Microstructures of rapidly solidified Al-In immiscible alloy

来源 :Transactions of Nonferrous Metals Society of China | 被引量 : 0次 | 上传用户:dengliguo1971
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The microstructural evolution and growth mechanism of the melt spun Al In monotectic alloy were studied. During the rapid solidification of Al 17.5%In, a cellular structure→equiaxed structure transition occurs through the ribbon thickness. The as solidified microstructures are characterized by a homogeneous distribution of nanometer sized indium particles embedded within the matrix. However, with increasing distance from the chilled surface, the average particle size increases. In the underside of the ribbon, some particle arrays are perpendicular to the growth front. Next, all of the indium particles distribute randomly within the matrix. In the upside of the ribbon, some bigger indium particles distribute along the equiaxed grain boundaries. The diameter distributions of indium particles within Al matrix are bimodal. Compared with the massive partitionless solidification, the liquid separation process is the prevailing process during the non equilibrium solidification. The cooling rate, the interface energies ( γ S1/L1 , γ S1/L2 and γ L1/L2 ) and the growth mechanism all have effects on the microstructure. [ The microstructural evolution and growth mechanism of the melt spun Al In monotectic alloys were studied. During the rapid solidification of Al 17.5% In, a cellular structure → equiaxed structure transition occurs through the ribbon thickness. The as solidified microstructures are characterized by a homogeneous distribution或者, with increasing distance from the chilled surface, the average particle size increases. In the underside of the ribbon, some particle arrays are perpendicular to the growth front. distribute the random within the matrix. In the upside of the ribbon, some bigger indium particles distribute along the equiaxed grain boundaries. Compared with the massive partitionless solidification, the liquid separation process is the prevailing process during the non-equilibrium solidification cooling rate, the interface energies (γ S1 / L1, γ S1 / L2 and γ L1 / L2) and the growth mechanism all have effects on the microstructure. [
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