• 한국세라믹학회지
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• 제18권4호
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• pp.257-261
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• 1981

The tendency of glass containing titanium-dioxide to separate into two phases can be attributed to a change of the coordination number of titanium from six to four on increase of temperature and to "freezing" of the high temperature four fold coordination on cooling of the melt. Addition of TiO2 to the basic glass 8.7 $Na_2O$ 22.4B2O3 68.9 $SiO_2$ was varied 5 to 25 parts. The phase separation in the temperature range of transformation was examined with each heating temperature and soaking time. As the experimental results, the most distinct phase separation were obtained from alkali extraction method when $TiO_2$ was added 15 parts. The apparant activation energy was 30.5 Kcal/mole by alkali extraction method derived from Arrhenius plots.ius plots.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2011년도 제40회 동계학술대회 초록집
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• pp.181-182
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• 2011

Phase-change materials can be cycled by exposure to laser beam, and as a function of the pulse intensity and duration, the laser beam triggers the switching from crystalline to amorphous phase and back. In other to progress better crystallization transition and amorphization long phase-transformation data of phase-change memory (PRAM), we investigated about the effect of Sb doping and Ag ions percolating into Ge-Se-Te phase-change material. Doped Sb concentrations was determined each of 10, 20 and 30 wt%. As the Sb-doping concentration was increased, the resistivity decreased and the crystallization temperature increased. Ionization of Ag was progressed by DPSS laser (532 nm) for 1 hour. The resistivity was more decreased and the crystallization temperature was more increased in case of adding Ag layer under Sb-(Ge-Se-Te) thin film. At the every condition of thin films included Ag layer more stable states were indicated compare with just Sb-doped Ge-Se-Te thin films.

• 한국분말재료학회지
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• 제3권3호
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• pp.174-180
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• 1996

Microstructure and phase transformation of mechanically alloyed TiNi powders added to aluminium matrix for enhancing the damping properties were studied. Four compositions between 48.5 and 51.5 at% Ti intermetallic compounds were selected to control the fraction of martensite phase. Mechanically alloyed TiNi powders were heat-treated at vacuum of $10^{-6}$ torr for crystallization. Ball milled AI/TiNi composite powders were swaged at room temperature and rolled at 450 $^{\circ}C$. After mechanical alloying for 10 hours, Ti and Ni elements were alloyed completely and amorphous phase was formed. Amorphous phase was crystallized to martensite (Bl9') and austenite(B2) after heat treating for 1 hour at the temperature of 850 $^{\circ}C$, and TiNi$_3$, intermetallic compound was partially formed. Considerable amount of martensite phase was remained after swaging and rolling.

• 한국재료학회지
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• 제10권9호
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• pp.619-623
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• 2000

알루미나 여과막은 boehmite 분말 (${\Upsilon}-AlOOH$)을 이용하여 졸-겔법으로 준비되어졌다. 제조된 여과막은 상전이 온도와 미세구조 변화를 관찰하기 위해 지지체 없이 형성된 여과막을 제조하였다. 여과 공정의 응용에서 균일한 기공크기와 분포를 제어하는 것이 중용하다. 다공성 담체 위에 형성된 여과막과 다공성 담체 없이 형성된 여과막의 ${\theta}-to\;{\alpha}-AL_2O_3$로의 상전이는 박막 XRD를 이용하여 분석하였고, 미세구조의 변화의 관찰은 주사전자현미경(SEM)을 사용하여 관찰하였다. XRD에서 분석된 결과는 다공성 담체 위에 형성된 여과막이 다공성 담체 없이 형성된 여과막과 비교하여 $100^{\circ}C$ 더 높은 상전이 온도를 가지는 것을 보여주었다. 이런 유사한 효과는 여과막의 미세구조 변화에서도 관찰되었다.

• 한국세라믹학회지
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• 제35권3호
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• pp.280-286
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• 1998

LaAlO3 Single crystals used as a substrate for thin film depositions of a high temperature oxide su-perconductor YB2Cu3O7 and applied to microwave frequencies were grown by the Traveling Solvent Flati-ing Zone (TSFZ) method and characterized. For the growth of LaAlO3 single crystals polycrystalline fe-edrods were prepared from powder mixture of La2O3 and Al2O3 with a mole ratio of 1:1 calcined at 110$0^{\circ}C$ for 3h and sintered at 140$0^{\circ}C$ for 4h The growth LaAlO3 crystals was 4-5mm in diameter 30mm in length and dark brown. The growth rate was 2-3mm/h and the rotation speeds were 10rpm for an upper ro-tation and 40 rpm for a lower rotation The growing crystals and the feedrods were counter-rotated. The orientation of the grown single crystals of LaAlO3 was identified to be [111] direction. Dielectric constants were measured to be 30-33 between 100 kHz and 1 MHz in the 30$0^{\circ}C$ to 45$0^{\circ}C$ temperature range and 102 in a range of 100 kHz at the phase transformation temperature of 522$^{\circ}C$ Dielectric losses were calculated to be 1.8$\times$10-4 at the room temperature and 5.7$\times$10-3 at the phase transformation temperature. Lattice con-stants of the grown crystlals were determined to be aR=5.3806 $\AA$ and $\alpha$=60.043$^{\circ}$ by the least square method.

• 태양에너지
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• 제5권2호
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• pp.77-83
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• 1985

An analysis is performed to investigate the influence of the buoyancy force and the thickness variation of melting layer in the containment that is filled with phase-change Material surrounding a cylindrical heating tube during melting process. The phase-change material is assumed to be initially solid at its phase-change temperature and the remaining solid at any given time is still at the phase-change temperature and neglecting the effect of heat transfer occuring within the solid. At the start of melting process, the thickness of melting layer is assumed to be a stefan-problem and after the starting process, the change of temperature and velocity is calculated using a two dimensional finite difference method. The governing equations for velocity and temperature are solved by a finite difference method which used SIMPLE (Semi Implicit Method Pressure linked Equations) algorithm. Results are presented for a wide range of Granshof number and in accordance with the time increment and it is founded that two dimensional fluid flow occurred by natural convection decreases the velocity of melting process at the bottom of container. The larger the radius of heating tube, the higher heat transfer is occurred in the melting layer.

• 한국세라믹학회지
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• 제29권8호
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• pp.630-638
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• 1992

Ta2O5 alloying into 3 mol% Y2O3-stabilized tetragonal ZrO2 polycrystals (3Y-TZP) increased the degradation during aging at 265℃ and the fracture toughness; both are determined by the amount of transformed m-ZrO2. It was proposed that the mechanism underlying the t→m transformation when aged at low temperatures is attributed to the reorientation of (Zzr'V ). complexes parallel to [111] lattice direction, which is accompanied by a relaxation of TZP lattice during annealing at low temperature. A small strain which results from the reorientation gives rise to a localized mechanical instability, thus lowering the nucleation barrier so that the t→m phase transformation (degradation) proceeds. The amount of transformed m-ZrO2 during aging becomes greater as the chemical free energy change related to the transformation, ΔGo, increases with increasing the Ta2O5 alloying content.

• Smart Structures and Systems
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• 제16권1호
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• pp.183-194
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• 2015

Shape memory alloy (SMA) helical springs have found a large number of different applications in industries including biomedical devices and actuators. According to the application of SMA springs in different actuators, they are usually under tension and torsion loadings. The ability of SMAs in recovering inelastic strains is due to martensitic phase transformation between austenite and martensite phases. Stress or temperature induced martensite transformation induced of SMAs is a remarkable property which makes SMA springs more superior in comparison with traditional springs. The present paper deals with the simulation of SMA helical spring at room temperature. Three-dimensional phenomenological constitutive model is used to describe superelastic behavior of helical spring. This constitutive model is implemented as a user subroutine through ABAQUS STANDARD (UMAT), and the process of the implementation is presented. Numerical results show that the developed constitutive model provides an appropriate approach to captures the general behavior of SMA helical springs.

• Korean Chemical Engineering Research
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• 제48권5호
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• pp.627-631
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• 2010

질산 알루미늄과 암모니아 용액을 출발물질로 하고 또한 금속 불화물을 첨가제로 사용하여 $\alpha$-알루미나 입자를 침전법으로 제조하였다. 이 때 제조과정에서 사용된 용매의 영향과 $AlF_3$, $CaF_2$, $MnF_2$ 등의 3 가지 금속 불화물 첨가제가 $\alpha$-알루미나로의 상전이 온도, 입자 크기 및 형태 등에 미치는 영향에 대해 조사하였다. $\alpha$-알루미나 제조시 사용된 용매는 상전이 온도에는 큰 영향을 미치지 않는 반면 입자 크기에 영향을 미쳤다. 첨가제 조성에 따라 $\alpha$-알루미나 상전이 온도가 차이가 났으나($AlF_3(800^{\circ}C)$ < $MnF_2(900^{\circ}C)$ < $CaF_2(950^{\circ}C)$), 첨가제를 사용하지 않은 경우($1,100^{\circ}C$)보다는 모두 상전이 온도가 낮음을 알 수 있었다. 3 가지 첨가제를 사용한 경우 모두 판상의 $\alpha$-알루미나 입자들이 얻어졌으나, 그 중 $MnF_2$를 첨가한 경우에 가장 작은 크기의 $\alpha$-알루미나 입자들이 생성되었다.

• 대한조선학회논문집
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• 제39권1호
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• pp.82-89
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• 2002

선상가열에 의한 판 변형 예측은 고유변형도법에 의해 효율적으로 예측할 수 있다. 종래의 용접에서의 고유변형도 결정 방법은 용접 실험을 통하여 온도분포와 강의 상변태 영역(Ac3)을 시편을 절단하여 계측하고 이를 고유변형도 영역으로 간주하는 것이었다. 선상가열의 현상은 용접과 유사하므로, 용접과 같은 조건 하에서 얻어진 결과를 그대로 선상가열 해석에 이용하여 왔으나 이 결과는 가열 패턴이나 판 두께에 제한을 가지고 있다. 또한 현장에서는 선상가열 후 수냉 처리하는데 그 과정에서 강이 원래의 상으로 돌아가지 않고 마르텐사이트가 되면서 전단 소성 변화를 일으킨다는 점에 착안하여, 본 연구에서는 종래에 시편의 온도계측과 상변태 영역을 직접 계측하는 파괴검사법을 FEM을 이용한 이론해석으로 대체하였다. 즉 임의의 적절한 열속 모델에 대한 온도 분포를 얻고, 조직변화에 따라 추가적으로 발생하는 소성 영역을 고려하기 위하여 공석 온도 영역까지 포함시켜 온도계측과 파괴실험 없이 순수한 이론만으로 고유변형도 영역을 결정하는 새로운 방법을 제안하였다. 이 방법으로 결정한 영역을 이용하여 판의 변형을 예측하고 실험 결과와 비교하여 잘 일치함으로써 본 논문에서 제안한 방법의 유효성을 입증하였다.