• Korean Journal of Materials Research
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• v.5 no.2
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• pp.184-190
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• 1995

IN 617 was crept under stresses of 107 and 180 MPa with monotonic deformation to strains of $\varepsilon$= 0.03 - 0.30 at 1073K. In order to determine the distances between the subgrain boundaries, the deformed specimens were examined at magnifications of one hundred thousand times by TEM. In cases . where TEM observations were not possible, subgrain angles($\theta$_{s}=sin^{-1}$(b/s))were measured by Kikuchi diffraction lines. The $\theta$_{k}$ converted from s values measured directly by TEM agreed very well with those measured from Kikuchi lines. Therefore, it was found that the $\theta$_{k}$ values could be used in obtaining s, especially in cases where it is impossible to measure s by TEM.

• Proceedings of the Korean Society of Propulsion Engineers Conference
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• 1997.11a
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• pp.27-27
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• 1997

최근 미사일 추진기관 및 기체 구조재로 사용되는 알루미늄 7175 합금의 형상의 변화와 제조공정 변화에 따른 미세조직 변화에 대하여 고찰하였다. 구조체는 사용처에 따라 Flange Type 또는 Ring Type 등으로 형상이 다양하므로 단조 조건과 제품의 위치에 따라 균일한 물성을 획득하기는 매우 어려운 숙제이다. 본 연구에서는 균일한 물성을 얻기 위한 여러 가지 제조 공정의 변화를 모색하였으며, 제조된 단조재의 미세조직을 통하여 물성과의 연관성을 검토하였다. 적용된 공정은 통상의 열간 단조공정, 아 결정립 미세화공정, 재 결정립 미세화 공정 등이며 단조재의 형상과 동일 부품에서도 부위에 따라 변형량이 다르므로 미세조직의 변화가 다르게 나타났다. 아결정립과 재결정립 미세화 공정은 제품의 형상에 따라 내·외부 결정립이 크기가 크게 변화되었다. 이는 내·외부에 재료에 축적되는 에너지의 양과 외적으로 가해지는 기계적 에너지 및 열적 에너지가 다르기 때문이며, 변형량이 큰 부분의 미세 석출물의 크기가 변형량이 적은 부분의 석출물보다 크게 감소됨은 준안정상이 기계적 에너지가 변형열에 의한 열에너지로 변환됨에 따라 상석출에 영향을 미친 것으로 판단된다. 이와 같은 결과는 미세 조직 제어가 알루미늄합금 단조재의 공정설계의 중요한 인자임을 재 확인시켜 주는 것으로 재료의 신뢰성이 필수적으로 요구되는 추진기관의 중요 부품에 적극 고려해야 할 요소라 할 수 있다.

• Transactions of the Korean Society of Mechanical Engineers
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• v.10 no.3
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• pp.292-297
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• 1986

Measurements of internal stress .sigma.$_{i}$, anelastic strain .epsilon.$_{A}$ and recovery rate .gamma. were made in steady state creep of 2024 Al alloys over a wide range of stresses at temperatures between 260.deg. C and 380.deg. C, for the purpose of investigating the relations among the three parameters. Values of .sigma.$_{i}$ were obtained by the method of strain transient dip test, and those of .epsilon.$_{A}$ and .gamma. were determined from the results of sudden stress removal or reduction tests. As a main result, it is thought that the anelastic behavior and recovery process are basically dependent on same deformation mechanisms.sms.sms.

• Proceedings of the Korea Committee for Ocean Resources and Engineering Conference
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• 2002.05a
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• pp.35-40
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• 2002

In the present study, we examined the influence of prestrain on creep strength of Class M alloy(STS310S) and Class A(STS310J1TB) alloys containing precipitates. Prestrain was given by prior creep at a higher stress than the following creep stresses. Creep behaviour before and after stress change and creep rate of pre-strianed specimens were compared with that of virgin specimens. Pre-straining produced the strain region where the strain rate was lower than that of a virgin specimen both for STS310J1TB and STS310S steels. The reason for this phenomenon was ascribable to the viscous motion of dislocations, the interaction between dislocations and precipitates in a STS310J1TB steel, and the interaction of dislocations with sub-boundaries in a STS310S steel which has the higher dislocation density and smaller subgrain size resulted from pre-straining at higher stress.

• Journal of Ocean Engineering and Technology
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• v.4 no.2
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• pp.262-262
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• 1990

In order to check the effect of dislocation behavior on creep rate in 12% Chromium steel, 14 samples of different compositions were examined by creep rupture test, and subgrain sizes, distribution of dislocations and precipitates were checked. And, authors reviewed the behaviors of dislocations, the formation and growth of subgrains and precipitates during creep. The results are as the following: 1) Creep rates calculated by .epsilon. over dot = .rho.bv show 10-15% higher values than actual data measured. However, authors conclude that the density and velocity of dislocations together with subgrain size are important factors governing deformation during creep in 12% chromium steel. 2) The values of the strength of obstacles in the mobility of dislocations are more clearly depended on the effective stress in the range of $10{\pm}5kgf/mm^{2}$ and increase with the increase of temperature. 3) Creep rates decrease with the smaller sizes of subgrains formed and can result in the longer creep rupture lives(hours). The smaller subgrains can be made by forming shorter free gliding distances of dislocations with very fine precipitates formed in the matrix during creep by applying proper alloy design. 4) Dislocation mobility gets hindered by precipitates occurring, which are coarsened by the softening process governed by diffusion during long time creep.

• Journal of Ocean Engineering and Technology
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• v.4 no.2
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• pp.112-120
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• 1990

In order to check the effect of dislocation behavior on creep rate in 12% Chromium steel, 14 samples of different compositions were examined by creep rupture test, and subgrain sizes, distribution of dislocations and precipitates were checked. And, authors reviewed the behaviors of dislocations, the formation and growth of subgrains and precipitates during creep. The results are as the following: 1) Creep rates calculated by .epsilon. over dot = .rho.bv show 10-15% higher values than actual data measured. However, authors conclude that the density and velocity of dislocations together with subgrain size are important factors governing deformation during creep in 12% chromium steel. 2) The values of the strength of obstacles in the mobility of dislocations are more clearly depended on the effective stress in the range of $10{\pm}5kgf/mm^{2}$ and increase with the increase of temperature. 3) Creep rates decrease with the smaller sizes of subgrains formed and can result in the longer creep rupture lives(hours). The smaller subgrains can be made by forming shorter free gliding distances of dislocations with very fine precipitates formed in the matrix during creep by applying proper alloy design. 4) Dislocation mobility gets hindered by precipitates occurring, which are coarsened by the softening process governed by diffusion during long time creep.

• Korean Journal of Materials Research
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• v.7 no.1
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• pp.50-56
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• 1997

급냉응고법을 이용하여 고용한도 이상으로 Mn량을 첨가할 때 Mn량에 따른 인장특성의 변화와 시효특성을 조사하였다. 원심분무법으로 AI-4.7%Zn-2.5%Mg-0.2%Zr합금에 Mn량을 각기 달리 첨가한 급냉응고 분말을 제조 하였다. 이 분말을 냉간압축, 진공 탈가스처리를 한 후 15:1로 압출하여 봉상 시편을 만들었다. 분말의 미세조직은 $\alpha$-AI수지상과 수지상간 편석부로 이루어져 있으며 Mn첨가에 따라 조직의 변화는 관찰되지 않았다. 빠른 냉각속도로 인하여 2.0%Mn을 첨가한 경우에도 초정 Mn상을 발견할 수 없었다. 압출재의 미세조직은 아결정립으로 이루어져 있으며 약간의 제2상들이 관찰되었다. 대부분의 Mn 분산상은 압출후 용체화처리 과정에서 형성되었으며 시효경화량은 Mn양에 관계없이 일정하였다. 46$0^{\circ}C$에서 1시간 용체화처리하고 12$0^{\circ}C$에서 24시간 시효처리한 경우 최대의 시효경도값을 나타내었다. 인장강도는 Mn첨가량에 따라 증가 하였는데 이것은 Mn분산상의 밀도증가에 의한 것으로 확인되었다. 2.0%Mn을 첨가한 합금의 시효후 인장강도는 590MPa, 연산율은 4%를 보였다.

• Korean Journal of Materials Research
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• v.9 no.11
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• pp.1123-1128
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• 1999

To investigate the effect of Sn on the recrystallization of Zr-based alloys. Zr-xSn (x=0.5, 0.8, 1.5, 2.0wt.%) alloys were manufactured to be the sheets through the defined manufacturing procedure. The specimens were annealed at $300^{\circ}C$ to $800^{\circ}C$ for 1 hour. The hardness, microstructure and precipitate of the alloys with the annealing temperature were investigated by using micro- knoop hardness tester, optical microscope(O/M) and transmission electron microscope(TEM), respectively. The cold-worked Zr-xSn alloys showed the typical behavior of the recovery. recrystallization, and grain growth. The recrystallization of Zr-xSn alloys occurred between $500^{\circ}C$ and $700^{\circ}C$. As the Sn content increased. the recrystallization temperature of the cold-worked alloys increased but their grain sizes after recrystallization decreased. It is suggested that the recrystallization of the cold- worked Zr alloys be occurred by the subgrain coalescence and growth mechanism.

• Journal of Ocean Engineering and Technology
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• v.16 no.3
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• pp.59-64
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• 2002

In the present study, we examined the influence of prestrain on creep strength of Class M alloy(STS310S) and Class A(STS310J1TB) alloys containing precipitates. Prestrain was given by prior creep at a higher stress than the following creep stresses. Creep behaviour before and after stress change and creep rate of pre-strained specimens were compared with that of virgin specimens. Pre-straining produced the strain region where the strain rate was lower than that of a virgin specimen both for STS310J1TB and STS310S steels. The reason for this phenomenon was ascribable to the viscous motion of dislocations, the interaction between dislocations and precipitates in a STS310J1TB steel, and the interaction of dislocations with sub-boundaries in a STS310S steen which has the higher dislocation density and smaller subgrain size resulted from pre-straining at higher stress.

• Korean Journal of Materials Research
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• v.5 no.3
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• pp.261-267
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• 1995

IN 617의 시편으로 1073K의 온도와 107과 180 MPA의 응력에서 $\varepsilon$=0.18까지 정압크\ulcorner을 한 직후 107 MPa로 응력을 낮추고 (응력강하시험), 또 다른 시편에는 180 ↔ 0.2 MPa의 응력으로 각각 17초씩 반복주기변형을 수행하여 정압크\ulcorner 변형시의 크\ulcorner곡선과 비교를 하엿다. 그 결과 IN 617 의 반복주기변형에서는 변형속도둔화(CCD)가 발생함을 알 수 있었고, 응력강하와 반복변형시험은 모두 거의 같은 모양의 회복 크\ulcorner곡선을 나타내었다. 이러한 회복 크\ulcorner은 아결정립크기와 자유전위밀도로서 그 회복기구를 설명할수 있었다.