Challenges in Thermo-mechanical Analysis of Friction Stir Welding Processes.pdf
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ORIGINAL PAPER
Challenges in Thermo-mechanical Analysis of Friction Stir
Welding Processes
N. Dialami1 ? M. Chiumenti1 ? M. Cervera1 ? C. Agelet de Saracibar1
Received: 21 December 2015 / Accepted: 29 December 2015
CIMNE, Barcelona, Spain 2016
Abstract This paper deals with the numerical simulation
of friction stir welding (FSW) processes. FSW techniques
are used in many industrial applications and particularly in
the aeronautic and aerospace industries, where the quality
of the joining is of essential importance. The analysis is
focused either at global level, considering the full com-
ponent to be jointed, or locally, studying more in detail the
heat affected zone (HAZ). The analysis at global (structural
component) level is performed defining the problem in the
Lagrangian setting while, at local level, an apropos kine-
matic framework which makes use of an efficient combi-
nation of Lagrangian (pin), Eulerian (metal sheet) and ALE
(stirring zone) descriptions for the different computational
sub-domains is introduced for the numerical modeling. As
a result, the analysis can deal with complex (non-cylin-
drical) pin-shapes and the extremely large deformation of
the material at the HAZ without requiring any remeshing or
remapping tools. A fully coupled thermo-mechanical
framework is proposed for the computational modeling of
the FSW processes proposed both at local and global level.
A staggered algorithm based on an isothermal fractional
step method is introduced. To account for the isochoric
behavior of the material when the temperature range is
close to the melting point or due to the predominant
deviatoric deformations induced by the visco-plastic
response, a mixed finite element technology is introduced.
The Variational Multi Scale method is used to circumvent
the LBB stability condition allowing the use of linear/linear
P1/P1 interpolations for displacement (or velocity, ALE/
Eulerian formulation) and pressure fields, respectively. The
same stabilization stra
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