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首页> 外文期刊>Powder Metallurgy and Metal Ceramics >EFFECT OF MICROWAVE HEATING ON THE MASS TRANSFER, PHASE FORMATION, AND MICROSTRUCTURAL TRANSFORMATIONS IN THE Y_2O_3-Al_2O_3 DIFFUSION COUPLE
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EFFECT OF MICROWAVE HEATING ON THE MASS TRANSFER, PHASE FORMATION, AND MICROSTRUCTURAL TRANSFORMATIONS IN THE Y_2O_3-Al_2O_3 DIFFUSION COUPLE

机译:微波加热对Y_2O_3-Al_2O_3扩散偶的传质,相形成和组织转变的影响

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The phase composition, phase growth kinetics, and structures of diffusion zones formed under microwave heating (24 GHz) (MWH) and conventional heating (CH) in two-layer Al_2O_3-Y_2O_3 samples are studied by optical and scanning electron microscopy and electron microprobe analysis. Diffusion annealing was conducted at 1700 °C for 5 h in vacuum, the heating rate being 10 °C/min in all experiments. The diffusion couples included alumina layers, such as coarse-grained polycore or sintered Al_2O_3—5 vol.% ZrO_2 layers, and yttria layers, such as sintered coarse-grained samples or fine Y_2O_3 powder layers on the Al_2O_3 surface. It is shown that the phases formed during reactive diffusion do not uniquely correspond to the phase diagram, but depend on the initial structure of contacting layers and the type of heating. This is attributed to the contribution of kinetic factors to the competitive phase growth, particularly to the structural sensitiveness of diffusion coefficients whereby the diffusive phases grow and the stresses appearing when new phases form. It is found that MWH influences the competitive phase growth in the Al_2O_3—Y_2O_3 system, which involves both the change in the phase composition of the diffusion zone compared to that formed under CH and the acceleration of phase growth. The maximum effect of the phase growth acceleration under MWH is observed for the YAG phase, which is 30 times as fast as that under CH. It is suggested that the structure of grain boundaries changes and, accordingly, their permeability increases under MWH. The accelerated GB diffusion under MWH promotes the YAG phase growth in both oxides as a result of opposite diffusion flows of Al and Y ions along GBs. Under TH the YAG phase is formed only in Y_2O_3 oxide because of the unipolar diffusion of Al~(3+) ions to Y_2O_3. The validity of the proposed mechanism is confirmed by numerical evaluations.
机译:通过光学和扫描电子显微镜以及电子探针分析研究了两层Al_2O_3-Y_2O_3样品在微波加热(24 GHz)(MWH)和常规加热(CH)下形成的相组成,相生长动力学和扩散区的结构。在真空中于1700°C进行扩散退火5 h,在所有实验中加热速率均为10°C / min。扩散对包括氧化铝层(例如,粗晶粒多核或烧结的Al_2O_3-5 vol。%ZrO_2层)和氧化钇层(例如,烧结的粗晶粒样品或Al_2O_3表面的细Y_2O_3粉末层)。结果表明,在反应性扩散过程中形成的相并不唯一对应于相图,而是取决于接触层的初始结构和加热类型。这归因于动力学因素对竞争相增长的贡献,特别是由于扩散系数的结构敏感性,由此扩散相增长并且在形成新相时出现应力。发现MWH影响Al_2O_3-Y_2O_3系统中竞争相的生长,这涉及扩散区相组成的变化(与CH形成的相比较)和相生长的加速。对于YAG相,在MWH下观察到相生长加速的最大影响,是CH时的30倍。建议在MWH下晶界的结构发生变化,因此其磁导率增加。由于Al和Y离子沿GBs的相反扩散流,MWH下GB加速的GB扩散促进了两种氧化物中YAG相的生长。在TH下,由于Al〜(3+)离子向Y_2O_3的单极扩散,YAG相仅在Y_2O_3氧化物中形成。通过数值评估证实了所提出机制的有效性。

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