| Project/Area Number |
62550515
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| Research Category |
Grant-in-Aid for General Scientific Research (C)
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| Allocation Type | Single-year Grants |
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| Research Field |
金属材料(含表面処理・腐食防食)
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| Research Institution | Tokyo University of Agriculture and Technology |
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Principal Investigator |
HASEGAWA Tadashi Tokyo Univ. of Agri. & Tech., Dept. of Mech. Eng., Professor, 工学部, 教授 (50005328)
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| Co-Investigator(Kenkyū-buntansha) |
YAKOU Takao Tokyo Univ. of Agri. & Tech., Dept. of Mech. Eng., Assosiate Professor, 工学部, 助教授 (40111637)
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| Project Period (FY) |
1987 – 1988
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| Project Status |
Completed (Fiscal Year 1988)
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| Budget Amount *help |
¥1,600,000 (Direct Cost: ¥1,600,000)
Fiscal Year 1988: ¥200,000 (Direct Cost: ¥200,000)
Fiscal Year 1987: ¥1,400,000 (Direct Cost: ¥1,400,000)
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| Keywords | Creep crack propagation / 316H austenitic steel / 9Cr-1Mo martensitic steel / 2(1 / 4)Cr-1Mo ferritic steel / Cavitation / Work-hardening / Work-softening / 損傷過程 / 9Cr-1Moマルテンサイト鋼 / 耐熱鋼 / 微小硬さ / 転移組織 / 高温クリープ / き裂伝播 / 21 / 4Cr-1Moフエライト鋼 |
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| Research Abstract |
Behavior of crack propagation and local deformation near the crack tip during high-temperature straining (T=923K, =-5x10^<-6>/s) was examined in three types of heat-resistant steel ( 316H austenitic steel, 9Cr-lMo martensitic steel and 2(1/4)Cr-lMo ferritic steel), in order to make clear the mechanism of creep crack propagation. Main results and conclusions are summarized as follows: (1) The rate of crack propagation and frequency of cavitation near the crack tip decreases in the order of austenititic steel, martensitic steel and ferritic steel, though the crack tip opening becomes larger in this order. (2) Even in the austenitic steel which exhibits typical intergranular crack growth with grain-boundary cavitation and is brittle macroscopically, the degree of stress concentration at the crack tip is quite small (1.2-1.3), indicating that a stress concentration at the crack tip is relaxed extensively by local plastic deformation near the crack tip. (3) With increasing degree of biaxial tensile state of stress, the crack propagation rate increases, being accompanied by an increase in the degree of stress concentration and the frequency of cavitation and also by decrease in the size of crack tip area where work-hardening and cavitation are concentrated. (4) The results (1)-(3) indicate that crack propagation depends on the establishment of critical states of both work-hardening and cavitation in crack tip area. Crack propagation rate in a material, which exhibits work-softening during deformation, is very low.
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