분산강화 동합금의 Creep 특성

The Characteristics of Creep for Dispersion Strengthened Copper

  • 박규철 (충북대학교 공과대학 재료공학과) ;
  • 김경환 (충북대학교 공과대학 재료공학과) ;
  • 문준영 (충북대학교 공과대학 재료공학과) ;
  • 최재하 (충북대학교 공과대학 재료공학과)
  • Park, K.C. (Department of Materials Engineering, Chungbuk National University) ;
  • Kim, G.H. (Department of Materials Engineering, Chungbuk National University) ;
  • Mun, J.Y. (Department of Materials Engineering, Chungbuk National University) ;
  • Choi, J.H. (Department of Materials Engineering, Chungbuk National University)
  • 투고 : 2001.06.14
  • 발행 : 2001.07.31

초록

The static creep behaviors of dispersion strengthened copper GlidCop were investigated over the temperature range of $650{\sim}690^{\circ}C$ (0.7Tm) and the stress range of 40~55 MPa (4.077~5.61 $kg/mm^2$). The stress exponents for the static creep deformation of this alloy was 8.42, 9.01, 9.25, 9.66 at the temperature of 690, 677, 663, and $650^{\circ}C$, respectively. The stress exponent, (n) increased with decreasing the temperature and became dose to 10. The apparent activation energy for the static creep deformation, (Q) was 374.79, 368.06, 361.83, and 357.61 kg/mole for the stress of 40, 45, 50, and 55 MPa, respectively. The activation energy (Q) decreased with increasing the stress and was higher than that of self diffusion of Cu in the dispersion strengthened copper. In results, it can be concluded that the static creep deformation for dispersion strengthened copper was controlled by the dislocation climb over the ranges of the experimental conditions. Larson-Miller parameter (P) for the crept specimens for dispersion strengthened copper under the static creep conditions was obtained as P=(T+460)(logtr+23). The failure plane observed for SEM slightly showed up transgranular at that experimental range, however, universally it was dominated by characteristic of the intergranular fracture.

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