• Bulletin of the Korean Chemical Society
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• 제12권5호
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• pp.490-494
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• 1991

The ${\beta} to {\alpha}$ phase transition in silver iodide is studied with the (N, V, E) and (N, P, T) molecular dynamics (MD) method. In experiments, the phase transition temperature is 420 K. Upon heating of ${\beta}$ form, the iodine ions undergo hcp to bcc transformation and silver ions become mobile. MD simulations for the ${\beta}$ and ${\alpha}$ phases are carried out at several temperatures and the radial distribution functions (rdf) are obtained at those temperatures in the (N, V, E) ensemble. But the phase transition is not found in our calculation. Next the phase transition is studied with the (N, P, T) MD and we find some evidences of phase transition. At 3 Kbars and 2 Kbars the phase transition temperatu re is about 300 K. For 3.55 Kbars, the phase transition is higher (420 K) than the low pressure case. The phase transition temperature is somewhat dependent on the pressure in our calculations.

• Bulletin of the Korean Chemical Society
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• 제32권2호
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• pp.451-454
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• 2011

The traditional BCS superconductors $AOs_2O_6$ (A=K, Rb, and Cs) were investigated to find the relationship between their structures and superconducting transition temperatures. The $T_c$ decreases with increasing the unit cell parameter of $AOs_2O_6$. This is in contrast to the case of conventional BCS superconductivity in a single bond model, where $T_c$ may increase with increasing the the unit cell parameter since the DOS at Fermi level increases as the unit cell parameter increases. Instead, the $T_c$ of a $\beta$-pyrochlore oxide is proportional to the lattice softness of the compound.

• Composites Research
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• 제26권2호
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• pp.123-128
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• 2013

PVDF(polyvinylidene fluoride) 섬유는 습식방사방법을 적용하여 제조하였다. PVDF 분자 내 압전 특성과 밀접한 관련을 갖는 ${\beta}$형태의 결정 함량을 높이기 위하여, 본 연구에서는 습식방사 된 섬유에 1단계 연신, 2단계 어닐링 공정으로 구성하여 후 처리를 도입하였다. 후 처리는 PVDF 고분자의 유리전이 온도($T_g$)와 용융온도($T_m$) 사이의 온도범위에서 진행하여, 최대의 ${\beta}$형태 결정을 생성 할 수 있는 열처리 조건을 최적화 하였다. 제조된 PVDF 섬유 내 분자 배향 특성과 결정 구조를 확인하기 위하여 적외선 분광 광도계(FT-IR)와 X선 회절 분석기(XRD)를 이용하여 분석하였으며, 전자현미경(SEM)을 통하여 섬유의 표면을 관찰하여 섬유의 평균직경을 확인하였다. 분석 결과, 후 처리 공정이 PVDF 결정 구조의 영향을 미치며, ${\beta}$형태의 결정 비율을 증가시킨다는 것을 확인하였다. 더불어 ${\beta}$형태 결정 향상으로 인해 기계적 강도가 증가되었으며, 압전 특성 향상까지 기대할 수 있었다.

• Journal of Mechanical Science and Technology
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• 제18권12호
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• pp.2204-2208
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• 2004

Ti-8Ta-3Nb has been developed as a new biomaterial. The experimental specimens are as-cast and forged Ti-8Ta-3Nb alloys. Treatment in a solution, ranging from 760 to 960$^{\circ}C$ has carried out. The microstructural research has carried out after the solution treatment and the hardness was measured. The specific heat and the length variations of Ti-8Ta-3Nb were also measured. The optimum temperature for the solution heat treatment of Ti-8Ta-3Nb was found to be 880$^{\circ}C$. This was based on the mechanical properties and the volume fraction of ${\alpha}$ phase and their phases shown from the results of the solution heat treatment. From the results, the ${\beta}$ transition temperature of Ti-8Ta-3Nb was found to be between 860$^{\circ}C$ and 880$^{\circ}C$.

• Current Applied Physics
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• 제18권11호
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• pp.1248-1254
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• 2018

Magnetization versus temperature and magnetic-field measurements, M(T, $H_a$), have been carried out to study the magnetic and critical properties of polycrystalline $La_{1-x}Ba_xCoO_3$ (x = 0.3 and 0.5) cobaltites. These compounds with the density of ${\sim}6.2g/cm^3$ crystallized in the $R{\bar{3}}c$ rhombohedral and $Pm{\bar{3}}m$ cubic structures, respectively. With an applied field $H_a=200Oe$, M(T) data have revealed that the samples with x = 0.3 and 0.5 exhibit the ferromagnetic-paramagnetic (FM-PM) phase transition at the Curie temperature points $T_C=202$ and 157 K, respectively. At 4.2 K, the saturation magnetization ($M_{sat}$) decreases from 35.9 emu/g for x = 0.3-26.1 emu/g for x = 0.5. Particularly, the critical-behavior analyses in the vicinity of $T_C$ reveal all samples undergoing a second-order phase transition, with critical exponent values (${\beta}=0.328$ and ${\gamma}=1.251$ for x = 0.3, and ${\beta}=0.331$ and ${\gamma}=1.246$ for x = 0.5) close to those expected for the 3D Ising model. This proves short-range magnetic order existing in $La_{1-x}Ba_xCoO_3$. We believe that magnetic inhomogeneities due to the mixture of hole-rich FM regions (confined in the trivalent-cobalt hole-poor anti-FM matrix) and uniaxial anisotropy prevent long-range order in $La_{1-x}Ba_xCoO_3$.

• 폴리머
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• 제36권4호
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• pp.507-512
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• 2012

순수 PMMA와 methacryl-polyhedral oligomeric silsesquioxane(Ma-POSS)를 5 wt% 첨가한 PMMA를 박막(~650 nm)과 초박막(~50 nm)으로 제조하였으며, 유리전이온도($T_g$)와 등온 물리적 시효에 미치는 박막의 두께에 미치는 POSS의 첨가 효과를 시차주사열량계(DSC)를 이용하여 조사하였다. 초박막화와 Ma-POSS의 첨가로 인해 $T_g$ 감소가 관찰되었다. 또한 등온 물리적 시효에 의한 엔탈피 완화값(${\Delta}H_{Relax}$)도 초박막화 Ma-POSS를 첨가하였을 때 감소하였다. 시효시간에 따른 ${\Delta}H_{Relax}$ 데이터에 KWW(Kohlrausch-Williams-Watts)식을 적용하여 최대 엔탈피(${\Delta}H_{\infty}$), 이완시간(${\tau}$) 그리고 이완시간의 분포상수(${\beta}$)를 결정하였으며 이를 비교 분석하였다.

• 멤브레인
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• 제13권4호
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• pp.291-299
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• 2003

PTMSP-PEI와 PDMS-PEI 복합막을 제조하고, 막의 특성을 FT-IR, $^1H-NMR,$ DSC, TGA, GPC, SEM을 사용하여 조사하였다. 제조된 PTMSP의 수평균분자량 (equation omitted)은 477,920 이었고, 중량평균분자량 (equation omitted)은 673,329이었고, 유리전이온도 ($T_g$)는 $224^{\circ}C$이었다. 제조된 고분자 복합막들에 의한 $H_2/N_2$ 혼합기체분리는 $25^{\circ}C$에서 압력의 변화에 따라 조사되었다. PTMSP-PEI와 PDMS-PEI 복합막들의 수소에 대한 분리인자 (${\alpha}, {\beta},$ equation omitted)값은 투과셀의 압력이 증가하면 증가하였다. PTMSP-PEI 복합막의 수소에 대한 (${\alpha}, {\beta},$ equation omitted 값은 ${\Delta}P$ 30psi 와 $25^{\circ}C$에서 2.28, 1.17, 1.96이었고, PDMS-PEI 복합막의 (${\alpha}, {\beta}$ equation omitted 값은 3.70, 1.53, 2.42 이었다.

• 한국초전도ㆍ저온공학회논문지
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• 제15권3호
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• pp.5-8
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• 2013

We have studied Hall effect for potassium (K)-doped $BaFe_2As_2$ superconducting thin films by analyzing the relation between the longitudinal resistivity (${\rho}_{xx}$) and the Hall resistivity (${\rho}_{xy}$). The thin films used in this study were fabricated on $Al_2O_3$ (000l) substrates by using an ex-situ pulsed laser deposition (PLD) technique under a high-vacuum condition of ~$10^{-6}$ Torr. The samples showed the high superconducting transition temperatures ($T_c$) of ~ 40 K. The ${\rho}_{xx}$ and the ${\rho}_{xy}$ for K-doped $BaFe_2As_2$ thin films were measured by using a physical property measurement system (PPMS) with a temperature sweep (T-sweep) mode at an applied current density of $100A/cm^2$ and at magnetic fields from 0 up to 9 T. We report the T-sweep results of the ${\rho}_{xx}$and the ${\rho}_{xy}$ to investigate Hall scaling behavior on the basis of the relation of ${\rho}_{xy}={A{\rho}_{xx}}^{\beta}$. The ${\beta}$ values are $3.0{\pm}0.2$ in the c-axis-oriented K-doped $BaFe_2As_2$ thin films, whereas the thin films with various oriented-directions like a polycrystal showed slightly lower ${\beta}$ than that of c-axis-oriented thin films. Interestingly, the ${\beta}$ value is decreased with increasing magnetic fields.

• 폴리머
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• 제31권4호
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• pp.343-348
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• 2007

이 논문에서는 vinylidene fluoride(VDF), trifluoroethylene(TrFE), chlorotrifluoroethylene(CTFE)을 사용하여 3성분계 고분자를 합성하였으며, 저온 개시제 di-tertiary-butylperoxide(DTBP)를 사용하여 현탁중합하였다. NMR, FT-IR을 통해 3성분계 고분자 사슬의 미세구조, 사슬형태의 변화에 대해 알 수 있었다. CTFE mol%가 증가할수록 $\beta$ 상태는 점차적으로 감소하고 $\gamma$ 상태는 증가하는 것을 알 수 있었다. DSC 분석결과, CTFE mol%가 증가할수록 상전이 온도($T_c$)는 상온으로 낮아지며 그 곡선은 점차 작아지고 넓게 퍼지는 현상을 확인하였다. 활성화 에너지는 Freeman-Carroll법에 의해 계산되었다.

• 한국염색가공학회지
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• 제9권6호
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• pp.18-25
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• 1997

The change of crystalline structure and mechanical properties of i-PP films which had before isothermally annealed at various temperature and times have been studied. The following results were abtain The crystallinity and crystallite size of the samples showed increasing above the annealing temperature of 13$0^{\circ}C$ and these are equilibrated after an annealing time of 30min. When the crystalline form was at annealling condition were below 13$0^{\circ}C$, 2min, subsequently achieving an $\alpha$, $\beta$ mixing form and at 13$0^{\circ}C$, 10min, the crystalline form entered an $\alpha$ form transition. It is achieved a typical $\alpha$ form at 15$0^{\circ}C$. The value of T'm was increasing until 13$0^{\circ}C$ but it was not founded at 15$0^{\circ}C$. The slopes which represented crystalline form in an Avrami plot differed from each other within the range of this experiment.