• Title/Summary/Keyword: Lamellar structure

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$Bi_2Te_3-PbTe$계 열전소재의 자연나노구조체 형성 및 특성

  • Im, Ju-Hyeok;Jeong, Gyu-Ho;Kim, Gwang-Cheon;Yu, Hyeon-U;Kim, Jin-Sang
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2009.11a
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    • pp.263-263
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    • 2009
  • The microtstructures and properties of alloys in the pseudo-binary $Bi_2Te_3-PbTe$ system were investigated as a first step towards the design of nanostructured materials with enhanced thermoelectric properties. The liquid alloys were cooled by water quenching method. Dendritic and lamellar structures were observed clearly by using environmental scanning electron microscope(eSEM) and electron probe micro analyzer(EPMA) take into account composition ratio between $Bi_2Te_3$ and PbTe. The compound $Pb_2Bi_6Te_{11}$ precipitated as a metastable phase under all conditions. The structure of those samples changed from dendritic to lamellar by increasing $Bi_2Te_3$ ratio of composition.

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Comparative study on the Spermatogenesis of two kinds of Korean planarias, Dugesia japonica and Phagocata vivida (한국산 플라나리아 Dugesia japonica와 Phagocata vivida 두종 사이의 정자 형성에 관한 비교연구)

  • Chang, Nam-Sub
    • Applied Microscopy
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    • v.22 no.2
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    • pp.75-83
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    • 1992
  • Comparative study on the spermatogenesis of two kinds of Korean planarias, Dugesia japonica and Phagocata vivida, were studied with light and electron microscope. Observation results were as follows. Except following details, fine structure and morphogenesis of the spermatogonia, primary spermatocyte, secondary spermatocyt spermatid and spermatozoon were consistant between the two species. The nucleus of primary spermatocyte of Dugesia japonica was surrounded with 36-38 microtubules, while that of Phagocata vivida with 40-42 microtubules. The C-shaped lamellar Golgi complex appeared in the spermatid cytoplasm of the former, while Straight-shaped lamellar Golgi complex in that of the latter. The four white spots were observed only in the nucleoplasm of matured spermatozoon in the latter, not in the former.

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A Study of Electro-Deposition for Pb-Sn-Cu Alloy System (연-주석-동계 합금속도에 관한 연구)

  • Kang, T.;Cho, C. S.;Yum, H. T.
    • Journal of the Korean institute of surface engineering
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    • v.4 no.1
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    • pp.16-23
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    • 1971
  • In this study , fluoborte solution consisting of lead fluoborate, tin fluoborate and cupric acetate was used. By addition of small amount of Cu+= ion to the solution, the Cu content of deposition layer was almost controlled less than 5%. The amount of Cu in deposition layer was almost constant without any influence of Pb++ & Sn++ in the solution, and the amount of Pb was increased by the increase of total concentration of Pb++ +Sn++ in the solution, and the amount of Pb was increased by the increase of total concentration of Pb++ +Sn++ in the solution . Agitation of plating solution & low current density result in the increase of Cu content. Analyzing of microscopic structures and etching tests of the deposited alloy, it was believed that the alloy had a lamellar structure consisting of copper rich lamellar and lead rich layer.

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Analysis of Rate Equation for Spherodization of Cold Rolled Lamellar Pearlite Structure (가공된 층상조직의 구상화 속도의 해석)

  • Wey, Myeong Yong
    • Journal of the Korean Society for Heat Treatment
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    • v.4 no.2
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    • pp.1-8
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    • 1991
  • The spheroidization of cold rolled lamellar pearlite in annealing at the temperatures between 600 and $700^{\circ}C$ has been studied by quantitative micrography. It was foud that the spheroidization proceeded as two stageh. The first stage was the stage of relieving the stored energy by cold work, the second was the stage of reducing the interface energy between ferrite and cementite. The spheroidization rate combining the spheroidization rate of each stages is described by the following equation : $$d(1/S)/dt=k_3{\cdot}D/_{(1/s)}\{{\sigma}V/_{(1/s)}+k_4{\cdot}{\exp}(-bt)\}$$ Where, S is the total area of the interface between ferrite and cementite per unit volume, D is the diffusion coefficient, ${\sigma}$ is the boundary energy, V is the volume fraction of the cementite, and $k_3$, $k_4$, b are constants.

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Comparison of the Crystallization Behavior of Syndiotactic Polypropylene and Isotactic Polypropylene (신디오택틱 폴리프로필렌과 아이소택틱 폴리프로필렌의 결정화 거동 비교)

  • Lee, Sang-Won;Huh, Wan-Soo;Hyun, Uk;Lee, Dong-Ho;Noh, Seok-Kyun
    • Polymer(Korea)
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    • v.27 no.6
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    • pp.509-520
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    • 2003
  • The study was made to compare the crystallization behavior of polypropylene (PP) with different stereo-regularity. The unit cell parameters, lamellar structure of PP, and the growth of thieir spherulites were strongly dependent upon the crystallization condition. It was shown that metastable structure appeared with increasing cooling rate. The structural change of isotactic PP (iPP) was larger than that of syndiotactic PP (sPP). The crystal structure of sPP showed body centered cell III when it is cooled down with 1 $^{\circ}C$/min. When sPP was grown to primitive cell II structure, both unit cell and lamellar structure were less affected by a cooling rate. The overall crystallization rate of ipp was faster than that of sPP.

Sensitivity Appraisal for Lamellar Tearing of Box-Column of Ultra Thick Plate (극후판 Box-Column의 Lamellar 균열 감수성 평가)

  • 노찬승;박창수;김흥주;방한서;이창우
    • Journal of Ocean Engineering and Technology
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    • v.17 no.4
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    • pp.31-36
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    • 2003
  • In case of this thick rolling-steel for a multistory building, a large oil-drilling structure, a large vessel, a bridge and so on, Lamella Tearing around the welded joint zone is the most serious problems. In order to prevent Lamella Tearing, not only is choice of material important, but also the comprehensive investigation for the structural design and the construction. The Lamella Tearing that is a staircase-shape occurs due to the contraction stress to the thickness direction of the plate and has the character that the cracks progress along the elongated inclusion by rolling. In general, because cracks occur at the heat affected zone and around HAZ, it is necessary to establish the safety and the confidence of the welded structure to restrain the welding defect such as Lamella Tearing. The mechanical approaches are the easier and more economical than the approaches of the material and the construction method. In addition, the appropriate welding profile and the optimum welding condition contribute toward the improvement of the productivity and influence on the standardization of the manufacturing technology.

The Ordered Structures of Poly(styrene-b-4vinylpridine)s

  • Pak, Soo-Young;Sul, Woo-Hwan;Chang, Yun-Jeong
    • Proceedings of the Polymer Society of Korea Conference
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    • 2006.10a
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    • pp.191-191
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    • 2006
  • The structures of the mesophases and their subunits of PS-b-P4VP in a toluene solution were studied by using SAXS, TEM and GIFT methods. The hierarchical structures of PS-b-P4VP, such as the individual micelle, the face-centered cubic (fcc) and body-centered cubic (bcc) structures and the lamellar structure, were identified for the first time. The diameter of the micelle core was ${\sim}80\;%$ of the most extended chain length of the core chain, suggesting that the core chains were quite stretched. The stretched chain in the core caused the core of the micelle to be not homogenous with a higher density at the center than at the outer part. As the concentration level increases, the fcc and both fcc and bcc appear for the packing of the micelles of PS(3.3k)-b-P4VP(4.7K) and PS(12K)-b-P4VP(11.8K), respectively. The lamellar structure was also identified, with a further increase in the concentration for PS(3.3k)-b-P4VP(4.7K). These hierarchical structures were also identified via TEM images.

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Changes in Hardness and Thermal Conductivity with Volume Fraction of Discontinuous Precipitates in Mg-Al Alloy (Mg-Al 합금에서 불연속 석출물의 부피 분율에 의한 경도 및 열전도도의 변화)

  • Jun, Joong-Hwan
    • Journal of the Korean Society for Heat Treatment
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    • v.34 no.6
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    • pp.302-308
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    • 2021
  • The aim of this study was to investigate the dependence of the hardness and thermal conductivity on the volume fraction of discontinuous precipitates (DPs) in the Mg-9.3%Al alloy with (α-(Mg)+DPs) dual phase structure. In order to obtain various DPs volume fractions, the alloy was solution-treated at 688 K for 24 h and then aged at 418 K for up to 144 h. The volume fraction of DPs increased from 0% to 63% with an increase in the aging time up to 72 h, over which, continuous precipitation was observed within the α-(Mg) grains. It is noticeable that the hardness and thermal conductivity of the alloy increased linearly with the volume fraction of DPs. The improved hardness and thermal conductivity with respect to volume fraction of DPs are closely associated with the higher hardness of the DPs with fine (α+β) lamellar structure and the lower Al concentration in the α phase layer of the DPs, respectively.

Lamellar Structured TaN Thin Films by UHV UBM Sputtering (초고진공 UBM 스퍼터링으로 제조된 라멜라 구조 TaN 박막의 연구)

  • Lee G. R.;Shin C. S.;Petrov I.;Greene J, E.;Lee J. J.
    • Journal of the Korean institute of surface engineering
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    • v.38 no.2
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    • pp.65-68
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    • 2005
  • The effect of crystal orientation and microstructure on the mechanical properties of $TaN_x$ was investigated. $TaN_x$ films were grown on $SiO_2$ substrates by ultrahigh vacuum unbalanced magnetron sputter deposition in mixed $Ar/N_2$ discharges at 20 mTorr (2.67 Pa) and at $350^{\circ}C$. Unlike the Ti-N system, in which TiN is the terminal phase, a large number of N-rich phases in the Ta-N system could lead to layers which had nano-sized lamella structure of coherent cubic and hexagonal phases, with a correct choice of nitrogen fraction in the sputtering mixture and ion irradiation energy during growth. The preferred orientations and the micro-structure of $TaN_x$ layers were controlled by varing incident ion energy $E_i\;(=30eV\~50eV)$ and nitrogen fractions $f_{N2}\;(=0.1\~0.15)$. $TaN_x$ layers were grown on (0002)-Ti underlayer as a crystallographic template in order to relieve the stress on the films. The structure of the $TaN_x$ film transformed from Bl-NaCl $\delta-TaN_x$ to lamellar structured Bl-NaCl $\delta-TaN_x$ + hexagonal $\varepsilon-TaN_x$ or Bl-NaCl $\delta-TaN_x$ + hexagonal $\gamma-TaN_x$ with increasing the ion energy at the same nitrogen fraction $f_{N2}$. The hardness of the films also increased by the structural change. At the nitrogen fraction of $0.1\~0.125$, the structure of the $TaN_x$ films was changed from $\delta-TaN_x\;+\;\varepsilon-TaN_x\;to\;\delta-TaN_x\;+\;\gamma-TaN_x$ with increasing the ion energy. However, at the nitrogen fraction of 0.15 the film structure did not change from $\delta-TaN_x\;+\;\varepsilon-TaN_x$ over the whole range of the applied ion energy. The hardness increased significantly from 21.1 GPa to 45.5 GPa with increasing the ion energy.

Microstructures and Thermal Properties of Water Quenched Thermoelectric Material in Bi2Te3-PbTe System (급속 응고 된 Bi2Te3-PbTe계 열전소재의 미세구조와 열전 특성)

  • Yim, Ju-Hyuk;Jung, Kyoo-Ho;You, Hyun-Woo;Kim, Kwang-Chon;Kim, Jin-Sang
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.23 no.6
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    • pp.502-507
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    • 2010
  • In order to design nano structured materials with enhanced thermoelectric properties, the alloys in the pseudo-binary $Bi_2Te_3$-PbTe system are investigated for their micro structure properties. For this synthesis, the liquid alloys are cooled by the water quenching method. Micro structure images are obtained by using an electron probe micro analyzer(EPMA). Dendritic and lamellar structures are clearly observed with the variation in the composition ratio between $Bi_2Te_3$ and PbTe. The increase in the $Bi_2Te_3$ composition ratio causes to change of the structure from dendritic to lamellar. The Seebeck coefficient of sample 5, in which the mixture rate of $Bi_2Te_3$ is 83%, is measured as the highest value. In contrast, the others decrease with the increase of the $Bi_2Te_3$ composition ratio. Meanwhile, p-type characteristics are observed in sample 6, at 91%-$Bi_2Te_3$ mixture rate. The power factors of the all samples are calculated with the Seebeck coefficient and resistivity.