JPH0737802B2 - Fluid oscillation element - Google Patents
Fluid oscillation elementInfo
- Publication number
- JPH0737802B2 JPH0737802B2 JP61300911A JP30091186A JPH0737802B2 JP H0737802 B2 JPH0737802 B2 JP H0737802B2 JP 61300911 A JP61300911 A JP 61300911A JP 30091186 A JP30091186 A JP 30091186A JP H0737802 B2 JPH0737802 B2 JP H0737802B2
- Authority
- JP
- Japan
- Prior art keywords
- vortex chamber
- vortex
- flow
- jet
- fluid
- 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.)
- Expired - Lifetime
Links
Landscapes
- Nozzles (AREA)
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。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a fluid oscillating element used for a jetting nozzle of a washing device or a sprinkler for washing dishes and a human body by jetting washing water.
従来の技術 従来の発振素子を第5図に示す。この素子は供給流路1
7、供給ノズル18、前記供給ノズル18下流両側に側壁1
9、20、側壁端部に設けられたつめ21、22と上下の出力
路23、24、及び大気連通口25、26とで構成されている。2. Related Art A conventional oscillator is shown in FIG. This element is the supply channel 1
7, supply nozzle 18, side wall 1 on both sides of the supply nozzle 18 downstream
9 and 20, claws 21 and 22 provided at the end portions of the side walls, upper and lower output paths 23 and 24, and atmosphere communication ports 25 and 26.
上記構成に於て供給流路17より流入した流体は供給ノズ
ル18より噴出する。この噴流は、つめ21、22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21によって分流され、下側の渦
室へ流入し、下側の渦の回転エネルギー、内圧などが増
す。一方上側の渦室内の流体はつめ22と噴流との隙間か
ら流出し、噴流と共に出力路23へ導かれる。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24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。大
気連通口は渦室圧をほぼ大気圧に等しくする働きをす
る。In the above structure, the fluid flowing from the supply passage 17 is ejected from the supply nozzle 18. This jet is split by the pawls 21 and 22. If the jet flow is bent downward, part of the jet flow is split by the lower pawl 21 and flows into the lower vortex chamber, so that the rotational energy and internal pressure of the lower vortex increase. On the other hand, the fluid in the upper vortex chamber flows out from the gap between the claw 22 and the jet flow and is guided to the output path 23 together with the jet flow. Therefore, the rotational energy of the upper vortex, the internal pressure, etc. are reduced, and the jet flow is coupled with the rotational energy of the lower vortex, the internal pressure, etc.
It is bent upward on the opposite side and flows out from the output path 24. The above states are repeated alternately, and oscillation is caused. The atmosphere communication port functions to make the vortex chamber pressure almost equal to atmospheric pressure.
上記従来の発振素子では、発振周波数は基本的には渦室
の容積により決まる。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の低周波発振
は非常にむずかしい。又、2つの出力路からの噴射のた
め洗浄、散水用の均一な噴射を要するノズル用素子とし
ては適さない。In the above conventional oscillator, the oscillation frequency is basically determined by the volume of the vortex chamber. In the case of incompressible fluid such as liquid, low frequency oscillation is performed. In particular, it is very difficult to oscillate a low frequency of a small oscillating element used for a nozzle of a cleaning device. Further, since the injection is performed from the two output paths, it is not suitable as a nozzle element that requires uniform injection for cleaning and water sprinkling.
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、流体発振素子は上向きに
形成した噴出口を有する流体素子本体と前記噴出口下部
に左右の側壁よりなる出力流路と、大気連通口を有した
渦室と、供給ノズルを順次形成し、前記渦室は、流れに
平行な成分の長さを流れに直角な成分の長さより長くす
ると共に、前記渦室に設けた大気連通口は、渦室の流れ
に平行な成分の長さ中心と同等、又は、下方に位置した
ものである。DISCLOSURE OF THE INVENTION Problems to be Solved by the Invention In order to solve the above-mentioned problems, a fluid oscillation element has a fluid element body having an ejection port formed upward, an output flow path composed of left and right side walls below the ejection port, and air communication. A vortex chamber having a mouth and a supply nozzle are sequentially formed, and the vortex chamber has a length of a component parallel to the flow longer than a length of a component perpendicular to the flow and an atmosphere communication port provided in the vortex chamber. Is located at or below the center of the length of the component parallel to the flow in the vortex chamber.
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がフィードバックされ、
生ずる噴流の左右の渦の回転エネルギーや、渦室内にお
いて主噴流によって渦室から流出する空気量と大気連通
口から渦室内に流入する空気量との差による渦室内圧の
変化で自己発振を起こすのである。この発振において、
渦室内での回転渦に含まれる空気量を多くし、空気の圧
縮性効果を利用し、発振の安定化と、交互に切り換る時
間を長くして自己発振周期を長くさせるものである。The jet energy injected from the supply nozzle of the action element is fed back by the rotational energy of the vortices on both sides of the jet generated in the vortex chamber.
Self-oscillation occurs due to the rotational energy of the left and right vortices of the jet flow and the change in vortex chamber pressure due to the difference between the amount of air flowing out of the vortex chamber due to the main jet in the vortex chamber and the amount of air flowing into the vortex chamber from the atmosphere communication port. Of. In this oscillation,
The amount of air contained in the rotating vortex in the vortex chamber is increased, the compressibility effect of air is utilized, the oscillation is stabilized, and the switching time is alternately lengthened to lengthen the self-oscillation cycle.
渦流の噴流に平行な長い成分は渦室内の圧縮効果で噴流
偏向を大きくし、逆に噴流に直角な成分短縮で渦流の壁
面接触流を少なくし、流体エネルギーロスを少なくな
る。A long component parallel to the jet of the vortex increases the deflection of the jet due to the compression effect in the vortex chamber, and conversely shortens the component perpendicular to the jet to reduce the wall contact flow of the vortex and reduce the fluid energy loss.
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4図
に基づいて説明する。Embodiment An embodiment of the fluid oscillating device of the present invention will be described below with reference to FIGS. 1 to 4.
第1図において、流体発振素子1は素子基盤2、上板
3、パッキン4の積層構造で、素子基盤2には供給流路
管5が取り付けてある。In FIG. 1, the fluid oscillation element 1 has a laminated structure of an element base 2, an upper plate 3 and a packing 4, and a supply flow path 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7に対し、直角に取り付けてある。8、9は供給ノ
ズル7の下流に位置し外部に連通する大気連通口10、11
を有し下流端が絞り部12形状の上下の渦室、13、14は絞
り部12の下流両側に設けた側壁、15は出力路、16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。
又、渦室8、9は、流れに平行な成分の長さを流れに直
角な成分の長さより長い、大気連通口、10、11は、渦室
の流れに平行な成分の長さ中心と同等、又は、上流側に
位置している。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 a right angle to the supply nozzle 7. 8 and 9 are atmosphere communication ports 10 and 11 which are located downstream of the supply nozzle 7 and communicate with the outside.
And the downstream end has upper and lower vortex chambers in the shape of the throttle portion 12, 13 and 14 are side walls provided on both sides of the downstream portion of the throttle portion 12, 15 is an output path, and 16 is formed at the downstream opening end of the side walls 13 and 14. It is a spout.
Further, the vortex chambers 8 and 9 make the length of the component parallel to the flow longer than the length of the component perpendicular to the flow, and 10 and 11 are the center of the length of the component parallel to the flow of the vortex chamber. Equivalent or located upstream.
第3図は素子の作動状態を示し、Fは噴出流、V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。FIG. 3 shows the operating state of the element. F is a jet flow, and V is a vortex generated in the vortex chambers 8 and 9 which is attracted by the main jet.
第4図は素子への液体供給が停止された時の状態を示
し、Lは液面であり、Aは気体層である。FIG. 4 shows a state when the liquid supply to the element is stopped, L is the liquid surface, and A is the gas layer.
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 described.
供給流路6に流入した液体は供給流路から供給ノズル7
へ流入する。この噴射流は渦室8、9の左右の圧力差に
より偏向される。今仮に、噴流の不安定現象により左側
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。主噴流Fは噴流の誘引作用により、主噴流Fの
両側に渦を形成すると共に、左側へ偏向する。主噴流F
の偏向により主噴流Fと絞り部間との距離が小さくな
り、主噴流Fと共に流出する空気量が減少し、渦室8の
圧力は時間と共に上昇する。The liquid that has flowed into the supply channel 6 is supplied from the supply channel to the supply nozzle 7
Flow into. This jet flow is deflected by the pressure difference between the left and right of the vortex chambers 8 and 9. Now, assume that the pressure in the left vortex chamber 8 is low and the pressure in the right vortex chamber 9 is high due to the unstable phenomenon of the jet flow. Due to the attraction of the main jet F, the main jet F forms vortices on both sides of the main jet F and is deflected to the left. Main jet F
Due to the deflection, the distance between the main jet F and the throttle portion becomes smaller, the amount of air flowing out together with the main jet F decreases, and the pressure in the vortex chamber 8 rises with time.
他方、右側の渦室9では、主噴流Fと絞り部間との距離
が大きくなり、主噴流Fと共に流出する空気量が増加
し、渦室9の圧力は時間と共に低下する。この圧力変化
速度は、主噴流Fと共に流出する空気量と大気から渦室
へ流入する空気量との割合によって決まる。On the other hand, in the vortex chamber 9 on the right side, the distance between the main jet F and the throttle portion increases, the amount of air flowing out together with the main jet F increases, and the pressure in the vortex chamber 9 decreases with time. This pressure change rate is determined by the ratio of the amount of air flowing out together with the main jet F and the amount of air flowing into the vortex chamber from the atmosphere.
左右の渦室の圧力変化が進行し右側の圧力が左側の圧力
より低くなると渦室差圧は左側が高く、右側は低くな
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。渦流の噴流に平行な長い成分は
渦室圧の圧縮性効果を高め噴流の偏向を大きくし、逆に
噴流に直角な成分短縮は渦流の壁面に発生する損失が少
なくなる。以下、左側偏向の場合に説明したと同じ動作
が右側偏向時にも起こる。When the pressure change in the left and right vortex chambers progresses and the right side pressure becomes lower than the left side pressure, the vortex chamber differential pressure becomes high on the left side and becomes low on the right side. Due to the pressure difference between the vortex chambers, the flow deflected to the left is deflected to the right. A long component parallel to the jet of the vortex increases the compressibility effect of the vortex chamber pressure and increases the deflection of the jet, and conversely, shortening the component perpendicular to the jet reduces the loss generated on the wall surface of the vortex. Hereinafter, the same operation as described in the case of the leftward deflection also occurs during the rightward deflection.
発振噴射が終ると素子内の液体は、大気連通口から大気
中へ流出し、液面は第4図Lで示す位置まで下る。逆に
空気層は第4図Aのようにほぼ渦室全体となる。この空
気は、次に液体が供給ノズルから噴射し発振が行われ時
に、前述したように渦室内で旋回し、渦室圧変化に影響
をおよぼす。即ち、渦室中の多量の空気の圧縮性により
渦室の圧力変化が緩慢となり、自己発振の周期が長くな
る。When the oscillating injection is finished, the liquid in the element flows out into the atmosphere through the atmosphere communication port, and the liquid level drops to the position shown in FIG. 4L. On the contrary, the air layer is almost the entire vortex chamber as shown in FIG. 4A. This air swirls in the vortex chamber as described above when the liquid is subsequently jetted from the supply nozzle and oscillates, and affects the vortex chamber pressure change. That is, due to the compressibility of a large amount of air in the vortex chamber, the pressure change in the vortex chamber becomes slow and the self-oscillation cycle becomes long.
発明の効果 1、渦室内の渦流に含まれる気泡の効果によって発振周
期が長い、低周波発振が可能となって、噴流の側壁への
付着が確実となる。その結果、飛散が少ない発振噴流が
得られ、この発振素子を洗浄等に使用した場合、高い洗
浄効果が得られる。Advantageous Effects of Invention 1. Due to the effect of bubbles included in the vortex in the vortex chamber, low-frequency oscillation with a long oscillation period is possible, and the adhesion of the jet to the side wall is ensured. As a result, an oscillating jet with little scattering is obtained, and when this oscillating element is used for washing or the like, a high washing effect is obtained.
2、素子内に滞留する水が少なくなって、停止後の再使
用に際し、残留液分の処理作動が少なくて済む、又、残
留液の凍結による破損防止効果がある。2. The amount of water retained in the element is reduced, and when the device is reused after being stopped, it is possible to reduce the treatment operation of the residual liquid component and to prevent damage due to freezing of the residual liquid component.
3.渦室圧の噴流に圧縮性効果が高まると共に、渦流のエ
ネルギー損失が減少し発振が安定する。3. The compressive effect is enhanced in the jet of vortex chamber pressure, the energy loss of the vortex is reduced, and oscillation is stabilized.
第1図は本発明の一実施例を示す流体発振素子の斜視
図、第2図は同流体発振素子の流路パターン図、第3
図、第4図 は同流体発振素子の作動を示す作動
状態図、第5図は従来の発振素子の流路パターン図であ
る。 6……供給流路、7……供給ノズル、8、9……渦室、
10、11……大気連通口、12……絞り部、13、14……側
壁、15……出力路、16……出力口。FIG. 1 is a perspective view of a fluid oscillating device showing an embodiment of the present invention, FIG. 2 is a flow path pattern diagram of the same fluid oscillating device, and FIG.
4 and 5 are operation state diagrams showing the operation of the fluid oscillating device, and FIG. 5 is a flow path pattern diagram of the conventional oscillating device. 6 ... Supply channel, 7 ... Supply nozzle, 8, 9 ... Vortex chamber,
10, 11 …… Atmosphere communication port, 12 …… Throttle section, 13,14 …… Sidewall, 15 …… Output path, 16 …… Output port.
Claims (1)
本体と前記噴出口下部に左右の側壁よりなる出力流路
と、大気連通口を有した渦室と、供給ノズルを順次形成
し、前記渦室は、流れに平行な成分の長さを流れに直角
な成分の長さより長くすると共に、前記渦室に設けた大
気連通口は、渦室の流れに平行な成分の長さ中心と同
等、又は、上方に位置した流体発振素子。1. A fluid element body having an ejection port formed upward, an output flow path consisting of left and right sidewalls at the lower portion of the ejection port, a vortex chamber having an atmosphere communication port, and a supply nozzle are sequentially formed. In the vortex chamber, the length of the component parallel to the flow is made longer than the length of the component perpendicular to the flow, and the atmosphere communication port provided in the vortex chamber is equal to the center of the length of the component parallel to the flow of the vortex chamber. Or a fluid oscillation element located above.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61300911A JPH0737802B2 (en) | 1986-12-17 | 1986-12-17 | Fluid oscillation element |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61300911A JPH0737802B2 (en) | 1986-12-17 | 1986-12-17 | Fluid oscillation element |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS63152703A JPS63152703A (en) | 1988-06-25 |
| JPH0737802B2 true JPH0737802B2 (en) | 1995-04-26 |
Family
ID=17890610
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP61300911A Expired - Lifetime JPH0737802B2 (en) | 1986-12-17 | 1986-12-17 | Fluid oscillation element |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0737802B2 (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5826282A (en) * | 1994-03-09 | 1998-10-27 | Matsushita Electric Industrial Co., Ltd. | Sanitary cleaning apparatus |
| CN107794990A (en) * | 2017-10-26 | 2018-03-13 | 江苏大学 | A kind of mixed gas pulse cleaning device for intelligent closestool |
| CN108240023A (en) * | 2017-12-18 | 2018-07-03 | 江苏大学 | A kind of water discharge device for toilet seat |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5210135B2 (en) * | 1973-05-21 | 1977-03-22 | ||
| JPS6141004A (en) * | 1984-07-31 | 1986-02-27 | Matsushita Electric Ind Co Ltd | Fluid oscillating device |
-
1986
- 1986-12-17 JP JP61300911A patent/JPH0737802B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS63152703A (en) | 1988-06-25 |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| EXPY | Cancellation because of completion of term |