A comparative assessment of cyclic deformation behaviour in SA333 Gr.6 steel using solid, hollow specimens under axial and shear strain paths
Introduction
Conventionally, low cycle fatigue (LCF) behaviour of metallic materials is studied under uniaxial loading conditions using solid specimens. Such experiments are sufficient to gather the basic information on the cyclic deformation behaviour of materials. However, the actual in-service conditions in many engineering materials involve complex loading schemes and often data from a simple uniaxial experiment is inadequate to understand cyclic deformation behaviour under such situations. More attention has therefore been laid of late to study the cyclic deformation behaviour of materials under complex loading situations such as thermo mechanical fatigue or multiaxial fatigue using thin walled hollow specimens. One of the main focus here is the extension of the basic understanding on uniaxial fatigue to more complex situations through a parametric development of a damage parameter that relates the uniaxial and multiaxial situations. One argument put forth by Fash et al. [1] in this regard is that an appropriate establishment be obtained to prove that the data and damage behaviour using a smooth uniaxial specimen represents that of a thin wall tubular specimen. It thus calls for a comparative assessment of cyclic deformation behaviour in solid and hollow specimens. This paper is aimed to share some of our recent experimental observations on this issue.
Unfortunately, barring a few, not many investigations are available on this issue. Research by Fash et al. [1] and few others [2], [3] have shown that even after considering the influence of all multiaxiality factors, the fatigue lives in solid and hollow specimens are not the same. It has been reasoned that the difference basically arises due to the variations in the stress/strain gradients brought forth by the specimen geometry. In another investigation [4] on low cycle fatigue using tubular specimens of varying wall thickness, it has been noticed that fatigue lives decreased with decreasing wall thickness and in general, fatigue lives in solid specimens were higher when compared to the results from hollow specimens under identical experimental conditions. Evidences for a shorter fatigue life in hollow specimens than their companion solid geometry is also available in [2]. Through simulation experiments Shatil et al. [2] have shown that the difference in lives is connected to the manner in which the radial stress/strain gradient varies from surface to mid section in the two geometries. Recently, Keun and Soon Bok [5] have also observed a similar variation in the fatigue lives of tubular and solid specimens. Their experimental and simulation results show that the ratio of the internal plastic strain between hollow and solid specimens were consistently higher than unity indicating that the internal plastic strain energy density in hollow specimens is more and thus explaining the shorter live in these geometries.
All these investigations clearly bring out the fact that the fatigue lives in solid and hollow specimen geometries need not be essentially the same. While these investigations provide sufficient evidence for the same, no major attempt has been made so far to understand the influence that this geometry effect can have on the cyclic deformation process itself. It is this aspect that we are reporting here. In this work, we provide a comparative assessment of the cyclic deformation behaviour in a carbon–manganese steel using solid and thin walled tubular specimens in axial strain path. Additionally, we also compare the influence of axial and shear strain paths on the cyclic deformation process using tubular specimens.
The process of cyclic deformation can be best represented by the analyses of the stress–strain hysteresis loops. We have adopted this technique to understand the influence of specimen geometry and/or strain path on cyclic deformation process such as hardening/softening behaviour, Masing/non-Masing behaviour, alterations in the proportional limit. We also employ a probability density function (PDF) based analyses of the branches of the hysteresis loops to understand the local alterations in cyclic deformation. The overall objective is to provide a fundamental understanding of changes in cyclic plastic phenomena due to specimen geometry and/or strain path. The work is aimed at providing a knowledge base on this issue and will be helpful for further evaluation of various plasticity models.
Section snippets
Experimental
The material used in this investigation is SA333 Gr.6 C–Mn steel. The material was available in the form of pipe with about 500 mm outer diameter and 50 mm wall thickness. The nominal composition of the SA333 steel is given in Table 1. Table 2 lists the mechanical properties of the material obtained from tensile tests at room temperature. The tensile flow curve of the steel exhibited prominent yield-point effect accompanied by non-hardening strain propagation (Lüders strain) of ∼2%.
Being a C–Mn
Fatigue life and hardening/softening behaviour in solid, hollow specimens
Prior to understanding the variations in cyclic deformation, if any, induced by the specimen geometry, the macroscopic data such as the fatigue life obtained on both the specimens employing both axial and shear strain paths has been examined. The intention of comparing the shear strain results here is not to investigate the specimen geometry effect, but to understand the manner in which the two strain paths can influence the cyclic deformation behaviour and the resultant fatigue life. Fig. 3
Conclusions
In this investigation a comparative assessment of cyclic plastic behaviour of SA333 Gr.6 C–Mn steel has been made using solid and hollow specimens under axial and/or shear strain cycling. The stress–strain hysteresis loops were analysed to understand the cyclic deformation behaviour in solid and hollow specimens. Observation of experimental results lead to the following conclusions:
The fatigue life in hollow-axial tests were marginally lower than that of its companion solid specimens. The
Acknowledgement
The authors would like to acknowledge Bhabha Atomic Research Center, Mumbai for supply of material and financial support.
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