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PREDICTION OF FLOW STRESS OF HIGH-SPEED STEEL DURING HOT DEFORMATION BY USING BP ARTIFICIAL NEURAL NETWORK

J. T. Liu , H.B. Chang , R.H. Wu , T. Y. Hsu(Xu Zuyao) and X.R. Ruan( 1)Department of Plasticity Technology , Shanghai Jiao Tong University , Shanghai 200030 , China 2)School of Materials Science and Engineering , Shanghai Jiao Tong University , Shanghai 200030 , China)

金属学报(英文版)

The hot deformation behavior of TI (18W-4Cr-1V) high-speed steel was investigated by means of continuous compression tests performed on Gleeble 1500 thermomechan- ical simulator in a wide range of tempemtures (950℃-1150℃) with strain rotes of 0.001s-1-10s-1 and true strains of 0-0. 7. The flow stress at the above hot defor- mation conditions is predicted by using BP artificial neural network. The architecture of network includes there are three input parameters:strain rate,temperature T and true strain , and just one output parameter, the flow stress ,2 hidden layers are adopted, the first hidden layer includes 9 neurons and second 10 negroes. It has been verified that BP artificial neural network with 3-9-10-1 architecture can predict flow stress of high-speed steel during hot deformation very well. Compared with the prediction method of flow stress by using Zaped-Holloman parumeter and hyperbolic sine stress function, the prediction method by using BP artificial neurul network has higher efficiency and accuracy.

关键词: T1 high-speed steel , null , null , null , null

Structure, transport and magnetic properties of electron-doped perovskites R(x)Ca(1-x)MnO(3) (R = La, Y and Ce)

Journal of Physics-Condensed Matter

In this study, the transport and magnetic properties of electron-doped perovskites R(x)Ca(1-x)MnO(3) (R = La, Y and Ce) were investigated. As the R ion content increases, the crystal structure, resistivity, magnetoresistance, magnetization and related characteristic temperature of these systems all vary systematically. The data show that the variations in the electrical transport properties are mainly dependent on carrier concentration, whereas the magnetic properties of these systems are also dependent on crystal structure. When the carrier concentration exceeds a certain level, charge ordering occurs, leading to the localized electronic state and peaks in the magnetization curves. The magnetic transition temperature T(N) can be well described by crystal structural parameters, suggesting that crystal structure and magnetic properties are strongly coupled to each other.

关键词: rare-earth manganates;phase-separation;colossal magnetoresistance;manganites;oxides;bandwidth;physics;camno3;ln

MAGNETOSTRICTIVE BEHAVIOUR OF R(Fe_(1-x)Al_x)_y ALLOYS(R = Dy_(0.65)Tb_(0.25)Pr_(0.1))

WANG Bowen , WU Changheng , ZHUANG Yuzhi , JIN Ximei , LI Jingyuan(Institute of Metal Research , Chinese Academy of Sciences , Shenyang 110015 , China)(Shenyang Institute of Technology , Shenyang 110023 , China)(Institute of Physics , Chinese Academy of Sciences , Beijing 100080 , China)

金属学报(英文版)

The structure and magnetostriction of R(Fe_(1-x)Al_x)_y alloys(R=Dy_(0.65)Tb_(0.25)Pr_(0.1),x≤0.3,y=1.8 and 2) have been investigated using metallography, X-ray diffraction, electron probe micro- analysis(EPMA) and standard strain gauge techniques.It was found that the matrix of R(Fe_(1-x)Al_x)_2 alloys is cubic Laves phase(Dy,Tb,Pr)(Fe,Al)_2 and the second phase is PuNi3-type (Dy,Tb,Pr)(Fe,Al)_3 when x<0.15.The R(Fe_(1-x)Al_x)_(1.8) alloys contain trace of rare earth-rich phase.The magnetostriction of R(Fe_(1-x)Al_x)_y alloys decreases with increasing x in high magnetic fields; however, it exhibits a peak when x = 0.05 in low magnetic fields(H≤ 160 kA / m).The magnetostriction of R(Fe_(1-x)Al_x)_(1.8) alloys is higher than that of R(Fe_(1-x)Al_x)_2 alloys when x<0.15.

关键词: :rare earth-iron alloy , null , null

Structure and magnetostriction of RFex (1.6<=x<=2.0) and R(Fe1-yTiy)(1.8) (y<=0.2) alloys (R=DY0.65Tb0.25Pr0.1)

Journal of Magnetism and Magnetic Materials

Structure, Curie temperature and magnetostriction of RFex (1.6 less than or equal to x less than or equal to 2.0) and R(Fe1-yTiy)(1.8) (y less than or equal to 0.2) alloys (R = Dy0.65Tb0.25Pr0.1) have been investigated using optical microscopy, X-ray diffraction, AC initial susceptibility and standard strain gauge techniques. The homogenized RFe, alloys are found to be essentially single phase in the range of 1.8 less than or equal to x < 1.85. The second phase is a rare-earth-rich phase when x < 1.8, and (Dy, Tb, Pr)Fe-3 phase when x greater than or equal to 1.85. X-ray diffraction indicates that the R(Fe1-yTiy)(1.8) alloys contain a small amount of Fe2Ti phase when y greater than or equal to 0.05, which increases with the increment of Ti content. The Curie temperature of R(Fe1-yTiy)(1.8) alloys slightly enhances with increasing Ti concentration when y less than or equal to 0.05, then remains almost unchanged in the range of 0.05 < y less than or equal to 0.20. The magnetostriction of RFex alloys is improved when x less than or equal to 1.80 and reduced by increasing Fe content when x greater than or equal to 1.85. The magnetostriction of R(Fe1-yTiy)(1.8) alloys is lowered by increasing Ti content.

关键词: rare earth iron compounds;substitution effects;laves phase;magnetostriction

Studies of the changes of Mn-Y (Y = S, Se, Te) bond lengths R with the Mn composition x in Zn1-xMnxY alloys from optical spectrum data

Journal of Physics and Chemistry of Solids

The changes of Mn-Y (Y = S, Se, Te) bond lengths R with the Mn composition x in the diluted magnetic semiconductors Zn1-xMnxY are calculated from the optical spectra and their pressure shifts. The calculated results suggest that the Mn-Y bond lengths change little with the Mn composition x-much less than expected from lattice parameters as determined by X-ray diffraction. These results are also in good agreement with the observed values obtained from the EXAFS measurements. It appears that for ternary A(1-x)M(x)Y (M denotes the divalent transition-metal ion) alloys the changes of M-Y bond lengths R with the M composition x can be studied from their optical spectrum data. (C) 2000 Elsevier Science Ltd. All rights reserved.

关键词: semiconductors;high pressure;crystal fields;luminescence;light;properties;absorption fine-structure;local-structure;dependence;pressure;exafs

R_2Fe_(17)N_x中子衍射研究(R=Y,Dy,Nd)

杨继廉 , 张百生 , 丁永凡 , 杨应昌 , 张晓东 , 潘树明

金属学报

用中子衍射法测定了R_2Fe_(17)N_x(R=Y,Dy,Nd)中N的占位及磁结构,初步讨论了N的占位对磁性能的影响

关键词: 中子衍射 , Curie temperature , permanent magnet

Multiferroic phase diagram of Y partially substituted Dy(1-x)Y(x)MnO(3)

Applied Physics Letters

The effect of nonmagnetic Y partial substitution at the Dy site in Dy(1-x)Y(x)MnO(3) up to x=0.2 on magnetism, specific heat, and ferroelectricity is investigated, which resulted in a preliminary multiferroic phase diagram. It is revealed that the Y partial substitution suppresses the Dy-spin ordering point (T(Dy)) and ferroelectric ordering point (T(FE)) but enhances the Mn-spin ordering point (T(N)). The interaction between the spins of Dy and Mn is remarkably affected by Y substitution. The measured electrical polarization depends on the Y substitution in a complex way because the ferroelectricity is sensitive to the interaction between the spins of Dy and Mn. (c) 2011 American Institute of Physics. [doi: 10.1063/1.3536506]

关键词: ferroelectricity;polarization

Tunable magnetocaloric effect around hydrogen liquefaction temperature in Tb(1-x)Y(x)CoC(2) compounds

Physica B-Condensed Matter

The magnetic properties and magnetocaloric effect of Tb(1-x)Y(x)CoC(2) (x = 0, 0.1, 0.2, 0.3, 0.4) compounds have been investigated systematically. All the compounds undergo second-order transitions from paramagnetic to ferromagnetic states without thermal and magnetic hysteresis. With increasing Y content from 0 to 0.4, the Curie temperatures decrease nearly linearly from 28 to 18 K. The nature of the second-order phase transitions can be confirmed by Arrott plots. For Tb(0.6)Y(0.4)CoC(2) compound, the maximum value of the magnetic entropy change -Delta S(M) at 20 K is 9.35 J kg(-1) K(-1) for an external field change of 5T (5.14 J kg(-1) K(-1) for 2T). The large reversible magnetic entropy change makes Tb(0.6)Y(04)CoC(2) compound an attractive candidate for the application at hydrogen liquefaction temperature. (C) 2010 Elsevier B.V. All rights reserved.

关键词: Curie temperature;Magnetocaloric effect;Magnetic properties;ac susceptibility

Y1-xRxBa2Cu3O7-δ体系R=Eu、Gd)的正电子寿命和超导性研究

薛运才 , 陈镇平 , 苏玉玲 , 郝俊红 , 党凯 , 王坦 , 吕全才

低温物理学报 doi:10.3969/j.issn.1000-3258.2005.z1.033

本文报道了对Y1-xRxBa2Cu3O7-δ(R=Eu、Gd)两个系列样品的超导电性研究结果.首先,发现随着Eu、Gd掺杂量x的增加,Y1-x〗EuxBa2Cu3O7-δ和Y1-xGdxBa2Cu3O7-δ的晶胞体积均随之增大,但所有样品均保持与Y-123样品相同的单相正交结构;正电子平均寿命实验结果表明Cu-O链处局域电子密度ne随Eu、Gd掺杂浓度x的增加而减小,说明Eu、Gd对Y位的替代引起晶胞结构参量的变化不仅改变了Y位的电子密度,同时也影响了Cu-O链周围的电子密度分布;超导转变温度T\-c随Eu、Gd掺杂浓度x增加而略有增加,反映了Eu、Gd掺杂虽然改变了体系的局域电子结构,但没有破坏超导所需的Cu-O链与CuO2面之间的耦合;Y位掺杂体系的超导电性与掺杂离子的磁性无关,而与掺杂离子的半径有关.

关键词: 高温超导体 , 正电子湮没 , 晶体结构

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