JPS6173820A - Laser hardening device - Google Patents
Laser hardening deviceInfo
- Publication number
- JPS6173820A JPS6173820A JP59195651A JP19565184A JPS6173820A JP S6173820 A JPS6173820 A JP S6173820A JP 59195651 A JP59195651 A JP 59195651A JP 19565184 A JP19565184 A JP 19565184A JP S6173820 A JPS6173820 A JP S6173820A
- Authority
- JP
- Japan
- Prior art keywords
- reflecting mirror
- rotating body
- hardening
- laser
- angle
- 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
Landscapes
- Laser Beam Processing (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
この発明ば、レーザ焼入れ装置に係シ、特に回転多面反
射鏡を用いたレーザ焼入れ装置に関するものである。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a laser hardening device, and more particularly to a laser hardening device using a rotating polygonal reflecting mirror.
従来、この種の装置としては、第5図に示すようなもの
(機械と工具、APR,1984P−58)があった。Conventionally, as this type of apparatus, there has been one shown in FIG. 5 (Machines and Tools, APR, 1984P-58).
図において、(1)け多角柱状または多角錐状の多面反
射鏡を構成する回転体、(2)け回転体(1)を回転速
度2000〜10000r、p、m程度に高速回転させ
る高速モータ、(3)はレーザ発振ヘッドからのレーザ
ビームを集光して多面反射鏡に照射し、その反射ビーム
の焦点を被加工物Wの表面近傍で結ばせるゲルマニウム
製のレンズである。In the figure, (1) a rotating body constituting a polygonal prism-shaped or polygonal pyramid-shaped polygonal reflecting mirror, (2) a high-speed motor that rotates the rotating body (1) at a high speed of about 2000 to 10000 r, p, m; (3) is a germanium lens that condenses the laser beam from the laser oscillation head and irradiates it onto the polygonal reflecting mirror, and focuses the reflected beam near the surface of the workpiece W.
次に、作用について説明する。レーザ発振ヘッドからの
レーザビームは、レンズ(3)により集光されて、モー
タ(2)によシ高速で回転する回転体(1)の各使面(
1at)〜(1an)に照射されて反射し、一定速度、
例えば約1m/minで移動する被加工物Wの金属表面
近傍に焦点を結び、その集中されたビームエネルギで被
加工物Wの金属表面を加熱し、表面焼入れを行う。この
場合、回転体(1)は高速で回転しているので、各反射
鏡面(1a+ )−(law )・・・・・・(1an
)と順次に反射される。この各反射鏡面での反射は、回
転によシ前面との稜線から平板状鏡面全経て次の面との
稜線へと移動しながら行なわれ、回転による入・反射角
の変化により、被加工物Wの表面における焦点(4)を
所定の幅で線状に走査するように移動させる。一方、被
加工物Wは一定速度で走査焦点線(4)とは直角方向に
移動しているので、各反射鏡面(la、)〜(Ian)
による走査焦点線(4)は平行となるように移勲し、金
属表面を所定の幌で焼入n処理する。Next, the effect will be explained. The laser beam from the laser oscillation head is focused by a lens (3) and is focused on each surface (
1at) to (1an) and reflected, at a constant speed,
For example, the beam is focused near the metal surface of the workpiece W moving at about 1 m/min, and the concentrated beam energy heats the metal surface of the workpiece W to perform surface hardening. In this case, since the rotating body (1) is rotating at high speed, each reflecting mirror surface (1a+) - (law)... (1an
) and are reflected sequentially. Reflection on each reflecting mirror surface is performed while moving from the ridge line with the front surface to the ridge line with the next surface through the entire flat mirror surface, and due to the change in the angle of incidence and reflection due to the rotation, the reflection on the workpiece The focal point (4) on the surface of W is moved so as to scan linearly with a predetermined width. On the other hand, since the workpiece W is moving at a constant speed in a direction perpendicular to the scanning focal line (4), each reflecting mirror surface (la,) to (Ian)
The scanning focal lines (4) are moved parallel to each other, and the metal surface is hardened with a predetermined hood.
上記のよりな従来のレーザ焼入れ装置は、多面反射鏡の
各反射鏡面が軸心より等距離に取付けられているので、
各反射鏡面による走査焦点線は、被加工物の移動と回転
体の回転速度とに応じた幅で平行に、かつ順次に14接
する。従って、レーザビームによる単位面積における単
位時間当夛のビームエネルギの集中度は、線状に間り力
って表面溶融を生じ、焼入れ性能を悪化させる。特に、
焼入れ部分の両端では、エネルギ集中度が特に高くなっ
て均一な焼入れが行えず、かつ溶融による表面状態の悪
化が生じていた。また、線状の焼入九処理となるので、
ビームの形(モード、集光性)の影響を受は易く、均一
な焼入れができない、等の問題虚があった。In the conventional laser hardening equipment described above, each reflective mirror surface of the multifaceted mirror is installed at an equal distance from the axis, so
The scanning focal lines of each reflecting mirror surface touch 14 times in parallel and sequentially with a width corresponding to the movement of the workpiece and the rotational speed of the rotating body. Therefore, the degree of concentration of beam energy per unit time in a unit area by a laser beam causes linear cracking force, which causes surface melting and deteriorates hardening performance. especially,
At both ends of the hardened portion, the degree of energy concentration was particularly high, making it impossible to achieve uniform hardening, and the surface condition deteriorated due to melting. In addition, since it is a linear quenching process,
It is easily affected by the shape of the beam (mode, light focusing ability), and there are problems such as uniform hardening being impossible.
この発BAは、かかる問題を解決するためになされるも
ので、良好な炉入れ性能を得られるようにしたレーザ焼
入れ装Rを提供することを目的とする0
〔問題点?解決するための手段〕
この発明に係るレーザ焼入れ装置は、回転体に構成され
る多面反射Cの各反射鏡面の取付は角度を、jiii次
て所定角度差ずつ異ならせたこと?]−特徴とする。This BA is made to solve such problems, and the purpose is to provide a laser hardening equipment R that can obtain good furnace hardening performance.0 [Problems? Means for Solving] In the laser hardening apparatus according to the present invention, the mounting angles of the respective reflecting mirror surfaces of the multifaceted reflection C formed on the rotating body are made to differ by a predetermined angle difference. ]-Characteristics.
この発明は、上記のように構成さnているので、夫々の
反射鏡面における側端から側端までの反射によるビーム
焦点の移動は従来例と同様であるが、隣接する反射鏡面
による平行した走査焦点線間の距離は、反射鏡面の取付
角度差に応じた幅だけ離間し、回転体の高速回転と被加
工物の一定速度移動とにより、所定面内での複数走査焦
点線、即ち矩形面状にビームエネルギを分散して照射す
るようになる。従って、焼入れ処理面におけるビームエ
ネルギのが対時間が長くなり、表面溶融状態を生じるこ
となく、焼入れ深さ′!!−深くすることかでき、かつ
、焼入れ部分の両端部におけるビームエネルギの過照射
(1回避される。Since the present invention is configured as described above, movement of the beam focus due to reflection from side edge to side edge on each reflecting mirror surface is the same as in the conventional example, but parallel scanning by adjacent reflecting mirror surfaces is possible. The distance between the focal lines is separated by a width corresponding to the difference in the mounting angle of the reflecting mirror surfaces, and by the high-speed rotation of the rotating body and the constant speed movement of the workpiece, multiple scanning focal lines within a predetermined plane, that is, a rectangular plane. The beam energy is distributed and irradiated. Therefore, the beam energy vs. time on the hardened surface becomes longer, and the hardening depth can be increased without causing surface melting. ! - can be deepened and over-irradiation of the beam energy at both ends of the hardened part (1 avoided);
また、面状の焼入れとなるので、レーザビームの形(モ
ード、集光性)の影響を受けることなく、均一な焼入れ
?行うことができる。Also, since it is a planar hardening, it is uniformly hardened without being affected by the shape of the laser beam (mode, light focusing ability). It can be carried out.
以下、この発明による一実施例を図によって説明する。 Hereinafter, one embodiment of the present invention will be described with reference to the drawings.
第1図において、(1)は回転体、(1,) 〜(1
,、)は何転体(IHに所定の角度差で順次に取付けら
れた各反射鏡面、(2)は回転体(1)を高速回転させ
るモータ、(3)はゲルマニウム製のレンズ、(4,)
〜(4tz )σ各反射釧面による被加工物W上の走査
焦点線である。In Figure 1, (1) is a rotating body, (1,) ~ (1
,,) are the rotating bodies (reflecting mirror surfaces sequentially attached to the IH at a predetermined angle difference, (2) is the motor that rotates the rotating body (1) at high speed, (3) is the germanium lens, (4) ,)
~(4tz) σ is the scanning focal line on the workpiece W by each reflecting surface.
次に、作用について説明する。回転体(1)に取付けら
れた各反射鏡面(1,)〜(1□、)は、第2図及び第
5図に示すように、軸線に対しての取付角度を、(1、
)は11θ、(1□)け10θ、と順次角度を6ずつ異
ならせて配置されている。こうして、レーf発m体ヘッ
ドからのレーザビームは、レンズ(3)によシ集光され
て、モータ(2)で高速回転する回転体(1)の各反射
鏡面(11)〜(11りに入射し、反射されて一定速度
で移動する被加工物Wの表面近傍に焦点を結び、そのビ
ームエネルギの集中により金属表面を加熱し、焼入れを
行う。この場合、各反射鏡面による夫々の走査焦点線は
従来例と同様であるか、取付角度が順次に所定角度θず
つ異なる各反射鏡面(1,)〜(1゜)による夫々の走
査焦点線(4,)〜(4□)ルJは、回転体(1)の回
転により、数句角度の差に比、じた距離7ビけそれぞれ
離間して平行となり、最初の走査焦点線(4、)と最後
の走査焦点線(4t)との間に所定の幅が形収され、回
転体(11の一回転で、ビームエネルギは矩形面状に分
散されて肋射される。また、各走査焦点線は、回転体(
1)の高速回転、例えば2000〜10000r、p、
m程度の回転と、抜加工物Wの一足速度、例えば1m/
min 程度の移L・・により、続いての回転で隣接
するように移動し、第4図に示されるように、各走査焦
点線間の未照射部分を埋めるように照射し、全体として
矩形面状のビームエネルギの照射を行うことになる。こ
の面状のビームエネルギ照射は、被加工物Wの省属猥面
におけるビームエネルギの照射時間を長くシ、表面溶、
融を生じることなく焼入れ深さを深くでき、特に焼入れ
部分の両端部における表面溶融による表面状態の悪化は
防止される。また、面状のビームエネルギの照射となる
ので、モードや集光性等によるレーザビームの形の影響
を受けることなく、均一な焼入れを行うことができる。Next, the effect will be explained. As shown in FIGS. 2 and 5, each reflective mirror surface (1,) to (1□,) attached to the rotating body (1) has an installation angle of (1,
) are arranged at different angles of 6 in sequence, such as 11θ, (1□) and 10θ. In this way, the laser beam from the laser f emitter head is focused by the lens (3), and is focused on each of the reflecting mirror surfaces (11) to (11) of the rotating body (1) that is rotated at high speed by the motor (2). The beam is reflected and focused near the surface of the workpiece W moving at a constant speed, and the concentrated beam energy heats and hardens the metal surface.In this case, each scanning by each reflecting mirror surface The focal lines are the same as those of the conventional example, or the scanning focal lines (4,) to (4□) are formed by the reflecting mirror surfaces (1,) to (1°) whose mounting angles are sequentially different by a predetermined angle θ. Due to the rotation of the rotating body (1), the first scanning focal line (4,) and the last scanning focal line (4t) become parallel and separated by a distance of 7 degrees, compared to the difference in angle. A predetermined width is accommodated between the rotating body (11), and in one rotation of the rotating body (
1) high speed rotation, e.g. 2000-10000r, p,
rotation of about m and the speed of the punched workpiece W, for example, 1 m/
With a shift L... of the order of min., the subsequent rotation moves them so that they are adjacent to each other, and as shown in Fig. 4, irradiation is performed to fill the unirradiated area between each scanning focal line, resulting in a rectangular surface as a whole. irradiation with a beam energy of . This planar beam energy irradiation requires a longer irradiation time of the beam energy on the surface of the workpiece W, resulting in surface melting and
The hardening depth can be increased without causing melting, and deterioration of the surface condition due to surface melting, especially at both ends of the hardened portion, is prevented. Further, since the beam energy is irradiated in a planar manner, uniform hardening can be performed without being affected by the shape of the laser beam due to the mode, convergence, etc.
更にまた、面状の焼入れとなるので、走査焦点線と直介
方向だけでなく、被加工物Wを任意の方向に移動させて
も焼入れを行えるので、その応用性を広げることができ
る。Furthermore, since hardening is performed in a planar manner, hardening can be performed not only in the scanning focal line and direct direction, but also when the workpiece W is moved in any direction, so that its applicability can be expanded.
この発明は、上記のように構成されているので、表面溶
融が生じることなく焼入れ深さを深くでき、かつ焼入れ
の均一性が得られ、レーザ焼入れ装置の性能を大幅に向
上させ、さらにその応用性を高めることができる。Since this invention is configured as described above, the hardening depth can be deepened without surface melting, and hardening uniformity can be obtained, greatly improving the performance of laser hardening equipment, and furthermore, its application You can increase your sexuality.
第1図は本発明による一実施例の説明図、第2図は回転
体の平面図、第6図は各反射鏡面の取付角度を示す線図
、第4図は各走査焦点線を示す説明図、第5図は従来例
を示す説明図である。
図において(1) a回転体、(1,)〜(11りは各
反射鏡面、(2)は高速モータ、(3)はレンズ、(4
)は走査焦点線である。なお、各図中向−杓号は同一ま
たは相当部分を示す。Fig. 1 is an explanatory diagram of an embodiment according to the present invention, Fig. 2 is a plan view of the rotating body, Fig. 6 is a line diagram showing the mounting angle of each reflecting mirror surface, and Fig. 4 is an explanation showing each scanning focal line. FIG. 5 is an explanatory diagram showing a conventional example. In the figure, (1) a rotating body, (1,) to (11) each reflecting mirror surface, (2) a high-speed motor, (3) a lens, and (4)
) is the scanning focal line. Note that the numbers in each figure indicate the same or corresponding parts.
Claims (2)
回転体にレーザビームを照射し、その反射ビームで金属
表面に焼入れを行うものにおいて、上記多面反射鏡のそ
れぞれの反射鏡面の取付角度を順次に異ならせたことを
特徴とするレーザ焼入れ装置。(1) In a device in which a rotating body constituting a polygonal columnar or polygonal pyramid-shaped polygonal reflecting mirror is irradiated with a laser beam and the metal surface is hardened with the reflected beam, the mounting angle of each reflecting mirror surface of the polygonal reflecting mirror is A laser hardening device characterized by having sequentially different values.
の差を一周にわたり等角度としたことを特徴とする特許
請求の範囲第1項記載のレーザ焼入れ装置。(2) The laser hardening apparatus according to claim 1, wherein the difference in the mounting angles of the respective reflecting mirror surfaces of the polygonal reflecting mirror is made equal over one circumference.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP59195651A JPS6173820A (en) | 1984-09-20 | 1984-09-20 | Laser hardening device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP59195651A JPS6173820A (en) | 1984-09-20 | 1984-09-20 | Laser hardening device |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS6173820A true JPS6173820A (en) | 1986-04-16 |
JPH0140891B2 JPH0140891B2 (en) | 1989-09-01 |
Family
ID=16344713
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP59195651A Granted JPS6173820A (en) | 1984-09-20 | 1984-09-20 | Laser hardening device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS6173820A (en) |
-
1984
- 1984-09-20 JP JP59195651A patent/JPS6173820A/en active Granted
Also Published As
Publication number | Publication date |
---|---|
JPH0140891B2 (en) | 1989-09-01 |
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