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Results and Outlook Development of a Friction Approach for the FE Method of Sheet Metal Forming Based on Multi-Scale Modeling Motivation Prof. Dr.-Ing. B.-A. Behrens Prof. Dr. P.-A. Guidault Goals Methods Dipl.-Math. B. Homann ViVaCE „Virtual Materials and their Validation: German-French School of Computational Engineering” – IRTG 1627 Correlations between occurring normal force, effective plastic strain, direction of motion, and resulting roughness = 1 n , max Function for friction coefficient of change in roughness, sliding velocity, and direction of motion = 2 , ∆, Angle between direction of motion and rolling direction Angle between direction of measurement and rolling direction Arithm. mean surface roughness measured in to rolling direction n Maximal occurring normal pressure max Maximal occurring effective plastic strain Friction coefficient Current sliding velocity Change in roughness Strong influence of friction on the part quality Existing laws for friction are not adequate for the realistic description of local contact conditions. Investigation of surface topography evolution Material: aluminum alloy AlMg3 (EN AW-5754) Basic experiments: Pressure test (PT) Tensile test (TT) Strip drawing test (SD) Roughness measurement before and after the tests Measurements in and to rolling direction Main influences on deep drawing processes Focus of study: Friction modeling in FE simulation Setup to apply contact pressure Setup for tensile test Setup for strip drawing test Strong influence of friction coefficient μ on the result, e.g. sheet thickness Friction modeling Mathematical description of the friction coefficient Depending on Roughness evolution Forming parameters Implementation In FE software LS-DYNA User subroutine usrfrc in dyn21.F Algorithm of the new friction law Specimens of different rolling directions Longitudinal 0° Transversal 90° Diagonal 45° 59 mm 730 mm 20 mm 9 mm Simulation of basic experiments To analyze the forming parameters With respect to rolling direction x y z Sheet thickness [mm] 1.10 1.08 1.06 1.04 1.02 1.00 0.99 0.97 0.95 0.93 0.91 initial Numerical models of tensile test (upper) and strip drawing test (lower) with evaluated element for roughness calculation Further investigations Further parameter studies to extend the model Adoption/adjustment of the model to different materials ViVaCE-Projects with strong Interaction Multiscale FEM for Rubber Friction on Rough Surfaces (P. Wagner) Multiphysics Homogenization Schemes for Microstructured Interfaces (N. Noii) y x z Initial state Stretched state Evaluated element Specimen Force Chafe body of the machine z x y Initial state Drawn state Evaluated element eps max [−] 0 [μm] Example of roughness-strain dependence of tensile test for -specimen 0° 0° -specimen 0° 90°

Development of a Friction Approach for the FE Method of ... · Results and Outlook Development of a Friction Approach for the FE Method of Sheet Metal Forming Based on Multi-Scale

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Page 1: Development of a Friction Approach for the FE Method of ... · Results and Outlook Development of a Friction Approach for the FE Method of Sheet Metal Forming Based on Multi-Scale

Results and Outlook

Development of a Friction Approach for the FE Method of

Sheet Metal Forming Based on Multi-Scale Modeling

Motivation

Prof. Dr.-Ing. B.-A. Behrens

Prof. Dr. P.-A. Guidault

Goals

Methods

Dipl.-Math. B. Homann

ViVaCE „Virtual Materials and their

Validation: German-French School of

Computational Engineering” – IRTG 1627

• Correlations between occurring normal force, effective plastic strain,

direction of motion, and resulting roughness

𝑅𝑎𝛽 = 𝑓1 𝑓n, 𝑒𝑝𝑠max, α

• Function for friction coefficient of change in roughness, sliding

velocity, and direction of motion

𝜇 = 𝑓2 𝑣, ∆𝑅𝑎, 𝛼

𝛼 Angle between direction of motion and rolling direction

𝛽 Angle between direction of measurement and rolling direction

𝑅𝑎𝛽 Arithm. mean surface roughness measured in 𝛽 to rolling direction

𝑓n Maximal occurring normal pressure

𝑒𝑝𝑠max Maximal occurring effective plastic strain

𝜇 Friction coefficient

𝑣 Current sliding velocity

∆𝑅𝑎 Change in roughness

• Strong influence of

friction on the part

quality

• Existing laws for friction

are not adequate for the

realistic description of

local contact conditions.

Investigation of surface topography evolution

• Material: aluminum alloy AlMg3 (EN AW-5754)

• Basic experiments:

Pressure test (PT)

Tensile test (TT)

Strip drawing test (SD)

• Roughness measurement before and after the tests

• Measurements in and to rolling direction

Main influences on deep drawing processes

Focus of study: Friction modeling in FE simulation

Setup to apply contact pressure

Setup for tensile test

Setup for strip drawing test

Strong influence of friction coefficient µ on the result, e.g. sheet thickness

Friction modeling

• Mathematical description of

the friction coefficient

• Depending on

Roughness evolution

Forming parameters

Implementation

• In FE software LS-DYNA

• User subroutine usrfrc in

dyn21.F Algorithm of

the new friction law

Specimens of different rolling directions

Longitudinal 0°

Transversal 90°

Diagonal 45°

59 mm 730 mm

20 mm 9 mm

Simulation of basic experiments

• To analyze the forming parameters

• With respect to rolling direction

x y

z

Sheet thickness [mm]

1.10

1.08

1.06

1.04

1.02

1.00

0.99

0.97

0.95

0.93

0.91

initial

Numerical models of tensile test (upper) and strip drawing test (lower)

with evaluated element for roughness calculation

Further investigations

• Further parameter studies to extend the

model

• Adoption/adjustment of the model to

different materials

ViVaCE-Projects with strong Interaction

• Multiscale FEM for Rubber Friction on

Rough Surfaces (P. Wagner)

• Multiphysics Homogenization Schemes for

Microstructured Interfaces (N. Noii)

y x

z

Initial state

Stretched state

Evaluated element

Specimen

Force

Chafe body of the machine

z x

y

Initial state Drawn state

Evaluated element

epsmax [−]

𝑅𝑎

0 [

µm

]

Example of roughness-strain dependence

of tensile test for -specimen 0°

0° -specimen

0° 90°