Measured Biaxial Residual Stress Maps in a Stainless Steel Weld
- Univ. of California, Davis, CA (United States). Dept. of Mechanical and Aerospace Engineering
- Australian Nuclear Science and Technology Organisation (ANSTO), Kirrawee-Sydney, NSW (Australia). Inst. of Materials Engineering
- Los Alamos National Lab. (LANL), Los Alamos, NM (United States)
Here, this paper describes a sequence of residual stress measurements made to determine a two-dimensional map of biaxial residual stress in a stainless steel weld. A long stainless steel (316L) plate with an eight-pass groove weld (308L filler) was used. The biaxial stress measurements follow a recently developed approach, comprising a combination of contour method and slitting measurements, with a computation to determine the effects of out-of-plane stress on a thin slice. The measured longitudinal stress is highly tensile in the weld- and heat-affected zone, with a maximum around 450 MPa, and compressive stress toward the transverse edges around ₋250 MPa. The total transverse stress has a banded profile in the weld with highly tensile stress at the bottom of the plate (y = 0) of 400 MPa, rapidly changing to compressive stress (at y = 5 mm) of ₋200 MPa, then tensile stress at the weld root (y = 17 mm) and in the weld around 200 MPa, followed by compressive stress at the top of the weld at around ₋150 MPa. Finally, the results of the biaxial map compare well with the results of neutron diffraction measurements and output from a computational weld simulation.
- Research Organization:
- Los Alamos National Lab. (LANL), Los Alamos, NM (United States)
- Sponsoring Organization:
- USDOE
- Grant/Contract Number:
- AC52-06NA25396
- OSTI ID:
- 1329566
- Report Number(s):
- LA-UR-15--21095
- Journal Information:
- Journal of Nuclear Engineering and Radiation Science, Journal Name: Journal of Nuclear Engineering and Radiation Science Journal Issue: 4 Vol. 1; ISSN 2332-8983
- Publisher:
- ASMECopyright Statement
- Country of Publication:
- United States
- Language:
- English
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