Non-Destructive Testing TechniquesMagnetic Properties and ApplicationsHydrogen embrittlement and corrosion behaviors in metals

Jiawen Zhang, Chisen Qin, Nan Liu, Zheng Lian, Guang-Kai Sun, Bin Liu, Lijian Yang

2026.3.5Magnetochemistry

DOI: 10.3390/magnetochemistry12030034

Abstract

A hard spot defect refers to structural defects that occur in long-distance oil and gas pipelines during the thermal processes. These defects arise from the combination of material phase changes and stress concentration, making them challenging to detect. Weak magnetic detection technology is an effective approach for identifying microscopic phase transformations and stress concentrations in materials. This study develops an ontological model linking hardness, stress, and magnetic signals at hard spots, and both simulations and real experiments are conducted to validate the model. The findings indicate a strong correlation between the model and experimental observations. The research also examined how hardness and defect shape influence magnetic signals and revealed that both the tangential and normal components of the weak magnetic signal at hard spots increase with higher hardness levels. Additionally, the peak value of the defect rises with an increasing depth-to-width ratio, and the difference between the center and peak values grows. According to the linear variation in the current constitutive model, the magnetic signal amplitude increases by approximately 35% for every 0.8% rise in hardness, with growth rates of 0.23% and 0.26% for the amplitude at the center and peak endpoint of the tangential magnetic signal, respectively. The hard spot shape parameter, Hd, is derived from the spacing of the tangential and normal peak-to-peak values, which indicates the size of the hard spot and increases consistently with the depth-to-radius ratio.

Citation format

ZHANG, Jiawen, et al. Characterization of weak magnetic internal detection signals of hard spot defects in long-distance oil and gas pipelines. Magnetochemistry, 2026, 12(3): 34.