日本金属学会誌
Online ISSN : 1880-6880
Print ISSN : 0021-4876
ISSN-L : 0021-4876
80 巻, 6 号
選択された号の論文の9件中1~9を表示しています
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論文
  • 齋藤 繁, 高島 敏行, 見山 克己, 成田 敏夫
    2016 年 80 巻 6 号 p. 350-354
    発行日: 2016年
    公開日: 2016/05/25
    [早期公開] 公開日: 2016/04/15
    ジャーナル フリー
     Formation of diffusion-barrier coating system with two-layered structure has been developed. The system comprises an inner χ-phase of the Re-Cr-Nb system as a diffusion-barrier layer and an outer Al-reservoir layer. In this study, Re film was formed on Nb substrate via electroplating and the film changed into χ-Re3Nb phase by preliminary heat treatment at 1500℃ for 1 h. Cr-pack cementation was conducted under vacuum of 10−5 Pa at 1300℃ and 1400℃ for 6 min and 1 h, respectively, using an Al2O3 crucible in which the specimens were buried in a powder mixture of pure Cr and Al2O3. The packed specimens were examined using an electron probe microanalyzer to determine the concentration profile of each element. The layer structure of the film on the Nb substrate after the Cr-pack cementation was discussed on the basis of composition paths plotted in the Re-Cr-Nb phase diagram.
      In the case of the specimen induced by Cr-pack cementation at 1300℃ for 6 min, the alloy layers in the Re-Cr-Nb system consists of the γ, Re-rich, χ and α phases. In the case of the specimen induced by Cr-pack cementation at 1300℃ for 1 h and 1400℃ for 6 min, the alloy layers in the Re-Cr-Nb system consisted of the γ, χ and α phases. By contrast, in the specimen induced by Cr-pack cementation at 1400℃ for 1 h, the alloy layers in the Re-Cr-Nb system consists of the γ, Nb(Cr, Re)2 and α phases.
  • 上田 恵輔, 久保 智愛, 神田 昌枝, 西 義武
    2016 年 80 巻 6 号 p. 355-359
    発行日: 2016年
    公開日: 2016/05/25
    ジャーナル フリー
     2-layer laminated sheets (PP/PA6) with polypropylene (PP) and nylon 6(PA6) were prepared by applying low dose homogeneous low energy electron beam irradiation (HLEBI) prior to hot-press under 10 MPa, 403 K and 3 min. Although the adhesion of the PP/PA6 was often observed with a weak hot-press without HLEBI, the HLEBI (≦1.29 MGy) induced adhesion raised the bonding forces as evidenced by using the adhesive forces of peeling resistance (oFp). Based on the 3-parameter Weibull equation, the lowest oFp value at peeling probability (Pp) of zero (Fs) could be estimated. An increasing trend in Fs occurred by applying HLEBI up to 0.64 MGy reaching a maximum at 21.98 Nm−1, improving the safety level without radiation damage. When HLEBI cut the chemical bonds in PP polymer and generated not-terminated atoms having dangling bonds, they probably induced the chemical bonding. Thus, increasing adhesion force between the laminated sheets could be explained.
  • 奥原 雅也, 野村 良, 西 義武
    2016 年 80 巻 6 号 p. 360-364
    発行日: 2016年
    公開日: 2016/05/25
    [早期公開] 公開日: 2016/05/13
    ジャーナル フリー
     Homogeneous low energy electron beam irradiation (HLEBI) to surface mostly improved the bending elastic modulus (b(dσ/dε)i) and tensile stiffnesst (t(dσ/dε)i) of composites sheets of glass fiber reinforced thermoplastic polypropylene (GFRTP). Although increasing dose of HLEBI decayed the ductility, optimal dosage of HLEBI from 0.22 to 0.86 MGy often improved the tensile strength (tσb) of the GFRTP with smaller variation in the data than untreated one. Based on the three parameter Weibull equation, the tσb at the lowest cummulative probability of fracture (Pf=zero) was estimated and defined as the lowest tensile strength (tσs). The highest tσs value estimated was 54 MPa for GFRTP irradiated at 0.65 MGy. Strengthening of both glass fiber and polypropylene, as well as their interfacial friction force mainly contributed to the results.
  • 野﨑 安衣, Somchuen Kittima, 谷原 康友, 桑原 泰隆, 大道 徹太郎, 亀川 孝, 森 浩亮, 山下 弘巳
    2016 年 80 巻 6 号 p. 365-369
    発行日: 2016年
    公開日: 2016/05/25
    [早期公開] 公開日: 2016/04/28
    ジャーナル フリー
     The catalytic performances of skeletal Cu prepared from Cu-Ti amorphous alloy heated at various temperatures were tested for the hydrogen generation from ammonia borane. The catalytic activity per surface area decreased with increasing heating temperatures of Cu-Ti amorphous alloy. The thermal treatment of Cu-Ti amorphous alloy leads to the high surface area of skeletal Cu. A skeletal Cu catalyst prepared from heated Cu-Ti amorphous alloy at 300℃ which is a moderate temperature somewhat lower than crystallization temperature, exhibited a higher catalytic activity in this reaction.
  • 矢部 岳大, 榎木 勝徳, 大谷 博司
    2016 年 80 巻 6 号 p. 370-378
    発行日: 2016年
    公開日: 2016/05/25
    ジャーナル フリー
     A thermodynamic analysis of the Al-Cu binary system has been performed to consider the metastable phase equilibria of the face-centered cubic (fcc) phase. The total energies of the ordered structures were obtained using first-principles calculations based on the fcc lattice. The cluster expansion method was applied to the results, and the free energies were calculated for the solid solution at finite temperatures. The results were analyzed together with some experimental data, and the equilibrium phase diagram of the Al-Cu binary system was calculated based on the CALPHAD (Calculation of Phase Diagrams) method. The results suggested a metastable two-phase separation of the fcc phase in the Al-rich region. The coherent spinodal line was calculated according to Cahn's treatment and revealed that the critical temperature decreased by about 100 K because of the coherency of the separated phases in the fcc matrix. In consideration of both Cahn's treatment and the effect of vacancies, it was suggested that the initial formation step of the Guinier-Preston zone might be relevant to the metastable coherent spinodal decomposition in the fcc solid solution.
  • 太田 美絵, 澤井 貴一, 南谷 大樹, 飴山 惠
    2016 年 80 巻 6 号 p. 379-385
    発行日: 2016年
    公開日: 2016/05/25
    ジャーナル フリー
     This investigation clarified the microstructural evolution in a two-phase stainless steel (329J1 grade), prepared by a mechanical milling (MM) and spark plasma sintering (SPS). The as-received stainless steel powder was produced by a plasma rotating electrode process and the microstructure of that was fully ferritic structure. After the MM, the single α phase coarse grain was changed to a bimodal α grain structure, formed nanocrystalline subsurface region and un-formed coarse grain inner region. SPS transformed from the powder with the bimodal α grain structure into “harmonic structure” of sintered compact. Namely, the fine-grain areas three dimensionally interconnect (“Shell” network) and the coarse-grain area periodically disperse (“Core”). The sintered (α+γ) two phase stainless steel exhibited a complex shell structure consisting of mid-shell and outer-shell regions. The α phase in the mid-shell is high angle boundaries and, that in the outer-shell is low angle boundaries. As the considered mechanism for such a complex microstructural evolution, the mid-shell is formed by grain growth of the α nano grains, followed by γ precipitation. On the other hand, the outer-shell is formed by the recovery of deformed α phase, and γ phase precipitates at the α subgrain boundaries. Consequently, the (α+γ) two phase stainless steel shows regularly aligned nano-duplex, micro-duplex and duplex structures, because of the competing procedure of recovery and recrystallization of α phase and γ precipitation.
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