Elsevier

Materials Letters

Volume 63, Issue 11, 30 April 2009, Pages 877-880
Materials Letters

A hyper-viscoelastic constitutive model for polyurea

https://doi.org/10.1016/j.matlet.2009.01.055Get rights and content

Abstract

This letter presents a new constitutive model for polyurea by superposing the hyperelastic and viscoelastic behaviors of polyurea. The Ogden model is used for the hyperelastic part and its parameters are determined from curve fitting of quasi-static test data. A nonlinear viscoelastic model is employed for describing the viscoelastic behavior and its relaxation time is obtained based on the test data of shear relaxation modulus. A special form of Zapas kernel for the damping function is found to be very effective to capture the viscoelastic behavior of polyurea subjected to wide ranges of strain rate. Both the versatility and accuracy of the model are examined via virtual testing.

Introduction

Polyurea is a product from the chemical reaction between an isocyanate and an amine. It has been widely used in the coating industry, because of its extensive benefits over existing epoxy adhesives and rubber linings in terms of impact, abrasion and corrosion resistance. With the development of polyurea spray coatings technology, specifically formulated polyurea can be directly and efficiently sprayed on the surface of structural components to enhance the mechanical strength and durability of civil and military structures.

Previous experimental studies [1] have revealed that polyurea exhibits elastic and nearly incompressible behavior to volumetric deformations and its stress–strain behavior depends on strain rate, temperature and pressure [2], [3]. Different from the rubbery behavior under low strain rates, polyurea displays a distinct leathery behavior [4] at high strain rates. Polyurea can be used in a wide range of temperature (from − 50 °C to 150 °C) and has shown a high heat resistance. However, its shear modulus decreases significantly with increasing temperature. The glass transition temperature Tg for polyurea is roughly − 50 °C [1]. Given the stiffening behavior of polyurea material with both increasing strain and strain rate, it has been used either as a protection coating on a metallic structure or an inserted layer between the outer facesheet and the foam core in a blast-tolerant sandwich structure.

Both material certification and performance evaluation of polyurea coated structural components under hostile environment by tests will be prohibitively expensive and time consuming. Development of a high fidelity constitutive model of polyurea is imperative to perform an optimal design of its coated components subjected to a combined dynamic and thermal loading. Currently, there are only two models have been developed specifically for polyurea although some similar models have been proposed for other hyperelastic or viscoelastic materials [5], [6]. One is an experimentally-based linear viscoelastic constitutive model proposed by Amirkhizi et al. [2]. It incorporates the classical Williams–Landel–Ferry (WLF) time-temperature transformation and pressure sensitivity, in addition to a thermodynamic energy dissipation mechanism. The model can reproduce experimental results for confined polyurea tests but has limited capability in simulating the unconfined test data. The other is a more complex model proposed by Elsayed [7] which consists of an elastoplastic network acting in parallel with several viscoelastic networks. Quasi-incompressible Ogden-type potentials were used and the number of model parameters is a function of the number of active Ogden terms and relaxation mechanisms, thus a procedure based on genetic algorithms was employed to calibrate model parameters based on existing experimental data. Although this model is relatively successful in reproducing experimental data, it seems to be too complicated for engineering practice.

A constitutive model for polyurea should cover a wide range of strain rates from static to high speed impact and capture both hyperelastic and viscoelastic material behavior. A rational approach based on a combination of hyperelasticity theory and viscoelasticity theory is needed in deriving the constitutive model. Also, for its practical applications, the model should be comparatively simple to be implemented in a general purpose finite element code while its parameters can be determined experimentally from the standard tests. To meet the model requirements, this letter presents a new hyper-viscoelastic constitutive model for polyurea.

Section snippets

Hyperelastic model for low strain rates

Given the compliant rubber-like behavior of polyurea from quasi-static tests, a hyperelastic constitutive model is selected to characterize its rubbery stress–strain behavior at low strain rates. The constitutive law for an isotropic hyperelastic material is decomposed into volumetric and deviatoric parts. The deviatoric part is defined by an equation relating the strain energy density of the material to the three invariants of the strain tensor. By assuming the incompressible behavior of the

Nonlinear viscoelastic model for high strain rates

Having established the rate-independent hyperelastic model for polyurea under static loading conditions, we are now focusing on the rate-dependent characteristic of polyurea. A viscoelastic constitutive law is a good choice for capturing its rate-dependent behavior. For viscoelastic materials, the stress state depends on the strain and strain rate histories. Here, we assume the material is isotropic and subjected to small strains under an isothermal condition. But different from a linear

Results and discussions

In this study, the data for the unconfined uniaxial compression test at strain rate of 2250 s 1 from Sarva et al. [4] is used to determine the parameters A1 and A2. The parameters determined from the fitting are A1 = 0.1435 and A2 = 0.1098. Fig. 3 displays the comparison between the test data and our prediction from the present model. The symbols triangle, square, pentagon, hexagon and circle represent, respectively, the test data under the strain rate 0.0016/s, 80/s, 800/s, 2250/s and 6500/s. The

Conclusions

This letter presents a new constitutive model for polyurea by including both its hyperelastic and viscoelastic behavior. The Ogden model is used for the hyperelastic part and its parameters are curve fitted using the quasi-static test data. A nonlinear viscoelastic model is proposed to characterize its viscoelastic part and the relaxation time is determined based on the test data of the shear relaxation modulus. A special form of Zapas kernel for the damping function is found to be very

Acknowledgement

This work is supported by the Office of Naval Research under Contract N00014-08-C-0614 with Dr. Roshdy Barsoum as the Program Manager.

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