TY - JOUR
T1 - Experimental and theoretical analysis of the response for 316L stainless steel tubes under pure bending creep and relaxation
AU - Lee, Kuo Long
AU - Pan, Wen-Fung
PY - 2015/1/1
Y1 - 2015/1/1
N2 - In this study, the response sharp-notched 316L stainless steel tubes subjected to pure bending creep and relaxation is experimentally and theoretically studied. Pure bending creep means to bend the specimen to a desired moment and hold that moment for a period of time; pure bending relaxation means to bend the specimen to a desired curvature and hold that curvature for a period of time. From the experimental result for pure bending creep, the curvature and ovalization increase with time until the tube buckles. A higher desired moment leads to higher curvature and ovalization. From the experimental result for pure bending relaxation, the bending moment rapidly decreases with time and becomes a steady value after all. As for the ovalization, the amount increases with time and gradually becomes a steady value. Due to the constant ovalization caused by the constant curvature under pure bending relaxation, the tube does not buckle. Finally, the formulation proposed Lee and Pan [1] is modified for simulating the initial and second stages of the creep curvature-time relationship under pure bending creep, and relaxation moment-time relationship under pure bending relaxation for sharp-notched 316L stainless steel tubes. Through comparing with the experimental finding, the theoretical analysis can reasonably describe the experimental result.
AB - In this study, the response sharp-notched 316L stainless steel tubes subjected to pure bending creep and relaxation is experimentally and theoretically studied. Pure bending creep means to bend the specimen to a desired moment and hold that moment for a period of time; pure bending relaxation means to bend the specimen to a desired curvature and hold that curvature for a period of time. From the experimental result for pure bending creep, the curvature and ovalization increase with time until the tube buckles. A higher desired moment leads to higher curvature and ovalization. From the experimental result for pure bending relaxation, the bending moment rapidly decreases with time and becomes a steady value after all. As for the ovalization, the amount increases with time and gradually becomes a steady value. Due to the constant ovalization caused by the constant curvature under pure bending relaxation, the tube does not buckle. Finally, the formulation proposed Lee and Pan [1] is modified for simulating the initial and second stages of the creep curvature-time relationship under pure bending creep, and relaxation moment-time relationship under pure bending relaxation for sharp-notched 316L stainless steel tubes. Through comparing with the experimental finding, the theoretical analysis can reasonably describe the experimental result.
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M3 - Article
AN - SCOPUS:84949804471
VL - 30
SP - 163
EP - 170
JO - Journal of Technology
JF - Journal of Technology
SN - 1012-3407
IS - 3
ER -