant flow field beyond a point of flow separation. Subsequently, the actuators 9 are controlled to reduce the divergence angle ' ⁇ ' or area ratio 'R' to re-attach the flow to the diffuser wall 7 and to cause a resultant flow field that is prior to and proximate to the point of flow separation.
- the point of flow separation is detected by a flow sensor 11 disposed in the flow path of the gas 5 inside the diffuser wall 7.
- the flow sensor 7 may include, for example, a pressure probe.
- the sensed pressure values by the pressure probe 11 increases. This is illustrated by a curve 13 in FIG 2 , wherein the axis 14 represents angle of divergence ' ⁇ ' and the axis 15 represents the corresponding sensed pressure 'P' by the pressure probe 11 disposed in the flow path of the gas 5.
- the proposed technique in this embodiment involves increasing ' ⁇ ' to cause a flow field beyond the point 16 of flow separation, to identify the threshold angle ⁇ S , and to then reduce ' ⁇ ' to a value ⁇ D less than ⁇ S so as to re-attach the flow to the diffuser wall and to cause the resultant flow field to reach a point 17 that is just before the point 16 of flow separation.
- a portion of the curve 13 in the region of the separation point 16 is flat having a slope equal or nearly equal to zero.
- the flow field corresponding to this portion is preferably avoided as this indicates is an unstable flow field where separated and attached flow alternate.
- the desired point 17 that is "substantially proximate and prior to" the point 16 of flow separation is determined, in this case, as the closest point to the point 16 on the curve 13 that has a positive slope.
- the flow sensor 11 to detect the point of flow separation may comprise a sonic probe. Still alternately, the point of flow separation may be detected using flow visualization or imaging techniques which detect the local direction of flow.
- the adjustable geometry which enables the forcing of the flow beyond the point of flow separation point allows the identification of the point of flow separation. Once the point of flow separation is identified, the geometry of the diffuser may be adjusted to re-attach the flow to the diffuser wall.
- the adjustable geometry proposed herein allows for adaptability of the technique discussed above to changes in mass-flow, such that the pressure recovery may be maximized even when the gas turbine is operating at part load.
- the diffuser wall 7 is made of a sheet 18 of metal wound in several turns in a spiral form to form conical shape.
- the spiral form provides the required elasticity for geometric adjustments.
- Actuators 9 may be disposed on the outer surface of one or more of these turns to, which, when actuated, apply the required pressure to increase or decrease the divergence angle of the diffuser wall 7.
- the diffuser wall 7 may be made from a sheet 20 of metal wound in a conical shape, such that the ends 21 and 22 are not welded to each other, but slide against each other on the application of pressure by one or more actuators 9 disposed on the outer surface of the diffuser wall 7, such that divergence angle or area ratio may be varied.
- the diffuser wall 7 is made of sheet metal and includes an adjustable portion 23 having a rectangular cross-section and a fixed portion 24, which may have a circular cross-section at the inlet 3.
- the rectangular portion 23 is made of flat plates 25, 26, 27, 28, one or more of which are flexibly connected to the fixed portion 24 by means of hinges 29, that allow the respective side 25, 26, 27, 28 to swivel with respect to the fixed portion 24 on application of pressure from the actuator 9 disposed thereon, to thus adjust the divergence angle/area ratio.
- the plates 25 and 27 are hinged such that the direction of angular movement is as illustrated by the arrows 30.
- the diffuser wall 7 has a rectangular cross-section formed by flat plates 31, 32, 33, 34 that are directly connected to a circular turbine manifold 35 by flexible joints 36 so as to allow angular movements of opposite plates 31 and 33 as depicted by the arrow 37.
- the diffuser wall 7 is made of angular plates 38, 39, 40, 41 that define the corners of a rectangle (herein, square).
- the angular plates 38, 39, 40, 41 are interspaced by flat plates 42, 43, 44, 45, which, together with the angular plates 38, 39, 40, 41 form the sides of the rectangular diffuser wall 7. As illustrated, the angular plates are slidable against the flat plates 42, 43, 44, 45 such that the rectangular cross-sectional geometry of the diffuser wall 7 may be adjusted along diagonal directions 46 and 47 by actuators (not shown) disposed on the corners 48, 49, 50, 51 of the rectangular diffuser wall 7.
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- Engineering & Computer Science (AREA)
- Mechanical Engineering (AREA)
- General Engineering & Computer Science (AREA)
- Control Of Turbines (AREA)
- Structures Of Non-Positive Displacement Pumps (AREA)
- Supercharger (AREA)
Abstract
The present invention relates to an exhaust diffuser assembly (1), particularly for a stationary gas turbine, and a method incorporating the same. The proposed exhaust diffuser assembly (1) comprises a longitudinal axis (2), a diffuser inlet (3) for receiving a turbine mainflow gas (5), a diffuser outlet (4), and a diverging diffuser wall (7) having an adjustable geometry and forming a conduit for flow of said gas (5) therethrough from said diffuser inlet (3) to said diffuser outlet (4). The diffuser wall (7) has a divergence angle 'α' with respect to said longitudinal axis (2). The proposed diffuser assembly (1) further comprises diffuser geometry control means (9,10) for controlling a recovery of pressure from said gas (5) between said diffuser inlet (3) and said diffuser outlet (4) by adjusting said divergence angle 'α' of said diffuser wall (7) to cause a resultant flow field of said gas (5) that is attached to said diffuser wall (7).
Description
- The present invention relates to exhaust diffusers for gas turbines, particularly for gas turbines in stationary or land based applications.
- In gas turbines, for example those used in power generation, exhaust diffusers serve to reduce the speed of the exhaust flow in a gas turbine and to thus recover pressure from the exhaust gas coming from the last stage of the turbine. The reduction in gas speed reduces the stress associated with the fluid flow on the exhaust equipment and enhances the performance levels of the turbine by recovering pressure from the exhaust gas, thus limiting head loss of the flow.
- In an exhaust diffuser, the pressure recovery from the exhaust gas is directly proportional to the outlet to inlet area ratio of the diffuser, which controls amount of effective flow diffusion following the last turbine stage. However, a high outlet to inlet area ratio for a given axial length of the diffuser (i.e., large diffuser angle) causes rapid expansion of the gas leading to a separation of flow of the gas from the diffuser wall, which, in turn, causes a reduction in the pressure recovery by the diffuser. Past attempts to solve the issue of flow separation from the diffuser wall involve the use of boundary layer control, for example, by suction or blowing, turbulators, among others.
- In practice, exhaust diffusers are designed to have area ratios that provide a maximum pressure recovery at full load, taking into account the flow separation at full load. In such a case, the pressure recovery, and hence the work extracted by the turbine, is substantially reduced when the gas turbine operates at part-load.
- The object of the present invention is to provide an exhaust diffuser assembly for a stationary gas turbine, and a method thereof, for achieving higher pressure recovery at different operating loads by reducing or eliminating excessive flow separation.
- The above object is achieved by the exhaust diffuser assembly according to claim 1 and the method according to
claim 11. - The underlying idea of the present invention is to provide a mechanism of controlling pressure recovery in an exhaust diffuser by controlling the geometry of the diffuser. To that end, the proposed exhaust diffuser assembly has a variable geometry diffuser wall, which allows the divergence angle of the diffuser wall with respect to the longitudinal diffuser axis to be adjusted, so as to cause a resultant flow field of the gas that is attached to the diffuser wall. The variability of diffuser wall geometry allows adaptability of the proposed diffuser assembly for adjustments in mass flows, i.e., operating loads.
- In one embodiment, said diffuser geometry control means comprises one or more actuators disposed on a surface said diffuser wall, said one or more actuators being adapted to exert an adjustable pressure said diffuser wall to resultantly adjust said divergence angle 'α' of said diffuser wall.
- In a preferred embodiment, wherein said one or more actuators are controllable for increasing said divergence angle 'α' to cause a resultant flow field beyond a point of flow separation of said gas from said diffuser wall and subsequently reducing said divergence angle 'α' to re-attach the flow of said gas to said diffuser wall, so as to cause a resultant flow of said gas through said diffuser wall that is substantially proximate and prior to said point of flow separation. Since pressure recovery increases with increase in the rate of expansion (i.e., divergence angle) for attached flow, maintaining the flow field just before separation point for any given mass-flow rate would maximize the pressure recovery at that mass -flow rate
- In one embodiment, the proposed diffuser assembly further comprises a pressure probe disposed in a flow path of said gas through flowing said diffuser wall, wherein said point of flow separation is detected based on a decrease in sensed pressure between two progressively increasing settings of the divergence angle 'α'. The above embodiment provides a simple means to detect flow separation, since pressure in the gas flow path decreases sharply after flow separation occurs
- In an alternate embodiment, the proposed diffuser assembly further comprises a sonic probe disposed in a flow path of said gas inside said diffuser wall to detect said point of flow separation.
- In a still further embodiment, said point of flow separation is determined by flow visualization means adapted for detecting local direction of flow.
- In an exemplary embodiment, said diffuser wall is made of a piece of sheet metal wound to spiral form. Such a diffuser wall provides increased elasticity for adjustment of divergence angle.
- In another exemplary embodiment, said diffuser wall is made from a piece of sheet metal wound into a conical shape, wherein the edges of said piece of sheet metal are slidable against each other. The above embodiment provides manufacturing simplicity.
- In yet another exemplary embodiment, said diffuser wall comprises an adjustable portion having a rectangular cross-section, wherein the diffuser wall at said adjustable portion is flexible attached to a fixed portion by a hinge. The above embodiment provides higher accuracy and increased geometric control.
- In still another embodiment, said diffuser wall has a rectangular cross-sectional geometry formed by angular plates forming corners of the rectangle, said angular plates being interspaced by and flat plates over which said angular plates are slidable such that said rectangular cross-sectional shape is adjustable along diagonal directions. This allows the rectangular geometry of the diffuser wall to be uniformly varied (maintaining the same aspect ratio) along the direction of the diagonals of the rectangle by placing actuators at the corner of the rectangle.
- The present invention is further described hereinafter with reference to illustrated embodiments shown in the accompanying drawings, in which:
-
FIG 1 a schematic illustration of an exhaust diffuser assembly for a gas turbine, -
FIG 2 is an exemplary graphical representation showing variation of pressure of the gas with diffuser geometry, also indicating the point of flow separation, -
FIG 3 is a schematic illustration of a first embodiment of an adjustable geometry diffuser wall, -
FIG 4 is a schematic illustration of a second embodiment of an adjustable geometry diffuser wall, -
FIG 5 is a schematic illustration of a third embodiment of an adjustable geometry diffuser wall, -
FIG 6 is a schematic illustration of a fourth embodiment of an adjustable geometry diffuser wall, and -
FIG 7 is a schematic illustration of a fifth embodiment of an adjustable geometry diffuser wall. - Referring now to
FIG 1 is illustrated an exhaust diffuser assembly 1 (also referred to as "diffuser 1") for a stationary gas turbine, for example, used in power generation and mechanical drives in land based applications. The diffuser 1 has aninlet 3 having a first cross-sectional area A1 for receiving a mainflow gas from a last stage of aturbine section 60. Thegas 5 flows along alongitudinal axis 2 through a conduit defined by a divergingdiffuser wall 7 extending from thediffuser inlet 3 to adiffuser outlet 4 having a second cross-sectional area A2. Thediffuser outlet 4 directs thegas 5 to anexhaust duct 80. - The
diffuser wall 7 serves to recover pressure from the gas by expanding the gas between theinlet 3 and theoutlet 4. This reduces the total head loss of the gas, thereby increasing the work extracted from thegas 5. Thediffuser wall 7 makes an angle of divergence 'α' with respect to thelongitudinal axis 2. In conventional diffusers, the divergence angle is normally fixed at about 5-6°. In accordance with the proposed technique, the pressure recovery from thegas 5 is controlled by controlling the geometry of thediffuser wall 7, i.e., by adjusting the divergence angle 'α', and resultantly, the ratio 'R' of the outlet area A2 to the inlet area A1 (where R=A2/A1). It is to be understood that for fixed length diffusers, the area ratio 'R' increases with increase in divergence angle 'α'. In general, the pressure recovery increases with increase in divergence angle 'α' or area ratio R, till the flow of thegas 5 is separated from thediffuser wall 7. Separation of flow reduces the pressure recovery from thegas 5. To achieve higher pressure recovery, the divergence angle 'α' is adjusted to cause a resultant flow of thegas 5 that is attached to thediffuser wall 7. To that end, thediffuser wall 7 has an adjustable geometry wherein the angle 'α' may be varied. Exemplary embodiments of an adjustable geometry diffuser wall are discussed below referring toFIGS 3-7 . Referring back toFIG 1 , to accommodate the resulting variation of cross-sectional area A2 of theoutlet 5,variable seals 12 are provided at the connection of thediffuser wall 7 to theexhaust duct 80. In the illustrated embodiment, one ormore actuators 9 are disposed on a surface (inner or outer) of thediffuser wall 7. In the illustrated embodiment, theactuators 9 are disposed on the outer surface of thediffuser wall 7. Theactuators 9 may comprise, for example, hydraulically or pneumatically operated actuators that are controlled by acontroller 10 to exert an adjustable pressure on thediffuser wall 7 to resultantly adjust the divergence angle 'α' of thediffuser wall 7. - As mentioned above, for attached flow, the pressure recovery increases with increase in divergence angle 'α' or area ratio 'R'. In a preferred embodiment, the pressure recovery is maximized by maintaining a flow field of the
gas 5 within thediffuser wall 7 that is just before the point of flow separation. For this, theactuators 9 are controlled to first increase the divergence angle 'α' or area ratio 'R' to cause a resultant flow field beyond a point of flow separation. Subsequently, theactuators 9 are controlled to reduce the divergence angle 'α' or area ratio 'R' to re-attach the flow to thediffuser wall 7 and to cause a resultant flow field that is prior to and proximate to the point of flow separation. - The point of flow separation is detected by a
flow sensor 11 disposed in the flow path of thegas 5 inside thediffuser wall 7. Theflow sensor 7 may include, for example, a pressure probe. For attached flow, with increase in the divergence angle 'α', the sensed pressure values by thepressure probe 11 increases. This is illustrated by acurve 13 inFIG 2 , wherein theaxis 14 represents angle of divergence 'α' and theaxis 15 represents the corresponding sensed pressure 'P' by thepressure probe 11 disposed in the flow path of thegas 5. As can be seen, with increase in 'α', the sensed pressure increases till apoint 16 is reached where the sensed pressure attains a maximum value, for α= αS. When 'α' is increased beyond this threshold angle αS, the flow begins to separate from the diffuser wall, as a result of which, the sensed pressure decreases, which is detected by a change in slope of thecurve 13 from positive negative. Thepoint 16 of flow separation is thus detected based on a decrease in sensed pressure 'P' between two progressively increasing settings of the divergence angle 'α'. The proposed technique in this embodiment involves increasing 'α' to cause a flow field beyond thepoint 16 of flow separation, to identify the threshold angle αS, and to then reduce 'α' to a value αD less than αS so as to re-attach the flow to the diffuser wall and to cause the resultant flow field to reach apoint 17 that is just before thepoint 16 of flow separation. Typically, a portion of thecurve 13 in the region of theseparation point 16 is flat having a slope equal or nearly equal to zero. The flow field corresponding to this portion is preferably avoided as this indicates is an unstable flow field where separated and attached flow alternate. The desiredpoint 17 that is "substantially proximate and prior to" thepoint 16 of flow separation is determined, in this case, as the closest point to thepoint 16 on thecurve 13 that has a positive slope. - Referring back to
FIG 1 , in an alternate embodiment, theflow sensor 11 to detect the point of flow separation may comprise a sonic probe. Still alternately, the point of flow separation may be detected using flow visualization or imaging techniques which detect the local direction of flow. In all cases, the adjustable geometry which enables the forcing of the flow beyond the point of flow separation point allows the identification of the point of flow separation. Once the point of flow separation is identified, the geometry of the diffuser may be adjusted to re-attach the flow to the diffuser wall. The adjustable geometry proposed herein allows for adaptability of the technique discussed above to changes in mass-flow, such that the pressure recovery may be maximized even when the gas turbine is operating at part load. - Referring to
FIG 3 is illustrated a first embodiment of an adjustablegeometry diffuser wall 7. Herein, thediffuser wall 7 is made of asheet 18 of metal wound in several turns in a spiral form to form conical shape. The spiral form provides the required elasticity for geometric adjustments.Actuators 9 may be disposed on the outer surface of one or more of these turns to, which, when actuated, apply the required pressure to increase or decrease the divergence angle of thediffuser wall 7. In a second embodiment illustrated inFIG 4 , thediffuser wall 7 may be made from asheet 20 of metal wound in a conical shape, such that the ends 21 and 22 are not welded to each other, but slide against each other on the application of pressure by one ormore actuators 9 disposed on the outer surface of thediffuser wall 7, such that divergence angle or area ratio may be varied. - In a third embodiment illustrated in
FIG 5 , thediffuser wall 7 is made of sheet metal and includes anadjustable portion 23 having a rectangular cross-section and a fixedportion 24, which may have a circular cross-section at theinlet 3. Therectangular portion 23 is made offlat plates portion 24 by means of hinges 29, that allow therespective side portion 24 on application of pressure from theactuator 9 disposed thereon, to thus adjust the divergence angle/area ratio. In the shown example, theplates arrows 30. Although thesides sides FIG 6 , thediffuser wall 7 has a rectangular cross-section formed byflat plates circular turbine manifold 35 byflexible joints 36 so as to allow angular movements ofopposite plates arrow 37. In yet another embodiment of a rectangular diffuser wall illustrated inFIG 7 , thediffuser wall 7 is made ofangular plates angular plates flat plates angular plates rectangular diffuser wall 7. As illustrated, the angular plates are slidable against theflat plates diffuser wall 7 may be adjusted alongdiagonal directions corners rectangular diffuser wall 7. - While this invention has been described in detail with reference to certain preferred embodiments, it should be appreciated that the present invention is not limited to those precise embodiments. Rather, in view of the present disclosure which describes the current best mode for practicing the invention, many modifications and variations would present themselves, to those of skill in the art without departing from the scope and spirit of this invention. The scope of the invention is, therefore, indicated by the following claims rather than by the foregoing description. All changes, modifications, and variations coming within the meaning and range of equivalency of the claims are to be considered within their scope.
Claims (15)
- An exhaust diffuser assembly (1) for a stationary gas turbine, comprising:- a longitudinal axis (2),- a diffuser inlet (3) for receiving a turbine mainflow gas (5),- a diffuser outlet (4),- a diverging diffuser wall (7) having an adjustable geometry and forming a conduit for flow of said gas (5) therethrough from said diffuser inlet (3) to said diffuser outlet (4), said diffuser wall (7) having a divergence angle 'α' with respect to said longitudinal axis (2), and- diffuser geometry control means (9,10) for controlling a recovery of pressure from said gas (5) between said diffuser inlet (3) and said diffuser outlet (4) by adjusting said divergence angle 'α' of said diffuser wall (7) to cause a resultant flow field of said gas (5) that is attached to said diffuser wall (7).
- The diffuser assembly (1) according to claim 1, wherein said diffuser geometry control means (9,10) comprises one or more actuators (9) disposed on a surface said diffuser wall (7), said one or more actuators (9) being adapted to exert an adjustable pressure said diffuser wall (7) to resultantly adjust said divergence angle 'α' of said diffuser wall (7).
- The diffuser assembly (1) according to claim 2, wherein said one or more actuators (9) adapted for increasing said divergence angle 'α' to cause a resultant flow field beyond a point of flow separation of said gas (5) from said diffuser wall (7) and subsequently reducing said divergence angle 'α' to re-attach the flow of said gas (5) to said diffuser wall (7), so as to cause a resultant flow of said gas (5) through said diffuser wall (7) that is substantially proximate and prior to said point of flow separation.
- The diffuser assembly (1) according to claim 3, further comprising a pressure probe (11) disposed in a flow path of said gas (5) inside said diffuser wall (7), wherein said point of flow separation is detected based on a decrease in sensed pressure between two progressively increasing settings of the divergence angle 'α'.
- The diffuser assembly (1) according to claim 3, further comprising a sonic probe (11) disposed in a flow path of said gas (5) inside said diffuser wall (7) to detect said point of flow separation.
- The diffuser assembly (1) according to claim 3, wherein said point of flow separation is determined by flow visualization means adapted for detecting local direction of flow.
- The diffuser assembly (1) according to any of the preceding claims, wherein said diffuser wall (7) is made of a piece of sheet metal (11) wound to spiral form.
- The diffuser assembly (1) according to any of the claims 1 to 6, wherein said diffuser wall (7) is made from a piece of sheet metal (20) wound into a conical shape, wherein the edges (21, 22) of said piece of sheet metal are slidable against each other.
- The diffuser assembly (1) according to any of the claims 1 to 6, wherein said diffuser wall (7) comprises an adjustable portion (23) having a rectangular cross-section, wherein the diffuser wall (7) at said adjustable portion (23) is flexibly attached to a fixed portion (24) by a hinge (29).
- The diffuser assembly (1) according to any of the claims 1 to 6, wherein said diffuser wall (7) has a rectangular cross-sectional geometry formed by angular plates (38,39,40,41) forming corners of the rectangle, said angular plates (38,39,40,41) being interspaced by and flat plates (42,43,44,45) over which said angular plates (38,39,40,41) are slidable such that said rectangular cross-sectional shape is adjustable along diagonal directions (46,47).
- A method for operating an exhaust diffuser (1) for a stationary gas turbine, comprising:- receiving a turbine mainflow gas (5) at a diffuser inlet (3),- passing said gas (5) through a diverging diffuser wall (7) having an adjustable geometry defining a conduit for flow said gas (5) between said diffuser inlet (3) and a diffuser outlet (4), said diffuser wall (7) having a divergence angle 'α' with respect to a diffuser longitudinal axis (2), and- controlling a recovery of pressure from said gas (5) between said diffuser inlet (3) and said diffuser outlet (4) by controlling a geometry of said diffuser wall (7), said controlling of said geometry comprising adjusting said divergence angle 'α' of said diffuser wall (7) to cause a resultant flow field of said gas (5) that is attached to said diffuser wall (7).
- The method according to claim 11, wherein controlling the geometry of said diffuser wall (7) comprises disposing one or more actuators (9) on a surface of said diffuser wall (7) and controlling said one or more actuators (9) to exert an adjustable pressure on said diffuser wall (7) to resultantly adjust said divergence angle 'α' of said diffuser wall (7).
- The method according to claim 12, comprising controlling said one or more actuators (9) to increase said divergence angle 'α' to cause a resultant flow field beyond a point of flow separation of said gas (5) from said diffuser wall (7) and subsequently reducing said divergence angle 'α' to re-attach the flow of said gas (5) to said diffuser wall (7), so as to cause a resultant flow of said gas (5) through said diffuser wall that is substantially proximate and prior to said point of flow separation.
- The method according to claim 13, further comprising disposing a pressure probe (11) in a flow path of said gas (5) inside said diffuser wall (7), and detecting said point of flow separation based on a decrease in sensed pressure between two progressively increasing settings of the divergence angle 'α'.
- The method according to claim 13, further comprising detecting said point of flow separation by a sonic probe (11) disposed in a flow path of said gas (5) inside said diffuser wall (7).
Priority Applications (6)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
EP10007757A EP2412941A1 (en) | 2010-07-26 | 2010-07-26 | Exhaust diffuser for a gas turbine, and method thereof |
PCT/EP2011/062246 WO2012013529A1 (en) | 2010-07-26 | 2011-07-18 | Exhaust diffuser for a gas turbine, and method thereof |
JP2013521061A JP5551316B2 (en) | 2010-07-26 | 2011-07-18 | Exhaust diffuser for gas turbine and method |
CN201180036687.9A CN103026009B (en) | 2010-07-26 | 2011-07-18 | For exhaust diffuser and the method thereof of gas turbine |
US13/811,943 US20130121806A1 (en) | 2010-07-26 | 2011-07-18 | Exhaust diffuser for a gas turbine, and method thereof |
EP11740594.4A EP2598725B1 (en) | 2010-07-26 | 2011-07-18 | Exhaust diffuser for a gas turbine, and method thereof |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
EP10007757A EP2412941A1 (en) | 2010-07-26 | 2010-07-26 | Exhaust diffuser for a gas turbine, and method thereof |
Publications (1)
Publication Number | Publication Date |
---|---|
EP2412941A1 true EP2412941A1 (en) | 2012-02-01 |
Family
ID=43242599
Family Applications (2)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP10007757A Withdrawn EP2412941A1 (en) | 2010-07-26 | 2010-07-26 | Exhaust diffuser for a gas turbine, and method thereof |
EP11740594.4A Not-in-force EP2598725B1 (en) | 2010-07-26 | 2011-07-18 | Exhaust diffuser for a gas turbine, and method thereof |
Family Applications After (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP11740594.4A Not-in-force EP2598725B1 (en) | 2010-07-26 | 2011-07-18 | Exhaust diffuser for a gas turbine, and method thereof |
Country Status (5)
Country | Link |
---|---|
US (1) | US20130121806A1 (en) |
EP (2) | EP2412941A1 (en) |
JP (1) | JP5551316B2 (en) |
CN (1) | CN103026009B (en) |
WO (1) | WO2012013529A1 (en) |
Families Citing this family (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
GB2489738B (en) * | 2011-04-08 | 2013-07-03 | Rolls Royce Plc | Improvements in or relating to gas turbine engine transition ducts |
GB2506876A (en) * | 2012-10-10 | 2014-04-16 | Rolls Royce Plc | A gas turbine engine system transition duct |
US10329945B2 (en) * | 2015-04-21 | 2019-06-25 | Siemens Energy, Inc. | High performance robust gas turbine exhaust with variable (adaptive) exhaust diffuser geometry |
CN105937415B (en) * | 2016-06-08 | 2017-06-06 | 西安交通大学 | A kind of supercritical carbon dioxide turbine installation for being suitable for back pressure on a large scale and flow |
WO2022201932A1 (en) * | 2021-03-24 | 2022-09-29 | 三菱パワー株式会社 | Turbine and gas turbine |
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US4398865A (en) * | 1978-11-10 | 1983-08-16 | Garkusha Anatoly V | Exhaust pipe of turbine |
US20080063516A1 (en) * | 2006-09-08 | 2008-03-13 | Siemens Power Generation, Inc. | Adjustable turbine exhaust flow guide and bearing cone assemblies |
US20090068006A1 (en) * | 2007-05-17 | 2009-03-12 | Elliott Company | Tilted Cone Diffuser for Use with an Exhaust System of a Turbine |
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GB607686A (en) * | 1945-02-01 | 1948-09-03 | Power Jets Res & Dev Ltd | Improvements relating to duct inlets for use in supersonic conditions |
US3391869A (en) * | 1966-05-23 | 1968-07-09 | Rohr Corp | Variable cone area convergentdivergent nozzle system |
FR2537657A1 (en) * | 1982-12-08 | 1984-06-15 | Snecma | TUYERE A VARIABLE SECTION FOR A TURBOJET ENGINE AND AIRCRAFT COMPRISING SUCH AN EQUIPMENT |
DE19905994A1 (en) * | 1999-02-15 | 2000-08-24 | Peter Kraus | Procedure to prevent shock boundary layer pulsations with annular diffusers in steam turbines entails providing time-controlled blow-in excitation in rear shell region in dead water zone |
US6261055B1 (en) * | 1999-08-03 | 2001-07-17 | Jerzy A. Owczarek | Exhaust flow diffuser for a steam turbine |
US6636320B1 (en) * | 2000-10-18 | 2003-10-21 | Lockheed Martin Corporation | Fiber optic tufts for flow separation detection |
US6896475B2 (en) * | 2002-11-13 | 2005-05-24 | General Electric Company | Fluidic actuation for improved diffuser performance |
EP1970539A1 (en) * | 2007-03-13 | 2008-09-17 | Siemens Aktiengesellschaft | Diffuser assembly |
JP5309818B2 (en) * | 2008-09-10 | 2013-10-09 | トヨタ自動車株式会社 | Airflow condition monitoring device |
-
2010
- 2010-07-26 EP EP10007757A patent/EP2412941A1/en not_active Withdrawn
-
2011
- 2011-07-18 US US13/811,943 patent/US20130121806A1/en not_active Abandoned
- 2011-07-18 JP JP2013521061A patent/JP5551316B2/en not_active Expired - Fee Related
- 2011-07-18 CN CN201180036687.9A patent/CN103026009B/en not_active Expired - Fee Related
- 2011-07-18 WO PCT/EP2011/062246 patent/WO2012013529A1/en active Application Filing
- 2011-07-18 EP EP11740594.4A patent/EP2598725B1/en not_active Not-in-force
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4398865A (en) * | 1978-11-10 | 1983-08-16 | Garkusha Anatoly V | Exhaust pipe of turbine |
US20080063516A1 (en) * | 2006-09-08 | 2008-03-13 | Siemens Power Generation, Inc. | Adjustable turbine exhaust flow guide and bearing cone assemblies |
US20090068006A1 (en) * | 2007-05-17 | 2009-03-12 | Elliott Company | Tilted Cone Diffuser for Use with an Exhaust System of a Turbine |
Also Published As
Publication number | Publication date |
---|---|
EP2598725B1 (en) | 2015-01-07 |
EP2598725A1 (en) | 2013-06-05 |
US20130121806A1 (en) | 2013-05-16 |
JP2013532793A (en) | 2013-08-19 |
WO2012013529A1 (en) | 2012-02-02 |
CN103026009B (en) | 2015-08-12 |
CN103026009A (en) | 2013-04-03 |
JP5551316B2 (en) | 2014-07-16 |
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