JPS6080285A - gas laser equipment - Google Patents

gas laser equipment

Info

Publication number
JPS6080285A
JPS6080285A JP58189110A JP18911083A JPS6080285A JP S6080285 A JPS6080285 A JP S6080285A JP 58189110 A JP58189110 A JP 58189110A JP 18911083 A JP18911083 A JP 18911083A JP S6080285 A JPS6080285 A JP S6080285A
Authority
JP
Japan
Prior art keywords
gas
laser
container
mixing
laser tube
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.)
Pending
Application number
JP58189110A
Other languages
Japanese (ja)
Inventor
Yasutada Iwaguchi
保忠 岩口
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP58189110A priority Critical patent/JPS6080285A/en
Publication of JPS6080285A publication Critical patent/JPS6080285A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/02Constructional details
    • H01S3/03Constructional details of gas laser discharge tubes
    • H01S3/036Means for obtaining or maintaining the desired gas pressure within the tube, e.g. by gettering, replenishing; Means for circulating the gas, e.g. for equalising the pressure within the tube
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/14Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range characterised by the material used as the active medium
    • H01S3/22Gases
    • H01S3/223Gases the active gas being polyatomic, i.e. containing two or more atoms

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Engineering & Computer Science (AREA)
  • Plasma & Fusion (AREA)
  • Optics & Photonics (AREA)
  • Lasers (AREA)

Abstract

PURPOSE:To obtain the titled device of a small size and a low cost whereby stable output can be obtained by a method wherein a gas container of the total amount of inflow gas for 5sec or more is provided between the position of starting mixing gasses of single constituents and a laser tube. CONSTITUTION:He21, N222,, and CO223 are supplied while being controlled to a fixed ratio of flow via valves 24-26. At this time, the mixing container 29 having a volume of the total amount of inflow gas for at least 5sec or more is provided between said position 27 and the laser tube 28. The gasses controlled only in the mixing ratio are sufficiently mixed and stirred in this container by utilizing the kinetic energy they have, and then supplied to the laser tube. Reserve chambers 30-32, used for reducing the mutual interference of gas flow based on the difference in the mixing ratio, are not necessary for a small amount of flow. The closer is this container to a regular cube in shape, the higher output and stabler laser can be obtained. Besides, it is exhausted through a vacuum pump 13. This construction unnecessitates a gas mixer of a high cost and a large size and enables the stable laser output to be obtained.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は、単独成分のガスを複数以上効率良く混合する
ことを必要とするガスレーザ装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a gas laser device that requires efficient mixing of a plurality of single component gases.

すなわち本発明のガスレーザ装置は、単にガスの混合比
が一定であるというだけでなく、一定の混合比を保持し
つつ、充分に混合してレーザ発振効率の向上を図ろうと
するものである。
That is, the gas laser device of the present invention not only maintains a constant gas mixture ratio, but also attempts to improve laser oscillation efficiency by maintaining a constant gas mixture ratio and sufficiently mixing the gases.

従来例の構成とその問題点 第1図は、従来のガスレーザ装置の回路図である。ガス
レーザ装置は、一般的にHe 、 N2 、002の3
種のガス1,2.3を用いる(場合によりCOまたは0
2を混合することもある)。このHe + N2 +0
02は一般的に80:16:5種度の混合比で使用され
る。この時それぞれのガス1)2+3の比重が異なる(
特にHeは軽<、CO2は重い)ため、ガス流量弁4.
 5. 6で混合比を制(財)してもガス・・の比重差
によりレーザ管7へ充分混合された状態で、かつ設定し
た混合比のまま供給されず充分なレーザ出力が得られな
かった。そのため従来は各々単独のHeガス1.N2ガ
ス21C02ガス3などをガス流量弁4,5.6を経由
してガスミキサー8に供給し、充分に混合してからレー
ザ管7へ供給。
Structure of the Conventional Example and Its Problems FIG. 1 is a circuit diagram of a conventional gas laser device. Gas laser equipment generally uses three of He, N2, and 002.
Seed gas 1,2.3 (possibly CO or 0
(2 may be mixed). This He + N2 +0
02 is generally used in a mixing ratio of 80:16:5. At this time, the specific gravity of each gas 1)2+3 is different (
In particular, since He is light and CO2 is heavy), gas flow valve 4.
5. Even if the mixing ratio was controlled at 6, due to the difference in specific gravity of the gas, the gas was not supplied to the laser tube 7 in a sufficiently mixed state and at the set mixing ratio, and sufficient laser output could not be obtained. Therefore, in the past, each individual He gas 1. N2 gas 21C02 gas 3, etc. are supplied to the gas mixer 8 via the gas flow valves 4, 5.6, thoroughly mixed, and then supplied to the laser tube 7.

真空ポンプ9で機外10へ排気していた。なお、11は
レーザ管7を放電させるための直流電源。
Vacuum pump 9 was evacuating air to outside the machine 10. Note that 11 is a DC power source for discharging the laser tube 7.

12はレーザ発振器である。従来はガス流量弁ユニット
13.ガスミキサー8.レーザ発振器12に分割されて
いる。
12 is a laser oscillator. Conventionally, the gas flow valve unit 13. Gas mixer8. It is divided into laser oscillators 12.

また第2図に示すように、あらかじめHe + N2 
+002などのガスを混合した充填形混合ガスボンベ1
4を用いて、ガス流量弁16を経て、レーザ管16へ供
給し、真空ポンプ17でガス流速を上げて機外18へ排
気した方式のガスレーザ装置もある。19はレーザ管1
6を放電させるための直流電源、20はレーザ発振器で
ある。そして第1図の従来例ではガスミキサー8の混合
方法がファンを使ったり、複雑なガス配管1反封板を用
いるため、ガスミキサー8が大形となり、レーザ発振器
とは別置する必要が生じたりして装置全体力;大形でか
つ高価なものとなっていた。
In addition, as shown in Fig. 2, He + N2
Filled mixed gas cylinder 1 containing gas such as +002
There is also a gas laser apparatus in which the gas is supplied to the laser tube 16 via a gas flow valve 16, the gas flow rate is increased by a vacuum pump 17, and the gas is exhausted to the outside of the machine 18. 19 is laser tube 1
6 is a DC power supply for discharging, and 20 is a laser oscillator. In the conventional example shown in Fig. 1, the mixing method of the gas mixer 8 uses a fan and a complicated anti-sealing plate for the gas piping 1, so the gas mixer 8 is large and needs to be installed separately from the laser oscillator. As a result, the entire device was large and expensive.

また第2図の従来例では、第1図の従来例の欠点をほぼ
解消したものとなるが、わら力1じめガスを混合すると
、ガス価格が各々単独の場合よりも約3倍になり、ガス
消費量の大きい中出力形レーザ(C02レーザの場合、
レーザ連続出力250W程度)以上ではランニングコス
トが高くなりすき゛て実用的でない欠点を有していた。
In addition, the conventional example shown in Figure 2 almost eliminates the drawbacks of the conventional example shown in Figure 1, but when the gases are mixed together, the gas price is approximately three times higher than when each gas is used alone. , medium power laser with large gas consumption (in the case of C02 laser,
If the continuous laser output is about 250 W or more, the running cost becomes high, which is extremely impractical.

発明の目的 本発明は、前記従来の欠点を除去するもので。Purpose of invention The present invention eliminates the above-mentioned conventional drawbacks.

各々単独の低価格のガスを用い、かつ充分なレーザ特性
(レーザ出力、安定性など)が得られる混合ガスを供給
することを目的としたものである。
The purpose is to supply a mixed gas that provides sufficient laser characteristics (laser output, stability, etc.) using each individual low-cost gas.

発明の構成 この目的を達成するために、本発明は、単独成分のガス
を複数以上混合してレーザを発振させるガスレーザ装置
において、単独成分のガスの混合開始位置とレーザ管と
の間にガスの持つ運動エネルギーを利用してガス混合を
行うためのガス容器を少なくとも流入ガス流量の6秒分
以上の大きさで設けたものである。
Structure of the Invention In order to achieve this object, the present invention provides a gas laser device that oscillates a laser by mixing a plurality of gases each having a single component, in which a gas is inserted between a mixing start position of the gases having a single component and a laser tube. A gas container for mixing gases using the kinetic energy possessed is provided with a size at least equal to or more than 6 seconds of the inflow gas flow rate.

実施例の説明 以下本発明の実施例について図面の第3図〜第9図に泪
って説明する。本実施例は単独のHe ガス21 + 
N2ガス22.CO2ガス23などをそれぞれガス流量
弁24+ 261 26でガス流量を約80:15:5
に制(財)しつつ供給するが、このとき単独成分ガスの
混合開始位置27とレーザ管28との間に少なくとも流
入ガス流量の6秒分以上の大きさでガス混合容器を設け
たものである。ガス流量6秒分以上の大きさとは、He
+N2+C02の流入ガス総流量が11/分の場合(1
1/分−1000Cd/分= 16.7 (1/秒・・
・・・・6秒分は1e、71/秒×5≠841)、84
1以上となり、217分の場合は1684以上のガス混
合容器となる。
DESCRIPTION OF EMBODIMENTS Embodiments of the present invention will now be described with reference to FIGS. 3 to 9 of the drawings. In this example, a single He gas 21 +
N2 gas22. Gas flow rate for CO2 gas 23 etc. is approximately 80:15:5 using gas flow valves 24 + 261 and 26, respectively.
At this time, a gas mixing container with a size of at least 6 seconds or more of the inflow gas flow rate is provided between the single component gas mixing start position 27 and the laser tube 28. be. A gas flow rate of 6 seconds or more means He
When the total inflow gas flow rate of +N2+C02 is 11/min (1
1/min - 1000Cd/min = 16.7 (1/sec...
...6 seconds is 1e, 71/second x 5≠841), 84
1 or more, and in the case of 217 minutes, there will be 1684 or more gas mixing containers.

ガス混合容器29は混合比のみ側副されて、充分に混合
、攪拌されておらないガスを、ガスの持つ運動エネルギ
ーを利用して充分に混ぜ合わせた後にレーザ管28へ供
給する効果を発生する。30 +31.32fdそれぞ
れのガス混合比が異なることによるガスの流れによる相
互干渉を低減するための予備室であるが、実験の結果で
は特に低流量(o、cs l1分以下)の場合以外は不
要であった。
The gas mixing container 29 generates the effect that only the mixture ratio is sidelined, and gases that are not sufficiently mixed or stirred are sufficiently mixed using the kinetic energy of the gases and then supplied to the laser tube 28. . 30 +31.32fd This is a preliminary chamber to reduce mutual interference due to gas flows due to different gas mixture ratios, but experimental results indicate that it is not necessary except in cases of particularly low flow rates (o, cs l1 min or less). Met.

ガス混合容器29の存在は第4図に示すように。The presence of gas mixing vessel 29 is shown in FIG.

レーザ出力に重大な影響を与える。すなわち流入ガス総
流量が11/分の場合では%6秒分以下のガス混合容器
では、その混合能力が充分でなく、6秒分以上の場合は
その効果が飽和状態となるので、過剰装置となる。なお
、33は真空ポンプである。
Severely affects laser output. In other words, when the total flow rate of incoming gas is 11/min, a gas mixing vessel with a flow rate of 6 seconds or less will not have sufficient mixing capacity, and if it is more than 6 seconds, its effect will be saturated, so it should not be used as an excess device. Become. Note that 33 is a vacuum pump.

次に本発明の具体的な実施例を説明する。第5図は本発
明の第1の具体構成例で、各々単独のガスは混合比を制
(財)された後、合流してガス人口34からガス混合容
器36に入り、容器の壁でガスの持つ運動エネルギーに
よって乱流状態となり、充分に混合されてガス出口36
よりレーザ管へ供給される。
Next, specific examples of the present invention will be described. FIG. 5 shows a first specific configuration example of the present invention, in which the individual gases are mixed at a mixing ratio, then merged and enter a gas mixing container 36 from a gas mixture 34, and the gas is mixed at the wall of the container. Due to the kinetic energy of the
is supplied to the laser tube.

第6図は本発明の第2の具体構成例で、ガスは入口34
から容器36へ送り込まれ、ガス管入口37よりガス管
38を経てガス管出口36へ出るが、第1の例と比較し
てガス管の存在分だけ混合がより充分に行われる効果が
ある。
FIG. 6 shows a second specific configuration example of the present invention, in which gas is supplied to the inlet 34.
The gas is fed into the container 36 from the gas pipe inlet 37, passes through the gas pipe 38, and exits to the gas pipe outlet 36. However, compared to the first example, the presence of the gas pipe has the effect of more thorough mixing.

第7図は本発明の第3の具体構成例で、ガスは入口34
から容器36へ送り込まれ、フィルタ39とガス抜穴4
0を経て出口36へ出る。この第3の例は、レーザ管へ
の粉塵類の異物浸入を防止でき、内部レーザ反射ミラー
類の寿命を延長させる効果があり、かつ市販されている
エアフィルターやオイルミストトラップ類をそのままガ
ス混合容器36として安価に供給できる効果がある。こ
の時、41はフィルタ支柱、42は気密用Oリング、4
3は容器ボディ、44Fi蓋、46はボディ43と蓋4
4を結合するためのネジを示す。
FIG. 7 shows a third specific configuration example of the present invention, in which gas is supplied to the inlet 34.
from the filter 39 and the gas vent hole 4.
0 and exit to exit 36. This third example can prevent dust from entering the laser tube, has the effect of extending the life of internal laser reflection mirrors, and can be used as a gas mixture with commercially available air filters and oil mist traps. There is an effect that the container 36 can be supplied at low cost. At this time, 41 is a filter support, 42 is an airtight O-ring, 4
3 is the container body, 44Fi lid, 46 is the body 43 and lid 4
The screws for connecting 4 are shown.

第8図は1本発明の第4の具体構成例で、第1の例の類
似形ではあるが、第1の例よりもガスが短絡的に出て行
かないのでより混合効果を高めることができる。しかし
、その効果は顕著でなく、ガス混合容器の内容量を大巾
に減少させ得る程ではない。すなわち第1〜第4の例に
示すように周辺構造は種々の方式が考えられるが、どの
例においても流入ガス総流量の6秒分以上のガス混合容
器を有する必要がある。そして第1〜第4の例ではほぼ
満足すべきレーザ出力が得られ相互の特性に大差はなか
った。
Figure 8 shows a fourth specific configuration example of the present invention, which is similar to the first example, but the gas does not go out in a short circuit than the first example, so the mixing effect can be further enhanced. can. However, the effect is not significant and is not sufficient to significantly reduce the content of the gas mixing container. That is, as shown in the first to fourth examples, various types of peripheral structures can be considered, but in all examples, it is necessary to have a gas mixing container with a capacity equal to or more than 6 seconds of the total flow rate of incoming gas. In the first to fourth examples, almost satisfactory laser outputs were obtained, and there was no significant difference in their characteristics.

本発明でいうガス混合容器の形状としては、第1〜第4
の例に示すように、なるべく正立方体に類似した形状は
ど得られるレーザ出力は高く、がつ安定する。
The shape of the gas mixing container according to the present invention includes the first to fourth shapes.
As shown in the example, the shape that resembles a regular cube as much as possible produces a high and stable laser output.

すなわち単純に少なくとも流入ガス流量の5秒分以上の
容量を得るkめに細長い円筒状の物、または配管用ホー
ス類を太くしてその代用する等の方法では充分な混合が
得られずレーザ出力は低くなる。
In other words, if you simply use a slender cylindrical object that has a capacity equal to at least 5 seconds of the inflow gas flow rate, or use thicker piping hoses instead, sufficient mixing cannot be achieved and the laser output is reduced. becomes lower.

レーザ発振器の定格出力によってガスの混合比。Gas mixture ratio depending on the rated output of the laser oscillator.

ガス量がともに多少異なるが、流入ガス流量の6秒分以
上の大きさでガス混合容器を設けることにより、安定し
たレーザ出力が得られる。
Although the gas amounts are somewhat different, by providing a gas mixing container with a size equal to or more than 6 seconds of the inflow gas flow rate, stable laser output can be obtained.

発明の効果 以上のように本発明によれば、高価かつ大形のガスミキ
サーを用いることなく、複数以」二のガスを充分に混合
した状態で供給することが可能となり、ガスレーザ装置
の小形化、低価格化を図ることができる。
Effects of the Invention As described above, according to the present invention, it is possible to supply two or more gases in a sufficiently mixed state without using an expensive and large gas mixer, and the gas laser device can be downsized. , it is possible to reduce the price.

【図面の簡単な説明】[Brief explanation of drawings]

第1図、第2図は従来のガスレーザ装置の概略構成図、
第3図は本発明によるガスレーザ装置の概略構成図、第
4図はガス混合容器の容量とレーザ出力の対比実験特性
図、第6図〜第8図は本発明のガスレーザ装置に使用す
るガス混合容器の各別の正面断面図である。 21.221 23・・・・・・ガス、24,25)2
6・・・・・・ガス流量弁、27・・・・・・混合開始
位置、28・・・・・・レーザ管、29.36・旧・・
ガス混合容器。 代理人の氏名 弁理士 中 尾 敏 男 はが1名第1
図 81′33図 ′?9 第4図 ε:35図 第6図 第8図 手続補正書 昭和69年 2月79日 l事件の表示 昭和68年特許願第189110号 2発明の名称 ガスレーザ装置 3補正をする者 事イ′1との関係 特 許 出 願 人任 所 大阪府
門真市大字門真1006番地名 称 (582)松下電
器産業株式会社代表者 山 下 俊 彦 4代理人 〒571 住 所 大阪府門真市大字門真1006番地松下電器産
業株式会社内 6補正の対象 明細書の発明の詳細な説明の欄 116.7cm’/秒」に補正いたします。 し) 同第6頁第4行の「841)、a41 Jをに補
正いだします。 (4)図面第4図を別紙のように補正いたします。 手続補正書 昭和69年3 月 ノ 日 昭和68年特許願第189110号 2発明の名称 ガスレーザ装置 3補正をする者 事f’lとの関係 特 許 出 願 人任 所 大阪府
門真市大字門真1006番地名 称 (582)松下電
器産業株式会社代表者 山 下 俊 彦 4代理人 〒571 住 所 大阪府門真市大字門真1006番地松下電器産
業株式会社内
Figures 1 and 2 are schematic configuration diagrams of conventional gas laser equipment;
Fig. 3 is a schematic configuration diagram of the gas laser device according to the present invention, Fig. 4 is a comparative experimental characteristic diagram of the capacity of the gas mixing container and the laser output, and Figs. 6 to 8 are gas mixtures used in the gas laser device of the present invention. FIG. 3 is a front sectional view of each container. 21.221 23...gas, 24,25)2
6... Gas flow valve, 27... Mixing start position, 28... Laser tube, 29.36 Old...
Gas mixing container. Name of agent: Patent attorney Toshio Nakao (1st person)
Figure 81'33'? 9 Figure 4 ε: 35 Figure 6 Figure 8 Procedural amendment February 79, 1988 l Indication of the case 1989 Patent Application No. 189110 2 Name of the invention Gas laser device 3 Person making the amendment I' Relationship with 1 Patent Application Person Address 1006 Kadoma, Kadoma City, Osaka Name (582) Matsushita Electric Industrial Co., Ltd. Representative Toshihiko Yamashita 4 Agent 571 Address 1006 Kadoma, Kadoma City, Osaka Prefecture We will make an amendment to 116.7 cm'/sec in the detailed description of the invention section of the specification subject to the 6th amendment within Matsushita Electric Industrial Co., Ltd. 841), a41 J on page 6, line 4 of the same. (4) Figure 4 of the drawing is amended as shown in the attached sheet. Procedural amendment March 1989, Showa 1968 Patent Application No. 189110 2 Name of the invention Gas laser device 3 Person making the amendment Relationship with f'l Patent application Person address 1006 Kadoma, Kadoma City, Osaka Prefecture Name Name (582) Matsushita Electric Industrial Co., Ltd. Representative: Toshihiko Yamashita 4 Agent: 571 Address: Matsushita Electric Industrial Co., Ltd., 1006 Kadoma, Kadoma City, Osaka Prefecture

Claims (1)

【特許請求の範囲】[Claims] 単独成分のガスを複数以上混合してレーザ発振させるガ
スレーザ装置において、単独成分のガスの混合開始位置
とレーザ管との間にガスの持つ運動エネルギーを利用し
てガス混合を行うためのガス容器を少なくとも流入ガス
流量の6秒分以上の大きさで設けたガスレーザ装置。
In a gas laser device that mixes multiple single component gases for laser oscillation, a gas container is provided between the mixing start position of the single component gases and the laser tube to mix the gases using the kinetic energy of the gases. A gas laser device provided with a size that is at least 6 seconds worth of inflow gas flow rate.
JP58189110A 1983-10-07 1983-10-07 gas laser equipment Pending JPS6080285A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58189110A JPS6080285A (en) 1983-10-07 1983-10-07 gas laser equipment

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58189110A JPS6080285A (en) 1983-10-07 1983-10-07 gas laser equipment

Publications (1)

Publication Number Publication Date
JPS6080285A true JPS6080285A (en) 1985-05-08

Family

ID=16235536

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58189110A Pending JPS6080285A (en) 1983-10-07 1983-10-07 gas laser equipment

Country Status (1)

Country Link
JP (1) JPS6080285A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4794613A (en) * 1987-07-27 1988-12-27 Prc Corporation Laser fluid flow control apparatus and method

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4794613A (en) * 1987-07-27 1988-12-27 Prc Corporation Laser fluid flow control apparatus and method

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