摘要
Dy–Cu intermediate alloys have shown substantial potential in the field of magnetostrictive and magnetic refrigerant materials.Therefore, this study focused on investigating the electrical conductivity of molten-salt systems for the preparation of Dy–Cu alloys and on optimizing the corresponding operating parameters. The electrical conductivity of molten LiF–DyF_3–Dy_2O_3–Cu_2O systems was measured from 910 to 1030°C using the continuously varying cell constant method. The dependencies of the LiF–DyF_3–Dy_2O_3–Cu_2O system conductivity on the melt composition and temperature were examined herein. The optimal operating conditions for Dy–Cu alloy production were determined via analyses of the electrical conductivity and activation energies for conductance, which were calculated using the Arrhenius equation. The conductivity of the molten system regularly increases with increasing temperature and decreases with increasing concentration of Dy_2O_3 or Cu_2O or both. The activation energy Eκ of the LiF–DyF_3–Dy_2O_3 and LiF–DyF_3–Cu_2O molten-salt systems increases with increasing Dy_2O_3 or Cu_2O content. The regression functions of conductance as a function of temperature(t) and the addition of Dy_2O_3(W(Dy_2O_3)) and Cu_2O(W(Cu_2O)) can be expressed as κ =-2.08435 + 0.0068 t-0.18929 W(Dy_2O_3)-0.07918 W(Cu_2O). The optimal electrolysis conditions for preparing the Dy–Cu alloy in Li F–DyF_3–Dy_2O_3–Cu_2O molten salt are determined to be 2.0 wt% ≤ W(Dy_2O_3) +W(Cu_2O) ≤ 3.0 wt% and W(Dy_2O_3):W(Cu_2O) = 1:2 at 970 to 1000 °C.
Dy–Cu intermediate alloys have shown substantial potential in the field of magnetostrictive and magnetic refrigerant materials.Therefore, this study focused on investigating the electrical conductivity of molten-salt systems for the preparation of Dy–Cu alloys and on optimizing the corresponding operating parameters. The electrical conductivity of molten LiF–DyF_3–Dy_2O_3–Cu_2O systems was measured from 910 to 1030°C using the continuously varying cell constant method. The dependencies of the LiF–DyF_3–Dy_2O_3–Cu_2O system conductivity on the melt composition and temperature were examined herein. The optimal operating conditions for Dy–Cu alloy production were determined via analyses of the electrical conductivity and activation energies for conductance, which were calculated using the Arrhenius equation. The conductivity of the molten system regularly increases with increasing temperature and decreases with increasing concentration of Dy_2O_3 or Cu_2O or both. The activation energy Eκ of the LiF–DyF_3–Dy_2O_3 and LiF–DyF_3–Cu_2O molten-salt systems increases with increasing Dy_2O_3 or Cu_2O content. The regression functions of conductance as a function of temperature(t) and the addition of Dy_2O_3(W(Dy_2O_3)) and Cu_2O(W(Cu_2O)) can be expressed as κ =-2.08435 + 0.0068 t-0.18929 W(Dy_2O_3)-0.07918 W(Cu_2O). The optimal electrolysis conditions for preparing the Dy–Cu alloy in Li F–DyF_3–Dy_2O_3–Cu_2O molten salt are determined to be 2.0 wt% ≤ W(Dy_2O_3) +W(Cu_2O) ≤ 3.0 wt% and W(Dy_2O_3):W(Cu_2O) = 1:2 at 970 to 1000 °C.
引文
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