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首页> 外文期刊>Journal of the European Ceramic Society >Thermal expansion of EB-PVD yttria stabilized zirconia
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Thermal expansion of EB-PVD yttria stabilized zirconia

机译:EB-PVD氧化钇稳定的氧化锆的热膨胀

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Yttria stabilized zirconia (YSZ) layers, suited for thermal barrier coatings (TBCs) in turbine engines, were produced by electron-beam physical vapour deposition (EB-PVD) on metallic (Ni-based alloys) ceramic (Al_2O_3 ) substrates (typically at 1000℃) using ingot compositions of about 4 mol% Y_2O_3-ZrO_2 . Employing powdered samples, removed from the surface of the as-deposited YSZ layers, precision X-ray diffraction data sets were recorded between 60 and 900 ℃ and the lattice parameters of the metastable, tetragonal (t') and the cubic (c) phases were refined using Rietveld's method. It was unambiguously verified that phase (c) was present in all investigated samples as a minority phase already in the as-deposited state. The thermal expansion coefficients of the tetragonal phase (t') (α_(11) = 9.3(2) × 10~(-6) K~(-1) , α_(33) =10.8(1) × 10~(-6) K~(-1)) and the cubic phase (c) (α_(11) = 8.5(2) × 10~(-6) K~(-1) ) were evaluated from the refined temperature dependent lattice parameter values of this study, and turned out to be close to each other, but significantly different from the coefficient of the monoclinic phase (m) (α_(11) = 9.0 × 10~(-6) K~(-1) , α_(22) = 1.2 × 10~(-6) K~(-1), α_(33) =11.9 × 10~(-6) K~(-1), α_(13) =0.0 × 10~(-6) K~(-1) ), which was derived from temperature dependent lattice parameter measurements published by Touloukian et al.~5 The expansion coefficient of the monoclinic phase (m) exhibited a very pronounced anisotropy in contrast to the tetragonal phases (t') and (t). Our values for (t') and (c) were in excellent agreement with that of other tetragonal and cubic phases from the literature with quite different Y_2O_3 contents.
机译:氧化钇稳定的氧化锆(YSZ)层适用于涡轮发动机的热障涂层(TBC),是通过在金属(基于镍的合金)陶瓷(Al_2O_3)基板上(通常为200纳米)对电子束进行物理气相沉积(EB-PVD)制成的1000℃)使用约4 mol%Y_2O_3-ZrO_2的铸锭成分。使用粉末状样品,从沉积的YSZ层表面去除,在60至900℃之间记录精确的X射线衍射数据集,以及亚稳相,四方相(t')和立方相(c)的晶格参数使用Rietveld方法精制而成。毫无疑问地证实,相(c)作为已处于沉积状态的少数相存在于所有研究样品中。四方相(t')的热膨胀系数(α_(11)= 9.3(2)×10〜(-6)K〜(-1),α_(33)= 10.8(1)×10〜(- 6)从精细的温度相关晶格参数值评估了K〜(-1))和立方相(c)(α_(11)= 8.5(2)×10〜(-6)K〜(-1))这项研究的结果彼此接近,但与单斜相的系数(m)显着不同(α_(11)= 9.0×10〜(-6)K〜(-1),α_( 22)= 1.2×10〜(-6)K〜(-1),α_(33)= 11.9×10〜(-6)K〜(-1),α_(13)= 0.0×10〜(-6 )K〜(-1)),这是由Touloukian等人发表的与温度相关的晶格参数测量结果得出的。〜5单斜晶相(m)的膨胀系数与四方相(t' ) 和T)。我们的(t')和(c)值与文献中Y_2O_3含量差异很大的其他四方相和立方相的值非常一致。

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