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Accurate Single Point Incremental Forming Simulations using Solid-Shell Elements

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Accurate Single Point Incremental Forming

Simulations using Solid-Shell Elements

Carlos Felipe Guzm´an1, Jos´e Il´ıdio Velosa de Sena2,

Laurent Duchˆene1 and Anne Marie Habraken1,3

1Department ArGEnCo, division MS2F, Universit´e de Li`ege, Belgium. 2Department of Mechanical Engineering, centre GRIDS, University of Aveiro, Portugal

3Research Director of the Fonds de la Recherche Scientifique-FNRS

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Presentation contents

1 Introduction

2 Simulations

3 Results

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Contents

1 Introduction

2 Simulations 3 Results

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Single point incremental forming

A sheet metal is deformed by a small tool.

The tool could be guided by a CNC (milling machine, robot).

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Single point incremental forming

Dieless, with high sheet formability. Easy shape generation.

For rapid prototypes, small batch productions, etc.

Challenges Geometrical inaccuracy. Process mechanics. Increased formability. Motivations

Through the thickness gradient are important.

2D constitutive laws cannot be used.

New advances on element formulation in FE codes.

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Single point incremental forming

Dieless, with high sheet formability. Easy shape generation.

For rapid prototypes, small batch productions, etc.

Challenges Geometrical inaccuracy. Process mechanics. Increased formability. Motivations

Through the thickness gradient are important.

2D constitutive laws cannot be used.

New advances on element formulation in FE codes.

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Single point incremental forming

Dieless, with high sheet formability. Easy shape generation.

For rapid prototypes, small batch productions, etc.

Challenges Geometrical inaccuracy. Process mechanics. Increased formability. Motivations

Through the thickness gradient are important.

2D constitutive laws cannot be used.

New advances on element formulation in FE codes.

(8)

Contents

1 Introduction

2 Simulations

3 Results

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Simulations

Material: DC01 ferritic steel (1 mm thickness). Two slope pyramid:

60◦ 30◦ y z 1 35 52 6 52 35 1 60 90 182 182 x y

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Constitutive modeling

Isotropic elasto-plastic constitutive law (HILL3D_KI.F). Voce and Armstrong-Frederick isotropic/kinematic hardening.

σY = σY 0+ K 1 − exp −nP ˙ X = Cx  Xsat˙P− ˙PX  Material parameters: σY 0 = 158 MPa Cx = 257

K = 255 MPa Xsat = 4 MPa

n = 13

Identification through classical (tensile, monotonic/Bauschinger shear) tests (OPTIM).

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Constitutive modeling

Isotropic elasto-plastic constitutive law (HILL3D_KI.F). Voce and Armstrong-Frederick isotropic/kinematic hardening.

σY = σY 0+ K 1 − exp −nP ˙ X = Cx  Xsat˙P− ˙PX  Material parameters: σY 0 = 158 MPa Cx = 257

K = 255 MPa Xsat = 4 MPa

n = 13

Identification through classical (tensile, monotonic/Bauschinger shear) tests (OPTIM).

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Mesh and boundary conditions

Displacement-controlled implicit simulation.

One layer with 2248 elements. Symmetry and rotational boundary conditions (BINDS.F): x y • O • P

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Solid-shell element

Formulation

Large aspect ratios =⇒ locking Enhanced Assumed Strain (EAS) Assumed Natural Strain (ANS)

• • • • • • • • • • ⊗ ⊗ ⊗ ←→ • • • • • • • • • • ⊗ ⊗ ⊗ ⊗ ... .. . .. . .. . ←→ • • • • • • • • • • ⊗

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Assumed natural strain

U com ANS B linear interpolation BANS

Sampling points (transverse shear and transverse normal strains):

r s t A C • r s t B • D • sr t E F • G H •

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Assumed natural strain

U com ANS B linear interpolation BANS

Sampling points (transverse shear and transverse normal strains):

r s t A C • r s t B • D • sr t E F • G H •

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Enhanced assumed strain

Enhanced strain field

 = com+ EAS com= ∆su = B(r , s, t)U EAS = G(r , s, t)α = |J0| |J(r , s, t)|F −T 0 M(r , s, t)α [M] =

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Enhanced assumed strain

Enhanced strain field

 = com+ EAS com= ∆su = B(r , s, t)U EAS = G(r , s, t)α = |J0| |J(r , s, t)|F −T 0 M(r , s, t)α [M] =         r 0 0 0 0 0 0 0 0 0 0 0 0 0 0 rs rt 0 0 0 0 0 0 0 rst 0 0 0 0 0 0 s 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 rs st 0 0 0 0 0 0 rst 0 0 0 0 0 0 t 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 rt st 0 0 0 0 0 rst 0 0 0 0 0 0 r s 0 0 0 0 rt st 0 0 0 0 0 0 0 0 0 0 rs 0 0 0 0 0 rst 0 0 0 0 0 0 0 r t 0 0 0 0 rs st 0 0 0 0 0 0 0 0 0 rt 0 0 0 0 0 rst 0 0 0 0 0 0 0 0 s t 0 0 0 0 rs rt 0 0 0 0 0 0 0 0 st 0 0 0 0 0 rst         03 EAS modes

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Enhanced assumed strain

Enhanced strain field

 = com+ EAS com= ∆su = B(r , s, t)U EAS = G(r , s, t)α = |J0| |J(r , s, t)|F −T 0 M(r , s, t)α [M] =         r 0 0 0 0 0 0 0 0 0 0 0 0 0 0 rs rt 0 0 0 0 0 0 0 rst 0 0 0 0 0 0 s 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 rs st 0 0 0 0 0 0 rst 0 0 0 0 0 0 t 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 rt st 0 0 0 0 0 rst 0 0 0 0 0 0 r s 0 0 0 0 rt st 0 0 0 0 0 0 0 0 0 0 rs 0 0 0 0 0 rst 0 0 0 0 0 0 0 r t 0 0 0 0 rs st 0 0 0 0 0 0 0 0 0 rt 0 0 0 0 0 rst 0 0 0 0 0 0 0 0 s t 0 0 0 0 rs rt 0 0 0 0 0 0 0 0 st 0 0 0 0 0 rst         11 EAS modes

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Enhanced assumed strain

Enhanced strain field

 = com+ EAS com= ∆su = B(r , s, t)U EAS = G(r , s, t)α = |J0| |J(r , s, t)|F −T 0 M(r , s, t)α [M] =         r 0 0 0 0 0 0 0 0 0 0 0 0 0 0 rs rt 0 0 0 0 0 0 0 rst 0 0 0 0 0 0 s 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 rs st 0 0 0 0 0 0 rst 0 0 0 0 0 0 t 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 rt st 0 0 0 0 0 rst 0 0 0 0 0 0 r s 0 0 0 0 rt st 0 0 0 0 0 0 0 0 0 0 rs 0 0 0 0 0 rst 0 0 0 0 0 0 0 r t 0 0 0 0 rs st 0 0 0 0 0 0 0 0 0 rt 0 0 0 0 0 rst 0 0 0 0 0 0 0 0 s t 0 0 0 0 rs rt 0 0 0 0 0 0 0 0 st 0 0 0 0 0 rst         24 EAS modes

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Solid-shell element

. . . in LAGAMINE

SSH3D RESS

Enhanced Assumed Strain (EAS) modes 24 1

Assumed Natural Strain (ANS) version 4

-In-plane integration full reduced*

Stabilization technique - Yes

⊗ ⊗ ⊗ ⊗ ... .. . .. . .. .

⊗ .. . SSH3D.F RESS3.F

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Running simulations

Not easy. . .

Complex toolpath and small contact zone. Several time increments.

Simulations can take weeks.

NIC machine

Near 1000 cores and 5 Tb memory.

LAGAMINE (and PREPRO) compiled in Linux. Possibility of using other machines

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Running simulations

Not easy. . .

Complex toolpath and small contact zone. Several time increments.

Simulations can take weeks.

NIC machine

Near 1000 cores and 5 Tb memory.

LAGAMINE (and PREPRO) compiled in Linux. Possibility of using other machines

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Contents

1 Introduction 2 Simulations

3 Results

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Shape results

Numerical/experimental (DIC) comparison Y = 0

−90 0 90 −90 −60 −10 X [mm] Z [mm ] 10 90 −90 −60 −10 X [mm] Numerical Experimental Nominal

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Shape results

Numerical/experimental (DIC) comparison Y = 0

−90 0 90 −90 −60 −10 X [mm] Z [mm ] 10 90 −90 −60 −10 X [mm] Numerical Experimental Nominal

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Shape results

Numerical/experimental (DIC) comparison Y = 0

−90 0 90 −90 −60 −10 X [mm] Z [mm ] 10 90 −90 −60 −10 X [mm] Numerical Experimental Nominal

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EAS and mesh influence

Strong EAS mode influence. Small mesh influence.

0 90 −90 Y [mm] Z [mm ] 03 modes 11 modes 24 modes 0 90 −90 Y [mm] Z [mm ] Coarse mesh Fine mesh

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Force evolution

Both EAS modes and mesh influence.

0 600 900 0 4 8 Time [s] F o rces [kN ] 03 EAS 11 EAS 24 EAS (coarse) 24 EAS (fine)

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Contents

1 Introduction 2 Simulations 3 Results

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Conclusions

EAS modes influence the accuracy of the results.

The elements are subjected to deformation modes reproduced only using the EAS technique.

ANS version has no effect on both the shape and the force. Material identification procedure important.

Future work

Identify the most important EAS modes.

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Conclusions

EAS modes influence the accuracy of the results.

The elements are subjected to deformation modes reproduced only using the EAS technique.

ANS version has no effect on both the shape and the force. Material identification procedure important.

Future work

Identify the most important EAS modes.

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Accurate Single Point Incremental Forming

Simulations using Solid-Shell Elements

Carlos Felipe Guzm´an1, Jos´e Il´ıdio Velosa de Sena2,

Laurent Duchˆene1 and Anne Marie Habraken1,3

1Department ArGEnCo, division MS2F, Universit´e de Li`ege, Belgium. 2Department of Mechanical Engineering, centre GRIDS, University of Aveiro, Portugal

3Research Director of the Fonds de la Recherche Scientifique-FNRS

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References

Henrard, C., Bouffioux, C., Eyckens, P., Sol, H., Duflou, J., van Houtte, P., Van Bael, A., Duchˆene, L., Habraken, A. M., Dec. 2010. Forming forces in single point incremental forming: prediction by finite element simulations, validation and sensitivity. Computational Mechanics 47 (5), 573–590.

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