微波烧结Al_2O_3陶瓷的研究

简要介绍了微波烧结的特点,对 Ａｌ２ Ｏ３ 陶瓷的微波烧结过程进行了介绍和分析,并同常规烧结进行了对比实验,在此基础上得出了一些结论,为陶瓷微波烧结提供了实验依据     

固相烧结法制备Mn-Zn铁氧体的工艺

采用固相烧结法制备Mn-Zn铁氧体样品,分别探讨了成型压力、预烧温度、烧结气氛、烧结温度对样品的致密性、相、结构及微结构的影响.样品的相组成成分、微结构及密度分别采用X射线衍射仪(XRD)、扫描电镜(SEM)、阿基米德法进行表征.结果表明:成型压力较小时,生胚体及烧结体的密度     

Li掺杂对ZnO陶瓷结构与电学性能的影响

研究了用传统方法在1200～1400℃烧结的ZnO陶瓷，以及用放电等离子体烧结(SPS)方法烧结的ZnO陶瓷的结构特征与电学性能。以ZnO为基添加了不同浓度的LiOH，制备了不同Li掺杂浓度的ZnO陶瓷。研究了掺杂、烧结温度，以及烧结方法等因素对ZnO基陶瓷的微观结构、电学性能的影响。实验表明，用传统方法烧结时，ZnO在烧结温度低于1400℃的情况下难以成瓷，而放电等离子体烧结(SPS)方法可以显著降低烧结温度。ZnO陶瓷的晶粒大小。密度随着烧结温度的增大而增大。在同样的烧结温度下，LiOH含量越大，ZnO基陶瓷的电阻率越大。     

High coercivity FePt-C bulk magnet processed by spark plasma sintering and hot deformation

A high coercivity of 11 kOe has been obtained in spark plasma sintered and hot-deformed Fe₅₃Pt₄₄C₃ bulk magnets. The origin for the high coercivity has been investigated using X-ray diffraction and transmission electron microscopy. The average grain size of the ordered phase was ∼100 nm, which is less than the single domain size of the L1₀-FePt phase. Fe₃C particles were found surrounding the L1₀-FePt grains, which suppress the grain growth. The L1₀ ordering is also found to increase in hot-deformed sample by annealing in a magnetic field of 10 T at 600 °C.     

Exploring the phase diagram of strongly interacting matter; news from SPS and RHIC

Two experimental programs are aiming to study nuclear collisions in the energy regime in order to explore an essential part of the phase diagram of strongly interacting matter. The programs are motivated by observations that indicate a phase transition to take place in this energy domain: the onset of deconfinement. The STAR collaboration proposes an energy scan in the Relativistic Heavy Ion Collider (RHIC) at BNL. The ongoing program of the NA61/SHINE experiment consists of a two-dimensional energy-system size scan in nuclear and elementary collisions. The goal of both programs is to study the properties of the onset of deconfinement and to eventually discover the conjectured critical point of strongly interacting matter. A comparison of the strengths and limitations reveals the complementarity of the two programs.     

Microstructure and mechanical properties of nano-Y2O3 dispersed ferritic steel synthesized by mechanical alloying and consolidated by pulse plasma sintering

Ferritic steel with compositions 83.0Fe–13.5Cr–2.0Al–0.5Ti (alloy A), 79.0Fe–17.5Cr–2.0Al–0.5Ti (alloy B), 75.0Fe–21.5Cr–2.0Al–0.5Ti (alloy C) and 71.0Fe–25.5Cr–2.0Al–0.5Ti (alloy D) (all in wt%) each with a 1.0?wt% nano-Y₂O₃ dispersion were synthesized by mechanical alloying and consolidated by pulse plasma sintering at 600, 800 and 1000°C using a 75-MPa uniaxial pressure applied for 5?min and a 70-kA pulse current at 3?Hz pulse frequency. X-ray diffraction, scanning and transmission electron microscopy and energy disperse spectroscopy techniques have been used to characterize the microstructural and phase evolution of all the alloys at different stages of mechano-chemical synthesis and consolidation. Mechanical properties in terms of hardness, compressive strength, yield strength and Young's modulus were determined using a micro/nano-indenter and universal testing machine. All ferritic alloys recorded very high levels of compressive strength (850–2850?MPa), yield strength (500–1556?MPa), Young's modulus (175–250?GPa) and nanoindentation hardness (9.5–15.5?GPa), with up to 1–1.5 times greater strength than other oxide dispersion-strengthened ferritic steels (<1200?MPa). These extraordinary levels of mechanical properties can be attributed to the typical microstructure of uniform dispersion of 10–20-nm Y₂Ti₂O₇ or Y₂O₃ particles in a high-alloy ferritic matrix.     

Capillary-driven interdiffusion along interphase boundaries in solids

We consider chemical interdiffusion along interphase boundary (IB) between two immiscible solid phases. We derive explicit expressions for capillary-related excess chemical potentials of the atoms diffusing along the IB. The obtained expressions contain both a local term which depends on local curvature of the IB, and a non-local one which depends on overall system geometry and on energy of all surfaces and interfaces in the system. The obtained expressions are employed for describing the sintering of two immiscible two-dimensional solid particles controlled by surface and IB diffusion processes. We demonstrate that the sintering of particles is accompanied by relative rigid-body rotation of the particles even for fully isotropic surfaces and interphase boundaries.     

选区激光烧结瞬态温度场模拟与测试方法研究

采用有限元方法,考虑实际的边界条件和热物性参量的变化,对Al2O3覆膜陶瓷粉末的选区激光烧结过程瞬态三维温度场进行动态模拟.通过比色测温法对红外热成像系统的发射系数进行修正后,对选区激光烧结过程瞬态温度场进行测试.数值模拟和实测结果显示,两者吻合较好.     

选择性激光烧结成型件密度的支持向量回归预测

根据不同工艺参数（层厚、扫描间距、激光功率、扫描速度、加工环境温度、层与层之间的加工时间间隔和扫描方式）下的选择性激光烧结成型件密度的实测数据集,应用基于粒子群算法寻优的支持向量回归（SVR）方法,建立了加工工艺参数与成型件密度间的预测模型,并与BP神经网络模型进行了比较.结果表明：基于相同的训练样本和检验样本,成型件密度的SVR模型比其BP神经网络模型具有更强的内部拟合能力和更高的预测精度;增加训练样本数有助于提高SVR预测模型的泛化能力;基于留一交叉验证法的SVR模型的预测误差最小.因此,SVR是一种预测选择性激光烧结成型件密度的有效方法. 关键词： 选择性激光烧结 密度 支持向量机 回归分析     

Effects of sintering temperature and Bi2O3 content on microstructure and magnetic properties of LiZn ferrites

The effects of sintering temperature and Bi₂O₃ content on the microstructure and magnetic properties of lithium–zinc (LiZn) ferrites prepared by a conventional ceramic method were investigated. The results show that the densification behavior and grain growth rate were greatly improved by the addition of Bi₂O₃, because a liquid phase sintering occurred during the sintering process at high temperature due to the low-melting point of Bi₂O₃ (825 °C). X-ray diffraction (XRD) patterns of the slightly doped samples did not reveal the appearance of any phase other than spinel LiZn ferrite. However, the secondary phase of perovskite BiFeO₃ was detected for Bi₂O₃ content of more than 0.25 wt%. The studies further show that Bi oxide was present at grain boundary, and promoted the grain growth as reaction center at lower temperature. A high saturation magnetization, squareness ratio, minimum ferromagnetic resonance linewidth and low coercive force were obtained for the sample with 1.00 wt% Bi₂O additive at lower sintering temperature (1100 °C).