首页> 外文会议>International Symposium on Solid Oxide Fuel Cells >Preparation of Structural Phase Diagram of Ln_2Ni_(1-x)Cu_xO_(4+δ) (Ln=La, Pr, Nd, Sm, Eu) as New Cathode Materials: Variation of Structural Phase Diagram on Kind of Ln
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Preparation of Structural Phase Diagram of Ln_2Ni_(1-x)Cu_xO_(4+δ) (Ln=La, Pr, Nd, Sm, Eu) as New Cathode Materials: Variation of Structural Phase Diagram on Kind of Ln

机译:制备LN_2NI_(1-X)CU_XO_(4 +δ)(LN = LA,PR,ND,SM,SM,SM,EU)的制备作为新的阴极材料:结构相图的变化

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Crystal structure of Ln_2Ni_(1-x)Cu_xO_(4+δ) (Ln= La, Pr, Nd, Sm and Eu), which are expected as new cathode materials for solid fuel cells, was investigated. Single phase with K_2NiF_4 structure, so-called T-phase, was obtained for La_2Ni_(1-x)Cu_xO_(4+δ) regardless of Cu content. Single phase with Nd_2CuO_4 structure, so-called T'-phase, was obtained for Sm_2Ni_(1-x)Cu_xO_(4+δ) and Eu_2Ni_(1-x)Cu_xO_(4+δ) for only 0.95≤x≤1.0 and x=1.0 respectively. No T-phase was obtained for the other composition of Ln_2Ni_(1-x)Cu_xO_(4+δ) (Ln=Sm, Eu). The single T-phase and T'-phase were obtained for Pr_2Ni_(1-x)Cu_xO_(4+δ) with x≤0.4 and x=1.0, respectively. For Pr_2Ni_(1-x)Cu_xO_(4+δ) with x between 0.5 and 0.9, phase separation into T-phase and T'-phase due to miscibility gap was observed, showing similar behavior with Nd_2Ni_(1-x)Cu_xO_(4+δ) except for little smaller x range of the miscibility gap. From high temperature X-ray diffraction measurements, it was revealed that the miscibility gap between 0.5 and 0.9 of Pr_2Ni_(1-x)Cu_xO_(4+δ) remained up to 700°C. Variation of the crystal structure of Ln_2Ni_(1-x)Cu_xO_(4+δ) on kinds of Ln and Cu content could be explained by using tolerance factor calculated from ionic radius of Ln~(3+), Ni~(2+) and Cu~(2+).
机译:Ln_2Ni_的晶体结构(1-X)Cu_xO_(4 +δ)(LN =镧​​,镨,钕,钐及铕),其被期待作为新的正极材料的固体燃料电池,进行了调查。对于La_2Ni_(1-X)Cu_xO_(4 +δ),得到单相K_2NiF_4结构,即所谓的T相,无论Cu含量的。得到单相Nd_2CuO_4结构,所谓T'-阶段,Sm_2Ni_(1-X)Cu_xO_(4 +δ)和Eu_2Ni_(1-X)Cu_xO_(4 +δ)为仅0.95≤x≤1.0和X分别= 1.0。为Ln_2Ni_的其他组合物,没有得到T相(1-X)Cu_xO_(4 +δ)(LN =钐,铕)。用x≤0.4且x = 1.0分别得到Pr_2Ni_(1-X)Cu_xO_(4 +δ)单T相和T'相,。对于Pr_2Ni_(1-X)Cu_xO_(4 +δ)与由于混溶隙0.5和0.9,相分离之间x转换成T相和T'相,观察到,示出具有Nd_2Ni_(1-X)Cu_xO_(类似的行为4 +δ)除了​​小一点X系列的混溶隙。从高温的X射线衍射测量时,它显露0.5和Pr_2Ni_(1-X)Cu_xO_ 0.9之间的互溶性间隙(4 +δ)仍高达700℃。 Ln_2Ni_(1-X)Cu_xO_的晶体结构的变化的种类Ln和Cu含量的(4 +δ)可以通过使用从LN〜(3+),镍〜的离子半径计算的容差因子来解释(2+)和Cu〜(2+)。

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