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The peridynamic model of viscoelastic creep and recovery

Muhammad Azim bin Azizi (Department of Mechanical and Material Engineering, Universiti Kebangsaan Malaysia, Bangi, Malaysia)
Ahmad Kamal Ariffin bin Mohd Ihsan (Department of Mechanical and Material Engineering, Universiti Kebangsaan Malaysia, Bangi, Malaysia)
Nik Abdullah bin Nik Mohamed (Faculty of Mechanical Engineering, Universiti Malaysia Pahang, Gambang, Malaysia)

Multidiscipline Modeling in Materials and Structures

ISSN: 1573-6105

Article publication date: 9 November 2015

425

Abstract

Purpose

The purpose of this paper is to establish a peridynamic method in predicting viscoelastic creep behaviour with recovery stage and to find the suitable numerical parameters of peridynamic method.

Design/methodology/approach

A rheological viscoelastic creep constitutive equation including recovery and an elastic peridynamic equation (with integral basis) are examined and used. The elasticity equation within the peridynamic equation is replaced by the viscoelastic equation. A new peridynamic method with two time parameters, i.e. numerical time and viscoelastic real time is designed. The two parameters of peridynamic method, horizon radius and number of nodes per unit volume are studied to get their optimal values. In validating this peridynamic method, comparisons are made between numerical and analytical result and between numerical and experimental data.

Findings

The new peridynamic method for viscoelastic creep behaviour is approved by the good matching in numerical-analytical data comparison with difference of < 0.1 per cent and in numerical-experimental data comparison with difference of 4-6 per cent. It can be used for further creep test which may include non-linear viscoelastic behaviour and creep rupture. From this paper, the variation of constants in Burger’s viscoelastic model is also studied and groups of constants values that can simulate solid, fluid and solid-fluid viscoelastic behaviours were obtained. In addition, the numerical peridynamic parameters were also manipulated and examined to achieve the optimal values of the parameters.

Research limitations/implications

The peridynamic model of viscoelastic creep behaviour preferably should have only one time parameter. This can only be done by solving the unstable fluctuation of dynamic results, which is not discussed in this paper. Another limitation is the tertiary region and creep rupture are not included in this paper.

Practical implications

The viscoelastic peridynamic model in this paper can serve as an alternative for conventional numerical simulations in viscoelastic area. This model also is the initial step of developing peridynamic model of viscoelastic creep rupture properties (crack initiation, crack propagation, crack branching, etc.), where this future model has high potential in predicting failure behaviours of any components, tools or structures, and hence increase safety and reduce loss.

Originality/value

The application of viscoelastic creep constitutive model on peridynamic formulation, effect of peridynamic parameters manipulation on numerical result, and optimization of constants of viscoelastic model in simulating three types of viscoelastic creep behaviours.

Keywords

Acknowledgements

Financial support for this study was provided by a grant from the Ministry of Higher Education (MOHE), University Putra Malaysia and University Kebangsaan Malaysia. The authors wish to thank Professor Ahmad Kamal Ariffin Mohd Ihsan and Professor Nik Abdullah Nik Mohamed for their guidance and suggestions in this work. Thanks are also due to dear colleagues Reza, Salvinder and Dr Elwaled for their help on preparing the manuscript.

Citation

bin Azizi, M.A., bin Mohd Ihsan, A.K.A. and bin Nik Mohamed, N.A. (2015), "The peridynamic model of viscoelastic creep and recovery", Multidiscipline Modeling in Materials and Structures, Vol. 11 No. 4, pp. 579-597. https://doi.org/10.1108/MMMS-03-2015-0017

Publisher

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Emerald Group Publishing Limited

Copyright © 2015, Emerald Group Publishing Limited

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