JP2658505B2 - Laser oscillation device - Google Patents

Laser oscillation device

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Publication number
JP2658505B2
JP2658505B2 JP2143492A JP14349290A JP2658505B2 JP 2658505 B2 JP2658505 B2 JP 2658505B2 JP 2143492 A JP2143492 A JP 2143492A JP 14349290 A JP14349290 A JP 14349290A JP 2658505 B2 JP2658505 B2 JP 2658505B2
Authority
JP
Japan
Prior art keywords
glass tube
cooling water
ring
peripheral surface
receiving portion
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
Application number
JP2143492A
Other languages
Japanese (ja)
Other versions
JPH0437176A (en
Inventor
崇弘 長嶋
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.)
Fuji Electric Co Ltd
Original Assignee
Fuji Electric 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 Fuji Electric Co Ltd filed Critical Fuji Electric Co Ltd
Priority to JP2143492A priority Critical patent/JP2658505B2/en
Publication of JPH0437176A publication Critical patent/JPH0437176A/en
Application granted granted Critical
Publication of JP2658505B2 publication Critical patent/JP2658505B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【産業上の利用分野】 この発明は、レーザロッドを内部に収容するガラス管
の両端部での冷却水漏洩を抑えることによって、レーザ
出力の変動を抑制するレーザ発振装置に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a laser oscillation device that suppresses fluctuations in laser output by suppressing leakage of cooling water at both ends of a glass tube containing a laser rod therein.

【従来の技術】[Prior art]

従来例について、その要部の側断面図である第2図を
参照しながら説明する。第2図において、1はレーザ媒
質としてのYAGロッド、2はこのYAGロッドを両端でそれ
ぞれ保持するホルダ、7はガラス管、6,8はそれぞれ側
板である。 ガラス管7は、内部にYAGロッド1を軸線を一致させ
て収容する。各側板6,8は、ガラス管7を各端部で軸線
方向と半径方向とにそれぞれ遊隙をもたせれ保持する。
遊隙をもたせるのは、ガラス管7の脆性に対する対策で
ある。両端部を固定する構造であると、熱変形などを逃
がすことができずに破損につながる。したがって、軸
線,半径の各方向にガラス管7の変形,変位を許容する
構造にする必要がある。 この遊隙は、軸線方向に0.5〜1mm、半径方向に0.2〜
0.4mm程度と比較的大きくなる。その理由は、ガラス管
7の寸法に性質上どうしてもバラツキがあるからであ
る。たとえば、内径,外径,長さの各寸法が、9.2,11.
2,80mmで、各公差がそれぞれ±0.2mmである。なお、相
手側の各側板6,8は銅合金材料からなるので、機械加工
によって寸法公差を小さくし得る。 各側板6,8の対向空間には、ここでは図示してない
が、励起ランプと反射体とが設けられ、励起ランプの発
熱を吸収,排出するための冷却水が循環する。この励起
ランプ用の冷却水と系統的には連通するYAGロッド1用
の冷却水が、実線矢印のように、左側のホルダ2の外周
に沿って流入し、側板8の中心孔を通り、YAGロッド1
とガラス管7との空隙を流路として流れ、右側の側板6
の中心孔を通り、右側のホルダ2の外周に沿って流出す
る。ガラス管7は、YAGロッド用冷却水の流路を形成す
るとともに、励起ランプに対するUVフィルタの役割をも
つ。
A conventional example will be described with reference to FIG. 2 which is a sectional side view of a main part thereof. In FIG. 2, 1 is a YAG rod as a laser medium, 2 is a holder for holding the YAG rod at both ends, 7 is a glass tube, and 6 and 8 are side plates, respectively. The glass tube 7 accommodates the YAG rod 1 therein with its axis aligned. Each of the side plates 6 and 8 holds the glass tube 7 with play at both ends in the axial direction and the radial direction.
Providing a play is a measure against the brittleness of the glass tube 7. With a structure in which both ends are fixed, thermal deformation and the like cannot be escaped, leading to breakage. Therefore, it is necessary to provide a structure that allows deformation and displacement of the glass tube 7 in each direction of the axis and the radius. This clearance is 0.5 to 1 mm in the axial direction and 0.2 to 1 in the radial direction.
It is relatively large, about 0.4 mm. The reason for this is that the dimensions of the glass tube 7 vary in nature. For example, if the inner diameter, outer diameter, and length dimensions are 9.2,11.
2,80mm, each tolerance is ± 0.2mm. Since the mating side plates 6, 8 are made of a copper alloy material, the dimensional tolerance can be reduced by machining. Although not shown here, an excitation lamp and a reflector are provided in the space facing each side plate 6, 8, and cooling water for absorbing and discharging heat generated by the excitation lamp circulates. The cooling water for the YAG rod 1 which systematically communicates with the cooling water for the excitation lamp flows along the outer periphery of the left holder 2 as shown by the solid line arrow, passes through the center hole of the side plate 8, and Rod 1
Flows through the gap between the glass tube 7 and the right side plate 6
And flows out along the outer periphery of the right holder 2. The glass tube 7 forms a flow path of the cooling water for the YAG rod and has a role of a UV filter for the excitation lamp.

【発明が解決しようとする課題】[Problems to be solved by the invention]

以上説明したような従来の技術では、第2図に示すよ
うに、YAGロッド1用冷却水の動圧によって、ガラス管
7の右端面が側板6の受面に押圧されるから、この箇所
からの冷却水の漏れはほとんど阻止される。しかし、冷
却水の流入側(上流側)のガラス管7の外周面と、側板
8の受部の内周面との間に、0.2〜0.4mm程度の遊隙があ
り、またガラス管7の左端面と側板8の受面との間に
も、0.5〜1mm程度の遊隙がある。したがって、破線矢印
のように、この箇所からの冷却水の漏れが生じる。その
漏れの主要因は、ガラス管7の外周面と、側板8の受部
の内周面との間の遊隙、つまり半径方向の遊隙にある。 この冷却水の漏れ自体も冷却効率を悪化させるためよ
くないが、さらに漏れの程度が細かく変動するから、YA
Gロッド1の冷却の度合が変動し、ひいてはレーザ出力
が変動するという問題がある。このレーザ出力の変動
は、レーザが加工に用いられるときには、加工能力をを
変動させて加工品質を低下させる。 この発明の課題は、従来の技術がもつ以上の問題点を
解消し、レーザロッドを内部に収容するガラス管の両端
部での冷却水漏洩を抑えることによって、レーザ出力の
変動を抑制するレーザ発振装置を提供することにある。
In the prior art described above, the right end face of the glass tube 7 is pressed against the receiving face of the side plate 6 by the dynamic pressure of the cooling water for the YAG rod 1 as shown in FIG. Of the cooling water is almost prevented. However, there is a clearance of about 0.2 to 0.4 mm between the outer peripheral surface of the glass tube 7 on the inflow side (upstream side) of the cooling water and the inner peripheral surface of the receiving portion of the side plate 8. There is also a gap of about 0.5 to 1 mm between the left end face and the receiving face of the side plate 8. Therefore, leakage of the cooling water from this location occurs as indicated by the broken arrow. The main cause of the leakage is the play between the outer peripheral surface of the glass tube 7 and the inner peripheral surface of the receiving portion of the side plate 8, that is, the play in the radial direction. This leakage of cooling water itself is not good because it deteriorates the cooling efficiency, but since the degree of leakage varies more finely,
There is a problem that the degree of cooling of the G rod 1 fluctuates and, consequently, the laser output fluctuates. This fluctuation in the laser output, when the laser is used for processing, changes the processing capability and lowers the processing quality. The object of the present invention is to solve the above problems of the prior art, and to suppress cooling water leakage at both ends of a glass tube containing a laser rod therein, thereby suppressing laser output fluctuation. It is to provide a device.

【課題を解決するための手段】[Means for Solving the Problems]

この課題を解決するために、本発明に係るレーザ発振
装置は、 中空部にレーザロッドを同軸に収容するガラス管と; このガラス管の少なくとも一方の端部にフランジ状に固
着され寸法精度の出しやすいリングと; このリングまたは前記ガラス管端部を、その軸線方向と
半径方向とにそれぞれ遊隙をもたせて支える各受部と; 前記リングに対応する一方の側の前記受部の中心孔から
流入し、前記レーザロッドの外周面と前記ガラス管の内
周面との間に形成される空隙を経て、他方の側の前記受
部の中心孔から流出する冷却水と;を備え、 この冷却水の動圧によって下流側の前記ガラス管の端面
または前記リングの端面が、対応する前記受部の受面に
押圧される。
In order to solve this problem, a laser oscillation device according to the present invention comprises: a glass tube which accommodates a laser rod coaxially in a hollow portion; and a flange-shaped fixture at least at one end of the glass tube to obtain dimensional accuracy. An easy ring; and respective receiving portions for supporting the ring or the end portion of the glass tube with play in the axial direction and the radial direction thereof; and a center hole of the receiving portion on one side corresponding to the ring. Cooling water flowing in and flowing out of a center hole of the receiving portion on the other side through a gap formed between the outer peripheral surface of the laser rod and the inner peripheral surface of the glass tube; The end face of the glass tube or the end face of the ring on the downstream side is pressed against the receiving face of the corresponding receiving part by the dynamic pressure of water.

【作用】[Action]

冷却水は、リング外周面と、対応する受部の内周面と
の遊隙を小さくできるから、ガラス管の上流側端部箇所
からの漏れが抑制され、また下流側端部箇所について
も、動圧によってガラス管端面またはリング端面が、対
応する受部の受面に押圧されるから、そこからの漏れが
抑制される。
Since the cooling water can reduce the play between the outer peripheral surface of the ring and the inner peripheral surface of the corresponding receiving portion, leakage from the upstream end portion of the glass tube is suppressed, and also regarding the downstream end portion, Since the end face of the glass tube or the end face of the ring is pressed against the receiving surface of the corresponding receiving portion by the dynamic pressure, leakage therefrom is suppressed.

【実施例】【Example】

本発明に係るレーザ発振装置の実施例について以下に
第1図を参照しながら説明する。第1図は実施例の要部
の側断面図である。 第1図において、この実施例が第2図の従来例と異な
る点は、ガラス管の上流側端部に外径の寸法精度の出た
リングをフランジ状に固着し、対応する側板の受部との
間の遊隙を小さくすることである。すなわち、4はテフ
ロン(デュポン社登録商標)からなる方形断面のリング
で、機械加工によって寸法精度を十分出し得る。側板5
の中心孔に加工された円筒状中空部の受部も、側板5が
銅合金材料であるから、機械加工によって寸法精度を十
分出し得る。 具体的には、リング4の外周面と、側板5の受部内周
面との遊隙、つまり半径方向の遊隙を0.1mm以下の程度
に小さくでき、ひいてはこの箇所での冷却水の流れ抵抗
を大きくなし得る。なお、リング4の左端面と側板5の
受面との間の遊隙、つまり軸線方向の遊隙の流れ抵抗に
及ぼす影響は、半径方向の遊隙のそれより小さい。その
ため、この箇所での流れ抵抗を大きくするには、半径方
向の遊隙だけを小さくすることで十分である。 したがって、冷却水の流れの、ガラス管3の左端部箇
所からの漏れが抑制される。また、ガラス管3の右端部
からの漏れは、もともと抑制されている。これは、従来
例におけるのと同様に、冷却水の動圧によってガラス管
3の右端面と側板6の受面とが押圧され密接しているか
らである。 ところで、実施例でのリングは、ガラス管の冷却水流
入側(上流側)端部だけに固着され、これで冷却水の漏
れ、ひいてはレーザ出力の変動は実用上支障ののない程
度に抑制された。しかし、リングをガラス管の両側の各
端部に固着した方が、冷却水の漏れをさらに抑えること
ができ、ひいてはレーザ出力の変動を抑える効果も大き
くなると考えられる。
An embodiment of the laser oscillation device according to the present invention will be described below with reference to FIG. FIG. 1 is a side sectional view of a main part of the embodiment. In FIG. 1, this embodiment is different from the conventional example of FIG. 2 in that a ring having an outer diameter dimensional accuracy is fixed to the upstream end of the glass tube in a flange shape, and a corresponding receiving portion of the side plate is provided. Is to reduce the play between them. That is, reference numeral 4 denotes a ring having a rectangular cross section made of Teflon (registered trademark of DuPont), which can provide sufficient dimensional accuracy by machining. Side plate 5
Since the side plate 5 is made of a copper alloy material, the receiving portion of the cylindrical hollow portion formed in the center hole of the above can also provide sufficient dimensional accuracy by machining. Specifically, the clearance between the outer peripheral surface of the ring 4 and the inner peripheral surface of the receiving portion of the side plate 5, that is, the clearance in the radial direction can be reduced to about 0.1 mm or less, and the flow resistance of the cooling water at this point can be reduced. Can be greatly increased. The play between the left end face of the ring 4 and the receiving surface of the side plate 5, that is, the influence of the play in the axial direction on the flow resistance is smaller than that in the play in the radial direction. Therefore, in order to increase the flow resistance at this point, it is sufficient to reduce only the play in the radial direction. Therefore, leakage of the flow of the cooling water from the left end portion of the glass tube 3 is suppressed. In addition, leakage from the right end of the glass tube 3 is originally suppressed. This is because, similarly to the conventional example, the right end face of the glass tube 3 and the receiving face of the side plate 6 are pressed by the dynamic pressure of the cooling water to be in close contact with each other. By the way, the ring in the embodiment is fixed only to the cooling water inflow side (upstream side) end of the glass tube, whereby the leakage of the cooling water and, consequently, the fluctuation of the laser output are suppressed to a level that does not hinder practical use. Was. However, it is considered that, when the ring is fixed to each end on both sides of the glass tube, the leakage of the cooling water can be further suppressed, and the effect of suppressing the fluctuation of the laser output is further increased.

【発明の効果】【The invention's effect】

以上説明したように、この発明においては、冷却水
は、リング外周面と、対応する受部の内周面との遊隙を
小さくできるから、ガラス管の上流側端部箇所からの漏
れが抑制され、また下流側端部箇所についても、動圧に
よってガラス管端面またはリング端面が、対応する受部
の受面に押圧されるから、そこからの漏れが抑制され
る。 したがって、この発明によれば、従来技術に比べて次
のようなすぐれた効果がある。 (1) 冷却水は、そのガラス管の上流側,下流側の各
端部箇所からの漏れが抑制されるから、流れが安定化
し、そのためのレーザ出力の変動が抑制されて、そのレ
ーザが加工に用いられる場合には加工能力が向上する。 (2) また、(1)項に関連して、ガラス管の寸法公
差を特に抑える必要がないから、生産性向上コスト低減
とが図れる。
As described above, in the present invention, since the cooling water can reduce the play gap between the outer peripheral surface of the ring and the inner peripheral surface of the corresponding receiving portion, the leakage from the upstream end portion of the glass tube is suppressed. At the downstream end portion, the end face of the glass tube or the end face of the ring is pressed against the receiving surface of the corresponding receiving portion by the dynamic pressure, so that leakage therefrom is suppressed. Therefore, according to the present invention, the following excellent effects are obtained as compared with the related art. (1) Cooling water is prevented from leaking from the upstream and downstream ends of the glass tube, so that the flow is stabilized and the fluctuation of the laser output is suppressed, and the laser is processed. When it is used for, the processing ability is improved. (2) Further, since it is not necessary to particularly suppress the dimensional tolerance of the glass tube in relation to the item (1), productivity can be improved and cost can be reduced.

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

第1図は本発明に係る実施例の要部の側断面図、第2図
は従来例の要部の側断面図である。 符号説明 1:YAGロッド、2:ホルダ、3:ガラス管、4:リング、5,6:
側板。
FIG. 1 is a side sectional view of a main part of an embodiment according to the present invention, and FIG. 2 is a side sectional view of a main part of a conventional example. Description of symbols 1: YAG rod, 2: holder, 3: glass tube, 4: ring, 5, 6:
Side plate.

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】中空部にレーザロッドを同軸に収容するガ
ラス管と;このガラス管の少なくとも一方の端部にフラ
ンジ状に固着される寸法精度の出しやすいリングと;こ
のリングまたは前記ガラス管端部を、その軸線方向と半
径方向とにそれぞれ遊隙をもたせて支える各受部と;前
記リングに対応する一方の側の前記受部の中心孔から流
入し、前記レーザロッドの外周面と前記ガラス管の内周
面との間に形成される空隙を経て、他方の側の前記受部
の中心孔から流出する冷却水と;を備え、この冷却水の
動圧によって下流側の前記ガラス管の端面または前記リ
ングの端面が、対応する前記受部の受面に押圧される構
成にしたことを特徴とするレーザ発振装置。
1. A glass tube in which a laser rod is coaxially accommodated in a hollow portion; a ring easily fixed in a flange shape to at least one end of the glass tube; And a receiving portion for supporting the portion with a play in the axial direction and the radial direction, respectively; and a central portion of the receiving portion on one side corresponding to the ring, and an outer peripheral surface of the laser rod and the outer peripheral surface of the laser rod. Cooling water flowing out of a center hole of the receiving portion on the other side through a gap formed between the glass tube and the inner peripheral surface of the glass tube; Or an end surface of the ring is pressed against a corresponding receiving surface of the receiving portion.
JP2143492A 1990-06-01 1990-06-01 Laser oscillation device Expired - Lifetime JP2658505B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2143492A JP2658505B2 (en) 1990-06-01 1990-06-01 Laser oscillation device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2143492A JP2658505B2 (en) 1990-06-01 1990-06-01 Laser oscillation device

Publications (2)

Publication Number Publication Date
JPH0437176A JPH0437176A (en) 1992-02-07
JP2658505B2 true JP2658505B2 (en) 1997-09-30

Family

ID=15339971

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2143492A Expired - Lifetime JP2658505B2 (en) 1990-06-01 1990-06-01 Laser oscillation device

Country Status (1)

Country Link
JP (1) JP2658505B2 (en)

Also Published As

Publication number Publication date
JPH0437176A (en) 1992-02-07

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