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1.
塔里木地块奥陶纪古地磁新结果及其构造意义   总被引:2,自引:1,他引:1       下载免费PDF全文
本文报道塔里木地块阿克苏—柯坪—巴楚地区奥陶纪古地磁研究新结果.对采自44个采点的灰岩、泥灰岩及泥质砂岩样品的系统岩石磁学和古地磁学研究表明,所有样品可分成两组:第一类样品以赤铁矿和少量磁铁矿为主要载磁矿物,该类样品通常可分离出特征剩磁组分A;第二类样品以磁铁矿为主要载磁矿物,系统退磁揭示出这类样品中存在特征剩磁组分B.特征剩磁组分A分布于绝大多数奥陶纪样品中,具有双极性,但褶皱检验结果为负,推测其可能为新生代重磁化.特征剩磁组分B仅能从少部分中晚奥陶世样品中分离出,但褶皱检验结果为正,且其所对应古地磁极位置(40.7°S,183.3°E,dp/dm=4.8°/6.9°)与塔里木地块古生代中期以来的古地磁极位置显著差别,表明其很可能为岩石形成时期所获得的原生剩磁.古地磁结果表明塔里木地块中晚奥陶世位于南半球中低纬度地区,很可能与扬子地块一起位于冈瓦纳古大陆的边缘;中晚奥陶世之后,塔里木地块通过大幅度北向漂移和顺时针旋转,逐步与冈瓦纳大陆分离、并越过古赤道;至晚石炭世,塔里木地块已到达古亚洲洋构造域的南缘.  相似文献   

2.
本文报道唐古拉山北坡开心岭地区的晚石炭-早二叠世地层的古地磁学研究结果.岩石磁学实验研究表明扎日根组灰岩样品中的磁性矿物以磁铁矿为主,诺日巴尕日保组砂岩样品中的磁性矿物以赤铁矿为主或磁铁矿与赤铁矿共存.采用系统热退磁方法对样品进行磁清洗,大部分样品的退磁曲线呈双分量特征,高温分量明显.高温特征分量成功通过了砾石可靠性检验,代表了地层岩石的原生剩磁信息.获得羌北地块晚石炭-早二叠世地层(16个采点127块样品)的原生剩磁分量的平均方向为Ds=30.2°,Is=-40.9°,ks=269.0,a95=2.3°;其对应的古地磁极位置为λ=25.7°N,φ=241.5°E,dp/dm=2.8/1.7,相应的古纬度为23.4°S.表明晚石炭-早二叠世时期羌北地块位于南纬低纬度地区,可能属于冈瓦纳大陆的北缘.结合前人古地磁学研究结果,该地块在其后快速北移,可能与早二叠世-晚三叠世古特提斯洋快速消亡以及新特提斯洋北支班公湖-怒江洋快速扩张相关.  相似文献   

3.
四川江油地区上泥盆统三分量样品和下石炭统样品的岩石磁学研究表明:上泥盆统样品的主要载磁矿物为磁铁矿,且以假单畴、多畴和少量单状态存在,下石炭统样品的载磁矿物则主要是假单畴和多畴磁铁矿的混合物,从样品中分离出的中温分量由假单畴磁铁矿携带,上泥盆统样品的高温分量则由记录了岩石原生剩磁的单畴磁铁矿携带。  相似文献   

4.
四川旺苍早三叠世古地磁学结果及其大地构造学意义   总被引:4,自引:0,他引:4  
对四川北部旺苍地区(32.14°106.17°)早三叠世地层进行了古地磁学和岩石磁学研究,其结果表明剩磁载磁矿物主要为磁铁矿,另有少量赤铁矿.采样地层岩石高温剩磁分量(D=45.1°,I=18.0°,a_(95)5. 9°),通过褶皱及倒转检验,表明认岩石中获得的高温分量为原生分量.由原生分量求得扬子地块早三叠世虚地磁极为:42.5°N,214.6°E(d_(p)=3.2,d_m=6.1),古纬度为9.2°.认为,华北与扬子地块在自早三叠世期间已基本拼合,现有古地磁结果支持秦岭造山带为陆内造山作用的结果  相似文献   

5.
对扬子地块北部地区的湖北兴山 秭归剖面寒武系至中生界进行了构造古地磁学研究 .对岩石标本剩磁载体和剩磁稳定性的分析以及褶皱检验和倒转检验的结果表明 ,从 82 5个岩芯 ( 84个采样点 ,代表古生界至侏罗系 )分离出的高温特征分量代表了原生剩磁分量 ,从而得到这一地区古生代至侏罗纪几个地质时代的古地磁极位置 ,补充了中国扬子地块古地磁极移曲线的基本数据 .  相似文献   

6.
拉萨地块是研究班公湖—怒江特提斯洋和雅鲁藏布江特提斯洋演化过程的关键,但印度—亚洲大陆的碰撞可能导致拉萨地块遭受不同程度的重磁化影响,为寻找理想地层进行古地磁研究,本文对拉萨地块中二叠世洛巴堆组砂岩、火山岩及灰岩样品进行详细的岩石磁学研究,以确定各类岩石是否具备记录原生剩磁信息的能力.结果表明砂岩样品中主要载磁矿物为磁黄铁矿,火山岩及灰岩样品中主要为磁铁矿或赤铁矿.结合区域地质资料和部分样品退磁实验,本文认为砂岩样品可能遭受林子宗群火山和岩浆活动所提供的区域热扰动影响,记录了古近系重磁化信息;火山岩和灰岩样品可能记录了岩石形成时期的原生剩磁信息,有望从中获得可靠古地磁数据.  相似文献   

7.
羌北地块中-晚侏罗世雁石坪群古地磁新结果   总被引:4,自引:0,他引:4       下载免费PDF全文
本文报道青藏高原羌北地区中-晚侏罗世雁石坪群古地磁新结果.对采自青海省格尔木市唐古拉山乡雁石坪剖面(33.6°N, 92.1°E)11个灰岩采点(118块)和10个碎屑岩采点(99块)定向样品系统古地磁学研究表明,大部分样品的退磁曲线具有双分量特征.低温分量方向在地理坐标系下较为集中,应该为地层褶皱之后的黏滞剩磁.高温特征剩磁分量方向可分为两类:(1)索瓦组(J3s)和布曲组(J2b)灰岩,以磁铁矿为主要载磁矿物,高温特征剩磁分量(Ds=355.7°,Is=42.1°,k=58.2,α95=6°)可通过99%置信度的褶皱检验.(2)雪山组(J2x)和雀莫错组(J2q)碎屑岩,以赤铁矿、磁铁矿为主要载磁矿物,高温特征剩磁分量(Ds=3.3°,Is=28.9°,k=30.7,α95=8.9°)可通过95%置信度的倒转检验和99%置信度的褶皱检验.两组分量都应该是岩石形成时的原生剩磁信息.碎屑岩组的磁倾角比灰岩组偏低13°左右,其剩磁方向很可能存在着与压实作用相关的剩磁倾角变浅的状况.本文取灰岩组平均磁化方向作为雁石坪群的原生剩磁分量,获得羌北地区雁石坪群古磁极位置:80.0°N,295.2°E(dp/dm=7.4/4.5).古地磁结果表明,羌北-昌都地区晚石炭-晚二叠世期间位于南纬中低纬度地区,早三叠世以后开始大规模北向漂移,至中-晚侏罗世已到达24.3°N.其快速北向运动主要发生在早三叠至早侏罗世期间(3500 km左右),与现今位置相比中晚侏罗世之后的北向迁移总量为900 km左右.  相似文献   

8.
华北地块早古生代古地磁结果的大地构造意义   总被引:4,自引:0,他引:4       下载免费PDF全文
对采自鄂尔多斯盆地边缘早古生代地层的1006块(153采点)定向古地磁岩芯标本的研究表明,大多数地层单元的岩石剩磁组分可分离出A、B两个主要分量.根据其稳定性检验结果,A分量(北西方向,低负倾角及其对方向)为岩石形成时期的特征剩磁分量,而B分量(北西方向,中至低正倾角及其对方向)则可能是晚古生代的重磁化分量.华北地块早古生代的古地磁参考极均位于大西洋;与此相应,华北地块位于南纬15°左右.  相似文献   

9.
羌塘地区是解决特提斯的演化和冈瓦纳大陆与欧亚大陆界线问题的关键地区.对青藏高原羌北地块晚古生代及早三叠世剖面(33.7°N,86.7°E)15个采点163块砂岩、灰岩和安山岩定向样品进行了系统的古地磁学实验研究.结果表明:样品中主要载磁矿物为赤铁矿和磁铁矿.在逐步热退磁和热-交变混合退磁过程中,大部分样品的剩磁具有明显的双分量特征,低温分量方向在地理坐标系下接近于现代地磁场偶极子场(PEF)方向,很可能是粘滞剩磁;高温分量显著不同于PEF方向.部分样品具有单分量特征,并与双分量样品的高温分量方向一致.高温特征剩磁分量可通过95%置信度的倒转检验和99%置信度的褶皱检验,并且有岩脉检验,应代表岩石形成时的原生剩磁.羌北古地磁极位置:晚石炭世(31.8°S,45.7°E,(dp=3.9,dm=2.1));早、中二叠世(31.7°S,46.8°E,(dp=16.9,dm=9.2));晚二叠世(34.4°S,54.1°E,(dp=12.5,dm=6.9));早三叠世(16.9°S,22.5°E(dp=9.2,dm=4.9)).  相似文献   

10.
豫北早古生代灰岩的岩石磁学研究   总被引:1,自引:0,他引:1  
对一些可分离出岩石形成时原生剩磁的样品进行深入的岩石磁学研究,发现天然剩磁的特征通常取决于磁铁矿的颗粒度(或单、多磁畴状态),单、多磁畴磁铁矿的含量不同,导致了中温与高温剩磁分量不同程度的叠加,也就造成了不同磁分量分离难易程度的不同  相似文献   

11.
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.  相似文献   

12.
对苏北盆地兴化1#钻孔岩心沉积物进行了质量磁化率、频率磁化率、变化曲线、等温剩磁和磁滞回线等参数的测试分析,结果表明,粘土质沉积物中的主要载磁矿物为磁铁矿和赤铁矿;砂质沉积物中的磁性矿物除了磁铁矿和赤铁矿外,还含有少量的磁赤铁矿和针铁矿.针铁矿普遍存在于钻孔下部的样品中.整个钻孔沉积物中的磁性矿物颗粒都是介于单畴和多畴之间的准单畴颗粒,但粘土质沉积物中的磁性矿物颗粒更趋近于单畴颗粒,而砂质沉积物中的磁性矿物颗粒更趋近于多畴.根据不同的磁性矿物组合特征,选择合理的温度和磁场强度区间对古地磁退磁结果进行分析,得到沉积物可靠的特征剩磁方向,为古地磁年代学提供依据.  相似文献   

13.
渤海南部莱州湾Lz908孔沉积物的岩石磁学性质   总被引:2,自引:2,他引:0       下载免费PDF全文
亚洲大陆边缘海和陆表海在区域的物质和能量交换以及区域气候与环境演化过程中扮演了关键角色.磁性地层学和环境磁学方法是建立年代框架和环境演变序列的有效手段,但是,由于该地区边缘海和陆表海沉积物中磁性矿物来源十分复杂,磁性地层学和环境磁学研究的重要基础是要精细地解译沉积物的岩石磁学性质.为此,本文利用渤海南部莱州湾Lz908孔与钻孔附近的现代沉积物样品进行了详细的岩石磁学对比研究.结果显示,渤海南部沉积物中的磁性矿物主要是较粗颗粒(较大的准单畴至多畴)磁铁矿,还有少量磁赤铁矿,部分沉积物还含有赤铁矿和针铁矿,其中磁铁矿是特征剩磁的主要载体;莱州湾现代河流-海洋沉积物和钻孔样品之间的磁性特征无显著差异,说明莱州湾沉积物堆积之后尚未经历明显的沉积后期改造.  相似文献   

14.
华北地块早古生代地层单元的岩石磁学特征研究   总被引:1,自引:1,他引:1       下载免费PDF全文
通过对采自华北地块西部鄂尔多斯盆地边缘早古生代地层单元中的44块定向岩芯样品的岩石磁学实验(饱和等温剩磁及剩磁矫顽力的测量,三轴磁化的饱和等温剩磁的系统热退磁和低温实验)研究,揭示出华北地块早古生代地层单元的各类岩石中,主要载磁矿物的构成具有磁铁矿或赤铁矿与中等居里温度的磁黄铁矿、磁赤铁矿等共存的特征;个别地层单元的岩石中以极低居里点的针铁矿为主要载磁矿物.  相似文献   

15.
Directional samples were taken to study rock magnetism and palaeomagnetic records from the Dong- sheng profile, which is 5 m thick and on the northwest edge of the Bose Basin. Mineralogy and rock magnetism of typical samples indicate that coarse granular titanomagnetite, and fine-grained hematite, superparamagnetic maghemite formed by pedogenesis are in the sediment, which has undergone many transformative processes during different stages of pedogenesis. Parallel samples were taken for thermal demagnetization (TH) (0 to 680℃) and alternating field (AF) demagnetization (0 to 80 mT) respectively. Experimental results of these two kinds of demagnetization illustrate that there are two or more magnetic components in the samples. Intensity of NRM decreases by almost 60% to 90% rapidly when the temperature ranges from 100℃ to 350℃, with a steady magnetic component. It is impossible to analyze the magnetic components at high temperature because those fluctuate widely when the temperature is higher than 400℃. Steady magnetic components from 100℃ to 350℃ indicate that the remanence was mainly carried by fine-grained hematite formed by pedogenesis, reflecting a change in the geomagnetic field while the magnetite was being oxidized into hematite by chemical weathering after deposition. The formative age of the sediments cannot be obtained by magnetic methods in this profile.  相似文献   

16.
本文对"鲁科一井"(CCSD-LK-Ⅰ)768.9~1112.3m之间的上白垩统沉积岩样品进行了岩石磁学、磁化率各向异性(AMS)以及天然剩磁组分的研究.在此基础上,分析了利用特征剩磁(ChRM)和黏滞剩磁(VRM)方向恢复岩芯原始方位的可行性.三轴等温剩磁热退磁曲线、磁滞回线、反向场退磁曲线、一阶反转曲线等岩石磁学测量结果表明,沉积岩的主要载磁矿物为磁铁矿和赤铁矿.335块样品的AMS测量结果表明磁化率椭球主轴的最大轴K1和中间轴K2与水平面夹角较小,最小轴K3接近垂直于水平面分布,说明沉积岩保留了原始沉积磁组构特征.系统热退磁实验表明,多数样品在25~350℃和500~690℃温度段分别获得VRM和ChRM分量.利用ChRM偏角方向,并考虑构造旋转量校正,对VRM偏角方向进行恢复,Fisher统计得到DVRM=-1.3°,IVRM=59.6°,与当地现代地磁场方向(D=-6.7°,I=53.9°)基本一致.用ChRM偏角方向对磁化率主轴K1偏角方向进行校正,校正的结果为:D_(ch_K1)=349.2°,I_(ch_K1)=-0.7°.本文研究结果对于地质勘探中利用古地磁学方法恢复钻孔岩芯原始方位具有一定参考意义.  相似文献   

17.
A detailed rock magnetic investigation of loess/palaeosol samples from the section at Lingtai on the central Chinese Loess Plateau (CLP) is presented. Thermal demagnetisation of isothermal remanent magnetisation (IRM) and Curie temperature measurements suggest the presence of magnetite, maghemite and hematite as remanence carrying components. Bulk and grain size fractionated samples have been analysed using coercivity spectra of remanence acquisition/demagnetisation curves, which identify four main remanence carriers in different grain size fractions of loesses and palaeosols. A linear source mixing model quantifies the contribution of the four components which have been experimentally derived as dominating endmembers in specific grain size fractions. Up to two thirds of the total IRM of the palaeosols are due to slightly oxidised pedogenic magnetite. Two detrital components dominate up to 90% of the IRM of the loess samples and are ascribed to maghemite of different oxidation degree. Detrital hematite is present in all samples and contributes up to 10% of the IRM. The iron content of the grain size fractions gives evidence that iron in pedogenically grown remanence carriers does not originate from the detrital iron oxides, but rather from iron-bearing clays and mafic silicates. The contribution of pedogenic magnetite to the bulk IRM increases with the increasing degree of pedogenesis, which depends in turn on climate change.  相似文献   

18.
Remanent coercivity spectra derived from IRM acquisition curves and thermal demagnetization of the IRM indicate that magnetite, haematite and minor amounts of goethite determine the magnetic properties of the Pliensbachian limestones at Bakonycsernye. These limestones have been sampled at approximately 7-cm intervals along a 10-m stratigraphic section which covers the whole Pliensbachian stage (Lower Jurassic) without any recognizable break in sedimentation. The primary natural remanent magnetization (NRM) is carried by detrital particles of magnetite and haematite, but it is seriously overprinted by a normal magnetization which originates from secondary haematite with a wide range of blocking temperatures. This haematite is believed to have formed diagenetically during one of the Mesozoic periods of normal polarity. However, the reversal pattern obtained after NRM thermal demagnetization at temperatures ≥450°C is thought to be characteristic of the Pliensbachian stage.  相似文献   

19.
Measurement of the remanent magnetization of samples of Jurassic oceanic red sediments recovered in the western Atlantic on Leg 11, site 105 of the Deep Sea Drilling Project yields quite different results, depending on the demagnetization processes used. Both the Jurassic section and the Berriasian-Valanginian part of the Lower Cretaceous were measured, but with less satisfactory results for the Lower Cretaceous. The natural remanent magnetization of the Jurassic section is almost entirely normal, with 44.6° inclinations (standard deviation = 13.9°) and is not changed by 1000 Oe alternating field (AF) demagnetization. Thermal demagnetization to temperatures of 630°C brings the inclination and polarity sequence in line with that expected for Oxfordian through Tithonian time at this site. The average inclination after thermal demagnetization is 22.1°, standard deviation = 12.1°, and the polarity pattern is one of frequently alternating polarity, much more similar to published reversal patterns for this time than the all normal results of AF demagnetization. The polarity pattern is not identical to the published ones as a result of insufficiently detailed sampling. Thermomagnetic and X-ray analyses were ambiguous, but suggest the presence of titanomagnetite, hematite, and possibly titanomaghemite and pyrrhotite. The primary remanence is carried by hematite.  相似文献   

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