Abstract

This study develops a unified phenomenological creep model for polymer-bonded composite materials, allowing for predicting the creep behavior in the three creep stages, namely the primary, the secondary, and the tertiary stages under sustained compressive stresses. Creep testing is performed using material specimens under several conditions with a temperature range of 20 °C–50 °C and a compressive stress range of 15 MPa–25 MPa. The testing data reveal that the strain rate–time response exhibits the transient, steady, and unstable stages under each of the testing conditions. A rational function-based creep rate equation is proposed to describe the full creep behavior under each of the testing conditions. By further correlating the resulting model parameters with temperature and stress and developing a Larson–Miller parameter-based rupture time prediction model, a unified phenomenological model is established. An independent validation dataset and third-party testing data are used to verify the effectiveness and accuracy of the proposed model. The performance of the proposed model is compared with that of an existing reference model. The verification and comparison results show that the model can describe all the three stages of the creep process, and the proposed model outperforms the reference model by yielding 28.5% smaller root mean squared errors on average.

Highlights

  • Creep is a time-dependent progressive inelastic deformation behavior

  • The purpose of this study is to develop a unified phenomenological creep model for polymer-bonded composite materials, allowing for prediction of the creep behavior and life under more general conditions without testing data

  • A unified phenomenological creep model was developed for polymer-bonded composite materials, allowing for predicting the creep behavior in the entire primary, secondary, and tertiary stages

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Summary

Introduction

Creep is a time-dependent progressive inelastic deformation behavior. It can cause the relaxation of stress and irreversible deformation, leading to functional failures when the part is intended to maintain the required stress and shape [1]. The secondary (stationary) creep is considered to be the dominant creep for many applications In this stage, the equilibrium between the softening and hardening of the material is assumed, leading to a stable strain rate [24,25,26]. Prior to the stationary stage, a short transient period of primary creep is required to reach such an approximate equilibrium between the softening and hardening processes. The final part of the creep process is the tertiary stage where the strain rate increases rapidly until rupture [27,28]

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