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**Viscoelastic Material Analysis**

Nonlinear Analysis: Viscoelastic Material Analysis

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**Section 3 – Nonlinear Analysis**

Module 4 – Viscoelastic Materials Page 2 Objectives The objective of this module is to provide an introduction to the theory and methods used in the analysis of components containing materials described by viscoelastic material models. Topics covered include models based on elastic and viscous mechanical elements; Representation of relaxation data in the form of a Prony series; Instantaneous and long term relaxation moduli; Data required by Autodesk Simulation Multiphysics to perform a viscoelastic analysis; and Results from a Mechanical Event Simulation Analysis with Nonlinear Material Models.

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**Viscoelastic materials exhibit hysteresis, creep, and relaxation.**

Section 3 – Nonlinear Analysis Module 4 – Viscoelastic Materials Page 3 Viscoelasticity Viscoelasticity is concerned with describing elastic materials that exhibit strain rate or time dependent response to applied stress. Viscoelastic materials exhibit hysteresis, creep, and relaxation. Polymers often exhibit viscoelastic properties. Linear Viscoelasticity The relaxation and creep functions are a function only of time. Nonlinear Viscoelasticity The relaxation and creep functions are a function of both time and stress or strain.

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**Time Dependent Responses**

Section 3 – Nonlinear Analysis Module 4 – Viscoelastic Materials Page 4 Time Dependent Responses Polymers respond differently to different types of time dependent loading. Instantaneous elasticity Creep under constant stress Relaxation under constant strain Instantaneous recovery followed by delayed recovery and permanent set W. N. Findley, Lai, J.S., Onaran, K., Creep and Relaxation of Nonlinear Viscoelastic Materials, Dover, 1989, pp.50.

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**Relaxation Curves for a Linear Viscoelastic Material**

Section 3 – Nonlinear Analysis Module 4 – Viscoelastic Materials Page 5 Relaxation Modulus When subjected to a constant strain, the stress in polymers will relax (i.e. stress will decrease to a steady state value). In a linear viscoelastic material the relaxation is proportional to the applied strain. The relaxation modulus is defined as: Relaxation Curves for a Linear Viscoelastic Material 2 times 2 times 2 times 2 times Tension Shear

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**Creep Curves for a Linear Viscoelastic Material**

Section 3 – Nonlinear Analysis Module 4 – Viscoelastic Materials Page 6 Creep Compliance When subjected to constant stress, polymers will creep (i.e. strain will continue to increase to a steady state value). If the creep response is proportional to the applied stress, the material is “linear”. The creep compliance is defined by: Creep Curves for a Linear Viscoelastic Material 2 times 2 times 2 times 2 times

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**The phase angle can be related to the damping of the material.**

Section 3 – Nonlinear Analysis Module 4 – Viscoelastic Materials Page 7 Sinusoidal Response When subjected to a sinusoidally varying stress there will be a phase angle between the stress and strain. This phase angle creates the hysteresis seen in cyclic stress- strain curves. The phase angle can be related to the damping of the material. t

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**Mechanical Element Analogs**

Section 3 – Nonlinear Analysis Module 4 – Viscoelastic Materials Page 8 Mechanical Element Analogs Mechanical elements provide a means to construct potential viscoelastic material models. Elastic Element – Stress is proportional to strain. Viscous Element – Stress is proportional to strain rate. The proportionality constant is called viscosity due to its similarity to a Newtonian fluid.

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**The Maxwell model uses a spring and dashpot in series.**

Section 3 – Nonlinear Analysis Module 4 – Viscoelastic Materials Page 9 Maxwell Model The Maxwell model uses a spring and dashpot in series. The Maxwell model doesn’t match creep response well. It predicts a linear change in stress versus time for the creep response. Derivation of Governing Equation Combining yields Units are seconds

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**The Kelvin model uses a spring and dashpot in parallel.**

Section 3 – Nonlinear Analysis Module 4 – Viscoelastic Materials Page 10 Kelvin Model The Kelvin model uses a spring and dashpot in parallel. The Kelvin model doesn’t match relaxation data. It doesn’t exhibit time dependent relaxation. Derivation of Governing Equation

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**Standard Linear Solid – Governing Equations**

Section 3 – Nonlinear Analysis Module 4 – Viscoelastic Materials Page 11 Standard Linear Solid – Governing Equations The Standard Linear Solid model is a three-parameter model that contains a Maxwell Arm in parallel with an elastic arm. Laplace transforms will be used to develop relaxation and creep constitutive equations. Derivation of Governing Equation Elastic Arm Maxwell Arm Characteristic Time

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**Standard Linear Solid – Laplace Domain**

Section 3 – Nonlinear Analysis Module 4 – Viscoelastic Materials Page 12 It is easier to determine the governing equation in the Laplace domain than in the time domain. Laplace Domain Time Domain The overscore indicates the Laplace transform of the variable. Elastic Arm Maxwell Arm Governing Equation in Laplace Domain

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**Standard Linear Solid – Relaxation Equations**

Section 3 – Nonlinear Analysis Module 4 – Viscoelastic Materials Page 13 Standard Linear Solid – Relaxation Equations The relaxation behavior is obtained by finding the response to a step change in strain. At time t=0, there is an instantaneous stress response equal to At infinite time the stress relaxes to a steady state value of Unit Step Function Substitution into the governing equation yields Taking the inverse Laplace transform yields

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**Standard Linear Solid – Relaxation Plot**

Section 3 – Nonlinear Analysis Module 4 – Viscoelastic Materials Page 14 Standard Linear Solid – Relaxation Plot The relaxation modulus, E(t), is shown in the figure. The values chosen for the parameters Er, Em, and t are for demonstration purposes only. The stress relaxes to a steady state value controlled by the parameter Er.

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**Standard Linear Solid – Creep Equations**

Section 3 – Nonlinear Analysis Module 4 – Viscoelastic Materials Page 15 Standard Linear Solid – Creep Equations The creep behavior is obtained by finding the response to a step change in stress. At time t=0, there is an instantaneous stress response equal to At infinite time the strain grows to a steady state value of Substitution into the governing equation yields Taking the inverse Laplace transform yields

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**Standard Linear Solid – Creep Plot**

Section 3 – Nonlinear Analysis Module 4 – Viscoelastic Materials Page 16 Standard Linear Solid – Creep Plot The creep compliance modulus, J(t), is shown in the figure. The values chosen for the parameters Er, Em, and t are for demonstration purposes only. The strain creeps to a steady state value controlled by the parameter Cr. Since Cg is greater than Cr the characteristic creep time is slower than that for relaxation.

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**Standard Linear Solid - Summary**

Section 3 – Nonlinear Analysis Module 4 – Viscoelastic Materials Page 17 Standard Linear Solid - Summary The Standard Linear Solid more accurately represents the response of real materials than does the Maxwell or Kelvin models. Instantaneous elastic strain when stress applied; Under constant stress, strain creeps towards a limit; Under constant strain, stress relaxes towards a limit; When stress is removed, instantaneous elastic recovery, followed by gradual recovery to zero strain; Two time constants One for relaxation under constant strain One for creep/recovery under constant stress (Relaxation is quicker than creep)

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**Section 3 – Nonlinear Analysis**

Module 4 – Viscoelastic Materials Page 18 Wiechert Model The Wiechert model is a generalization of the Standard Linear Solid model and can be used to model the viscoelastic response of many materials. It consists of a linear spring in parallel with a series of springs and dashpots (Maxwell elements). The shear relaxation modulus is used from this point forward since Simulation expects data for the shear relaxation modulus to be entered. Relaxation Modulus Relaxation Time

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**is the value of G(t) at time equal to zero.**

Section 3 – Nonlinear Analysis Module 4 – Viscoelastic Materials Page 19 is the value of G(t) at time equal to zero. It is the instantaneous shear modulus. is the value of G(t) at time equal to infinity. It is the final or fully relaxed shear modulus. Relaxation function versus time

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**Weichert Model – Multiple Relaxation Times**

Section 3 – Nonlinear Analysis Module 4 – Viscoelastic Materials Page 20 Weichert Model – Multiple Relaxation Times The Wiechert model can accurately model the response characteristics of real materials because it can include as many relaxation times and corresponding moduli as needed. In the figure, five Maxwell elements are used to fit the experimental data. Each Maxwell element has a relaxation modulus and corresponding relaxation time constant. Example Relaxation Data for a Real Material t1 t2 t3 t4 tn

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**Section 3 – Nonlinear Analysis**

Module 4 – Viscoelastic Materials Page 21 Prony Series The challenge in describing a material by the Weichert model is to find the coefficients, Gi and relaxation times, ti, of the Prony Series. Specialized optimization algorithms are used to determine the best set of moduli, Gi, and relaxation times, ti , that match experimental data. Prony Series

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**Section 3 – Nonlinear Analysis**

Module 4 – Viscoelastic Materials Page 22 Alternate Forms This form of the equation is used when the relaxation properties are specified in terms of the long term modulus, This form of the equation is used when the relaxation properties are specified in terms of the instantaneous modulus, G0.

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**Autodesk Simulation Multiphysics Material Data Screen**

Section 3 – Nonlinear Analysis Module 4 – Viscoelastic Materials Page 23 Autodesk Simulation Multiphysics Material Data Screen The instantaneous form of the relaxation modulus equation is used. (Mooney-Rivlin) Defines the instantaneous shear modulus First Constant Second Constant

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**Volumetric Relaxation Data**

Section 3 – Nonlinear Analysis Module 4 – Viscoelastic Materials Page 24 Volumetric Relaxation Data Unless the “Independent Volumetric/Deviatoric Relaxation” box is checked, the relaxation data will be applied to both the deviatoric (shear) and volumetric material properties. Many polymers are nearly incompressible and remain so (i.e. no relaxation of the volumetric properties). Zeros have been added for the volumetric Prony series data.

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**Example - Sandwich Problem**

Section 3 – Nonlinear Analysis Module 4 – Viscoelastic Materials Page 25 Example - Sandwich Problem Elastomeric adhesives are commonly used as vibration dampers. The hysteresis associated with elastomers provides natural damping. A sandwich type construction where the elastomer is placed between two stiff materials is shown in the figure. Locating the elastomer in the middle exposes it to the highest shear stresses. Section of Sandwich Beam 6061-T6 Aluminum 1/16 in 1/32 in 1/16 in 6061-T6 Aluminum ISR Industrial Adhesive

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**The beam is modeled using a 2D plane strain representation.**

Section 3 – Nonlinear Analysis Module 4 – Viscoelastic Materials Page 26 Example – 2D Model The beam is modeled using a 2D plane strain representation. A 3D representation would require elements in the thickness direction. The plane strain representation is acceptable since there will be little stress variation through the thickness direction. Thickness Direction

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**Example – Beam Geometry**

Section 3 – Nonlinear Analysis Module 4 – Viscoelastic Materials Page 27 Example – Beam Geometry The dynamic response of the cantilevered sandwich beam will be computed. The beam is ½ inch wide and 12 inches long. The top and bottom plates are made from 1/16 inch thick T6 aluminum. The adhesive layer (shown in blue) is 1/32 inch thick. Portion of the Inventor model of the sandwich beam.

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**Loads and Boundary Conditions**

Section 3 – Nonlinear Analysis Module 4 – Viscoelastic Materials Page 28 Loads and Boundary Conditions The displacements at one end of the beam are fixed to simulate a clamped condition. The other end is exposed to a step force of 1 lbs. Displacement Constraints 1 lb divided among 21 nodes

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**Section 3 – Nonlinear Analysis**

Module 4 – Viscoelastic Materials Page 29 FEA Model A nonlinear dynamic analysis will be performed using the MES with Nonlinear Material Models analysis type. The 2D elements will allow the analysis to run much quicker than if 3D elements were used. Section of Sandwich Beam 6061-T6 Aluminum 1/16 in 1/32 in 1/16 in 6061-T6 Aluminum Simson Industrial Adhesive Mesh absolute element size is 1/64th of an inch.

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**Element Definition: Adhesive**

Section 3 – Nonlinear Analysis Module 4 – Viscoelastic Materials Page 30 Element Definition: Adhesive A viscoelastic Mooney-Rivlin Material is selected. This will give a nonlinear stress- strain relationship with a linear viscoelastic response. The plane strain option is selected. The mid-side nodes option is selected. By default, this is a large displacement analysis.

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**Example – Material Properties**

Section 3 – Nonlinear Analysis Module 4 – Viscoelastic Materials Page 31 Example – Material Properties Tension relaxation properties for ISR adhesive are given in the referenced document. Mpa Sec. Reference Garcia-Barruetabena, J., et al, Experimental Characterization and Modelization of the Relaxation and Complex Moduli of a Flexible Adhesive, Materials and Design, 32 (2011)

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**Example - Shear Relaxation Properties**

Section 3 – Nonlinear Analysis Module 4 – Viscoelastic Materials Page 32 Example - Shear Relaxation Properties The relaxation properties given on the previous slide are for tension. Simulation expects shear relaxation properties. Poisson’s ratio for an incompressible material is 0.5. The shear relaxation data is obtained by dividing the tension data by three. Shear Relaxation Data Mpa Sec.

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**Example - Instantaneous Form**

Section 3 – Nonlinear Analysis Module 4 – Viscoelastic Materials Page 33 Example - Instantaneous Form The shear relaxation data will be entered into the Simulation Prony series table using the instantaneous option. Instantaneous Shear Modulus Relaxation Data Sec.

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**Example - Mooney-Rivlin Properties**

Section 3 – Nonlinear Analysis Module 4 – Viscoelastic Materials Page 34 Example - Mooney-Rivlin Properties The adhesive will be modeled using a hyperelastic material model in conjunction with linear viscoelasticity. The Mooney-Rivlin hyperelastic material model will be used. These constants are normally obtained from the slope and y- intercept of a Mooney curve. As an approximation, the ratio of C10/C01 will be set equal to 4. These two equations lead to constants of C10 = psi and C01 = 99.1 psi.

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**The bulk modulus will be approximated from the equation**

Section 3 – Nonlinear Analysis Module 4 – Viscoelastic Materials Page 35 Example - Bulk Modulus The bulk modulus will be approximated from the equation For an incompressible material n=0.5, and the bulk modulus is infinite. A Poisson’s ratio of will be assumed, which results in a bulk modulus of approximately 496,000 psi.

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**Example - Prony Series Data**

Section 3 – Nonlinear Analysis Module 4 – Viscoelastic Materials Page 36 Example - Prony Series Data The alpha constants and relaxation times are entered in the Prony series table for the Deviatoric Relaxation data. Note the alpha constants are non- dimensional since they have been normalized by the instantaneous shear modulus, G0. Assuming that there is no relaxation of the bulk modulus, the volumetric relaxation data will be set to zeros.

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**Section 3 – Nonlinear Analysis**

Module 4 – Viscoelastic Materials Page 37 Analysis Parameters The response will be computed for 1 second (Event Duration). The response will be captured at 500 time points. This gives an initial time step of seconds. Autodesk Simulation Multiphysics will automatically adjust the time step as needed. The multiplier in the Load Curve table is set to 1 at the beginning and end of the event. This will result in the loads being applied as a step input.

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**Computed displacement history at the tip of the cantilever.**

Section 3 – Nonlinear Analysis Module 4 – Viscoelastic Materials Page 38 Example - Results The plot shows the computed displacement history for the tip of the cantilever. The peak displacement is approximately twice the steady state response which is consistent with the step response of a linear system. The effect of the damping in the adhesive layer is very evident. Computed displacement history at the tip of the cantilever.

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**Section 3 – Nonlinear Analysis**

Module 4 – Viscoelastic Materials Page 39 Module Summary An introduction to viscoelastic materials has been provided to help explain the parameters and information required by Autodesk Simulation Multiphysics software. Shear relaxation data is needed to define the deviatoric material properties. Volumetric relaxation data can also be entered and used during the analysis. Autodesk Simulation Multiphysics software provides the ability to couple nonlinear hyperelastic material models with linear viscoelastic models. Although the material is defined in terms of relaxation data, the creep and dynamic response can also be computed.

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Copyright © 2011, Elsevier Inc. All rights reserved. Chapter 6 Author: Julia Richards and R. Scott Hawley.

Copyright © 2011, Elsevier Inc. All rights reserved. Chapter 6 Author: Julia Richards and R. Scott Hawley.

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