Numerical simulation of mechanically and moisture loaded ...

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1 Institute for Structural Analysis Numerical simulation of mechanically Joint Focussed Meeting of COST Actions IE0601 and FP0802, 2010 “Modeling mechanical behavior of wooden cultural objects” and moisture loaded wooden structures Institute for Structural Analysis Susanne Saft, Michael Kaliske Institute for Structural Analysis www.tu-dresden.de/isd Federal Foundation of Culture, Germany Händel-Haus Halle, Germany Introduction Outline motivation modeling of mechanical behavior modeling of moisture transfer hygro-mechanical coupling examples outlook Institute for Structural Analysis 2

Transcript of Numerical simulation of mechanically and moisture loaded ...

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Institute for Structural Analysis

Numerical simulation of mechanically

Joint Focussed Meeting of COST Actions IE0601 and FP0802, 2010

“Modeling mechanical behavior of wooden cultural objects”

and moisture loaded wooden structures

Institute for Structural Analysis

Susanne Saft, Michael Kaliske

Institute for Structural Analysiswww.tu-dresden.de/isd

Federal Foundation of Culture, Germany

Händel-HausHalle, Germany

Introduction

Outline

• motivation

• modeling of mechanical behavior

• modeling of moisture transfer

• hygro-mechanical coupling

• examples

• outlook

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Introduction

Motivation

restoration of historical music instruments

• conservation of original substance

• maintenance of original usage

large deformations of the structure, local damages

• caused by string loading

• enforced by climatic fluctuations

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analysis of the load bearing behavior of historical keyboard instruments using the Finite Element Method

requirement: appropriate material models for simulation of mechanics, moisture transfer and coupling

potential at material coordinate system

Modeling of Cylindrical Anisotropy

Modeling of Mechanical Behavior

linear-elastic stress-strain-dependency

elasticity tensor in material coordinates

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with respect to

Schmidt, Kaliske [2009]

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rotation between material coordinates and global coordinates

f l b l l d

Modeling of Cylindrical Anisotropy

Modeling of Mechanical Behavior

• rotation of global strains to material coordinates

• rotation of local stresses to global coordinate system

• structural tensor

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center of element

scantling

3 3 3

2 2 2

Modeling of Compression Failure

multi-surface plasticity model with C1-continous yield criterion

Modeling of Mechanical Behavior

• failure due to compression loading

• ductile, nearly plastic behavior

• C1-continuous anisotropic yield criterion

associated flow rule

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Resch, Kaliske [2010]

• associated flow rule

• assumption of linear hardening

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Modeling of Compression Failure

definition of the C1-continuous yield criterion

Modeling of Mechanical Behavior

• yield criterion:

• tensor of strength:

• activation of octant of stress domain:

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Resch, Kaliske [2010]

• strength information:

interface-element formulation

Modeling of Brittle Failure

Modeling of Mechanical Behavior

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Schmidt, Kaliske [2007]

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interface-material approach

di ti d d t t th l

Modeling of Brittle Failure

Modeling of Mechanical Behavior

• direction dependent strength values f and fracture energies G

• coupling of material directions

• C1-continuous material formulation

parameters of the model

• displacement at integration point

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• displacement at integration point

• elastic range

• parameter of C1-continuous damage path

• history variableSchmidt, Kaliske [2007]

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Modeling of Brittle Failure

elastic range

Modeling of Mechanical Behavior

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g

softening range

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C1-continuous transition

elastic range of damage

3

4

Schmidt, Kaliske [2007]

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Modeling of Moisture Diffusion

moisture transport below fibre saturation point (diffusion) described by Fick’s Law

Modeling of Moisture Transfer

described by Fick s Law

• steady state form transient form

• q: moisture flux [kg/(mm²s)]

• ρ0: density in absolute dry condition [kg/mm³]

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• m: moisture content [-]

• D: diffusion coefficient subject to moisture content [mm²/s]

anisotropic tensor of moisture conductivity

Modeling of Moisture Diffusion

Modeling of Moisture Transfer

• approach of Hanhijärvi

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• nonlinearity of D(m) is considered within tangent matrix consistent linearization

Hanhijärvi [1997]

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Why Fick’s Law?

Modeling of Moisture Diffusion

Modeling of Moisture Transfer

• transient form of Fick’s law merely approximation for simulation of moisture diffusion in wood

• resulting difference between model and experimental results often denoted as “Non-Fick’ian Behavior” difference increases with increasing gradient of moisture content

• more appropriate models require many input parameters, hardly known for most wood types

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• application on music instruments: most surfaces varnished

increase of surface resistance, decrease of moisture gradient

usage of Fick’s Law, when diffusions coefficients determined by steady- state experiments

consideration of changes in ambient atmosphere: boundary conditions of Neumann type

Modeling of Surface Resistance

Modeling of Moisture Transfer

boundary conditions of Neumann type

• qn: moisture flux across the boundary [kg/(mm²s)]

• ρ0: density in absolute dry condition [kg/mm³]

• mecm: equilibrium moisture content [-]

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• ms: moisture content at the surface

• S: surface emissivity coefficient subject to moisture content [mm/s]

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• evaluation of equilibrium moisture content: approach of Avramidis

Modeling of Surface Resistance

Modeling of Moisture Transfer

• surface emissivity coefficient: approach of Hanhijärvi

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• nonlinearity of S(m) is considered within tangent matrix consistent linearization

Avramidis [1989], Hanhijärvi [1997]

coupling of anisotropic mechanics and anisotropic moisture transfer

Coupling of Mechanics and Moisture Diffusion

Hygro-mechanical Coupling

• modeling of influence of moisture content on mechanical properties

• influence of loading state on moisture transport neglectable for small strains

• internal forces of solid-elements: mechanics extended by swelling/shrinkage

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for linear elasticity

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• vector of shrinkage strains (stress-independent)

Coupling of Mechanics and Moisture Diffusion

Hygro-mechanical Coupling

β: shrinkage values [-]

m: nodal moisture content [-]

mref: reference moisture content [-]

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• components of the tangent matrix for linear elastic range

components of compliance tensor subject to moisture content

Moisture-dependent Elastic Properties

Hygro-mechanical Coupling

approximation of experimental results carried out by Neuhaus for spruce

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symmetry of elasticity tensor only partly validated by experimental results interpolation

Neuhaus [1981]

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example: S22(m)

Hygro-mechanical Coupling

Moisture-dependent Elastic Properties

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Neuhaus [1981]

Moisture-dependent Strength Properties

Hygro-mechanical Coupling

first simplifying approach:

• linear dependence of each strength value on moisture content

• strength decreases with increasing moisture content

• approximate values from literature (mostly spruce)

• validity:

• example: compression strength in radial direction

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Gerhards [1982], Kollmann [1982]

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Examples

Elasticity: Shrinkage Deformations

• FE-model

• material: linear elastic anisotropic mechanics and anisotropic moisture

• consideration of cylindrical anisotropy

• steady-state simulation

• loading

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• reduction of moisture content

• realistic simulation of shrinkage deformations

Examples

Plasticity: Model Problem

• FE-model

• element with unit volume and statically determinate support

• loading: 5 load steps

1. compressive load in radial direction (z-direction)

2. reduction of moisture content

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3. mechanical unloading

4. reduction of moisture content

5. compressive re-loading

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Examples

Plasticity: Model Problem

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Examples

Cantilever Beam

• FE-model

• material 1: linear elastic anisotropic mechanics and anisotropic moisture

• material 2: multi-surface plasticity and anisotropic moisture

• steady-state simulation

• loading

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• constant surface loading

• change of ambient atmosphere from T1=10°C, RH1=0.4 to T2=28°C, RH2=0.7

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Examples

Cantilever Beam

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Examples

Cantilever Beam

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Examples

Swelling Beam

• FE-model

• beam, virtually cut out of the middle of a stem

• consideration of cylindrical anisotropy

• material 1: linear elastic anisotropic mechanics and anisotropic moisture

• material 2: multi-surface plasticity and

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anisotropic moisture

• steady-state and transient simulation

Examples

Swelling Beam

• loading

• increase of moisture content from absolutely dry state to equilibrium moisture content 0.237 (corresponding to ambient climate of T=22°C, RH=0.95)

• transient simulation: increase of moisture content during 1 h, afterwards simulation continued for further

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1.000.000 sec (11.57 days)

• study of lower part of beam

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Examples

Swelling Beam

linear elastic

3rd principal stress

ductile

3rd principal stress

ductile

plastified parts3rd principal stress [N/mm²]

3rd principal stress [N/mm²]

plastified parts

time

1 min

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10 min

Examples

Swelling Beam

linear elastic

3rd principal stress

ductile

3rd principal stress

ductile

plastified parts3rd principal stress [N/mm²]

3rd principal stress [N/mm²]

plastified parts

time

30 min

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50 min

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Examples

Swelling Beam

linear elastic

3rd principal stress

ductile

3rd principal stress

ductile

plastified parts3rd principal stress [N/mm²]

3rd principal stress [N/mm²]

plastified parts

time

11,62 days

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steadystate

Outlook

Outlook

• modeling of brittle failure subject to moisture content (fracture mechanics)content (fracture mechanics)

• consideration of time-dependent behavior(viscoelastic and mechano-sorptive creep)

• adaption of the material models to other wood types, used in instrument making

• if necessary, development and realisation of experimental studies to evaluate moisture-

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dependent mechanical properties

• completion, verification and iterative improvement of the FE models of historical pianofortes

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Thank you for your attention.

This project is supported by the KUR-program for the Conservation of Moveable Cultural Assets.

project partners: Händel-Haus Halle

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Clemens Birnbaum (director)Stefan Ehricht (conservator)Achim Haufe (conservator)