JPH0578680B2 - - Google Patents
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- Publication number
- JPH0578680B2 JPH0578680B2 JP60105090A JP10509085A JPH0578680B2 JP H0578680 B2 JPH0578680 B2 JP H0578680B2 JP 60105090 A JP60105090 A JP 60105090A JP 10509085 A JP10509085 A JP 10509085A JP H0578680 B2 JPH0578680 B2 JP H0578680B2
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- JP
- Japan
- Prior art keywords
- drive
- fluid
- diaphragm
- frequency
- space
- 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
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- Reciprocating Pumps (AREA)
Description
産業上の利用分野
この発明は気体や液体などの流体を搬送するた
めの流体駆動装置に関するものである。
従来の技術
往復運動をする駆動源を用いて気体や液体を搬
送する従来の流体駆動装置では、第6図に示すよ
うに、吸入弁2、吐出弁3が必要であるため構造
が複雑になり、安価なものを提供し難い。また往
復運動の駆動源によつているので吸入行程と吐出
行程を経ているため流量変動が大きく、流量を一
定化するためには、容量の大きな貯蓄タンク等の
平滑装置6が必要であるとともに、流量制御が難
しくなる。
また羽根車等の回転体を駆動源とする第7図に
示すような従来装置では、一定した流量を得やす
いが電動機8や羽根車7を使用するため高価であ
る。また、電動機8のロータや羽根車7が回転慣
性を有しているためこの種の流体駆動装置も流量
変化をさせる際の応答性が悪く流量制御が難し
い。また電子技術の発達した現在、高度な制御装
置と特殊な電動機を用いれば、高精度な制御がで
きるが更に高価なものになるとともに、従来のポ
ンプや送風機は構造が固定的なものであるため機
械装置への組込み勝手が悪い。
発明が解決しようとする問題点
以上に述べたように従来技術は、構造が複雑で
高価なこと、流量変動が大きいこと、制御性が悪
いこと、形状が固定的で組込み勝手が悪いことな
どの問題がある。
本発明は上記問題点に鑑みてなされたもので、
振動板を駆動源とする簡単な構成で、流量の安定
した、制御性の良い流体駆動装置を安価に提供す
ることを目的としている。
問題点を解決するための手段
本発明は上記問題点を解決するために、中空容
器の内部に振動板を設けて容積Vなる空間を形成
し、前記容積Vなる空間に臨んで外部に連通して
断面積A、長さLの駆動管を連接すると共に、前
記振動板の駆動電源周波数を前記空間Vと前記駆
動管A・Lの寸法条件によつて定まる周波数に一
致させる、周波数調節機能を有する駆動電源装置
を具備せしめて、一種のヘルムホルツの共鳴系を
構成したものである。
作用
本発明は上記構成により、中空容器内の振動板
を系の共鳴周波数で振動させることにより、駆動
管内部に被駆動流体と同じ流体のピストン運動を
発生せしめ、駆動管先端部に駆動管軸線方向の流
体流れを発生させるもので、往復運動をする振動
板を駆動源としているにもかかわらず吸入弁や吐
出弁を必要とせずに駆動管の先端から流量一定
で、しかも制御性の良好な流体流を得ることがで
きる。
実施例
第1図は本発明の一実施例を示す横断面図で、
筐体10には断面積A、長さLの駆動管12が連
接されていて外部に連通している。筐体10の内
部には振動板13がスプリング14を介して筐体
10に取付けられ、筐体10の内部は振動板13
とスプリング14によつて気密に2室に分割さ
れ、振動板を境として駆動管側に容積Vの大きな
空間11が形成される。駆動管12は空間11と
でヘルムホルツの共鳴器を形成する。振動板13
にはコイル15が固定されて永久磁石16と同心
円状に相対している。17は周波数の調節機能を
有する電源装置でコイル15に所定の周波数の電
圧で電力を供給する。
前述のように駆動管13(断面積:A、長さ:
L)は空間11(容積:V)とでヘルムホルツの
共鳴器を形成し、次式で示される周波数0Hzで共
鳴する。
INDUSTRIAL APPLICATION FIELD This invention relates to a fluid drive device for conveying fluid such as gas or liquid. BACKGROUND ART Conventional fluid drive devices that transport gas or liquid using a reciprocating drive source require a suction valve 2 and a discharge valve 3, as shown in FIG. 6, resulting in a complicated structure. , it is difficult to provide cheap products. In addition, since it is based on a reciprocating drive source, the flow rate fluctuates greatly due to the suction stroke and discharge stroke, and in order to keep the flow constant, a smoothing device 6 such as a large-capacity storage tank is required. Flow control becomes difficult. Further, in a conventional device as shown in FIG. 7 which uses a rotating body such as an impeller as a driving source, it is easy to obtain a constant flow rate, but it is expensive because it uses an electric motor 8 and an impeller 7. Further, since the rotor of the electric motor 8 and the impeller 7 have rotational inertia, this type of fluid drive device also has poor responsiveness when changing the flow rate, making it difficult to control the flow rate. In addition, with the advancement of electronic technology, highly accurate control is possible using advanced control devices and special electric motors, but they are also more expensive, and conventional pumps and blowers have fixed structures. It is difficult to integrate into mechanical equipment. Problems to be Solved by the Invention As mentioned above, the conventional technology has problems such as complicated and expensive structure, large flow rate fluctuations, poor controllability, and fixed shape that makes installation difficult. There's a problem. The present invention has been made in view of the above problems, and
The object of the present invention is to provide a fluid drive device with a simple configuration using a diaphragm as a drive source, stable flow rate, and good controllability at a low cost. Means for Solving the Problems In order to solve the above problems, the present invention provides a diaphragm inside a hollow container to form a space with a volume V, and faces the space with a volume V and communicates with the outside. drive tubes having a cross-sectional area A and a length L are connected to each other, and a frequency adjustment function is provided to match the drive power frequency of the diaphragm to a frequency determined by the dimensional conditions of the space V and the drive tubes A and L. A type of Helmholtz resonance system is constructed by providing a driving power supply device having the following characteristics. Effects With the above configuration, the present invention generates a piston motion of the same fluid as the driven fluid inside the drive tube by vibrating the diaphragm in the hollow container at the resonance frequency of the system, so that the drive tube axis is aligned at the tip of the drive tube. It generates a fluid flow in the same direction, and although it uses a reciprocating diaphragm as the drive source, it does not require suction or discharge valves and has a constant flow rate from the tip of the drive pipe, with good controllability. Fluid flow can be obtained. Embodiment FIG. 1 is a cross-sectional view showing an embodiment of the present invention.
A drive pipe 12 having a cross-sectional area A and a length L is connected to the housing 10 and communicates with the outside. A diaphragm 13 is attached to the casing 10 via a spring 14 inside the casing 10.
The chamber is airtightly divided into two chambers by a spring 14, and a space 11 with a large volume V is formed on the drive tube side with the diaphragm as a boundary. The drive tube 12 and the space 11 form a Helmholtz resonator. Vibration plate 13
A coil 15 is fixed to and faces the permanent magnet 16 concentrically. A power supply device 17 has a frequency adjustment function and supplies power to the coil 15 with a voltage at a predetermined frequency. As mentioned above, the drive tube 13 (cross-sectional area: A, length:
L) forms a Helmholtz resonator with the space 11 (volume: V), and resonates at a frequency of 0 Hz expressed by the following equation.
【化】
ここにCは流体の音速、πは円周率、αは修正
係数を示す。次にこの装置の作用について説明す
る。電源装置17によつて(1)式で定まる0の周波
数の正弦波形電圧でコイル15に電力を供給する
と、スプリング14に支持された振動板13とコ
イル15は第1図において左右の方向に0の周波
数で振動し、空間11内に圧力波を放射する。前
述のように空間11と駆動管12とで共鳴周波数
f0のヘルムホルツ共鳴系が構成されているため、
駆動管12内の流体は、図の点線で示すように柱
状流体23として、あたかも剛体であるかの様に
一体となつて振幅abで振動する。この柱状流体
23の振動運動によつて第二の駆動源が構成され
る。
直径18mm、長さが160mmの駆動管で共鳴周波数
135Hzの例では、abは約10mmであつた。柱状流体
23が図の右方向、aからbに動くとき駆動管1
2のab部分の流体は右方向に駆動される。柱状
流体23が右側最大振幅bの位置に至ると、次に
bからaの左方向の運動に変わる。柱状流体23
が左に移動するにつれて、駆動管12の入口部分
に負圧が発生するが、右方向に駆動された流体は
慣性力で、駆動管12の軸心に沿つて右方向に流
れ続ける。
その結果、駆動管12の端部に発生した負圧部
分には、駆動管12の入口端部の全円周域から、
周囲近傍の流体が流れ込む。柱状流体23が左方
向に動くにつれて、この周囲の流体も流れ込み続
ける。柱状流体23は、左側最大振幅の位置aに
到達すると、再び右方向に運動方向を変える。こ
の時周囲より流れ込んだ流体は、柱状流体23部
分に流れ込むことなく右方向に駆動され図中、曲
線Aで示すように流れ、さらにBの流れとなる。
この様子はストロボスコープと煙とで観測するこ
とが出来る。
駆動管ab部分に流れ込んだ流体が右方向に駆
動されBの流れになる段階では、駆動管12の周
囲近傍の流体は、Bの流れの粘性力により、一部
が右方向に流れるものと考えられる。この伴流の
流れの状態及び駆動管12の出力直近の流れの状
態は、観測が難しく十分には解明できていない。
以降同じ過程が繰り返されることにより、駆動
管12の軸心にそう右方向の連続的な流れが形成
される。駆動管12の軸心上、出口bの下流(右
方向)5cm位置で流速を測定すると、平均流速
3.4m/secに対して流速変動が+0.08m/secで、
脈動の少ない一定流速の右方向の流れが形成され
ていることが確認された。
この流体駆動装置は、流れを運転開始後数サイ
クルで形成することができ、非常に応答性の高い
流れを得ることが出来る。また、往復運動をする
振動板13を第一駆動源として、駆動管12内部
の柱状流体23の往復運動として形成される第二
の駆動源を直接的な駆動源としながら、脈動を吸
収する平滑装置等を用いることなく、安定した流
速の流れを得ることが出来るものである。しかも
流速や流量の変更や制御はコイル15にかける電
圧または周波数を変更、制御することによつて容
易に達成できる。
次に本発明の他の実施例について説明する。第
2図はコイル15前面の空間11の壁面部分を円
錐台形状の壁体18にしたもので、壁体18の底
面に平行に振動板13を設けてあり、頂部の面に
垂直に駆動管12が連接されている。その他の構
成及び動作は第1図の実施例と同じである。ただ
し壁体18を円錐台状にすることによつて仕事効
率を向上する効果が得られる。
第3図は第1図に示した実施例のスプリング1
4、振動板13、コイル15、永久磁石16で構
成した駆動源を圧電素子22を振動板21に接着
した構成を駆動源としたもので、より簡単な構造
のものにできる。その他の作用効果は第1図の実
施例と同じである。
また、第1図や第3図の実施例に示した駆動源
の振動系スプリング14、振動板13、コイル1
5の組合わせや、圧電素子22と振動板21とで
組合わせで構成された振動系の固有振動数を、空
間11と駆動管12とで構成されるヘルムホルツ
の共鳴器の共鳴周波数0Hzに等しくすることによ
つて能力の大きい流体駆動装置を提供することが
できる。
第4図aは駆動管12の端部にテーパ19を設
けた実施例、同図bは丸味20を設けた実施例を
示す図でその他の構成作用は第1図の実施例と同
じであるが、第4図a,bの構成によつて、仕事
効率の向上が図れる。第5図は、駆動管の断面形
状が矩形形状の駆動管23を装置した実施例を示
す図で、断面が矩形状の流体流が得られる。その
他の構成、作用効果は第1図の実施例と同じであ
る。
発明の効果
本発明は往復運動をする駆動源を用いながら、
吸入弁、吐出弁が不要で、しかも流れの平滑装置
を用いることなく、脈動成分の少ない安定した流
量、流速の流れを発生し、流量、流速の変更や制
御は電源電圧または電源周波数を変更、制御する
だけでよく、応答性も良好な流体駆動装置を提供
することができる。
しかも本発明によれば、流体は駆動装置の内部
を通過することなく駆動されるので、流体の温度
や清浄性を変えることなく、エツチング装置等特
殊な装置における流体駆動手段とすることが出来
るものである。
また、上記説明から解るように、基本的には中
空容器とそれに連通する枝管と振動枝とで構成さ
れる装置であるので、使用目的に合わせて自由な
形状のものにできるので従来の送風機やポンプよ
り使い勝手がよく、簡単な構造で安価な流体駆動
装置を提供することができる。[C] Here, C is the sound velocity of the fluid, π is pi, and α is the correction coefficient. Next, the operation of this device will be explained. When the power supply device 17 supplies power to the coil 15 with a sinusoidal voltage with a frequency of 0 determined by equation (1), the diaphragm 13 supported by the spring 14 and the coil 15 move in the left and right direction in FIG. It vibrates at a frequency of and radiates pressure waves into the space 11. As mentioned above, the resonance frequency between the space 11 and the drive tube 12
Since the Helmholtz resonance system of f 0 is constructed,
The fluid in the drive tube 12 vibrates as a columnar fluid 23 with an amplitude ab as if it were a rigid body, as shown by the dotted line in the figure. The vibrational movement of the columnar fluid 23 constitutes a second driving source. Resonance frequency with drive tube 18mm in diameter and 160mm in length
In the 135Hz example, ab was approximately 10mm. When the columnar fluid 23 moves to the right in the figure, from a to b, the drive tube 1
The fluid in part 2 ab is driven to the right. When the columnar fluid 23 reaches the position of the maximum amplitude b on the right side, the movement changes from b to a to the left. Columnar fluid 23
As it moves to the left, negative pressure is generated at the inlet of the drive tube 12, but the fluid driven rightward continues to flow rightward along the axis of the drive tube 12 due to inertia. As a result, the negative pressure generated at the end of the drive tube 12 has the following effects:
Fluid from the surrounding area flows in. As the columnar fluid 23 moves to the left, the surrounding fluid also continues to flow in. When the columnar fluid 23 reaches the position a of maximum amplitude on the left side, it changes its direction of motion to the right again. At this time, the fluid flowing in from the surroundings is driven to the right without flowing into the columnar fluid 23 portion, and flows as shown by curve A in the figure, and then becomes a flow B.
This situation can be observed using a stroboscope and smoke. At the stage where the fluid that has flowed into the drive tube AB section is driven to the right and becomes the flow B, it is assumed that part of the fluid near the periphery of the drive tube 12 flows to the right due to the viscous force of the flow B. It will be done. The flow state of this wake and the flow state immediately before the output of the drive tube 12 are difficult to observe and have not been fully elucidated. Thereafter, by repeating the same process, a continuous flow is formed in the right direction around the axis of the drive tube 12. When the flow velocity is measured at a position 5 cm downstream (to the right) of outlet b on the axis of the drive tube 12, the average flow velocity is
The flow velocity fluctuation is +0.08m/sec compared to 3.4m/sec,
It was confirmed that a rightward flow with a constant velocity and little pulsation was formed. This fluid drive device can form a flow within a few cycles after starting operation, and can obtain a highly responsive flow. In addition, while the reciprocating diaphragm 13 is used as the first drive source and the second drive source formed as the reciprocating movement of the columnar fluid 23 inside the drive tube 12 is used as the direct drive source, a smooth vibration absorber that absorbs pulsation is used. It is possible to obtain a flow at a stable flow rate without using any equipment or the like. Moreover, changing and controlling the flow rate and flow rate can be easily achieved by changing and controlling the voltage or frequency applied to the coil 15. Next, other embodiments of the present invention will be described. In FIG. 2, the wall portion of the space 11 in front of the coil 15 is made into a truncated conical wall 18. A diaphragm 13 is provided parallel to the bottom surface of the wall 18, and the drive tube is perpendicular to the top surface. 12 are connected. Other configurations and operations are the same as the embodiment shown in FIG. However, by forming the wall 18 into a truncated cone shape, the effect of improving work efficiency can be obtained. Figure 3 shows the spring 1 of the embodiment shown in Figure 1.
4. The drive source composed of the diaphragm 13, the coil 15, and the permanent magnet 16 is configured by bonding the piezoelectric element 22 to the diaphragm 21 as the drive source, allowing for a simpler structure. Other functions and effects are the same as those of the embodiment shown in FIG. In addition, the vibration system spring 14, diaphragm 13, and coil 1 of the drive source shown in the embodiments of FIGS.
5, or the combination of the piezoelectric element 22 and the diaphragm 21, the natural frequency of the vibration system is set to the resonance frequency of the Helmholtz resonator, which is composed of the space 11 and the drive tube 12, at 0 Hz. By making them equal, a fluid drive device with a large capacity can be provided. FIG. 4a shows an embodiment in which a taper 19 is provided at the end of the drive tube 12, and FIG. However, with the configurations shown in FIGS. 4a and 4b, work efficiency can be improved. FIG. 5 is a diagram showing an embodiment in which a drive tube 23 having a rectangular cross section is installed, and a fluid flow having a rectangular cross section can be obtained. Other configurations, functions and effects are the same as those of the embodiment shown in FIG. Effects of the Invention The present invention uses a reciprocating drive source while
Generates a stable flow rate and flow rate with few pulsating components without the need for suction or discharge valves, and without using a flow smoothing device.The flow rate and flow rate can be changed or controlled by changing the power supply voltage or power frequency. It is possible to provide a fluid drive device that only needs to be controlled and has good responsiveness. Furthermore, according to the present invention, the fluid is driven without passing through the inside of the drive device, so it can be used as a fluid drive means in special devices such as etching devices without changing the temperature or cleanliness of the fluid. It is. In addition, as can be seen from the above explanation, the device is basically composed of a hollow container, branch pipes communicating with it, and vibrating branches, so it can be made into any shape according to the purpose of use, so it is different from the conventional blower. It is possible to provide a fluid drive device that is easier to use, has a simpler structure, and is less expensive than a pump.
第1図は本発明の一実施例による流体駆動装置
の横断面図、第2図は第2の実施例による流体駆
動装置の横断面図、第3図は第3の実施例による
流体駆動装置の横断面図、第4図a,bは同装置
の駆動管の端部を示す詳細横断面図、第5図は同
駆動管の断面形状を矩形にした実施例を示す正面
図、第6図は往復運動を駆動源とした従来例を示
す横断面図、第7図は回転運動を駆動源とした従
来例を示す横断面図である。
10……筐体、11……空間、12……駆動
管、13……振動板、14……スプリング、15
……コイル、16……永久磁石、17……電源装
置、21……振動板、22……圧電素子。
FIG. 1 is a cross-sectional view of a fluid drive device according to an embodiment of the present invention, FIG. 2 is a cross-sectional view of a fluid drive device according to a second embodiment, and FIG. 3 is a cross-sectional view of a fluid drive device according to a third embodiment. FIGS. 4a and 4b are detailed cross-sectional views showing the ends of the drive tube of the device, FIG. 5 is a front view showing an embodiment in which the drive tube has a rectangular cross-sectional shape, and FIG. The figure is a cross-sectional view showing a conventional example using reciprocating motion as a driving source, and FIG. 7 is a cross-sectional view showing a conventional example using rotary motion as a driving source. 10... Housing, 11... Space, 12... Drive tube, 13... Vibration plate, 14... Spring, 15
... Coil, 16 ... Permanent magnet, 17 ... Power supply device, 21 ... Vibration plate, 22 ... Piezoelectric element.
Claims (1)
Vなる空間を形成し、前記容積Vなる空間に臨ん
で外部に連通して断面積A、長さLの駆動管を連
接すると共に、前記振動板の駆動電源周波数を、
前記空間Vと前記駆動管A・Lの寸法条件によつ
て定まる周波数に一致させる周波数調節機能を有
する駆動電源装置を具備したことを特徴とする流
体駆動装置。 2 振動板の固有振動数を、空間容積Vと駆動管
の断面積A及び長さLの寸法条件によつて定まる
周波数に一致させた特許請求の囲第1項記載の流
体駆動装置。 3 中空容器の形状を円錐台形状にすると共に、
前記円錐台形状の中空容器の頂部に駆動管を連接
し、前記円錐台形状の中空容器の底部に平行に振
動板を装置してなる特許請求の範囲第1項記載の
流体駆動装置。[Scope of Claims] 1. A diaphragm is airtightly provided inside a hollow container to form a space with a volume V, and a drive pipe having a cross-sectional area A and a length L is connected to the space facing the volume V and communicating with the outside. and the drive power frequency of the diaphragm,
A fluid drive device characterized by comprising a drive power supply device having a frequency adjustment function to match a frequency determined by the dimensional conditions of the space V and the drive tubes A and L. 2. The fluid drive device according to claim 1, wherein the natural frequency of the diaphragm is made to match the frequency determined by the dimensional conditions of the spatial volume V and the cross-sectional area A and length L of the drive tube. 3 The shape of the hollow container is made into a truncated cone shape, and
2. The fluid drive device according to claim 1, further comprising: a drive tube connected to the top of the truncated conical hollow container, and a diaphragm arranged parallel to the bottom of the truncated conical hollow container.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60105090A JPS61265398A (en) | 1985-05-17 | 1985-05-17 | fluid drive device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60105090A JPS61265398A (en) | 1985-05-17 | 1985-05-17 | fluid drive device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS61265398A JPS61265398A (en) | 1986-11-25 |
| JPH0578680B2 true JPH0578680B2 (en) | 1993-10-29 |
Family
ID=14398215
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP60105090A Granted JPS61265398A (en) | 1985-05-17 | 1985-05-17 | fluid drive device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS61265398A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2945932B2 (en) * | 1989-07-31 | 1999-09-06 | 本多電子株式会社 | Ultrasonic pump |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS58140491A (en) * | 1982-02-16 | 1983-08-20 | Matsushita Electric Ind Co Ltd | Flow generating device |
-
1985
- 1985-05-17 JP JP60105090A patent/JPS61265398A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS61265398A (en) | 1986-11-25 |
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