专利摘要:
LASER WELDING METHOD AND WELDING STRUCTURE. A laser welding method includes the formation of a fused section (Y) in which several metallic workpieces (W1, W2) within a weld region (S) are fused by projecting a first laser beam (L1) in said weld region with parts of the workpieces being configured as the weld region when the workpieces are welded, and the projection of a second laser beam (L2) while the molten section is being solidified or after a solidified section in which the molten section is solidified is formed so that the second laser beam circulates around the center (C) of the molten section or the solidified section from an initial position deviated from said center towards said center or so that the second laser beam is focused on the center of the fused section or the solidified section from the initial irradiation region that includes the center and a periphery thereof.
公开号:BR102015007881B1
申请号:R102015007881-1
申请日:2015-04-08
公开日:2021-01-12
发明作者:Kohei Hisada;Atsushi Kawakita;Masahiro Nakata
申请人:Toyota Jidosha Kabushiki Kaisha;
IPC主号:
专利说明:

[0001] [0001] The invention relates to a laser welding method that is favorable for welding various workpieces with the use of a laser beam and a welding structure. Description of the Related Art
[0002] [0002] For example, workpieces from two metal plates are stacked or supported irradiated with a laser beam for laser welding. In order to increase reliability and intensity by laser welding, for example, Japanese patent publication No. 3596, a technique of a laser welding method for projecting a laser beam onto a welding region with parts of surfaces of several metal workpieces being configured as the weld region when the workpieces are welded is suggested.
[0003] [0003] In this technique, the laser beam is designed (digitized) to circle the center of the weld region. In this way, workpieces can be fused together receiving a uniform amount of heat over a wide range. As a result, the reliability of a weld section welded by the laser beam can be increased.
[0004] [0004] However, in the case where parts of workpieces are fused by the projection of the laser beam as described in Japanese patent publication No. 3-80596, heat is more likely to be dissipated from a periphery of a molten section (a molten puddle) that has been molten instead of the center of the molten section, and thus the solidification of the molten section begins from the periphery of the molten section and progresses towards the center of the molten section. At this time, a solidification rate from the start of solidification from the center of the molten section to the completion of solidification (that is, a cooling rate) is greater than a solidification rate (a cooling rate) from the periphery of the molten section.
[0005] [0005] As a result, there is a case where the solidification shrinkage of the center of the weld section is completed before being compensated for by the liquid phase flow and where this causes the generation and extension of a crack that begins at the center of the weld section. weld (a solidified section), where the molten section is solidified, or close to it. This crack extends from the center of the weld section (the solidification section), and thus a break mode is difficult to predict. Especially when aluminum alloy workpieces are used, this phenomenon is significant. Summary of the Invention
[0006] [0006] The invention provides a laser welding method and a welding structure that can reduce a crack in a solidified section where a molten section is solidified.
[0007] [0007] A first aspect of the invention relates to a laser welding method. The laser welding method includes: the formation of a fused section in which several metal workpieces within a weld region are fused by projecting a first laser beam into the weld region with parts of the workpiece surfaces being configured as a weld region when workpieces are welded; and projecting a second laser beam while the molten section is being solidified or after a solidified section in which the molten section is solidified is formed so that the second laser beam circulates around the center of the molten section or solidified section from from an initial irradiation position deviated from said center towards said center or so that the second laser beam is focused on the center of the molten section or solidified section from an initial irradiation region that includes the center and a periphery of the same.
[0008] [0008] According to the above aspect, in the irradiation of the first laser beam, the first laser beam is designed for the weld region, in order to form the molten section (a molten puddle) in which the work pieces in the weld region are fused. In the irradiation of the second laser beam, in the case where the second laser beam is projected until the molten section is solidified, when the second laser beam circulates around the center of the molten section from the initial position of irradiation that is deflected from the center towards the center, the solidification of the center of the molten section can be delayed. Similarly, also when the second laser beam is focused on the center from the initial irradiation region that includes the center of the molten section and its periphery, the solidification of the center of the molten section can be delayed. Accordingly, the flow of liquid together with the solidification shrinkage of the center of the molten section, and thus the generation of a crack in the vicinity of the center of the molten section can be suppressed.
[0009] [0009] Meanwhile, in the irradiation of the second laser beam, in the case where the second laser beam circulates around the center from the initial irradiation position which is deviated from the center of the solidified section towards the center after the solidified section in which the molten section is solidified, an irradiated part is melted again, and in this way, the crack that is formed from the center of the solidified section towards a peripheral edge of the solidified section can be sealed. Similarly, also when the second laser beam is focused on the center from the initial irradiation region that includes the center of the solidified section and its periphery, the crack that is formed from the center of the solidified section towards the edge peripheral of the solidified section can be sealed.
[0010] [00010] Here, the "center of the molten section" in the invention refers to a part of the molten section that is solidified at the end while the solidification of the molten section is initiated from its periphery. The "center of the solidified section" refers to a part of the melted section before solidification which is solidified at the end while solidification of the same is initiated from its periphery.
[0011] [00011] When the second laser beam is projected until the molten section is solidified, the second laser beam is projected onto a molten part of the molten section. Meanwhile, when the second laser beam is projected after the solidified section in which the solidified molten section is formed, the second laser beam is projected into a solidified section. This is because the molten section is completely solidified.
[0012] [00012] Here, in the above aspect, the second laser beam can be projected until the molten section is solidified. Upon irradiation of the second laser beam, the second laser beam is projected onto the molten section together with the progress of solidification in one direction from the peripheral edge of the molten section towards the center of the molten section. In this way, the progress of solidification in the direction from the peripheral edge of the molten section towards the center of the molten section can be slowed.
[0013] [00013] According to the above aspect, with respect to the progress of the solidification of the molten section from the peripheral edge towards the center after the irradiation of the first laser beam, the molten section is irradiated with the second laser beam. Accordingly, the molten section is heated by the second laser beam, and the progress of solidification in the direction from the peripheral edge of the molten section towards the center of the molten section can be slowed. In this way, the liquid flows together with the solidification shrinkage of the molten section, and in this way, the generation of cracks near the center of the molten section can be suppressed.
[0014] [00014] Here, in the above aspect, in the irradiation of the second laser beam, the initial position of the irradiation can be located at the peripheral edge of the fused section. In this case, in addition to the effect described above, a fluctuation in a solidification rate (a cooling rate) can be suppressed from the peripheral edge of the molten section to the center of the molten section, and thus the molten section can be solidified to have an additional uniform structure. Similarly, the initial irradiation region can be a region that is surrounded by the peripheral edge of the fused section. In addition, in this case, the molten section can be solidified to have an additional uniform structure from the peripheral edge of the molten section to the center of the molten section.
[0015] [00015] Additionally, in the above aspect, in the irradiation of the second laser beam, the initial irradiation position can be located between the peripheral edge of the molten section and the center of the molten section. In this case, the progress of solidification of at least the center of the molten section and its periphery can be slowed. Accordingly, in addition to the effect described above, the solidification rate (cooling rate) in the center and the periphery can be approximated to the solidification rate (cooling rate) in the vicinity of the peripheral edge of the molten section. Similarly, the initial irradiation region can be a region, the peripheral edge of which is located between the peripheral edge of the molten section and the center of the molten section and which includes the center. The fused section can be solidified to have a uniform structure from the peripheral edge of the fused section to the center of the fused section.
[0016] [00016] In the above aspect, in the irradiation of the second laser beam, the second laser beam can be designed so that the columnar crystal structure grows from the peripheral edge of the molten section to the center of the molten section together with the solidification progress. In any case, the rate of solidification in any parts that are located from the peripheral edge of the molten section to the center of the molten section can be approximated to each other. In this way, the solidified section in which the molten section is solidified (the weld section) is formed from the column crystal structure from the peripheral edge of the solidified section to the center of the solidified section and in the columnar crystal structure, the columnar crystal extends towards the peripheral edge of the solidified section towards the center of the solidified section. As a result, in the columnar crystal structure of the solidified section, even when the crack that begins in the center is generated, the extent of the crack can be reduced. This occurs since the growth of each of the columnar crystals from the peripheral edge of the solidification section to the center of the solidification section is intermittent.
[0017] [00017] In the above aspect, in a period after the irradiation of the first laser beam and before the irradiation of the second laser beam, irradiation of the second laser beam can be initiated after the columnar crystal structure grows from the edge peripheral of the molten section towards the center of the molten section in order to surround the center of the molten section together with the progress of solidification and then the growth of the equiaxial crystal structure is initiated after the growth of said columnar crystal structure be completed. In said irradiation process of the second laser beam, the second laser beam can be designed so that the equiaxial crystal structure remains in a way that surrounds the center of the molten section and that the columnar crystal structure grows from said crystal structure equiaxial to the center of the fused section.
[0018] [00018] According to the above aspect, the solidified section in which the molten section is solidified (the molten section) includes: a first columnar crystal region that is formed from the columnar crystal structure in which the columnar crystal extends from the peripheral edge of the solidified section in the direction from the peripheral edge of the solidified section towards the center of the solidified section; an equiaxial crystal region that is formed from the equiaxial crystal structure formed to surround the center of the solidified section from the first columnar crystal region; and a second columnar crystal region that is formed from the columnar crystal structure from the equiaxial crystal region to the center of the solidified section, and in the columnar crystal structure, the columnar crystal extends towards the center of the solidified section . In this way, even when the crack that starts from the center is generated in the columnar crystal structure of the second columnar crystal region during solidification, the extent of the crack can be reduced. This is because the growth of the columnar crystal is intermittent. Additionally, even when the crack further extends, that crack can be stopped by the equiaxial crystal structure of the equiaxial crystal region. As a result, the extent of the crack can be suppressed.
[0019] [00019] Additionally, in the aspect described above, the case in which the second laser beam is projected until the molten section is solidified is described. In the meantime, an aspect of the case in which the second laser beam is projected after the solidified section in which the molten section is solidified is formed will be described below.
[0020] [00020] In the above aspect, in the irradiation of the second laser beam, the second laser beam is designed for the solidified section in which the molten section is solidified in order to fuse the solidified section again. In this case, a position on a peripheral edge of a region that includes the center of the solidified section and its surroundings can be determined as the starting position of irradiation so that the cooling rate, in which the region that includes the center of the solidified section and the vicinity of it and which is fused again by the irradiation of the second laser beam is solidified, be slower than the cooling rate, in which the region that includes the center of the molten section and the vicinity of it is solidified after irradiation of the first laser beam. According to this aspect, the crack is likely to be generated in the center of the solidified section and in the vicinity of it. However, a region from the initial irradiation position to the center of the solidified and fused section again, and in this way, the crack that is formed in the center of the solidified section and in the vicinity of it can be sealed.
[0021] [00021] A region that is surrounded by the center of the solidified section and the peripheral edge of the region in the vicinity of it can be configured as the region of beginning of irradiation, and the second laser beam can be projected at that point. In this case, the same effect can be expected since a part irradiated in the region of beginning of irradiation is fused again, and, thus, the crack that is formed from the center of the solidified section towards the peripheral edge of the solidified section can be sealed.
[0022] [00022] In the above aspect, the solidified section may include: the equiaxial crystal region that is formed with an equiaxial crystal structure in order to include the center of the solidified section; and the columnar crystal region that is formed with a columnar crystal structure in order to surround the equiaxial crystal region from the peripheral edge of the solidified section towards the equiaxial crystal region. The second laser beam can be designed so that the equiaxial crystal structure of the equiaxial crystal region becomes the columnar crystal structure.
[0023] [00023] According to the above aspect, with the irradiation of the second laser beam, the entire equiaxial crystal structure becomes the columnar crystal structure to include the center of the solidified section. Thus, the solidified section is formed from the columnar crystal structure from the peripheral edge of the solidified section to the center of the solidified section, and in the columnar crystal structure, the columnar crystal extends in the direction from the peripheral edge of the solidified section. solidified section towards the center of the solidified section. As a result, in the columnar crystal structure of the solidified section, even when the crack that starts in the center is generated, the extent of the crack can be reduced. This is because the growth of each of the columnar crystals from the peripheral edge of the solidified section to the center of the solidified section is intermittent.
[0024] [00024] Additionally, in the above aspect, the solidified section can include the equiaxial crystal region that is formed with an equiaxial crystal structure in order to include the center of the solidified section; and the columnar crystal region that is formed with a columnar crystal structure in order to surround the equiaxial crystal region from the peripheral edge of the solidified section towards the equiaxial crystal region. The second laser beam can be projected onto the equiaxial crystal regions so that a part of the equiaxial crystal structure of the equiaxial crystal region surrounds the center of the solidified section and that the remaining equiaxial crystal structure of the equiaxial crystal region becomes the columnar crystal structure.
[0025] [00025] According to the above aspect, the solidified section (the weld section) includes the first columnar crystal region is formed from the columnar crystal structure in which the columnar crystal extends from the peripheral edge of the solidified section towards the peripheral edge of the solidified section towards the center of the solidified section; the equiaxial crystal region that is formed from the equiaxial crystal structure formed to surround the center of the solidified section from the first columnar crystal region; and the second columnar crystal region that is formed from the columnar crystal structure from the equiaxial crystal region to the center of the solidified section, and in the columnar crystal structure, the columnar crystal extends towards the center of the solidified section . In this way, even when the crack starting in the center is generated in the columnar crystal structure of the second columnar crystal region during solidification, the extent of the crack can be reduced. This is because the growth of the columnar crystal is intermittent. Additionally, even when the crack further extends, that crack can be stopped by the equiaxial crystal structure of the equiaxial crystal region. As a result, the extent of the crack can be suppressed.
[0026] [00026] A second aspect of the invention concerns a weld structure. The weld structure includes a weld section in which the parts of various metal workpieces are fused by a laser beam and welded. The weld section is formed from a columnar crystal structure from a peripheral edge of the weld section to the center of the weld section, and in the columnar crystal structure, a columnar crystal extends towards the peripheral edge of the weld section towards the center of the weld section.
[0027] [00027] According to the above aspect, the weld section is formed from the columnar crystal structure from the peripheral edge of the weld section to the center of the weld section, and in the columnar crystal structure, the columnar crystal extends in the direction from the peripheral edge of the weld section to the center of the weld section. In this way, in the columnar crystal structure of the weld section, even when the crack that starts in the center is generated, the extent of the crack can be reduced. This is because the growth of each of the columnar crystals from the peripheral edge of the weld section to the center of the weld section is intermittent.
[0028] [00028] Additionally, a third aspect of the invention concerns a weld structure. The weld structure includes a weld section in which the parts of the various metal workpieces are fused by a laser beam and welded. The weld section includes a first columnar crystal region that is formed from a columnar crystal structure where a columnar crystal extends from a peripheral edge of the weld section in a direction from the peripheral edge of the weld section towards a center of the weld section; an equiaxial crystal region that is formed from an equiaxial crystal structure formed to surround the center of the weld section from the first columnar crystal region; and a second columnar crystal region that is formed from the columnar crystal structure from said equiaxial crystal region to the center of the weld section; and in the columnar crystal structure, the columnar crystal extends towards the center of the weld section.
[0029] [00029] According to the above aspect, even when a crack starting from the columnar crystal structure of the second columnar crystal region where the crack is likely to be generated during the weld is generated, the extent of the crack can be reduced . This is because the growth of the columnar crystal is intermittent. Additionally, even when the crack extends further, that crack can be stopped by the equiaxial crystal structure of the equiaxial crystal region. As a result, the extent of the crack can be suppressed.
[0030] [00030] Additionally, a fourth aspect of the invention relates to a weld structure. The weld structure includes a weld section in which the parts of various metal workpieces are fused by a laser beam and welded. A surface of the weld section on one side that is irradiated with the laser beam is formed from a primary surface with recesses that is recessed from a peripheral edge of the weld section towards a center of the weld section; and a secondary recessed surface which is further recessed from said primary recessed surface in the vicinity of the center of said weld section. A rear surface of the weld section that corresponds to the recessed secondary surface is not necessarily recessed or is a shallower recessed surface than the recessed secondary surface.
[0031] [00031] In weld structures according to the above aspects, such a surface shape can be formed in the case where the weld structure is welded by the laser beam welding method as described above. In a general welding method, a large recess is formed on the back surface on the opposite side of the surface irradiated with the laser beam. However, in the above aspects of the invention, the surface on the side that is irradiated with the laser beam is formed with the primary surface with recesses that is recessed from the peripheral edge of the weld section towards the center of the weld section; and the recessed secondary surface which is further recessed from the recessed primary surface in the vicinity of the center of the weld section. Accordingly, the recessed secondary surface can be easily repaired by a sealant or the like after welding. In addition, the rear surface of the weld section that corresponds to the recessed secondary surface is not recessed or is a shallower recessed surface than the recessed secondary surface. In this way, water or the like is less likely to accumulate, and a chance of corrosion on the part can be reduced.
[0032] [00032] According to the above aspect of the invention, a crack that is generated in the weld section located in the parts of the workpieces, that is, in the solidified section in which the molten section is solidified, can be reduced. Brief Description of Drawings
[0033] [00033] Characteristics, advantages and technical and industrial significance of illustrative modalities of the invention will be described below with reference to the attached drawings, in which numerical references denote similar elements, and where:
[0034] [00034] Figure 1A is a schematic view of an example of a laser welding device for implementing a laser welding method according to a first embodiment of the invention and is a view of a welding state in a lateral direction. ;
[0035] [00035] Figure 1B is a schematic view of an example of the laser welding device for implementing the laser welding method according to the first embodiment of the invention and is a view of the welding state in a forward direction;
[0036] [00036] Figure 2 shows schematic views illustrating a first laser beam irradiation process according to the laser welding method of the first embodiment of the invention, where figure 2A to figure 2C illustrate that the workpieces are radiated with a first laser beam in that order;
[0037] [00037] Figure 3 illustrates schematic views of a state in which a molten section is cooled without performing a second laser beam irradiation process after the irradiation process illustrated in figure 2, where figures 3A and 3B illustrate that the section melted is cooled in that order;
[0038] [00038] Figure 4 includes schematic views to illustrate the second laser beam irradiation process according to the laser welding method of the first embodiment of the invention, where figures 4A to 4D illustrate that the workpieces are radiated with a second laser beam in that order and where figure 4E is a view of the weld section after irradiation of the second laser beam;
[0039] [00039] Figure 5 includes schematic views to illustrate the second laser beam irradiation process according to the laser welding method of a modification of the first embodiment of the invention, where Figure 5A illustrates the irradiation of the second laser beam. , where figures 5BB to 5BD illustrate that the workpieces are irradiated with the second laser beam in that order and where figure 5BE is a view of the weld section after irradiation of the second laser beam;
[0040] [00040] Figure 6 includes schematic views to illustrate the second laser beam irradiation process according to the laser welding method of a second embodiment of the invention, where figure 6A and figure 6B are seen from a modification in solidification of the molten section, where figure 6C and figure 6D illustrate that the workpieces are irradiated with the second laser beam in that order, and where figure 6E is a view of the weld section after irradiation of the second laser beam ;
[0041] [00041] Figure 7 includes schematic views to illustrate the second laser beam irradiation process according to the laser welding method of a modification of the second embodiment of the invention, where Figure 7A and Figure 7B are views of the change in the solidification of the molten section, where figure 7C and figure 7D illustrate that the workpieces are irradiated with the second laser beam in that order, and where figure 7E is a view of the weld section after irradiation of the second beam of laser;
[0042] [00042] Figure 8 includes schematic views to illustrate the second laser beam irradiation process according to the laser welding method of a third embodiment of the invention, where Figure 8A is a view of the solidified section, after irradiation of the first laser beam, where figure 8B and figure 8C illustrate that the workpieces are irradiated with the second laser beam in that order, and where figure 8D is a view of the solidified section after irradiation of the second laser beam ;
[0043] [00043] Figure 9 includes schematic views to illustrate the second laser beam irradiation process according to the laser welding method of a modification of the third embodiment of the invention, where Figure 9A is a view of the solidified section after irradiation of the first laser beam, where figure 9B and figure 9C illustrate that the workpieces are irradiated with the second laser beam in that order, and where figure 9D is a view of the solidified section after irradiation of the second laser beam laser;
[0044] [00044] Figure 10A is an image of a weld section structure according to a first example of the invention;
[0045] [00045] Figure 10B is an image of the weld section structure according to a second example of the invention;
[0046] [00046] Figure 10C is an image of the structure of the weld section according to a comparable example;
[0047] [00047] Figure 11A is an image of a cross section of the weld section according to the first example of the invention;
[0048] [00048] Figure 11B is an image of the cross section of the weld section according to the comparative example;
[0049] [00049] Figure 12A is a graph of maximum fracture lengths in the weld sections according to the first example, second example and comparative example of the invention;
[0050] [00050] Figure 12B is a graph of the total fracture lengths in the weld sections according to the first example, the second example and the comparative example of the invention;
[0051] [00051] Figure 13A is an image of a fracture surface in the weld section according to the second example of the invention when a shear load acts on the weld section;
[0052] [00052] Figure 13B is an image of the fracture surface in the weld section according to the comparative example when the shear load acts on the weld section;
[0053] [00053] Figure 14A is an image of the fracture surface in the weld section according to the second example of the invention when a stress load acts on the weld section; and
[0054] [00054] Figure 14B is an image of the fracture surface in the weld section according to the comparative example when the stress load acts on the weld section. Detailed Description of the Modalities
[0055] [00055] A laser welding method according to some embodiments of the invention will be described below. First Mode
[0056] [00056] Figure 1 is a schematic view of an example of a laser welding device for implementing a laser welding method according to a first embodiment of the invention. Figure 1A is a view of a weld state in a side direction, and Figure 1B is a view of the weld state in a front direction. 1. About configuring a device
[0057] [00057] Figure 1 is a schematic view of a general configuration of a laser welding device 100 according to the embodiment of the invention. Figure 1A is a view of the weld state in the side direction and Figure 1B is a view of the weld state in the front direction.
[0058] [00058] The laser welding device illustrated in figures 1A and 1B includes a laser beam irradiation section 1 as a main component. The laser beam irradiation section 1 is a device that provides laser beams for welding (first and second laser beams) L1, L2 and projects a selected laser beam onto two metal workpieces W1, W2 that are stacked or arranged with a slight space interspersed between them. In this mode, the two workpieces W1, W2 are welded by stacking. However, the number of workpieces is not limited to two. For example, two workpieces can be subjected to contact welding or fillet welding in one method, which will be described below.
[0059] [00059] The first and second laser beams L1, L2, which will be described below, are each reflected sequentially by a fixed mirror 7 and a driven mirror 8 as optical systems and designed with respect to two workpieces W1, W2. Here, the driven mirror 8 is controlled to be driven so that a reflex direction of the first laser beam L1 incident on the driven mirror 8 is controlled and that the first and second laser beams L1, L2 are projected in a desired position. These beams can be digitized in a trajectory (for example, in a circular shape or a helical shape) that is determined in advance as illustrated in figure 1B, for example. First and second laser beam irradiation processes, which will be described below, are performed by using such a laser welding device 100. 2. Regarding the first laser beam irradiation process
[0060] [00060] Figure 2 includes schematic views to illustrate the first laser beam irradiation process according to the laser welding method of the first embodiment, where figure 2A through figure 2C illustrate that the workpieces are radiated with the first laser beam in that order.
[0061] [00061] As illustrated in figure 2, in the first laser beam irradiation process, when two metal workpieces W1, W2 are welded, parts of the workpiece are determined as a weld region P, and the weld region P is irradiated with the first laser beam L1. In this way, a cast section Y in which the workpieces in the weld region P are cast is formed.
[0062] [00062] More specifically, in this modality, as illustrated in figure 2A, the first laser beam L1 is digitized at a periphery R1 so that the first laser beam L1 circulates around the center of the weld region P and founds the parts at the R1 periphery of the P welding region.
[0063] [00063] Next, as illustrated in figure 2B, the first laser beam L1 is digitized on a periphery R2, a radius of which is larger than that of the periphery R1, so that the first laser beam L1 circulates around from the center of the P weld region, and found the workpieces in the vicinity of the R2 periphery of the P weld region.
[0064] [00064] Additionally, as illustrated in figure 2C, the first laser beam L1 is digitized on a periphery R3, a radius of which is larger than that of the periphery R2, so that the first laser beam L1 circulates around the center of the weld region P and founds the workpieces near the periphery R3 of the weld region P. As described, the first laser beam L1 circulates around the center from the center of the weld region P in the direction of a peripheral edge of the weld region P, and the material in the region is fused by the first laser beam L1.
[0065] [00065] Thus, in the melted Y section that is formed, a temperature at the peripheral edge is greater than a temperature in the center. In this way, compared to a case in which the first L1 laser beam is scanned from the peripheral edge to the center, a solidification rate in the center can be reduced. As described, the center is gradually solidified in the same way as the peripheral border. In this way, it is possible to prevent the generation of cracks in the vicinity of the center after the weld section is solidified.
[0066] [00066] Here, in the case where the second laser beam irradiation process, which will be described below, is not performed after the irradiation process illustrated in figure 2 and the molten section Y is cooled, as illustrated in figure 3A, the heat is more easily radiated from a peripheral edge S of the molten section Y than from the center C thereof. Accordingly, solidification begins from the peripheral edge S of the melted section Y, and the solidification of the melted section Y progresses towards the center.
[0067] [00067] Then, as illustrated in figure 3B in a solidified section G in which the molten section Y is solidified, an equiaxial crystal structure G2 (an equiaxial crystal region) is formed to include the center C of the solidified section G , and a columnar crystal structure (a columnar crystal region) G1 is formed from the peripheral edge S of the solidified section G towards the equiaxial crystal region so as to surround the equiaxial crystal structure G2 (the equiaxial crystal region ).
[0068] [00068] Here, regardless of the formation of the equiaxial crystal structure, and the columnar crystal structure, a solidification rate (i.e., a cooling rate) from the start of solidification from center C of the molten section Y to complete solidification is greater than a solidification rate (a cooling rate) of the peripheral edge S of the molten section Y. As a result, the solidification shrinkage of the center C of the molten section Y is completed before being compensated for by the liquid phase flow in the center C, and the structure is pulled in a circumferential direction. This possibly causes the generation and extension of the crack that begins in the center of the solidified section G or in the vicinity of it,
[0069] [00069] In view of the above, in this modality, the second laser beam irradiation process, which will be described below, is performed. Note that, in this modality, the fused section (a fused pool) Y is formed by digitizing the first L1 laser beam. However, a method of forming the molten section and the like is not particularly limited as long as the molten section Y with the peripheral edge as illustrated in figure 2C can be formed. 3. Reference to the second laser beam irradiation process
[0070] [00070] Figure 4 includes schematic views to illustrate the second laser beam irradiation process according to the laser welding method of the first modality, where figures 4A to 4D illustrate that the workpieces are irradiated with a second laser beam in that order and where figure 4E is a view of the weld section after irradiation of the second laser beam.
[0071] [00071] In this modality, in the second laser beam irradiation process, the second laser beam L2 is projected on a melted part in the melted section Y until the melted section Y is solidified. More specifically, the second laser beam L2 circulates around the center C from an initial irradiation position that is offset from the center C of the molten section Y towards the center C, and then the second laser beam L2 and focused on the center C.
[0072] [00072] More specifically, as illustrated in figure 4A, in this modality, the initial irradiation position is located at the peripheral edge S of the fused section Y. The second laser beam L2 is projected on the fused section Y from that position while circulating in around the center C so that the columnar crystal structure grows from the peripheral edge S of the molten section Y to the center of the molten section Y along with the progress of solidification in a direction from the peripheral edge S of the molten section Y in the direction of the center C of the molten section Y. In this case, the second laser beam L2 can be designed to draw concentric circles with gradually reduced radii with the center C being the center. Alternatively, the second laser beam L2 can be projected in a helical shape towards the center C.
[0073] [00073] As described with reference to figure 3A, after the irradiation of the first laser beam, the solidification of the fused section Y progresses from the peripheral edge S towards the center C. However, as described above, the progress of the solidification in the direction from the peripheral edge S of the fused section Y towards the center C of the fused section Y is delayed by the projection of the second laser beam L2 in the fused section Y.
[0074] [00074] In this way, a fluctuation in the solidification rate (the cooling rate) from the peripheral edge S of the molten section Y to the center C of the molten section Y is suppressed so that the molten section Y can be solidified to have the structure additional uniform. In this embodiment, the solidified section G in which the molten section Y is solidified is formed from the columnar crystal structure from the peripheral edge S of the solidified section G to the center C of the solidified section G, and in the columnar crystal structure, a columnar crystal extends in a direction from the peripheral edge S of the solidified section G towards the center C of the solidified section G (for example, see figure 10A, which will be described below).
[0075] [00075] As a result, in the columnar crystal structure of the solidified section G, even when the crack starting at the center C is generated, the extent of the crack can be reduced. This is because the growth of each of the columnar crystals from the peripheral edge S of the solidified section G to the center of the solidified section G is intermittent.
[0076] [00076] Figure 5 includes schematic views to illustrate the second laser beam irradiation process according to the laser welding method of a modification of the first modality, where Figure 5A illustrates the irradiation of the second laser beam, where figures 5B to 5BD illustrate that the workpieces are irradiated with the second laser beam in that order, and where figure 5BE is a view of the weld section after irradiation of the second laser beam.
[0077] [00077] In the mode described above, the second laser beam L2 is digitized in the fused Y section. For example, as illustrated in figure 5A, a position of a focal point of the second laser beam L2 can be adjusted to adjust the irradiation region of the second laser beam L2 with respect to the workpieces. In this case, the irradiation region (an irradiation area) can be adjusted by moving a condensing lens of the second laser beam L2 at a high speed. Here, the second laser beam L2 is projected from a position T2 (T2 ') as a blurred position to a focused position of T1 while the result of the laser beam is adjusted so that its intensity becomes constant, for example.
[0078] [00078] In this modality, the second laser beam L2 is designed so that the second laser beam L2 is focused from the initial region of irradiation, which includes the center C of the fused section Y and the periphery thereof, for the center C. More specifically, as illustrated in figure 5BB, the initial irradiation region is determined as a region that is surrounded by the peripheral edge S of the molten section Y. Then, as illustrated in figure 5BB to 5BD, the progress of solidification in the direction from the peripheral edge S of the molten section Y towards the center C of the molten section Y is retarded so that the columnar crystal structure grows from the peripheral edge S of the molten section Y to the center C of the molten section Y by the focus of the second laser beam L2 in the fused section Y together with the progress of solidification in the direction from the peripheral edge S of the fused section Y towards the center C of the fused section Y. As a result, the same effect as in the casedescribed above can be expected.
[0079] [00079] In this modification and modification thereof, the second laser beam L2 is designed so that the columnar crystal structure grows from the peripheral edge S of the molten section Y to the center C of the molten section Y. However, for example, in the case where the progress of solidification in the direction from the peripheral edge S of the molten section Y towards the center C of the molten section Y is delayed and where the liquid can flow together with the solidification shrinkage of the center C of the molten section Y, the extent of the crack in the center C can be suppressed. Thus, irradiation of the second laser beam L2 together with the growth of the structure during solidification are not necessarily necessary. Second Mode
[0080] [00080] Figure 6 includes schematic views to illustrate the irradiation process of the second laser beam according to the laser welding method of a second modality, where figures 6A and 6B are seen from a change in the solidification of the molten section. , where figures 6C and 6D illustrate that the workpieces are irradiated with the second laser beam in that order, and where figure 6E is a view of the weld section after irradiation of the second laser beam.
[0081] [00081] The second mode differs from the first mode in the starting position of the irradiation of the second laser beam L2 and in the timing of the second laser beam L2. It is noted that the second modality is the same as the first modality at a point that, in the second laser beam irradiation process, the molten part in the molten section Y is irradiated with the second laser beam L2 until the molten section Y is solidified . The same points of the second modality as the first modality will not be described in detail.
[0082] [00082] In the second modality, in the second laser beam irradiation process, the initial irradiation position is located between the peripheral edge S of the molten section Y and the center C of the molten section Y (see figure 6C, for example). Here, in this modality, in a period after the first laser beam irradiation process (see figure 2C) and before the irradiation of the second laser beam (see figure 6C), as illustrated in figure 6A and figure 6B, the structure of columnar crystal G1 grows from the peripheral edge S of the fused section Y towards the center C of the fused section Y in order to surround the center C of the fused section Y together with the progress of solidification. At this point, the second laser beam is not projected.
[0083] [00083] Next, after the growth of the G2 equiaxial crystal structure is started after the growth of the columnar crystal structure G1 is completed, as illustrated in figure 6C, the second laser beam irradiation process is started. In the second laser beam irradiation process, the second laser beam L2 is designed so that the equiaxial crystal structure G2 remains to surround the center C of the molten section Y and the columnar crystal structure grows from the structure of equiaxial crystal G2 for the center C of the fused section Y. In this case, the second laser beam L2 can be designed to draw concentric circles with gradually reduced radii with the center C being the center. Alternatively, the second laser beam L2 can be projected in a helical shape towards the center C.
[0084] [00084] As described, as illustrated in figures 6E and 10B, which will be described below, in the solidified section (aa weld section) G where the molten section Y is solidified, a first columnar crystal region formed from the crystal structure columnar G1 is formed in the direction from the peripheral edge S of the solidified section G towards the center C of the solidified section G, and in the columnar crystal structure G1, the columnar crystal extends from the peripheral edge S of the solidified section G. Additionally, the equiaxial crystal region formed from the equiaxial crystal structure G2 is formed to surround the center C of the solidified section G from the first columnar crystal region (the columnar crystal structure G1). In addition, the second columnar crystal region formed from the columnar crystal structure G3 is formed from the equiaxial crystal region (the equiaxial crystal structure G2) for the center C of the solidified section G, and in the columnar crystal structure G3 , the columnar crystal extends towards the center C of the solidified section G.
[0085] [00085] Accordingly, even when a crack starting at center C is generated in the columnar crystal structure of the second columnar crystal region (the columnar crystal structure G3) during solidification, the extent of the crack can be reduced. This is because the growth of the columnar crystal is intermittent. Additionally, even when the crack extends further, that crack can be stopped by the equiaxial crystal structure G2 of the equiaxial crystal region. As a result, the extent of the crack can be suppressed.
[0086] [00086] Here, the second laser beam can be used as described in the modification of the first modality. In this case, the region of onset of irradiation must be a region, a peripheral edge of which is located between the peripheral edge S of the melted section Y and the center C of the melted section Y and which includes the center C.
[0087] [00087] Figure 7 includes schematic views to illustrate the second laser beam irradiation process according to the laser welding method of a modification of the second modality, where figures 7A and 7B are seen from the change in section solidification. cast, where figures 7C and 7D illustrate that the workpieces are irradiated with the second laser beam in that order, and where figure 7E is a view of the weld section after irradiation of the second laser beam.
[0088] [00088] In this modification, as illustrated in figures 7A to 7D, in the second laser beam irradiation process, the second laser beam L2 is designed together with the progress of solidification just before or even the equiaxial crystal is formed. time when the equiaxial crystal is formed so that the equiaxial crystal does not remain and the columnar crystal structure G1 grows from the peripheral edge S of the molten section Y to the center C of the molten section Y. As a result, the same weld section (solidified section G) that in the first modality can be obtained.
[0089] [00089] The solidification rate of the peripheral edge S of the molten section Y can be brought closer to the center C of the molten section Y. In this way, as illustrated in figure 7E, the solidified section G in which the molten section Y is solidified it is formed from the columnar crystal structure from the peripheral edge S of the solidified section G to the center of the solidified section G, and in the columnar crystal structure, the columnar crystal extends in the direction from the peripheral edge S of the solidified section G towards the center C of the solidified section G. As a result, in the columnar crystal structure of the solidified section G, even when the crack starting from the center C is generated, the crack length can be reduced. This is because the growth of each of the columnar crystals from the peripheral edge S of the solidified section G to the center of the solidified section G is intermittent.
[0090] [00090] Figure 8 includes schematic views to illustrate the second laser beam irradiation process according to the laser welding method of a third embodiment, in which figure 8A is a view of the solidified section after irradiation of the first laser beam, where figures 8B and 8C show that the workpieces are irradiated with the second laser beam in that order, and where figure 8D is a view of the solidified section after irradiation of the second laser beam.
[0091] [00091] The third mode differs from the first and second modes in that the second laser beam is projected after the molten section is solidified. In this embodiment, after the solidified section G, in which the molten section Y is solidified is formed (that is, see figure 3B and figure 8A), the second laser beam L2 is designed so that the second laser beam L2 circulates around the center C from the starting irradiation position that is deviated from the center C of the solidified section G towards the center C. In this way, the irradiated part is fused again, and thus a crack that is formed at from the center C of the solidified section G towards the peripheral edge S of the solidified section G can be sealed.
[0092] [00092] More specifically, in the second laser beam irradiation process, the second laser beam L2 is projected onto the solidified section G and merges the solidified section G again. Here, a position on a peripheral edge of a region that includes the center C of the solidified section G and the vicinity of it is determined as the starting position of irradiation so that the rate of solidification to the region that includes the center of the section solidified and the vicinity of the same and which is fused again by irradiation of the second laser beam L2 to be solidified is lower than the solidification rate until the region that includes the center C of the fused section Y and the vicinity of the same solidified after the irradiation of the first laser beam L1 (the cooling rate in the state shown in figure 3B). At this point, for the cooling rate, the intensity of the second laser beam is adjusted, the heat absorbed by the solidified section G is also adjusted. In addition, similar to the first modality, the second laser beam L2 can be designed to draw concentric circles with gradually reduced radii with the center C being the center. Alternatively, the second laser beam L2 can be projected helically in the direction of the center C.
[0093] [00093] In this modality, as described above, the solidified section G includes the region of equiaxial crystal that is formed with the equiaxial crystal structure G2 so as to include the center of the solidified section G; and the columnar crystal region that is formed from the columnar crystal structure G1 from the peripheral edge S of the solidified section G towards the equiaxial crystal region in order to surround the equiaxial crystal region. In this way, as illustrated in figure 8B, the second laser beam is projected on the equiaxial crystal region and merges the equiaxial crystal region again (the fused section Y is formed) so that a part of the G2 equiaxial crystal structure of equiaxial crystal surround the center of the solidified section G and let the remaining equiaxial crystal structure in the equiaxial crystal region become the columnar crystal structure G3.
[0094] [00094] As described, similar to the second modality, in the solidified section (the weld section) G in which the molten section is solidified, the first columnar crystal region that is formed from the columnar crystal structure G1 is formed in the direction from the peripheral edge S of the solidified section G towards the center C of the solidified section G, and in the columnar crystal structure G1, the columnar crystal s extends from the peripheral edge S of the solidified section G. Additionally, the region of equiaxial crystal formed from the equiaxial crystal structure G2 is formed to surround the center C of the solidified section G from the first columnar crystal region (the columnar crystal structure G1). In addition, the second columnar crystal region formed from the columnar crystal structure G3 'is formed from the equiaxial crystal region (the equiaxial crystal structure G2) for the center C of the solidified section G, and in the columnar crystal structure G3, the columnar crystal extends towards the center C of the solidified section G.
[0095] [00095] Accordingly, even when a crack starting from the center C is generated in the columnar crystal structure of the second columnar crystal region (the columnar crystal structure G3) during solidification, the extent of the crack can be reduced. This is because the growth of the columnar crystal is intermittent. Additionally, even when the crack extends further, that crack can be stopped by the equiaxial crystal structure G2 of the equiaxial crystal region. As a result, the extent of the crack can be suppressed.
[0096] [00096] Similarly, also when a laser beam irradiation method as in the modification of the first modality is used to focus the second laser beam from the initial irradiation region that includes the center C of the solidified section G and the of the same (more specifically, the region on an internal side of the equiaxial crystal region) to the center C of the solidified section G, the crack that is formed from the center C of the solidified section G towards the peripheral edge S of the section solidified G can be sealed.
[0097] [00097] Figure 9 includes schematic views to illustrate the second laser beam irradiation process according to the laser welding method of a modification of the third modality, where Figure 9A is a view of the solidified section after irradiation of the first laser beam, where figures 9B and 9C illustrate that the workpieces are irradiated with the second laser beam in that order, and where figure 9D is a view of the solidified section after irradiation of the second laser beam.
[0098] [00098] In the mode described above, the second laser beam L2 is designed so that a part of the G2 equiaxial crystal structure remains. However, as illustrated in figure 9B and figure 9C, the second laser beam can be designed so that the equiaxial crystal structure G2 of the equiaxial crystal region becomes the columnar crystal structure G1.
[0099] [00099] Thus, in a welded structure obtained, the entire equiaxial crystal structure becomes the columnar crystal structure in such a way as to include the center C of the solidified section (the weld section) G. Accordingly, the section solidified G is formed from the columnar crystal structure from the peripheral edge S of the solidified section G to the center of the solidified section G, and in the columnar crystal structure, the columnar crystal extends in the direction from the peripheral edge S of the solidified section G towards the center C of the solidified section G. As a result, in the columnar crystal structure G3 of the solidified section G, even when the crack starting at the center C is generated, the extent of the crack can be reduced. This is because the growth of each of the columnar crystals from the peripheral edge S of the solidified section G to the center of the solidified section G is intermittent.
[0100] [000100] Note that, in any of the modalities, the laser beam is projected in the molten section or the center of the solidified section for a long time in the weld structure that includes the weld section (the solidified section G which is welded by the first and second laser beams. Accordingly, in any of the modalities, as exemplified in figure 9C, for example, a surface of the solidified section G on one side that is irradiated with the laser beam is formed from a primary indented surface F1 which is indented from the peripheral edge S of the solidified section G towards the center of the weld section and a secondary indented surface F2 which is additionally indented from the primary indented surface F1 in the vicinity of the center of the solidified section G. Additionally , a posterior surface of the solidified section G corresponding to the secondary recessed surface F2 is formed from a recessed surface F3 that is shallower than the secondary recessed surface F two. In addition, as illustrated in other embodiments, the rear surface of the solidified section G that corresponds to the secondary recessed surface F2 may not be recessed (see figure 7E, for example).
[0101] [000101] As a result, the secondary recessed surface F2 is formed on the surface on the side that is irradiated with the laser beam. In this way, the secondary recessed surface F2 can be easily repaired by a sealant or the like after welding. Additionally, the rear surface of the weld section that corresponds to the secondary recessed surface F2 is either not recessed or is formed from the recessed surface F3 which is shallower than the secondary recessed surface F2. In this way, water or the like is less likely to be collected, and a chance of corrosion on the part can be reduced. Examples
[0102] [000102] Examples according to the invention will be described below. First example (corresponding to figure 4)
[0103] [000103] Plate materials (work pieces) that are made of 6000 series aluminum alloy and have thicknesses of 1.2 mm and 1.0 mm, respectively, were prepared. The first laser beam was designed to have a welding radius of 8 mm. Additionally, using the method illustrated in the first modality (illustrated in figure 4), a scanning path of the second laser beam was gradually focused from the outer periphery of the cast section to the inside, and the cast section was slowly cooled to solidification to form the weld section in each of these materials. The first laser beam had an output of 2.5 to 4.0 kw, and the second laser beam had an output in a range of 0.5 to 1.5 kw. Similarly, the plate materials as workpieces were folded into an L shape and welded as shown in figure 14. Second example (see figure 6)
[0104] [000104] Plate materials such as workpieces were welded in the same way as in the first example. The second example differed from the first example in that, in the method described in the second modality (see figure 6), the laser beam irradiation remained stopped in a period after the projection of the first laser beam and before the center solidified. from the molten section until the formation of the equiaxial crystal starts, then the laser beam was projected again after the formation of the equiaxial crystal, and the region on the inner side of the equiaxial crystal was slowly cooled to solidify the molten section (to form the welded section ). Comparative example
[0105] [000105] The plate materials as workpieces were welded in the same way as in the first example. The comparative example differed from the first example in that the second laser beam was not projected. Observation of structures
[0106] [000106] The weld sections according to the first and second examples and the comparative example were subjected to electro polishing and then observed with a microscope. Figure 10A is an image of the weld section structure according to the first example, Figure 10B is an image of the weld section structure according to the second example, and Figure 10C is an image of the weld section structure. weld according to the comparative example.
[0107] [000107] As illustrated in figure 10A, it can be understood that the weld section of the first example was formed from the columnar crystal structure from the peripheral edge of the weld section to the center of the weld section, and in the weld structure. columnar crystal, the columnar crystal extended in the direction from the peripheral edge of the weld section towards the center of the weld section.
[0108] [000108] As illustrated in figure 10B, in the weld section of the second example, the first columnar crystal region that was formed from the columnar crystal structure was formed, and in the columnar crystal structure, the columnar crystal s extended from from the peripheral edge of the weld section in the direction from the peripheral edge of the weld section towards the center of the weld section. Additionally, the equiaxial crystal region that was formed from the equiaxial crystal structure was formed from the first columnar crystal region, and the equiaxial crystal structure being formed to surround the center of the weld section. In addition, the second columnar crystal region that was formed from the columnar crystal structure was formed from the equiaxial crystal region to the center of the weld section, and in the columnar crystal structure, the columnar crystal extended towards the center of the weld section.
[0109] [000109] As illustrated in figure 10C, in the weld section of the comparative example, the equiaxial crystal structure was formed to include the center of the weld section, and the columnar crystal structure was formed from the peripheral edge of the weld section towards the equiaxial crystal region in a way around the equiaxial crystal region. Observation of cross sections
[0110] [000110] The cross sections of the weld sections according to the first example and the comparative example were observed with the microscope. Figure 11A is an image of a cross section of the weld section according to the first example, and figure 11B is an image of the cross section of the weld section according to the comparative example.
[0111] [000111] As illustrated in figure 11A, in the weld section of the first example, the surface of the weld section on the side that was irradiated with the laser beam was formed with the primary indented surface F1 that was recessed from the peripheral edge of the weld section towards the center of the weld section and the secondary recessed surface F2 which has been further recessed from the primary recessed surface F1 in the vicinity of the center of the weld section. In addition, the rear surface of the solidified section G that corresponds to the secondary recessed surface F2 was formed with the recessed surface F3 which was shallower than the secondary recessed surface F2.
[0112] [000112] As illustrated in figure 11B, in the weld section of the comparative example, the surface of the weld section on the side that is irradiated with the laser beam was formed with the primary indented surface F1 that was recessed from the peripheral edge of the weld section towards the center of the weld section. However, the secondary indented surface F2 which was additionally indented from the primary indented surface F1 in the vicinity of the center of the weld section as described in the first example has not been formed. Unlike the rear surface of the solidified section G in the first example, the rear surface of the solidified section G, which corresponds to the secondary recessed surface F2, was formed with the recessed surface F3 which is deeper than the secondary recessed surface F2. Observation of fractures
[0113] [000113] Three samples were used to measure the maximum fracture lengths and the total fracture lengths with respect to the weld sections according to the first and second examples and the comparative example. It is considered that, in the case of the first example, compared to the comparative example, the columnar crystal structure was formed from the peripheral edge of the solidified section to the center of the solidified section, the growth of each of the columnar crystals in the structure columnar crystal was intermittent, so that the extent of the crack can be reduced. It is also considered that, in the case of the second example, in comparison with the first example and the comparative example, even when the crack that started from the center was generated in the columnar crystal structure of the second columnar crystal region during solidification, this cracking can be stopped by the equiaxial crystal structure of the equiaxial crystal region. Observation of fracture morphology
[0114] [000114] With respect to the first example and the comparative example, the surface states at a time when a shear load acts on the weld sections were observed. Figure 13A is an image of the surface of the weld section according to the second example when a shear load acts on the weld section, and figure 13B is an image of the fracture surface in the weld section according to the comparative example. when the shear load acts on the weld section.
[0115] [000115] For the first example and the comparative example, the states of the surface at a time when a voltage load acts on the weld section were observed. Figure 14A is an image of the surface of the weld section according to the second example when the stress load acts on the weld section, and figure 14B is an image of the fracture surface in the weld section according to the comparative example. when the tension load acts on the weld section.
[0116] [000116] As illustrated in figure 13A and figure 13B, in the case of the second example, the fracture was generated at the peripheral edge of the weld section (a border section). However, in the case of the comparative example, the fracture was generated in the center of the weld section. In other words, in the second example, the fracture was not generated from the crack that was generated by welding.
[0117] [000117] As illustrated in figure 14B, in the case of the second example, the fracture was not generated. However, in the case of the comparative example, the fracture was generated in the center of the weld section.
[0118] [000118] The description has been made so far by using the modalities of the invention. Specific configurations are not limited to these modalities and examples, and any design changes that are made within the scope of the heart of the invention are included in the invention.
权利要求:
Claims (10)
[0001]
Laser welding method, characterized by the fact that it comprises: the formation of a fused section (Y) in which several metallic workpieces (W1, W2) within a weld region (S) are fused by projecting a first laser beam (L1) into said weld region (S ) with parts of the workpieces (W1, W2) being configured as the weld region (S) when the workpieces (W1, W2) are welded; and the projection of a second laser beam (L2) while the molten section (Y) is being solidified or after a solidified section (G) in which the molten section (Y) is solidified is formed so that the second laser beam (L2) circulate around a center (C) of the molten section (Y) or the solidified section (G) from an irradiation start position deviated from said center (C) in the direction of said center (C ) or so that the second laser beam (L2) is focused on the center (C) of the molten section (Y) or the solidified section (G) from an irradiation onset region that includes the center (C) and a periphery of it, being that the fused section (Y) including the center (C) is progressed to solidify, or the solidified section (G) is remelted and a remelted section is progressed to solidify while projecting the second laser beam (L2); and a solidification rate of at least the center (C) of the molten section (Y) or the remelted section is reduced by the projection of the second laser beam (L2).
[0002]
Laser welding method, according to claim 1, characterized by the fact that: the second laser beam (L2) is projected until the molten section (Y) is solidified; and when irradiating the second laser beam (L2), the second laser beam (L2) is projected onto the molten section (Y) together with the progress of solidification in one direction from a peripheral edge of the molten section (Y) at direction of the center (C) of the molten section (Y), so that the progress of solidification in the direction from the peripheral edge of the molten section (Y) towards the center (C) of the molten section (Y) is slowed.
[0003]
Laser welding method, according to claim 2, characterized by the fact that: in the irradiation of the second laser beam (L2), the position of beginning of irradiation is located at the peripheral edge of the fused section (Y), or the region of beginning of irradiation is a region that is surrounded by the peripheral edge of the fused section (Y ).
[0004]
Laser welding method, according to claim 2, characterized by the fact that in the irradiation of the second laser beam (L2), the position of beginning of irradiation is located between the peripheral edge of the fused section (Y) and the center (C) of the fused section (Y), or the region of beginning of irradiation is a region, a peripheral edge of which is located between the peripheral edge of the molten section (Y) and the center (C) of the molten section (Y) and which includes the center (C).
[0005]
Laser welding method, according to claim 3, characterized by the fact that: when irradiating the second laser beam (L2), the second laser beam (L2) is designed so that a columnar crystal structure grows from the peripheral edge of the molten section (Y) to the center (C) of the molten section (Y) together with the progress of solidification.
[0006]
Laser welding method, according to claim 4, characterized by the fact that: a second laser beam irradiation is initiated after a columnar crystal structure grows from the peripheral edge of the molten section (Y) towards the center (C) of the molten section (Y) in order to surround the center (C) of the fused section (Y) together with the progress of solidification and then the growth of an equiaxial crystal structure is initiated after the growth of said columnar crystal structure is completed in a period after the irradiation of the first laser beam (L1 ) and before the irradiation of the second laser beam (L2); and when irradiating the second laser beam (L2), the second laser beam (L2) is designed so that the equiaxial crystal structure remains in a way that surrounds the center (C) of the molten section (Y) and that the structure columnar crystal grow from the equiaxial crystal structure to the center (C) of the fused section (Y).
[0007]
Laser welding method, according to claim 1, characterized by the fact that: when irradiating the second laser beam (L2), the second laser beam (L2) is projected onto the solidified section (G) in which the molten section (Y) is solidified, so as to fuse the solidified section (G) again, and the second laser beam (L2) is designed so that a cooling rate, in which the region that includes the center of the solidified section (G) and close to it and that are fused again by the irradiation of the second laser beam (L2) is solidified, it is slower than the cooling rate, in which the region that includes the center (C) of the molten section (Y) and its surroundings is solidified after the irradiation of the first laser beam (L1 ), in a position on a peripheral edge of the region that includes the center of the solidified section (G) and its surroundings being determined as the initial irradiation position, or in a region that is surrounded by the peripheral edge of the region that includes the center of the solidified section (G) and the vicinity of the same co nfigured as the initial irradiation region.
[0008]
Laser welding method, according to claim 7, characterized by the fact that: the solidified section (G) includes: an equiaxial crystal region that is formed with an equiaxial crystal structure to include the center of the solidified section (G); and a columnar crystal region that is formed with a columnar crystal structure in a way to surround the equiaxial crystal region from the peripheral edge of the solidified section (G) towards the equiaxial crystal region; and the second laser beam (L2) is designed so that the equiaxial crystal structure of the equiaxial crystal region becomes the columnar crystal structure.
[0009]
Laser welding method, according to claim 7, characterized by the fact that: the solidified section (G) includes: an equiaxial crystal region that is formed with an equiaxial crystal structure in such a way as to include the center of the solidified section (G); and a columnar crystal region that is formed with a columnar crystal structure in a way to surround the equiaxial crystal region from the peripheral edge of the solidified section (G) towards the equiaxial crystal region; and the second laser beam (L2) is projected in the equiaxial crystal region so that a part of the equiaxial crystal structure of the equiaxial crystal region surrounds the center of the solidified section (G) and so that the remaining crystal structure of the region equiaxial crystal becomes the columnar crystal structure.
[0010]
Welding structure, comprising: a welding section (G) in which several parts of metal workpieces (W1, W2) are fused by a laser beam and welded, characterized by the fact that the weld section (G) is formed from a first columnar crystal region (G1), an equiaxial crystal region (G2), and a second columnar crystal region (G3) in a direction from a peripheral edge (S) of the weld section (G) towards a center (C) of the weld section (G), the first columnar crystal region (G1) being formed from a columnar crystal structure in which a columnar crystal extends from the peripheral edge (S) of the weld section (G), the equiaxial crystal region (G2) being formed from the first columnar crystal region (G1) and formed from an equiaxial crystal structure that is formed to surround the center (C) of the weld section (G), and the second columnar crystal region (G3) being formed from said equiaxial crystal region (G2) to the center (C) of the weld section (G ) and formed from the columnar crystal structure in which the columnar crystal extends towards the center (C) of the weld section (G).
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同族专利:
公开号 | 公开日
EP2960007B1|2017-07-19|
US20150283648A1|2015-10-08|
KR20150116794A|2015-10-16|
CN107116302A|2017-09-01|
JP2015199097A|2015-11-12|
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JP6032236B2|2016-11-24|
EP2960007A2|2015-12-30|
US11084126B2|2021-08-10|
KR20170002353A|2017-01-06|
EP2960007A3|2016-04-20|
US20190070695A1|2019-03-07|
CN107116302B|2019-09-24|
BR102015007881A2|2016-04-19|
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CN104972223A|2015-10-14|
CN104972223B|2017-01-11|
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法律状态:
2016-04-19| B03A| Publication of a patent application or of a certificate of addition of invention [chapter 3.1 patent gazette]|
2018-10-30| B06F| Objections, documents and/or translations needed after an examination request according [chapter 6.6 patent gazette]|
2019-08-06| B06U| Preliminary requirement: requests with searches performed by other patent offices: procedure suspended [chapter 6.21 patent gazette]|
2020-11-10| B09A| Decision: intention to grant [chapter 9.1 patent gazette]|
2021-01-12| B16A| Patent or certificate of addition of invention granted|Free format text: PRAZO DE VALIDADE: 20 (VINTE) ANOS CONTADOS A PARTIR DE 08/04/2015, OBSERVADAS AS CONDICOES LEGAIS. |
优先权:
申请号 | 申请日 | 专利标题
JP2014-079702|2014-04-08|
JP2014079702A|JP6032236B2|2014-04-08|2014-04-08|Laser welding method and welded structure|
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