EP0698800A1 - Procédé de la répartition de l'intensité du rayonnement laser pour le traitement de surfaces d'éléments - Google Patents
Procédé de la répartition de l'intensité du rayonnement laser pour le traitement de surfaces d'éléments Download PDFInfo
- Publication number
- EP0698800A1 EP0698800A1 EP95111747A EP95111747A EP0698800A1 EP 0698800 A1 EP0698800 A1 EP 0698800A1 EP 95111747 A EP95111747 A EP 95111747A EP 95111747 A EP95111747 A EP 95111747A EP 0698800 A1 EP0698800 A1 EP 0698800A1
- Authority
- EP
- European Patent Office
- Prior art keywords
- modulated
- intensity distribution
- laser
- vibration
- amplitude
- 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
- 238000000034 method Methods 0.000 title claims abstract description 30
- 238000009826 distribution Methods 0.000 claims abstract description 28
- 230000010355 oscillation Effects 0.000 claims abstract description 24
- 238000007493 shaping process Methods 0.000 claims abstract description 10
- 230000005855 radiation Effects 0.000 claims description 8
- 238000003754 machining Methods 0.000 claims description 7
- 238000004381 surface treatment Methods 0.000 abstract description 2
- 239000000463 material Substances 0.000 description 5
- 230000001276 controlling effect Effects 0.000 description 3
- 230000005284 excitation Effects 0.000 description 3
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 2
- 150000001875 compounds Chemical class 0.000 description 2
- 229910052802 copper Inorganic materials 0.000 description 2
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- 238000011161 development Methods 0.000 description 2
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- 229910052751 metal Inorganic materials 0.000 description 2
- VVQNEPGJFQJSBK-UHFFFAOYSA-N Methyl methacrylate Chemical compound COC(=O)C(C)=C VVQNEPGJFQJSBK-UHFFFAOYSA-N 0.000 description 1
- 229920005372 Plexiglas® Polymers 0.000 description 1
- 238000005275 alloying Methods 0.000 description 1
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Images
Classifications
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F21—LIGHTING
- F21S—NON-PORTABLE LIGHTING DEVICES; SYSTEMS THEREOF; VEHICLE LIGHTING DEVICES SPECIALLY ADAPTED FOR VEHICLE EXTERIORS
- F21S8/00—Lighting devices intended for fixed installation
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F21—LIGHTING
- F21W—INDEXING SCHEME ASSOCIATED WITH SUBCLASSES F21K, F21L, F21S and F21V, RELATING TO USES OR APPLICATIONS OF LIGHTING DEVICES OR SYSTEMS
- F21W2131/00—Use or application of lighting devices or systems not provided for in codes F21W2102/00-F21W2121/00
- F21W2131/40—Lighting for industrial, commercial, recreational or military use
- F21W2131/401—Lighting for industrial, commercial, recreational or military use for swimming pools
Definitions
- the invention relates to a method for controlling the laser beam intensity distribution for the machining of component surfaces. It takes place during the laser processing of surfaces, e.g. Transformation hardening, remelting, alloying, coating etc., of surfaces in the solid and / or liquid state Application.
- One area of application in which the invention can be used particularly advantageously is the laser beam surface hardening of components made of metallic materials.
- cw laser constant laser power
- CW continuous wave mode
- P pulse mode
- the operating mode delivers a continuous laser beam up to max. to the nominal output power of the device.
- the output power can be regulated within limits by changing the excitation power.
- the high thermal conductivity of the metals generally requires oscillation frequencies of greater than 100 Hz, so that the frequency-dependent temperature fluctuations on the surface subside quickly into the interior of the workpiece.
- the galvanoscanners used for controllable oscillating mirror systems can generally only carry out harmonic vibrations in this frequency range. The reason for this is the mass moment of inertia of the moving vibration system components (rotor of the vibration motor and laser mirror), with the copper mirrors with a diameter required for beam transmission, in particular in the laser power range from 1 kW, making up the majority of the moment of inertia.
- this effect can be used for surface hardening in order to achieve a homogeneous machining geometry by compensating for the higher heat conduction losses at the track edges (DD 242 358 and "Homogeneous laser beam hardening by means of high-frequency beam oscillation", S. Völlmar; W. Pompe; H. Junge in Neue Wegte, 31st vol., issue 11, Nov. 86, pages 414 - 418).
- a method for controlling the laser beam intensity distribution for the processing of components by means of laser radiation is used, in which conventional mirrors or mirror systems (for laser powers from 1 kW or more, copper mirrors) are used for laser beam shaping and in which laser beam shaping is based on the sinusoidal, harmonic beam oscillation as Control function for the mirror or the mirror system by means of at least one galvanoscanner.
- the intensity distribution generated in laser beam shaping on the basis of the sinusoidal beam oscillation on a component surface is set independently of the selected shape and size of the scanned surface area, without having to act on the laser used.
- This is achieved by a predefinable superposition of sinusoidal oscillations as a control function for the oscillating mirror system (scanner system).
- This setting of the intensity distribution is carried out in such a way that several harmonic control functions are modulated by superimposition so that the The instantaneous speed of the moving laser spot is influenced in the desired sense. This means that in the area of the track edges an amplitude modulation with a high degree of modulation (close to 1) must be used as a rule because of intensity increases.
- galvanoscanners with the mirrors usually used for laser material processing do not perform other than harmonic vibrations at the required high frequencies, which, as already described, can be modulated according to the invention by superimposing several harmonic control functions so that the instantaneous speed of the moving laser spots is influenced in the desired sense.
- the intensity distribution integrated over many modulation periods is primarily effective for workpiece machining. Their shape can now be varied by modulating the carrier vibration without changing the effective size and shape of the scanned area depicted on the workpiece surface.
- the moment of inertia of the metal mirrors usually used in material processing has the consequence that the scanner mirror deflecting the laser beam with higher-frequency excitation ( ⁇ 100Hz) of the galvanoscanners used, regardless of the shape (time course) of the periodic excitation function (triangle, rectangular functions), grinds them into sinusoidal vibrations .
- the galvanoscanner is excited with such harmonic oscillation profiles (sine or cosine) that can be practically implemented with respect to frequency and amplitude.
- a harmonic overall vibration is composed of a carrier vibration B and at least one further, modulated vibration component A and / or C.
- the track width can be set by the amplitude of the carrier oscillation (taking into account the spot diameter), while the superimposed modulated components (A and / or C) form the desired integral intensity distribution in the period.
- FIGS. 1 to 6 serve for a better understanding, in which the modulation of the control functions according to the invention is represented by superposition.
- FIG. 1 and 2 show, for example, composite scanner control functions.
- the amplitude-time functions demonstrate the exclusively sine or cosine scanner control functions.
- portions of the carrier vibration B with further modulated vibration portions A and C are shown in FIG. 1, which are composed as a harmonic overall vibration.
- the degree of modulation m in the range from zero to one, is a measure of the modulated cycle.
- FIG 3 the raw beam profile of a CO2 laser with the mod structure TEM20 is shown.
- the raw laser beam 1 with a diameter of 32 mm, is focused by a focusing mirror 2 with a focal length of 400 mm and directed onto the specimen 5 via a plane mirror 3, which is attached to a galvanoscanner 4.
- Focusing mirror 2, plane mirror 3 and galvanoscanner 4 are integrated in an oscillating mirror processing head.
- the digital control of the galvanoscanner is realized by a host computer 6, its output signal on the data bus is subjected to a digital / analog conversion 7 and then an amplification 8 (output amplifier).
- the desired control functions which represent the desired intensity profiles 9, here exemplified here as intensity profiles 9 a), b) and c), are generated in software with the above-mentioned parameters in accordance with the intensity profile sought.
- the deflection of the plane mirror 3 in the oscillating mirror head is based on the output of the current amplitude value.
Landscapes
- Engineering & Computer Science (AREA)
- General Engineering & Computer Science (AREA)
- Laser Beam Processing (AREA)
- Lasers (AREA)
- Mechanical Light Control Or Optical Switches (AREA)
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DE4430220A DE4430220C2 (de) | 1994-08-25 | 1994-08-25 | Verfahren zur Steuerung der Laserstrahlintensitätsverteilung auf der Oberfläche zu bearbeitender Bauteile |
DE4430220 | 1994-08-25 |
Publications (2)
Publication Number | Publication Date |
---|---|
EP0698800A1 true EP0698800A1 (fr) | 1996-02-28 |
EP0698800B1 EP0698800B1 (fr) | 2001-10-17 |
Family
ID=6526575
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP95111747A Expired - Lifetime EP0698800B1 (fr) | 1994-08-25 | 1995-07-26 | Procédé de la répartition de l'intensité du rayonnement laser pour le traitement de surfaces d'éléments |
Country Status (4)
Country | Link |
---|---|
EP (1) | EP0698800B1 (fr) |
JP (1) | JPH08103878A (fr) |
AT (1) | ATE207209T1 (fr) |
DE (2) | DE4430220C2 (fr) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO1997041995A2 (fr) * | 1996-05-06 | 1997-11-13 | Fraunhofer-Gesellschaft zur Förderung der angewandten Forschung e.V. | Procede d'usinage de pieces au laser |
EP0872303A2 (fr) * | 1997-04-14 | 1998-10-21 | Schott Glas | Procédé et dispositif pour découper de pièces pleines en matériau fragiles, notamment en verre |
GB2534056A (en) * | 2012-09-06 | 2016-07-13 | Etxe-Tar S A | Method and system for laser hardening of a surface of a journal of a crankshaft |
US10864603B2 (en) | 2015-03-17 | 2020-12-15 | Ikergune A.I.E. | Method and system for heat treatment of sheet metal |
Families Citing this family (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE202006020669U1 (de) | 2005-11-23 | 2009-07-02 | Homag Holzbearbeitungssysteme Ag | Vorrichtung zur Beschichtung von Bauteilen |
DE102009025064A1 (de) * | 2009-06-10 | 2011-04-28 | Ks Kolbenschmidt Gmbh | Verfahren zur Herstellung eines Kolbens einer Brennkraftmaschine mittels induktiver Energiezufuhr und Laserbestrahlung |
DE102015101263B4 (de) | 2015-01-28 | 2016-12-15 | Precitec Gmbh & Co. Kg | Vorrichtung zur Materialbearbeitung mittels Laserstrahlung |
Citations (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE227904C (fr) | ||||
US3848104A (en) | 1973-04-09 | 1974-11-12 | Avco Everett Res Lab Inc | Apparatus for heat treating a surface |
US3952180A (en) | 1974-12-04 | 1976-04-20 | Avco Everett Research Laboratory, Inc. | Cladding |
CH616357A5 (en) | 1976-05-28 | 1980-03-31 | Siemens Ag | Method of accurately machining a workpiece arranged in the working zone of a machining laser and apparatus for carrying out the method |
EP0055463A2 (fr) * | 1980-12-26 | 1982-07-07 | Kabushiki Kaisha Toshiba | Dispositif de chauffage |
DE4017734A1 (de) * | 1989-06-28 | 1991-01-10 | Fortschritt Veb K | Ansteuersystem fuer einen scannerantrieb |
EP0445699A2 (fr) | 1990-03-05 | 1991-09-11 | Mazda Motor Corporation | Procédé et dispositif de fabrication de surfaces trempées |
Family Cites Families (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DD227904A1 (de) * | 1984-11-01 | 1985-10-02 | Ilmenau Tech Hochschule | Verfahren zum entrosten von teilen |
DD242358B1 (de) * | 1985-10-30 | 1988-10-26 | Akad Wissenschaften Ddr | Verfahren zum abbau von temperaturueberhoehungen in der laserwaermebehandlungszone |
-
1994
- 1994-08-25 DE DE4430220A patent/DE4430220C2/de not_active Expired - Fee Related
-
1995
- 1995-07-26 EP EP95111747A patent/EP0698800B1/fr not_active Expired - Lifetime
- 1995-07-26 AT AT95111747T patent/ATE207209T1/de active
- 1995-07-26 DE DE59509713T patent/DE59509713D1/de not_active Expired - Lifetime
- 1995-08-24 JP JP7216000A patent/JPH08103878A/ja not_active Withdrawn
Patent Citations (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE227904C (fr) | ||||
US3848104A (en) | 1973-04-09 | 1974-11-12 | Avco Everett Res Lab Inc | Apparatus for heat treating a surface |
US3952180A (en) | 1974-12-04 | 1976-04-20 | Avco Everett Research Laboratory, Inc. | Cladding |
CH616357A5 (en) | 1976-05-28 | 1980-03-31 | Siemens Ag | Method of accurately machining a workpiece arranged in the working zone of a machining laser and apparatus for carrying out the method |
EP0055463A2 (fr) * | 1980-12-26 | 1982-07-07 | Kabushiki Kaisha Toshiba | Dispositif de chauffage |
DE4017734A1 (de) * | 1989-06-28 | 1991-01-10 | Fortschritt Veb K | Ansteuersystem fuer einen scannerantrieb |
EP0445699A2 (fr) | 1990-03-05 | 1991-09-11 | Mazda Motor Corporation | Procédé et dispositif de fabrication de surfaces trempées |
Non-Patent Citations (1)
Title |
---|
S. VOELLMAR, W. POMPE, H. JUNGE: "Homogene Laserstrahlhaertung mittels hochfrequenter Strahloszillation", NEUE HUETTE, vol. 31.JG., November 1986 (1986-11-01), pages 414 - 418, XP000770155 |
Cited By (12)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO1997041995A2 (fr) * | 1996-05-06 | 1997-11-13 | Fraunhofer-Gesellschaft zur Förderung der angewandten Forschung e.V. | Procede d'usinage de pieces au laser |
WO1997041995A3 (fr) * | 1996-05-06 | 1997-12-11 | Fraunhofer Ges Forschung | Procede d'usinage de pieces au laser |
EP0872303A2 (fr) * | 1997-04-14 | 1998-10-21 | Schott Glas | Procédé et dispositif pour découper de pièces pleines en matériau fragiles, notamment en verre |
EP0872303A3 (fr) * | 1997-04-14 | 1999-12-01 | Schott Glas | Procédé et dispositif pour découper de pièces pleines en matériau fragiles, notamment en verre |
US6112967A (en) * | 1997-04-14 | 2000-09-05 | Schott Glas | Method and apparatus for cutting through a flat workpiece made of brittle material, especially glass |
GB2534056A (en) * | 2012-09-06 | 2016-07-13 | Etxe-Tar S A | Method and system for laser hardening of a surface of a journal of a crankshaft |
GB2534056B (en) * | 2012-09-06 | 2017-04-19 | Etxe-Tar S A | Method and system for laser hardening of a surface of a journal of a crankshaft |
GB2520214B (en) * | 2012-09-06 | 2017-05-03 | Etxe-Tar S A | Method and system for laser hardening of a surface of a workpiece |
US10138528B2 (en) | 2012-09-06 | 2018-11-27 | Etxe-Tar, S.A. | Method and system for laser hardening of a surface of a workpiece |
US10961597B2 (en) | 2012-09-06 | 2021-03-30 | Exteotar, S.A. | Method and system for laser hardening of a surface of a workpiece |
US11898214B2 (en) | 2012-09-06 | 2024-02-13 | Etxe-Tar, S.A. | Method and system for heat treating a workpiece |
US10864603B2 (en) | 2015-03-17 | 2020-12-15 | Ikergune A.I.E. | Method and system for heat treatment of sheet metal |
Also Published As
Publication number | Publication date |
---|---|
DE4430220A1 (de) | 1996-02-29 |
JPH08103878A (ja) | 1996-04-23 |
ATE207209T1 (de) | 2001-11-15 |
DE4430220C2 (de) | 1998-01-22 |
EP0698800B1 (fr) | 2001-10-17 |
DE59509713D1 (de) | 2001-11-22 |
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