• 한국자기학회지
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• 제4권4호
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• pp.347-354
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• 1994

밀링 및 화학적 처리에 의해 제조된 소재의 구조해석 및 자기적 특성은 X선회절, 투과 전자현미경, 쾨스바우어 분광 및 비탄성 중성자산란 등의 측정에 의해 조사되었다. 질화처리에 의해 제조된 ${\gamma}'-Fe_{4}N$분말의 기계적 밀링처리에 의해, 대부분의 fcc ${\gamma}'-Fe_{4}N$상은 밀링 초기단계에 bct ${\alpha}'-Fe(N)$상으로 변태를 하며, 이러한 변태는 응력유기 마르텐사이트 변태로 규정지을 수 있다. 밀링처리에 제조한 bct ${\alpha}'-Fe(N)$ 초미세 분말의 열처리에 의해 673~773 K의 온도범위에서 ${\alpha}'-Fe_{16}N_{2}$상이 부분적으로 생성되며, 이로 인해 포화자화값이 증가한다. Mn-45, 70, 85 at.% Al의 조성으로 혼합한 분말은 기계적 합금화에 의해, Al은 부분적으로 ${\alpha}-Mn$상에 고용된다. 이로 인해 ${\alpha}-Mn$형 Mn-Al합금의 자기적 성질은 상자성에서 강자성으로 특성이 변하며, 특히 밀링처리한 Mn-70 at.% Al 계에 있어서 포화자화값은 11 emu/g을 나타낸다. 한편, 밀링처리한 Mn-85 at.% Al계에서 화학적 추출법을 이용하는 것에 의해 skeleton-type의 순 ${\alpha}-Mn$분말상을 제조한 결과 포화자화값은 36 emu/g으로 급격히 증가하였다.

• 열처리공학회지
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• 제11권2호
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• pp.111-120
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• 1998

The effects of chemical composition and thermal cycling on the martensitic transformation characteristics in Cu-rich, equiatomic and Zr-rich CuZr binary alloys have been studied by calorimetry. Only martensite could be indentified in equiatomic $Cu_{49.9}Zr_{50.1}$ alloy, while $Cu_{10}Zr_7$ and $CuZr_2$ intermetallic compounds as well as martensite were formed by rapid cooling from the melts in Cu-rich $Cu_{52.2}Zr_{47.5}$ alloy and Zr-rich $Cu_{48.4}Zr_{51.6}$ alloy, respectively. The $M_s$ temperature of $Cu_{49.9}Zr_{50.1}$ was $156^{\circ}C$ but those of $Cu_{52.5}Zr_{47.5}$ and $Cu_{48.4}Zr_{51.6}$ alloys, being $109^{\circ}C$ and $138^{\circ}C$, were lower than that of equiatomic $Cu_{49.9}Zr_{50.1}$ alloy. In all the alloys, the $M_s$ temperature has fallen but the $A_s$ temperature has risen, resulting in widening of the transformation hysteresis with thermal cycling. The anomalous characteristics in the transformation temperature are due to the presence of the intermetallic compounds i.e. $Cu_{10}Zr_7$ and $CuZr_2$ formed by an eutectoid reaction during thermal cycling in the temperature range between $-100^{\circ}C$ < $T_c$ < $400^{\circ}C$.

• 한국결정성장학회지
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• 제12권4호
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• pp.172-177
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• 2002

CuZnAl계 형상기억합금은 경제성, 열간 가공성 등이 우수하며 변태온도의 조절이 쉬운 등 여러 장점을 가지고 있으나, 열간 가공 중에 결정립이 쉽게 커지며, 취성이 심하고, 열이력에 대해서 형상기억 효과가 빨리 감소되는 등의 단점이 있다. 이러한 단점들은 결정립크기를 미세화함으로써 어느 정도 해소할 수 있다고 알려져 있다. 본 연구에서는 Cu-24.78Zn-9.11Al(at.%)과 Cu-13.22Zn-17.24Al(at.%)의 조성을 갖으며 비교적 작은 결정립크기를 갖는 형상기억합금을 99.9% 이상의 순도를 갖는 Cu, Zn 및 Al원소분말을 이용하여 SPS(spark plasma sintering) 방법으로 제조하였다. SPS 공정을 통하여 원소분말을 이용한 합금화가 가능함을 확인하였으며, 75-150 $\mu \textrm{m}$ 크기의 원소분말을 이용하여 제조한 경우, 두 조성 모두에서 약 70$\mu$m 의 결정립크기를 얻을 수 있었으며, 조성에 따라 상온에서 오스테나이트 단상 혹은 마르텐사이트 단상을 나타냄을 확인하였다.

• 대한기계학회논문집A
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• 제40권10호
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• pp.901-906
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• 2016

본 논문은 두께 10 mm의 조선용 강판 AH36에 대해 레이저-아크 하이브리드 용접을 사용하여 원패스 관통용접을 실시함으로써 실제 조선 산업에서의 생산성 향상을 목적으로 연구되었다. 10 mm두께의 후판을 사용하였기 때문에 관통용접을 얻기 위해서는 더욱 높은 레이저 및 아크의 출력이 요구되었다. 그러나 보다 더 증가된 레이저 및 아크 출력의 사용은 비드 양단에 언더컷과 같은 결함을 야기하였다. 이러한 언더컷은 노치로 작용하여 용접 구조물의 강도를 약화시키므로 반드시 방지되어야하며, 본 실험에서는 아크의 변수인 용접 전압 및 펄스컬렉션을 조절함으로써 제어할 수 있었다. 용접된 시험편의 기계적 특성을 파악하기 위해 레이저 영역 및 아크 영역에 대해 경도 측정을 실시하였다. 그 결과, 열영향부는 조직의 변태로 인해 최대 경도가 용접부보다 높은 것을 확인할 수 있었다. 미세조직 관찰 결과, 열영향부는 마르텐사이트 및 베이나이트와 같은 경한 조직으로 구성되어 있는 것을 알 수 있었다.

• 열처리공학회지
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• 제10권2호
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• pp.93-100
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• 1997

Effect of austenite grain size on starting temperature of ${\gamma}{\rightarrow}{\varepsilon}$ martensitic transformation($M_s$) has been studied in an Fe-18%Mn alloy. Particular attention was paid on the variation of stacking fault energy with austenite grain size, which is considered to be a important factor affecting ${\gamma}{\rightarrow}{\varepsilon}$ martensitic transformation. Austenite grain size was increased in a wide range from $13{\mu}m$ to $185{\mu}m$ with increasing solution treatment temperature from $700^{\circ}C$ to $1100^{\circ}C$. Hardness was decreased with increasing austenite grain size while the volume fraction of ${\varepsilon}$ martensite showed a reverse tendency, which indicates that the hardness is more dependent on austenite grain size than ${\varepsilon}$ martensite content. No significant change was found in $M_s$ temperature when the grain size was larger than about $30{\mu}m$. In case that, the austenite grain size was smaller than about $30{\mu}m$, however, $M_s$ temperature was marlkedly decreased with decreasing austenite grain size. A linear relationship between $M_s$ temperature and the stacking fault formation probability, i.e. the reciprocal of the stacking fault energy was obtained, which suggests that the variation of $M_s$ temperature with austenite grain size is closely related to the change in stacking fault energy.

• 한국분말재료학회지
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• 제28권3호
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• pp.246-252
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• 2021

The effect of sintering conditions on the austenite stability and strain-induced martensitic transformation of nanocrystalline FeCrC alloy is investigated. Nanocrystalline FeCrC alloys are successfully fabricated by spark plasma sintering with an extremely short densification time to obtain the theoretical density value and prevent grain growth. The nanocrystallite size in the sintered alloys contributes to increased austenite stability. The phase fraction of the FeCrC sintered alloy before and after deformation according to the sintering holding time is measured using X-ray diffraction and electron backscatter diffraction analysis. During compressive deformation, the volume fraction of strain-induced martensite resulting from austenite decomposition is increased. The transformation kinetics of the strain-induced martensite is evaluated using an empirical equation considering the austenite stability factor. The hardness of the S0W and S10W samples increase to 62.4-67.5 and 58.9-63.4 HRC before and after deformation. The hardness results confirmed that the mechanical properties are improved owing to the effects of grain refinement and strain-induced martensitic transformation in the nanocrystalline FeCrC alloy.

• 대한금속재료학회지
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• 제46권12호
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• pp.780-787
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• 2008

For the advanced high strength steels (AHSS), high-manganese TWIP (twinning induced plasticity) steels exhibit high tensile strength (800-1000 MPa) and high elongation (50-60%). However, the TWIP steels need to be understood of delayed fracture following the cup drawing test. Among the factors to cause delayed fracture, i.e, martensite transformation, hydrogen embrittlement and residual stress, the effects of martensite transformation (${\gamma}{\rightarrow}{\varepsilon}$ or ${\gamma}{\rightarrow}{\alpha}^{\prime}$) were investigated on the delayed fracture phenomenon. Microstructural phase analysis was conducted for cold rolled (20, 60, 80% reduction ratio) steels and tensile deformed (20, 40, 60% strain) steels. For the Al-added TWIP steels, no martensite phase was found in the cold rolled and tensile deformed specimen. But, the TWIP steels with no Al addition indicated the martensite transformation. The cup drawing specimens showed the martensite transformation irrespective of the Al-addition to the TWIP steel. However, the TWIP steel with no Al exhibited the larger amount of martensite than the case of the TWIP steel with Al addition. For the reason, it was possible to conclude that the Al addition suppressed the martensite transformation in TWIP steels, therefore preventing the delayed fracture effectively. However, it was interesting to note that the mechanism of delayed fracture should be incorporated with hydrogen embrittlement and/or residual stress as well as the martensite transformation.

• 열처리공학회지
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• 제23권5호
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• pp.233-238
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• 2010

The phase transformations and the shape memory effect in In-rich Pb alloys and In rich-Sn alloys have been studied by means of X-ray diffractometry supplemented by metallographic observations. The alloys containing 12~15 at.%Pb transform from the ${\alpha}_2$ (fct) phase to the ${\alpha}_1$ (fct) phase by way of an intermediate phase (m phase) on cooling. The results of X-ray diffraction show that the metastable intermediate phase is observed both on cooling and heating, and has a face-centered orthorhombic (fco) structure. It is concluded that the ${\alpha}_1{\rightleftarrows}{\alpha}_2$ transformation is expressed by the ${\alpha}_1{\rightleftarrows}m{\rightleftarrows}{\alpha}_2$ transformation both on usual cooling and heating with the rate more than $8{\times}10^{-3}$ K/s. The $m{\rightleftarrows}{\alpha}_2$ transformation takes place with a mechanism involving macroscopic shear and are of diffusionless (martensitic) type. The temperature hysteresis in the two transformations is 10~13 K between the heating and cooling transformations. The alloys containing 0~11 at.%Sn are -phase solid solutions with a face centered tetragonal structure (c/a > 1) at room temperature, the axial ratio increasing continuously with tin content. The In-(11~15) at.%Sn alloys are mixtures of ${\alpha}$ and ${\beta}$ phases, the ${\beta}$ phase having a f. c. tetragonal structure (c/a < 1). The alloys containing more than 15 at.%Sn are ${\beta}$-phase solid solutions. The In-(12.9~15.0) at.%Sn alloys show a shape memory effect only when quenched to the temperature of liquid nitrogen, although their effect becomes weak and finally disappears after keeping at room temperature for a long time. The ${\beta}{\rightarrow}{\alpha}^{\prime}$ phase transformation is of the diffusionless (martensitic) type, and takes place between 330 K at 12.9 at.%Sn and 150 K at 14.5 at.%Sn. The hysteresis of transformation temperatures on heating and cooling is considerably large (29~40 K), depending on the composition. Both In-Pb and In-Sn alloys showed distinct the shape memory effects.