JPH0223078A - Jet generator using electric field - Google Patents
Jet generator using electric fieldInfo
- Publication number
- JPH0223078A JPH0223078A JP17328388A JP17328388A JPH0223078A JP H0223078 A JPH0223078 A JP H0223078A JP 17328388 A JP17328388 A JP 17328388A JP 17328388 A JP17328388 A JP 17328388A JP H0223078 A JPH0223078 A JP H0223078A
- Authority
- JP
- Japan
- Prior art keywords
- electrode
- liquid
- holes
- electrodes
- electric field
- 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
- 230000005684 electric field Effects 0.000 title claims description 15
- 239000007788 liquid Substances 0.000 claims abstract description 30
- 239000000463 material Substances 0.000 claims abstract description 6
- 239000007772 electrode material Substances 0.000 abstract description 14
- 238000004519 manufacturing process Methods 0.000 description 3
- 238000000034 method Methods 0.000 description 3
- 238000009835 boiling Methods 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- AJDIZQLSFPQPEY-UHFFFAOYSA-N 1,1,2-Trichlorotrifluoroethane Chemical compound FC(F)(Cl)C(F)(Cl)Cl AJDIZQLSFPQPEY-UHFFFAOYSA-N 0.000 description 1
- 229910001369 Brass Inorganic materials 0.000 description 1
- 240000007594 Oryza sativa Species 0.000 description 1
- 235000007164 Oryza sativa Nutrition 0.000 description 1
- 239000010951 brass Substances 0.000 description 1
- 235000013339 cereals Nutrition 0.000 description 1
- 238000001816 cooling Methods 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 238000005553 drilling Methods 0.000 description 1
- 230000001788 irregular Effects 0.000 description 1
- 210000003127 knee Anatomy 0.000 description 1
- 230000007774 longterm Effects 0.000 description 1
- 239000011148 porous material Substances 0.000 description 1
- 238000010248 power generation Methods 0.000 description 1
- 235000009566 rice Nutrition 0.000 description 1
- 229910001220 stainless steel Inorganic materials 0.000 description 1
- 239000010935 stainless steel Substances 0.000 description 1
- 238000003756 stirring Methods 0.000 description 1
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 1
Landscapes
- Particle Formation And Scattering Control In Inkjet Printers (AREA)
- Oxygen, Ozone, And Oxides In General (AREA)
Abstract
Description
【発明の詳細な説明】
(産業上の利用分野)
本発明は、液体中で対向設置された電極間に高電圧を印
加することにより該液体にジェット流を発生させるよう
にした装置の改良に関し、更に詳しくは該ジェット発生
装置に使用される電極の改良に関する。Detailed Description of the Invention (Field of Industrial Application) The present invention relates to an improvement in a device that generates a jet flow in a liquid by applying a high voltage between electrodes placed opposite each other in the liquid. More specifically, the present invention relates to improvements in electrodes used in the jet generator.
本発明者等は高電圧電場を利用して液体中にジェット流
を発生させる方法を既に提案している。(特開昭59−
663425号公報参照)この方法をPt5a図を参照
して説明すると、液体1中において、面電極2に対して
所定間隔を隔ててリング状の電極3を設け、両電極間に
高電圧を印加する。すると、リング状の電極3を構成す
る電線の回りに電界の強い部分と弱い部分が生じ、その
電界の強弱により液体はリング状の電極3の外側より両
電極間の間隙を通って電線で囲まれたリング状の電極3
の内部5を通過し、ジェット流4となって流出する。The present inventors have already proposed a method of generating a jet stream in a liquid using a high voltage electric field. (Unexamined Japanese Patent Publication No. 59-
663425) This method will be explained with reference to diagram Pt5a. In the liquid 1, a ring-shaped electrode 3 is provided at a predetermined distance from the surface electrode 2, and a high voltage is applied between both electrodes. . Then, a strong electric field and a weak electric field are created around the electric wire that constitutes the ring-shaped electrode 3, and depending on the strength of the electric field, the liquid passes from the outside of the ring-shaped electrode 3 through the gap between the two electrodes and is surrounded by the electric wire. ring-shaped electrode 3
It passes through the interior 5 of the jet stream 4 and flows out as a jet stream 4.
しかし、この公知の方法では、ジェット流・tが狭いリ
ング状の電極3の内部5がら噴出するので、全体として
流れが小さすぎ、液全本の流動、攪拌を十分に行ない得
なかった。However, in this known method, since the jet stream t is ejected from the inside 5 of the narrow ring-shaped electrode 3, the overall flow is too small and the entire liquid cannot be sufficiently flowed and stirred.
前記欠点を改善するため、第4図及びj@5図に示すよ
うに、多数の電線15を縦横に交叉させ、各電線15の
間隔を異ならせてメツシュの異なる網状電極13(不等
間隔電極)を作り、この網状電極13を面電極12に対
向設置したジェット発生装置も既に提案されている。In order to improve the above-mentioned drawbacks, as shown in FIGS. 4 and 5, a large number of electric wires 15 are made to intersect vertically and horizontally, and the intervals between the electric wires 15 are varied, so that the mesh electrodes 13 with different meshes (irregularly spaced electrodes) are formed. ), and a jet generating device in which this mesh electrode 13 is placed opposite to the surface electrode 12 has already been proposed.
上述のごとき構成の電極間に高電圧を印加すると電場が
形成され、電極13の各線状電極材15と面電極12と
の間には電気力線が作用するが、その大きさを面電極1
2に沿った方向に比較すると電極材により形成する間隔
16の狭い領域Sの電界は間隔16の広い領域Wの電界
より強くなる。電界が液体に作用すると、液体の圧力は
(1/2)εE2
(ε:誘電率、E:電界の強さ)
だけ大きくなるので、各線状電極材15の真下が一番大
きくなり、線状電極材15により形成する間隔16の狭
い領域Sが次いで大きく、電極材の形成する間隔の広い
領域Wの圧力が一番小さくなる。When a high voltage is applied between the electrodes configured as described above, an electric field is formed, and lines of electric force act between each linear electrode material 15 of the electrode 13 and the surface electrode 12.
2, the electric field in a region S with a narrow interval 16 formed by the electrode material is stronger than the electric field in a region W with a wide interval 16. When an electric field acts on the liquid, the pressure of the liquid increases by (1/2) εE2 (ε: dielectric constant, E: electric field strength), so the pressure is greatest right below each linear electrode material 15, The region S where the spacing 16 formed by the electrode material 15 is narrow is the next largest, and the pressure in the region W where the spacing is wide and the electrode material is formed is the smallest.
その結果、第4図の矢印で示すように液体には線材の構
成する間隔の狭い領域Sを通って面1!i12へ向かう
流れが生じ、この流れは面電極12で向きを変えて広い
領域Wへ向かってジェット流となる。As a result, as shown by the arrows in FIG. 4, the liquid passes through the narrowly spaced region S formed by the wire rods and passes through the surface 1! A flow toward i12 is generated, and this flow changes direction at the surface electrode 12 and becomes a jet flow toward the wide area W.
第15!、21において、■は電極間より流れ出すノヱ
ッ) ’titをr↑う、■は電極間に液体が流れ込む
流れを・Rす。15th! , 21, ■ represents the flow of liquid flowing between the electrodes.
即ち、電界の強い狭い領域Sの液体の圧力が電界の弱い
広い領域Wの液体の圧力より大きくなり、圧勾勾配によ
って上記ジェットの方向が決定される。狭い領域Sでは
線状電極材15が互いに接圧しているため、間隔が広い
領域Wに比べて同じ電圧を印加すれば、この付近の電界
がより強くなり、それだけ液体の圧力が上昇するものと
なり、圧力勾配が大きくなってジェットの流速は大きく
なる。That is, the pressure of the liquid in the narrow region S where the electric field is strong is greater than the pressure of the liquid in the wide region W where the electric field is weak, and the direction of the jet is determined by the pressure gradient. In the narrow area S, the linear electrode materials 15 are in contact with each other, so if the same voltage is applied as compared to the wider area W, the electric field in this area will be stronger, and the pressure of the liquid will increase accordingly. , the pressure gradient increases and the jet flow velocity increases.
電極13を構成する線状電極材15としては真ちゅう、
ステンレス等の線材を用いており、線材の直径dは0.
5〜5II1ms両電極材の狭い領域の間隔Sは 1〜
50+am の範囲が好い。The linear electrode material 15 constituting the electrode 13 is made of brass,
A wire material such as stainless steel is used, and the diameter d of the wire material is 0.
5~5II1ms The spacing S between the narrow areas of both electrode materials is 1~
A range of 50+am is preferred.
上記狭い領域Sに対する広い領域Wの幅は1.25〜2
0倍 の範囲、即ち狭い領域の間隔Sに対する広い領域
の間隔Wの割合は、S/W=0.05〜0.8 の範
囲が良く、面電極12と不等間隔電極13の間隔りは0
.5−50+1Ia1 の間隔が好適であり、D/d≧
1.5になるような上述の範囲で構成した電極に5〜3
0KVの電圧を印加すると、電極材の広い領域よりジェ
ット流が効果的に噴射する。The width of the wide area W with respect to the narrow area S is 1.25 to 2
The range of 0 times, that is, the ratio of the interval W of the wide area to the interval S of the narrow area, is preferably in the range of S/W = 0.05 to 0.8, and the interval between the surface electrode 12 and the unevenly spaced electrode 13 is 0
.. A spacing of 5-50+1Ia1 is suitable, and D/d≧
5 to 3 to the electrode configured in the above range such that the value is 1.5.
When a voltage of 0 KV is applied, a jet stream is effectively ejected from a wide area of the electrode material.
(発明が解決しようとする課題)
ところが、上記のような網状電極13は構成が複雑であ
るため製作精度を上げることが比較的困難であり、製造
コストが高くなるおそれがあった。(Problems to be Solved by the Invention) However, since the mesh electrode 13 as described above has a complicated structure, it is relatively difficult to improve the manufacturing accuracy, and there is a risk that the manufacturing cost will increase.
そこで、本発明の目的は、ジェット流を面電極の全面に
渡って容易に発生させることができ、かつ電極の製造が
容易であるジェ・ント発生装置を提供するにある。SUMMARY OF THE INVENTION Therefore, an object of the present invention is to provide a jet generating device that can easily generate a jet flow over the entire surface of a surface electrode and that can easily manufacture the electrode.
(課題を解決するための手段)
上記目的を達成するため、本発明によるジェット発生装
置では面電極と対向する他方の電極を板材を打ち抜いた
多孔板状電極とし、隣合った孔同士の間隔や配列を異な
るように穿孔したり、隣合った孔の径を異なるように穿
孔して不等間隔電極を構成して成るものである。(Means for Solving the Problems) In order to achieve the above object, in the jet generating device according to the present invention, the other electrode facing the surface electrode is a porous plate-shaped electrode punched out of a plate material, and the distance between adjacent holes is The electrodes are formed by forming electrodes at unequal intervals by forming holes in different arrangements or forming adjacent holes with different diameters.
上記のように不等の孔を穿孔したりある−・は孔の間隔
や配列を異ならせることにより隣合っている電極間の間
隙が等間隔にならないように枯成し、上記面電極と上記
多孔板電極間に高電圧を印加すると、多孔板電極の間隔
の狭い領域より液体が両電極間に流入し、間隔の広い領
域よりジェット流が流出する。By drilling unequal holes as described above, by varying the spacing and arrangement of the holes, the gaps between adjacent electrodes are unequal, so that the surface electrodes and the When a high voltage is applied between the porous plate electrodes, liquid flows between the porous plate electrodes from the narrowly spaced areas, and a jet stream flows out from the widely spaced areas.
(実施例)
以下、本発明の実施例について、図を参照して工明する
。(Example) Hereinafter, examples of the present invention will be explained with reference to the drawings.
第1図は本発明によるジェット発生電極の多孔板電極1
3の一実施例を示すものである。FIG. 1 shows a perforated plate electrode 1 of a jet generating electrode according to the present invention.
This shows an example of No. 3.
本発明の多孔板電極は複数の大きな孔19aと小さな孔
19bとを交互に穿設した板状電極材18より植成され
る。板状電極材18に穿設された孔は前記第9.10図
における間隔16に相当し、大きな孔19aは広い領域
Wとなり、小さな孔19t+は狭い領域Sの作用を行な
い、これらが交互に配列されていることがら、前記実施
例と同様にこの構成の多孔板電極13と面電極12の間
に高電圧を印加すると、多孔板電極13の真下の液体が
最も圧力が高く、大きな孔19aの領域の液体の圧力は
最も低くなるので、液体は小さな孔19bより両電極間
に流れ込み、大きな孔19aよりジェット流となって流
出する。The perforated plate electrode of the present invention is implanted from a plate-shaped electrode material 18 in which a plurality of large holes 19a and small holes 19b are alternately bored. The holes drilled in the plate-shaped electrode material 18 correspond to the spacing 16 in FIG. Because of the arrangement, when a high voltage is applied between the perforated plate electrode 13 and the surface electrode 12 with this configuration as in the previous embodiment, the liquid directly under the perforated plate electrode 13 has the highest pressure, and the large pores 19a Since the pressure of the liquid in the region is lowest, the liquid flows between the two electrodes through the small hole 19b and flows out as a jet stream through the large hole 19a.
多孔板電極13の穿孔は打ち抜き加工で良く、孔の形状
は円形に限らず、矩形、楕円形でも良いが、隣合って穿
設される孔の大きさが少なくとも異なるように配置する
。小さい孔の等価直径Wはその比S/Wは前述の実施例
と同様に0.05〜0.8
の範囲が好ましい。The holes in the perforated plate electrode 13 may be punched, and the shape of the holes is not limited to circular, but may be rectangular or elliptical, but adjacent holes are arranged so that their sizes are at least different. As for the equivalent diameter W of the small hole, the ratio S/W is preferably in the range of 0.05 to 0.8 as in the above embodiment.
又、面電極との間隔は 0.5〜5IIII の範囲が好適である。Also, the distance from the surface electrode is 0.5-5III A range of is suitable.
又、ジェット流を発生させるための液体としては、フロ
ン113のような
10−”Ω−1・lll−1以上の電気伝導度を有する
液体であれば有効に用い得る。Further, as the liquid for generating the jet stream, any liquid having an electrical conductivity of 10-''Ω-1·ll-1 or more, such as Freon 113, can be effectively used.
第2図は本発明のジェット発生装置の不等間隔電極13
の他の実施例を示し、同じ大きさの直径の孔を一つ置き
にベアになるように穿設した板状電極材18より構成さ
れる。この場合、高電圧を印加すると、近接した二つの
隣接した孔20aで広い領域Wの働外を行なって、この
領域の圧力は単独の孔20t+の領域Sの圧力よりも小
さくなり、従って前の実施例と同様に液体は小さな径の
孔20bより両電極間に流れ込み、隣接している二つの
孔20aよりジェット状に流出する。これらの二つの孔
の間には境界があっても良く、又二つの孔がつながって
いても良い。FIG. 2 shows unevenly spaced electrodes 13 of the jet generating device of the present invention.
Another embodiment of the present invention is shown, and is composed of a plate-shaped electrode material 18 in which holes of the same size and diameter are bored so that every other hole is bare. In this case, when a high voltage is applied, the two adjacent holes 20a work in a wide area W, and the pressure in this area becomes smaller than the pressure in the area S of the single hole 20t+, and therefore As in the embodiment, the liquid flows between the two electrodes through the small diameter hole 20b and flows out in a jet form through the two adjacent holes 20a. There may be a boundary between these two holes, or the two holes may be connected.
(発明の効果)
上記の説明で明らかなように、本発明によれば、可動部
が存在せずに、液体中にジェット流を生起させることが
できるので、種々の分野への応用に適用しうる。(Effects of the Invention) As is clear from the above description, according to the present invention, a jet flow can be generated in a liquid without the presence of a moving part, so it can be applied to various fields. sell.
例えば、微少重量環境での利用、即ち具体的には宇宙で
の液体流水発生装置、ポンプ、熱交換装置などに適用可
能である。For example, it is applicable to use in a micro-weight environment, specifically, to a liquid water generating device, a pump, a heat exchange device, etc. in space.
特に、熱交換器への応用は上記微少!111環境ばかり
でなく、地上の高性能熱交換器、発電用熱文換器、トラ
ンスの冷却装置等の熱交換装置に適用することにより、
対流熱伝達、沸騰熱伝達を促進することができる。この
場合、面電極間を伝熱面として用いれば良く、容易に既
設の装置へ適用することができる。又、気泡の発生を伴
なう沸騰、蒸発熱交換の場合はジェットの発生により液
体自身の攪はん、移動に上り面電極を付着していた気泡
は薄利され、面電極における伝達効果が大幅に向上する
。In particular, the application to heat exchangers is extremely small! By applying it not only to the 111 environment, but also to heat exchange devices such as high-performance ground heat exchangers, heat exchangers for power generation, and transformer cooling devices,
It can promote convective heat transfer, boiling heat transfer. In this case, it is sufficient to use the area between the plane electrodes as a heat transfer surface, and it can be easily applied to existing devices. In addition, in the case of boiling or evaporative heat exchange that involves the generation of bubbles, the generation of jets stirs and moves the liquid itself, and the bubbles attached to the upper surface electrode are weakened, and the transfer effect at the surface electrode is greatly increased. improve.
又、本発明によると不等間隔電極を簡単かつ低コストに
得られる。Further, according to the present invention, electrodes having irregular intervals can be obtained easily and at low cost.
更に、本発明の板状の打ち抜き電極は、籾材を用いるも
のと比べて、耐久性が高く、かつ長期の使用に当たって
変形がないので、信頼性が向上する。Furthermore, the plate-shaped punched electrode of the present invention has higher durability than one using rice grain material, and does not deform during long-term use, so reliability is improved.
第1図は本発明の一実施例になる板状電極からなる不等
間隔電極を示す平面図、第2図は本発明の池の実施例を
示す平面図、第3図は従来公知のジェット発生装置を説
明するための断面図、第4図は既提案のジェット発生V
装置を示す断面図、第5図は第4図の平面図である。
18:板状電極材 19a:大きな孔
19b:小さな孔 20a:隣接した孔20 bニー1
11独の孔
なす
河1
第2
■
図
図
第3
図FIG. 1 is a plan view showing an unevenly spaced electrode made of plate-shaped electrodes according to an embodiment of the present invention, FIG. 2 is a plan view showing an embodiment of a pond according to the present invention, and FIG. 3 is a plan view showing a conventionally known jet. A sectional view for explaining the generator, Fig. 4 is the jet generator V of the existing proposal.
FIG. 5 is a sectional view showing the device, and FIG. 5 is a plan view of FIG. 4. 18: Plate electrode material 19a: Large hole 19b: Small hole 20a: Adjacent hole 20b knee 1
11 German Hole River 1 2 ■ Figure Figure 3
Claims (1)
高電圧を印加し、液中に生ずる電場の強弱によって液体
が力を受けてジェット流を発生させる装置において、 前記一対の電極の内、一方の電極が平面状の面電極であ
り、他方の電極が板材を穿孔した多孔板電極からなるこ
とを特徴とする電場によるジェット発生装置。[Scope of Claims] A device in which a high voltage is applied to a pair of electrodes placed opposite each other in a liquid with a predetermined gap therebetween, and the liquid is subjected to a force depending on the strength of an electric field generated in the liquid to generate a jet flow, comprising: A jet generating device using an electric field, wherein one of the pair of electrodes is a planar surface electrode, and the other electrode is a perforated plate electrode formed by perforating a plate material.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63173283A JPH0734663B2 (en) | 1988-07-12 | 1988-07-12 | Jet generator by electric field |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63173283A JPH0734663B2 (en) | 1988-07-12 | 1988-07-12 | Jet generator by electric field |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0223078A true JPH0223078A (en) | 1990-01-25 |
| JPH0734663B2 JPH0734663B2 (en) | 1995-04-12 |
Family
ID=15957578
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP63173283A Expired - Lifetime JPH0734663B2 (en) | 1988-07-12 | 1988-07-12 | Jet generator by electric field |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0734663B2 (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2007203222A (en) * | 2006-02-02 | 2007-08-16 | Chiba Univ | Fluid control method and fluid device using the same |
Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5966342A (en) * | 1982-10-05 | 1984-04-14 | Agency Of Ind Science & Technol | Generation of liquid flow due to high voltage electric field |
-
1988
- 1988-07-12 JP JP63173283A patent/JPH0734663B2/en not_active Expired - Lifetime
Patent Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5966342A (en) * | 1982-10-05 | 1984-04-14 | Agency Of Ind Science & Technol | Generation of liquid flow due to high voltage electric field |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2007203222A (en) * | 2006-02-02 | 2007-08-16 | Chiba Univ | Fluid control method and fluid device using the same |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0734663B2 (en) | 1995-04-12 |
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