JPS63158305A - Fluid oscillation element - Google Patents
Fluid oscillation elementInfo
- Publication number
- JPS63158305A JPS63158305A JP30413686A JP30413686A JPS63158305A JP S63158305 A JPS63158305 A JP S63158305A JP 30413686 A JP30413686 A JP 30413686A JP 30413686 A JP30413686 A JP 30413686A JP S63158305 A JPS63158305 A JP S63158305A
- Authority
- JP
- Japan
- Prior art keywords
- oscillation
- jet
- pressure
- vortex chamber
- vortex
- 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.)
- Granted
Links
- 230000010355 oscillation Effects 0.000 title claims abstract description 30
- 239000012530 fluid Substances 0.000 title claims description 17
- 238000006073 displacement reaction Methods 0.000 claims description 12
- 238000012856 packing Methods 0.000 claims description 9
- 238000007789 sealing Methods 0.000 claims 1
- 238000004140 cleaning Methods 0.000 abstract description 6
- 230000000694 effects Effects 0.000 abstract description 5
- 238000009792 diffusion process Methods 0.000 abstract description 2
- 238000002347 injection Methods 0.000 abstract 1
- 239000007924 injection Substances 0.000 abstract 1
- 230000007423 decrease Effects 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 239000007788 liquid Substances 0.000 description 2
- 230000029058 respiratory gaseous exchange Effects 0.000 description 2
- 239000007921 spray Substances 0.000 description 2
- 238000005406 washing Methods 0.000 description 2
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 2
- 239000003795 chemical substances by application Substances 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 238000005507 spraying Methods 0.000 description 1
- 239000004575 stone Substances 0.000 description 1
- 239000000758 substrate Substances 0.000 description 1
Landscapes
- Special Spraying Apparatus (AREA)
- Nozzles (AREA)
Abstract
Description
【発明の詳細な説明】
産業上の利用分野
本発明は、洗浄水の噴射により、食器や人体を洗浄する
洗浄装置や散水装置の噴射ノズルに利用される流体発振
素子に関するものである。DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a fluid oscillation element used in a spray nozzle of a washing device or a water spray device that washes tableware or the human body by spraying washing water.
従来の技術
従来の発振素子を第6図に示す。この素子は供給流路2
1、供給ノズル22、前記供給ノズル22下流両側に側
壁23.24、側壁端部に設けられたつめ25.26と
上下の出力路27.28とで構成されている。Prior Art A conventional oscillation element is shown in FIG. This element is the supply channel 2
1. It consists of a supply nozzle 22, side walls 23.24 on both sides downstream of the supply nozzle 22, pawls 25.26 provided at the ends of the side walls, and upper and lower output paths 27.28.
上記構成に放て供給流路21より流入した流体は供給ノ
ズル22より噴出する。この噴流は、つめ25.26に
より分流される。いま仮に噴流が下側に曲げられたとす
ると、噴流の一部は、下側のつめ25によって分流され
、下側の部室へ流入し、下側の渦の回転エネルギー、内
圧などが増す。The fluid flowing into the above-mentioned structure through the supply channel 21 is ejected from the supply nozzle 22. This jet is diverted by pawls 25,26. If the jet is now bent downward, part of the jet will be diverted by the lower pawl 25 and flow into the lower chamber, increasing the rotational energy, internal pressure, etc. of the lower vortex.
−力士側の渦室内の流体はつめ26と噴流との隙間から
流出し、噴流と共に出力路28へ専かれる。- The fluid in the vortex chamber on the sumo wrestler side flows out from the gap between the pawl 26 and the jet, and is directed to the output path 28 together with the jet.
従って、上側の渦の回転エネルギー、内圧などが減少し
、下側の渦の回転エネルギー、内圧などの増加と相まっ
て噴流は、反対側の上側に曲げられて、出力路28から
流出する。以上の状態が交互に繰返され、発振を起すこ
とになる。Therefore, the rotational energy, internal pressure, etc. of the upper vortex are reduced, and combined with the increase in the rotational energy, internal pressure, etc. of the lower vortex, the jet is bent upward on the opposite side and flows out from the output path 28. The above conditions are repeated alternately, causing oscillation.
上記従来の発振素子では、発振周波数は基本的には渦室
の容積によシ決まる。液体等の非圧縮性流体の場合には
低周波発振を行なわすことがこんなんである。特に、洗
浄装置のノズル等に使用する小形発振素子での低周波発
振は非常にむすかしい0
発明が解決しようとする問題点
上記問題点を解決するために、自己発振の圧力変化を決
定する渦室部の1部に圧力に応じ変位する変位壁面を設
け、発振時に渦室容積が変化する構成とし、この容積変
化により発振周期を長くし、低周波発振を可能にしよう
とするものである。In the conventional oscillation element described above, the oscillation frequency is basically determined by the volume of the vortex chamber. In the case of incompressible fluids such as liquids, this is how low frequency oscillations occur. In particular, it is extremely difficult to generate low-frequency oscillations with small oscillation elements used in cleaning equipment nozzles, etc.Problems to be Solved by the InventionIn order to solve the above problems, we have developed A part of the chamber is provided with a displacement wall surface that displaces in response to pressure, and the volume of the vortex chamber changes during oscillation.This volume change lengthens the oscillation period and enables low-frequency oscillation.
作 用
素子の供給ノズルから噴射する噴流は、渦室で発生する
噴流両側の渦の回転エネルギーや内圧の差によシ偏向さ
れ、更に、渦室下流の出力路の側壁に付着し、噴出口よ
り噴射される。この噴流偏向は、渦室部において噴流の
1部がフィードバンクされ、噴流左右の渦の回転エネル
ギーや内圧の差が交互に変えられ、自己発振を起こすの
である。The jet jet ejected from the supply nozzle of the working element is deflected by the difference in internal pressure and the rotational energy of the vortices on both sides of the jet generated in the vortex chamber, and is further attached to the side wall of the output path downstream of the vortex chamber, and the jet nozzle is deflected by the jet nozzle. More sprayed. In this jet deflection, part of the jet is fed banked in the vortex chamber, and the difference in rotational energy and internal pressure between the left and right vortices of the jet is alternately changed, causing self-oscillation.
この時の内圧変化を圧力により変位壁の効果で遅らせる
ことにより、交互に切換る時間を長くして、自己発振周
期を長くさせるのである。By delaying the internal pressure change at this time by the effect of the displacement wall due to pressure, the time for alternate switching is lengthened, and the self-oscillation period is lengthened.
実施例
以下本発明の流体発振素子の一実施例を第1図〜第7図
に基づいて説明する。EXAMPLE An example of the fluid oscillation device of the present invention will be described below with reference to FIGS. 1 to 7.
第1図において、流体発振素子1は、素子基盤2、上板
3、パツキン4の積層構造で、素子基盤2には供給流路
管5が取り付けである。In FIG. 1, a fluid oscillation element 1 has a laminated structure of an element base 2, an upper plate 3, and a packing 4, and a supply channel pipe 5 is attached to the element base 2.
第2図は素子基盤2に形成された流路パターンを示し、
6は供給流路、7は供給ノズル、供給流路6は供給ノズ
ルに対し、直角に取シ付けである。FIG. 2 shows a flow path pattern formed on the element substrate 2,
6 is a supply channel, 7 is a supply nozzle, and the supply channel 6 is attached at right angles to the supply nozzle.
8.9は供給ノズル7の下流に位置し、外部に連通ずる
大気連通口10.11を有し下流端が絞り部12、形状
の左右の渦室、13.14は絞り部12の下流両側に設
けた左右の側壁、15は前記側壁13.14の下流開口
端で形成された噴出口である。側壁13.14は噴射流
の利用目的に応じある程度の広がり角を有している。8.9 is located downstream of the supply nozzle 7, has an atmosphere communication port 10.11 that communicates with the outside, the downstream end is the constriction part 12, left and right swirl chambers in shape, and 13.14 are the downstream sides of the constriction part 12. The left and right side walls 15 are provided at the downstream opening ends of the side walls 13. The side walls 13, 14 have a certain degree of divergence depending on the purpose of use of the jet stream.
第3図は上板3の平面図でパツキン4のずれを防止する
溝部を形成する段差16を有している。FIG. 3 is a plan view of the upper plate 3, which has a step 16 forming a groove to prevent the packing 4 from slipping.
第4図はパツキン4の平面図で、左右の渦室8.9部の
1部、又は全体に相当する位置に取付けられ、渦室の内
圧により変位する変位壁面17.18を有している。FIG. 4 is a plan view of the packing 4, which is attached at a position corresponding to a part or the whole of the left and right vortex chambers 8.9, and has displacement wall surfaces 17.18 that are displaced by the internal pressure of the vortex chambers. .
第5図はパツキン4の変位壁面17.18の断面を示し
、変位壁面17.18はパツキン4の他の部分に対し薄
肉構造になっている。FIG. 5 shows a cross section of the displacement wall surface 17.18 of the packing 4, and the displacement wall surface 17.18 has a thinner wall structure than the other parts of the packing 4. As shown in FIG.
第6図、第7図は素子の作動状態を示し、Fiは主噴流
、Foは噴出流、VL、VRは主噴流により誘引され渦
室8.9内に発生する渦である。第7図19.20は変
位壁面17.18が部室圧により変位したときの状態を
示す。6 and 7 show the operating state of the element, where Fi is the main jet flow, Fo is the jet flow, and VL and VR are vortices induced by the main jet flow and generated in the vortex chamber 8.9. FIG. 7 19.20 shows the situation when the displacement wall 17.18 is displaced by the chamber pressure.
上記構成に基づく作動について説明する。The operation based on the above configuration will be explained.
供給流路6に流入した流体は、供給ノズル7がら渦室8
.9部へ噴出する。この噴射流は左右の渦室8.9の圧
力差により偏向される。今仮に、左側の渦室8の圧力が
低く、右側の渦室9の圧力が高いと仮定する。この場合
主噴流Fiは左側に偏向され、絞り部12の左側に当り
、更に、出力路の左側の側壁13に付着偏向されて、噴
出口15から噴出する(第6図F0)。この時、絞り部
に当たり分流した1部の流れは左側渦室8の壁に沿って
流れ渦VLを形成する。この渦VLは渦室8の圧力を徐
々に高める。The fluid flowing into the supply flow path 6 flows through the supply nozzle 7 into the vortex chamber 8
.. Gushes to part 9. This jet stream is deflected by the pressure difference between the left and right vortex chambers 8.9. Assume now that the pressure in the left vortex chamber 8 is low and the pressure in the right vortex chamber 9 is high. In this case, the main jet Fi is deflected to the left, hits the left side of the constriction part 12, is further deflected by adhering to the left side wall 13 of the output path, and is ejected from the jet nozzle 15 (FIG. 6 F0). At this time, the part of the flow that hits the constriction part and is divided flows along the wall of the left vortex chamber 8 and forms a vortex VL. This vortex VL gradually increases the pressure in the vortex chamber 8.
他方、右側の渦室9の流体は噴流に誘引され噴流と共に
排出され、渦室内の圧力は低下する。この圧力低下が進
み右側の渦室圧が、左側の渦室圧より低くなると渦室差
圧として、右側が高く、左側が低くなる。この渦室間の
差圧により、左側に偏向されていた流れは右側に偏向さ
れる。石側偏向が完了すると、前記左側偏向時に説明し
たと同じ動作が右側偏向時にも起こる。このような偏向
動作が繰返されて自己発振が起こる。一方、パツキン4
に設けられた変位壁面は、左側偏向で左側渦室8の圧力
が低く、右側渦室9の圧力が高い場合は、左側変位壁が
第7図点線19の位置に、右側変位壁が第7図実線18
の位置となる。この結果、各渦室8.9の容積が変化し
たことになり、この変化に応じ渦室内の圧力変化時間が
長くなって、自己発振周期が長くなる。On the other hand, the fluid in the right vortex chamber 9 is attracted by the jet and discharged together with the jet, and the pressure inside the vortex chamber decreases. As this pressure decrease progresses and the vortex chamber pressure on the right side becomes lower than the vortex chamber pressure on the left side, the vortex chamber differential pressure becomes higher on the right side and lower on the left side. This differential pressure between the vortex chambers causes the flow that was deflected to the left to be deflected to the right. Once the stone side deflection is complete, the same actions described for the left side deflection occur during the right side deflection. Such a deflection operation is repeated and self-oscillation occurs. On the other hand, Patsukin 4
When the pressure in the left side vortex chamber 8 is low and the pressure in the right side vortex chamber 9 is high due to left side deflection, the left side displacement wall is located at the position indicated by the dotted line 19 in Figure 7, and the right side displacement wall is located at the position indicated by the dotted line 19 in Figure 7. Figure solid line 18
The position will be . As a result, the volume of each vortex chamber 8.9 has changed, and in accordance with this change, the pressure change time in the vortex chamber becomes longer, and the self-oscillation period becomes longer.
大気連通口10.11は渦室8.9と大気との差圧に応
じ、渦室内に大気を萼大したり、逆に、渦室内の液体を
外部へ放出する呼吸作用をしている。この呼吸作用によ
り自己発振の安定性が兄進されている。The atmosphere communication port 10.11 has a breathing function that expands the atmosphere inside the vortex chamber, or conversely releases the liquid inside the vortex chamber to the outside, depending on the pressure difference between the vortex chamber 8.9 and the atmosphere. This breathing action improves the stability of self-oscillation.
発明の効果
1、 以上のように、フィードバック流路等の信号路を
有しない流路構成であるだめ、流路がシンプルとなる。Effect 1 of the invention: As described above, since the flow path configuration does not have a signal path such as a feedback flow path, the flow path becomes simple.
そのため、信号路のつまシによるトラブルがなく、作動
が安定すると共に、素子製造が容易となる。Therefore, there are no troubles caused by jams in the signal path, the operation is stable, and the device manufacturing is facilitated.
26 噴流の発振周期が長い、低周波発振が可能にな
ることにより、噴流の側壁への付着が確実となって、噴
流の拡散が少い発振噴流となる。この結果、洗浄等に使
用した場合、洗浄効果が高まる。26 By enabling low-frequency oscillation with a long oscillation period of the jet, the jet can be reliably attached to the side wall, resulting in an oscillating jet with less jet diffusion. As a result, when used for cleaning etc., the cleaning effect is enhanced.
3、パツキンの1部を変位壁とするため、部品の共用化
ができ、信慎性が向上すると共に、低コストとなる。3. Since part of the packing is a displacement wall, parts can be shared, reliability is improved, and costs are reduced.
第1図は本発明の一実施例を示す流体発振素子の外観斜
視図、第2図は同流体発振素子の流路パターン図、第3
図は同流体発振素子上板の平面図、第4図は同流体発振
素子パツキンの平面図、第5図は同発振素子パツキンの
断面図、第6図は同流体発振素子の作動を示す状態図、
第7図は同流体発振素子の作動状態を示すパツキンの断
面図、第8図は従来の発振素子の流路パターン図である
。
4・・・・・・パツキン、6・・・・・・供給流路、7
・・・・・・供給ノズル、8.9・・・・・・渦室、1
0.11・・・・・・大気連通口、13.14・・・・
・・側壁、15・・・・・・噴出口、17.18・・・
・・・変位壁面。
代理人の氏名 弁理士 中 尾 敏 男 ほか1名第1
図
4=−パツキン
第2図
7j!13図 第4図
第5図 第6図
必 z4 22
5Z3FIG. 1 is an external perspective view of a fluid oscillation device showing an embodiment of the present invention, FIG. 2 is a flow path pattern diagram of the same fluid oscillation device, and FIG.
The figure is a plan view of the upper plate of the fluid oscillation element, Figure 4 is a plan view of the gasket of the fluid oscillation element, Figure 5 is a sectional view of the gasket of the oscillation element, and Figure 6 is a state showing the operation of the fluid oscillation element. figure,
FIG. 7 is a sectional view of a packing showing the operating state of the fluid oscillation element, and FIG. 8 is a flow path pattern diagram of a conventional oscillation element. 4...Packing, 6...Supply channel, 7
...Feed nozzle, 8.9 ... Vortex chamber, 1
0.11...Atmospheric communication port, 13.14...
...Side wall, 15... Spout, 17.18...
...displacement wall surface. Name of agent: Patent attorney Toshio Nakao and 1 other person No. 1
Figure 4=-Patsukin 2nd Figure 7j! Figure 13 Figure 4 Figure 5 Figure 6 Required z4 22 5Z3
Claims (2)
通口を有した渦室、渦室の下流に位置し左右の側壁より
なる出力路と前記渦室の一部を圧力に応じ変位する変位
壁面構成とした流体発振素子。(1) A supply channel, a supply nozzle, a vortex chamber having an atmosphere communication port downstream of the supply nozzle, an output path located downstream of the vortex chamber and consisting of left and right side walls, and a portion of the vortex chamber are displaced according to pressure. Fluid oscillation element with a displacement wall configuration.
けた特許請求の範囲第1項記載の流体発振素子。(2) The fluid oscillation element according to claim 1, wherein the displacement wall surface is provided with a thin wall portion in a part of the sealing packing.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP30413686A JPH0718447B2 (en) | 1986-12-19 | 1986-12-19 | Fluid oscillation element |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP30413686A JPH0718447B2 (en) | 1986-12-19 | 1986-12-19 | Fluid oscillation element |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS63158305A true JPS63158305A (en) | 1988-07-01 |
JPH0718447B2 JPH0718447B2 (en) | 1995-03-06 |
Family
ID=17929473
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP30413686A Expired - Lifetime JPH0718447B2 (en) | 1986-12-19 | 1986-12-19 | Fluid oscillation element |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0718447B2 (en) |
-
1986
- 1986-12-19 JP JP30413686A patent/JPH0718447B2/en not_active Expired - Lifetime
Also Published As
Publication number | Publication date |
---|---|
JPH0718447B2 (en) | 1995-03-06 |
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Legal Events
Date | Code | Title | Description |
---|---|---|---|
EXPY | Cancellation because of completion of term |