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31.
[研究目的]开展水阳江流域标准孔BZK0402孔多重地层划分,探讨长江支流水阳江流域冰后期海平面变化的沉积响应以及古丹阳湖的成因和形成时代.[研究方法]以岩石地层为基础,在磁性地层和年代地层的双重约束下,对BZK0402孔进行多重地层划分.对比分析BZK0402孔和长江河谷、长江三角洲等邻区钻孔.[研究结果]BZK04...  相似文献   
32.
从亚洲大陆块体拼贴过程看大陆造山带的形成与演化   总被引:14,自引:1,他引:13  
肖文交  杨振宇 《地质论评》2000,46(3):270-275
本文就亚洲大陆喜马拉雅造山带和大别-苏鲁造山带构造演化模式进行详细评述,并据大地构造学和古地磁学最新研究成果讨论并总结大陆造山带形成与演化模式,即大陆碰撞造山带的演化可能涉及以下5个连续的过程: 碰撞旋转拼合陆内挤压反弹.  相似文献   
33.
张世红  李海燕 《现代地质》2004,18(4):415-422
第32届国际地质大会接受关于地磁学、古地磁学、环境磁学方面的摘要120余篇,主要内容涉及:(1)古地磁学在古大陆再造中的应用;(2)地磁场倒转和长期变的理论、观测和应用以及磁性地层学;(3)磁化率测量在地层划分和对比中的应用;(4)气候变化的环境磁学证据;(5)环境污染监测的环境磁学方法等研究领域。此外,磁法勘探也有很好的成果展出。基于物质磁学和地磁学的方法技术在日益广阔的地学研究领域中有很好的应用前景。  相似文献   
34.
RECORD OF BLOCK ROTATION AND MAGNETIC FIELD REVERSALS IN THE TETHYAN HIMALAYA (HIDDEN VALLEY, CENTRAL NEPAL)  相似文献   
35.
Magnetic carriers in remagnetized Cretaceous granitic rocks of northeast Japan were studied using paleomagnetism, rock magnetism, optical microscopy and scanning electron microscopy (SEM) by comparison with unremagnetized granitic rocks. The natural remanent magnetization (NRM) of the remagnetized rocks is strong (0.3–1.7 A/m) and shows a northwesterly direction with moderate inclination (NW remanence), whereas the unremagnetized rocks preserve weak NRM (<0.5 A/m) with westerly and shallow direction (W remanence). Although thermal demagnetization shows that both NRMs are carried by magnetite, the remagnetized rocks reveal a higher coercivity with respect to alternating field demagnetization (20 mT相似文献   
36.
浙江丽水Ⅰ盆地白垩纪古地磁学研究   总被引:1,自引:0,他引:1  
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。  相似文献   
37.
东昆仑造山带海西—印支期构造古地理演化的古地磁证据   总被引:5,自引:3,他引:2  
东昆仑造山带从北向南依次可划分出东昆北带、东昆中混杂岩带、东昆南带、阿尼玛卿混杂岩带和巴颜喀拉带5个大地构造地层带.根据对各地层带物质建造序列和构造古地理的研究基础之上所进行的古地磁分析认为,东昆北、东昆南、阿尼玛卿3个构造单元,在海西—印支期均处于北纬14°~20°之间.迄今为止,三者由南而北已漂移了约1500~2000km.3个构造单元在不同时期的古纬度及古纬度差反映了多岛洋盆扩张和闭合的多旋回性.从东昆中到巴颜喀拉带,其洋盆的开裂、收缩、关闭和前陆盆地的演化更替,无论在时间上和地理位置上均呈现规律性的从北向南依次迁移的特点,即在时间和平面上构成定向性构造迁移和多旋回.  相似文献   
38.
Possible configurations of the magnetic field in the outer magnetosphere during geomagnetic polarity reversals are investigated by considering the idealized problem of a magnetic multipole of order m and degree n located at the centre of a spherical cavity surrounded by a boundless perfect diamagnetic medium. In this illustrative idealization, the fixed spherical (magnetopause) boundary layer behaves as a perfectly conducting surface that shields the external diamagnetic medium from the compressed multipole magnetic field, which is therefore confined within the spherical cavity. For a general magnetic multipole of degree n, the non-radial components of magnetic induction just inside the magnetopause are increased by the factor 1 + [(n + 1)/n] relative to their corresponding values in the absence of the perfectly conducting spherical magnetopause. An exact equation is derived for the magnetic field lines of an individual zonal (m = 0), or axisymmetric, magnetic multipole of arbitrary degree n located at the centre of the magnetospheric cavity. For such a zonal magnetic multipole, there are always two neutral points and n – 1 neutral rings on the spherical magnetopause surface. The two neutral points are located at the poles of the spherical magnetopause. If n is even, one of the neutral rings is coincident with the equator; otherwise, the neutral rings are located symmetrically with respect to the equator. The actual existence of idealized higher-degree (n > 1) axisymmetric magnetospheres would necessarily imply multiple (n + 1) magnetospheric cusps and multiple (n) ring currents. Exact equations are also derived for the magnetic field lines of an individual non-axisymmetric magnetic multipole, confined by a perfectly conducting spherical magnetopause, in two special cases; namely, a symmetric sectorial multipole (m = n) and an antisymmetric sectorial multipole (m = n – 1). For both these non-axisymmetric magnetic multipoles, there exists on the spherical magnetopause surface a set of neutral points linked by a network of magnetic field lines. Novel magnetospheric processes are likely to arise from the existence of magnetic neutral lines that extend from the magnetopause to the surface of the Earth. Finally, magnetic field lines that are confined to, or perpendicular to, either special meridional planes or the equatorial plane, when the multipole is in free space, continue to be confined to, or perpendicular to, these same planes when the perfectly conducting magnetopause is present.Also Honorary Research Associate, Rutherford Appleton Laboratory, Chilton, Didcot, Oxon OX11 0QX, UK and Visiting Reader in Physics. University of Sussex, Falmer, Brighton BN1 9QH, UK  相似文献   
39.
Cretaceous terrestrial sediments deposited in a series of intracratonic basins across the Gobi Desert region of southern Mongolia and northern China contain a unique and diverse vertebrate fauna. In 1996 an expedition jointly sponsored by the Mongolian Paleontological Center and the Hayashibara Museum of Natural Sciences revisited a number of famous vertebrate fossil localities in the eastern Gobi region of Mongolia and, as part of a broad geological and paleontological study, collected a series of paleomagnetic samples from measured sections at Bayn Shireh, Burkhant and Khuren Dukh, as well as from an unmeasured locality adjacent to Khuren Dukh. Expedition members also collected palynologic samples from Khuren Dukh and the adjacent locality. Paleomagnetic analysis shows that all the sites from which samples were collected display detrital remnant magnetization that is consistently normal in polarity. The measured Cretaceous magnetic directions are oriented to the east or northeast of the present day expected direction (declination 356.2°, inclination 65.2°), and they are wholly concordant with that expected for a mid-latitude Northern Hemisphere sampling locality, and with the directions for this period reported by other workers. These results, when considered in tandem with the known biostratigraphy, strongly suggest that the sedimentary deposits at all four localities in the eastern Gobi correlate to the normal polarity chron 34 (the Cretaceous Long Normal), which ranges in age from approximately 121 to 83.5 million years. Previous vertebrate, invertebrate and palynological data from Khuren Dukh suggest that the lower and middle parts of the stratigraphic interval exposed there (which have been assigned to the Shinekhudag Formation) are ‘Khukhtekian’ in age and correspond to the Aptian–Albian interval that can be broadly correlated to the older, Early Cretaceous part of the Cretaceous Long Normal, C34n. New palynologic data presented here indicate that these strata are no older than middle to late Albian. The rocks at Bayn Shireh (the Bayn Shireh Formation) have been assigned a ‘Baynshirenian’ biostratigraphic age that may range from Cenomanian to early Campanian. The magnetostratigraphy results presented here indicate that the strata at both the Bayn Shireh and Burkhant localities do not cross the Santonian/Campanian Stage boundary, however, as this is believed to lie at, or very near, the C34n/C33r reversal boundary. Thus, the Bayn Shireh Formation was most likely deposited near the end of the Cretaceous Long Normal Interval, no later than the latest Santonian.  相似文献   
40.
塔里木地块上石炭统的古地磁研究   总被引:3,自引:1,他引:2  
本文对塔里木地块西北缘柯坪地区的3条上石炭统康克林组剖面进行了古地磁研究。95个定向岩心样品的逐步热退磁和交变退磁揭示出3个磁性组分,第一个是具有低解阻温度谱或低矫顽力谱在现代地磁场作用下形成的粘滞剩磁A(D=10°;I=56°,α95=4°);第二个是红色石英砂岩的具有反极性的高温组分B(D=217°,I=-43°,λ=56°,Φ=184°E;A25=6°详细研究表明,该分量受附近晚二叠世脉岩侵入的重磁化;第三个是灰岩高矫顽力谱的反极性组分C(D=241°、I=-51°,λ=41°N,Φ=160°E,A(?)=4°)。这一分量通讨倾斜检验,在95%概率水平上明显不同于塔里木地块目前已有的石炭纪以后的古地磁方向,它代表了原生剩磁。研究结果表明:(1)晚石炭世塔里木地块已和哈萨克斯坦地块、苏联西天山地块以及西伯利亚地块发生碰撞:(2)苏联西天山地块相对塔里木地块曾逆时针旋转了70°(欧拉极位置λ=8°N,Φ=69°E),而塔里木地块则相对西伯利亚地块逆时计旋转了21°(欧拉极位置λ=20°N,Φ=34°E)。从该区已有的晚古生代至早三叠世占地磁数据看,这些地块之间的相对旋转运动发生于早三叠世之后。  相似文献   
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