Two kinds of experimental methods were tried in the present work:(i)the powder metallurgy method combined with differential thermal analysis(DTA)to determine the metastable liquidus miscibility gap for a Fe–Cu binary...Two kinds of experimental methods were tried in the present work:(i)the powder metallurgy method combined with differential thermal analysis(DTA)to determine the metastable liquidus miscibility gap for a Fe–Cu binary system and(ii)the high-temperature melting method combined with isothermal treatment to determine the stable liquidus miscibility gap for a Fe–Sn binary system.The experimental method was adopted according to the characteristics of the liquidus miscibility gap of the specific system.Using the powder metallurgy method,a uniform microstructure morphology and chemical composition was obtained in the DTA specimen,and the phase-separation temperature of the supercooled metastable liquid was measured.The isothermal treatment was applied for the samples inside the stable liquidus miscibility gap;here,equilibrated compositions were reached,and a layered morphology was formed after rapid cooling.The liquid miscibility gaps of the Fe–Cu and Fe–Sn binary systems were measured,and the peak temperatures of the corresponding miscibility gaps were determined to be about 1417°C at x(Cu)=0.465 at%and 1350°C at x(Sn)=0.487 at%,respectively.On the basis of the experimental results,both the Fe–Cu and the Fe–Sn binary systems were thermodynamically assessed.展开更多
Abstract The as-cast microstructures and solidification paths of the Nb-Si-Ti ternary alloys in the NbsSi3-TisSi3 region were investigated. Since there exist some isomor- phous compounds in the NbsSi3-TisSi3 region, s...Abstract The as-cast microstructures and solidification paths of the Nb-Si-Ti ternary alloys in the NbsSi3-TisSi3 region were investigated. Since there exist some isomor- phous compounds in the NbsSi3-TisSi3 region, such as aNbsSi3 with B3Cr5 prototype, 13NbsSi3 with Si3W5 pro- totype, 7NbsSi3 with MnsSi3 prototype, and TisSi3 with MnsSi3 prototype, the primary solidification areas of these compounds were not typically indentified in previous experiments. In the present paper, the microstructure observation, the phase identification, and the composition measurement were performed using scanning electron microscopy (SEM), X-ray diffraction (XRD), and electron probe microanalysis (EPMA), respectively. No ternary compound is found. There exist three primary solidification areas, 13Nbs_x(Ti)xSi3, ~Nbs_x(Ti)xSi3, and Tis-x(Nb)xSi3 in the NbsSi3-TisSi3 region. Together with the literaturereported experimental data and optimization results, the liquidus projection of the whole Nb-Si-Ti ternary system is constructed, and totally ten primary solidification areas-- diamond-Si, Nb1-x(Ti)xSi2, Ti1-x(Nb)xSi2, Ti1-x(Nb)xSi, Ti5-x(Nb)xSi4, βNb5-x(Ti)xSi3,αNb5-x(Ti)xSi3, Ti5-x (Nb)xSi3, (Nb,Ti)3Si, and BCC--and nine transitional invariant reactions-L + Nb1-x(Ti)xSi2 → Ti1-x(Nb)x Si2 + Si, L + Nb1-x(Ti)xSi2 → Ti1-x(Nb)xSi2 + Ti5- (Nb)xSi4, L + Ti5-x(Nb)xSi4 → Ti1-x(Nb)xSi2 + Ti1-x (Nb)xSi, L + 13Nb5-x(Ti)5Si3→ Nb1-x(Ti)xSi2 + Ti5-x (Nb)xSi4, L + βNb5-x(Ti)xSi3→b5-x(Ti)xSi3 +Ti5-x (Nb)xSi4, L + αNb5-x(Ti)αSi3 → Ti5-x(Nb)xSi3 + Ti5-x(Nb)x Si4, L + αNb5-x(Ti)xSi3 →βNb5-x(Ti)xSi3 + Ti5-x(Nb)xSi3, L + βNb5-xTb-xSi3 → Ti5-x(Nb)xSi3 + (Nb,Ti)3Si, and L + (Nb,Ti)3Si → Ti5-x(Nb)xSi3 + BCC are confirmed.展开更多
The Ge-La binary system was critically assessed by means of the calculation of phase diagram (CALPHAD) technique. The asso- ciate model was used for the liquid phase containing the constituent species Ge, La, Ge3La5...The Ge-La binary system was critically assessed by means of the calculation of phase diagram (CALPHAD) technique. The asso- ciate model was used for the liquid phase containing the constituent species Ge, La, Ge3La5, and Ge1.7La. The terminal solid solution diamond-(Ge) with a small solubility of La was described using the substitutional model, in which the excess Gibbs energy was formulated with the Redlich-Kister equation. The compounds with homogeneity ranges, μ(Gel.7La), β(Ge1.7La), and (GeLa), were modeled using two sublatrices asα(Ge,La)l.7La, β(Ge,La)l.7La, and (Ge,La)(Ge,La), respectively. The intermediate phases with no solubility ranges, Ge4Las, GeaLa4, Ge3Las, and GeLa3, were treated as stoichiometric compounds. The three allotropic modifications of La, dhcp-La, fcc-La, and bcc-La, were kept as pure element phases since no solubility of Ge in La was reported. A set of self-consistent thermodynamic parameters of the Ge-La binary system was obtained. The calculation results agree well with the available experimental data from literatures.展开更多
基金supported by National Key Research and Development Program of China (No. 2016YFB0701201)National Natural Science Foundation of China (No. 51271027)
文摘Two kinds of experimental methods were tried in the present work:(i)the powder metallurgy method combined with differential thermal analysis(DTA)to determine the metastable liquidus miscibility gap for a Fe–Cu binary system and(ii)the high-temperature melting method combined with isothermal treatment to determine the stable liquidus miscibility gap for a Fe–Sn binary system.The experimental method was adopted according to the characteristics of the liquidus miscibility gap of the specific system.Using the powder metallurgy method,a uniform microstructure morphology and chemical composition was obtained in the DTA specimen,and the phase-separation temperature of the supercooled metastable liquid was measured.The isothermal treatment was applied for the samples inside the stable liquidus miscibility gap;here,equilibrated compositions were reached,and a layered morphology was formed after rapid cooling.The liquid miscibility gaps of the Fe–Cu and Fe–Sn binary systems were measured,and the peak temperatures of the corresponding miscibility gaps were determined to be about 1417°C at x(Cu)=0.465 at%and 1350°C at x(Sn)=0.487 at%,respectively.On the basis of the experimental results,both the Fe–Cu and the Fe–Sn binary systems were thermodynamically assessed.
基金supported by the National Natural Science Foundation of China (No. 51271027)the National High Technology Research and Development Program of China (No. 2013AA031601)
文摘Abstract The as-cast microstructures and solidification paths of the Nb-Si-Ti ternary alloys in the NbsSi3-TisSi3 region were investigated. Since there exist some isomor- phous compounds in the NbsSi3-TisSi3 region, such as aNbsSi3 with B3Cr5 prototype, 13NbsSi3 with Si3W5 pro- totype, 7NbsSi3 with MnsSi3 prototype, and TisSi3 with MnsSi3 prototype, the primary solidification areas of these compounds were not typically indentified in previous experiments. In the present paper, the microstructure observation, the phase identification, and the composition measurement were performed using scanning electron microscopy (SEM), X-ray diffraction (XRD), and electron probe microanalysis (EPMA), respectively. No ternary compound is found. There exist three primary solidification areas, 13Nbs_x(Ti)xSi3, ~Nbs_x(Ti)xSi3, and Tis-x(Nb)xSi3 in the NbsSi3-TisSi3 region. Together with the literaturereported experimental data and optimization results, the liquidus projection of the whole Nb-Si-Ti ternary system is constructed, and totally ten primary solidification areas-- diamond-Si, Nb1-x(Ti)xSi2, Ti1-x(Nb)xSi2, Ti1-x(Nb)xSi, Ti5-x(Nb)xSi4, βNb5-x(Ti)xSi3,αNb5-x(Ti)xSi3, Ti5-x (Nb)xSi3, (Nb,Ti)3Si, and BCC--and nine transitional invariant reactions-L + Nb1-x(Ti)xSi2 → Ti1-x(Nb)x Si2 + Si, L + Nb1-x(Ti)xSi2 → Ti1-x(Nb)xSi2 + Ti5- (Nb)xSi4, L + Ti5-x(Nb)xSi4 → Ti1-x(Nb)xSi2 + Ti1-x (Nb)xSi, L + 13Nb5-x(Ti)5Si3→ Nb1-x(Ti)xSi2 + Ti5-x (Nb)xSi4, L + βNb5-x(Ti)xSi3→b5-x(Ti)xSi3 +Ti5-x (Nb)xSi4, L + αNb5-x(Ti)αSi3 → Ti5-x(Nb)xSi3 + Ti5-x(Nb)x Si4, L + αNb5-x(Ti)xSi3 →βNb5-x(Ti)xSi3 + Ti5-x(Nb)xSi3, L + βNb5-xTb-xSi3 → Ti5-x(Nb)xSi3 + (Nb,Ti)3Si, and L + (Nb,Ti)3Si → Ti5-x(Nb)xSi3 + BCC are confirmed.
基金supported by the National Natural Science Foundation of China (Nos.50731002 and 50671009)
文摘The Ge-La binary system was critically assessed by means of the calculation of phase diagram (CALPHAD) technique. The asso- ciate model was used for the liquid phase containing the constituent species Ge, La, Ge3La5, and Ge1.7La. The terminal solid solution diamond-(Ge) with a small solubility of La was described using the substitutional model, in which the excess Gibbs energy was formulated with the Redlich-Kister equation. The compounds with homogeneity ranges, μ(Gel.7La), β(Ge1.7La), and (GeLa), were modeled using two sublatrices asα(Ge,La)l.7La, β(Ge,La)l.7La, and (Ge,La)(Ge,La), respectively. The intermediate phases with no solubility ranges, Ge4Las, GeaLa4, Ge3Las, and GeLa3, were treated as stoichiometric compounds. The three allotropic modifications of La, dhcp-La, fcc-La, and bcc-La, were kept as pure element phases since no solubility of Ge in La was reported. A set of self-consistent thermodynamic parameters of the Ge-La binary system was obtained. The calculation results agree well with the available experimental data from literatures.