• 제목/요약/키워드: Creep behavior

검색결과 591건 처리시간 0.023초

이방과압밀점토의 비배수크리프파괴 (V%drained Creep Rupture of an Anisotropically Overconsolidated Clay)

  • 강병희;오선호
    • 한국지반공학회지:지반
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    • 제12권6호
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    • pp.153-162
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    • 1996
  • 이방압밀이 과압밀점토의 비배수크리프파괴거동에 미치는 영향을 연구하기 위하여 등방 및 이방과압일시킨 점토시료에 대해서 비배수상태에서 크리프시험을 수행하였다. 연구결과 비배수 크리프파괴거동은 점토시료의 응력이력 즉 과압밀비와 압밀응력비$(\sigma_{3c}/\sigma_{le})$의 크기에 의해서 영향을 크게 받는다는 사실이 밝혀졌다. 즉 점토의 크리프강도는 과압밀비와 압밀응력비가 클수록 증가하므로 정지토압계수가 1.0보다 작은 점토지반의 크리프파괴 가능성을 등방압밀크리프피 괴시험에 의해서 판단하는 것은 위험하다. 그리고 점토의 크리프강도는 과압밀비와 압밀응력비의 크기에 관계없이 Finn과 Shead(1973)의 제안식에 의한 상한항복강도로서 구할 수 있었다.

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일반 크리프 거동을 고려한 균열 구조물 C*-적분 예측 (Estimation of C*-Integral for Defective Components with General Creep-Deformation Behaviors)

  • 김영진;김진수;김윤재
    • 대한기계학회논문집A
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    • 제26권5호
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    • pp.795-802
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    • 2002
  • For assessing significance of a defect in a component operating at high (creeping) temperatures, accurate estimation of fracture mechanics parameter, $C^{*}$-integral, is essential. Although the J estimation equation in the GE/EPRl handbook can be used to estimate the $C^{*}$-integral when the creep -deformation behavior can be characterized by the power law creep, such power law creep behavior is a very poor approximation for typical creep behaviors of most materials. Accordingly there can be a significant error in the $C^{*}$-integral. To overcome problems associated with GE/EPRl approach, the reference stress approach has been proposed, but the results can be sometimes unduly conservative. In this paper, a new method to estimate the $C^{*}$-integral for deflective components is proposed. This method improves the accuracy of the reference stress approach significantly. The proposed calculations are then validated against elastic -creep finite element (FE) analyses for four different cracked geometries following various creep -deformation constitutive laws. Comparison of the FE $C^{*}$-integral values with those calculated from the proposed method shows good agreements.greements.

오스테나이트계 25Cr-20Ni 스테인리스강의 실온예변형이 크리프 수명에 미치는 영향 (Effect of Room Temperature Prestrain on Creep Life of Austenitic 25Cr-20Ni Stainless Steels)

  • 박인덕;안석환;남기우
    • 대한기계학회논문집A
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    • 제28권4호
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    • pp.453-459
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    • 2004
  • 25Cr-20Ni series strainless steels have an excellent high temperature strength high oxidation and high corrosion resistance. However, further improvement can be expected of creep strength by work hardening prior creep. In the present study, the effect of prestraining at room temperature on the creep behavior of a Class M(STS310S) and a Class A(STS310J1TB) alloy containing precipitates have been examined. Prestaining was carried out at room temperature and range of prestrain was 0.5-2.5 % at STS310J1TB and 2.0-7.0% at STS310S. Creep behavior and creep rate of pre-strained specimens were compared with that of virgin specimens. Room temperature prestraining produced the creep life that is longer than that of a virgin specimen both for STS310J1TB and STS310S when creep test was carried out at the temperature lower than recrystallization temperature. The reason for this improvement of creep life was ascribable to the interaction between dislocations and precipitates in addition to the dislocation-dislocation interaction in STS310J1TB and the dislocation-dislocation interaction in STS310S. The beneficial effect of prestraining in STS310J1TB was larger than that of STS310S.

마그네슘 합금의 크리이프 거동에 표면처리가 미치는 영향 (The Effect of Surface Treatment on Creep Behaviors of Mg Alloy)

  • 강대민;안정오;강민철
    • 소성∙가공
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    • 제18권4호
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    • pp.347-353
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    • 2009
  • The apparent activation energy, the applied stress exponent, and rupture life have been measured from creep experiments over the range of $200^{\circ}C$ to $220^{\circ}C$ and the applied stress range of 64MPa to 94MPa. The materials were used AZ31 magnesium alloys treated by plasma electrolytic oxidation of $20{\mu}m$ and $40{\mu}m$ at surface to investigate the its influence on creep behavior, and creep tests were carried out under constant applied stress and temperature. The experimental results showed that the dipper the thickness of surface treatment the higher the activation energy and stress exponent. And the higher temperature and applied stress, the lower stress exponent and activation energy, respectively. Also the dipper the thickness of surface treatment the longer creep rupture time.

고온 기기의 크리프-피로 균열성장 평가 (Assessment of Creep-Fatigue Crack Growth for a High Temperature Component)

  • 이형연;김종범;이재한
    • 대한기계학회:학술대회논문집
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    • 대한기계학회 2008년도 추계학술대회A
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    • pp.264-268
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    • 2008
  • An assessment of creep-fatigue crack behavior is required to ensure the structural integrity for high temperature components such as fast breeder reactor structures or thermal power plant components operating at an elevated temperature. In this study, an evaluation of creep-fatigue crack growth has been carried out according to the French assessment guide of the RCC-MR A16 for austenitic stainless steel structures. The assessment procedures for creep-fatigue crack growth in the recent version of the A16 (2007 edition) have been changed considerably from the previous version (2002 edition) and the material properties (RCC-MR Appendix A3) have been changed as well. The impacts of those changes on creep-fatigue crack growth behavior are quantified from the assessments with a structural model. Finally the assessment results were compared with the observed images obtained from the structural tests of the same structural specimen.

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세립분 함량을 고려한 동결 사질토의 장기변형 예측 모델 평가 (Evaluation of Long-Term Deformation Prediction Model on Frozen Sand Considering Fine Contents)

  • 황범식;채덕호;조완제
    • 대한토목학회논문집
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    • 제37권1호
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    • pp.93-103
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    • 2017
  • 남극 대륙은 연구가치가 높은 다양한 생명체들과 풍부한 자원이 매장되어 있어 세계의 많은 국가들이 남극 개발에 관심을 가지고 있다. 우리나라는 2014년 제2의 남극과학기지인 장보고 과학기지를 준공한데 이어 남극 활주로 건설과 제3의 남극 과학기지 건설을 준비하며 남극 개발에 박차를 가하는 중이다. 하지만 동토의 경우 일반적인 흙과는 달리 얼음과 부동수분의 영향으로 시간에 따른 변형이 크게 나타나기 때문에 크리프 변형 특성을 파악할 필요가 있다. 그러나 크리프 변형 특성을 파악하기 위한 시험의 경우 많은 비용과 시간이 소모되기 때문에 예전부터 동토의 크리프 거동을 추정할 수 있는 모델에 대한 연구들이 많이 진행되어 왔으며, 본 연구에서는 동결 사질토의 함빙비를 고려한 장기변형 모델인 Ting의 Tertiary creep model의 모델 도출 방법에 세립분 함량을 고려할 수 있는 계수를 추가하여 다양한 흙에 적용할 수 있는 크리프 모델을 제안하고자 하였다. 이를 위해 세립분 함량이 0, 5, 10, 15%인 동결 시료로 -5, -10, -$15^{\circ}C$의 온도에서 일축 크리프 시험을 수행하였고, 시험 결과를 바탕으로 세립분 함량을 고려한 장기변형 예측 모델을 제안하였다. 그 결과, Tertiary creep model의 모델 도출 방법만을 사용하여 세립분함량을 고려한 장기변형 예측 모델을 제안하는 것은 무리가 있는 것으로 판단되어 동토의 크리프 변형을 고려하기 위한 새로운 개념의 모델이 필요할 것으로 판단된다.

Uniaxial fatigue, creep and stress-strain responses of steel 30CrNiMo8

  • Brnic, Josip;Brcic, Marino;Krscanski, Sanjin;Lanc, Domagoj;Chen, Sijie
    • Steel and Composite Structures
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    • 제31권4호
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    • pp.409-417
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    • 2019
  • The choice of individual material for industrial application is primarily based on knowledge of its behavior in similar applications and similar environmental conditions. Contemporary design implies knowledge of material behavior and knowledge in the area of structural analysis supported by large capacity computers. Bearing this in mind, this paper presents and analyzes the experimental results related to the mechanical properties of the material considered (30CrNiMo8/1.6580/AISI 4340) at different temperatures as well as its creep and fatigue behavior. All experimental tests were carried out as uniaxial tests. The test results related to the mechanical properties are presented in the form of engineering stress-strain diagrams. The results related to the creep behavior of the material are shown in the form of creep curves, while the fatigue of the material is shown in the form of stress - life (S - N) diagram. Based on these experimental results, the values of the following properties are determined: ultimate tensile strength (${\sigma}_{m,20}=696MPa$), yield strength (${\sigma}_{0.2,20}=355.5MPa$), modulus of elasticity ($E_{,20}=217GPa$) and fatigue limit (${\sigma}_{f,20,R=-1}=280.4MPa$). Results related to fatigue tests were obtained at room temperature and stress ratio R = -1.

미소시험편에 의한 재질열화된 내열강의 고온 크리프 특성 평가 (High Temperature Creep Characteristics Evaluation for Degraded Heat Resistance Steel of Power Plant by Mini-Specimen)

  • 류대영;백승세;유효선
    • 한국재료학회지
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    • 제13권7호
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    • pp.429-435
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    • 2003
  • In this study the new creep test using miniaturized specimen(10${\times}$10${\times}$0.5 ㎣) was performed to evaluate the creep characteristics for degraded materials of 2.25Cr-1Mo steel. For this creep test, the artificially aged materials for 330 hrs and 1820hrs at $630^{\circ}C$ were used. The test temperatures applied for the creep deformation of miniaturized specimens was X$630^{\circ}C$ and the applied loads were between 45 kg∼80 kg. After creep test, macro- and microscopic observation were conducted by the scanning electron microscope(SEM). The creep curves depended definitely on applied load and microstructure and showed the three stages of creep behavior like uniaxial tensile creep curves. The load exponents of virgin, 330 hrs and 1820 hrs materials based on creep rate showed 14.8, 9.5 and 8.3 at $550^{\circ}C$ respectively, The 1820 hrs material showed the lowest load exponent and this behavior was also observed in the case of load exponent based on creep rupture time. In contrast to virgin material which exhibited fined dimple fractography, a lot of carbides like net structure and voids were observed on the fractography of degraded materials.

Sp-Creep 시험에 의한 고온 크리프 특성 평가 기술 개발(ll) - 보일러 헤더 - (Development of Evaluation Technique of High Temperature Creep Characteristics by Small Punch-Creep Test Method (ll) - Boiler Header -)

  • 백승세;이동환;하정수;유효선
    • 대한기계학회논문집A
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    • 제26권1호
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    • pp.55-60
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    • 2002
  • For the development of a new creep test technique, the availability of SP-Creep test is discussed for 1Cr-0.5Mo boiler header material. And some results are also compared with those of 2.25Cr- 1Mo steel which widely uses as boiler superheater tube. The results can be summarized as follows. The load exponents(n) obtained by SP-Creep test for 1Cr-0.5Mo steel are decreased with increasing creep temperature and the values are 15.67, 13.89, and 17.13 at 550$^{circ}C$ ,575$^{circ}C$ and 600$^{circ}C$, respectively. The temperature dependence of the load exponent is given by n = 107.19 - 0.1108T. This reason that load exponents show the extensive range of 10∼16 is attributed to the fine carbide such as M$_{23}$C$_{6}$ in lath tempered martensitic structures. At the same creep condition, the secondary creep rate of 1Cr-0.5Mo steel is lower than the 2.25Cr-1Mo steel1 due to the strengthening microstructure composed by normalizing and tempering treatments. Through a SEM observation, it can be summarized that the primary, secondary, and tertiary creep regions of SP-Creep specimen are corresponding to plastic bending, plastic membrane stretching, and plastic instability regions among the deformation behavior of four steps in SP test, respectively.y.

25Cr-20NirP 스테인리스강의 예변형에 의한 크리프 거동 (Effect of Prestrain on Creep Behavior of Austenitic 25Cr-20Ni Stainless Steels)

  • 박인덕;안석환;남기우
    • 한국해양공학회:학술대회논문집
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    • 한국해양공학회 2003년도 추계학술대회 논문집
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    • pp.100-105
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    • 2003
  • 25Cr-20Ni series strainless steel have an excellent high temperature strength, high oxidation and high corrosion resistance. However, further improvement can be creep strength by work hardening prior creep. In the present study, the effect of prestraining at room temperature on the creep behavior of a Class M(STS310S) and a Class A(STS310J1TB) alloy containing precipitates have been examined. Prestraining was carried out at room temperature and range of prestrain was $0.5{\sim}2.5$ % at STS310J1TB and $2.0{\sim}7.0$ % at STS310S. Creep behavior and creep rate of pre-strained specimens were compared with that of virgin specimens. Room temperature prestraining produced the creep life that is longer than that of a virgin specimen both for STS310J1TB and STS310S when creep test carried out at the temperature lower than recrystallization temperature. The reason for this improvement of creep life was ascribable to the interaction between dislocations and precipitates in addition to the dislocation-dislocation interaction in STS310J1TB and the dislocation-dislocation interaction in STS310S. The beneficial effect of prestraining in STS310J1TB was larger than that of STS310S.

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