tube hydroforming
DESCRIPTION
TRANSCRIPT
Finite element analysis of tube hydroforming process in a rectangular die
Presented by Khushboo Shrivastava
Roll No. 123370001
AimUse the Finite Element Method to explore the
plastic flow pattern of a circular tube that is hydraulically expanded or crushed into a rectangular cross-section.
DEFORMThe plastic flow patterns of the forming tube
and the thickness distribution of the formed product are explored while a circular tube is expanded or crushed into a rectangular cross-section, using a commercially available FE code “DEFORM”.
Finite element modelingAn implicit and static FE code “DEFORM”The finite element code is based on the flow
formulation approach using an updated Lagrange procedure. The basic equation for the finite element formulation from the variational approach is
Finite Element Simulations AssumptionsDie is rigid, the tube is rigid-plastic,The plastic deformation of the tube is under a
plane strain state, and the interface between the tube
Die has a constant friction coefficientThe flow stress of the tube material of SUS 304 is
assumed to be expressed by a power law of its equivalent strain, i.e.σ=Ke^n, where K = 1452
MPa is the strength coefficient and n = 0.6 is the strain-hardening exponent.
Modelling ParameterFour-node isoparametric elements are used.The tube is divided into about 1000 elements,
and there are six layers of elements in the thickness direction.
The configurations of the meshes in the tube before crushing and preforming are shown in
Fig.
Iteration MethodsDirect iteration methods Generate a good initial guess for the
Newton Raphson methodNewton-Raphson: Speedy final convergence
Simulation works for expansionThe upper die is always in contact with the bottom
die without movement.The internal pressure input into the tube is
increased gradually. Following the increase of the internal pressure, the tube comes in contact with the short sides of the die and then the corner radius of the free bulged region, R, decreases. When the programmed internal pressure reaches 300 MPa, the simulation is stopped, and the corner radius and the thickness distribution of the formed product are
measured.
Simulation works for crushingThe dimension of the upper die is the same as
that for the expansion process. The step increment is set to be 0:01 s. At the beginning and early stage of the crushing process, no internal pressure is input into the tube to make the tube expanded outwards. On the contrary, two side dies with a radius of 15 mm at the left and right sides of the tube are used to push the tube inwards to prevent the tube from being pinched by the upper and lower dies as the upper die goes downwards.
Simulation works for crushingAfter the side dies move 17 mm inwards, as
shown in Fig. 4(b), the side dies move backwards immediately and then the crushing process starts. As the upper die is ready to touch the lower die, a gradually increased pressure is input into the tube to calibrate the tube and make the tube material 1ow into the corners of the die as much as possible. The crushed and hydroformed
product is shown in Fig. 4(d).
Results from the simulation
ConclusionsFrom the simulation results, some conclusions can
be drawn as below:The maximum forming pressure needed by
crushing processes is only 5% of that by hydraulic expansion processes.
The maximum crushing force needed in the crushing process is only about 7% of the clamping force in the hydraulic expansion process.
The thickness distribution of the formed product obtained by crushing processes is much more uniform than that by hydraulic expansion processes.
ConclusionsThe expansion process is a very simple forming
process that does not need extra equipment, such as the side dies and cylinders, or a procedure control for the internal pressure and movement of the dies. However, it needs a large press machine and a high-pressure hydraulic system.
By introducing the crushing process into the hydroforming processes, the clamping forces and forming pressures
can be greatly reduced. Furthermore, highly uniform thickness distributions of the formed products
can be obtained.
ReferencesF. Dohmann, Ch. Hartl, Tube hydroforming:
research and practical application, J. Mater. Proc. Technol. 71 (1997) 174–186
Finite element analysis of tube hydroforming processes in a rectangular die Yeong-Maw Hwanga; ∗, Taylan Altanb
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