The paper reports on the atomic investigation aboutβphase in Mg_(96)Gd_(2)Y_(1)Ni_(1) alloy by using the first-principles study and the high-angle annular dark-field scanning transmission electron microscope(HAADF-ST...The paper reports on the atomic investigation aboutβphase in Mg_(96)Gd_(2)Y_(1)Ni_(1) alloy by using the first-principles study and the high-angle annular dark-field scanning transmission electron microscope(HAADF-STEM)corrected by atomic Cs.By using HAADF-STEM,the rectangularβphases were observed in the underage and peak aging stages in Mg_(96)Gd_(2)Y_(1)Ni_(1) alloy.Theβphase could be precipitated from the previously precipitatedβphase,and theβphase grew in steps when it was precipitated.A special transition structure of three atomic layer thicknesses was first observed at the edge of theβphase and the structure of this interface is probably as theβ/Mg_(1) interface for the analysis of thermodynamic characterization and electronic characterization.Theβ'phase and theβ_(H) structure were precipitated only at the edge of the length directions of theβphase.Theβ'phase continues to grow into aβphase directly without the formation ofβ_(1) phase,resulting in an increase in the length of theβphase,which is discovered for the first time.展开更多
The bulk interaction between two phases in AgI(η-Al_(2)O_(3) orα-Fe_(2)O_(3))has been investigated by means of electrical conductivity,DTA and Mössbauer spectra.It shows that bothα→βphase transition of AgI a...The bulk interaction between two phases in AgI(η-Al_(2)O_(3) orα-Fe_(2)O_(3))has been investigated by means of electrical conductivity,DTA and Mössbauer spectra.It shows that bothα→βphase transition of AgI and Morin transition ofα-Fe_(2)O_(3) influence each other.展开更多
A model specimen with a single boundary of theα/βphase simulating Mg-Al alloys was successfully fabricated by spark plasma sintering.A small electrode area ofαphase orβphase was prepared using the model specimen,a...A model specimen with a single boundary of theα/βphase simulating Mg-Al alloys was successfully fabricated by spark plasma sintering.A small electrode area ofαphase orβphase was prepared using the model specimen,and the OCPs(open-circuit potentials)of each phase and a small electrode area containing theα/βphase boundary in 0.1 M NaCl at pH 8.0 were compared:theβphase exhibited a higher potential,and theαphase showed a lower potential.The OCP of the small area containing theα/βphase boundary was the intermediate value of these phases.In a small area containingα/βphase boundary,discoloration and gas bubbles were observed on theαphase,but no bubble generation was detected on theβphase.The gas bubbles were initially generated on theαphase near theβphase,but as the discoloration(corrosion)of theαphase approached theβphase,the bubbles were generated on theβphase.In micro-galvanic corrosion of theαandβphases,theβphase did not always function as the preferred cathode.Theαphase partially corroded(or discolored)and became the anodes,so that the surrounding areas were most likely to be the cathodes.When corroded areas(anodes)in theαphase approached theβphase,theβphase would become cathodes.In addition to the micro-galvanic corrosion mechanism,the role of Al in corrosion resistance at theα/βphase boundary was determined by surface analysis.展开更多
The variations of the ^(63)Cu NMR,spectra of Cu_(83)-Zn_(17) powder mixtures with time of ball milling arc shown and analyzed.With increasing the ball-milling time,theαphase is developed as terminal phase over 5h.acc...The variations of the ^(63)Cu NMR,spectra of Cu_(83)-Zn_(17) powder mixtures with time of ball milling arc shown and analyzed.With increasing the ball-milling time,theαphase is developed as terminal phase over 5h.accompanying the emergence aid following disappearance of siiiall aniountβphase.The microstructural changes after aging at room temperature are also detected.Some valuable conclusions related to the alloying reaction on an atomic scale have been drawn.展开更多
基金financially supported by the National Natural Science Foundation of China(Grant No.51825101)the National Key Research and Development Program of China(Grant No.2016YFB0701201)。
文摘The paper reports on the atomic investigation aboutβphase in Mg_(96)Gd_(2)Y_(1)Ni_(1) alloy by using the first-principles study and the high-angle annular dark-field scanning transmission electron microscope(HAADF-STEM)corrected by atomic Cs.By using HAADF-STEM,the rectangularβphases were observed in the underage and peak aging stages in Mg_(96)Gd_(2)Y_(1)Ni_(1) alloy.Theβphase could be precipitated from the previously precipitatedβphase,and theβphase grew in steps when it was precipitated.A special transition structure of three atomic layer thicknesses was first observed at the edge of theβphase and the structure of this interface is probably as theβ/Mg_(1) interface for the analysis of thermodynamic characterization and electronic characterization.Theβ'phase and theβ_(H) structure were precipitated only at the edge of the length directions of theβphase.Theβ'phase continues to grow into aβphase directly without the formation ofβ_(1) phase,resulting in an increase in the length of theβphase,which is discovered for the first time.
文摘The bulk interaction between two phases in AgI(η-Al_(2)O_(3) orα-Fe_(2)O_(3))has been investigated by means of electrical conductivity,DTA and Mössbauer spectra.It shows that bothα→βphase transition of AgI and Morin transition ofα-Fe_(2)O_(3) influence each other.
基金supported by JSPS KAKENHI Grant Numbers JP17H01331 and JP21K18804supported by The Light Metal Educational Foundation Inc.of Japansupported by Amano Institute of Technology and China Scholarship Council。
文摘A model specimen with a single boundary of theα/βphase simulating Mg-Al alloys was successfully fabricated by spark plasma sintering.A small electrode area ofαphase orβphase was prepared using the model specimen,and the OCPs(open-circuit potentials)of each phase and a small electrode area containing theα/βphase boundary in 0.1 M NaCl at pH 8.0 were compared:theβphase exhibited a higher potential,and theαphase showed a lower potential.The OCP of the small area containing theα/βphase boundary was the intermediate value of these phases.In a small area containingα/βphase boundary,discoloration and gas bubbles were observed on theαphase,but no bubble generation was detected on theβphase.The gas bubbles were initially generated on theαphase near theβphase,but as the discoloration(corrosion)of theαphase approached theβphase,the bubbles were generated on theβphase.In micro-galvanic corrosion of theαandβphases,theβphase did not always function as the preferred cathode.Theαphase partially corroded(or discolored)and became the anodes,so that the surrounding areas were most likely to be the cathodes.When corroded areas(anodes)in theαphase approached theβphase,theβphase would become cathodes.In addition to the micro-galvanic corrosion mechanism,the role of Al in corrosion resistance at theα/βphase boundary was determined by surface analysis.
文摘The variations of the ^(63)Cu NMR,spectra of Cu_(83)-Zn_(17) powder mixtures with time of ball milling arc shown and analyzed.With increasing the ball-milling time,theαphase is developed as terminal phase over 5h.accompanying the emergence aid following disappearance of siiiall aniountβphase.The microstructural changes after aging at room temperature are also detected.Some valuable conclusions related to the alloying reaction on an atomic scale have been drawn.
