• Applied Microscopy
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• 제46권3호
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• pp.160-163
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• 2016

Effect of dealloying condition on the formation of nanoporous structure in melt-spun $Al_{60}Ge_{30}Mn_{10}$ alloy has been investigated in the present study. In as-melt-spun $Al_{60}Ge_{30}Mn_{10}$ alloy spinodal decomposition occurs in the undercooled liquid during cooling, leading to amorphous phase separation. By immersing the as-melt-spun $Al_{60}Ge_{30}Mn_{10}$ alloy in 5 wt% HCl solution, Al-rich amorphous region is leached out, resulting in an interconnected nano-porous $GeO_x$ with an amorphous structure. The dealloying temperature strongly affects the whole dealloying process. At higher dealloying temperature, dissolution kinetics and surface diffusion/agglomeration rate become higher, resulting in the accelerated dealloying kinetics, i.e., larger dealloying depth and coarser pore-ligament structure.

• 한국주조공학회지
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• 제13권5호
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• pp.462-475
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• 1993

A numerical analysis on the microstructural evolutions of microcellular and cellular ${\alpha}-aluminum$ phase in the gas-atomized Al-8wt. pct droplets was represented. The 2-dimensional non-Newtonian heat transfer and the dendritic growth theory in the undercooled melt were combined under the assumptions of a point nucleation on droplet surface and the macroscopically smooth solid-liquid interface enveloping the cell tips. It reproduced the main characteristic features of the reported microstructures quite well. It predicted a considerable volume fraction of segregation-free region in a droplet smaller than $l0{\mu}m$ if an initial undercooling larger than 100K is given. The volume fractions of the microcellular region($g_A$) and the sum of the microcellular and cellular region($g_a$) were predicted as functions of the heat transfer coefficient, h and initial undercooling, ${\triangle}T$. It was shown that $g_A$ and $g_a$, in the typical gas-atomization processes with $h=0.1-1.0W/cm^2K$, are dominated by ${\triangle}T$ and h, respectively, but for h larger than $4.0W/cm^2K$, a fully microcellular structure can be obtained irrespective of the initial undercooling.

• 한국재료학회지
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• 제11권3호
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• pp.171-177
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• 2001

급냉응고방식으로 제조한 비정질 Z $r_{62-x}$N $i_{10}$C $u_{20}$A $l_{8}$ $Ti_{x}$ (x=3, 6, 9at%) 합금을 사용하여 열적, 기계적 성질을 조사하였다. 시효온도에 따른 결정화 거동은 Ti 3at%에서는 비정질$\longrightarrow$비정질+Z $r_2$A $l_3$+Zr+(Ni,Ti)$\longrightarrow$Z $r_2$Cu+Al+(Ni,Ti)의 결정화 거동을 나타내었으며, Ti 6at%에서는 비정질$\longrightarrow$비정질+Al$\longrightarrow$A $l_2$Ti+NiZr+CuTi, Ti 9at%에서는 비정질$\longrightarrow$비정질+Zr+Al$\longrightarrow$Zr+A $l_2$Zr+Al $Ti_3$+CuTi의 결정화 거동을 보였다. 시효온도가 증가할수록 비정질 모상에 석출상의 체적율( $V_{f}$ )이 증가하고 그에 따라 비커스 경도 ( $H_{v}$ )간이 증가하였다. 파괴인장강도($\sigma_{f}$ )는 $V_{f}$ 의 증가에 따라 증가하다가 Z $r_{59}$A $l_{10}$N $i_{20}$C $u_{8}$ $Ti_3$은 $V_{f}$ =38%에서 1219MPa의 최대값을 보이고, Z $r_{56}$A $l_{10}$N $i_{20}$C $u_{8}$ $Ti_{6}$은 $V_{f}$ =2%에서 1203MPa의 최대값을 보이고, Z $r_{53}$A $l_{10}$N $i_{20}$C $u_{8}$ $Ti_{9}$ $V_{f}$ =5%에서 1350MPa의 최대값을 나타낸 후 그 이상의 $V_{f}$ 에서는 급격히 감소하였다. $\sigma_{f}$ 가 급격히 감소하는 $V_{f}$ 와 연성 파면에서 취성파면으로 천이되는 $V_{f}$ 가 일치하였다.f/가 일치하였다.