JPS63285988A - Laser oscillator - Google Patents

Laser oscillator

Info

Publication number
JPS63285988A
JPS63285988A JP12090787A JP12090787A JPS63285988A JP S63285988 A JPS63285988 A JP S63285988A JP 12090787 A JP12090787 A JP 12090787A JP 12090787 A JP12090787 A JP 12090787A JP S63285988 A JPS63285988 A JP S63285988A
Authority
JP
Japan
Prior art keywords
gas
laser
blower
pulsating
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
Application number
JP12090787A
Other languages
Japanese (ja)
Inventor
Norio Karube
規夫 軽部
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.)
Fanuc Corp
Original Assignee
Fanuc Corp
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 Fanuc Corp filed Critical Fanuc Corp
Priority to JP12090787A priority Critical patent/JPS63285988A/en
Publication of JPS63285988A publication Critical patent/JPS63285988A/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

Landscapes

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

Abstract

PURPOSE:To prevent laser gas from pulsating and to improve high speed stability by providing a pulsation preventing gas reservoir between a Root's blower and a discharge tube. CONSTITUTION:Laser gas is fed at a high speed by a Root's blower 6 in a discharge tube 1, and cooled by a collar 7 at the output side of the tube 1. A high frequency voltage of the frequency sufficient to cause an electron collection is supplied from an excitation power source 4 to generate a stable laser light 8. In order to prevent the laser gas from pulsating, a gas reservoir 9 is provided between the blower 6 and the tube. Thus, it can prevent the gas from pulsating to stabilize the output of the light. The volume V of the reservoir is given by V = 200 L/r, where L is the step volume of the blower 6 and r is compression ratio. A chamber is divided into three sections by partition plates 13a, 13b, and a pipe 10 for connecting them, and branch pipes 11, 12 are provided. The shape of the entirety can be largely reduced by the inductance effect of the pipes 10 and 11, 12 and the condenser effect of the partitioned chamber.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は金属などの切断加工用大出力レーザ発振装置に
関し、特にレーザガスの脈流を防止するようにしたレー
ザ発振装置に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a high-output laser oscillation device for cutting metals and the like, and particularly to a laser oscillation device designed to prevent pulsating flow of laser gas.

〔従来の技術〕[Conventional technology]

軸流CO2レーザは小型高出力レーザとして金属などの
切断加工用に盛んに使用されている。とくに、軸流CO
□レーザは横方向モード特性に優れている。
Axial flow CO2 lasers are widely used as small, high-power lasers for cutting metals and the like. In particular, axial CO
□Laser has excellent transverse mode characteristics.

第3図に従来の軸流CO□レーザの構成を示す。FIG. 3 shows the configuration of a conventional axial CO□ laser.

図において、■は放電管、2は全反射鏡、3は出力結合
鏡である。レーザガスは放電管l内をルーツブロワ6に
よって高速に流れ、放電管1の出力側で冷却器7によっ
て冷却される。5a及び5bは放電管1の外部に設けら
れた電極であり、電子捕捉現象を引き起こすに充分な周
波数の高周波電圧が励起用電源4から供給される。この
とき安定なレーザ光8が発生する。
In the figure, ■ is a discharge tube, 2 is a total reflection mirror, and 3 is an output coupling mirror. The laser gas flows through the discharge tube 1 at high speed by a Roots blower 6, and is cooled by a cooler 7 on the output side of the discharge tube 1. Reference numerals 5a and 5b are electrodes provided outside the discharge tube 1, to which a high-frequency voltage having a frequency sufficient to cause an electron trapping phenomenon is supplied from the excitation power source 4. At this time, stable laser light 8 is generated.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

しかし、軸流CO2レーザでは高速の出力安定性で、直
交型レーザや低速レーザに比べ劣ることがある。とくに
、加工の面粗さが直交型レーザや低速レーザに比較して
悪い。
However, axial CO2 lasers may be inferior to orthogonal lasers and low-speed lasers in terms of high-speed output stability. In particular, the surface roughness of machining is worse compared to orthogonal lasers and low-speed lasers.

この高速の不安定性は電源動作の揺らぎ、放電の揺らぎ
、レーザ発振器の機械的振動等があるが、特にルーツブ
ロワの脈流による要素も大きいことが経験的に判明した
。これを第4図に示す。図において、横軸は時間、縦軸
はレーザガスの圧力であり、脈流の周期は使用するルー
ツブロワによって変化する。これらの脈流はルーツブロ
ワ6が2葉のときは回転数×4の周波数で約12%程度
の脈流があり、ルーツブロワ6が3葉のときは回転数×
6の周波数で発生し、脈流の値は約8%程度である。レ
ーザ光の出力は放電管1内のレーザガスの圧力に大幅に
依存するので、これらの脈流は当然に加工に対しても悪
影響を及ぼす。
This high-speed instability is caused by fluctuations in power supply operation, discharge fluctuations, mechanical vibrations in the laser oscillator, etc., but it has been empirically found that the pulsating flow in the Roots blower is a particularly large factor. This is shown in FIG. In the figure, the horizontal axis is time, the vertical axis is laser gas pressure, and the period of the pulsating flow changes depending on the Roots blower used. When the roots blower 6 has two leaves, there is a pulsating flow of about 12% at the frequency of rotation speed x 4, and when the roots blower 6 has three leaves, the frequency is about 12%.
It occurs at a frequency of 6, and the value of pulsating flow is about 8%. Since the output of the laser beam largely depends on the pressure of the laser gas within the discharge tube 1, these pulsating currents naturally have a negative effect on processing.

本発明の目的は上記問題点を解決し、レーザガスのi流
を防止するようにしたレーザ発振装置を提供することに
ある。
SUMMARY OF THE INVENTION An object of the present invention is to solve the above problems and provide a laser oscillation device that prevents the i-flow of laser gas.

〔問題点を解決するだめの手段〕 本発明では上記の問題点を解決するために、第1図に示
すように、 ルーツブロワ(6)からの吐出ガスを放電管(1)に導
いてレーザ発振を行わせるレーザ発振装置において、 ルーツブロワ(6)と放電管(1)の間にレーザガス脈
流防止機能を有するガス溜め(9)を設けたことを特徴
とするレーザ発振装置が、提供される。
[Means for Solving the Problems] In order to solve the above problems, the present invention, as shown in FIG. Provided is a laser oscillation device that is characterized in that a gas reservoir (9) having a function of preventing laser gas pulsation is provided between the Roots blower (6) and the discharge tube (1).

〔作用〕[Effect]

ガス溜めによって、ガスの脈流を吸収して、レーザ光の
出力を安定させる。
The gas reservoir absorbs the pulsating gas flow and stabilizes the output of the laser light.

〔実施例〕〔Example〕

以下本発明の一実施例を図面に基づいて説明する。 An embodiment of the present invention will be described below based on the drawings.

第1図に本発明の一実施例のブロック図を示す。FIG. 1 shows a block diagram of an embodiment of the present invention.

第1図において、lは放電管、2は全反射鏡、3は出力
結合鏡である。レーザガスは放電管1内をルーツブロワ
6によって高速に流れ、放電管1の出力側で冷却器7に
よって冷却される。5a及び5bは放電管1の外部に設
けられた電極であり、電子捕捉現象を引き起こすに充分
な周波数の高周波電圧が励起用電源4から供給される。
In FIG. 1, l is a discharge tube, 2 is a total reflection mirror, and 3 is an output coupling mirror. The laser gas flows through the discharge tube 1 at high speed by a Roots blower 6, and is cooled by a cooler 7 on the output side of the discharge tube 1. Reference numerals 5a and 5b are electrodes provided outside the discharge tube 1, to which a high-frequency voltage having a frequency sufficient to cause an electron trapping phenomenon is supplied from the excitation power source 4.

このとき安定なレーザ光8が発生する。そしてレーザガ
スの風流を防止するために、ルーツブロワ6と放電管の
間にガス溜め9を追加している。これによって、レーザ
ガスの脈流を防止し、レーザ光の出力を安定させる。こ
のガス溜めの体積Vはルーツブロワ6の工程容積をLと
し、圧縮比をrとすると、V=200L/r で与えられるものを使用すると効果的である。例えば、
3葉のルーツブロワを使用したときのガス溜めの容積の
一例を示すと、 50H2での送風1 890m”/H 工程容積      0.824L 圧縮率       1.67 から約100リツトルとなり、相当大容量のガス溜めが
必要になる。
At this time, stable laser light 8 is generated. A gas reservoir 9 is added between the Roots blower 6 and the discharge tube to prevent the laser gas from flowing. This prevents pulsating flow of laser gas and stabilizes the output of laser light. It is effective to use the volume V of this gas reservoir given by V=200L/r, where L is the process volume of the Roots blower 6 and r is the compression ratio. for example,
An example of the volume of the gas reservoir when using a three-leaf Roots blower is as follows: Air blowing at 50H2 1 890 m"/H Process volume 0.824 L Compression ratio 1.67 It becomes approximately 100 liters, which is a fairly large capacity gas reservoir. is required.

第2図にガス溜め9の他の構成を示す。これは上記の中
空の場合に比べて、その容積を小さくするものである。
FIG. 2 shows another configuration of the gas reservoir 9. This reduces the volume compared to the hollow case described above.

図において、13a及び13bの境板で室を3個に仕切
り、それぞれを連結するパイプ10及びブランチパイプ
11及び12を設けたものである。これらのパイプエ0
とブランチパイプII及びI2のインダクタンス効果と
仕切られた室のコンデンサ効果により、全体の形状を大
幅に減少させることができる。脈流防止を行うときはガ
ス流の共振周波数が脈流の周波数と一致しないように注
意する必要がある。
In the figure, the chamber is partitioned into three by boundary plates 13a and 13b, and a pipe 10 and branch pipes 11 and 12 are provided to connect each part. These pipes 0
Due to the inductance effect of the branch pipes II and I2 and the capacitor effect of the partitioned chamber, the overall shape can be significantly reduced. When preventing pulsating flow, care must be taken to ensure that the resonance frequency of the gas flow does not match the frequency of the pulsating flow.

上記の★施例では、ガス溜めは単独で構成されているが
、ガス溜めと冷却器を一体にして、共通部の部品を省略
することも可能である。
In the above embodiment, the gas reservoir is constructed independently, but it is also possible to integrate the gas reservoir and the cooler and omit common parts.

〔発明の効果〕〔Effect of the invention〕

以上説明したように本発明では、ルーツブロワと放電管
の間に脈流防止のガス溜めを設けたので、レーザガスの
脈流を防止し、軸流CO□レーザの長所である小型、高
出力及び横方向モードの緒特性を維持したままで、高速
安定性を高めることができる。
As explained above, in the present invention, a gas reservoir to prevent pulsation is provided between the Roots blower and the discharge tube, which prevents pulsation of the laser gas. High-speed stability can be improved while maintaining the directional mode characteristics.

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

第1図は本発明の一実施例のブロック図、第2図は他の
ガス溜めの構成図、 第3図は従来の軸流CO□レーザのブロック図、第4図
はレーザガスの脈流を示す図である。 1−・・−・−−一一−−放電管 2−−−−−−−−−−−−−−一全反射鏡3−−−−
−−一・−一一−−−−出力結合鏡4−・−・・−・−
・−励起用電源 6・−・−・−・−・−ルーツブロワ 9−・・−・−・−ガス溜め 10・−−−−一−・・・・・−結合パイブ11−・−
・−・・・・・−ブランチパイプ12・−・−・−・−
・−・−ブランチパイプ13a・・・・・−・−・−境
板 13 b−・−・・・境板 特許出願人 ファナック株式会社 代理人   弁理士  服部殺巖 4励に用電源 第1図 第2図 4励起田電逓 第3図 第4図
Fig. 1 is a block diagram of an embodiment of the present invention, Fig. 2 is a configuration diagram of another gas reservoir, Fig. 3 is a block diagram of a conventional axial flow CO□ laser, and Fig. 4 shows a pulsating flow of laser gas. FIG. 1-・・-・--11--Discharge tube 2----------1 total reflection mirror 3--
−−1・−11−−−Output coupling mirror 4−・−・・−・−
- Excitation power supply 6 - Roots blower 9 - Gas reservoir 10 - - - - Connection pipe 11 - -
・−・・・−Branch pipe 12・−・−・−・−
・−・−Branch pipe 13a・・・・・−・−・−Boundary plate 13 b−・−・Boundary plate Patent applicant FANUC Co., Ltd. agent Patent attorney Hattori Sakugan 4th power supply Figure 1 Fig. 2 4 Excited Field Transmission Fig. 3 Fig. 4

Claims (3)

【特許請求の範囲】[Claims] (1)ルーツブロワからの吐出ガスを放電励起部に導い
てレーザ発振を行わせるレーザ発振装置において、 ルーツブロワと放電励起部の間にレーザガス脈流防止機
能を有するガス溜めを設けたことを特徴とするレーザ発
振装置。
(1) A laser oscillation device that conducts laser oscillation by guiding gas discharged from a roots blower to a discharge excitation part, characterized in that a gas reservoir having a function of preventing laser gas pulsation is provided between the roots blower and the discharge excitation part. Laser oscillation device.
(2)前記ガス溜めが中空構造であることを特徴とする
特許請求の範囲第1項記載のレーザ発振装置。
(2) The laser oscillation device according to claim 1, wherein the gas reservoir has a hollow structure.
(3)前記ガス溜めが、境板によって隔離された複数の
室と、該室を結合するパイプとから構成されていること
を特徴とする特許請求の範囲第1項記載のレーザ発振装
置。
(3) The laser oscillation device according to claim 1, wherein the gas reservoir is composed of a plurality of chambers separated by a boundary plate and a pipe connecting the chambers.
JP12090787A 1987-05-18 1987-05-18 Laser oscillator Pending JPS63285988A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP12090787A JPS63285988A (en) 1987-05-18 1987-05-18 Laser oscillator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP12090787A JPS63285988A (en) 1987-05-18 1987-05-18 Laser oscillator

Publications (1)

Publication Number Publication Date
JPS63285988A true JPS63285988A (en) 1988-11-22

Family

ID=14797949

Family Applications (1)

Application Number Title Priority Date Filing Date
JP12090787A Pending JPS63285988A (en) 1987-05-18 1987-05-18 Laser oscillator

Country Status (1)

Country Link
JP (1) JPS63285988A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02281674A (en) * 1989-04-21 1990-11-19 Matsushita Electric Ind Co Ltd Gas laser device
JPH02281673A (en) * 1989-04-21 1990-11-19 Matsushita Electric Ind Co Ltd Gas laser device

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02281674A (en) * 1989-04-21 1990-11-19 Matsushita Electric Ind Co Ltd Gas laser device
JPH02281673A (en) * 1989-04-21 1990-11-19 Matsushita Electric Ind Co Ltd Gas laser device

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