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Catalysis of Organic..

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Yamauchi 161was -0.0009, -0.0032 and -0.0030 (MPa/s) for conventional Raney Ni, RWA andMA, respectively.Although the activity obtained by the MA route was not the highest in this case, theeffectiveness <strong>of</strong> MA was still much higher than that <strong>of</strong> conventional catalyst. Insome cases, MA is more effective than rapid solidification for making supersaturatedprecursors. An example is the Al-Co-Cu ternary system (11). The ranking<strong>of</strong> effectiveness <strong>of</strong> these methods may in general depend on the alloy system.Extension <strong>of</strong> Rapid Solidification to Ternary AlloyNi and Co are immiscible elements with Ag or Cu. Especially Ag is not misciblewith Ni or Co even in liquid state. Therefore, there were no previous attempts tomake Raney Ni or Co with dissolved Ag and no studies on their catalytic properties.Here, we will show an approach to make Raney Ni or Co with Cu or Ag. In the case<strong>of</strong> Al-Co-Cu system precursor, MA was an effective process to prepare a supersaturatedsingle solid solution as shown in Fig.9 (11). The crystallographic structureafter leaching <strong>of</strong> this specimen showed a broad fcc phase and no other phases wereobserved. To examine the as-leached state, the variation <strong>of</strong> magnetization wasmeasured with the temperature (12). Figure 10 shows the result. The magnetizationIntensity, I/arbitrary unitMechanical alloyedRapidly solidifiedSlowly solidifiedRelative saturated magenization (Ms/Mso)1.00.90.80.70.6heatingheatingheatingheatingcoolingMA+leachingrapid solidification+leachingMA(Co 50Cu 50)rapid solidification(Co 50 Cu 50 )20304050 602θ →Figure 9. XRD patterns <strong>of</strong> precursors <strong>of</strong>Al 75 Co 12.5 Cu 12.57080900.5300400500600 700Temperature, K800900Figure 10. Variation <strong>of</strong> saturatedmagnetization with temperature1000change by heating was a maximum for MA + leaching specimen. It suggests thatsome amount <strong>of</strong> Co dissolved in the Cu phase as-leached state. The precipitation <strong>of</strong>the ferro-magnetic Co phase by heating increased the magnetization. The as-leachedstate was a metastable state which can not be attained by conventional methods.However, another possible explanation for Fig.10 is that Co particles already exist inthe as-leached state, but they are very small and may show super-paramagneticbehavior that is <strong>of</strong>ten observed in ferro-magnetic materials with a few nano-sizeparticles. The Co particle size became coarser by heating. This is the subject <strong>of</strong> a

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