Steel wire
AssigneeSumitomo Electric Industries, Ltd.
InventorsKei Hirai, Tetsuya Nakajima, Akifumi Matsuoka, Takumi Akada
Life of this patent
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Abstract
A steel wire is composed of a steel containing not less than 1.0 mass % and not more than 1.1 mass % C, not less than 0.15 mass % and not more than 0.25 mass % Si, not less than 0.25 mass % and not more than 0.35 mass % Mn, and not less than 0.15 mass % and not more than 0.25 mass % Cr, with the balance being Fe and unavoidable impurities. The steel wire has a wire diameter of not less than 0.15 mm and not more than 0.42 mm. The steel has a pearlite structure. The steel has a dislocation density of not less than 2.4×1016 m−2 and not more than 5.0×1016 m−2. The steel has a full width at half maximum in a circumferential direction of not less than 42° at a peak of a maximum intensity of a Debye ring for Fe (211) plane.
Claims10
A steel wire composed of a steel containing:
- not less than 1.0 mass % and not more than 1.1 mass % C,
- not less than 0.15 mass % and not more than 0.25 mass % Si,
- not less than 0.25 mass % and not more than 0.35 mass % Mn, and
- not less than 0.15 mass % and not more than 0.25 mass % Cr,
- with the balance being Fe and unavoidable impurities;
- the steel wire having a wire diameter of not less than 0.15 mm and not more than 0.42 mm,
- the steel having a pearlitic microstructure formed by patenting, wherein the patenting includes austenitizing at a temperature Acm or higher and then isothermal transformation to obtain a fine pearlite structure;
- the steel having a dislocation density of not less than 2.4×1016 m−2 and not more than 5.0×1016 m−2, the dislocation density being determined from X-ray diffraction line-profile analysis of Fe (110), (200), (211), (220), and (310) reflections using a synchrotron radiation source and calculated by the modified Williamson-Hall method and the modified Warren-Averbach method;
- and
- the steel having a full width at half maximum in a circumferential direction of not less than 42° at a peak of a maximum intensity of a Debye ring for Fe (211) plane, the full width at half maximum being measured using an X-ray residual-stress analyzer with a Cr tube while aligning the wire axis with the incident direction and setting an incident angle of 35°, and determined as the angular distance between half-maximum points on a circle concentric with the Debye ring that passes through the maximum-intensity peak.
Dependencies are inferred from the claim text.