• 제목/요약/키워드: Inverse pole figure

검색결과 7건 처리시간 0.018초

Application of Inverse Pole Figure to Rietveld Refinement: II. Rietveld Refinement of Tungsten Liner using Neutron Diffraction Data

  • Kim, Yong-Il;Lee, Jeong-Soo;Jung, Maeng-Joon;Kim, Kwang-Ho
    • The Korean Journal of Ceramics
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    • 제6권3호
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    • pp.240-244
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    • 2000
  • The three-dimensional orientation distribution function of a conical shaped tungsten liner prepared by the thermo-mechanical forming process was analyzed by 1.525$\AA$ neutrons to carry out the Rietveld refinement. The pole figure data of three reflections, (110)(220) and (211) were measured. The orientation distribution functions for the normal and radial directions were calculated by the WIMV method. The inverse pole figures of the normal and radial directions were obtained from their orientation distribution functions. The Rietveld refinement was performed with the RIETAN program that was slightly modified for the description of preferred orientation effect. We could successfully do the Rietveld refinement of the strongly textured tungsten liner by applying the pole density of each reflection obtained from the inverse pole figure to the calculated diffraction pattern. The correction method of preferred orientation effect based on the inverse pole figures showed a good improvement over the semi-empirical texture correction based on the direct usage of simple empirical functions.

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Application of Inverse Pole Figure to Rietveld Refinement: I. Rietveld Refinement of Copper Sheet using X-ray Diffraction Data

  • Kim, Yong-Il;Jung, Maeug-Joon;Kim, Kwang-Ho
    • The Korean Journal of Ceramics
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    • 제6권3호
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    • pp.236-239
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    • 2000
  • Both the X-ray diffraction data of the normal direction in the sample orientation and the pole figure data of three reflections, (111), (200) and (220), were used to do the Rietveld refinement for the copper sheet prepared by a cold rolling process. The agreement between calculated and observed patterns was not satisfactory, which was attributed to the preferred orientation effect of the copper sheet. The Rietveld refinement for the copper sheet could be done successfully by applying the pole density of each reflection obtained from the corresponding inverse pole figure to the X-ray diffraction data of the normal direction. The R-weighted pattern, $R_{wp}$ was 12.99% and the goodness-of-fit indicator, S, was 3.68.

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Application of Inverse Pole Figure to Rietveld Refinement: III. Rietveld Refinement of $SnO_2$ Thin Film using X-ray Diffraction Data

  • Kim, Yong-Il;Jung, Maeng-Joon;Kim, Kwang-Ho
    • The Korean Journal of Ceramics
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    • 제6권4호
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    • pp.354-358
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    • 2000
  • The SnO$_2$film was deposited on a corning glass 1737 substrate by plasma enhanced chemical vapor deposition using a gas mixture of SnCl$_4$, $O_2$, and Ar. The film thickness was measured using $\alpha$-step and was about 9400$\AA$. The conventional X-ray diffractometry and pole figure attachment were used to refine the crystal structure of SnO$_2$ thin film. Six pole figures, (200), (211), (310), (301), (321), and (411), were measured with CoK$_\alpha$ radiation in reflection geometry. The X-ray diffraction data were measured at room temperature using CuK$_\alpha$ radiation with graphite monochromator. The agreement between calculated and observed patterns for the normal direction of SnO$_2$ thin film was not satisfactory due to the severely preferred orientation effect. The Rietveld refinement of heavily textured SnO$_2$ thin film was successfully achieved by adopting the pole density distribution of each reflection obtained from the inverse pole figure as a correction factor for the preferred orientation effect. The R-weighted pattern, R$_wp$, was 15.30%.

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제어 압연과 가속 냉각에 의해 저탄소강에서 형성되는 미세조직의 특징과 구분 (Microstructure Characteristics and Identification of Low-Carbon Steels Fabricated by Controlled Rolling and Accelerated Cooling Processes)

  • 이상인;홍태운;황병철
    • 한국재료학회지
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    • 제27권11호
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    • pp.636-642
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    • 2017
  • In the present study the microstructure of low-carbon steels fabricated by controlled rolling and accelerated cooling processes was characterized and identified based on various microstructure analysis methods including optical and scanning electron microscopy, and electron backscatter diffraction(EBSD). Although low-carbon steels are usually composed of ${\alpha}-ferrite$ and cementite($Fe_3C$) phases, they can have complex microstructures consisting of ferrites with different size, morphology, and dislocation density, and secondary phases dependent on rolling and accelerated cooling conditions. The microstructure of low-carbon steels investigated in this study was basically classified into polygonal ferrite, acicular ferrite, granular bainite, and bainitic ferrite based on the inverse pole figure, image quality, grain boundary, kernel average misorientation(KAM), and grain orientation spread(GOS) maps, obtained from EBSD analysis. From these results, it can be said that the EBSD analysis provides a valuable tool to identify and quantify the complex microstructure of low-carbon steels fabricated by controlled rolling and accelerated cooling processes.

Study of the Microstructural Evolution of Tempered Martensite Ferritic Steel T91 upon Ultrasonic Nanocrystalline Surface Modification

  • He, Yinsheng;Yang, Cheol-Woong;Lee, Je-Hyun;Shin, Keesam
    • Applied Microscopy
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    • 제45권3호
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    • pp.170-176
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    • 2015
  • In this work, various electron microscopy and analysis techniques were used to investigate the microstructural evolution of a 9% Cr tempered martensite ferritic (TMF) steel T91 upon ultrasonic nanocrystalline surface modification (UNSM) treatment. The micro-dimpled surface was analyzed by scanning electron microscopy. The characteristics of plastic deformation and gradient microstructure of the UNSM treated specimens were clearly revealed by crystal orientation mapping of electron backscatter diffraction (EBSD), with flexible use of the inverse pole figure, image quality, and grain boundary misorientation images. Transmission electron microscope (TEM) observation of the specimens at different depths showed the formation of dislocations, dense dislocation walls, subgrains, and grains in the lower, middle, upper, and top layers of the treated specimens. Refinement of the $M_{23}C_6$ precipitates was also observed, the size and the number density of which were found to decrease as depth from the top surface decreased. The complex microstructure and microstructural evolution of the TMF steel samples upon the UNSM treatment were well-characterized by combined use of EBSD and TEM techniques.

B,Nb 및 Ti 를 함유한 극저탄소강에서 탄화물 및 질화물의 석출이 집합조직에 미치는 영향(I)-집합조직과 기계적 성질- (Effects of the Precipitation of Carbides and Nitrides on the Textures in Extra Low Carbon Steel Sheets containing B, Nb and Ti(l))

  • 이종무;윤국한;이도형
    • 한국재료학회지
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    • 제3권1호
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    • pp.43-49
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    • 1993
  • AI킬드한 극저탄소강에 Ti, Nb등의탄화물 또는 질화물 형성원소를 첨가하면 우수한 디프드로잉특성과 내시효성을 나타내는 강판을 얻을 수 있다고 알려져 있으므로 본 연구에서는 Ti및 Nb를 단독 또는 동시에 첨가하거나 B를 추가로 첨가한 고강도 극저탄소 강판을 제조하여 각각의재결정 집합조직과 기계적 성질을 측정비교하여 보았다. 역극점도에 나타난 집합조직강도의 변화를 조사한 결과 어닐링처리에 의하여 (100)면 강도와 (111)면 강도의 변화가 가장 많이 나타난 것은 Nb첨가강이며, Nb와 Ti를 단독으로 첨가한 강과 Ti를 단독으로 첨가한 강은 변화정도가 비슷하였다.극점도를 비교하면,Nb와 Ti를 동시에 첨가한강, Nb를 단독으로 첨가한 강 그리고 Ti를 단독으로 첨가한강 모두 냉간 압연한 상태에서는{112}<110>집합조직이 발달하였으며 어닐링처리한 후에는 {111}<112>집합조직이 잘 발달하였다. 그러나 세 종류의 강간에 집합조직의 차이는 별로 없었다. 결정립도와 관계가 깊은 경도에서는 결정립도가 가장 작은 Nb 및 Ti동시첨가강에서 경도가 가장 높고, Nb단독첨가강, Ti단독첨가강의 순서로 감소하는 경향을 보였다.

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수소취화된 스테인리스강 316L의 VHCF(Very High Cycle Fatigue) 피로특성과 UNSM 효과에 관한 연구 (Study on VHCF Fatigue Behaviors and UNSM Effects of Hydrogen Attacked STS 316L)

  • 남승훈;백운봉;서창민;편영식
    • 대한기계학회논문집A
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    • 제41권11호
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    • pp.1011-1020
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    • 2017
  • 본 연구는 실온에서 미처리재와 UNSM처리재, 수소취화재(100 bar, $300^{\circ}C$에서 120 h) 및 이 수소취화재의 UNSM처리재의 스테인리스강 316L 시험편의 재료특성파악을 위한 실험을 실시하였다. 여기서 수소취화재는 기존의 미처리재의 S-N곡선보다 피로강도가 약간 감소하는 경향을 나타내었으며, 수소취화효과는 적게 나타났다. 미처리재에 비해서 UNSM처리재의 피로한도는 약 43.8 % 상승하였고, 수소취화재의 UNSM처리재는 수소취화재보다 약 57.1 % 상승하는 경향을 나타내었다. EBSD에 의한 IQ, IPF 및 KAM 맵에서 UNSM처리 후, 이 처리의 영향을 받는 나노 입자 표면층의 두께는 약 $152{\mu}m$이다. 그러나 세 가지 맵에서 수소취화의 깊이 영향을 정량적으로 평가할 수 없었다. 시험편상에서 발생하는 표면균열은 수소취화의 영향으로 평균입경($35{\mu}m$)보다 작은 균열의 비율이 약 90 %를 차지하였다.