Fe—Mn—Si基合金fcc反铁磁与马氏体相变

采用电阻和内耗分析测定了不同Ｍｎ含量Ｆｅ－Ｍｎ－Ｓｉ基形状记忆合金（ＳＭＡ）相变临界点Ｍｓ、Ｍｆ、Ａｓ、Ａｆ和ＴＮ,研究了母相反铁磁状态时γ←→ε马氏体相变热诱发和应力诱发的影响。发现,随着Ｍｎ含量的增加,Ｍｓ、Ｍｆ、Ａｓ、Ａｆ降低,而ＴＮ升高直至热马氏体完全被抑制。当ＴＮ接近Ｍｓ时,母相反铁磁状态并不能完全抑制马氏体相变,而是使相变温区延伸到ＴＮ以下达－１５０℃的低温。即使热马氏体完全被事应力仍     

Fe-Mn-Si基合金中ε马氏体逆相变的内耗

利用音频内耗仪测试了Ｆｅ－Ｍｎ－Ｓｉ基形状记忆合金热诱发马氏体、一般应力诱发马氏体和热－机械训练后的应力诱发马氏体的逆相变过程．结果表明，热诱发马氏体的逆相变在４００～５００Ｋ完成；经训练后的应力诱发马氏体逆相变开始温度与热诱发马氏体逆相变开始温度相近，但高于一般应力诱发马氏体的逆相变开始温度；一般应力诱发马氏体的逆相变温度低于热马氏体的逆相变温度，随应变量的增加，Ａｓ降低     

Fe-Mn-Si形状记忆合金fc(γ)→hcp(ε)马氏体相变温度的热力学预报

借助于Ｆｅ－Ｍｎ－Ｓｉ合金层错几率Ｐｓｆ的Ｘ射线测量,计算了Ｐｓｆ与合金成分的关系,得到Ｆｅ－Ｍｎ－Ｓｉ三元系的１／Ｐｓｆ表达式．结合层错形核的热力学模型,经回归得Ｆｅ－Ｍｎ－Ｓｉ合金ｆｃ（γ）→ｈｃｐ（ε）马氏体相变的临界相变驱动力和Ｐｓｆ的关系式,进而得到临界相变驱动力与合金成分的关系．借助Ｐｓｆ建立了成分与相变驱动力之间的关系,结合有关热力学分析计算得到的Ｆｅ－Ｍｎ－Ｓｉ合金γ和ε两相Ｇｉｂｂｓ自由能曲线,预报了Ｆｅ－Ｍｎ－Ｓｉ三元系合金的ｆｃｃ（γ）→ｈｃｐ（ε）马氏体相变的温度．     

Fe—Mn—Si基形状记忆合金的奈尔温度（TN）对马氏体相变...

用静电音频内耗仪测量了Ｆｅ－３０．３Ｍｎ－６．１Ｓｉ,Ｆｅ－２９．０５Ｍｎ－６．２７Ｓｉ－ＲＥ,Ｆｅ－２６．４Ｍｎ－６．０２Ｓｉ－５．２Ｃｒ形状记忆合金在１５０￣６００Ｋ温度范围的内耗及模量变化,确定了三种合金的ＴＮ温度及Ｍｓ温度,通过计算ε→γ相变内耗峰的面积,研究了奈尔温度ＴＮ对γ→ε马氏体相变的影响。结果表明,合金成分显著地影响ＴＮ温度,其中ＲＥ和Ｃｒ均降低ＴＮ温度。随着ＴＮ温度的降低,Ｍｓ     

Fe—Mn—Si形状记忆合金fcc（γ）→hco（ε）马氏体相变温度的 …

借助于Ｆｃ－Ｍｎ－Ｓｉ合金层错几率Ｐｓｆ的Ｘ射线测量,计算了Ｐｓｆ与合金成分的关系,得到Ｆｅ－Ｍｎ－Ｓｉ三元系的１／Ｐｓｆ表达式。结合层错形核的热力学模型,经回归得Ｆｅ－Ｍｎ－Ｓｉ合金ｆｃｃ（γ）→ｈｃｐ（ε）马氏体相变的临界相变驱动力的Ｐｅｓｆ的关系式,进而得到临界相变驱动力与合金成分的关系。     

Fe-Mn-Si-Cr-Ni 系形状记忆合金 γε 相变温度与成份的关系

对现有ＦｅＭｎＳｉ、ＦｅＭｎＳｉＣｒＮｉ系形状记忆合金的成份和γε马氏体相变温度的实验测定数据进行了多元线性回归处理,建立了马氏体相变温度Ｍεｓ、Ａεｓ以及相变热滞（Ａεｓ－Ｍεｓ）与合金成份之间的定量经验关系．结果表明：Ｍｎ、Ｃｒ、Ｎｉ元素均降低相变温度Ｍεｓ和Ａεｓ;但Ｓｉ明显使其升高．同时表明此类合金中的Ｓｉ、Ｃｒ含量增加,合金的相变热滞增大．这一结果为此类合金的成份设计提供了依据．     

Fe—Mn—Si—Cr—Ni系形状记忆合金γ→←ε相变温度与成份？…

对现有Ｆｅ－Ｍｎ－Ｓｉ,Ｆｅ－Ｍｎ－Ｓｉ－Ｃｒ－Ｎｉ系形状记忆合金的成份和γ→←ε马氏体相变温度的实验测定数据进行了多元线性回归处理,建立了马氏体相变器Ｍεｓ,Ａεｓ以及相变热滞（Ａεｓ－Ｍεｓ）与合金成份之间的定理经验关系,结果表明：Ｍｎ,Ｃｒ,Ｎｉ元素均降低相变温度Ｍεｓ和Ａεｓ,但Ｓｉ明显使用升高,同时表明此类合金中的Ｓｉ,Ｃｒ含量增加,合金的相变热滞增大,这一结果为此类合金的成份设计提供了     

固溶硬化对Fe－Mn基合金SME的影响

固溶硬化对Ｆｅ－Ｍｎ基合金ＳＭＥ的影响Ｆｅ－高Ｍｎ－Ｓｉ合金会发生γ（ｆｃｃ）→（ｈｃｐ）马氏体转变，并显示出显著的形状记忆效应（ＳＭＥ）。研究表明，为了获得良好的ＳＭＥ，合金的形状变化必须通过应力诱发马氏体转变来完成，而在奥氏体相（γ）中不发生永久...     

Fe—Mn—Si合金中层错几率和淬火空位对ε马氏体相变温度的影响

用Ｘ衍射线形分析法测定了Ｆｅ－３０．３％Ｍｎ－６．１％Ｓｉ（质量分数）形状记忆合金经不同温度淬火和经退火后的层错几率Ｐｓｆ．研究了淬火空位、层错几率与马氏体相变点Ｍｓ的关系．结果表明,增加淬火空位将促进层错的形成,使Ｍｓ提高;且Ｍｓ与１／Ｐｓｆ呈线性关系．对可能的机理进行了讨论．     

Fe—Mn—Si—Cr形状记忆合金马氏体相变新结构的研究

用ＴＥＭ和ＸＲＤ详细研究了Ｆｅ－２８Ｍｎ－６Ｓｉ－５Ｃｒ合金在不同温度下经多次“训练”后的应力诱发马氏体相变及微观组织。发现了４Ｈ－（２,２）和６Ｈ－（３,３）两种具有正交点阵的新结构,并提出了相应的切变模型。上述正交结构被认为是应力诱发γ→ε马氏体相变及其逆相变受到阻碍而协调的结果,正交结构的出现不利于形状记忆效应的提高。     

An Index mechanism for multi-scale view in spatial databases

There are numerous geometric objects stored in the spatial databases. An importance function in a spatial database is that users can browse the geometric objects as a map efficiently. Thus the spatial database should display the geometric objects users concern about swiftly onto the display window. This process includes two operations:retrieve data from database and then draw them onto screen. Accordingly, to improve the efficiency, we should try to reduce time of both retrieving object and displaying them. The former can be achieved with the aid of spatial index such as R-tree, the latter require to simplify the objects. Simplification means that objects are shown with sufficient but not with unnecessary detail which depend on the scale of browse. So the major problem is how to retrieve data at different detail level efficiently. This paper introduces the implementation of a multi-scale index in the spatial database SISP (Spatial Information Shared Platform) which is generalized from R-tree. The difference between the generalization and the R-tree lies on two facets: One is that every node and geometric object in the generalization is assigned with a importance value which denote the importance of them, and every vertex in the objects are assigned with a importance value,too. The importance value can be use to decide which data should be retrieve from disk in a query. The other difference is that geometric objects in the generalization are divided into one or more sub-blocks, and vertexes are total ordered by their importance value. With the help of the generalized R-tree, one can easily retrieve data at different detail levels.Some experiments are performed on real-life data to evaluate the performance of solutions that separately use normal spatial index and multi-scale spatial index. The results show that the solution using multi-scale index in SISP is satisfying.     

Characterization of Ordovician carbonate reservoirs, southeastern Saskatchewan, Canada

The discovery of the prolific Ordovician Red River reservoirs in 1995 in southeastern Saskatchewan was the catalyst for extensive exploration activity which resulted in the discovery of more than 15 new Red River pools. The best yields of Red River production to date have been from dolomite reservoirs. Understanding the processes of dolomitization is, therefore, crucial for the prediction of the connectivity, spatial distribution and heterogeneity of dolomite reservoirs.The Red River reservoirs in the Midale area consist of 3～4 thin dolomitized zones, with a total thickness of about 20 m, which occur at the top of the Yeoman Formation. Two types of replacement dolomite were recognized in the Red River reservoir: dolomitized burrow infills and dolomitized host matrix. The spatial distribution of dolomite suggests that burrowing organisms played an important role in facilitating the fluid flow in the backfilled sediments. This resulted in penecontemporaneous dolomitization of burrow infills by normal seawater. The dolomite in the host matrix is interpreted as having occurred at shallow burial by evaporitic seawater during precipitation of Lake Almar anhydrite that immediately overlies the Yeoman Formation. However, the low δ18O values of dolomited burrow infills (-5.9‰～ -7.8‰, PDB) and matrix dolomites (-6.6‰～ -8.1‰, avg. -7.4‰ PDB) compared to the estimated values for the late Ordovician marine dolomite could be attributed to modification and alteration of dolomite at higher temperatures during deeper burial, which could also be responsible for its 87Sr/86Sr ratios (0.7084～0.7088) that are higher than suggested for the late Ordovician seawaters (0.7078～0.7080). The trace amounts of saddle dolomite cement in the Red River carbonates are probably related to "cannibalization" of earlier replacement dolomite during the chemical compaction.     

A computer generator for randomly layered structures

AcomputergeneratorforrandomlylayeredstructuresYUJia shun1,2,HEZhen hua2(1.TheInstituteofGeologicalandNuclearSciences,NewZealand;2.StateKeyLaboratoryofOilandGasReservoirGeologyandExploitation,ChengduUniversityofTechnology,China)Abstract:Analgorithmisintrod…     

Perspherical Approaches for Electrons in Atoms and Charged Excitons in Quantum Wells

Instead of following Fock’s expansion,we solve the Schrodinger equation for some quantum mechanical manybody systems such as electrons in atoms and charged excitons in quantum wells in a similar way in hyperspherical coordinates by expanding the wave functions into orthonormal complete basis sets of the hyperspherical hannonics(HHs)of hyperangles and generalized Laguerre polynomials(GLPs)of the hyperradius.This leads the equation to     

Advances in broadband wireless communications under high-mobility scenarios

Future mobile communication systems aim at providing very high data transmission rates, even in high-mobility scenarios such as high-speed wheel-track trains, maglev trains, highway vehicles, airplanes, guided missiles or spacecraft. A particularly important commercial application is the strong and increasing worldwide demand for high- speed broadband wireless communications （up to 574.8 km/ h test speeds or 380 km/h commercial speeds） in railways, providing data, voice and video services for applications such as onboard entertainment services to passengers, train control, train dispatch, train sensor status handling and sur- veillance. In such high-mobility scenarios, there are a number of communication challenges, including fast hand- over, location updating, high-speed channel modeling, estimation and equalization, anti-Doppler spreading tech- niques, fast power control, and dedicated network architec- ture. Because signal transmission in very high-speed scenarios will inevitably experience serious deterioration, it is imperative to develop key broadband mobile communi- cation techniques for such high-speed vehicles.     

Wuhan University Journal of Natural Sciences TOTAL CONTENTS

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海南岛地体及其毗邻陆缘晚中生代—新生代古地磁研究和构造演化

本文叙述了对海南岛及其毗邻大陆边缘白垩纪到第四纪地层岩石进行古地磁研究的全部工作过程。通过分析岩石中剩余磁矢量的磁偏角及磁倾角的变化,提出海南岛白垩纪以来经历的构造演化模式如下:早期伴随顺时针旋转而向南迁移,后期伴随逆时针转动并向北运移。联系该地区及邻区的地质、地球物理资料,对海南岛上述的构造地体运动提出以下认识:北部湾内早期有一拉张作用,主要是该作用使湾内地壳显著伸长减薄,形成北部湾盆地。从而导致了海南岛的早期构造运动,而海南岛后期的构造运动则主要是受南海海底扩张的影响。海南地体运动规律的阐明对于了解北部湾油气盆地的形成演化有重要的理论和实际意义。     

Scale-based spatial data model for GIS

Being the primary media of geographical information and the elementary objects manipulated, almost all of maps adopt the layer-based model to represent geographic information in the existent GIS. However, it is difficult to extend the map represented in layer-based model. Furthermore, in Web-Based GIS, It is slow to transmit the spatial data for map viewing. In this paper, for solving the questions above, we have proposed a new method for representing the spatial data. That is scale-based model. In this model we represent maps in three levels: scale-view, block, and spatial object, and organize the maps in a set of map layers, named Scale-View, which associates some given scales.Lastly, a prototype Web-Based GIS using the proposed spatial data representation is described briefly.     

Exciton Seebeck in Molecular Systems

Various applications relevant to the exciton dynamics,such as the organic solar cell,the large-area organic light-emitting diodes and the thermoelectricity,are operating under temperature gradient.The potential abnormal behavior of the exicton dynamics driven by the temperature difference may affect the efficiency and performance of the corresponding devices.In the above situations,the exciton dynamics under temperature difference is mixed with     

Achieving Unusual States of Matter Under High Pressure

The elongation method,originally proposed by Imamura was further developed for many years in our group.As a method towards O(N)with high efficiency and high accuracy for any dimensional systems.This treatment designed for one-dimensional(ID)polymers is now available for three-dimensional(3D)systems,but geometry optimization is now possible only for 1D-systems.As an approach toward post-Hartree-Fock,it was also extended to