Journal of the Society of Materials Science, Japan
Online ISSN : 1880-7488
Print ISSN : 0514-5163
ISSN-L : 0514-5163
On the Stress-Relaxation Properties of TAF Steel
Ryoichi SASAKITetsumori SHINODA
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1967 Volume 16 Issue 162 Pages 150-155

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Abstract

Despite the extensive studies on the stress-relaxation properties of heat resisting steels, there are several questions left unanswered, in which, for example, the subjects on the extrapolation of stressrelaxation data and effect of re-loading on the stress relaxation properties are included.
The authors have taken interest in these subjects and have been carrying out the stress-relaxation tests on TAF which is 12% chromium heat resisting steel.
Tests were made with the specimens of a 10mm guage dia. and 100mm gauge length by using the automatic type stress-relaxation testing machines of 4 tons capacity, and were processed by the following methods: (1) Applying the same initial stress of 30kg/mm2 at the temperature range of 550°∼650°C (this test procedure was termed as“initial-loading 1st”); (2) The specimens subjected to the foregoing procedure being re-loaded to the same initial stress of 30kg/mm2 at the same temperature range (termed as“re-loading”); and (3) On the other hand, to another group of specimens applying the initial strain equal to the residual plastic strain left in the“initial-loading 1st”plus initial strain in the “re-loading”(termed as“initial-loading 2nd”).
The results obtained are as follows;
(1) As far as the present tests are concerned, the predicted value of“re-loading”stress-relaxation properties assessed from the data of“initial-loading 2nd”based on the well-known Strain-Hardening Theory deviates significantly from the actual“re-loading”value.
On the other hand, the predicted value calculated from Time-Hardening Theory by using suitable material constants is in comparatively good agreement with the actual one within the range of observed duration.
(2) The equation which correlate plastic strain rate εp calculated from“initial-loading”stress-relaxation data for TAF steel, residual stress (kg/mm2), and test temperature T (°K), within the temperature range of 800°∼900°K and the stress range of 24∼14kg/mm2, takes the form;
εp≈A exp(ασ)exp(-Q'/RT)
where
Q'={124(kcal/mole)……σc
267-7σ(kg/mole)……σc
where A and α are material constants which are determined separately according to the two stages definend by stress level (corresponding to the two straight portions in log εp-log σ curves), and σc is the critical value of about 21(kg/mm2).
(3) All the initial loading stress-relaxation data obtained at various test temperatures on TAF steel have been successfully expressed on a single master relaxation curve within the limit range of stress and temperature by using the parameter P (=log Et-Q4.6 T, where E is Young's modulus depending on temperature, t is time, T is absolute temperature, and Q is material constant). This relationship could be also available successfully to other alloys.

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