JPH06326379A - Gas laser oscillator - Google Patents
Gas laser oscillatorInfo
- Publication number
- JPH06326379A JPH06326379A JP11266893A JP11266893A JPH06326379A JP H06326379 A JPH06326379 A JP H06326379A JP 11266893 A JP11266893 A JP 11266893A JP 11266893 A JP11266893 A JP 11266893A JP H06326379 A JPH06326379 A JP H06326379A
- Authority
- JP
- Japan
- Prior art keywords
- laser
- gas
- laser gas
- taper
- discharge 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
Links
Landscapes
- Lasers (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】本発明は放電管の軸方向と光軸方
向が一致したガスレーザ発振装置に関するものであり、
レーザガスの循環路中の圧力損失を低減させるようにし
たガスレーザ発振装置に関するものである。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a gas laser oscillating device in which the axial direction of a discharge tube is aligned with the optical axis direction,
The present invention relates to a gas laser oscillating device configured to reduce pressure loss in a circulation path of laser gas.
【0002】[0002]
【従来の技術】従来のガスレーザ発振装置は、図3に示
すものであった。この図において、1はガラスなどの誘
電体よりなる放電管、2,3はそれぞれ前記放電管1の
内部に設けられた金属電極、4は前記電極2,3に接続
された高圧電源、5は前記高圧電源4の電圧を印加する
両電極2,3間にはさまれた放電管1内の放電空間、6
は全反射鏡、7は部分反射鏡、この全反射鏡6と部分反
射鏡7は前記放電空間5の両端に固定配置され、光共振
器を形成している。8は前記部分反射鏡7より出力され
るレーザビームである。矢印9はレーザガスの流れる方
向を示しており、軸流形レーザ装置の中を循環してい
る。10は送気管11,12はそれぞれ前記放電空間5
にて温度上昇したレーザガスの温度を下げるためのレー
ザガス冷却用熱交換器、13はレーザガス循環用送風機
である。2. Description of the Related Art A conventional gas laser oscillator is shown in FIG. In this figure, 1 is a discharge tube made of a dielectric material such as glass, 2 and 3 are metal electrodes provided inside the discharge tube 1, 4 is a high-voltage power supply connected to the electrodes 2 and 3, and 5 is Discharge space in the discharge tube 1 sandwiched between the electrodes 2 and 3 for applying the voltage of the high voltage power source 4,
Is a total reflection mirror, 7 is a partial reflection mirror, and the total reflection mirror 6 and the partial reflection mirror 7 are fixedly arranged at both ends of the discharge space 5 to form an optical resonator. A laser beam 8 is output from the partial reflecting mirror 7. The arrow 9 indicates the direction in which the laser gas flows, and the laser gas circulates in the axial flow type laser device. 10 is an air supply pipe 11, 12 is the discharge space 5
A heat exchanger for cooling the laser gas for lowering the temperature of the laser gas whose temperature has risen at 13 and a blower for circulating the laser gas.
【0003】以上が従来の軸流形レーザ装置の構成であ
り、次にその動作について説明する。The above is the configuration of the conventional axial flow laser device, and its operation will be described below.
【0004】まず一対の金属電極2,3に高電圧電源4
から高電圧を印加し、放電空間5にグロー状の放電を発
生させる。放電空間5を通過するレーザガスは、この放
電エネルギーを得て励起され、その励起されたレーザガ
スは全反射鏡6および部分反射鏡7により形成された光
共振器で共振状態となり、部分反射鏡7からレーザビー
ム8が出力される。このレーザビーム8がレーザ加工等
の用途に用いられる。First, a high voltage power source 4 is provided on the pair of metal electrodes 2 and 3.
A high voltage is applied to generate a glow-like discharge in the discharge space 5. The laser gas passing through the discharge space 5 is excited by obtaining this discharge energy, and the excited laser gas is brought into a resonance state by the optical resonator formed by the total reflection mirror 6 and the partial reflection mirror 7, and is excited from the partial reflection mirror 7. The laser beam 8 is output. This laser beam 8 is used for applications such as laser processing.
【0005】図4は放電管導入、排出部のレーザガスの
流れの状態を示した図である。放電管と送気管とは互い
に段差がついていた。このため流体の流れを乱して渦を
つくり圧力損失を生ずる。FIG. 4 is a diagram showing the state of the flow of laser gas in the discharge tube introduction / discharge section. The discharge tube and the air supply tube were stepped from each other. For this reason, the flow of the fluid is disturbed to form a vortex and a pressure loss occurs.
【0006】[0006]
【発明が解決しようとする課題】上記の構成では、放電
管の導入、排出部の段差においてレーザガス流の収縮、
拡大による圧力損失が大きく、それだけ大容量送風機の
動力が必要となり、その騒音が大きくなるという問題点
を有していた。In the above structure, the laser gas flow contracts at the steps of the discharge tube and the discharge portion,
There is a problem that the pressure loss due to the expansion is large, the power of the large capacity blower is required accordingly, and the noise is increased.
【0007】本発明は上記従来の問題点を解決するもの
で、レーザガスの循環路中の圧力損失を低下させること
を目的とする。The present invention solves the above-mentioned conventional problems, and an object thereof is to reduce the pressure loss in the circulation path of the laser gas.
【0008】[0008]
【課題を解決するための手段】本発明は、上記問題点を
解決するために放電管のレーザガス導入部または/レー
ザガス排出部にテーパを設けた構成を有するガスレーザ
発振装置である。In order to solve the above problems, the present invention is a gas laser oscillating device having a structure in which a laser gas introducing portion or a laser gas discharging portion of a discharge tube is provided with a taper.
【0009】[0009]
【作用】この構成により放電管のレーザガス導入部また
は/およびレーザガス排出部に設けたテーパにより流れ
が管壁面から剥離しにくくなり流れが乱れず、レーザガ
ス流の収縮、拡大による圧力損失が低減し、レーザガス
循環路中の圧力損失を低下するものである。With this configuration, the taper provided at the laser gas introduction portion and / or the laser gas discharge portion of the discharge tube makes it difficult for the flow to be separated from the wall surface of the tube, the flow is not disturbed, and pressure loss due to contraction and expansion of the laser gas flow is reduced The pressure loss in the laser gas circulation path is reduced.
【0010】[0010]
【実施例】以下本発明の実施例について、図1を参照し
ながら説明する。Embodiments of the present invention will be described below with reference to FIG.
【0011】図1において1〜13は従来同様のもので
あり、1はガラスなどの誘電体よりなる放電管、2,3
はそれぞれ前記放電管1の内部に設けられた金属電極、
4は前記電極2,3に接続された高圧電源、5は前記高
圧電源4の電圧を印加する両電極2,3管にはさまれた
放電管1内の放電空間、6は全反射鏡、7は部分反射
鏡、この全反射鏡6と部分反射鏡7は前記放電空間5の
両端に固定配置され、光共振器を形成している。8は前
記部分反射鏡7より出力されるレーザビーム、矢印9は
レーザガスの流れる方向を示しており、軸流形レーザ装
置の中を循環している。10は送気管、11,12はそ
れぞれレーザガス冷却用熱交換器、13はレーザガス循
環用送風機である。14は放電管1のレーザガス導入部
に設けられたテーパ、15は放電管1のレーザガス排出
部に設けられたテーパである。なおこの図においては放
電管1のレーザガス導入部、レーザガス排出部両方にそ
れぞれテーパ14,15を設けているがどちらか片側に
テーパを用いる構造であってもよい。In FIG. 1, 1 to 13 are the same as conventional ones, 1 is a discharge tube made of a dielectric material such as glass, and 2, 3
Are metal electrodes provided inside the discharge tube 1,
4 is a high-voltage power supply connected to the electrodes 2 and 3, 5 is a discharge space in the discharge tube 1 sandwiched between the two electrodes 2 and 3 for applying the voltage of the high-voltage power supply 4, 6 is a total reflection mirror, Reference numeral 7 denotes a partial reflection mirror, and the total reflection mirror 6 and the partial reflection mirror 7 are fixedly arranged at both ends of the discharge space 5 to form an optical resonator. Reference numeral 8 indicates a laser beam output from the partial reflecting mirror 7, and arrow 9 indicates the direction in which the laser gas flows, which circulates in the axial flow laser device. Reference numeral 10 is an air supply pipe, 11 and 12 are heat exchangers for cooling the laser gas, and 13 is a blower for circulating the laser gas. Reference numeral 14 is a taper provided at the laser gas introduction portion of the discharge tube 1, and 15 is a taper provided at the laser gas discharge portion of the discharge tube 1. In this figure, the taper 14 and the taper 15 are provided on both the laser gas introduction part and the laser gas discharge part of the discharge tube 1, but the taper may be provided on either side.
【0012】図2は、本実施例におけるレーザガス導入
部におけるテーパ角度(deg.)とガスレーザ発振装
置の圧力損失(Torr)の特性曲線図である。またレ
ーザガス排出部にテーパを設けた場合もこの図と同様な
特性を示し、レーザガス導入部、レーザガス排出部両方
にテーパを設けた場合はそれぞれにおける圧力損失が最
も小さいテーパ角度の組み合わせで、さらに圧力損失が
最小となる。FIG. 2 is a characteristic curve diagram of the taper angle (deg.) In the laser gas introducing portion and the pressure loss (Torr) of the gas laser oscillator in this embodiment. Also, when the laser gas discharge part has a taper, the same characteristics as this figure are shown.When both the laser gas introduction part and the laser gas discharge part are provided with a taper, the combination of the taper angles with the smallest pressure loss causes Minimal loss.
【0013】また図2から明らかなようにテーパ長50
mm以下のテーパを設けた場合にはテーパ角度5度から6
0度の範囲内にガスレーザ発振装置の圧力損失が最も小
さくなるテーパ角度が存在することがわかる。As is apparent from FIG. 2, the taper length 50
When a taper of mm or less is provided, the taper angle is 5 to 6 degrees.
It can be seen that the taper angle in which the pressure loss of the gas laser oscillator is the smallest exists within the range of 0 degree.
【0014】[0014]
【発明の効果】以上のように、本発明によれば放電管導
入、排出部にテーパを設けることによりレーザガス循環
路中の圧力損失が低下し、送風機の容量を小さくするこ
とができ小形で低価格なガスレーザ発振装置を提供でき
る。As described above, according to the present invention, by providing the discharge tube introducing / exhausting portion with a taper, the pressure loss in the laser gas circulation path is reduced, the capacity of the blower can be reduced, and the size and size are small. An inexpensive gas laser oscillator can be provided.
【図1】本発明の実施例におけるガスレーザ発振装置の
構成図FIG. 1 is a configuration diagram of a gas laser oscillator according to an embodiment of the present invention.
【図2】実施例におけるテーパ角度と圧力損失の特性曲
線図FIG. 2 is a characteristic curve diagram of taper angle and pressure loss in the example.
【図3】従来のガスレーザ発振装置の構成図FIG. 3 is a block diagram of a conventional gas laser oscillator.
【図4】従来のガスレーザ発振装置における放電管導
入、排出部の流れの状態を示す図FIG. 4 is a diagram showing a flow state of a discharge tube introduction / discharge portion in a conventional gas laser oscillator.
1 放電管 4 高圧電源 10 送気管 11 レーザガス冷却用熱交換器 12 レーザガス冷却用熱交換器 13 レーザガス循環用送風機 14 テーパ 15 テーパ DESCRIPTION OF SYMBOLS 1 Discharge tube 4 High-voltage power supply 10 Air supply pipe 11 Laser gas cooling heat exchanger 12 Laser gas cooling heat exchanger 13 Laser gas circulation blower 14 Taper 15 Taper
Claims (3)
管の途中に設けられたレーザガス循環用送風機と、レー
ザガス冷却用熱交換器と、誘電体よりなる放電管と、こ
の放電管内に放電を発生させる高圧電源とを備え、送気
管内径を放電管内径より大きく形成し、前記放電管のレ
ーザガス導入部または/およびレーザガス排出部にテー
パを備えたガスレーザ発振装置。1. An air supply pipe through which a laser gas flows, a blower for circulating a laser gas provided in the middle of the air supply pipe, a heat exchanger for cooling a laser gas, a discharge tube made of a dielectric material, and a discharge generated in the discharge tube. A gas laser oscillator device having a high voltage power supply, an inner diameter of an air supply tube formed larger than an inner diameter of a discharge tube, and a laser gas introduction portion and / or a laser gas discharge portion of the discharge tube having a taper.
60度のテーパ角度を有する請求項1記載のガスレーザ
発振装置。2. The gas laser oscillator according to claim 1, wherein the taper has a taper length of 50 mm or less and a taper angle of 5 to 60 degrees.
きく形成した請求項1記載のガスレーザ発振装置。3. The gas laser oscillator according to claim 1, wherein the inner diameter of the air supply tube is formed larger than the inner diameter of the discharge tube by 5 mm or more.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP11266893A JPH06326379A (en) | 1993-05-14 | 1993-05-14 | Gas laser oscillator |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP11266893A JPH06326379A (en) | 1993-05-14 | 1993-05-14 | Gas laser oscillator |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH06326379A true JPH06326379A (en) | 1994-11-25 |
Family
ID=14592496
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP11266893A Pending JPH06326379A (en) | 1993-05-14 | 1993-05-14 | Gas laser oscillator |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH06326379A (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP1248332A1 (en) * | 2000-05-30 | 2002-10-09 | Matsushita Electric Industrial Co., Ltd. | Laser oscillating device |
EP1315256A2 (en) * | 2000-05-30 | 2003-05-28 | Matsushita Electric Industrial Co., Ltd. | Laser oscillator |
US7664155B2 (en) | 2006-07-13 | 2010-02-16 | Fanuc Ltd | Gas laser oscillating unit |
CN114188801A (en) * | 2020-09-14 | 2022-03-15 | 中国科学院大连化学物理研究所 | Stimulated Raman scattering frequency conversion device for flowing gas |
-
1993
- 1993-05-14 JP JP11266893A patent/JPH06326379A/en active Pending
Cited By (9)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP1248332A1 (en) * | 2000-05-30 | 2002-10-09 | Matsushita Electric Industrial Co., Ltd. | Laser oscillating device |
EP1248332A4 (en) * | 2000-05-30 | 2003-01-29 | Matsushita Electric Ind Co Ltd | Laser oscillating device |
EP1315256A2 (en) * | 2000-05-30 | 2003-05-28 | Matsushita Electric Industrial Co., Ltd. | Laser oscillator |
EP1315256A3 (en) * | 2000-05-30 | 2003-11-05 | Matsushita Electric Industrial Co., Ltd. | Laser oscillator |
US6895030B1 (en) | 2000-05-30 | 2005-05-17 | Matsushita Electric Industrial Co., Ltd. | Laser oscillating device |
US6944200B2 (en) | 2000-05-30 | 2005-09-13 | Matsushita Electric Industrial Co., Ltd. | Laser oscillator |
US7664155B2 (en) | 2006-07-13 | 2010-02-16 | Fanuc Ltd | Gas laser oscillating unit |
CN114188801A (en) * | 2020-09-14 | 2022-03-15 | 中国科学院大连化学物理研究所 | Stimulated Raman scattering frequency conversion device for flowing gas |
CN114188801B (en) * | 2020-09-14 | 2023-11-17 | 中国科学院大连化学物理研究所 | Flowing gas stimulated Raman scattering frequency conversion device |
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