We report the crystallization and magnetic properties of non-equilibrium alloy powders produced by rod-milling as well as by new chemical leaching. X-ray diffractometry, transmission electron microscopy, differential scanning calorimetry and vibrating sample magnetometry were used to characterize the as-milled and leached specimens. After 400 h or 500 h milling, only the broad peaks of nano bcc crystalline phases were detected in the XRD patterns. The crystallite size, the peak and the crystallization temperatures increased with increasing Fe. After being annealed at for 1 h for as-milled alloy powders, the peaks of bcc are observed. After being annealed at for 1 h for leached specimens, these non-equi-librium phases transformed into fcc Cu and phases for the x=0.25 specimen, and into bcc phases for both the x=0.50 and the x=0.75 specimens. The saturation magnetization decreased with increasing milling time for alloy powders. On cooling the leached specimens from ,\;the magnetization first sharply increase at about for x=0.25, x=0.50, and x=0.75 specimens, repectively.

In order to investigate behavior of abnormal expansion of the iron-copper compacts, we compared the dilatometric curves of the compacts which mixed the copper powder to the iron powder with those of compacts which mixed the copper powder to the iron-copper alloy powder. The dilatometric curves were obtained below the sintering conditions, which heated up to 115 by a heating rate of 1/min, held for 60min at 115 and cooled down at a rate of 2/min to room temperature. The dilatometric curves of the compacts showed the different expansion behavior at temperatures above the copper melting point in spite of same chemical composition. All of the compacts of former case showed large expansion, but all of the compacts in latter case showed large contraction. The microstructures of sintered compacts also showed the different progress in alloying of the copper into the iron powder. Namely we could observe the segregation at alloy part of copper into iron powder in case of the sintered compacts, which mixed the copper powder to the iron powder, but could not observe the segregation in compacts which mixed the copper powder to the iron-copper alloy powder. But the penetration of liquid copper into the interstices between solid particles was occurred at both cases. Therefore, the showing of the different dimensional changes in the compacts in spite of same chemical composition is due to more the alloying of copper into iron powder than the penetration of liquid copper into the interstices between solid particles.

Nanoscale Cu-Ni alloy nanopowders have been produced by a pulsed wire evaporation method in an inert gas. The effect of Cu-Ni alloy nanopowders as additives to motor oil on the tribological properties was studied at room temperature. The worn surfaces were characterized by Scanning Electron Microscopy (SEM) and Energy-Dispersive X-ray Spectroscopy (EDS). Cu-Ni alloy nanopowders as additives lowered coefficient of friction and wear rate. It was found that a copper containing layer on the worn surface was formed, and deposited layers of the metal cladding acted as lubricant on the worn surface, reducing the friction coefficient. It was clearly demonstrated that Cu-Ni alloy nanopowders as additives are able to restore the worn surface and to preserve the friction surfaces from wear

The mechanical alloying effect has been studied on the three Cu-based alloy systems with a positive heat of mixing. The extended bcc solid solution has been formed in the Cu-V system and an amorphous phase in the Cu-Ta system. However, it is round that a mixture of nanocrystalline Cu and Mo Is formed in the Cu-Mo system. The neutron diffraction has been employed at a main tool to characterize the detailed amorphization process. The formation of an amorphous phase in Cu-Ta system can be understood by assuming that the smaller Cu atoms preferentially enter into the bcc Ta lattice during ball milling.

We report the structure, thermal and magnetic properties of a non-equilibrium alloy powder produced by rod milling and chemical leaching. An X-ray diffractometry(XRD), a transmission electron microscope(TEM), a differential scanning calorimeter(DSC), a vibrating sample magnetometer(VSM), and superconducting quantum interference device(SQUID) were utilized to characterize the as-milled and leaching specimens. The crystallite size reached a value of about 8.82 nm. In the DSC experiment, the peak temperatures and crystallization temperatures decreased with increasing milling time. The activation energy of crystallization is 200.5 kJ/mole for as-milled alloy powder. The intensities of the XRD peaks of as-milled powders associated with the bcc type structure formative at sharply increase with increasing annealing temperature. Above , peaks alloted to and are observed. After annealing at for 1h, the leached Ll specimen transformed into bcc -Fe and fcc Cu phases, accompanied by a change in the structural and magnetic properties. The saturation magnetization decreased with increasing milling time, and a value of about 8.42 emu/g was reached at 500 h of milling. The coercivity reached a maximum value of about 142.7 Oe after 500 h of milling. The magnetization of leached specimens as function of fields were higher at 5 K, and increased more sharply at 5 K than at 100 K.

Al-Cu-Mn 주조합금의 피로성질에 미치는 Cd 첨가의 영향을 저주기 및 고주기 피로시험을 통하여 조사하였다. Cd 첨가량이 증가함에 따라 피로수명이 증가하였으며, 인장강도도 증가하였다. 고주기 피로시험결과 피로강도는 115MPa이었으며 피로비는 0.31이었다. 피로시험 결과 균열이 표면에서 발생하여 입계를 따라 전파되었는데 이러한 입계파괴는 입계를 따라 존재하는 무석출대의 영향으로 생각된다. 인장강도값은 Cd이 첨가되지 않았을 경우 330MPa이었으나 0.15%의 Cd이 첨가됨으로써 401MPa 까지 증가되었다.

급냉응고방식으로 제조한 비정질 Z r62-xN i10C u20A l8 Tix (x=3, 6, 9at%) 합금을 사용하여 열적, 기계적 성질을 조사하였다. 시효온도에 따른 결정화 거동은 Ti 3at%에서는 비정질→비정질+Z r2A l3+Zr+(Ni,Ti)→Z r2Cu+Al+(Ni,Ti)의 결정화 거동을 나타내었으며, Ti 6at%에서는 비정질→비정질+Al→A l2Ti+NiZr+CuTi, Ti 9at%에서는 비정질→비정질+Zr+Al→Zr+A l2Zr+Al Ti3+CuTi의 결정화 거동을 보였다. 시효온도가 증가할수록 비정질 모상에 석출상의 체적율( Vf )이 증가하고 그에 따라 비커스 경도 ( Hv )간이 증가하였다. 파괴인장강도(σf )는 Vf 의 증가에 따라 증가하다가 Z r59A l10N i20C u8 Ti3은 Vf =38%에서 1219MPa의 최대값을 보이고, Z r56A l10N i20C u8 Ti6은 Vf =2%에서 1203MPa의 최대값을 보이고, Z r53A l10N i20C u8 Ti9 Vf =5%에서 1350MPa의 최대값을 나타낸 후 그 이상의 Vf 에서는 급격히 감소하였다. σf 가 급격히 감소하는 Vf 와 연성 파면에서 취성파면으로 천이되는 Vf 가 일치하였다.f/가 일치하였다.