新型镁质膨胀材料的制备与性能研究

主要研究了以多种富镁矿物为原料，制备适合于大掺量粉煤灰混凝土的新型镁质膨胀材料，用以补偿大坝由于温度应力引起的收缩。通过在不同粉煤灰掺量的水泥浆体中，外掺不同比例的新型镁质膨胀材料和传统MgO膨胀剂，研究水泥浆体压蒸膨胀率的变化规律以及40℃水中长龄期养护膨胀率的变化过程及趋势。结果表明，随着膨胀材料掺量的增加，膨胀率相应增加。随着养护龄期的延长，膨胀率相应增大，到120d左右，膨胀趋于平缓。粉煤灰对传统MgO膨胀剂具有明显的抑制作用，且随着粉煤灰掺量的增加，抑制作用加强。新型镁质膨胀材料能很好的改善抑制作用，从而满足大掺量粉煤灰混凝土工程的要求。     

活性MgO碳化固化土的抗硫酸盐侵蚀性研究

既有研究表明,活性MgO固化土经CO2碳化几小时后其强度能达到甚至超过28 d的水泥固化土强度,碳化反应生成镁的碳酸化合物能有效降低固化土的含水率和孔隙率,提高土颗粒胶结能力。通过室内试验进一步研究碳化固化土的抗硫酸盐侵蚀特性。采用硫酸钠溶液、硫酸镁溶液浸泡碳化固化土,对浸泡不同龄期后的碳化固化土进行无侧限抗压强度试验和微观测试（XRD,SEM和MIP）,并与硫酸盐侵蚀后的水泥固化土进行试验对比。结果表明：活性MgO固化粉土碳化3 h,试样的无侧限抗压强度可达5 MPa左右,经硫酸盐溶液浸泡28 d后其强度基本保持不变,试样质量变化也不大;而水泥土试样的早期强度（7 d）则有一定增长,随龄期增长,强度大大降低,质量则明显增长。通过对硫酸盐侵蚀前后的碳化土的微观机制分析,发现活性MgO碳化固化土中的镁碳酸化合物的化学成分并未发生明显变化,孔隙结构也未明显改变,从而保证其强度稳定。因此,活性MgO固化粉土碳化后具有比水泥固化土更强的抗硫酸盐侵蚀能力。     

基于ArcGIS的月球虹湾地区数字地质图编制研究

虹湾幅月球数字地质图是中国首次编制的关于月球地质演化的地质图,应用的主要数据资料来源于"中国首次月球探测工程"嫦娥一号CCD影像数据、DEM数据,结合Clementine750nm影像数据,主要月坑的高分辨率图片,同时结合前人的研究成果,如主要矿物元素含量分布图、多波段反射率特征分布图等编制完成。所有的数据处理应用的是ArcMap平台,同时结合使用了MapGIS软件和Photoshop软件,数据模型采用Geodatabase地理数据模型。详细介绍了基于ArcGIS平台编制月球数字地质图的工作流程,编制方法及依据、编制规则及数据库的建立等,为今后开展月球数字地质图的编制积累了经验。     

利用盐湖氯化镁-石灰制备硅热法炼镁用煅白的实验研究

以盐湖副产水氯镁石为原料,与一定比例的石灰反应得到氢氧化镁和氢氧化钙的混合沉淀物,该混合物经过滤、洗涤、烘干后在一定温度下煅烧得到符合皮江法炼镁用的合成煅白。实验结果表明,该工艺是可行的,在石灰/氯化镁摩尔比2.05~2.10：1,反应时间1.5,煅烧温度为800℃,煅烧时间为60min时,合成的煅白中钙镁摩尔比： 0.95~1.07：1,煅白的平均水活度达34%,符合硅热法炼镁用中间原料煅白的参数条件。该技术可为利用盐湖氯化镁制备金属镁新工艺开发提供了数据参考。     

溶胶-凝胶法制备纳米氧化镁研究

以硝酸镁和硬脂酸为原料,用溶胶—凝胶(Sol-Gel)法制备得到了纳米氧化镁微粒,并用热重(TG)分析、X-射线粉末衍射(XRD)、红外光谱(IR)和透射电镜(TEM)等对该纳米微粒的结构与形貌进行了表征。结果表明,控制Mg(NO3)2和CH3(CH2)16COOH物质的量比为1∶4,在90℃反应20 min并于360℃热处理4 h,得到立方相氧化镁纳米微粒,形貌为椭球体,分散性好,平均粒径约为33 nm。     

特殊形貌MgO材料的研究

科技的发展、进步对材料的要求越来越高,随之而来的是各种特殊功能的复合材料的问世。作为复合材料,增强改性添加剂的特殊形貌MgO材料也获得了长足的发展。系统介绍了晶须MgO、纳米MgO及其他特殊形貌MgO的用途和制备方法。指出盐湖镁资源的综合利用和可持续发展并兼顾环境保护是今后研究开发的方向。     

Electron density distribution and bond critical point properties for forsterite, Mg2 SiO4, determined with synchrotron single crystal X-ray diffraction data

A generalized X-ray scattering factor model experimental electron density distribution has been generated for the orthosilicate forsterite, using an essentially extinction and absorption free set of single crystal diffraction data recorded with intense, high energy synchrotron X-ray radiation (E=100.6 keV). A refinement of the model converged with an R(F)=0.0061. An evaluation of the bond critical point, bcp, properties of the distribution at the (3, –1) stationary points for the SiO and MgO bonded interactions, yielded values that agree typically within ~5%, on average, with theoretical values generated with quantum chemical computational strategies, using relatively robust basis sets. On the basis of this result, the modeling of the experimental distribution is considered to be adequate. As the bcp properties increase in magnitude, the MgO and SiO bonds decrease in length as calculated for a number of rock forming silicates. As asserted by Coppens (X-ray charge densities and chemical bonding. Oxford University Press, Oxford, 1997), large negative ²(r_c) values, characteristic of shared interactions involving first row atoms, may not be characteristic of closed shell covalent bonded interactions involving second row Si, P and S atoms bonded to O. This study adds new evidence to the overall relatively good agreement between theoretical bcp properties generated with computational quantum strategies, on the one hand, and experimental properties generated with single crystal high energy synchrotron diffraction data on the other. The similarity of results not only provides a basis for using computational strategies for studying and modeling structures, defects and the reactivity of representative structures, but it also provides a basis for improving our understanding of the crystal chemistry of earth materials and the character of the SiO bonded interaction.     

甘肃金川铜镍矿石中MgO对浮选的影响

金川铜镍矿浮选精矿中MgO高,影响闪速熔炼。对金川主力矿山二矿区矿石中MgO分布特征与赋存状态的研究,分析影响浮选过程中MgO难以抑制原因。认为矿石本身MgO含量高、矿石蚀变严重、含镁矿物自然可浮性的良好是造成精矿中MgO高的主要原因。提出研究含镁矿物的浮选特性和矿石的矿物组成特点是精矿降镁的前提。     

Effect of pressure on the thermal expansion of MgO up to 8.2 GPa

Isobaric volume measurements for MgO were carried out at 2.6, 5.4, and 8.2 GPa in the temperature range 300–1073 K using a DIA-type, large-volume apparatus in conjunction with synchrotron X-ray powder diffraction. Linear fit of the thermal expansion data over the experimental pressure range yields the pressure derivative, (∂α/∂P) _T , of −1.04(8) × 10⁻⁶ GPa⁻¹ K⁻¹ and the mean zero-pressure thermal expansion α_{0, T}  = 4.09(6) × 10⁻⁵ K⁻¹. The α_{0, T} value is in good agreement with results of Suzuki (1975) and Utsumi et al. (1998) over the same temperature range, whereas (∂α/∂P) _T is determined for the first time on MgO by direct measurements. The cross-derivative (∂α²/∂P∂T) cannot be resolved because of large uncertainties associated with the temperature derivative of α at all pressures. The temperature derivative of the bulk modulus, (∂K _T/∂T) _P , of −0.025(3) GPa K⁻¹, obtained from the measured (∂α/∂P) _T value, is in accord with previous findings. Received: 2 April 1999 / Revised, accepted: 22 June 1999     

Accuracy in measurements and the temperature and volume dependence of thermoelastic parameters

To obtain the temperatureT and volumeV (or pressureP) dependence of the Anderson-Grüneisen parameter _T , measurements with high sensitivity are required. We show two examples:P, V, T measurements of NaCl done with the piston cylinder and elasticity measurements of MgO using a resonance method. In both cases, the sensitivity of the measurements leads to results that provide information about _T (,T), where V/V ₀ andV ₀ is the volume at zero pressure. We demonstrate that determination of _T leads to understanding of the volume and temperature dependence ofq=( ln / lnV) _T over a broadV, T range, where is the Grüneisen ratio.