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1.
亚热带富铁土的磁学性质及其磁性矿物学   总被引:7,自引:3,他引:4  
通过55个亚热带富铁土的磁化率(χ)、频率磁化率(χfd)、非滞后剩磁(ARM)和饱 和等温剩磁(SIRM)等磁性参数测定,结合氧化铁化学形态分析和矿物鉴定,初步明确了亚热 带富铁土的磁学特征及其磁性矿物.磁测数据表明富铁土中存在强磁性的矿物,其磁化率χ 与土壤游离氧化铁(Fe)含量呈极显著指数正相关(R=0.5971),频率磁化率χfd与土壤游离氧 化铁含量呈极显著直线正相关(R=0.4289).富铁土的χfd和非滞后磁化率χARM。值表明土壤 中的磁性矿物以超顺磁性(SP)和稳定单畴(SSD)颗粒为主,富铁上的χ和χARM呈极显著直线 正相关(R 0.9429),证明富铁土的磁性是由风化成土过程产生的 SP和 SSD磁性颗粒贡献 的.矿物磁测结合X-衍射证明富铁土中的氧化铁矿物由赤铁矿、磁赤铁矿和针铁矿组成。  相似文献   

2.
为了进一步认识间歇性多重X线重联的特征,本文分析计算结果,发现入流自边界进入后向两侧发散,沿着x轴(z=0)和出流边界(z=2),压强P和磁场B的分布形态表明这种非稳态重联属快模式扩张型.数值结果还表明,进入扩散区的入流马赫数M与磁雷诺数Rm之间基本满足关系式M≈1.5R-1/2─1.75R-1/2,而且等离子体的加速与压强P(P  相似文献   

3.
根据北京白家疃测站8台GEO潮汐重力仪对比观测的资料,采用标准线性体流变模型模拟重力仪及记录系统的力学特性,计算各台仪器的格值改正系数、主潮汐波的振幅衰减系数和相位滞后;确定北京重力地球潮的振幅因子δ和相让滞后为δ(M)=1.1784,δ(O)=1.1804,δ(M)/δ(O)=0.9983,(M)=0.07°,(O)=0.10°.  相似文献   

4.
从Rankine-Hugoniot关系出发,以激波切向磁场ξ、上游激波角θ和等离子体β值为参数研究各类激波解的特性及相互关系,阐明各类激波强度随介质β值的变化规律.结果指出:(1)在ξ<-1的Ⅰ型中间激波区和ξ>4的快激波区存在双解;(2)慢激波可以直接和中间激波连接,但不能和快激波直接连接;(3)各类激波强度(用激波密度比衡量)随β值均有变化:Ⅰ型中间激波上支随β值增加而下降,下支则上升;Ⅰ型中间激波和慢激波都随β值增加而下降;快激波双解区上支随β值增加而下降。下支上升;快激波在1<ξ<4区间的解随β值增加而上升。  相似文献   

5.
塔里木盆地库车坳陷克拉苏河沿岸发育良好的新生界地层.我们对克拉苏河沿岸新生界剖面分A、B两段进行系统采样,获得定向岩芯样品1700余块. 岩石磁学研究表明,新生代沉积岩中磁性矿物以赤铁矿为主,含有少量磁铁矿;磁组构测试结果显示,两段剖面磁面理均较磁线理发育,最小磁化率主轴近于直立,显示原生沉积组构. A剖面磁化率主轴к1的偏角指示古流向. 库姆格列木群沉积时的古水流方向为NEE-SWW向,至苏维依组沉积时,流向变为NNE-SSW向. 河流古流向在苏维依组形成时发生急剧变化,说明南天山此时可能发生了明显的隆升,且以北西部隆升为主;B剖面为吉迪克组、康村组和库车组粗粒碎屑岩,磁组构显示к12构成的磁面理与层理面小角度相交,к3呈叠瓦状分布,可以用来指示古水流方向.从吉迪克组至库车组下段,古流向均为NNW-SSE,但逐渐偏东,暗示天山在此期间处于缓慢的隆升期或东西部处于同步隆升,且西部隆升速度快于东部.  相似文献   

6.
以IPS速度、光球磁场、K─日冕偏振亮度和卫星实地观测数据为基础,综合生成处于太阳活动上升期的1976年10个太阳周(1643─1652卡林顿周)的源表面高度(R=2.5R,R为太阳半径)和日球空间中(IAU)太阳同质量流量速度谱。结果表明,速度谱存在与太阳活动上升期一致的"三段"结构,且各段分别与不同的磁结构区相对应。  相似文献   

7.
国际参考电离层用于中国地区时的修正计算方法   总被引:13,自引:5,他引:13       下载免费PDF全文
在充分利用中国电离层台站长期观测资料的基础上,阐述了国际参考电离层用于中国地区时的一种修正计算方法.它采用“亚大地区F电离层预测方法”计算f和M(3000)F,合理地描述F层的出现和提高E层的峰值高度.与实测的电离层数据的系统比较说明,该方法在中国地区使用时,其精度比国际参考电离层有明显提高.  相似文献   

8.
各向异性介质中地震波前面的偏微分方程   总被引:7,自引:0,他引:7       下载免费PDF全文
从含21个弹性参数的各向异性介质中关于位移分量u、u与u的偏微分波动方程组出发,通过假定平面波位移函数解,导出准P波、准SV波与准SH波的波前面偏微分控制方程,进而对各类特殊各向异性介质(横向各向同性介质、椭圆及立方体各向异性介质)中地震波前面偏微分方程进行了讨论.以上结果为研究各向异性介质中地震波传播规律以及进行正、反演研究奠定了理论基础.  相似文献   

9.
地磁场Sq的经度效应和UT变化   总被引:4,自引:0,他引:4       下载免费PDF全文
使用国际地球物理年(IGY)和国际地球物理合作年(IGC)期间全球地磁台网的资料和中国台站的同期地磁记录,对地磁场太阳日变化S的经度效应和UT变化进行了分析研究.将适用于瞬时全球磁场的球谐分析法与适用于平均场的双调和分析法相结合,提出了一种分析S磁场的新方案,得到了(θ,T,t)坐标系中组成S场的三个部分,即仅随地方时LT变化的部分SLT,仅随世界时UT变化的部分SUT以及既随LT变化又随UT变化的部分SLUT.从全球来看,在IGY/IGC期间,这三部分的强度之比分别为:X分量1.0:0.2:0.3,y分量1.0:0.1:0.6,Z分量1.0:0.4:1.0.S的经度效应和UT变化虽然表现了同一物理过程,但它们有不同的表达形式,其决定因素是地磁轴对地理轴的倾斜,地磁场的非偶极子成分(即区域性异常)和地球内部电性的横向不均匀性(包括海陆分布、地壳上地幔电导率的区域差异)  相似文献   

10.
本文利用磁化率张量k、导磁率张量μ和剩余磁化强度Jr的概念表征磁性体的各向异性,给出了磁法勘探正问题在磁各向异性条件下的数学提法,即总磁位U应由下列的偏微分方程和定解条件确定: 其中,A1+是磁性体Q1的边界面,S1-和S分别是无磁性空间Q0的内外边界面,n为各区域封闭界面上一点的外法线向量,ρr是剩余磁荷密度,U0是地磁场的磁位。 然后,又给出了应用有限元法解上述正问题的计算公式(二度)和实例。  相似文献   

11.
超导岩样磁力仪是以超导量子干涉器(SQUID)为磁传感器用来测量岩样剩磁的仪器,是研究岩石磁学和古地磁学的重要手段。它比常规的古地磁仪器--无定向磁力仪、旋转磁力仪具有灵敏度高、响应时间短、动态范围大、又可三分量同时测量等优点,满足了弱磁岩样测量的要求。本文叙述了超导测磁的理论基础,仪器的组成,原理,研制情况及实测结果。  相似文献   

12.
许同春  刘秀铭 《地震学报》1989,11(3):303-308
磁化率各向异性(AMS)是岩石的普遍特性,它反映岩石磁性矿物的择优取向,即磁组构(Magnetic fabric).近三十年来,磁组构技术逐渐应用于地质和地球物理学,显示广阔的研究前景.测量磁组构的仪器有多种,原理不一,故有必要用同一样品在不同原理的仪器上进行比测,以便确认数据的一致性和可靠性.用黄土、变质岩、玄武岩及掺有铁粉的断层泥制成正方体或圆柱体样品,在卡帕桥(KLY-1和KLY-2)和旋转式磁化率仪(Minisep)上进行比测发现:(1)前者的精度(即重复性)在多数情况下优于后者;2)用旋转式磁化率仪测量之前,必须先测得样品z轴的体磁化率,其标定值取决于厂家在标准样品上标示的数值及被测样品与标准样品的相对体积.就旋转样品测量AMS而言,其标定值应为z轴体磁化率测量标定值的一半.   相似文献   

13.
阜平猴石顶太古界褶皱的岩石磁性组构   总被引:1,自引:0,他引:1       下载免费PDF全文
猴石顶太古界重褶皱位于阜平太古宙穹状复合褶皱群中一个钩状褶皱的“钩子”部位。其中一层斜长角闪岩标志层的岩石磁性组构的分布情况为:1.在翼部的磁化率量值椭球是压扁形的,磁性叶理面的方向与变质层面及片麻理的方向基本一致,表现为向北西倾斜的倒转褶皱;2.在太古宙再次变形阶段所形成的转折端部位,磁性叶理面的走向变化较大,并出现拉长形的磁化率量值椭球,反映了经受过拉张作用的变形和多于一次的不同方向应力的作用;3.西翼的磁性线理值与磁性叶理值以及磁化率各向异性度都大,反映它经受过较强的剪切应力与压应力的作用;4.磁性线理主要倾向北半球,而且部分磁性线理近南北方向分布。 推测猴石顶重褶皱可能处于向北倾伏的主体构造的东侧。 上述岩石磁性是由自行设计的静态测量方法,用国产的数字式无定向磁力仪测定的。  相似文献   

14.
Summary The degree of astaticism is the fundamental parameter of an astatic magnetometer, an instrument used in geophysics for magnetic measurements of rock specimens. The degree of astaticism is formulated with a view to the vectorial character of the defining quantities and with a view to the effect of the geomagnetic field. As regards measuring the parameter, the mirror method is given, which makes use of the positive and negative orientation of the astatic system relative to the north or east. The measure of the value of the parameter is the change of the sensitivity of the system and the deflection of its zero position, compensated for by the magnetic field of the calibration coil. The problem of the degree of astaticism is treated complexly, inclusive of the measurement of the parameter, which in practice is of fundamental importance for adjusting the systems for manufacturing astatic magnetometers.  相似文献   

15.
Summary A magnetic study of metabasic dykes of pre-Cambrian age in Gomoh has been done. 9 magnetic profiles have been taken with Schmidt vertical force variometer. Direction and intensity of NRM have been determined for 25 oriented samples with an astatic magnetometer. Magnetic susceptibility of the samples has been determined. The magnetic profiles have been interpreted by considering both natural remanence and susceptibility of the rock samples. The remanent magnetic directions have two groups, one corresponding to the northern hemisphere and the other to the southern hemisphere. The corresponding latitudes of the place would then be 34°N and 42°S. It is suggested here that metamorphism of the basic rocks of this area took place during two distinct geologic epochs, one when India was in northern hemisphere and the other when in southern hemisphere, presuming that continental drift has taken place.  相似文献   

16.
The intensity of natural remanence magnetisation (NRM) is measured along the three mutually-perpendicular directions using an astatic magnetometer. The intensity of induced magnetisation is measured using an apparatus fabricated in the laboratory. The Koenigsberger ratio has been calculated for all the samples and the ratio has been used to test the stability of NRM in the samples. The mean direction of magnetisation is determined from the three components of the NRM intensity. The palaeomagnetic pole position of the samples is determined using the direction of magnetisation and the site location. An attempt has been made to fix the geological age of the charnockites using palaeomagnetic methods.  相似文献   

17.
我国磁法勘探的研究与进展   总被引:7,自引:2,他引:7       下载免费PDF全文
管志宁 《地球物理学报》1997,40(Z1):299-307
简要概述了我国磁法勘探50年来的研究与进展,主要包括:地面、航空与海洋磁测工作,磁力仪研制与生产,磁异常处理与转换技术,磁异常解释理论与方法,岩石磁性研究,磁法勘探在基础地质研究、固体矿产勘查、油气勘查和其他领域中的应用.  相似文献   

18.
The principle of optical pumping allows the design of magnetometers with high sensitivity. When mapping the field of the total magnetic force, it is no longer possible to make full use of the accuracy of the instruments because the accuracy of the reduction of the diurnal variation is limited. By simultaneously recording with two instruments in different altitudes, the vertical gradient can be measured which doe's not depend on the time variation of the magnetic field. Therefore, the gradiometer seems to be a more adequate tool for oil exploration than the magnetometer. It is investigated in this article whether the results of this gradiometer or the measurements of the total magnetic field by the high sensitive magnetometer are more useful in oil exploration. The article comes to the conclusion that for most problems of oil exploration the total magnetic field is a more valuable unit than the vertical gradient measured directly by the gradiometer. The total magnetic field allows a better investigation of the tectonics than the vertical gradient. The apparent advantages of the gradiometer claimed by its supporters are mainly based on inconsistent mathematical concepts.  相似文献   

19.
Summary 38 oriented samples of Deccan Traps have been collected from the neighbourhood of Chincholi, Mysore State, India. The Natural Remanent Magnetisation of these rocks has been studied using an astatic magnetometer. It has been found that these rocks are magnetically reversed, the mean magnetic direction being N154°E in declination and 61° down in inclination. Thermoremanance studies conducted on four specimens showed that two specimens with weak NRM and a high secondary magnetisation have Curie temperatures around 560°C for the NRM and exhibited partial reversal of TRM at room temperature, while two specimens with high NRM and with little secondary magnetisation have Curie temperatures much lower than 560°C for the NRM.  相似文献   

20.
The low-temperature (K1) transition has been measured in prepared samples with a low concentration of magnetite to test the validity of the technique for identifying magnetite in weakly magnetized rocks. Using an astatic magnetometer, magnetite concentrations as low as 1 part in 100,000 can be satisfactorily detected.Measurements on natural samples show the presence of magnetite in a variety of limestones which are known to have a stable natural remanent magnetization.  相似文献   

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