• 폴리머
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• 제29권6호
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• pp.605-612
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• 2005

폴리올레핀계 공중합체 수지인 polypropylene-polyethylene-(1-butene) 미발포 수지에 부탄 가스를 물리적 발포제로 이용하여 단열 팽창시킨 발포체의 등온 결정화 거동을 DSC(differential scanning calorimeter)와 편광 현미경을 이용하여 고찰하였으며, 얻어진 결과는 Avrami 식을 이용하여 해석하였다. 발포체의 결정화 반감 시간이 미발포체의 결정화 반감 시간보다 짧고 핵 생성 속도 증가에 따른 nucleation density증가 및 구정 성장 속도가 더 빠름이 발견되었는데, 이는 가공 공정 중의 분자량 감소보다는 단열 팽창 과정에서 진행되는 연신 배향 결정화에 의해 결정화 속도가 증가하였기 때문인 것으로 사료된다. 또한, 단열 구조 발포체는 직경 30 $\mu$m 이하의 균일한 closed cell 형태를 나타내고 있음을 SEM 을 이용하여 관찰하였고, 발포체의 물성은 미발포체에 비해 단열성이 크기 때문에 열전도도가 감소하였고 압축강도는 발포비가 증가할수록 감소하는 것을 알 수 있었다.

• 대한기계학회논문집A
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• 제35권7호
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• pp.717-722
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• 2011

본 연구의 목적은 Al6061 의 T6 열처리 시 발생되는 잔류응력의 변화를 예측하는 것이다. Al6061-T6 의 일반적인 열처리 조건인 용체화처리($530^{\circ}C$, 2hr)와 인공시효($175^{\circ}C$, 9hr)에서 인공시효 시간에 따라 잔류응력 변화를 고려하였다. 잔류응력 예측은 열처리 실험을 수행하여 대류 열전달계수를 확보하고, 탄소성 모델로 가정한 유한요소해석을 적용하였다. 또한 인공시효와 같이 재료가 고온에서 장시간 유지되는 경우의 Zener-Wert-Avrami 함수를 적용하여 잔류응력 변화를 확인하였다. 잔류응력의 측정은 X 선 회절법으로 측정하고 측정결과는 예측된 유한요소해석 결과와 비교하여 해석의 신뢰성을 확보하고 해석기법을 확립하였다.

• 대한금속재료학회지
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• 제50권3호
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• pp.256-262
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• 2012

This study investigated the hydrogen storage properties of Zr-Based $AB_{2-x}M_x$ metal hybride made by HCS (Hydriding Combustion Synthesis). The materials were prepared by HCS 80 wt% $AB_2$-15 wt% Mg-5 wt% Mm, HCS 80 wt% $AB_2$-20 wt% Mg and pure Zr-Based $AB_2$, These materials were activated at 298 K under 20 bar. Both HCS 80 wt% $AB_2$-20 wt% Mg and HCS 80 wt% $AB_2$-15 wt% Mg-5 wt% Mm were absorbed within 1 minute. In the case of the $AB_2$, it was perfectly absorbed within 6 minutes. Then, the materials were evaluated to obtain P-C-T (Pressure-Composition-Temperature) curves at 298K. As a result, the hydrogen storage capacity of HCS 80 wt% $AB_2$-20 wt% Mg, HCS 80 wt% $AB_2$-15 wt% Mg-5 wt% Mm and pure Zr-Based $AB_2$ were determined to be 1.2, 1.6 and 1.74 wt%, respectively. The activation energy and rate controlling step were calculated by the Johnson-Mehl Avrami equation. The activation energies of HCS 80 wt% $AB_2$-20 wt% Mg, HCS 80 wt% $AB_2$-15 wt% Mg-5 wt% Mm and pure Zr-Based $AB_2$ were 26.91, 20.45, and 60.41 kJ/mol, respectively. Also, the values of ${\eta}$ in the Johnson-Mehl Avrami equation for HCS 80 wt% $AB_2$-20 wt% Mg, HCS 80 wt% $AB_2$-15 wt% Mg-5 wt% Mm and pure Zr-Based $AB_2$ are 0.60, 0.51, and 0.44. So, the rate controlling steps which indicate hydrogen storage mechanism are an one dimensional diffusion process.

• 한국자기학회지
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• 제4권1호
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• pp.12-19
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• 1994

비정질 $Fe_{73.5}Cu_{1}Nb_{3}Si_{16.5}B_{6}$ 합금의 $552^{\circ}C$에서 등온열처리시간에 따른 결정화 거동을 $M\"{o}ssbauer$ 분광법으로 연구하였다. 열처리된 시료는 $Do_{3}-FeSi$ 초미세결정립, Cu-cluster 및 비정질이 공존함이 $M\"{o}ssbauer$ spectrum 분석에 의해 확인되었다. 결정화 초기단계에 Cu-cluster가 형성되기 때문에 FeSi 초미세결정립의 Si함량은 높아지며, 열처리시간이 60분이 될 때까지 Si함량은 감소하는데 이는 FeSi 초미세결정립의 평균초미세자기장의 증가를 일으키며, 이후 Si함량은 거의 일정하다. 60분 이후의 열처리에서 FeSi 초미세결정립과 잔류비정질의 체적분율이 미소하게 변화함에도 잔류비정질의 평균초미세자기장이 감소하는 것은 잔류비정질에서의 Nb, B원자의 존재비의 증가에 기인된다. $552^{\circ}C$에서 60분 열처리 할 경우 FeSi 초미세결정립과 잔류비정질의 초미세자기장의 방향이 모두 무질서하게 분포된다. FeSi 초미세결정립과 Cu-cluster의 Avrami지수는 각각 0.51, 0.65, 잠복기는 각각 2.4분, 0.8분, 활성화에너지는 각각 2.35 eV, 2.44 eV이며, Cu-cluster가 FeSi 초미세결정립보다 먼저 생성된다는 것은 Cu 원자가 FeSi 초미세결정립의 생성을 촉진시킨다는 해석과 부합한다.

• 한국소성가공학회:학술대회논문집
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• 한국소성가공학회 2000년도 추계학술대회 논문집
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• pp.33-36
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• 2000

The dynamic recrystallization (DRX) of medium carbon steels (SCM 440 and POSMA45) was studied with torsion test in the temperature range of $900-1100^{\circ}C$ and the strain rate range of $5.0x10^{-2}\;-\;5.0x10^0/sec$. To establish the quantitative equations for DRX, the evolution of flow stress curve with strain was analyzed. The critical strain (${\varepsilon}_c$) and strain for maximum softening rate ( ${\varepsilon}^{*}$) could be confirmed by the analysis of work hardening rate ($d{\sigma}/d{\varepsilon}\;=\; \theta$). The volume fraction of dynamic recrystallization ($X_{DRX}$) as a function of processing variables, such as strain rate ( $\dot{\varepsilon}$ ), temperature (T), and strain ( $\varepsilon$ ) were established using the ${\varepsilon}_c$ and ${\varepsilon}^{*}$. For the exact prediction, the ${\varepsilon}_c$, ${\varepsilon}^{*}$ and Avrami' exponent (m') were quantitatively expressed by dimensionless parameter, Z/A respectively. The transformation-effective strain-temperature curve for DRX could be composed. It was found that the calculated results were agreed with the experimental data for the steels at any deformation conditions.

• 한국결정성장학회지
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• 제6권2호
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• pp.275-285
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• 1996

The effect of heat-treatment on catalytic crystallization in $LI_2O-Al_2O_3-SiO_2$ glass system over its glass transition temperature was investigated. Glass composition $4Li_2O{cdot}22AL_2O_3{cdot}66SiO_2{cdot}2TiO_2{cdot}2.5ZrO_2{cdot}1.5P_2O_5{cdot}1.0Na_2O{cdot}1.0As_2O_3$ (wt%) was selected and heat-treated at different heating conditions to obtain transparent glass-ceramic. Nucleation and crystallization behaviour of this composition were estimated by differential thermal analysis (DTA) and X-ray diffractometer (XRD) and its thermal expansion coefficients were measured by Dilatometer. As a result, glass transition temperature was $730^{\circ}C$ and two maximum nucleation temperatures were estimated at $730^{\circ}C$ and 82$0^{\circ}C$ using JMA(Johson-Mehl-Avrami) equation by DTA. $ZrTiO_4$ $\beta$-Quartz solid solution and $\beta$-Spodumene crystals were identified by XRD. The optimum crystallization temperature was 92$0^{\circ}C$ and three step heating schedule was expected to be useful to obtain transparent glass-ceramic.

• Macromolecular Research
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• 제17권7호
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• pp.476-482
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• 2009

The crystallization behavior of poly(vinyl alcohol) (PVA) in the presence and absence of polypyrrole nanoparticles (PPy NPs) was investigated in terms of the heterogeneous nucleation effect of PPy NPs using FTIR, X-ray diffraction, differential scanning calorimeter and polarized optical microscope analysis. PPy NPs were prepared by dispersion polymerization method stabilized by PVA in aqueous solution. A polymer nanocomposite with uniform dispersity could be readily obtained due to the enhanced compatibility between the filler and matrix. Compared with the PPy NP-absent PVA, the PPy NP/PVA nanocomposite exhibited an enhanced degree of crystallinity. The degree of crystallinity increased up to 17% at the PPy NP concentration of 1 wt%, compared to the pristine PVA. The PPy NP acted as an effective nucleating agent during the crystallization process, thereby enhancing the degree and rate of crystallization. The kinetics study of the crystallization also revealed the decreased value of the Avrami coefficient in the case of the PPy NP/PVA nanocomposite.

• 한국식품조리과학회지
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• 제16권5호
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• pp.402-409
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• 2000

수분의 첨가수준을 달리하여 제조한 절편의 저장기간에 따른 노화특성 및 품질특성을 평가하였다. 색도는 저장기간에 따른 시료간의 유의적인 차이를 보였는데, 수분첨가량이 감소함에 따라 저장기간에 따른 수분의 손실로 황색도는 증가하고 명도는 감소하였다. 물성특성치는 저장기간이 증가함에 따라 그 값이 증가하여 떡이 단단해 졌는데, 35∼45%의 수분첨가구가 저장 72시간째까지 일정한 값을 나타내어 물성적으로 가장 안정하였다. 저장기간에 따른 노화속도는 35% 수분 첨가구는 노화가 다른 시험구에 비해서 가장 천천히 진행되는 것으로 나타났다. 관능검사 결과 35∼45% 수분첨가구를 가장 선호하였다. 노화속도가 느린 35% 수분첨가구가 관능적으로도 우수하여 본 실험에서 가장 알맞은 수분첨가량으로 설정할 수 있었다.

• Journal of Ceramic Processing Research
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• 제20권1호
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• pp.63-68
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• 2019

We investigated the effects of Al2O3 addition on (1-x)Li2B4O7-xAl2O3 (LBAO; x = 0, 0.005, 0.01, 0.05, 0.07, and 0.1) glasses. The glasses were synthesized by a conventional melt-quench method. Structural transformations of the LBAO glasses were assessed via X-ray diffraction analysis. Estimations of ΔT, KGS = (Tc-Tg)/(Tm-Tc), activation energy, and the Avrami parameter were performed using differential thermal analysis and differential scanning calorimetry. An interpretation of non-isothermal kinetics of the crystallization process is presented using the modified Ozawa equation. The activation energy E increased from 3.3 to 3.5 eV for the LBAO (x < 0.01) glasses whereas those of the LBAO (x > 0.05) glasses slightly increased from 3.75 to 4.05 eV. The exponent n was estimated to be 3.9 ± 0.1 for the LBAO (x < 0.01) glasses and 3.2 ± 0.02 for the LBAO (x > 0.05) glasses. Microstructural characterization of the glassy and crystalline phases using atomic force microscopy was investigated. The effects of Al2O3 on the LBAO glasses include a decreased nucleation rate in the crystallization process and a significantly reduced crystal size.

• 한국소성가공학회:학술대회논문집
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• 한국소성가공학회 2001년도 추계학술대회 논문집
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• pp.293-296
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• 2001

The dynamic softening mechanisms of AISI 316, AISI 304 and AISI 430 stainless steels were studied with torsion test in the temperature range of $900 - 1200^{\circ}C$ and the strain rate range of $5.0x10^{-2}-5.0x10^0/sec$. The austenitic stainless steels, such as AISI 316 and AISI 304 were softened by dynamic recrystallization (DRX) during hot deformation. Also, the evolutions of flow stress and microstructure of AISI 430 ferritic stainless steel show the characteristics of continuous dynamic recrystallization (CDRX). To establish the quantitative equations for DRX of AISI 316 stainless steel, the evolution of flow stress curve with strain was analyzed. The critical strain (${\varepsilon}_c$) and strain for maximum softening rate (${\varepsilon}^{*}$) could be confirmed by the analysis of work hardening rate ($d{\sigma}/d{\varepsilon}={\theta}$). The volume fraction of dynamic recrystallization ($X_{DRX}$) as a function of processing variables, such as strain rate ( $\varepsilon$ ), temperature (T), and strain ( $\varepsilon$ ) were established using the ${\epsilon}_c$ and ${\varepsilon}^{*}$. For the exact prediction the ${\varepsilon}_c,\;{\varepsilon}^{*}$ and Avrami' exponent (m') were quantitatively expressed by dimensionless parameter, Z/A, respectively. It was found that the calculated results were agreed with the experimental data for the steels at my deformation conditions. Also, we can reasonably conclude that the DRX, CDRX and grain refinement of stainless steels can be achieved by large strain deformation at high Z parameter condition.