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Technology of laser deposition of narrow bead overlays using solid and flux-cored wires

机译:使用实芯和药芯焊丝激光沉积窄珠层的技术

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The use of high-power diode laser in the process of surfacing with a wire filler material makes it possible to deposit high quality, narrow beads on both flat surfaces and working edges of, say, tools. High quality of overlays feed is a decisive one when the weld- face quality is considered. Too low a rate results in a drop-melting mode of the wire and produces a very uneven weld face, the uneveness corresponds to the instants at which separation of drops of the molten metal from the wire end takes place (Fig 4). Increase of the rate to over the optimal value produces, for the given wire and power of the laser beam, an overlay characterised by partly melted wire elements which then appear on the weld face (Fig 5). Similarly, the quality of the weld face is affected by the location of the wire terminal with respect to the laser beam focus. As the depth of advance of the wire into the laser-beam increases, the surface of it absorbing laser radiation, also increases. The mode of the wire melting changes from continuous to interrupted droplet-form, and a considerable uneveness in the weld face is produced (Fig 4). With a solid wire it becomes possible to locate its terminal within the boundary of the laser-beam at about 1/3 of its length (Fig 3). A further shift of the wire terminal into the laser beam results in the droplet mode of its melting. Positioning of a flux-cored wire on the edge of the laser-beam focus will produce an overlay with fragments of partially melted elements of the wire, just as will be the case when the wire is shifted along the transverse axis of the laser beam focus (Fig 5). Overlays with smooth and even weld faces were deposited only when the wire terminal was located at about 1/3 of the focal length (Fig 3). The very small difference between the width of the laser beam focus, and the wire diameter calls, in both cases, for the positioning of the wire terminal exactly in the middle of the focus width. Even a minimal change in the location of the wire end will immediately produce a deterioration in the quality of the deposited overlay by leaving partly melted elements of the wire protruding from the weld face (Fig 5).
机译:在用焊丝填充材料进行堆焊的过程中使用大功率二极管激光器,可以在工具的平坦表面和工作边缘上沉积高质量的窄珠。考虑到焊接面质量,高质量的堆焊层是决定性的因素。太低的速度会导致焊丝的熔滴模式,并产生非常不均匀的焊接面,不均匀度对应于熔融金属滴从焊丝末端分离的瞬间(图4)。对于给定的激光束和功率,将速率增加到超过最佳值会产生一个覆盖层,该覆盖层的特征是部分熔化的焊丝元素随后出现在焊接面上(图5)。类似地,焊接面的质量受电线端子相对于激光束焦点的位置的影响。随着导线进入激光束的深度增加,吸收激光辐射的导线表面也会增加。焊丝熔化的方式从连续的液滴状变为中断的液滴状,并在焊缝表面产生相当大的不均匀性(图4)。使用实心线,可以将其端子定位在激光束边界内大约其长度的1/3处(图3)。导线端子进一步移入激光束会导致其熔化的液滴模式。将药芯焊丝放置在激光束焦点的边缘将产生覆盖部分熔化的焊丝元素的碎片,就像当焊丝沿着激光束焦点的横轴移动时一样(图5)。仅当电线端子位于焦距的约1/3时,才能沉积具有平滑且平整的焊接面的覆盖层(图3)。在两种情况下,激光束聚焦的宽度和导线直径之间的很小差异都要求将导线端子准确地定位在聚焦宽度的中间。焊丝末端位置的最小变化,都会使焊丝的部分熔化元素从焊接面突出(图5),从而立即导致熔敷层质量下降。

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