• Title/Summary/Keyword: 원소치환

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Magnetic Properties of Zn and La-Zn Substituted Strontium Ferrite (Zn 및 La-Zn 치환에 따른 Sr 페라이트의 자기적 특성에 관한 연구)

  • 장세동;김종오;김종희
    • Journal of the Korean Magnetics Society
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    • v.11 no.6
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    • pp.256-261
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    • 2001
  • These experiments were carried out to examine the effects of element substitution of Zn and La-Zn for Sr-ferrite. The calcined properties of Zn and La-Zn element substitution were examined, and also the sintered magnetic properties were compared with the stoichiometric condition. The magnetization properties of calcined SrM materials is as follows; M$\_$s/ : 61.06 emu/g. Also, the magnetization properties of calcined Zn$\_$0.3/-SrM materials is as follows; M$\_$s/ : 66.90 emu/g. The sintered magnetic properties of (La-Zn)$\_$0.3/-SrM composition is as follows; B$\_$r/ : 4.21 kG, BH$\_$max/: 4.19 MGOe.

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A Historical Note on Permutation Polynomials over Finite Fields (유한체상의 치환다항식에 관한 역사적 고찰)

  • Park Hong Goo
    • Journal for History of Mathematics
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    • v.18 no.2
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    • pp.117-126
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    • 2005
  • In this paper, we analyze the basic concepts of permutation polynomials over finite fields, and the historical background through the use of the major classes of permutation polynomials over the fields. And also, we find a method of the polynomial representation with respect to cycles on the fields.

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A Design of Circuit for Computing Multiplication in Finite Fields GF($2^m$) (유한체 GF($2^m$)상의 승산기 설계에 관한 연구)

  • 김창규;이만영
    • The Journal of Korean Institute of Communications and Information Sciences
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    • v.14 no.3
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    • pp.235-239
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    • 1989
  • A multiplier is proposed for computing multiplication of two arbitrary elements in the finite fields GF($2^m$), and the operation process is described step by step. The modified type of the circuit which is constructed with m-stage feedgack shift register, m-1 flip-flop, m AND gate, and m-input XOR gate is presented by referring to the conventional shift-register multiplier. At the end of mth shift, the shift-register multiplier stores the product of two elements of GF($2^m$); however the proposed circuit in this paper requires m-1 clock times from first input to first output. This circuit is simpler than cellulra-array or systolic multiplier and moreover it is faster than systolic multiplier.

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Electromagetic Wave Absorbing Properties of $Ni_{0.5}-Zn_{0.4}-X_{0.1}{\cdot}Fe_2O_4$(X=Cu, Mg, Mn)-Rubber Composite ($Ni_{0.5}-Zn_{0.4}-X_{0.1}{\cdot}Fe_2O_4$(X=Cu, Mg, Mn)-Rubber Composite의 전파흡수특성에 관한 연구)

  • Im, Hui-Dae;Yun, Guk-Tae;Lee, Chan-Gyu
    • Korean Journal of Materials Research
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    • v.9 no.12
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    • pp.1234-1239
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    • 1999
  • Electromagnetic wave asorbing properties of the $Ni_{0.5}-Zn_{0.4}-X_{0.1}{\cdot}Fe_2O_4$, where X was replaced by substitution elements Cu, Mg, Mn, have been studied. The structure, shape, size and magnetic properties of the $Ni_{0.5}-Zn_{0.4}-X_{0.1}{\cdot}Fe_2O_4$ were analyzed by XRD, SEM, VSM. The relative complex permittivity, permeability, and electromagnetic wave absorbing properties were measured by Network Analyzer. The structure, shape, size and magnetization value of the $Ni_{0.5}-Zn_{0.4}-X_{0.1}{\cdot}Fe_2O_4$ were found to be similar in spite of substitution elements. The coercive force and hysteresis-loss showed maximum value when Mg was substituted for X. The dielectric loss(${\varepsilon}_r"/{\varepsilon}_r'$) was found to be maximum value when Mn was substituted for X. Also the magnetic loss(${\mu}_r"/{\mu}_r'$} was found to be maximum with Cu substitution. The electromagnetica wave absorbing property of the $Ni_{0.5}-Zn_{0.4}-X_{0.1}{\cdot}Fe_2O_4$-Rubber composite with 4mm thickness was excellent as over - 40dB at 9GHz, and the $Ni_{0.5}-Zn_{0.4}-X_{0.1}{\cdot}Fe_2O_4$-Rubber composite with 8mm thickness was over-40dB at 2GHz. Those composites also showed superior microwave absorbing properties.

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Phase Relation in the System Pt-Sb-Bi at $600^{\circ}C$ and Their Mineralogical Implication ($600^{\circ}C$에서의 백금-안티모니-비스머스계 상평형 관계 및 광물학적 의의)

  • 김원사;이석훈
    • Journal of the Mineralogical Society of Korea
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    • v.13 no.1
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    • pp.44-52
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    • 2000
  • 천연에서 발견되는 geversite (PtSb2), stumpflite (PtSb), insizwaite (PtBi2), unnamed PtBi 등의 광물에 대한 안정영역과 원소치환에 따른 고용체 존재를 규명하기 위해 백금-안티모니-비스머스 등 3성분계에 대한 합성실험적 연구를 실시하였다. 이번 연구에서 설정된 $600^{\circ}C$ 온도의 실험결과에 의하면, 등축정계의 geversite와 insizwaite 사이에 완전고용체가 형성되며, Sb를 치환하는 Bi의 함량에 따라 단위포 상수는 6.4415(0 at.%), 6.4361(15 at.%), 6.5204(30 at.%), 6.5411(51 at.%), 6.6261(70 at%), 6.6540(85 at%), 6.728$\AA$(100 at.%)로 증가함을 알 수 있었다. 육방정계인 stumpflite와 unnamed PtBi 사이에도 완전고용체가 형성되며, Sb를 치환하는 Bi의 함량이 증가함에 따라 a 단위포 상수의 크기는 4.1388(0 at.%), 4.2118(20 at.%), 4.2118(40 at.%), 4.2485(80 at.%), 4.3242$\AA$(100 at.%)등 연속적으로 증가하지만, c 단위포 상수는 각각 5.4902, 5.4799, 5.508, 5.4817, 5.5045$\AA$등 불규칙하게 변함을 알 수 있었다. 0~33.33 at.% Pt 영역에서의 상평형 관계는 액체가 Pt(Sb,Bi)2 고용체와 공존하고 있고, Sb가 많이 함유된 액체에서는 geversite+원소광물 안티모니+백금이 거의 함유되지 않은 액체와 공생하는 3-phase assemblage를 형성한다. 자연계에서는 geversite와 insizwaite 및 stumpflite와 unnamed PtBi 사이의 화학조성을 가지는 광물이 발견되고 있는데, 이들은 각각 독립적인 광물종이 아니라 위 광물들의 고용체에 속하는 것임을 알 수 있었다. 이들 광물을 명명하고 해석하는데 매우 세심한 주의가 필요함을 알 수 있었다. 또한 단위포 상수를 측정을 통해 해당 고용체 광물의 Sb↔Bi 치환 양을 추정할 수 있다는 점과 광물 공생관계를 통해 생성온도를 추정할 수 있다는 사실을 알 수 있었다.

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Factors Affecting Hydrogen Induced Amorphization of ErCo2 C15 Laves Compound (ErCo2 C15 Laves 화합물의 수소유기 비정질화에 영향을 미치는 인자)

  • Yong, Y.J.;Lee, J.Y.
    • Transactions of the Korean hydrogen and new energy society
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    • v.4 no.2
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    • pp.17-22
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    • 1993
  • $ErCo_2$화합물에서 Co를 천이원소로 10%만큼 치환한 $Er(Co_{0.9}M_{0.1})_2$화합물(M=Cr, Mn, Fe, Ni, Cu)의 비정질화 온도를 측정해서 수소유기 비정질화에 영향을 미치는 인자에 대해 살펴보았다. 비정질화 온도는 치환원소의 원자반경과 비례함을 알 수 있었다 그러므로 $ErCo_2$ Laves 화합물에서 수소유기 비정질화에 영향을 미치는 인자는 확산과 밀접한 연관이 있는 원자의 크기임을 알 수 있다.

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Evaluation of Creep Properties of W-substituted 2205 Duplex Stainless Steel (W치환 2205 이상 스테인리스강의 크리프 특성 평가에 관한 연구)

  • Kim, Gi-Yeob;Choi, Byong-Ho;Nam, Ki-Woo;Ahn, Yong-Sik
    • Journal of the Korean Society for Nondestructive Testing
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    • v.24 no.1
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    • pp.29-37
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    • 2004
  • The effect of the substitution of Tungsten(W) for Molybdenum(Mo) on the creep behaviour of 22Cr-5Ni duplex stainless steel(DSS) has been investigated. Creep tests were carried out at $600^{\circ}C\;and\;650^{\circ}C$. Intermetallic ${\sigma}$ phase is precipitated during creep at $650^{\circ}C$, at which creep rupture time was much lower compared with at $600^{\circ}C$. The substitution of W for Mo in the duplex stainless steel was known to retard the formation of ${\sigma}$ phase. Minimum creep rate and creep rupture time, however, were hardly influenced by the substitution of 2wt.% W. An ultrasonic measurement for the creep specimens has been carried out for the evaluation of creep damage. The sound velocity increases propotionally with the increase of creep rupture time at $600^{\circ}C$ of creep temperature. On the contrary, the sound velocity decreases with the increase of rupture time at $650^{\circ}C$, which can be correlated with the microstructural evolution during creep.