婆罗洲北部岩石密度和磁化率特征及其对南海南部前新生界岩性识别的约束

基于540块样品的体积磁化率-比重测量和矿物-岩性鉴定结果,分析了婆罗洲北部岩石类型、密度、磁化率特征,据此明确重磁资料对于南海南部中生界岩性识别的适用性.结果表明婆罗洲北部发育3类25种岩石,以发育中基性火成岩和外碎屑沉积岩为主,发育少量内源沉积岩、酸性火成岩和变质岩.具有极强磁性-强磁性,高密度-中等密度特征的岩石多为火成岩和凝灰质砂岩及其变质岩.弱磁性-无磁性、中等-极低密度特征的岩石多为砾岩、砂岩、粉砂岩、泥岩和煤等.弱-逆磁性、高-中等密度的岩石多为灰岩和硅质岩.新生界岩石具有密度较低、磁化率中等的特征.中生界岩石具有密度中等、磁化率中高的特征.前中生界岩石具有密度高、磁性低的特征.结合分布特征可知,前中生界岩石产生局部弱重力异常,中生界沉积岩产生区域性的负重力异常,火成岩产生区域性的正重力异常.南海南部的区域性高磁力异常来源于中生代的基性火成岩(及其变质岩),区域性中等磁力异常可能来源于酸性火成岩(及其变质岩).据此进行了南海南部中生界岩性的识别,结果表明南海南部存在大面积的中生界沉积岩分布区,认为南海南部中生界地层具有油气勘探潜力.     

秦岭造山带晚三叠世糜署岭岩体的岩石磁学及磁组构可靠性约束

近年来,针对秦岭造山带晚三叠世花岗岩体侵位机制的巨大争议,一些研究采用磁组构方法分析了岩体的内部组构特征及其与区域构造的关系,提出了具有重要意义的新认识.然而,目前这些研究均缺乏对岩体磁组构本质意义的分析,利用该方法约束岩体内部组构的可靠性并不十分清晰.针对这一问题,本文以秦岭造山带内具典型代表性意义的晚三叠世糜署岭花岗岩体为例,开展了该岩体的磁组构、岩石磁学、矿物形态组构和显微构造的综合研究.结果表明,糜署岭岩体的磁化率总体较低,属钛铁矿系列花岗岩.绝大部分样品的磁化率受控于顺磁性的黑云母等铁镁硅酸盐矿物,部分高磁化率样品包含了少量多畴磁铁矿等铁磁性组分的贡献,且随磁化率增大,铁磁性组分的贡献更为明显.样品的磁组构也主要是黑云母组构或由黑云母与磁铁矿的亚组构复合而成.由于样品中磁铁矿含量较低且与黑云母密切共生,磁组构与黑云母形态组构基本一致,因此,黑云母与磁铁矿的亚组构基本共轴.糜署岭岩体的磁组构本质上等同于黑云母组构,反映了黑云母等页硅酸盐矿物在岩体中的分布,可以有效的指示岩体的内部构造特征.宏观和显微构造观察还显示,糜署岭岩体的内部组构形成于岩浆侵位的晚期阶段,叠加了同岩浆期区域构造的关键信息,是从岩体构造角度开展区域构造演化的良好载体.     

泥河湾盆地大长梁剖面河湖相沉积物的岩石磁学性质

以热磁分析为主,对中国北方泥河湾盆地更新世河湖相地层中灰绿色粉砂和灰黄色粉砂/细砂两种典型沉积物进行了详细的岩石磁学研究,有效确定了这两类沉积物中磁性矿物的种类、粒度特征以及加热过程中磁性矿物的变化过程和产物,并对其包含的古环境意义进行了初步探讨.灰绿色粉砂样品主要含有磁铁矿和赤铁矿两种磁性矿物,磁性相对较弱,颗粒相对较细;灰黄色粉砂/细砂主要含有磁铁矿和磁赤铁矿,磁性相对较强,颗粒相对较粗.在氩气环境中经700℃加热处理后,这两种沉积物中的绿泥石都分解,并生成超细粒（处于超顺磁和单畴颗粒区间）的磁铁矿,导致磁化率大幅升高.因此泥河湾盆地沉积物的热磁特征可以用来检测样品中绿泥石的相对含量,进而反映该地区化学风化作用强度的变化.此外,灰绿色粉砂样品中绿泥石含量比灰黄色粉砂/细砂样品的含量高,在氩气中加热后,磁化率升高幅度也较高,可能反映了化学风化相对较弱的沉积环境.     

甘肃敦煌—阿克塞地区岩(矿)石磁化率特征分析及应用

各类岩(矿)石的磁性差异是进行航磁资料地质解释的物理基础.为全面、系统了解甘肃敦煌—阿克塞地区岩(矿)石的磁性特征,2015—2017年在该区开展了系统的岩(矿)石的磁化率调查工作,实测物性点320处,获得有效磁化率数据10154个.对实测资料进行了详细的分类统计,分析总结了区内沉积岩、侵入岩、火山岩、变质岩、矿石及围岩等各类岩矿(石)的磁性特征,沉积岩一般呈弱或无磁性;火山岩具有中等-强磁性,可引起一定走向的磁异常;基性-超基性岩多具有强磁性,可以引起一定强度、尖锋状或带状的磁异常;中、酸性侵入岩和变质岩磁化率变化范围较大,弱磁性的一般在磁场上无异常显示,中等-强磁性的一般在磁场上表现为带状或团块状异常区;磁铁矿、磁黄铁矿等磁性矿物含量的增多,不同类型矿石磁化率由中等磁性逐渐变为极强磁性.在此基础上将实测磁化率应用于磁性地层、侵入岩圈定,探讨了磁化率与矿产之间的联系.研究结果为该地区高精度航磁资料解释提供了基础资料和参考依据.     

呼伦湖湖泊沉积物磁化率变化的环境磁学机制

对内蒙古呼伦湖地区的研究表明当湖泊水深较大时 (对应于湿润气候 ) ,所沉积的泥质沉积物的磁性较高 ;反之 ,水位低时 (对应于干旱气候 ) ,所沉积的砂性沉积物的磁化率较低 .深入的岩石磁学研究证实 ,来自湖泊流域火山岩中的碎屑磁铁矿广泛地存在于泥质及砂性样品之中 .当湖泊水位较高时 ,在相对的还原条件下 ,在泥质沉积物中形成次生的铁磁性硫化铁矿物 .该磁性矿物叠加在少量的碎屑成因的磁铁矿上 ,主导了泥质沉积物的磁性 ,导致了磁化率的上升     

南岭及邻区中生代含锡花岗岩的多样性:显著的矿物特征差异

南岭及邻区分布一系列与中生代花岗岩有关的锡矿床,这些岩石可以是含角闪石黑云母花岗岩,或是(黄玉)钠长石-(铁)锂云母花岗岩,其岩石化学特征指示它们分别对应于准铝质和过铝质花岗岩.细致的矿物学研究表明它们具有完全不同的矿物学特征.准铝质含锡花岗岩的矿物学特征表现为:(1)角闪石、黑云母、条纹长石等组成特征性的造岩矿物组合:(2)标志性副矿物榍石、磁铁矿等显示其原始岩浆具有较高的氧逸度;(3)含锡矿物为锡石、黑云母、榍石等;(4)锡石的成分比较纯,微量元素含量低.过铝质含锡花岗岩的矿物学特征主要表现为:(1)铁锂云母-锂云母、钾长石、钠长石为典型造岩矿物;(2)富铝矿物黄玉是较常见的副矿物,与花岗岩铝过饱和特征相符;(3)锡石是重要的锡矿物,且富含Nb、Ta.造成两类含锡花岗岩显著矿物学差异的原因可能包括熔体的氧逸度、挥发组分和岩浆分异程度的差异.氧化型准铝质花岗岩熔体中锡以四价为主,这导致锡容易富集在含钛的造岩矿物或副矿物中,在岩浆结晶分异阶段形成富锡矿物;这些富锡矿物可成为含锡花岗岩的标志性矿物.相对还原的过铝质花岗岩熔体中锡以二价为主,不易进入造岩矿物和副矿物,常常在岩浆结晶分异阶段形成岩浆成因的锡石;因此,岩浆成因锡石成为这类花岗岩的重要成矿和找矿标志.岩浆性质和锡在两类花岗岩岩浆中地球化学行为的差异,导致形成的矿床类型有所不同.准铝质花岗岩主要形成岩体浸染型、绿泥石-石英脉型、云英岩型、矽卡岩型等矿床,而过铝质花岗岩除形成云英岩型、矽卡岩型、石英脉型等矿床外,更易形成岩体浸染型锡矿化.     

三门峡盆地晚新生代沉积物磁性载体类型

对三门峡盆地晚新生代沉积岩样品进行岩石磁学研究,通过三轴饱和等温剩磁和剩磁矫顽力实验、交变退磁和热退磁实验及磁化率测定,发现黄土-古土壤、河湖相灰绿层和冲洪积层3种不同岩性的磁载体存在显著差异.即黄土-古土壤以磁铁矿为主,赤铁矿和磁赤铁矿很少;河湖相灰绿色沉积磁性矿物含量较低,主要为赤铁矿和磁铁矿,但磁铁矿较多,此外还有一些不稳定磁性矿物(如针铁矿、菱铁矿等);冲洪积物以磁铁矿和赤铁矿为主,磁铁矿相对较多.     

塔里木盆地南缘8.5 ka以来的黄土岩石磁学特征及其磁化率变化机制

黄土岩石磁学参数是古气候研究中的重要指标,其中磁化率应用最为广泛,并在黄土高原地区取得重大进展,其受控于成壤作用的变化机制也被普遍接受.然而在黄土高原外缘的新疆地区,磁化率的变化机制仍不明确,导致磁化率的古气候意义在该区存在较大争议.本文选取塔里木盆地南缘具有精确年代控制的典型黄土剖面（羊场剖面）开展岩石磁学和高分辨率磁化率研究,利用交叉小波分析方法并结合剖面粒度、矿物及元素特征对该地区磁化率变化机制进行初步探讨.结果显示,羊场剖面的岩石磁学性质主要由粗颗粒软磁性矿物所控制,同时也表现出一定的顺磁性特征.根据载磁矿物和磁化率变化特征可将剖面进一步划分为两个阶段：阶段Ⅰ（8.5~2.5 ka）,载磁矿物以亚铁磁性的磁铁矿为主,磁化率值整体较高;阶段Ⅱ（2.5~0.2 ka）,亚铁磁性矿物依然占据主导地位,但硬磁性矿物和以黄铁矿为代表的顺磁性矿物相对增多,磁化率值显著降低.相关性研究和交叉小波分析表明：阶段Ⅰ磁化率与粗颗粒组分的变化具有一致性,符合"风速论"模式;阶段Ⅱ磁化率不仅与粗颗粒组分具有明显的正相关关系,而且与指示成壤作用强度的频率磁化率百分含量呈现出显著的负相关关系,暗示了阶段Ⅱ的磁化率变化可能受到"风速论"和"还原性成壤"模式的共同影响.本文拓宽了对新疆地区黄土岩石磁学特征及其磁化率变化机制的深入理解,也为利用磁化率恢复新疆及中亚地区全新世以来的古气候变化历史提供了新的线索.     

内蒙古南部麻粒岩中辉石的特征

冀北和内蒙古南部西起酒馆东至涞源,处于华北地台的边缘,这里出露前震旦纪变质岩系,属角闪岩相至麻粒岩相。岩石由斜方辉石、角闪石、石榴石、斜长石、微斜长石、黑云母、石英、单斜辉石、磁铁矿、金红石、磷灰石等矿物组成,以含斜方辉石、角闪石、石榴石为特征。由于矿物含量不等,其中变质     

上海及其邻域居里面与地震活动趋势

一、居里面的计算及其物理、地质意义众所周知,在地壳中,随深度增加地温也逐渐升高,到某一深度,地温会达到铁磁性物质的居里点,铁磁性物质变为顺磁性,磁化率急剧减小,可以认为岩石失去了磁性.因此,利用磁测资料计算的磁性体底界面,在一定条件下可以代表居里点深度.      

南海北部陆区岩石磁化率的矿物学研究

基于2517套现场测量资料,245块岩石样品的体积磁化率测量和详细的岩矿鉴定及硅酸盐全分析结果,结合单矿物磁化率特征及各岩石之间的对比研究,发现岩石磁化率主要受组成岩石的矿物磁化率控制.即岩石磁化率(κr)与组成岩石各个矿物磁化率(κ1)及其体积含量(C2)成正比.例如侵入岩磁化率,κr=-5.68×102Cq+2.8...     

MAGNETIC SUSCEPTIBILITY ANISOTROPY OF VARIOUS ROCK TYPES AND ITS SIGNIFICANCE FOR GEOPHYSICS AND GEOLOGY*

In the interpretation of magnetic anomalies and in paleomagnetism, the anisotropy of magnetic susceptibility is commonly neglected. Nevertheless, this property has basic significance, because, owing to susceptibility anisotropy, the directions of the vectors of induced and remanent magnetization are deflected from the direction of the Earth's magnetic field. Almost all rock types investigated possess higher or lower degree of the susceptibility anisotropy. Effusive and sedimentary rocks have the lowest degree of anisotropy. For the latter, the “masking effect” of the paramagnetic mineral components has some influence on the anisotropy degree due to the low mean susceptibility of sedimentary rocks. Metamorphic and plutonic rocks usually exhibit a considerable degree of anisotropy. The highest degree of anisotropy has been found in the rocks containing ferromagnetic minerals with mimetic fabric. The dependence of the degree of the susceptibility anisotropy on the degree of metamorphism proved to be very complicated; of the rock sequence from slates to gneisses, the transient rocks (roofing slates and mica-schist-gneisses) showed the highest degree of anisotropy. This result can be used in geology for reliable determination of these rock types.     

扬子克拉通太古代崆岭群角闪岩相与麻粒岩相岩石的岩石磁学研究

提供了扬子克拉通太古代基底崆岭群２０件代表性岩石样品的密度与磁性参数的测量结果．结果表明，变碎屑岩与ＴＴＧ（英云闪长－奥长花岗－花岗间长质）片麻岩（１３个样品）的磁化率与饱和剩磁普遍大于斜长角闪岩和辉长岩．前者的磁化率与饱和剩磁平均值分别为１２１３×１０^－６ＳＩ与１９．９４Ａ／ｍ，而后者的则为８０２×１０^－６ＳＩ与１０．７７Ａ／ｍ．变碎屑岩与ＴＴＧ片麻岩呈明显的亚铁磁性状态；斜长角闪岩和辉长岩则以顺磁性或顺磁性与亚铁磁性混合状态分布为主．热磁分析结果表明，变碎屑岩与ＴＴＧ片麻岩的剩磁载体以磁铁矿与磁赤铁矿为主；斜长角门岩和辉长岩则明显含有磁黄铁矿与次要的磁铁矿．变碎屑岩与ＴＴＧ片麻岩的磁性具有很强的非均一性．推断崆岭群中的变碎屑岩为麻粒岩相变质级，视深度相当于大陆下地壳；而斜长角闪岩的变质级明显低于变碎屑岩，可能为角门岩相，视深度相当于中地壳．变碎屑岩与ＴＴＧ片麻岩磁性的强非均一性可能与该区后期广泛发生的混合岩化作用密切相关。     

Physical properties of Vilppula drill cores and petrographic analysis of associated breccias in Keurusselk? impact structure, central Finland

The Mesoproterozoic deeply eroded Keurusselk? impact structure in central Finland is situated within the ??1860?C1890 Ma Central Finland Granitoid Complex. An estimate for the original size of the structure is 30 km, yielding a 5 km wide central uplift with insitu shatter cones and shock metamorphic features in quartz. Petrophysical and rock magnetic properties of the three shallow drill cores (V-001, V-002 and V-003) in the vicinity of the central uplift are determined in order to assess the dimensions of the central uplifts magnetic anomalies. The drill core lithologies consist of schists (metagraywackes), metavolcanic rocks, gneisses and breccia. Petrophysical properties of the drill core rocks show average densities (D) of 2644?C2752 kg/m³, susceptibilities (??) of 160?C761 × 10^?6 SI and natural remanent magnetization (NRM) of 3?C306 mA/m and Koenigsberger Q ratios of 0.1?C10. Rock magnetic measurements with temperature dependence of susceptibility (??-T) curves and hysteresis indicated mostly paramagnetic behaviour. However, a fraction of fine-grained ferromagnetic minerals (pyrrhotite and magnetite) was detected from all lithologies. Breccia veins cutting the parautochthonous subcrater floor show lower values of petrophysical properties (D, ??, NRM, Q) and this could be related to the impact event. Amphiboles and micas in the breccia are strongly altered and replaced by secondary chlorite. Chloritization may indicate widespread impact-induced hydrothermal alteration of the target rocks or it may be related to regional tectonic shearing. However, planar deformation features in quartz, found from shatter cones in the central uplift area, are decorated with fluid inclusions indicating that alteration by post-impact processes was present.     

巴基斯坦Bahawalpur黄土岩石磁学特征及磁化率变化机制研究

风成黄土是陆地上分布最广泛的沉积物之一,记载了各种古气候演化信息.目前巴基斯坦的黄土研究甚少,磁化率与气候对应的变化机制研究尚未开展.本文对位于巴基斯坦印度河平原Bahaw alpur地区新发现的黄土-古土壤剖面进行系统的岩石磁学研究,结合粒度和漫反射光谱(DRS)数据,讨论巴基斯坦黄土的磁化率变化机制.实验结果显示:...     

Anisotropy of magnetic remanence: A brief review of mineralogical sources,physical origins,and geological applications,and comparison with susceptibility anisotropy

The magnetic fabric of rocks and sediments is most commonly characterized in terms of the anisotropy of low-field magnetic susceptibility (AMS). However, alternative methods based on remanent magnetization (measured in the absence of a magnetic field) rather than induced magnetization (measured in the applied field) have distinct advantages for certain geological applications. This is particularly true for; (1) adjunct studies in paleomagnetism, in order to assess the fidelity with which a natural remanence records the paleofield orientation; (2) studies of weakly magnetic or weakly deformed rocks, for which susceptibility anisotropy is very difficult to measure precisely; and (3) quantitative applications such as strain estimation. The fundamental differences between susceptibility and remanence (and their respective anisotropies) are due to several factors: (1) susceptibility arises from all of the minerals present in a sample, whereas remanence is carried exclusively by a relatively small number of ferromagnetic minerals; (2) ferromagnetic minerals are generally more anisotropic than para- and diamagnetic minerals; (3) for ferromagnetic minerals, remanence is inevitably more anisotropic than susceptibility; and (4) a number of common minerals, including single-domain magnetites, possess an inverse anisotropy of susceptibility, i.e., they tend to have minimum susceptibility parallel to the long axis of an individual particle; remanence is immune to this phenomenon. As a consequence of all these factors, remanence anisotropy may generally provide a better quantitative estimate of the actual distribution of particle orientations in a rock sample.Contribution number 9102 of the Institute for Rock Magnetism, University of Minnesota.     

High magnetic susceptibility produced by thermal decomposition of core samples from the Chelungpu fault in Taiwan

We carried out thermomagnetic susceptibility analyses of fault rocks from core samples from Hole B of the Taiwan Chelungpu Fault Drilling Project (TCDP) to investigate the cause of high magnetic susceptibilities in the fault core. Test samples were thermally and mechanically treated by heating to different maximum temperatures of up to 900 °C and by high-velocity frictional tests before magnetic analyses. Thermomagnetic susceptibility analyses of natural fault rocks revealed that magnetization increased at maximum heating temperatures above 400 °C in the heating cycle, and showed three step increases, at 600 to 550 °C and at 300 °C during the cooling cycle. These behaviors are consistent with the presence of pyrite, siderite and chlorite, suggesting that TCDP gouge originally included these minerals, which contributed to the generation the magnetic susceptibility by thermomechanical reactions. The change in magnetic susceptibility due to heating of siderite was 20 times that obtained by heating pyrite and chlorite, so that only a small fraction of siderite decomposition is enough to cause the slight increase of the susceptibility observed in the fault core. Color measurement results indicate that thermal decomposition by frictional heating took place under low-oxygen conditions at depth, which prevented the minerals from oxidizing to reddish hematite. This finding supports the inference that a mechanically driven chemical reaction partly accounts for the high magnetic susceptibility. A kinetic model analysis confirmed that frictional heating can cause thermal decomposition of siderite and pyrite. Our results show that decomposition of pyrite to pyrrhotite, siderite and, to some extent, chlorite to magnetite is the probable mechanism explaining the magnetic anomaly within the Chelungpu fault zone.