LS-DYNA Anwendungsmöglichkeiten für die Fügesimulation ... · 15 For a 3D representation...

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LS-DYNA Anwendungsmöglichkeiten für die Fügesimulation Thomas Klöppel DYNAmore GmbH DYNAmore GmbH

Transcript of LS-DYNA Anwendungsmöglichkeiten für die Fügesimulation ... · 15 For a 3D representation...

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LS-DYNA –

Anwendungsmöglichkeiten

für die Fügesimulation

Thomas Klöppel DYNAmore GmbH

DYNAmore GmbH

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■ Introduction to LS-DYNA

■ Clinches and Rivets

■ Friction Stir Welding

■ Inductive Welding

■ Resistive Welding

Agenda

DYNAmore GmbH

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1976: John Hallquist develops DYNA3D at Lawrence Livermore National Laboratories

1987: John Hallquist founds LSTC in Livermore CA, DYNA3D becomes LS-DYNA3D

1988: Prof. Schweizerhof + co-workers start with crash simulations in Germany

2001: DYNAmore is established

2011: DYNAmore acquires ERAB Nordic

2011: DYNAmore assigned as Master distributor

2011: DYNAmore SWISS established

2013: DYNAmore Italia S.r.l. established

LS-DYNA – LSTC – DYNAmore History

DYNAmore GmbH

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LSTC Product Range

FREE OF CHARGE!

LS-DYNA

LS-PrePost LS-OPT/LS-TaSC

USA Dummies & Barriers DYNAmore GmbH

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LS-DYNA R8 – The Applications

Automotive

Crash and Safety NVH Durability

Aerospace

Bird strike Containment Crash

Manufacturing

Stamping Forging

Consumer

Products

Civil Engineering

Concrete structures Earthquake safety Wind- & Waterpower

Elektronics

Drop analysis Package analysis Thermal

Defense

Detonations

Penetrations

Biomechanics

DYNAmore GmbH

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■ Combine the capabilities

■ Explicit/ Implicit structural solver ■ Thermal solver & heat transfer ■ Incompressible fluid solver (ICFD) ■ Compressible fluid solver (CESE) ■ Electromagnetics solver (EM) ■ Frequency domain, acoustics, modal analysis ■ Finite elements, iso-geometric elements,

ALE, EFG, SPH, DEM, CPM, … ■ User elements, materials, loads

■ Into one scalable code for ■ highly nonlinear transient problems ■ static problems

■ To enable the solution of ■ coupled multi-physics and ■ multi-stage problems

■ On massively parallel systems

LS-DYNA R8 – The Multiphysics Solver

[coil heating water]

Heart valve: Courtesy of H. Mohammadi,

McGill University

DYNAmore GmbH

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■ No need for co-simulation, as all solvers are included!

LS-DYNA R8 – The Multiphysics Solver

Temperature Pl

astic

Wor

k D

ispl

acem

ent

Thermal Solver Implicit

Double precision

Mechanical Solver Implicit / Explicit

Double precision / Single precision

EM Solver Implicit

Air (BEM) Conductors (FEM) Double precision

Fluid Solver Implicit / Explicit

ICFD / CESE ALE / CPM

Double precision

DYNAmore GmbH

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EFG SPG

MEFEM MLPG

ICFD

LS-DYNA R8 – Continuum Meshfree Methods

Solid Fluid Gas

F

T

p

Material law for stress tensor Equation of State

Crashworthiness Airbag

Metal Forming

Material

Strength

Momentum

Extrusion

Forging

SPH Hydroplaning

Sloshing

Bird strike

Explosion/

Penetration

Fracture

Incompressible

fluids

Splashing

Foam packing CPM

Kinetic Molecular theory

(Maxwell-Boltzman Equ.)

DYNAmore GmbH

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■ Introduction to LS-DYNA

■ Clinches and Rivets

■ Friction Stir Welding

■ Inductive Welding

■ Resistive Welding

Agenda

DYNAmore GmbH

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■ 2 or more sheets are to be joined together

■ Highly distorted structures

■ Topology changes for self piercing rivets

Clinches and Rivets

DYNAmore GmbH

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■ METHOD 1: Use 2D axisymmetric remeshing: ■ Switch on R-adaptivity

in *PART set adpopt=2 ■ Use volume-weighted axisymmetric solid

in *SECTION_SHELL set eltyp=15 ■ Use reasonable values for adaptivity

*CONTROL_ADAPTIVE *PART_ADAPTIVE_FAILURE

2D axisymmetric model

DYNAmore GmbH

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■ Simulation not restricted to 2 blanks

Extension to 3 blanks

DYNAmore GmbH

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■ Cross tension test

■ Tension test

Serviceability analysis

DYNAmore GmbH

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■ Cross tension test

■ Tension test

Serviceability analysis

DYNAmore GmbH

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■ For a 3D representation adaptive EFG seems to be promising

■ Basic ideas ■ Replace the continuum by a set of particles ■ Construction of shape functions without a mesh

[Lucy 1977, Gingold & Monaghan 1977, Liu 2003]

■ In contrast to other element-free methods, a background

mesh (or integration cells) is needed ■ Define the physical domain ■ Contact conditions ■ Impose boundary conditions ■ Perform volume integration via “stress points”

■ Based on Galerkin weak form of the problem

Modeling Clinches and Rivets in 3D with EFG

e

SPH nodal

integration

EFG stress point

integration DYNAmore GmbH

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■ Adaptive EFG might be needed to deal with „ severe material deformation

■ Current numerical limitations ■ RH-adaptivity for solids (H-adaptivity is limited to shells) ■ Failure analysis is limited to metal cutting problems ■ Not applicable to rubber-like materials

Adaptive EFG

DYNAmore GmbH

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■ Computation times ■ LS-DYNA (explicit): 1 day on 6 CPU ■ LS-DYNA (implicit): 20 min on 6 CPU

Cold forming of a pre-stressed rivet head

DYNAmore GmbH

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■ Computation times ■ LS-DYNA (explicit): 1 day on 6 CPU ■ LS-DYNA (implicit): 20 min on 6 CPU

Cold forming of a pre-stressed rivet head

DYNAmore GmbH

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■ Introduction to LS-DYNA

■ Clinches and Rivets

■ Friction Stir Welding

■ Inductive Welding

■ Resistive Welding

Agenda

DYNAmore GmbH

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■ Process:

■ Two materials ■ Fast rotating cylinder ■ Cylinder is translated through the seam ■ Due to the friction, materials meld ■ Rotation mixes the materials

■ Material mixing requires meshless methods

■ The SPH method is most suitable for these high velocities

Friction stir welding

Courtesy Kirk Fraser (Predictive Engineering)

DYNAmore GmbH

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■ Basic ideas ■ Replace the continuum by a set of particles ■ Construction of shape functions without a mesh

[Lucy 1977, Gingold & Monaghan 1977, Liu 2003]

■ Integral interpolant as approximation function ■ Exploitation of the identities

Smoothed-Particle Hydrodynamics (SPH)

DYNAmore GmbH

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■ Approximation of the displacement/velocity

■ Approximation of the displacement/velocity gradient

Smoothed-Particle Hydrodynamics (SPH)

Kernel function θ

DYNAmore GmbH

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■ Double sided FSW @ 600 RPM, 1200 mm/min ■ Plastic work and friction energy to heat

Friction Stir Welding Example

Courtesy Kirk Fraser (Predictive Engineering)

temperature contours material mixing DYNAmore GmbH

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■ Double sided FSW @ 600 RPM, 1200 mm/min ■ Plastic work and friction energy to heat

Friction Stir Welding Example

Courtesy Kirk Fraser (Predictive Engineering)

temperature contours material mixing DYNAmore GmbH

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■ Introduction to LS-DYNA

■ Clinches and Rivets

■ Friction Stir Welding

■ Inductive Welding

■ Resistive Welding

Agenda

DYNAmore GmbH

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■ Electro-magnetic solver at a glance and its connection to the other solvers

Electromagnetism (EM) Solver in LS-DYNA

BjEF e

Lorentz forces Joule heating 2dQ

p j Rdt

Displacement Temperature

Mechanical Solver Thermal Solver

Ampere„s Law: Faraday„s Law: Gauss law: Gauss flux theorem: Continuity:

Ohm‟s law: sjEj

: rotation : divergence E : electric field B : magnetic flux density j : total current density js : source current density ε, μ, and σ : material

electrical properties

EM Solver

Maxwell Equations

Eddy-current formulation

DYNAmore GmbH

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■ Subcycling for the Joule (induced) heating problem ■ Timescale of oscillating coil is much smaller than for the total problem ■ Many small EM time steps would be needed ■ Introduction of a “micro” and “macro” time step

Electromagnetism

DYNAmore GmbH

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■ Preparation for welding applications ■ Heating of a plate by induction

Electromagnetism

Exp

erim

ent

LS-D

YNA

Courtesy of Miro Duhovic

DYNAmore GmbH

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■ Continuous induction welding [Moser & Mitschang 2012] ■ Carbon-fiber reinforcements form conductive loops ■ Joule heating to the melting point ■ Pressure application for consolidation

Electromagnetism

Courtesy of Miro Duhovic

[Duhovic et al. 2013] DYNAmore GmbH

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■ Introduction to LS-DYNA

■ Clinches and Rivets

■ Friction Stir Welding

■ Inductive Welding

■ Resistive Welding

Agenda

DYNAmore GmbH

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Analysis of the welding process

[greitmann2013]

[tu-chemnitz]

DYNAmore GmbH

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■ Typical force, current and voltage curves during the resistance spot welding

Typical welding process

[wick2012] DYNAmore GmbH

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Aim of the process simulation

[DIN14329]

deu .. indentation width eu .. indentation depth dn .. nugget width p .. penetration

■ Determination of the nugget geometry according to DIN 4329

DYNAmore GmbH

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■ Influence of electrode contact angle on the nugget size and shape

Aim of the process simulation

[zhang2005] DYNAmore GmbH

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■ 2 Electrods ■ only foot of the electrode meshed ■ electrode shape according DIN 5821

■ 2 metal sheets

Geometry

[zhang2005]

DYNAmore GmbH

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■ Material definitions (incl. electromagnetical properties)

■ Definition of an electrical circuit

■ Definition of an electro-magnetic contact

Electro-Magnetical Input

MID 1 (EM)

MID 1 (EM)

MID 2 (EM)

MID 3 (EM)

Source (Current)

Output (Current) DYNAmore GmbH

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History of the 3d temperature field

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DYNAmore GmbH

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■ Contours and vector plot of the current density

Contours and Vector Plot of the Current Density

[zhang2005]

DYNAmore GmbH

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■ Contours plot of the electric field

■ Contours and vector plot of the electric field

Contours and Vector Plot of the Electric Field

DYNAmore GmbH

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Thank you!

DYNAmore GmbH