The present invention relates to a laser machining apparatus and method for machining works, e.g., metal plates, by using laser beam transmitted from an optical fiber.
The optical fibers have been used as laser transmitting means of the laser machining apparatus. Typically, the optical fiber has a central core and a clad disposed around the core. The core is made of, for example, quartz or transparent plastic. Also, the core is made of material with a certain refraction index larger than that of the clad in order to confine the beam within the core. Practically, however, the beam is not confined completely within the core and, unavoidably, a small amount of beam may leak from the core into the clad. To remove the leaked beam from the clad, JP 2003-139996 A proposes to mount a beam removing member around the clad. Also proposed in U.S. Pat. No. 4,575,181 is to rough a part of the outer peripheral surface of the clad for allowing the leaked beam in the clad to emit from the clad therethrough. These techniques, however, can not remove the leaked beam completely or substantially completely, which allows a small amount of light to be projected through the clad against the works. It has been understood that the amount of beam to be projected against the work is so small that it does not provide a significant affect to the laser machining accuracy. However, the experiments conducted by the inventors revealed that, when cutting the metal plate by using the fiber-laser in which the laser is generated in the active fiber, the small amount of clad transmitting laser caused small irregularities on the cut surface.
Accordingly, an object of the present invention is to provide an apparatus and a method for laser machining which prevent the unwanted clad transmitting laser effectively.
According to the invention, a laser beam is transmitted through an optical fiber with a core and a clad and projected to works for the machining thereof while providing an assist gas of oxygen to the work. During the machining, the beam transmitting in the clad of the fiber is removed or reduced at a removing and/or reducing portion.
With the arrangement, a high quality cutting surface with less irregularities is attained on the cut surface in the metal works.
Referring to the accompanying drawings, several preferred embodiments of the present invention will be described below. Like reference numerals designate like parts throughout the embodiments.
Referring back to
In the first embodiment, the optical fiber 14 has a beam remover 30 adjacent the machining head 16 for removing the leaked beam in the clad 22 therethrough. As shown in
As shown in
With the laser machining device 10 so constructed, the laser beam generated from the laser oscillator 12 is transmitted through the optical fiber 14 to the machining head 16 from which it is projected onto the work 18. The beam 36 leaked from the core 12 into the clad in the optical fiber 14 is absorbed by the absorbing member 34 of the beam remover 30 as shown in
As discussed above, the inventors have first revealed that the cutting quality was drastically increased by reducing the beam transmitting the clad of the optical fiber in the cutting operation using laser beam being transmitted through the optical fiber. Conventionally, it has been known in the art that, in the cutting of the mild steel plate by using CO2 laser in which the laser beam from the oscillator is transmitted in the air and then concentrated for cutting due to the fact that its wavelength is about 10 μm and therefore it is unable to be used with the optical fibers, the weak beam portion existing around the main beam portion provides an adverse affect on the cutting quality. It has also been known that, in the CO2 laser cutting of the mild steel in which the burning reaction of oxygen may affect the cutting quality, a threshold of energy density necessary for the conventional mild steel or iron to be machined is considered to be about 50 kW/cm2. Typically, the energy density of the laser beam at the cutting position or focusing point is set to be 10 MW/cm2 or more. In contrast, the threshold is considerably low. Therefore, it is considered that only a small amount of energy around the main beam portion may provide an adverse affect on the cutting quality. In the cutting of stainless steel in which nitrogen is used for the assist gas so that no burning reaction would occur between the assist gas and the work to be machined, the threshold of energy density is considerably high, i.e, 1 MW/cm2, so that the weak beam portion around the main beam portion may not provide a significant affect on the cutting quality.
The laser beam generated by YAG laser or fiber laser has a wavelength of 1 μm which is about one tenth of that generated by the CO2 laser and therefore it can be transmitted by the use of optical fiber. Typically, as described with reference to
A machining threshold of energy density for cutting the mild steel or other irons using laser with a wavelength of about 1 μm is considered to be 50 kW/cm2 which is equivalent to that using CO2 laser or less than 50 kW/cm2 because the absorption rate by those materials for the laser with the wavelength of about 1 μm is higher than that for CO2 laser. In order to improve the cutting quality, among other things, the laser energy density of the laser beam transmitted through the clad and transferred on the work should be equal to or less than the machining threshold. For this purpose, when cutting the mild steel or other irons, the energy density of the laser beam is preferably equal to or less than 50 kW/cm2, more preferably equal to or less than 30 kwa/cm2.
In the actual test result shown in
The energy density of the laser at the machining portion can be calculated. For example, since the output port of the fiber is transferred on the machining point, a combined diameter of core and clad portions, transferred on the machining point, is measured by using Focus Monitor, commercially available from PRIMES GmbH in German. The distribution of the laser beam from the clad is supposed to be substantially uniform at the output of the fiber and therefore the energy density of the laser beam portion transmitted from the clad can be determined from the following equation:
E=W{π(Rc2−Rs2}
wherein E is energy density, Rc is a radius of core, and Rc is an outer radius of the clad.
Referring to
According to this technique, the ratio of power transmitting in the clad can be determined precisely. For example, if the focal length f1 of the collimator lens 406 is 20 mm and the focal length f2 of the collecting lens 408 is 150 mm, the transfer magnification is 7.5. Then, for the single-mode optical fiber with a clad diameter of 125 μm, the optical image emitted from the clad has a diameter of 900 μm on the transfer point, which is sufficient for measuring the optical power and the power ratio of the beam transmitting in the clad.
It is noted that the energy density distribution of the collected laser beam can be measured by FocusMonitor commercially available from PRIMES GmbH in Germany. Using the measurement, the energy, the ratio, and the energy density of the beam transmitting in the clad can be determined.
According to the laser machining device 40 with plural beam removers, the removing efficiency of each beam remover can be reduced while ensuring the necessary removability in total. This reduces the heat increase in the absorbing member 34. Also, the optical power from the transmitting member 38 can be controlled easily. Further, even if the optical power of the beam transmitting in the clad is large, the substantial part of the entire power of the beam can be removed while reducing the load of each remover. As above, this arrangement restricts the optical power of the beam transmitting in the clad. Consequently, the energy density of the beam emitted from the clad onto the machining point is reduced to equal to or less than 50 kW/cm2, preferably equal to or less than 30 kW/cm2, more preferably equal to or less than 15 kW/cm2, which ensures a high quality smoothness with only minimum roughness Rz in the metal surface cut by the laser from the machining head.
According to the laser machining device 50 with the removers 52 and 54 on opposite ends of the optical fiber 14, the laser beam leaked into the clad at the end of the optical fiber 14, connected to the laser oscillator 12, can be removed immediately after the leakage of the beam into the clad. This prevents the heat generation and/or the resultant damages caused thereby on the clad 22 due to the beam leaked in the clad and reduces the load of the other remover 52. Also, the substantially the entire part of the clad transmitting beam can be removed through the removers 52 and 54. As above, this arrangement restricts the optical power of the beam transmitting in the clad. Consequently, the energy density of the beam emitted from the clad onto the machining point is reduced to equal to or less than 50 kW/cm2, preferably equal to or less than 30 kW/cm2, more preferably equal to or less than 15 kW/cm2, which ensures a high quality smoothness with only minimum roughness Rz in the metal cutting surface cut by the laser emitted from the machining head.
Also in the fourth embodiment, the optical fibers 14a, 14b, and 14 have removers 70a, 70b, and 70c mounted thereon, respectively. Each of the removers 70a, 70b, and 70c may be any one of the structures shown in
Although each of the optical fibers 14a, 14b, and 14 has one remover in this embodiment, it may has one or more removers at respective portions adjacent the laser oscillator and the fiber bundle.
Also, although the removers 72 and 74 are provided on opposite ends of the optical fiber 64 connecting between the fiber bundle 62 and the machining head 66, it is not necessary to provide the remover on opposite ends of the optical fiber and may be provided on one end of the optical fiber.
In addition, a plurality of removers may be provided on one or the other end of the optical fiber 64.
According to the laser machining device 60 so constructed, the laser beams from the laser oscillators 12a, 12b, and 12c are transmitted through the optical fibers 14a, 14b, and 14c, respectively, into the fiber bundle 62 where they are combined with each other. The combined beam is then transmitted through the optical fiber 64 to the machining head 66 from which it is projected to the work 68. The laser beams leaked into the clad from the core or directly transmitted into the clad of the optical fibers 14a, 14b, and 14c are removed at the removers 70a, 70b, and 70c. Also, the laser beam leaked into the clad from the core or directly transmitted into the clad of the optical fiber 64 is removed at the removers 72 and 74.
As described above, the laser machining device according to the fourth embodiment of the invention ensures that the beam to be transmitted through the clad into the fiber bundle 62 is reduced or eliminated. This restricts the heat generation at the fiber bundle 62 due to the beam transmitting in the clad, which increases the reliability of the fiber bundle 62. Also, since the remover 72 is provided on the optical fiber 64 transmitting the combined laser beam, in particular at a portion adjacent the fiber bundle 62, the beam leaked at the portion where the optical fiber is fused and connected to the fiber bundle 62 is removed therefrom immediately after the leakage. This prevents the heat generation and/or the resultant damages due to the beam transmitting in the clad and also reduces the load of the remover 74 provided adjacent the machining head 66. As described above, the substantially part of the clad transmitting beam can be removed at the removers 72 and 74, which reduces the optical power of the beam transmitting in the clad. Consequently, the energy density of the beam emitted from the clad onto the machining point is reduced to equal to or less than 50 kW/cm2, preferably equal to or less than 30 kW/cm2, more preferably equal to or less than 15 kW/cm2, which ensures a high quality smoothness with only minimum roughness Rz in the metal cutting surface cut by the laser emitted from the machining head.
Although the optical fibers 14a, 14b, and 14c are fused and optically connected at the fiber bundle 62, they may be optically connected to the optical fiber 64 by using optical member such as lens.
As described above, the laser machining device 80 according to the fourth embodiment of the invention reduces or eliminates the beam to be transmitted through the clad into the fiber bundle 62
As described above, the laser machining device 80 according to the fifth embodiment of the invention ensures that the beam to be transmitted through the clad into the fiber bundle 62 is reduced or eliminated by the removers 70a, 70b, and 70c provided adjacent the fiber bundle 62. This restricts the heat generation at the fiber bundle 62 due to the beam transmitting in the clad, which increases the reliability of the fiber bundle 62. Also, since the remover is provided on the optical fiber 64 transmitting the combined laser beam, in particular at a portion adjacent the fiber bundle 62, the beam leaked at the portion where the optical fiber is fused and connected to the fiber bundle 62 is removed therefrom immediately after the leakage. This prevents the heat generation and/or the resultant damages due to the beam transmitting in the clad and also reduces the load of the remover 74 provided adjacent the machining head 66. As described above, the substantially part of the clad transmitting beam can be removed at the removers 72 and 74, which reduces the optical power of the beam transmitting in the clad. Consequently, the energy density of the beam emitted from the clad onto the machining point is reduced to equal to or less than 50 kW/cm2, preferably equal to or less than 30 kW/cm2, more preferably equal to or less than 15 kW/cm2, which ensures a high quality smoothness with only minimum roughness Rz in the metal cutting surface cut by the laser emitted from the machining head.
According to the machining head 16 so constructed, the beam 36 including beam components 36a and 36b, emitted from the optical fiber 14, is collected by the first lens 214. The beam component 36a from the core 20 of the collected beam 36 is transmitted through the aperture 222 of the aperture plate 220 into the second lens 214. The beam component 36b from the clad 22, on the other hand, is cut off by the aperture plate 220. This results in that only the beam component 36a from the clad 22 is transformed into a parallel beam by the second lens 216 and then collected again by the third lens 218 onto the machining point 202 through the output port 210.
Therefore, according to the machining head 16 of the embodiment, the beam component 36b from the clad does not illuminate and heat the housing portion defining the output port 210 to transform it. This ensures that the beam with a predetermined, constant shape is projected to the work to prevent the machining accuracy from being damaged, which would otherwise be caused by the thermally-deformed housing.
If no aperture plate exists in the machining head, the beam from the head includes the beam component from the clad as shown in
Although the aperture plate is disposed between the first and the second lenses in the embodiment, the position is not restrictive. Also, the shape of the aperture is not limited to the circle and it may take any configurations. Ideally, it is preferable to remove the entire beam component from the clad by the aperture plate, however, the removing rate is not needed to be 100%.
According to the embodiment, the beam power from the clad is restricted. Consequently, the energy density of the beam emitted from the clad onto the machining point is reduced to equal to or less than 50 kW/cm2, preferably equal to or less than 30 kW/cm2, more preferably equal to or less than 15 kW/cm2, which ensures a high quality smoothness with only minimum roughness Rz in the metal cutting surface cut by the laser emitted from the machining head.
The distal end of the optical fiber 112, i.e., the right end in the drawing, has an exposed portion 128 of the first clad 120 which is formed by removing a part of the second clad 122 and a part of the jacket 128 within a region 124 which extends back a certain distance L1 from the output end 126 of the core 114. The exposed portion 128 of the first clad 120 within the region 124 is continuously tapered toward the distal end of the clad. The taper is provided by dipping the optical fiber in hydrofluoric acid to dissolve the glass-clad in part, which ensures a smooth outer peripheral surface on the taper. The distal end of the optical fiber 112 including the exposed portion 128 is mounted in a sleeve 136 so that the optical fiber 112 stays out of contact with the sleeve 136. The sleeve 136 retains the optical fiber 112 by a first annular retainer 138 disposed around the distal end of the core 114 and a second annular retainer 140 disposed around the jacket 118. Preferably, the sleeve 136 and the first retainer 138 are made of material such as metal which provides a high absorption rate to the laser beam so as to prevent the laser beam to be emitted from the clad from leaking out into the atmosphere.
According to the fiber laser device 150 so constructed, the laser beam excited between the opposed fiber bragg gratings 162 and 164 is transmitted into the core 114 of the optical fiber 112 and then projected from the output end 126 of the core against the work. Since the tapered exposed portion 128 has a reduced allowable NA, the exciting laser beam introduced in the clad or the leaked laser beam from the core 114 are scattered radially outwardly from the exposed portion 128. The scattered laser beam is absorbed in the sleeve 136 spaced away from the optical fiber 112 and/or first retainer 138 where it is heat-dissipated. Also, the distal end of the clad disposed around the core is so small in size that no or, if any, only a small amount of laser beam reflected at the work is introduced into the clad.
As described above, since the distal end of the clad in the distal end portion of the optical fiber 112 is continuously tapered toward the output end of the core, the laser beam transmitting in the clad is reliably discharged and then absorbed in the sleeve disposed and spaced around the optical fiber. Therefore, the laser beam transmitting in the clad is reliably removed from the optical fiber and the optical fiber device and fiber laser device with the optical fiber. Also, the laser beam reflected at the work is substantially or completely prohibited from entering into the clad. Further, the tapered external surface of the clad is so smoothed that no substantial deterioration of strength occurs in the optical fiber. Furthermore, the taper of the clad exposed portion 128 is machined in a relatively easy way, which allows the optical fiber, the optical fiber device, and the fiber laser device to be manufactured economically.
According to the embodiment, the laser beam introduced and/leaked in the clad 20 is removed from the clad at each boundary portions between the enlarged and reduced portions and depending upon the reduction rate of the cross section. The removed laser beam is then heat-absorbed by the sleeve 136 and the first retainer 138. Also, the distal end of the clad disposed around the core is so small in size that no or, if any, only a small amount of laser beam reflected at the work is introduced into the clad. Therefore, the laser beam transmitting in the clad is reliably removed from the optical fiber. Further, the tapered external surface of the clad is so smoothed that no substantial deterioration of strength occurs in the optical fiber. Furthermore, the taper of the clad exposed portion 128 is machined in a relatively easy way, which allows the optical fiber, the optical fiber device, and the fiber laser device to be manufactured economically.
According to the optical fiber device 110″ and the optical fiber 112″, the laser beam transmitting in the clad 120 from the enlarged diameter portion 180a to the reduced diameter portion 180b is removed at the reducing boundary surface portion 180c connecting between the enlarged and reduced diameter portions 180a and 180b, depending on the reduction of the cross section. Since the plurality of enlarged and reduced diameter portions 180 are formed in the embodiment, the laser beam transmitting in the clad is reduced repeatedly and effectively. Also, no need to reduce the outer diameter of the clad so much, which ensures a certain strength required for the clad. Further, the tapered external surface of the clad is so smoothed that no substantial deterioration of strength occurs in the optical fiber. Furthermore, the enlarged and reduced diameter portions 180a and 180b are formed in a relatively easy way simply by reducing the diameter of the exposed portion 128″ of the clad at certain intervals, which allows the optical fiber, the optical fiber device, and the fiber laser device to be manufactured economically.
Although the optical fiber 112 has two clad layers in the above-described embodiments 7-9, it may have a single clad layer.
According to the embodiments 7-9, the optical power of the clad transmitting laser beam to be projected to the work is reduced. Consequently, the energy density of the beam emitted from the clad onto the machining point is reduced to equal to or less than 50 kW/cm2, preferably equal to or less than 30 kW/cm2, more preferably equal to or less than 15 kW/cm2, which ensures a high quality smoothness with only minimum roughness Rz in the metal cutting surface cut by the laser emitted from the machining head.
It is noted that, in the above-described embodiments, significant advantages are obtained in particular when the laser oscillator is made of laser fiber because a relatively large amount of laser beam tends to be introduced into the clad in the oscillator and then delivered into the clad of the subsequent fiber.
Number | Date | Country | Kind |
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2007-097905 | Apr 2007 | JP | national |
2007-097906 | Apr 2007 | JP | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/JP2008/056773 | 4/4/2008 | WO | 00 | 10/5/2009 |