GAS LASER APPARATUS

Abstract: Gas laser appts. circulates a laser gas in a closed space and produces laser light by discharge excitation of the gas and in which a main unit (10) comprising a laser gas oscillation control section and a robot control section, etc. is sepd. from a laser light emission section (2, 5, 6) comprising a resonator (2), -transverse multimode oscillation is used, - the discharge power source is a high frequency source, - and the laser light emission section has a structure permitting mounting on the end of a robot, etc.

Description: The present invention relates to a gas laser device, and more particularly to a gas laser device which can produce a high laser output for metal machining operation such as welding or the like and which can be coupled to a robot or the like. Laser machining requires a machining system comprising a laser oscillator and a robot coupled thereto for achieving its advantages. US-A-4547885 discloses a system in which the laser oscillator is mounted on the robot and which, in order to emit the laser beam from the tip of the robot arm, mirrors are attached to articulation joints of the robot arm for guiding the laser beam along a complex path from the oscillator. Rather than the reflecting mirror, an optical fibre may be employed to guide the laser beam. The reflecting mirror is however expensive and very difficult to adjust. The system employing the optical fibre can transmit energy up to several hundred watts at most, and hence cannot guide energy up to several kilowatts which is needed to effect metal machining operations such as welding or the like. It is an object of the present invention to provide a gas laser device which will solve the above problems, can produce a high laser output for metal machining operation such as welding or the like, and can be coupled to a robot or the like. In order to solve the above problems, there is provided according to the present invention a gas laser device in which a laser medium gas is circulated in an airtight container and a laser beam is generated when the gas is excited by an electric discharge, the device comprising: a robot having a jointed movable arm; a main unit including a laser gas ocsillation controller and a robot controller; a laser beam emitter including a lateral multimode resonator separate from the main unit, the resonator having a lateral or vertical gas flow produced by a compressor having a high compression ratio and being connected to the main unit by flexible gas pipe(s) for supplying the laser medium gas from the main unit to the resonator; characterised in that: the laser gas oscillation controller has a power supply discharging in the RF range, the laser beam emitter is mounted on the distal end of the robot arm, and the laser beam emitter has a single aspherical reflecting mirror which is controllably rotatable to direct the laser beam in the required direction. Since the main unit and the laser beam emitter are separate from each other, the laser beam emitter is easily attached to the tip end of the robot. With the lateral multimode, high-frequency power supply, and the lateral gas flow being employed, a high-output laser beam can be generated by the small-size laser beam emitter. One example of a device according to the invention will now be described with reference to the accompanying drawings, in which:- FIG. 1 is a perspective view of an embodiment of the present invention; FIG. 2 is a perspective view of a portion of a resonator; and FIGS. 3 (a), 3 (b), and 3 (c) are views of parabolic surfaces used as rotating mirrors. Designated in FIG. 1 at 1 is a jointed-arm robot which is a widely known ordinary jointed-arm robot, and 2 a resonator which comprises high-order lateral multimode resonator. FIG. 2 shows a portion of the resonator 2. Denoted in FIG. 2 at 11 is a laser tube made of a dielectric material such as ceramics and having a rectangular cross section, which is of a square shape in the embodiment. The reference numerals 12, 13 denote electrodes mounted on outer sides of the laser tube 11. A high-frequency power supply is applied to the electrodes through leads 14, 15. Optical parts such as an output coupling mirror, a reflecting mirror, and the like, and a laser gas passage are omitted from illustration in FIG. 2. Assuming that the cross-sectional area of the laser tube is represented by S, the length thereof by L, and the output density by ρ , the laser output P can be expressed by: P = SL ρ. Unlike the length L, the cross-sectional area S increases in proportion to the square of the length L. Therefore, it is effective to increase the cross-sectional area S. Heretofore, however, if S is large, it is difficult to achieve uniform discharge excitation, and a lateral multimode results, making beam convergence characteristics poor. As a consequence, this arrangement has not been relied upon. To eliminate the above drawback, a high-frequency power supply, described later, and a lateral gas flow may be employed to reduce the size of the resonator. The value of ρ when uniform discharge excitation is possible ranges from 2 to 8 W/cc. Therefore, the volume of a resonator having a square-shaped cross section with one side ranging from 5 to 10 cm and a length of 30 cm is in the range of from 750 to 3000 cc, and the laser output P ranges from 1.5 to 24 kW. Welding or the like of metal can be effected at this output level. The resonator of this size can be attached to the distal end of a conventioal jointed-arm robot to construct a laser machining system. With the structure of the laser tube 11 as shown in FIG. 2, if a direct current were supplied, an electric discharge would concentrate on one point, and no uniform electric discharge could be produced in the laser tube 11. By applying a high-frequency power supply in an RF range through the laser tube 11 which is of a dielectric material, according to the embodiment, a uniform electric discharge is produced by a ballast effect due to distributed capacitance. This is because the wall of the laser tube 11 of the dielectric material is divided into a number of sections and serves as an array of capacitors on an XY plane. An unstable-type resonator may be expected for use as a laser resonator of this type. However, a stable-type resonator is employed in the embodiment. As a result, the lateral mode becomes an extreme multimode. The small-size laser resonator is made possible by using the high-frequency power supply. Particularly, an RF electric discharge in an RF range is preferred. A lateral gas flow employing a compressor having a high compression ratio such as a Roots blower is used in order to circulate the laser medium gas in the resonator 2. Since the cross-sectional area of the resonator 2 is large, a lateral gas flow is needed to cool the gas effectively. As the air blower is separate from the resonator and coupled thereto by flexible pipes, the air blower such as Roots blower which has a sufficient compression ratio is employed because of the resistance presented by the pipes. The gas flow may be a vertical gas flow. Turning back to FIG. 1, the reference numeral 3 indicates an electric pipe containing wires from the high-frequency power supply in the main unit 10, and the reference numeral 4 indicates a gas pipe for supplying the laser medium gas from the main unit 10. A rotating mirror 5 converges and changes the direction of the laser beam from the resonator 2. Unlike one used on a joint of a conventional jointed-arm robot, the rotating mirror 5 has a short focal length and is single in number, its adjustments are not difficult to make. The rotating mirror is movable axially along and rotatable about an axis indicated by the dotted line in FIG. 1. Through movement of the robot arm and the movement of the rotating mirror, the laser beam can be applied to a necessary workpiece portion. For laser machining such as metal welding or the like, a large depth of focus which would be required for metal cutting, and a very small converging radius are not required, but the converging radius may be about 1 mm. The beam of a large cross section for metal welding or the like may be converged by an aspherical optical system such as a parabolic mirror. Those parallel rays which are parallel to the axis of rotation of the parabolic mirror may be converged without aberrations no matter how large the radius may be. The problem is beam divergence due to a beam diverging angle ϑ. Assuming that the parabolic mirror has a focal length f, the diameter at the focal point is given by 2fϑ. It has experimentally confirmed that even in an extreme multimode obtained by the resonator 2, the value of the focus diameter may be about 1 mm. Dependent on the workpiece to be machined, parabolic mirrors as shown in FIGS. 3(a), 3(b), and 3(c) may selectively be used as the rotating mirror 5. In particular, the off-axis parabolic mirror as illustrated in FIG. 3(b) is preferable for machining operation such as welding or the like. With the small-size, high-output laser resonator 2 being coupled the tip end of the jointed-arm robot 1, a flexible machining system can be constructed. By coupling the rotating mirror to the tip end of the resonator 2, the direction in which the laser beam is emitted can freely be controlled for machining, e.g., welding a more complex workpiece. Denoted at 10 is a main unit containing a robot controller for controlling servomotors for robot arms, and a laser oscillation controller for controlling laser oscillation. The robot controller comprises an ordinary robot controller. The laser oscillation controller is composed of a laser gas controller, a high-frequency power supply, and an output controller. The laser gas controller has an air blower and a heat exchanger for circulating and cooling the laser gas, and also discharges and introduces the gas, controls the gas pressure, and introduces a purging gas. The high-frequency power supply has a high-frequency power supply unit including an inverter for rectifying and converting a commercial power supply voltage to a high-frequency voltage, a sequence controller for controlling the starting and stopping of oscillation of the high-frequency power supply unit, and a pulse oscillator for controlling the output. The output controller has an output selector for selecting either a pulse output or a continuous output, and an output control unit for controlling the output under feedback control. The laser oscillator controller and the robot controller may be of separate controllers, but they are housed in one locker to make the device compact according to the embodiment. In the aforesaid embodiment, a jointed-arm robot is employed. However, robots of other configurations may be selected to meet the desired object. The device may be used to effect operation such as heat treatment of metal or the like. With the present invention, as described above, a high-output, small-size resonator which is of a lateral multimode using a high-frequency power supply is separate from a power supply and an air blower and coupled to the tip end of a robot. Therefore, a flexible laser machining system is provided.

Claims: 1. A gas laser device in which a laser medium gas is circulated in an airtight container and a laser beam is generated when the gas is excited by an electric discharge the device comprising: a robot (1) having a jointed movable arm; a main unit (10) including a laser gas oscillation controller, and a robot controller; a laser beam emitter (2) including a lateral multimode resonator (2) separate from the main unit (10), the resonator (2) having a lateral or vertical gas flow produced by a compressor having a high compression ratio and being connected to the main unit by flexible gas pipe(s) (4) for supplying the laser medium gas from the main unit (10) to the resonator (2); characterised in that; the laser gas oscillation controller has a power supply discharging in the RF range, the laser bean emitter (2) is mounted on the distal end of the robot arm, and the laser bean emitter (2) has a single aspherical reflecting mirror (5) which is controllably rotatable to direct the laser beam in the required direction. 2. A device according to claim 1, wherein the reflecting mirror has a parabolic curved surface. 3. A device according to claim 1 or claim 2, wherein the aspherical reflecting mirror (5) is movable in a direction normal to the direction in which the reflecting mirror is rotatable. 4. A device according to any of claims 1 to 3, wherein the laser oscillation controller includes a laser gas control unit, a high-frequency power supply, and an output controller having an output selector for selecting either a pulse output or a continuous output, and an output control unit for controlling the output under feedback control.

Inventors: KARUBE, NORIO
Applicants: FANUC LTD.
Application year: 1987
Main classification: B23K26
IPC codes: B25J19, H01S3, B23K26