WO2008035465A1 - Centrifugal compressor - Google Patents
Centrifugal compressor Download PDFInfo
- Publication number
- WO2008035465A1 WO2008035465A1 PCT/JP2007/052391 JP2007052391W WO2008035465A1 WO 2008035465 A1 WO2008035465 A1 WO 2008035465A1 JP 2007052391 W JP2007052391 W JP 2007052391W WO 2008035465 A1 WO2008035465 A1 WO 2008035465A1
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- WO
- WIPO (PCT)
- Prior art keywords
- wall surface
- diffuser
- side wall
- centrifugal compressor
- diffuser passage
- 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.)
- Ceased
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Classifications
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F04—POSITIVE - DISPLACEMENT MACHINES FOR LIQUIDS; PUMPS FOR LIQUIDS OR ELASTIC FLUIDS
- F04D—NON-POSITIVE-DISPLACEMENT PUMPS
- F04D29/00—Details, component parts, or accessories
- F04D29/40—Casings; Connections of working fluid
- F04D29/403—Casings; Connections of working fluid especially adapted for elastic fluid pumps
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F04—POSITIVE - DISPLACEMENT MACHINES FOR LIQUIDS; PUMPS FOR LIQUIDS OR ELASTIC FLUIDS
- F04D—NON-POSITIVE-DISPLACEMENT PUMPS
- F04D29/00—Details, component parts, or accessories
- F04D29/40—Casings; Connections of working fluid
- F04D29/42—Casings; Connections of working fluid for radial or helico-centrifugal pumps
- F04D29/44—Fluid-guiding means, e.g. diffusers
- F04D29/441—Fluid-guiding means, e.g. diffusers especially adapted for elastic fluid pumps
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F04—POSITIVE - DISPLACEMENT MACHINES FOR LIQUIDS; PUMPS FOR LIQUIDS OR ELASTIC FLUIDS
- F04D—NON-POSITIVE-DISPLACEMENT PUMPS
- F04D29/00—Details, component parts, or accessories
- F04D29/002—Details, component parts, or accessories especially adapted for elastic fluid pumps
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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
- F05D2210/00—Working fluids
- F05D2210/10—Kind or type
- F05D2210/12—Kind or type gaseous, i.e. compressible
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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
- F05D2250/50—Inlet or outlet
- F05D2250/52—Outlet
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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
- F05D2260/00—Function
- F05D2260/60—Fluid transfer
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- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y10—TECHNICAL SUBJECTS COVERED BY FORMER USPC
- Y10S—TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y10S415/00—Rotary kinetic fluid motors or pumps
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y10—TECHNICAL SUBJECTS COVERED BY FORMER USPC
- Y10S—TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y10S417/00—Pumps
Definitions
- the present invention relates to a centrifugal compressor such as a turbocharger.
- centrifugal compressor such as a turbocharger used for an internal combustion engine for automobiles is known.
- FIG. 5A is a cross-sectional view showing a main part of a conventional centrifugal compressor.
- the illustrated centrifugal compressor 10 compresses a fluid such as gas or air introduced from the outside of the housing 11 by rotating an impeller 13 having a large number of blades 12 in a housing 11.
- the fluid flow (air flow) formed in this way is sent to the outside through the impeller outlet (hereinafter also referred to as “diffuser inlet”) 14, the diffuser passage 15 and the scroll 16 which is the outer peripheral end of the impeller 13.
- reference numeral 17 in the figure denotes an axial center line around which the impeller 13 rotates.
- the diffuser passage 15 described above is provided between the impeller outlet 14 and the scroll 16, and is a passage for recovering the static pressure by decelerating the airflow discharged from the impeller outlet 14.
- the diffuser passage 15 is usually formed by a pair of opposed wall surfaces. In the following description, one of the pair of opposed wall surfaces is referred to as a shroud side wall surface 15a, and the other is referred to as a groove side wall surface 15b.
- the mechanism for generating surging is considered to occur when the backflow region of the airflow reaches the outlet end of the diffuser passage 15.
- the above-described backflow region is generated. It is considered that the raw material is caused by the flow on the compressor shroud side in the diffuser passage 15, that is, the flow distortion along the shroud side wall surface 15a. Therefore, a diffuser for reducing such flow distortion is used. A structure has been proposed.
- the flow distortion described above is a state in which the flow velocity distribution and the pressure distribution are non-uniform.
- the flow passage cross-sectional area of the diffuser passage 15 is changed, or A structure and a method using a circulation passage are employed.
- the emphasis is on reducing the distortion that occurs on the inlet side (impeller outlet 14 side) of the diffuser passage 15.
- Patent Document 1 JP-A-10-176699
- the conventional diffuser passage 15 generally has a shroud side wall surface 15a and a nove side wall surface 15b, which are a pair of opposing wall surfaces, in a parallel shape.
- the axial flow width W of the is constant in the circumferential direction.
- the reverse flow region indicated by arrow A in the figure
- the flow is separated from the side wall surface 15b near the diffuser outlet 18 and the reverse flow area (arrow in the figure) It was found that it was formed with a mark B). In other words, not the shroud side reverse flow region A but the reverse flow region B is considered to cause surging.
- the present invention has been made in view of the above circumstances, and its object is to separate the flow from the hub side wall surface downstream of the hub side wall surface in the diffuser passage (near the diffuser outlet). It is to provide a centrifugal compressor having a diffuser structure that is difficult to perform.
- the present invention employs the following means in order to solve the above problems.
- the centrifugal compressor according to the present invention is provided with a diffuser passage that restores static pressure by decelerating the airflow discharged from the outer peripheral end force of the impeller rotating in the housing.
- the hub of the diffuser passage The side wall surface is provided with an inclined region approaching the shroud side at a position downstream of the portion parallel to the normal direction of the impeller outlet cross section.
- the hub side wall surface of the diffuser passage is provided with an inclined region that approaches the shroud side at a position downstream of the portion parallel to the normal direction of the impeller outlet cross section. Therefore, in the inclined region, the radial velocity in the low speed region generated on the side wall of the hub increases, and the radial velocity distribution in the diffuser passage becomes uniform.
- the inclined region is, for example, an inclined flat surface, a curved surface or a stepped portion formed on the nove side wall surface, and in this inclined region, the closer to the downstream side wall surface, the closer to the downstream side.
- the axial wall width of the diffuser passage may be narrowed from the upstream side to the downstream side by inclining the hub side wall surface.
- a preferred position in the length direction of the diffuser passage where the inclined region is provided is a ratio of 0.3 to 0.3 of the diffuser passage from the diffuser inlet to the diffuser outlet (1) with the base point (0) as a base point. This is the range on the downstream side (exit side) from 0.7.
- the inclined region provided in the diffuser passage is the hub side wall surface. It is preferable to set so that the maximum amount of protrusion toward the side wall of the shroud is about 1Z3 to 1Z5 of the passage width that is equivalent to the size of the backflow area measured.
- a preferable inclination angle is a force that is 20 degrees or less with respect to the normal line of the impeller outlet cross section.
- a more preferable inclination angle is a method of the impeller outlet cross section. It is 2 degrees or more and 10 degrees or less with reference to the line. If the angle of inclination is excessive, the air flow is accelerated again by reducing the passage area, which is not preferable.
- the hub side wall surface of the diffuser passage is provided with an inclined region that approaches the shroud side at a position downstream of a portion parallel to the normal direction of the impeller outlet cross section. Therefore, in this inclined region, the radial speed of the low speed region generated on the hub side wall surface increases. For this reason, the radial velocity distribution in the diffuser passage is made uniform and local separation is less likely to occur, so that the surge flow rate can be reduced and a wide range operation can be achieved to widen the compressor operating range.
- the present invention described above is suitable for a wide range of a small centrifugal compressor equipped with a vaneless diffuser, such as an automotive turbocharger that requires a wide compressor operating range.
- FIG. 1 is a cross-sectional view of a diffuser passage showing a first embodiment of a centrifugal compressor according to the present invention.
- FIG. 2 is a cross-sectional view showing a first modification of FIG.
- FIG. 3 is a cross-sectional view showing a second modification of FIG.
- FIG. 4 is a cross-sectional view of a diffuser passage showing a second embodiment of the centrifugal compressor according to the present invention.
- FIG. 5A is a cross-sectional view showing the main parts of a centrifugal compressor.
- FIG. 5B is a cross-sectional view showing a conventional structure of a diffuser passage.
- the centrifugal compressor 10 includes a diffuser passage 15 that recovers static pressure by decelerating the airflow discharged from the outer peripheral end of the impeller 13 that rotates in the housing 11.
- the diffuser passage 15 is provided so as to connect between the impeller outlet (diffuser inlet) 14 and the scroll 16, and is formed between a pair of opposing wall surfaces including the shroud side wall surface 15a and the nozzle side wall surface 15b. Has been.
- FIG. 1 is a cross-sectional view of the diffuser passage 15 showing the first embodiment.
- This diffuser passage 15 also introduces the air flow (indicated by the white arrow in the figure) from which the outer peripheral end force of the impeller 13 is also discharged into the diffuser inlet 14 force between the shroud side wall surface 15a and the hub side wall surface 15b.
- the airflow guided to the formed flow path is caused to flow from the diffuser outlet 18 to the scroll 16.
- the hub side wall surface 15b of the diffuser passage 15 is provided with an inclined plane 20 approaching in the direction of the shroud side wall surface 15a at a position downstream of a portion parallel to the normal direction of the impeller outlet cross section. ing.
- This inclined plane 20 is an inclined area formed on the hub side wall surface 15b of the diffuser passage 15, and is closer to the shroud side wall surface 15a as it is separated from the diffuser inlet 14 and closer to the diffuser outlet 18, and between the opposing wall surfaces.
- the axial flow path width W which is the distance, is reduced to Wa.
- the inclined region formed by the inclined wall surface 20 is upstream of the passage in the diffuser passage 15 in which the flow path length in the normal direction is L and parallel to the normal direction and the flow path length is La. Is inclined toward the shroud side wall surface 15a, and is provided in the downstream portion where the flow path length is Lb.
- a suitable length of the downstream portion Lb that becomes the inclined region is set to a length La of the upstream portion parallel to the normal direction of 0.3 to 0.7. The remaining part on the downstream side.
- the inclination angle ⁇ when the inclined region is a plane is preferably set to 20 degrees or less with reference to the normal line of the impeller outlet cross section.
- the more suitable inclination angle ⁇ is 2 degrees or more and 10 degrees or less with respect to the normal line of the impeller outlet cross section.
- the above-mentioned normal line and normal direction of the impeller outlet cross section mean a straight line extending in the radial direction from the axial center line 17 around which the impeller 13 rotates through the impeller outlet cross section and its direction. It is similar to the air flow direction.
- the diffuser passage 15 including the inclined region formed by the inclined wall surface 20 has the shroud side wall surface 15a and the hub side wall surface 15b both parallel to the normal direction and the axial flow path width W.
- the axial flow path width W is toward the diffuser outlet 18 side due to the upstream region where the is constant and the inclined wall surface 20 where the hub side wall surface 15b is inclined toward the shroud side wall surface 15a. It is narrowed and has an inclined area on the downstream side.
- the airflow introduced from the diffuser inlet 14 is decelerated by flowing through the diffuser passage 15 to recover the static pressure.At this time, on the downstream side approaching the diffuser outlet 18, it is generated near the wall surface. A low-speed region air flow, which is considered to cause separation from the side wall surface 15b, is gradually guided toward the shroud side wall surface 15a by being guided to the inclined wall surface 20.
- the low speed region is a region where the velocity component in the radial direction from the diffuser inlet 14 toward the diffuser outlet 18 is low.
- the radial direction and the normal direction described above coincide.
- the surge flow rate can be reduced, so that a wide range expansion that extends the operating range of the centrifugal compressor can be achieved.
- a vane-less diffuser such as an automobile turbocharger
- the axial flow path width W is conversely narrowed toward the diffuser outlet 18 side.
- the airflow guided to the inclined wall surface 20 gradually flows toward the hub side wall surface 15b. It is accelerated by following. For this reason, the velocity distribution in the radial direction is force! This increases the speed difference between the speed shroud side wall surface 15a and the hub side wall surface 15b where the low speed region exists, thereby further increasing non-uniformity.
- an inclined region is formed by an inclined curved surface 21 instead of the inclined plane 20 of FIG.
- This inclined curved surface 21 is in the length direction of the diffuser passage that provides the inclined region.
- the preferred position (ratio of length Lb) and the maximum protrusion Wb from the wall side wall surface 15b to the shroud side wall surface 15a are the same as those of the inclined plane 20, and are appropriately curved to satisfy this condition. Etc. may be set.
- the curved surface may be either a concave curved surface or a convex curved surface as viewed from inside the diffuser passage 15.
- an inclined region is formed by an inclined folding line 22 instead of the inclined plane 20 of FIG.
- the inclined fold line 22 is composed of a flat inclined portion 22a and a parallel portion 22b on the diffuser outlet 18 side.
- the parallel portion 22b is parallel to the shroud side wall surface 15a and the hub side wall surface 15b.
- the inclined folding line 22 is a suitable position in the length direction of the diffuser passage where the inclined region is provided (the ratio of the length Lb) and the maximum value Wb of the protrusion amount from the side wall wall surface 15b to the shroud side wall surface 15a. Is the same as the inclined plane 20.
- the inclined folding line 22 shown in the figure may be combined with an inclined portion 22a having a force of two or more steps, which is a combination of the inclined portion 22a and the parallel portion 22b, or may be combined with a curved surface.
- FIG. 4 is a cross-sectional view showing a second embodiment of the centrifugal compressor according to the present invention.
- symbol is attached
- path 30 is divided
- the hub side wall surface 30b is downstream of the parallel portion 32 that is a portion parallel to the normal direction of the impeller outlet cross section.
- An inclined region approaching the shroud side is provided at a position on the side. That is, when the hub side wall surface 30b of the shroud-side inclined portion 33 approaches the shroud side, an inclined region having substantially the same function as the inclined plane 20 described above is formed.
- the hub side wall surface 30b having an inclined plane similar to the inclined plane 20 increases the velocity component in the radial direction in the low speed region generated near the wall surface of the hub side wall surface 30b.
- the velocity distribution in the radial direction becomes uniform, and local peeling is less likely to occur.
- the hub side wall surface 15a of the diffuser passage 15 is provided with an inclined region that approaches the shroud side at a position downstream of the portion parallel to the normal direction of the impeller outlet cross section. Therefore, the radial speed in the low speed region generated on the hub side wall surface 15a increases, and the radial speed distribution in the diffuser passage 15 becomes uniform. Therefore, in the vicinity of the diffuser outlet 18 in the diffuser passage 15, local air flow separation from the wall surface occurs, so that the surge flow can be reduced and a wide range operation that widens the compressor operating range is achieved. it can.
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Abstract
Description
明 細 書 Specification
遠心圧縮機 Centrifugal compressor
技術分野 Technical field
[0001] 本発明は、ターボチャージャ等の遠心圧縮機に関する。 [0001] The present invention relates to a centrifugal compressor such as a turbocharger.
背景技術 Background art
[0002] 従来、たとえば自動車用の内燃機関に使用されるターボチャージャ等の遠心圧縮 機が知られている。 Conventionally, a centrifugal compressor such as a turbocharger used for an internal combustion engine for automobiles is known.
図 5Aは、従来の遠心圧縮機の要部を示す断面図である。図示の遠心圧縮機 10は 、ハウジング 11内で多数のブレード 12を備えたインペラ 13が回転することにより、ハ ウジング 11の外部から導入したガスや空気等の流体を圧縮する。こうして形成された 流体の流れ (気流)は、インペラ 13の外周端となるインペラ出口(以下では、「ディフユ 一ザ入口」とも呼ぶ) 14、ディフューザ通路 15及びスクロール 16を通って外部へ送 出される。なお、図中の符号 17は、インペラ 13が回転する軸中心線である。 FIG. 5A is a cross-sectional view showing a main part of a conventional centrifugal compressor. The illustrated centrifugal compressor 10 compresses a fluid such as gas or air introduced from the outside of the housing 11 by rotating an impeller 13 having a large number of blades 12 in a housing 11. The fluid flow (air flow) formed in this way is sent to the outside through the impeller outlet (hereinafter also referred to as “diffuser inlet”) 14, the diffuser passage 15 and the scroll 16 which is the outer peripheral end of the impeller 13. . Note that reference numeral 17 in the figure denotes an axial center line around which the impeller 13 rotates.
[0003] 上述したディフューザ通路 15は、インペラ出口 14とスクロール 16との間に設けられ ており、インペラ出口 14から吐出される気流を減速させることで静圧を回復させるた めの通路である。このディフューザ通路 15は、通常一対の対向した壁面で形成され ており、以下の説明では、対向する一対の壁面の一方をシユラウド側壁面 15aと呼び 、他方をノ、ブ側壁面 15bと呼ぶ。 [0003] The diffuser passage 15 described above is provided between the impeller outlet 14 and the scroll 16, and is a passage for recovering the static pressure by decelerating the airflow discharged from the impeller outlet 14. The diffuser passage 15 is usually formed by a pair of opposed wall surfaces. In the following description, one of the pair of opposed wall surfaces is referred to as a shroud side wall surface 15a, and the other is referred to as a groove side wall surface 15b.
なお、内燃機関と組み合わせて使用される自動車用のターボチャージャでは、広い 圧縮機作動範囲が要求されることから、通常べーンを持たな 、タイプのディフューザ (ベーンレスディフューザ)が採用されている。 Since turbochargers for automobiles used in combination with internal combustion engines require a wide compressor operating range, a type of diffuser (vaneless diffuser) that does not normally have a vane is used. .
[0004] ところで、近年においては、遠心圧縮機 10の流量増大と高圧力比化に伴い、ディ フューザ通路 15へ流入する気流の歪みは大きくなつている。歪みの大きな流れがデ ィフューザ通路 15に入ることにより、ディフューザ通路 15内で小流量側作動限界を 決定するサージングと呼ばれる現象が起きると考えられている。 [0004] Incidentally, in recent years, the distortion of the airflow flowing into the diffuser passage 15 has become larger as the flow rate of the centrifugal compressor 10 increases and the pressure ratio increases. It is considered that a phenomenon called surging that determines the operation limit on the small flow rate side in the diffuser passage 15 occurs when a flow having a large strain enters the diffuser passage 15.
サージングが発生するメカニズムは、気流の逆流領域がディフューザ通路 15の出 口側端部に到達した時に発生すると考えられている。また、上述した逆流領域の発 生は、ディフューザ通路 15内における圧縮機シュラウド側の流れ、すなわち、シユラ ウド側壁面 15aに沿う流れの歪みに原因があると考えられているので、このような流れ の歪みを低減するためのディフューザ構造が提案されている。 The mechanism for generating surging is considered to occur when the backflow region of the airflow reaches the outlet end of the diffuser passage 15. In addition, the above-described backflow region is generated. It is considered that the raw material is caused by the flow on the compressor shroud side in the diffuser passage 15, that is, the flow distortion along the shroud side wall surface 15a. Therefore, a diffuser for reducing such flow distortion is used. A structure has been proposed.
[0005] 上述した流れの歪みは、流速分布や圧力分布が不均一な状態のことであり、これを 均一化するための従来技術として、ディフューザ通路 15の流路断面積を変更したり、 あるいは、循環通路を利用するなどした構造及び手法が採用されている。このような 従来技術の場合、いずれもディフューザ通路 15の入口側 (インペラ出口 14側)に生 じる歪みを低減することに重点をおいたものである。 [0005] The flow distortion described above is a state in which the flow velocity distribution and the pressure distribution are non-uniform. As a conventional technique for making this uniform, the flow passage cross-sectional area of the diffuser passage 15 is changed, or A structure and a method using a circulation passage are employed. In the case of such conventional techniques, the emphasis is on reducing the distortion that occurs on the inlet side (impeller outlet 14 side) of the diffuser passage 15.
上述した歪み低減の従来技術としては、たとえばディフューザ通路 15の壁面に流 路断面積を変化させるための凸部または凹部を設けることが提案されている。このよ うな凸部及び凹部は、周方向に通路形状を変更して周方向に沿う空気の流れを一 様化するので、これによつて圧縮効率の向上が可能になるとされる。(たとえば、特許 文献 1参照) As a conventional technique for reducing the above-described distortion, for example, it has been proposed to provide a convex portion or a concave portion on the wall surface of the diffuser passage 15 to change the cross-sectional area of the flow passage. Such protrusions and recesses change the shape of the passage in the circumferential direction to equalize the flow of air along the circumferential direction, which can improve the compression efficiency. (For example, see Patent Document 1)
特許文献 1 :特開平 10— 176699号公報 Patent Document 1: JP-A-10-176699
発明の開示 Disclosure of the invention
[0006] し力しながら、特に自動車用ターボチャージャのような小型の遠心圧縮機では、デ ィフューザ通路内を流れる気流など内部流動の計測が困難である。従って、実際の 内部流動の歪みは未だ十分に把握されておらず、さらに、サージングに至るまでの 現象につ!ヽても解明されて 、な 、ため、これらを解明して効果的なサージング防止 手段を開発し、遠心圧縮機の作動範囲を拡大すること (ワイドレンジ化)が必要となつ ている。 [0006] However, particularly in a small centrifugal compressor such as a turbocharger for automobiles, it is difficult to measure an internal flow such as an airflow flowing in the diffuser passage. Therefore, the distortion of the actual internal flow is not yet fully understood, and further, the phenomena leading to surging have been elucidated. It is necessary to develop means and expand the operating range of centrifugal compressors (wide range).
[0007] 従来のディフューザ通路 15は、一般的には図 5Bに示すように、対向する一対の壁 面であるシュラウド側壁面 15a及びノヽブ側壁面 15bが平行な形状とされ、ディフュー ザ通路 15の軸方向流路幅 Wは周方向に一定である。このように構成された従来の ディフューザ通路 15について、モデルによる内部流動計測を実施してサージングに 至るまで流動パターンを確認したところ、逆流領域(図中に矢印 Aで表示)がディフユ 一ザ通路 15のディフューザ出口 18側端部に到達するような流れ場となるより前に、 ディフューザ出口 18の近傍でノ、ブ側壁面 15bから流れが剥離して逆流域(図中に矢 印 Bで表示)を形成しているとの知見を得た。すなわち、シュラウド側逆流領域 Aでは なく逆流域 Bが起因となってサージングを引き起こすと考えられる。 As shown in FIG. 5B, the conventional diffuser passage 15 generally has a shroud side wall surface 15a and a nove side wall surface 15b, which are a pair of opposing wall surfaces, in a parallel shape. The axial flow width W of the is constant in the circumferential direction. For the conventional diffuser passage 15 configured in this way, we measured the internal flow using the model and confirmed the flow pattern until surging. As a result, the reverse flow region (indicated by arrow A in the figure) showed the diffuser passage 15 Before the flow field reaches the end of the diffuser outlet 18 side, the flow is separated from the side wall surface 15b near the diffuser outlet 18 and the reverse flow area (arrow in the figure) It was found that it was formed with a mark B). In other words, not the shroud side reverse flow region A but the reverse flow region B is considered to cause surging.
[0008] このようにディフューザ出口 18の近傍で発生するハブ側壁面 15bからの流れの剥 離は、たとえば特許文献 1に記載されているように、周方向に通路形状を変更して周 方向に沿う空気の流れを一様ィ匕するような従来技術では、これを抑制することはでき ないと考えられる。 [0008] In this way, the separation of the flow from the hub side wall surface 15b that occurs in the vicinity of the diffuser outlet 18 can be achieved by changing the shape of the passage in the circumferential direction as described in Patent Document 1, for example. It is thought that this cannot be suppressed by the conventional technology in which the flow of the air along is uniform.
本発明は、上記の事情に鑑みてなされたものであり、その目的とするところは、ディ フューザ通路内のハブ側壁面下流側(ディフューザ出口の近傍)において、ハブ側 壁面カゝら流れが剥離しにくいディフューザ構造を備えた遠心圧縮機を提供することに ある。 The present invention has been made in view of the above circumstances, and its object is to separate the flow from the hub side wall surface downstream of the hub side wall surface in the diffuser passage (near the diffuser outlet). It is to provide a centrifugal compressor having a diffuser structure that is difficult to perform.
[0009] 本発明は、上記の課題を解決するため、下記の手段を採用した。 The present invention employs the following means in order to solve the above problems.
本発明に係る遠心圧縮機は、ハウジング内で回転するインペラの外周端力 吐出 される気流を減速させることで静圧を回復させるディフューザ通路が設けられている 遠心圧縮機において、前記ディフューザ通路のハブ側壁面が、インペラ出口断面の 法線方向に平行な部分の下流側となる位置に、シュラウド側へ接近する傾斜領域を 備えて 、ることを特徴とするものである。 The centrifugal compressor according to the present invention is provided with a diffuser passage that restores static pressure by decelerating the airflow discharged from the outer peripheral end force of the impeller rotating in the housing. In the centrifugal compressor, the hub of the diffuser passage The side wall surface is provided with an inclined region approaching the shroud side at a position downstream of the portion parallel to the normal direction of the impeller outlet cross section.
[0010] このような遠心圧縮機によれば、ディフューザ通路のハブ側壁面が、インペラ出口 断面の法線方向に平行な部分の下流側となる位置に、シュラウド側へ接近する傾斜 領域を備えて ヽるので、傾斜領域ではハブ側壁面に発生する低速領域の半径方向 速度が増大し、ディフューザ通路内の半径方向速度分布が均一化する。 [0010] According to such a centrifugal compressor, the hub side wall surface of the diffuser passage is provided with an inclined region that approaches the shroud side at a position downstream of the portion parallel to the normal direction of the impeller outlet cross section. Therefore, in the inclined region, the radial velocity in the low speed region generated on the side wall of the hub increases, and the radial velocity distribution in the diffuser passage becomes uniform.
この場合の傾斜領域は、たとえばノヽブ側壁面に形成した傾斜平面、曲面または段 差面の部分であり、この傾斜領域では、対向するシユラウド側壁面へ向けて、下流側 へ行くほど接近するようにハブ側壁面を傾斜させることにより、ディフューザ通路の軸 方向流路幅が上流側から下流側へ狭まるものであればよい。 In this case, the inclined region is, for example, an inclined flat surface, a curved surface or a stepped portion formed on the nove side wall surface, and in this inclined region, the closer to the downstream side wall surface, the closer to the downstream side. The axial wall width of the diffuser passage may be narrowed from the upstream side to the downstream side by inclining the hub side wall surface.
[0011] 上記の発明において、傾斜領域を設けるディフューザ通路長さ方向の好適な位置 は、ディフューザ入口を基点(0)にしたディフューザ出口(1)までのディフューザ通路 のうち、比率で 0. 3〜0. 7よりも下流側(出口側)の範囲となる。 [0011] In the above invention, a preferred position in the length direction of the diffuser passage where the inclined region is provided is a ratio of 0.3 to 0.3 of the diffuser passage from the diffuser inlet to the diffuser outlet (1) with the base point (0) as a base point. This is the range on the downstream side (exit side) from 0.7.
また、上記の発明において、ディフューザ通路に設ける傾斜領域は、ハブ側壁面か らシユラウド側壁面へ向けた突出量の最大値が計測による逆流領域の大きさ同等と なる通路幅の 1Z3〜1Z5程度となるように設定することが好ま U、。 In the above invention, the inclined region provided in the diffuser passage is the hub side wall surface. It is preferable to set so that the maximum amount of protrusion toward the side wall of the shroud is about 1Z3 to 1Z5 of the passage width that is equivalent to the size of the backflow area measured.
また、上記の発明において、傾斜領域を平面とした場合の好適な傾斜角度は、イン ペラ出口断面の法線を基準として 20度以下である力 より好適な傾斜角度は、イン ペラ出口断面の法線を基準として 2度以上 10度以下である。傾斜角度が過大である と通路面積縮小により気流が再度加速されてしまうため好ましくない。 In the above invention, when the inclined region is a plane, a preferable inclination angle is a force that is 20 degrees or less with respect to the normal line of the impeller outlet cross section. A more preferable inclination angle is a method of the impeller outlet cross section. It is 2 degrees or more and 10 degrees or less with reference to the line. If the angle of inclination is excessive, the air flow is accelerated again by reducing the passage area, which is not preferable.
[0012] 上述した本発明によれば、ディフューザ通路のハブ側壁面には、インペラ出口断面 の法線方向に平行な部分の下流側となる位置にシユラウド側へ接近する傾斜領域が 設けられているので、この傾斜領域においては、ハブ側壁面に発生する低速領域の 半径方向速度が増大する。このため、ディフューザ通路内の半径方向速度分布が均 一化し、局所的な剥離を生じにくくなるので、サージ流量の低減が可能になって圧縮 機作動範囲を広げるワイドレンジィ匕を達成できる。 [0012] According to the present invention described above, the hub side wall surface of the diffuser passage is provided with an inclined region that approaches the shroud side at a position downstream of a portion parallel to the normal direction of the impeller outlet cross section. Therefore, in this inclined region, the radial speed of the low speed region generated on the hub side wall surface increases. For this reason, the radial velocity distribution in the diffuser passage is made uniform and local separation is less likely to occur, so that the surge flow rate can be reduced and a wide range operation can be achieved to widen the compressor operating range.
また、上述した本発明は、特に広い圧縮機動作範囲が要求される自動車用ターボ チャージャのように、ベーンレスディフューザを備えた小型の遠心圧縮機をワイドレン ジ化する場合に適している。 Further, the present invention described above is suitable for a wide range of a small centrifugal compressor equipped with a vaneless diffuser, such as an automotive turbocharger that requires a wide compressor operating range.
図面の簡単な説明 Brief Description of Drawings
[0013] [図 1]本発明に係る遠心圧縮機の第 1の実施形態を示すディフューザ通路の断面図 である。 FIG. 1 is a cross-sectional view of a diffuser passage showing a first embodiment of a centrifugal compressor according to the present invention.
[図 2]図 1の第 1変形例を示す断面図である。 2 is a cross-sectional view showing a first modification of FIG.
[図 3]図 1の第 2変形例を示す断面図である。 3 is a cross-sectional view showing a second modification of FIG.
[図 4]本発明に係る遠心圧縮機の第 2の実施形態を示すディフューザ通路の断面図 である。 FIG. 4 is a cross-sectional view of a diffuser passage showing a second embodiment of the centrifugal compressor according to the present invention.
[図 5A]遠心圧縮機の要部を示す断面図である。 FIG. 5A is a cross-sectional view showing the main parts of a centrifugal compressor.
[図 5B]ディフューザ通路の従来構造を示す断面図である。 FIG. 5B is a cross-sectional view showing a conventional structure of a diffuser passage.
符号の説明 Explanation of symbols
[0014] 10 遠心圧縮機 [0014] 10 Centrifugal compressor
11 ハウジング 11 Housing
12 インペラ 14 インペラ出口(ディフューザ入口) 12 Impeller 14 Impeller exit (diffuser entrance)
15, 30 ディフューザ通路 15, 30 Diffuser passage
15a, 30a シュラウド側壁面 15a, 30a shroud side wall
15b, 30b ハブ側壁面 15b, 30b Hub side wall
16 スクローノレ 16 scronore
18 ディフューザ出口 18 Diffuser outlet
20 傾斜平面 (傾斜領域) 20 Inclined plane (Inclined area)
21 傾斜曲面 (傾斜領域) 21 Inclined curved surface (inclined area)
22 傾斜折線 (傾斜領域) 22 Inclined fold line (inclined area)
33 シュラウド側傾斜部 (傾斜領域) 33 Shroud side slope (slope area)
発明を実施するための最良の形態 BEST MODE FOR CARRYING OUT THE INVENTION
[0015] 以下、本発明に係る遠心圧縮機の一実施形態を図面に基づいて説明する。 Hereinafter, an embodiment of a centrifugal compressor according to the present invention will be described with reference to the drawings.
図 5Aに示すように、遠心圧縮機 10は、ハウジング 11内で回転するインペラ 13の外 周端から吐出される気流を減速させることで静圧を回復させるディフューザ通路 15を 備えている。このディフューザ通路 15は、インペラ出口(ディフューザ入口) 14とスク ロール 16との間を連結するように設けられており、シュラウド側壁面 15a及びノヽブ側 壁面 15bよりなる対向する一対の壁面間に形成されている。 As shown in FIG. 5A, the centrifugal compressor 10 includes a diffuser passage 15 that recovers static pressure by decelerating the airflow discharged from the outer peripheral end of the impeller 13 that rotates in the housing 11. The diffuser passage 15 is provided so as to connect between the impeller outlet (diffuser inlet) 14 and the scroll 16, and is formed between a pair of opposing wall surfaces including the shroud side wall surface 15a and the nozzle side wall surface 15b. Has been.
[0016] 図 1は、第 1の実施形態を示すディフューザ通路 15の断面図である。このディフユ 一ザ通路 15は、インペラ 13の外周端力も吐出された気流(図中に白抜き矢印で示 す)をディフューザ入口 14力も導入し、シュラウド側壁面 15a及びハブ側壁面 15bの 壁面間に形成された流路に導かれた気流をディフューザ出口 18からスクロール 16 へ流出させる。 FIG. 1 is a cross-sectional view of the diffuser passage 15 showing the first embodiment. This diffuser passage 15 also introduces the air flow (indicated by the white arrow in the figure) from which the outer peripheral end force of the impeller 13 is also discharged into the diffuser inlet 14 force between the shroud side wall surface 15a and the hub side wall surface 15b. The airflow guided to the formed flow path is caused to flow from the diffuser outlet 18 to the scroll 16.
図示の実施形態では、ディフューザ通路 15のハブ側壁面 15bが、インペラ出口断 面の法線方向に平行な部分の下流側となる位置に、シュラウド側壁面 15aの方向へ 接近する傾斜平面 20を備えている。この傾斜平面 20は、ディフューザ通路 15のハ ブ側壁面 15bに形成した傾斜領域であり、ディフューザ入口 14から離間してディフユ 一ザ出口 18に近づくほどシュラウド側壁面 15aに接近し、対向する壁面間距離であ る軸方向流路幅 Wを Waまで狭めている。 [0017] すなわち、傾斜壁面 20により形成された傾斜領域は、法線方向の流路長さを Lとし たディフューザ通路 15において、法線方向に平行で流路長さを Laとした通路上流 側からシュラウド側壁面 15aの方向へ向けて傾斜し、流路長さを Lbとした下流部分に 設けられている。ここで、流路長さ Lを 1とすれば、傾斜領域となる下流部分 Lbの好適 な長さは、法線方向と平行な上流部分の長さ Laを 0. 3〜0. 7とした下流側の残りの 部分となる。換言すれば、ディフューザ通路 15の長さ方向において傾斜領域を設け る好適な位置は、ディフューザ入口 14を基点(0)にして終点(1)となるディフューザ 出口 18までの流路長さを L (L= 1)とすれば、上流部分の長さ Laを 0. 3〜0. 7の比 率に設定し、かつ、下流部分の長さ Lbを 0. 7〜0. 3の比率に設定すればよい。従つ て、流路長さ Lは上流部分の長さ Laと下流側の長さ Lbとの合計値 (L = La + Lb)で あるから、上流部分の長さ Laと下流側の長さ Lbとの合計値 Lは常に「1」となる。 In the illustrated embodiment, the hub side wall surface 15b of the diffuser passage 15 is provided with an inclined plane 20 approaching in the direction of the shroud side wall surface 15a at a position downstream of a portion parallel to the normal direction of the impeller outlet cross section. ing. This inclined plane 20 is an inclined area formed on the hub side wall surface 15b of the diffuser passage 15, and is closer to the shroud side wall surface 15a as it is separated from the diffuser inlet 14 and closer to the diffuser outlet 18, and between the opposing wall surfaces. The axial flow path width W, which is the distance, is reduced to Wa. [0017] That is, the inclined region formed by the inclined wall surface 20 is upstream of the passage in the diffuser passage 15 in which the flow path length in the normal direction is L and parallel to the normal direction and the flow path length is La. Is inclined toward the shroud side wall surface 15a, and is provided in the downstream portion where the flow path length is Lb. Here, if the flow path length L is 1, a suitable length of the downstream portion Lb that becomes the inclined region is set to a length La of the upstream portion parallel to the normal direction of 0.3 to 0.7. The remaining part on the downstream side. In other words, the preferred position for providing the inclined region in the length direction of the diffuser passage 15 is that the flow path length from the diffuser inlet 14 to the diffuser outlet 18 that is the base point (0) to the end point (1) is L ( If L = 1), the length La of the upstream portion is set to a ratio of 0.3 to 0.7, and the length Lb of the downstream portion is set to a ratio of 0.7 to 0.3. That's fine. Therefore, the flow path length L is the sum of the upstream length La and the downstream length Lb (L = La + Lb), so the upstream length La and the downstream length L The total value L with Lb is always “1”.
[0018] また、ディフューザ通路 15に設ける傾斜領域は、ハブ側壁面 15bからシュラウド側 壁面 15aへ向けた傾斜壁面 20の突出量力 最大値 Wbとなるディフューザ出口 18に おいて通路幅の 1Z3〜1Z5程度となるように設定することが好ましい。すなわち、突 出量の最大値 Wbは 1Z3〜: LZ5W程度 (Wb^ lZ3〜: LZ5W)となるので、傾斜壁 面 20により狭められた軸方向流路幅 Waは、軸方向流路幅 Wの 2Z3〜4Z5程度( Wa = 2Z3〜4Z5W)となるように設定される。 [0018] In addition, the inclined region provided in the diffuser passage 15 is about 1Z3 to 1Z5 of the passage width at the diffuser outlet 18 where the protruding amount force Wb of the inclined wall surface 20 from the hub side wall surface 15b to the shroud side wall surface 15a becomes the maximum value Wb. It is preferable to set so that. That is, the maximum value Wb of the protruding amount is about 1Z3 to: LZ5W (Wb ^ lZ3 to: LZ5W), so that the axial channel width Wa narrowed by the inclined wall surface 20 is equal to the axial channel width W. It is set to be about 2Z3 to 4Z5 (Wa = 2Z3 to 4Z5W).
また、上述した傾斜壁面 20のように、傾斜領域を平面とした場合の傾斜角度 Θは、 インペラ出口断面の法線を基準として 20度以下に設定することが好ましい。しかし、 より好適な傾斜角度 Θは、インペラ出口断面の法線を基準として 2度以上 10度以下 である。 In addition, as in the case of the inclined wall surface 20 described above, the inclination angle Θ when the inclined region is a plane is preferably set to 20 degrees or less with reference to the normal line of the impeller outlet cross section. However, the more suitable inclination angle Θ is 2 degrees or more and 10 degrees or less with respect to the normal line of the impeller outlet cross section.
なお、上述したインペラ出口断面の法線及び法線方向は、インペラ 13が回転する 軸中心線 17からインペラ出口断面を通過して外側へ放射状に延びる直線及びその 方向を意味するものであり、実質的には気流の流れ方向と近似している。 The above-mentioned normal line and normal direction of the impeller outlet cross section mean a straight line extending in the radial direction from the axial center line 17 around which the impeller 13 rotates through the impeller outlet cross section and its direction. It is similar to the air flow direction.
[0019] 上述したように、傾斜壁面 20により形成された傾斜領域を備えて ヽるディフューザ 通路 15は、シュラウド側壁面 15a及びハブ側壁面 15bがともに法線方向と平行で軸 方向流路幅 Wが一定となる上流側の領域と、ハブ側壁面 15bがシユラウド側壁面 15 aへ向けて傾斜する傾斜壁面 20により軸方向流路幅 Wがディフューザ出口 18側へ 狭められて 、く下流側の傾斜領域とを備えて 、る。 [0019] As described above, the diffuser passage 15 including the inclined region formed by the inclined wall surface 20 has the shroud side wall surface 15a and the hub side wall surface 15b both parallel to the normal direction and the axial flow path width W. The axial flow path width W is toward the diffuser outlet 18 side due to the upstream region where the is constant and the inclined wall surface 20 where the hub side wall surface 15b is inclined toward the shroud side wall surface 15a. It is narrowed and has an inclined area on the downstream side.
このため、ディフューザ入口 14から導入した気流は、ディフューザ通路 15を流れる ことにより減速されて静圧を回復するが、このとき、ディフューザ出口 18に近づいた下 流側では、壁面近傍に発生してハブ側壁面 15bから剥離する原因になると考えられ る低速領域の気流が、傾斜壁面 20に導かれることで徐々にシユラウド側壁面 15aの 方向へ流れていく。 For this reason, the airflow introduced from the diffuser inlet 14 is decelerated by flowing through the diffuser passage 15 to recover the static pressure.At this time, on the downstream side approaching the diffuser outlet 18, it is generated near the wall surface. A low-speed region air flow, which is considered to cause separation from the side wall surface 15b, is gradually guided toward the shroud side wall surface 15a by being guided to the inclined wall surface 20.
[0020] この場合の低速領域は、ディフューザ入口 14からディフューザ出口 18へ向かう半 径方向の速度成分が低い領域である。なお、図示の例においては、半径方向と上述 した法線方向とがー致している。 In this case, the low speed region is a region where the velocity component in the radial direction from the diffuser inlet 14 toward the diffuser outlet 18 is low. In the example shown in the figure, the radial direction and the normal direction described above coincide.
[0021] この結果、ハブ側壁面 15bの壁面近傍に発生した低速領域の気流は、半径方向の 速度成分が増大する。このため、ディフューザ通路 15内においては、半径方向の速 度分布が均一化するので、局所的な剥離は発生しに《なる。 [0021] As a result, the velocity component in the radial direction increases in the airflow in the low speed region generated near the wall surface of the hub side wall surface 15b. For this reason, in the diffuser passage 15, the radial velocity distribution is made uniform, so that local peeling does not occur.
このように、ディフューザ通路 15内に局所的な剥離が生じに《なると、サージ流量 の低減が可能になるため、遠心圧縮機の作動範囲を広げるワイドレンジィ匕を達成で きる。特に、自動車用ターボチャージャのように、ベーンレスディフューザを備えてい る小型の遠心圧縮機に広い圧縮機動作範囲が要求される場合に適用すれば、ワイ ドレンジィ匕の達成が容易になる。 As described above, when local separation occurs in the diffuser passage 15, the surge flow rate can be reduced, so that a wide range expansion that extends the operating range of the centrifugal compressor can be achieved. In particular, when applied to a small centrifugal compressor equipped with a vane-less diffuser, such as an automobile turbocharger, where a wide compressor operating range is required, it is easy to achieve a wide range.
[0022] ところで、シュラウド側壁面 15aに同様の傾斜領域を設けた場合を考えると、軸方向 流路幅 Wは反対にディフューザ出口 18側へ狭められる。しかし、シュラウド側壁面 15 aのディフューザ出口 18付近では、剥離の原因と考えられる低速領域が壁面近傍に 存在しないため、傾斜壁面 20に導かれた気流が徐々にハブ側壁面 15bの方向へ流 れていくことにより加速される。このため、半径方向の速度分布は、力!]速したシュラウ ド側壁面 15aと低速領域が存在するハブ側壁面 15bとの速度差を増すことになるの で、不均一がさらに増大することになる。 By the way, considering the case where a similar inclined region is provided on the shroud side wall surface 15a, the axial flow path width W is conversely narrowed toward the diffuser outlet 18 side. However, in the vicinity of the diffuser outlet 18 on the shroud side wall surface 15a, there is no low-speed region in the vicinity of the wall surface that is considered to be a cause of separation, so the airflow guided to the inclined wall surface 20 gradually flows toward the hub side wall surface 15b. It is accelerated by following. For this reason, the velocity distribution in the radial direction is force! This increases the speed difference between the speed shroud side wall surface 15a and the hub side wall surface 15b where the low speed region exists, thereby further increasing non-uniformity.
[0023] 次に、上述した傾斜領域の第 1変形例を図 2に基づ 、て説明する。なお、上述した 実施形態と同様の部分には同じ符号を付し、その詳細な説明は省略する。 Next, a first modification of the above-described inclined area will be described based on FIG. In addition, the same code | symbol is attached | subjected to the part similar to embodiment mentioned above, and the detailed description is abbreviate | omitted.
この第 1変形例では、図 1の傾斜平面 20に代えて、傾斜曲面 21により傾斜領域を 形成している。この傾斜曲面 21は、傾斜領域を設けるディフューザ通路長さ方向の 好適な位置 (長さ Lbの比率)及びノ、ブ側壁面 15bからシュラウド側壁面 15aへ向けた 突出量の最大値 Wbについては傾斜平面 20と同じであり、この条件を満足するように 適宜曲率等を設定すればよい。なお、この場合の曲面は、ディフューザ通路 15内か ら見て凹曲面及び凸曲面のいずれでもよい。 In this first modification, an inclined region is formed by an inclined curved surface 21 instead of the inclined plane 20 of FIG. This inclined curved surface 21 is in the length direction of the diffuser passage that provides the inclined region. The preferred position (ratio of length Lb) and the maximum protrusion Wb from the wall side wall surface 15b to the shroud side wall surface 15a are the same as those of the inclined plane 20, and are appropriately curved to satisfy this condition. Etc. may be set. In this case, the curved surface may be either a concave curved surface or a convex curved surface as viewed from inside the diffuser passage 15.
[0024] このような傾斜曲面 21による傾斜領域を設けても、ハブ側壁面 15bの壁面近傍に 発生した低速領域の気流は半径方向の速度成分が増大するので、ディフューザ通 路 15内においては、半径方向の速度分布が均一化して局所的な剥離を発生しにく くなる。 [0024] Even if such an inclined region by the inclined curved surface 21 is provided, the velocity component in the radial direction of the airflow in the low speed region generated in the vicinity of the wall surface of the hub side wall surface 15b increases, so in the diffuser passage 15, The radial velocity distribution becomes uniform and local delamination is less likely to occur.
従って、サージ流量の低減が可能になるため遠心圧縮機の作動範囲を広げるワイ ドレンジィ匕を達成でき、特に、ベーンレスディフューザを備えている小型の遠心圧縮 機に広い圧縮機動作範囲が要求される場合に適用すれば、ワイドレンジ化を容易に 達成できる。 Therefore, it is possible to reduce the surge flow rate and achieve a wide range that expands the operating range of the centrifugal compressor. In particular, a small centrifugal compressor equipped with a vaneless diffuser requires a wide compressor operating range. If applied to the case, wide range can be easily achieved.
[0025] 次に、上述した傾斜領域の第 2変形例を図 3に基づ 、て説明する。なお、上述した 実施形態と同様の部分には同じ符号を付し、その詳細な説明は省略する。 Next, a second modification of the above-described inclined region will be described based on FIG. In addition, the same code | symbol is attached | subjected to the part similar to embodiment mentioned above, and the detailed description is abbreviate | omitted.
この第 2変形例では、図 1の傾斜平面 20に代えて、傾斜折線 22により傾斜領域を 形成している。この傾斜折線 22は、平面の傾斜部 22aとディフューザ出口 18側の平 行部 22bとにより構成されており、この場合の平行部 22bは、シュラウド側壁面 15a及 びハブ側壁面 15bと平行とされる。 In the second modification, an inclined region is formed by an inclined folding line 22 instead of the inclined plane 20 of FIG. The inclined fold line 22 is composed of a flat inclined portion 22a and a parallel portion 22b on the diffuser outlet 18 side. In this case, the parallel portion 22b is parallel to the shroud side wall surface 15a and the hub side wall surface 15b. The
また、傾斜折線 22は、傾斜領域を設けるディフューザ通路長さ方向の好適な位置 ( 長さ Lbの比率)及びノ、ブ側壁面 15bからシュラウド側壁面 15aへ向けた突出量の最 大値 Wbについては傾斜平面 20と同じである。 In addition, the inclined folding line 22 is a suitable position in the length direction of the diffuser passage where the inclined region is provided (the ratio of the length Lb) and the maximum value Wb of the protrusion amount from the side wall wall surface 15b to the shroud side wall surface 15a. Is the same as the inclined plane 20.
[0026] このような傾斜折線 22による傾斜領域を設けても、ハブ側壁面 15bの壁面近傍に 発生した低速領域の気流は半径方向の速度成分が増大するので、ディフューザ通 路 15内においては、半径方向の速度分布が均一化して局所的な剥離を発生しにく くなる。 [0026] Even if such an inclined region by the inclined fold line 22 is provided, the air velocity in the low speed region generated near the wall surface of the hub side wall surface 15b increases the velocity component in the radial direction. Therefore, in the diffuser passage 15, The radial velocity distribution becomes uniform and local delamination is less likely to occur.
従って、サージ流量の低減が可能になるため遠心圧縮機の作動範囲を広げるワイ ドレンジィ匕を達成でき、特に、ベーンレスディフューザを備えている小型の遠心圧縮 機に広い圧縮機動作範囲が要求される場合に適用すれば、ワイドレンジ化を容易に 達成できる。 Therefore, it is possible to reduce the surge flow rate and achieve a wide range that expands the operating range of the centrifugal compressor. In particular, a small centrifugal compressor equipped with a vaneless diffuser requires a wide compressor operating range. If applied to the case, wide range can be easily Can be achieved.
なお、図示の傾斜折線 22は傾斜部 22aと平行部 22bとの組み合わせとした力 2段 階以上の傾斜部 22aを組み合わせてもよいし、さらに、曲面を組み合わせることも可 能である。 In addition, the inclined folding line 22 shown in the figure may be combined with an inclined portion 22a having a force of two or more steps, which is a combination of the inclined portion 22a and the parallel portion 22b, or may be combined with a curved surface.
[0027] 図 4は、本発明に係る遠心圧縮機の第 2実施形態を示す断面図である。なお、上述 した第 1の実施形態と同様の部分には同じ符号を付し、その詳細な説明は省略する この実施形態では、ディフューザ通路 30が三つの領域に分割される。すなわち、上 流側から順に、ハブ側傾斜部 31と、インペラ出口断面の法線方向に平行な平行部 3 2と、シュラウド側傾斜部 33とが一体に連結されている。このため、図 1に示す第 1の 実施形態に対し、最も上流側にハブ側傾斜部 31を追加するとともに、シュラウド側傾 斜部 33では、シュラウド側壁面 30aとハブ側壁面 30bとが平行に配置され、同じ傾斜 角度でシュラウド側へ向けて傾斜したものとなる。 FIG. 4 is a cross-sectional view showing a second embodiment of the centrifugal compressor according to the present invention. In addition, the same code | symbol is attached | subjected to the part similar to 1st Embodiment mentioned above, The detailed description is abbreviate | omitted In this embodiment, the diffuser channel | path 30 is divided | segmented into three area | regions. That is, in order from the upstream side, the hub side inclined portion 31, the parallel portion 32 parallel to the normal direction of the impeller outlet cross section, and the shroud side inclined portion 33 are integrally connected. For this reason, a hub-side inclined portion 31 is added to the most upstream side with respect to the first embodiment shown in FIG. 1, and at the shroud-side inclined portion 33, the shroud side wall surface 30a and the hub side wall surface 30b are parallel to each other. It is arranged and inclined toward the shroud side at the same inclination angle.
[0028] このような構成を採用しても、ディフューザ通路 30のシユラウド側傾斜部 33におい ては、ハブ側壁面 30bが、インペラ出口断面の法線方向に平行な部分となる平行部 32の下流側となる位置に、シュラウド側へ接近する傾斜領域を備えている。すなわち 、シュラウド側傾斜部 33のハブ側壁面 30bがシユラウド側へ接近することにより、上述 した傾斜平面 20と略同様の作用を有する傾斜領域が形成されている。 [0028] Even if such a configuration is adopted, in the shroud side inclined portion 33 of the diffuser passage 30, the hub side wall surface 30b is downstream of the parallel portion 32 that is a portion parallel to the normal direction of the impeller outlet cross section. An inclined region approaching the shroud side is provided at a position on the side. That is, when the hub side wall surface 30b of the shroud-side inclined portion 33 approaches the shroud side, an inclined region having substantially the same function as the inclined plane 20 described above is formed.
このため、傾斜平面 20と同様の傾斜平面となるハブ側壁面 30bにより、ハブ側壁面 30bの壁面近傍に発生した低速領域の気流は半径方向の速度成分が増大するので 、ディフューザ通路 30内においては、半径方向の速度分布が均一化して局所的な 剥離を発生しにくくなる。 For this reason, the hub side wall surface 30b having an inclined plane similar to the inclined plane 20 increases the velocity component in the radial direction in the low speed region generated near the wall surface of the hub side wall surface 30b. In addition, the velocity distribution in the radial direction becomes uniform, and local peeling is less likely to occur.
従って、サージ流量の低減が可能になるため遠心圧縮機の作動範囲を広げるワイ ドレンジィ匕を達成でき、特に、ベーンレスディフューザを備えている小型の遠心圧縮 機に広い圧縮機動作範囲が要求される場合に適用すれば、ワイドレンジ化を容易に 達成できる。 Therefore, it is possible to reduce the surge flow rate and achieve a wide range that expands the operating range of the centrifugal compressor. In particular, a small centrifugal compressor equipped with a vaneless diffuser requires a wide compressor operating range. If applied to the case, wide range can be easily achieved.
[0029] このように、ディフューザ通路 15のハブ側壁面 15aには、インペラ出口断面の法線 方向と平行な部分の下流側となる位置に、シュラウド側へ接近する傾斜領域が設けら れているので、ハブ側壁面 15aに発生する低速領域の半径方向速度が増大し、ディ フューザ通路 15内の半径方向速度分布が均一化する。従って、ディフューザ通路 1 5のディフューザ出口 18付近では、壁面からの局所的な気流の剥離を生じに《なる ので、サージ流量の低減が可能になって圧縮機作動範囲を広げるワイドレンジィ匕を 達成できる。 [0029] In this manner, the hub side wall surface 15a of the diffuser passage 15 is provided with an inclined region that approaches the shroud side at a position downstream of the portion parallel to the normal direction of the impeller outlet cross section. Therefore, the radial speed in the low speed region generated on the hub side wall surface 15a increases, and the radial speed distribution in the diffuser passage 15 becomes uniform. Therefore, in the vicinity of the diffuser outlet 18 in the diffuser passage 15, local air flow separation from the wall surface occurs, so that the surge flow can be reduced and a wide range operation that widens the compressor operating range is achieved. it can.
なお、本発明は上述した実施形態に限定されるものではなぐ本発明の要旨を逸 脱しな 、範囲内にお 、て適宜変更することができる。 It should be noted that the present invention is not limited to the above-described embodiment, and can be appropriately changed within the scope without departing from the gist of the present invention.
Claims
Priority Applications (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| EP07714007A EP2072834A1 (en) | 2006-09-21 | 2007-02-09 | Centrifugal compressor |
| US11/989,241 US20100129209A1 (en) | 2006-09-21 | 2007-02-09 | Centrifugal Compressor |
Applications Claiming Priority (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2006-255383 | 2006-09-21 | ||
| JP2006255383A JP2008075536A (en) | 2006-09-21 | 2006-09-21 | Centrifugal compressor |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| WO2008035465A1 true WO2008035465A1 (en) | 2008-03-27 |
Family
ID=39200296
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| PCT/JP2007/052391 Ceased WO2008035465A1 (en) | 2006-09-21 | 2007-02-09 | Centrifugal compressor |
Country Status (6)
| Country | Link |
|---|---|
| US (1) | US20100129209A1 (en) |
| EP (1) | EP2072834A1 (en) |
| JP (1) | JP2008075536A (en) |
| KR (1) | KR20080042073A (en) |
| CN (1) | CN101341341A (en) |
| WO (1) | WO2008035465A1 (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US20160317766A1 (en) * | 2009-04-29 | 2016-11-03 | Fisher & Paykel Healthcare Limited | Fan unit with improved surge characteristics |
| CN115038878A (en) * | 2020-01-07 | 2022-09-09 | 涡轮增压系统瑞士有限公司 | Outflow region of a compressor, compressor having an outflow region of said type and turbocharger having a compressor |
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| JP4969433B2 (en) * | 2007-12-19 | 2012-07-04 | 三菱重工業株式会社 | Centrifugal compressor |
| JP5233436B2 (en) * | 2008-06-23 | 2013-07-10 | 株式会社日立プラントテクノロジー | Centrifugal compressor with vaneless diffuser and vaneless diffuser |
| FR2937385B1 (en) | 2008-10-17 | 2010-12-10 | Turbomeca | DIFFUSER WITH AUBES A ORIFICES |
| JP5905268B2 (en) * | 2012-01-17 | 2016-04-20 | 三菱重工業株式会社 | Centrifugal compressor |
| US9303561B2 (en) | 2012-06-20 | 2016-04-05 | Ford Global Technologies, Llc | Turbocharger compressor noise reduction system and method |
| US10337529B2 (en) | 2012-06-20 | 2019-07-02 | Ford Global Technologies, Llc | Turbocharger compressor noise reduction system and method |
| US10280936B2 (en) | 2012-07-06 | 2019-05-07 | Toyota Jidosha Kabushiki Kaisha | Compressor for supercharger of internal combustion engine |
| JP6119862B2 (en) | 2013-08-06 | 2017-04-26 | 株式会社Ihi | Centrifugal compressor and turbocharger |
| WO2015076102A1 (en) * | 2013-11-22 | 2015-05-28 | 株式会社Ihi | Centrifugal compressor and supercharger |
| GB2531029B (en) * | 2014-10-07 | 2020-11-18 | Cummins Ltd | Compressor and turbocharger |
| CN104948504A (en) * | 2015-07-10 | 2015-09-30 | 南阳新威机电有限公司 | Electrical system and centrifugal pump thereof |
| DE102016217446A1 (en) * | 2016-09-13 | 2018-03-15 | Bosch Mahle Turbo Systems Gmbh & Co. Kg | loader |
| WO2018179100A1 (en) * | 2017-03-28 | 2018-10-04 | 三菱重工エンジン&ターボチャージャ株式会社 | Centrifugal compressor and turbocharger |
| DE102017127758A1 (en) * | 2017-11-24 | 2019-05-29 | Man Diesel & Turbo Se | Centrifugal compressor and turbocharger |
| US10851801B2 (en) * | 2018-03-02 | 2020-12-01 | Ingersoll-Rand Industrial U.S., Inc. | Centrifugal compressor system and diffuser |
| JP7011502B2 (en) * | 2018-03-20 | 2022-01-26 | 本田技研工業株式会社 | Centrifugal compressor pipe diffuser |
| WO2019193683A1 (en) * | 2018-04-04 | 2019-10-10 | 三菱重工エンジン&ターボチャージャ株式会社 | Centrifugal compressor and turbocharger comprising said centrifugal compressor |
| US10823195B2 (en) * | 2018-04-17 | 2020-11-03 | Pratt & Whitney Canada Corp. | Diffuser pipe with non-axisymmetric end wall |
| CN113785111B (en) * | 2019-06-05 | 2024-07-05 | 三菱重工发动机和增压器株式会社 | Vortex structure of centrifugal compressor and centrifugal compressor |
| JP2021011828A (en) * | 2019-07-04 | 2021-02-04 | 三菱重工業株式会社 | Multistage centrifugal compressor |
| DE112020007267T5 (en) * | 2020-09-07 | 2023-03-30 | Mitsubishi Heavy Industries Engine & Turbocharger, Ltd. | Compressor housing and centrifugal compressor |
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| CN115038878A (en) * | 2020-01-07 | 2022-09-09 | 涡轮增压系统瑞士有限公司 | Outflow region of a compressor, compressor having an outflow region of said type and turbocharger having a compressor |
Also Published As
| Publication number | Publication date |
|---|---|
| JP2008075536A (en) | 2008-04-03 |
| KR20080042073A (en) | 2008-05-14 |
| EP2072834A1 (en) | 2009-06-24 |
| CN101341341A (en) | 2009-01-07 |
| US20100129209A1 (en) | 2010-05-27 |
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