EP1655458A1 - Diffuseur pour une turbine à vapeur - Google Patents
Diffuseur pour une turbine à vapeur Download PDFInfo
- Publication number
- EP1655458A1 EP1655458A1 EP04026196A EP04026196A EP1655458A1 EP 1655458 A1 EP1655458 A1 EP 1655458A1 EP 04026196 A EP04026196 A EP 04026196A EP 04026196 A EP04026196 A EP 04026196A EP 1655458 A1 EP1655458 A1 EP 1655458A1
- Authority
- EP
- European Patent Office
- Prior art keywords
- diffuser
- flow
- coolant
- wall
- medium
- 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.)
- Withdrawn
Links
- 239000002826 coolant Substances 0.000 claims abstract description 27
- 238000011084 recovery Methods 0.000 claims abstract description 11
- 238000001816 cooling Methods 0.000 claims abstract description 10
- 238000005507 spraying Methods 0.000 claims description 16
- 230000000670 limiting effect Effects 0.000 claims description 6
- 238000000034 method Methods 0.000 claims description 6
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 claims description 5
- 238000004519 manufacturing process Methods 0.000 claims description 4
- 230000036961 partial effect Effects 0.000 claims description 3
- 239000012530 fluid Substances 0.000 description 14
- 239000002245 particle Substances 0.000 description 11
- 230000005494 condensation Effects 0.000 description 5
- 238000009833 condensation Methods 0.000 description 5
- 238000006243 chemical reaction Methods 0.000 description 4
- 238000000926 separation method Methods 0.000 description 3
- 239000000498 cooling water Substances 0.000 description 2
- 238000009434 installation Methods 0.000 description 2
- 238000005381 potential energy Methods 0.000 description 2
- 239000007921 spray Substances 0.000 description 2
- 230000003068 static effect Effects 0.000 description 2
- 230000001133 acceleration Effects 0.000 description 1
- 230000003247 decreasing effect Effects 0.000 description 1
- 230000003111 delayed effect Effects 0.000 description 1
- 238000004090 dissolution Methods 0.000 description 1
- 230000005611 electricity Effects 0.000 description 1
- 238000012821 model calculation Methods 0.000 description 1
- 230000002829 reductive effect Effects 0.000 description 1
- 230000002441 reversible effect Effects 0.000 description 1
- 230000009466 transformation Effects 0.000 description 1
Images
Classifications
-
- 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
-
- 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
- F01D25/08—Cooling; Heating; Heat-insulation
- F01D25/12—Cooling
-
- 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
- F05D2240/00—Components
- F05D2240/10—Stators
- F05D2240/14—Casings or housings protecting or supporting assemblies within
-
- 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
- F05D2250/50—Inlet or outlet
- F05D2250/52—Outlet
-
- 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
- F05D2260/00—Function
- F05D2260/20—Heat transfer, e.g. cooling
-
- 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
- F05D2260/00—Function
- F05D2260/20—Heat transfer, e.g. cooling
- F05D2260/201—Heat transfer, e.g. cooling by impingement of a fluid
Definitions
- the invention relates to a diffuser for pressure recovery in the outflow region of a steam turbine, with an inlet and a housing wall for limiting a flow medium.
- the invention also relates to a method for producing a diffuser comprising an inlet and a housing wall for limiting a flow medium.
- a turbomachine is z.
- a diffuser is connected downstream to increase the efficiency of a steam turbine as an embodiment of a turbomachine of a final stage.
- kinetic energy is converted into pressure.
- the static pressure at the blade outlet can be lowered below the condenser pressure. This allows a greater pressure gradient in the final stage and thus a higher power output of the steam turbine. Without a diffuser, the pressure difference would be lower.
- a diffuser is understood as meaning a flow channel through which a flow medium can be flowed, wherein the flow medium has a pressure increase in a flow direction. In this case, a conversion of kinetic energy into potential energy takes place. This energy conversion is desirable in many technical applications. So z. B. the Diffuser of a compressor to convert the high kinetic energy of the flow medium at the impeller outlet as completely as possible and low-loss in static pressure.
- the achievable in a diffuser flow pressure recovery depends on several parameters. It is influenced by the diffuser opening angle as well as the flow conditions and the boundary layer thickness in the diffuser inlet.
- Diffusers are known with a conical surface which widens in the direction of flow ("axial diffuser").
- the opening angle of such a diffuser is usually not more than 15 °, since above this opening angle, the flow separates from the walls of the diffuser, which leads to strong flow losses and causes flow noise. In addition, the unsteady flow due to the separation leads to an increased structural load on the diffuser.
- diffusers with a maximum opening angle of 15 ° are too long, their installation in existing installations is more difficult.
- axial diffusers also axial-radial and radial diffusers are used. In the case of the axial-radial diffuser, the inflow takes place axially and the outflow radially. The radial diffuser is flowed through purely radially. All other considerations include these designs.
- the flow separation on the diffuser wall is caused by the friction of decelerated fluid particles of the flow medium. These braked fluid particles no longer have sufficient kinetic energy to overcome a pressure increase. In extreme cases, fluid particles on the wall can reverse their direction of flow. The diffuser would therefore be ineffective.
- diffusers without measures affecting the boundary layer are executed and essentially by means of empirical Experiences designed. Design parameters here are the opening angle and the cross-sectional profile. In part, baffles are used to favorably influence the flow in the diffuser.
- Diffusers with high pressure recovery require the largest possible ratio of exit area to entrance area.
- a known technical solution to increase the pressure recovery is to open the diffusers strong, but to prevent the flow separation by a Grenz fürabsaugung or -blasblasung. This requires a suction device which leads to a pressure sink on the diffuser wall, wherein the achievable by the suction pressure should be below the wall pressure.
- the object of the invention is to provide a diffuser with which a high pressure recovery is possible.
- a further object of the invention is to provide a method for producing a diffuser, with which it is possible to achieve a high pressure recovery.
- the object directed towards the diffuser is achieved by a diffuser for pressure recovery in the outflow region of a steam turbine, having an inlet and a housing wall for defining a flow medium, the diffuser having coolant for cooling partial regions of the housing wall, wherein the coolant is designed such that the flow medium condenses during operation on the housing wall.
- the invention is based on the fact that the flow medium can be locally condensed in the case of diffusers in the vicinity of the housing wall.
- the strong increase in density resulting from the condensation acts like a boundary layer suction.
- the increase in density can be at a factor of 30,000.
- the invention further assumes that the subregions of the housing wall are cooled to a temperature below the saturation temperature. Thermal energy is withdrawn near slow flow of fluid from the housing wall, causing it to condense on the housing wall.
- the condensed fluid particles can hardly obstruct or block the flow. The condensation of slow fluid particles affects the flow boundary layer of the flow.
- Another advantage of the diffuser according to the invention is that the total volume can be reduced, since the boundary layer influencing by local condensation of the diffuser can be built shorter.
- the invention assumes that even at low condensation rates, which lead to small pressure sinks, a significant increase in the ratio of exit to the inlet surface of the diffuser is possible by increasing the ratio of exit to the entrance surface, a higher pressure recovery is possible.
- the coolant can flow through channels with cold medium on an inside or outside of the housing wall.
- the coolant with a spray device for spraying an inside or outside of the housing wall formed with a cold medium.
- cold water is used as the medium.
- the cold water can z. B. be taken from the cooling water circuit of the entire power plant.
- the second object is achieved by a method for producing a diffuser comprising an inlet and a housing wall for limiting a flow medium, wherein cooling means are attached to the diffuser for cooling partial regions of the housing wall.
- channels through which cold medium can flow are arranged on an inside or outside of the housing wall.
- a spraying device for spraying the inside or outside of the housing wall with a cold medium is arranged.
- water is used as the cold medium.
- a flow medium flows through a flow channel 3 which has a substantially widening flow cross-section and comprises guide vanes 4 and rotor blades 5 via an inlet channel 2, which is not illustrated in more detail.
- the blades 5 are fixedly mounted on a rotor 6.
- the rotor 6 is rotatably supported via a bearing device 7.
- the rotor 6 is set by a relaxation of the flow medium and subsequent energy conversion in a rotation through which a generator, not shown, can be driven to generate electricity.
- a diffuser 9 is arranged.
- the diffuser 9 is used to convert the kinetic energy of the flow medium into pressure energy. This conversion should take place as far as possible with low energy losses.
- FIG. 2 shows a section through a diffuser 9 according to the prior art.
- the diffuser 9 essentially has a hub-side wall 10 and an outer housing wall 11.
- the rotor 6 is rotatably mounted about a rotation axis 12.
- FIG. 2 only one moving blade 5 is shown by way of example.
- a fluid particle flowing out after an output stage 8 flows along a movement path (trajectory).
- FIG. 2 several trajectories 13 are shown by way of example.
- On the outer housing wall can be formed by a detachment, a trajectory 13 ', which is characterized by a reversal of the Direction of movement of the fluid particle back to the power amplifier 8 is characterized. This trajectory 13 'is undesirable.
- FIG. 3 shows a diffuser 9 according to the invention.
- the diffuser 9 is arranged in the outflow region 14 of the steam turbine 1.
- the diffuser has an inlet 15 and a hub-side wall 10 and a housing wall 11 for limiting a flow medium.
- the diffuser 9 is characterized by a coolant 16 for cooling.
- the coolant comprises a pipe 19 which is flowed through by a cold medium.
- the coolant 16 is in this case designed such that the flow medium condenses during operation of the steam turbine 1 on the surface of the pipe 19, and thus generates a pressure sink.
- the pipe 19 should be mounted in a near area to the diffuser 9 for this purpose.
- the coolant 16 can in this case be arranged in such a way that it has channels through which cold medium can flow. Furthermore, the channel through which the cold medium can flow can be arranged on an inner side of the hub-side wall 10 or the housing wall 11.
- the embodiments of the coolant shown in Figures 3 and 4 are arranged for clarity, only the outer housing wall 11. Of course, the coolant 16 may be disposed on the hub side wall 10.
- the through-flowable with cold medium channel can also be arranged on an outer side 18 of the hub-side wall 10 or the outer housing wall 11.
- the coolant 16 can be applied to the locations in the diffuser where release of the flow medium is to be expected.
- FIG. 4 shows a further embodiment of the coolant 16.
- the coolant 16 is in this case formed as a spraying device for spraying the hub-side wall 10 or housing wall 11 with a cold medium.
- the cooling means 16 designed as a spraying device is designed in such a way that the cold medium is sprayed onto the inside 17 of the housing wall.
- the coolant 16 designed as a spraying device can be designed such that the cold medium is sprayed onto the outside 18 of the housing wall 11.
- coolant 16 designed as a spraying device can also be arranged on the hub-side wall 10.
- cold water can be removed from the cooling water circuit.
Landscapes
- Engineering & Computer Science (AREA)
- Mechanical Engineering (AREA)
- General Engineering & Computer Science (AREA)
- Structures Of Non-Positive Displacement Pumps (AREA)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
EP04026196A EP1655458A1 (fr) | 2004-11-04 | 2004-11-04 | Diffuseur pour une turbine à vapeur |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
EP04026196A EP1655458A1 (fr) | 2004-11-04 | 2004-11-04 | Diffuseur pour une turbine à vapeur |
Publications (1)
Publication Number | Publication Date |
---|---|
EP1655458A1 true EP1655458A1 (fr) | 2006-05-10 |
Family
ID=34927239
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP04026196A Withdrawn EP1655458A1 (fr) | 2004-11-04 | 2004-11-04 | Diffuseur pour une turbine à vapeur |
Country Status (1)
Country | Link |
---|---|
EP (1) | EP1655458A1 (fr) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2010242759A (ja) * | 2009-04-07 | 2010-10-28 | General Electric Co <Ge> | 排出損失を減少させるための冷却式排出フードプレート |
Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE907180C (de) * | 1951-03-08 | 1954-03-22 | Rolf Roeder Dipl Ing | Auslassdiffusor kurzer Baulaenge fuer Dampfturbinen |
FR1209527A (fr) * | 1958-08-12 | 1960-03-02 | Westinghouse Electric Corp | Appareil de contrôle d'écoulement |
CH388986A (de) * | 1960-12-05 | 1965-03-15 | Licentia Gmbh | Anordnung zum Mischkühlen des aus der Endstufe von Dampfturbinen austretenden Dampfes |
EP0600129A1 (fr) * | 1992-01-13 | 1994-06-08 | BRANDON, Ronald E. | Diffuseur-condenseur pour la vapeur saturée |
-
2004
- 2004-11-04 EP EP04026196A patent/EP1655458A1/fr not_active Withdrawn
Patent Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE907180C (de) * | 1951-03-08 | 1954-03-22 | Rolf Roeder Dipl Ing | Auslassdiffusor kurzer Baulaenge fuer Dampfturbinen |
FR1209527A (fr) * | 1958-08-12 | 1960-03-02 | Westinghouse Electric Corp | Appareil de contrôle d'écoulement |
CH388986A (de) * | 1960-12-05 | 1965-03-15 | Licentia Gmbh | Anordnung zum Mischkühlen des aus der Endstufe von Dampfturbinen austretenden Dampfes |
EP0600129A1 (fr) * | 1992-01-13 | 1994-06-08 | BRANDON, Ronald E. | Diffuseur-condenseur pour la vapeur saturée |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2010242759A (ja) * | 2009-04-07 | 2010-10-28 | General Electric Co <Ge> | 排出損失を減少させるための冷却式排出フードプレート |
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