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<metadata xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:dc="http://purl.org/dc/elements/1.1/"><dc:title>Advances in the understanding of the annular laser beam wire cladding process</dc:title><dc:creator>Kotar,	Matjaž	(Avtor)
	</dc:creator><dc:creator>Fujishima,	Makoto	(Avtor)
	</dc:creator><dc:creator>Levy,	Gideon N.	(Avtor)
	</dc:creator><dc:creator>Govekar,	Edvard	(Avtor)
	</dc:creator><dc:subject>annular laser beam</dc:subject><dc:subject>laser wire cladding</dc:subject><dc:subject>nominal workpiece irradiation proportion</dc:subject><dc:subject>process stability</dc:subject><dc:subject>clad geometry</dc:subject><dc:subject>melt pool and workpiece temperature</dc:subject><dc:description>This paper experimentally studies the influence of conventional process parameters (laser beam power, P, workpiece, and wire feeding velocities), and the nominal workpiece irradiation proportion WIP$_N$ parameter, on ALB-WC process stability and generated clad geometry. The study was based on an extensive set of single clad experiments using stainless steel AISI 316L wire of 0.6 mm diameter and a stainless steel AISI 304 workpiece. The results show that the laser beam power required for a stable process increases non-linearly with WIP$_N$, and this relationship can be described by quadratic regression. An increase in either the workpiece or wire feeding velocity respectively causes a reduction or enlargement of the stability region in the P- WIP$_N$ stability diagrams. The influences on stability diagrams are explained by means of the increase in the nominal WIP$_N$ to the effective WIP$_E$, as a result of the clad height generated. With respect to clad geometry, it was shown that an increase in the WIP$_N$ causes a decrease in the dilution ratio, which is linearly correlated with the workpiece and melt pool temperatures, while clad width and height are not influenced by the WIP$_N$. The paper further explains the complex influences of the process parameters observed on process stability and generated clad geometry using a phenomenological description of the ALB-WC process at a low and high nominal WIP$_N$. For this purpose, heat transfer, Marangoni flow, and laser beam reflections are considered qualitatively and supported by IR and visual images of the wire-end and melt pool as well as the workpiece and melt pool temperatures.</dc:description><dc:date>2021</dc:date><dc:date>2021-06-01 07:42:03</dc:date><dc:type>Članek v reviji</dc:type><dc:identifier>127263</dc:identifier><dc:identifier>UDK: 621.9.04(045)</dc:identifier><dc:identifier>ISSN pri članku: 0924-0136</dc:identifier><dc:identifier>DOI: 10.1016/j.jmatprotec.2021.117105</dc:identifier><dc:identifier>COBISS_ID: 52257539</dc:identifier><dc:language>sl</dc:language></metadata>
