Numéro |
J. Phys. IV France
Volume 120, December 2004
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Page(s) | 299 - 306 | |
DOI | https://doi.org/10.1051/jp4:2004120034 |
J. Phys. IV France 120 (2004) 299-306
DOI: 10.1051/jp4:2004120034
Modelling the Marangoni convection in laser heat treatment
J.-M. Drezet1, S. Pellerin1, C. Bezençon2 and S. Mokadem21 Calcom ESI SA, Parc Scientifique, 1015 Lausanne, Switzerland
2 Laboratoire de Métallurgie Physique, EPF-Lausanne, 1015 Lausanne, Switzerland
Abstract
Epitaxial Laser Metal Forming (E-LMF) consists in impinging a jet of
metallic powder onto a molten pool formed by controlled laser heating and
thereby, generating epitaxially a single crystal deposit onto the damaged
component. This new technique aims to be used for the repair and reshape
single crystal gas turbine components. Because of the very localised melting
pool, the high temperature gradients produced during the process must be
carefully controlled in order to avoid both the columnar-to-equiaxed
transition (CET) and the appearance of hot tears. To this end, heat flow
modelling is required to establish the relationship between process
parameters such as laser power, beam diameter and scanning speed, and the
local solidification conditions. When modelling the heat transfer within the
sample, it is necessary to include the liquid flow pattern generated by the
surface tension driven convection known as the Marangoni effect. Indeed, the
fluid flow in the liquid pool dictates the shape of the traces as shown by
the measurements carried out at EPF-Lausanne in re-melting experiments. A
three dimensional (3D) model is implemented in the finite element software
calcosoft
in order to model the
development of the fluid convection within the liquid pool. It is shown that
the velocities due to natural convection are of the order of 1 mm/sec
whereas Marangoni convection produces velocities of the order of 1 m/sec.
Moreover, at low scanning speeds, the liquid pool becomes larger than the
beam diameter and the development of Marangoni eddies leads to a widening
and deepening of the pool. The local solidification conditions such as the
thermal gradient and the solidification speed can be extracted at both the
solidus and liquidus temperatures to assess the risk of CET and hot
cracking.
© EDP Sciences 2004