| 1 | Solidification pathway and phase transformation behavior in a beta-solidified gamma-TiAl based alloy显示文摘The phase transformation behavior of an as-cast Ti-42Al-5 Mn(at.%)alloy after subsequent quenching from 1380℃to 1000℃was investigated based on the differential thermal analysis(DTA),electron probe micro analyzer-backscattered electrons(EPMA-BSE),transmission electron microscope(TEM)and X-ray diffraction(XRD).The results show that,the solidification path can be summarized as follows:Liquid→Liquid+β→β→β→α→β+α+γ→βo+α2+γ→βo+γ+α2/γ→βo+γ+α2/γ+βo,sec,with the phase transformationα→βtemperature(Tβ)=1311℃,phase transformationγ→βtemperature of(Tγsolv)=1231℃,phase transformationα2→αorβo→βtemperature(Tα2→α/Tβo→β)=1168 C,eutectoid temperature(Teut)=1132℃and T(α2/γ→βo,sec)≈1120℃.In comparison with Ti-42 Al alloy,the Teut and Tγsolv are slightly increased while both the Tp is decreased obviously by 5%Mn addition.When quenched from the temperature of 1380-1260℃,the martensitic transformationβ→α'could occur to form the needlelike martensite structure inβarea.This kind of martensitic structure is much obvious with the increase of temperature from 1260℃to 1380℃.When the temperature is below Tγsolv(1231℃),theγgrains would nucleate directly from theβphase.For the temperature slightly lower than T(eut)(1132℃),the dottedβ(o,sec)phases could nucleate in the lamellar colonies besides theγlamellae precipitated withinα2 phase.Finally,at room-temperature(RT),the alloy exhibits(po+α2+γ)triple phase with microstructure ofβo+lamellae+γ,of which the lamellar structure consists ofα2,γandβo,sec phases.The phase transformation mechanisms in this alloy,involvingβ→α',β→γ,α2→α2/γandα2→βo,sec were discussed. | H.Xu X.B.Li W.W.Xing L.Shu Y.C.Ma K.Liu | 2019 | Journal of Materials Science & Technology2019，35，11： | 2 |
| 2 | Determination of Vapor Pressure of Liquid Copper by Carrier Gas Method显示文摘The relationship between the vapor pressure of liquid copper and the flow rate of carrier gas argon was discussed,when the carrier gas method was used to determine the vapor pressure of liquid copper at 1892 K.The proper argon flow rate range obtained was 150e500 mL/min and enough evidence was provided to verify the vapor pressure-flow rate of carrier gas relationship at the target temperature.Based on the proper flow rate range,the vapor pressure of liquid copper was measured at 1609e1892 K.The relationship of vapor pressureetemperature obtained by the method of regression analysis can be expressed as:ln(p/Pa)(25.470 0.903)(39099.8 1574.5)/T.Further,the thermodynamic properties including the heat of vaporization and the Gibbs free energy of the Cu(l)Cu(g)reaction were calculated by the vapor pressure obtained over the temperature range covered. | Y.J.Duan B.Chen Y.C.Ma M.Gao K.Liu | 2013 | Journal of Materials Science & Technology2013，29，12： | 0 |
| 3 | Kinetics of Al Evaporation from Liquid U-Al Alloys in Vacuum Induction Melting显示文摘A research on kinetics of Al evaporation from liquid U—Al alloys was made in a vacuum induction melting(VIM) furnace at 1673—1843 K.The evaporation rate of Al was found to be first order with respect to Al content in the melt.The overall mass transfer coefficient of Al was determined and it was found that the evaporation rate of Al increased with increasing temperatures.The apparent activation energy of Al evaporation at 1673-1843 K was 171.5 kJ mol^(-1).The value of mass transfer coefficient of Al in the liquid phase was estimated to be 3.77 × 10^(-6),7.41×10^(-6),and 9.40 × 10^(-6) m s^(-1) at 1673,1753,and 1843 K,respectively.Meanwhile,rate determining steps were discussed and it was concluded that the evaporation rate of Al is mainly controlled by liquid phase mass transfer. | Y.J.Duan B.Chen Y.C.Ma K.Liu | 2015 | Journal of Materials Science & Technology2015，31，4： | 0 |
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