The relationship between the magnetic and strain fabrics of some haematite-bearing Welsh slates

The anisotropy of magnetic susceptibility and the natural remanent magnetization of haematite-bearing Welsh Cambrian slates, showing a gradation in degree of deformation, have been related to the known strain of these rocks. An approximate quantitative relationship between strain and magnetic susceptibility anisotropy has been deduced, which would allow rapid strain estimation in this region by magnetic analysis.     

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(κi)及其体积含量(Ci)成正比.例如侵入岩磁化率,κr= -5.68×102Cq +2.86×102Cf +3.28×102Ca +1.18×104Cb +1.27×104Cam +5.35×105Cm;其中多项式各项的系数是与该矿物磁化率值成正比的常数,C为该矿物在该岩石中的体积含量,依次为石英q(κ=-1.3)、斜长石f(κ=0.01)、碱性长石a(κ=0.01)、黑云母b(κ=100)、角闪石am(κ=80)和磁铁矿m(κ=100000).对区内火山岩、侵入岩、沉积岩和变质岩磁化率研究发现,其他三类岩石磁化率与其组成矿物磁化率的关系和侵入岩的情况相同,矿物对岩石磁化率的贡献顺序为铁磁性矿物>顺磁性矿物>逆磁性矿物.其中,火成岩磁化率变化大,主要取决于岩石中磁铁矿、角闪石和黑云母的含量;沉积岩多为无磁性、弱磁性,其磁化率主要由黑云母、碱性长石及岩屑提供;变质岩的磁性变化较大,从无磁性到极强磁性,主要决定于其原岩的类型,副变质岩(沉积原岩)磁化率类似于沉积岩类,正变质岩(火成原岩)类似于火成岩类;石英岩和碳酸盐岩是所有岩石中磁性最弱的.岩石蚀变会对其磁化率产生显著性影响,通常,黑云母、角闪石等铁镁硅酸盐矿物经蚀变会因形成含铁质氧化物而使岩石的磁化率升高;长石等弱顺磁矿物的粘土矿化、绢云母化会升高磁化率而碳酸盐化、高岭土化作用会使磁化率降低;岩石的绿泥石化会增加磁化率;含铁磁性矿物的岩石风化时会因高磁性组分破碎、流失而致使岩石的磁化率降低.从岩石磁化率与其组成矿物的磁化率之间的关系,推测地质体的总磁化率与构成地质体各个岩石的磁化率-体积含量之间也应存在类似关系.     

塔里木盆地前寒武地层岩石磁化率

在塔里木盆地前寒武结晶基底研究过程中,为了准确建立地层地磁模型,对库鲁克塔格地区岩浆岩、柯坪地区沉积岩、塔什库尔干地区变质岩地层进行系统取样及岩石薄片鉴定和准确命名,并测量岩石密度、磁化率.研究发现:①库鲁克塔格地区:基性、超基性岩蛇纹石化析出磁铁矿,磁化率剧烈变化,而中、酸性侵入岩磁化率随黑云母含量增加而增大;②柯坪...     

The origin of cleavage in the light of magnetic anisotropy investigations

The cleavage origin in rocks ranging from unmetamorphosed sediments, through slates to phyllites of the Nízký Jeseník Mts. (northern Moravia, Czechoslovakia), which show a range of deformation styles, from undeformed through fracture and slaty cleavage to the development of metamorphic foliation, was studied by means of magnetic anisotropy. These studies have shown that the fracture cleavage probably originated during a post-plastic rock deformation. Therefore the orientation of the fracture cleavage with respect to the strain-tensor components cannot be studied by means of magnetic anisotropy. The magnetic fabric of rocks with slaty cleavage was generated through componental movements during the ductile rock deformation. The slaty cleavage developed perpendicularly to the maximum shortening direction. In the rocks exhibiting macroscopically observable marks of slippage along the slaty cleavage, the slippage probably took place after the slaty cleavage developed, when the rock ductility was lower. The metamorphic foliation developed from the slaty cleavage in the course of continuous strain.     

核磁共振测井在火成岩地层应用的适应性分析

火成岩岩石具有高磁化率特征,与沉积岩差别明显,岩石的高磁化率会对核磁共振信号产生显著影响,开展核磁共振测井在火成岩地层应用的适应性分析研究,为广泛使用核磁共振测井用于火成岩储层评价提供参考.采用理论模拟、实验分析及实际测井资料相结合的方法,分析了高磁化率岩石的核磁共振响应特征.分析结果表明,火成岩岩石具有很高的磁化率,从酸性火成岩到基性火城岩,岩石的磁化率一般是逐渐增大的.高磁化率岩石孔隙内部会产生强梯度磁场,孔隙内部的磁场梯度越强,核磁共振的T2谱前移越明显,核磁信号衰减幅度也越大,核磁分析孔隙度与常规分析的孔隙度误差也越大;相同岩石磁化率情况下,岩石孔径越小,岩石孔隙内部磁场梯度越强,核磁信号衰减越大,核磁共振测井计算的孔隙度也越低.因此,核磁共振测井与岩性有关系,核磁共振测井会受到高磁化率岩石的显著影响.核磁共振测井在部分火成岩,尤其在中基性火成岩和小孔径火成岩储层中应用具有很大的局限性.     

Magnetic susceptibility anisotropy,strain, and progressive deformation in Permian sediments from the Maritime Alps (France)

The relationships among magnetic susceptibility anisotropy, finite strain, and progressive deformation have been studied in Permian red shales and slates of the Maritime Alps (southeastern France). These rocks contain deformed reduction spots which serve as finite strain indicators. The magnetic fabric of undeformed regions is modified during deformation to yield characteristic magnetic susceptibility anisotropy patterns and a magnetic equivalent of the deformation path derived from strain measurements. The magnetic fabric changes progressively from oblate to prolate, and back to oblate as deformation increases. The quantitative relationships between natural strain and magnetic anisotropy in these rocks have been determined. They differ between the less and more deformed areas, perhaps due to a change in deformation mechanism accompanying an increase in metamorphism. The relationships provide a rapid means of strain determination using magnetic measurements but their variation emphasizes the need for local structural control.     

岩石磁组构对剩磁稳定性的制约探讨: 以印支地块中生代碎屑岩和拉萨林周盆地设兴组红层为例

岩石磁组构因能提供磁性矿物晶体形状、排列方式等赋存信息而被广泛应用于判别岩石剩磁是否受到了后期构造应力的显著影响; 但常规岩石磁化率各向异性(AMS)是否能够准确限定岩石剩磁的稳定性, 目前尚无深入探讨.本文以印支地块Nakhon Thai盆地中生代Nam Phong、Phu Kradung和Phra Wihan组三套碎屑岩样品及拉萨地块林周盆地设兴组红层样品为例, 通过岩石磁化率组构和剩磁组构的对比分析发现, 尽管Nam Phong组绝大多数样品和Phu Kradung组全部样品的AMS组构显示其具有铅笔状至强劈理过渡型构造变形组构特征, 但高场等温剩磁各向异性(hf-AIR)显示其高矫顽力赤铁矿所携带的特征剩磁组构仍具有典型沉积组构特征, 表明其以赤铁矿为主的载磁矿物未遭受后期构造应力的显著影响, 仍然能够准确记录岩石形成时期的古地球磁场方向.另一方面发现有且仅有剩磁组构才是判别碎屑沉积岩特征剩磁是否遭受了后期构造应力影响的充分必要条件.也就是说, 如果岩石剩磁组构(如以赤铁矿为主要载磁矿物的岩石hf-AIR组构)指示其原始沉积组构已被构造组构显著叠加或取代, 则必然说明该岩石剩磁方向已受到构造应力的作用而发生了显著偏转, 因而不能直接用于构造演化和古地理重建等块体运动学研究.

     

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.     

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.

     

Sources of magnetic susceptibility in a slate

Magnetic susceptibility and its anisotropy in the Borrowdale Volcanic slates at Kentmere in the English Lake District are attributed largely to preferred orientation of a paramagnetic chlorite of diabantite-ripidolite composition. In units of 10⁻⁶ cgs/g, the principal susceptibilities for the slates are 9.61; 9.42; 8.69 and for the chlorite grains the minimum anisotropy is represented by principal susceptibilities of 11.57; 11.22 and 9.15. Because the magnetic susceptibility is carried by a tightly packed, matrix-forming mineral that has recrystallised during the deformation it is not possible to imagine simple grain rotation as being responsible for the anisotropy of susceptibility.     

Changes of anisotropy of the magnetic susceptibility of rocks induced by a magnetic field

Summary The changes of the anisotropy of magnetic susceptibility of igneous rocks, induced by a magnetic field, are studied. It is proved that changes in the degree of anisotropy of susceptibility and of the orientation of the susceptibility ellispoid of specimens occur due to the configuration of the domain structure under the effect of the magnetic field. The influence of this effect on the total anisotropy of rocks depends on the degree of anisotropy due to the shape factor and on the stability of the domain structure. A model concept is presented, explaining the qualitatively different pattern of the changes of the anisotropy of susceptibility under the effect of the magnetic field in various directions of the specimens.     

Magnetic Anisotropy as an Aid to Identifying CRM and DRM in Red Sedimentary Rocks

To further evaluate the potential of magnetic anisotropy techniques for determining the origin of the natural remanent magnetization (NRM) in sedimentary rocks, several new remanence anisotropy measurement techniques were explored. An accurate separation of the remanence anisotropy of magnetite and hematite in the same sedimentary rock sample was the goal.In one technique, Tertiary red and grey sedimentary rock samples from the Orera section (Spain) were exposed to 13 T fields in 9 different orientations. In each orientation, alternating field (af) demagnetization was used to separate the magnetite and hematite contributions of the high field isothermal remanent magnetization (IRM). Tensor subtraction was used to calculate the magnetite and hematite anisotropy tensors. Geologically interpretable fabrics did not result, probably because of the presence of goethite which contributes to the IRM. In the second technique, also applied to samples from Orera, an anisotropy of anhysteretic remanence (AAR) was applied in af fields up to 240 mT to directly measure the fabric of the magnetite in the sample. IRMs applied in 2 T fields followed by 240 mT af demagnetization, and thermal demagnetization at 90°C to remove the goethite contribution, were used to independently measure the hematite fabric in the same samples. This approach gave geologically interpretable results with minimum principal axes perpendicular to bedding, suggesting that the hematite and magnetite grains in the Orera samples both carry a depositional remanent magnetization (DRM). In a third experiment, IRMs applied in 13 T fields were used to measure the magnetic fabric of samples from the Dome de Barrot area (France). These samples had been demonstrated to have hematite as their only magnetic mineral. The fabrics that resulted were geologically interpretable, showing a strong NW-SE horizontal lineation consistent with AMS fabrics measured in the same samples. These fabrics suggest that the rock's remanence may have been affected by strain and could have originated as a DRM or a CRM.Our work shows that it is important to account for the presence of goethite when using high field IRMs to measure the remanence anisotropy of hematite-bearing sedimentary rocks. It also shows that very high magnetic fields (>10 T) may be used to measure the magnetic fabric of sedimentary rocks with highly coercive magnetic minerals without complete demagnetization between each position, provided that the field magnetically saturates the rock.     

Anisotropy of magnetic susceptibility parameters: Guidelines for their rational selection

Twenty-eight parameters used to characterize measurements of the anisotropy of magnetic susceptibility are compared theoretically in this work by introducing the concept of the field of susceptibility tensors, which allows the representation of parameters as families of lines in a plane. It is demonstrated that the foliation and lineation parameters are but a special case of the shape parameters, implying that the resolution of these two rock fabric elements using AMS measurements alone is more an artifact of the numerical range of definition of some parameters than a quantification of two physically independent features. Also, it is shown that parameters presumably of the same type do not necessarily yield equivalent interpretation of results in a qualitative sense, and therefore, caution should be strongly exercised when parameters are to be selected. Paramters quantifying the degree of anisotropy are, in general, equivalent to each other because of the very small departure observed in natural rocks from the isotropic case. However, a final consideration of the possible ability to differentiate rock types and a convenient range of values allowing expression of the degree of anisotropy in a well-defined percentage are pointed out as the main factors to be considered before selecting one parameter within this class.     

A combined rock magnetic and geochemical investigation of Upper Cretaceous volcanic rocks in the Pontides,Turkey

Upper Cretaceous volcanic rocks were collected at 24 sites along the Pontides, N-NE Turkey, for rock magnetic and geochemical studies. Rock magnetic and petrographic methods showed that the lavas are characterized predominantly by titanomagnetites with a mixture of pseudo-single and multi-domain grains, whereas in tephrite single domain titanohematite was dominant. Measurements of magnetic susceptibility and the geochemical properties on different volcanic rock types provide important knowledge about the magnetic stability of the rocks. The magnetic properties are interpreted in terms of the composition, concentration, magma generation. Tephrite and phonotephrites with the highest intensities (5200 mA/m) and high magnetic susceptibility values (2585 × 10⁻⁵), largest grain sizes and Fe/Ti values, showing minor or no alteration are the most magnetic stable samples in contrast to dacites with the lowest intensity-magnetic susceptibility (520 mA/m − 573 × 10⁻⁵) and high alteration degree. The basanite samples show very low NRM (48–165 mA/m) but very high magnetic susceptibility (2906–3100 × 10⁻⁵) values suggesting the alteration of Fe-Ti minerals. It is shown that the magnetic properties of the basic to acidic rocks show a systematic variation with magma differentiation and could be related to fractional crystallization. Major and trace elements revealed that the lavas are compatible with complex magma evolution, with mineral phases of olivine+magnetite+clinopyroxene in basic series, amphibole+ +clinopyroxene in intermediate rocks and plagioclase+clinopyroxene+biotite in acidic series.     

Magnetic anisotropy and fabric of some foliated rocks from S.E. Australia

Summary The magnetic anisotropy of foliated rocks of several types has been measured by the torque-meter method, and shows that the alignment of long axes of magnetic grains in rocks normally follows the pattern of foliation evident in field observations. In a sharp fold in a lit-par-lit formation the magnetic anisotropy indicated an otherwise undetected lineation independent of the bedding and superimposed upon the foliation determined by the layering. In two adamellites, each with two alignment patterns separated by an angle of 30° the magnetic data are shown to be consistent with two foliations but not with one foliation plus a lineation. Magnetic anisotropy data can be ambiguous for rocks in which two or more grain alignment processes have operated, but combined with other observations magnetic measurements can provide a valuable new tool in the study of rock fabrics.     

On the theory of depositional remanent magnetization in sedimentary rocks

The effects of various factors such as thermal agitation, coagulation, anisotropy of susceptibility, and shape irregularity on the alignment of magnetic carrier grains during the process of acquisition of depositional remanent magnetization in sedimentary rocks is discussed.     

Track of fluid paleocirculation in dolomite host rock at regional scale by the Anisotropy of Magnetic Susceptibility (AMS): An example from Aptian carbonates of La Florida,Northern Spain

The present study aims to apply the AMS method (Anisotropy of Magnetic Susceptibility) at a regional scale to track the fluid circulation direction that has produced an iron metasomatism within pre-existing dolomite host rock. The Urgonian formations hosting the Zn–Pb mineralizations in La Florida (Cantabria, northern Spain) have been taken as target for this purpose. Sampling was carried out, in addition to ferroan dolomite host rock enclosing the Zn–Pb mineralizations, in dolomite host rock and limestone to make the comparison possible between magnetic signals from mineralized rocks, where fluid circulation occurred, and their surrounding formations. AMS study was coupled with petrofabric analysis carried out by texture goniometry, Scanning Electron Microscopy (SEM) observations and also Shape Preferred Orientation (SPO) statistics. SEM observations of ferroan dolomite host rock illustrate both bright and dark grey ribbons corresponding respectively to Fe enriched and pure dolomites. SPO statistics applied on four images from ferroan dolomite host rock give a well-defined orientation of ribbons related to the intermediate axis of magnetic susceptibility K₂. For AMS data, two magnetic fabrics are observed. The first one is observed in ferroan dolomite host rock and characterized by a prolate ellipsoid of magnetic susceptibility with a vertical magnetic lineation. The magnetic susceptibility carrier is Fe-rich dolomite. These features are probably acquired during metasomatic fluid circulations. In Fe-rich dolomite host rock, ?c? axes are vertical. As a rule, (0001) planes (i.e. planes perpendicular to ?c? axes) are isotropic with respect to crystallographic properties. So, the magnetic anisotropy measured in this plane should reflect crystallographic modification due to fluid circulation. This is confirmed by the texture observed using the SEM. Consequently, AMS results show a dominant NE–SW elongation interpreted as the global circulation direction and a NW–SE secondary elongation that we have considered as sinuosities of the fluid trajectory. The second type of magnetic fabric is essentially observed in the limestone and characterized by an oblate form of the ellipsoid of magnetic susceptibility, a horizontal magnetic foliation and mixed magnetic susceptibility carriers. It is interpreted as a sedimentary fabric.     

Magnetic anisotropy of rocks and its application in geology and geophysics

Magnetic anisotropy in sedimentary rocks is controlled by the processes of deposition and compaction, in volcanic rocks by the lava flow and in metamorphic and plutonic rocks by ductile deformation and mimetic crystallization. In massive ore it is due to processes associated with emplacement and consolidation of an ore body as well as to ductile deformation. Hence, it can be used as a tool of structural analysis for almost all rock types. Morcover, it can influence considerably the orientation of the remanent magnetization vector as well as the configuration of a magnetic anomaly over a magnetized body. For these reasons it should be investigated in palaeomagnetism and applied geophysics as well.     

Anisotropies of in-phase,out-of-phase,and frequency-dependent susceptibilities in three loess/palaeosol profiles in the Czech Republic; methodological implications

The relationship between the anisotropy of frequency-dependent magnetic susceptibility (fdAMS) and the anisotropy of out-of-phase magnetic susceptibility (opAMS) was investigated theoretically and also empirically at three loess/palaoesol profiles in Prague and in Southern Moravia. The data treatment was made in terms of mean susceptibility, degree of AMS, and orientations of principal susceptibilities. It has shown that the fdAMS and opAMS can serve as indicators of the preferred orientations of ultrafine magnetic particles that are on transition between superparamagnetic and stable single domain states in rocks, soils and environmental materials. In loess/palaeosol sequences, the fdAMS and opAMS correlate reasonably, because they are due to magnetic particles of similar grain sizes. The fdAMS and opAMS can be both coaxial with standard AMS (i.e. anisotropy of in-phase susceptibility - ipAMS) or non-coaxial indicating slightly different orientations of viscous magnetic particles.     

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.