关于水文地质水井钻探工程中新型自动解垢过滤器的分析研究

水文地质钻探、水井钻探是探矿工程的重要组成部分。随着水资源需求量的增加和生态环境保护要求的提高,水文地质和水井钻探工程显得更为重要。在其成井过程中,常见过滤器腐蚀结垢,直接影响井眼进水量和抽水效果,甚至导致过滤器和井眼报废。俄罗斯南方国立技术大学Третьяк А.Я.教授等人发明了自动解垢过滤器,解决了过滤器腐蚀结垢问题。     

A new preparation process of coal-based magnetically activated carbon

Fe/C-based magnetically activated carbon （MAC） was obtained by carbonizing and activating its precursor, that was prepared by co-precipitation of anthracite coal impregnated in ferric chloride solution. The effect of the concentrations of FeC13 and pH of solution on BET surface area, pore volume and magnetic properties of the MAC was studied by BET N2 adsorption and VSM method. The results indicated that the magnetization of MAC gradually increases with increasing concentration of FeC13 and pH value of solution, and BET surface area was inclined to fluctuation. The largest BET surface area and magnetization of MAC were 1327.5 m2/g and 35.56 emu/g, respec- tively. The form of magnetic matter in the magnetically activated carbon was mainly Fe3C by X-ray powder diffrac- tion （XRD） and magnetic attraction test.     

原位磁化X射线粉末衍射法测还原铁粉的微观磁致伸缩系数

首次报导X射线粉末衍射法测量铁粉晶胞的磁致伸缩系数。还原铁粉样品原位磁化后 ,铁立方晶胞产生磁致伸缩效应 ,晶胞参数的变化引起衍射峰位置和晶面间距的变化。实验测得铁晶胞λ1 0 0 为 3 .3 3× 10 - 4,此结果表明铁晶胞的微观磁致伸缩系数比棒状、薄膜或粉末压片的系数大约 16倍。对此现象进行了合理的理论解释 ,指出大块材料中的粉末多晶之间具有较大的空隙 ,从而使得宏观磁致伸缩系数变小     

磁法在煤火探测中的应用

对采自宁夏汝箕沟煤田上覆盖层的原岩样品在温度作用下的磁性变化进行了系统研究.通过分析煤火区不同燃烧阶段围岩的温度变化情况,对原岩样品进行了模拟“燃烧”试验,试验结果表明,岩石磁性在不同温度作用条件下存在明显差异,从而从岩石磁性的角度讨论了磁法勘探圈定煤田火烧区的可行性.最后,采用人机交互法对地面实测磁异常剖面进行反演,有效地圈定了煤火区着火点的位置及范围.     

Paleomagnetic studies of the Late Mesozoic deformation stage in the southern Primorye region

The analysis of paleomagnetic data available for the southern Primiorye region revealed that the studied objects were magnetized under regional remagnetization presumably during the Late Mesozoic folding and this magnetization can be interpreted as being synfolding. The interpretation is based on the parameter that characterizes the folding completion degree immediately before regional remagnetization. It is shown that the relaxation of Late Mesozoic horizontal stresses was irregular. The obtained estimates of the degree of folding completion are consistent with the available geological data and Talitskii’s model for tectonic deformations.     

新疆阿希金矿床地球物理特征

阿希金矿床含金石英脉具高阻、高极化、高密度特征，蚀变英安岩呈低阻、低极化、高密度和无磁性，构造破碎带为低阻、低密度特征。以下石炭统阿恰勒河组及大哈拉军山组部分岩性为背景场，并在二者接触部位陪衬出次一级高阻、高极化、微磁，较明显的低负自然电位；位于磁场负极值间的△Ｚ值趋于零的过渡平台的出现；地表低的自然伽马射线；矿体沿一定位移方向ηｓ异常出现等，是寻找该类型矿床的重要物性标志。     

浙江丽水Ⅰ盆地白垩纪古地磁学研究

在浙江丽水Ⅰ盆地白垩系采集古地磁样品０１个,经测试得出晚白垩世末期的古地磁偏角为２４．７５°,古地磁倾角为４８．１４°,古纬度为２９．１６°Ｎ,为中国东部晚白垩世末期边南移、边顺时针旋转的区域性构造运动提供了证据。     

Automated AF-demagnetization on the 2G-Enterprises through-bore,cryogenic magnetometer

Since the early sixties, alternating field demagnetization (AFD) has been a standard laboratory technique for demagnetizing rocks to expose the multicomponent structure of their natural remanent magnetization (NRM). In the majority of AFD implementations, however, the procedure remains as labour-intensive as ever. The implementation that we have developed at the Australian Geological Survey Organisation, automates the procedure for AFD based on the static method, and results in significant productivity and efficiency gains without compromising data quality. A properly formulated procedure for static AFD may be the only method of retrieving higher-coercivity components of natural remanence in samples prone to developing gyroremanence at higher alternating fields (AFs). Our AFD environment comprises: a 2G-Enterprises through-bore, cryogenic magnetometer; 2G AF-coils and control equipment; and personal computer software, developed by us, to control all procedural aspects for a complete AFD of a sample including, importantly, a counteracting procedure to neutralize the effects of gyroremanence build-up at higher AFs. With our system, AFD of 8 samples/day, each of 20+ steps, requires only 20 min of user attention compared with a full day for conventional systems.     

黄河兰州段2018年汛期沉积物的磁学特征研究: 对古洪水重建的启示

现代洪水沉积物的沉积学特征研究是开展古洪水重建的一项基础工作.2018年黄河汛期洪水沉积物在兰州体育公园形成了一道天然堤.对该天然堤剖面的岩石磁学研究显示：沉积物中的磁性矿物既有磁铁矿,又有赤铁矿/针铁矿.磁化率、饱和等温剩磁、非磁滞剩磁、S-ratio和L-ratio等参数在剖面上没有明显变化,指示2018年洪水沉积物源区、磁性矿物的种类和含量变化不显著.剖面下部（66~110 cm）沉积物的磁化率各向异性（AMS）椭球最大轴偏角集中分布（K₁-Dec=22.8°±10.3°）,上部（0~64 cm）沉积物的磁化率最大轴偏角在上半平面内随机分布;下部沉积物的磁性矿物粒度指标（χ_ARM/χ和χ_ARM/SIRM）和天然剩磁（NRM）强度低于上部;指示洪水沉积物的下部和上部分别形成于2018年黄河二号和三号洪水期间.由于二号洪水流量及水位陡升陡降、持续时间短,三号洪水水位升降相对缓慢、持续时间长;造成了两次洪水沉积物的AMS特征、χ_ARM/χ、χ_ARM/SIRM以及NRM强度差异.本研究揭示洪水沉积物的磁学参数能够灵敏地响应不同水动力条件和持续时间的洪水期次,从而具有高分辨率区分洪水事件的潜力.

     

Where did rotational shortening occur in the Himalayas? - Inferences from palaeomagnetic remagnetisations

In metacarbonates of the Lesser (LH) and Tethyan (TH) Himalayas of Kumaon/Garhwal (N-India) characteristic remanent magnetisations carried by pyrrhotite (unblocking temperatures: 250-330°C) and magnetite (demagnetising spectra: 15-50 mT) have been identified. Negative fold tests indicate remanence acquisition after the main folding phase, which is of short-wavelength character and occurs during the early orogenese of the Himalayas. A thermal or thermochemical origin of magnetisation is likely and the age of remanence acquisition is indicated to be about 40 Ma by ⁴⁰K/³⁹Ar cooling and ⁴⁰Ar/³⁹Ar crystallisation ages. In the Kumaon LH a long-wavelength tilting is indicated by a distribution of the remanence directions along a small-circle in N-S direction. Steepening of the remanence directions in the TH related to ramping on the Main Central Thrust (MCT) was not observed, in contrast to other related studies. In the Alaknanda valley of LH a 38±8 Ma age of remanence acquisition is supported by comparison of observed inclinations to the apparent polar wander path of India. Clockwise rotation of 20.3±11.7° (LH/Alaknanda valley) and 11.3±8.5° (TH) with respect to the Indian plate is observed, indicating that there is no significant evidence for rotational shortening along the MCT since about 40 Ma. Our results suggest that most of rotational underthrusting and oroclinal bending has not been accommodated by the MCT, but by the main thrusts south of it. The latest Miocene/Pliocene age of the Main Boundary Thrust indicates that oroclinal bending is a late-orogenic process.