利用磷灰石裂变径迹对断层摩擦生热探测或测量的初步探讨          下载免费PDF全文

刘建辉 《第四纪研究》2009,29(3):644-652

以青藏高原东北缘断裂带为研究对像,对利用磷灰石裂变径迹热年代学对地震断层滑动摩擦生热的探测或测量进行了初步探讨。其基本思路是利用磷灰石裂变径迹热年代计的热敏感,通过对横跨断层垂直方向断层岩和围岩的磷灰石裂变径迹年龄及围限径迹长度分布的对比分析,对断层滑动摩擦生热进行探测。本次研究对来自3个断层剖面的13个样品进行了磷灰石裂变径迹分析,样品包括断层主滑动面上的断层泥、碎裂岩和断层围岩,分析结果并没有获得断层摩擦生热的证据,表明这些断层在地震滑动过程中的摩擦增温非常有限,没有达到磷灰石裂变径迹热年代计体系可加载热信息的温度－时间要求。结合前人已有的相关研究,对利用磷灰石裂变径迹热年代学对地震断层滑动摩擦生热进行探测或测量存在的主要问题及可行性进行了初步总结和探讨,认为只适应于对震级大、断层滑动距离和速率大,摩擦强度强,位于一定深度有大量摩擦热生成,并使断层附近增温达到或超过磷灰石裂变径迹部分或完全退火温度的断层进行滑动摩擦生热的探测或测量,将是一种潜在的能对地震断层滑动摩擦生热或增温进行测量的“热量计或温度计”。  相似文献   

负温条件下激光位移传感器的标定     

杜玉霞  马巍  赵淑萍  张泽  明姣 《冰川冻土》2016,38(6):1583-1591

在使用激光位移传感器测试冻土位移中,由于测试现场环境条件恶劣,厂家给出的传感器线性度会降低,因此,需要对所有传感器在使用前应模拟使用时的环境条件重新进行标定。为验证激光位移传感器在冻土测试中的适用性,依据德国森萨帕特FT-50RLA220型激光位移传感器的结构、使用特点、技术指标,设计了由控温箱、标定支架、激光位移传感器、量块及数据采集装置组成的标定的装置,进行了不同负温条件下对激光位移传感器标定,并依据标定试验结果进行拟合参数修正,得到不同环境温度下的试验结果的线性度和迟滞特性。试验结果表明：不同的环境温度下,两个激光位移传感器与标准厂家测试曲线存在差异,不同负温条件下标定的两个激光位移传感器的拟合优度R²分别为0.999和1;线性度最大值分别为0.88%FS和0.32%FS。  相似文献   

四川盆地南部地区新生代隆升剥露研究——低温热年代学证据   总被引：1，自引：1，他引：0       下载免费PDF全文

邓宾  刘树根  王国芝  李智武  刘顺  曹俊兴 《地球物理学报》2013,56(6):1958-1973

本文通过背斜褶皱变形与低温热年代学年龄(磷灰石和锆石(U-Th)/He、磷灰石裂变径迹)端元模型研究,约束低起伏度、低斜率地貌特征的四川盆地南部地区新生代隆升剥露过程.四川盆地南部沐川和桑木场背斜地区新生代渐新世-中新世发生了相似的快速隆升剥露过程(速率为~0.1 mm/a、现今地表剥蚀厚度1.0~2.0 km),反映出盆地克拉通基底对区域均一性快速抬升冷却过程的控制作用.川南沐川地区磷灰石(U-Th)/He年龄值为~10-28.6 Ma, 样品年龄与古深度具有明显的线性关系,揭示新生代~10-30 Ma以速率为0.12±0.02 mm/a的稳态隆升剥露过程.桑木场背斜地区磷灰石裂变径迹年龄为~36-52 Ma,古深度空间上样品AFT年龄变化不明显(~50 Ma)、且具有相似的径迹长度(~12.0 μm).磷灰石裂变径迹热演化史模拟表明桑木场地区经历三个阶段热演化过程:埋深增温阶段(~80 Ma以前)、缓慢抬升冷却阶段(80-20 Ma)和快速隆升剥露阶段(~20 Ma-现今),新生代隆升剥露速率大致分别为~0.025 mm/a和~0.1 mm/a.新生代青藏高原大规模地壳物质东向运动与四川盆地克拉通基底挤压,受板缘边界主断裂带差异性构造特征控制造就了青藏高原东缘不同的边界地貌特征.  相似文献   

西南大面积低温成矿域：研究意义、历史及新进展   总被引：8，自引：0，他引：8  

黄智龙  胡瑞忠  苏文超  温汉捷  刘燊  符亚洲 《矿物学报》2011,31(3):309-314

我国西南大面积低温成矿域是目前世界上公认的2个大面积低温成矿域之一,其面积之大（约100万km^2）、包含的矿种之多（Au、Hg、sb、As、P、Pb—Zn、Ag以及萤石、冰洲石、水晶、分散元素等）、矿床组成和组合之复杂全球罕见,是我国重要的Au、Hg、sb、As、Pb—zn、Ag以及多种分散元素生产基地。国内外学者对该成矿域进行了近30年的研究工作,取得了大量高水平研究成果,同时也存在许多有待深人研究的科学问题。本文回顾了我国西南大面积低温成矿域的研究历史,总结了各研究阶段的主要研究内容、主要研究成果和存在的主要科学问题,同时介绍了近年来我国西南大面积低温成矿域研究新进展。  相似文献   

一株低温降解菌的分离鉴定及其降解特性研究   总被引：1，自引：0，他引：1  

闫法军  田相利  董双林  牛宇峰 《中国海洋大学学报(自然科学版)》2011,41(3):24-30

从刺参(Apostichopus japonicus)养殖池塘环境中驯化分离筛选到1株低温有机物和氨氮降解菌株DB11。根据其形态特征、生理生化特性以及16S rDNA序列分析,将该菌株鉴定为马氏副球菌(Paracoccus marcusii)。经驯化,该菌株以刺参饵料为唯一营养源,低温(15℃)、低接种量(<5×10-3)条件下能同时高效降解饵料中的有机物和氨态氮,5 d时间内对富集培养基中COD和NH4+-N的降解率分别达50%和98%。进一步研究其降解特性表明,菌株生长适温15~30℃,生长适宜pH值为7~10,降解刺参饵料中COD和NH4+-N的最适温度条件为15~20℃、最适pH条件为8.0~8.5;在最适降解条件下、接种量为5×10-3时,对10~20 g/L高质量浓度的刺参饵料液中COD降解效果显著,3 d时间去除率达56.9%~65.7%,对1~20 g/L质量浓度的刺参饵料液中NH4+-N 3 d时间的去除率达91.7%~99.9%。  相似文献   

Post‐Palaeozoic uplift history of southeastern Australia revisited: Results from a process‐based model of landscape evolution     

P. A. Van der Beek  J. Braun  K. Lambeck 《Australian Journal of Earth Sciences》2013,60(2):157-172

Digital elevation models (DEMs) are widely relied upon as representations of the Earth's topographic morphology. The most widely used global DEMs available are ETOPO5, TerrainBase and JGP95E at a 5‐arc‐minute spatial resolution, and the GTOPO30 and GLOBE (version 1) global DEMs at a 30‐arc‐second spatial resolution. This paper presents the results of intercomparisons of these global DEMs over Australia, and with the GEODATA 9‐arc‐second DEM (version 1) of Australia. These DEMs were also compared to an independently produced, altimeter‐derived orthometric height database. This allows not only a totally independent assessment of the quality of these different DEMs over Australia, but also an insight into the ERS‐1 radar altimeter's ability to measure orthometric heights on land. The results of all these comparisons reveal large differences among the DEMs, with the greatest difference between JGP95E and ETOPO5 (mean 49 m, standard deviation ±274 m). The comparison with the altimeter‐derived database shows good agreement with the version 1 GEODATA DEM (mean 2 m, standard deviation ±27 m), thus demonstrating that the altimeter is a viable method for quality assessment of DEMs in lowland regions. A further conclusion is that the representation of the Australian land surface in both the JGP95E and TerrainBase global DEMs is more accurate than the higher resolution GLOBE (version 1) global DEM, even though JGP95E displays a disparity along the 140°E meridian because of the different data sources used in its construction.  相似文献   

Late Neoproterozoic to Holocene thermal history of the Precambrian Georgetown Inlier,northeast Australia     

R. A. Spikings  D. A. Foster  B. P. Kohn  P. B. O'Sullivan 《Australian Journal of Earth Sciences》2013,60(1):9-24

Carboniferous‐Permian volcanic complexes and isolated patches of Upper Jurassic — Lower Cretaceous sedimentary units provide a means to qualitatively assess the exhumation history of the Georgetown Inlier since ca 350 Ma. However, it is difficult to quantify its exhumation and tectonic history for earlier times. Thermochronological methods provide a means for assessing this problem. Biotite and alkali feldspar ⁴⁰Ar/³⁹Ar and apatite fission track data from the inlier record a protracted and non‐linear cooling history since ca 750 Ma. ⁴⁰Ar/³⁹Ar ages vary from 380 to 735 Ma, apatite fission track ages vary between 132 and 258 Ma and mean track lengths vary between 10.89 and 13.11 μm. These results record up to four periods of localised accelerated cooling within the temperature range of ～320–60°C and up to ～14 km of crustal exhumation in parts of the inlier since the Neoproterozoic, depending on how the geotherm varied with time. Accelerated cooling and exhumation rates (0.19–0.05 km/10⁶ years) are observed to have occurred during the Devonian, late Carboniferous‐Permian and mid‐Cretaceous — Holocene periods. A more poorly defined Neoproterozoic cooling event was possibly a response to the separation of Laurentia and Gondwana. The inlier may also have been reactivated in response to Delamerian‐age orogenesis. The Late Palaeozoic events were associated with tectonic accretion of terranes east of the Proterozoic basement. Post mid‐Cretaceous exhumation may be a far‐field response to extensional tectonism at the southern and eastern margins of the Australian plate. The spatial variation in data from the present‐day erosion surface suggests small‐scale fault‐bounded blocks experienced variable cooling histories. This is attributed to vertical displacement of up to ～2 km on faults, including sections of the Delaney Fault, during Late Palaeozoic and mid‐Cretaceous times.  相似文献   

Disequilibrium Between Short Term and Long Term Exhumation Rates in the Gongga Granite, Western Sichuan     

Kristen L. COOK  Yuan-Hsi Lee  Arjun Heimsath 《《地质学报》英文版》2013,87(Z1):38-38

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Diffusion Coefficients of Noble Gases in Natural Minerals: An Apparent Experimental Time Dependence Caused by Domain Size Spectra     

C. Fulda  H. J. Lippolt 《Mathematical Geology》2000,32(1):31-47

Noble gas diffusion coefficients in natural minerals are of use for evaluating geochronometric dates and other geochemical data. Usually, they are determined by degassing at elevated temperatures grain powders of natural samples containing radiogenic or cosmogenic noble gases. For conventional evaluations of diffusion parameters from degassing experiments, the grains should be uniform with respect to structure, composition, shape, and size. The shape and size prerequisites can hardly be fulfilled, because even two very narrowly meshed sieves produce spectra of domain sizes, partly because of the inhomogeneity of the minerals. Accurate determination of the actual spectrum is difficult and hardly practicable. Calculations of the fractional gas loss of a sample with a spectrum of domain sizes, presented in this study, show that almost any domain size spectrum leads to apparent diffusion coefficients that depend on the extent of degassing. The exception of this rule is given. The deviation from the physical diffusion coefficient can be several orders of magnitude as shown by examples. This effect, resulting from shape and width of the domain size spectra, possibly is responsible both for the large spread of Arrhenius parameters for the same mineral in the literature and for the deviation from linearity of some published Arrhenius lines. For limited domain size spectra and short degassing times, the formula for fractional gas loss is very similar to the formula of the fractional gas loss of a single domain size. An effective domain radius, which ensures that at least the measured diffusion coefficient for very short degassing times equals the physical diffusion coefficient, is given. In addition, the dimensionless treatment of the problem is presented that leads to a method to determine Arrhenius parameters without knowing the domain size spectrum. Accurate diffusion measurements of samples with a spectrum of domain sizes may also be possible if the domain size spectrum is taken into consideration. To this end the domain size spectra should be approximated by Taylor-expandable functions or by series of discrete domain sizes. For both cases, the formulae are given.  相似文献   

The causes of low-temperature demagnetization of remanence in multidomain magnetite   总被引：2，自引：0，他引：2  

A. R. Muxworthy  & E. McClelland 《Geophysical Journal International》2000,140(1):115-131

In this paper, the mechanisms of low-temperature demagnetization of remanence in multidomain magnetite are considered. New experimental observations of the behaviour of the saturation isothermal remanence, thermoremanence and partial thermoremanence at low temperatures are presented. The results show that there are two main contributions to this low-temperature demagnetization. The first and predominant contribution (type-1 demagnetization) is due to 'kinematic' domain state reorganization and occurs throughout cooling from room temperature to the Verwey transition, T _v , at 120–124  K. The second contribution arises from the change in anisotropy from cubic to monoclinic at T _v , which changes the overall domain structure of the grain. On warming in zero field, some domain walls will not return to their original positions but will take up a position that leads to a lower net remanence (type-2 demagnetization). In stoichiometric magnetite, demagnetization does not occur at 130  K at the isotropic point, T _k , contrary to some previous predictions. In non-stoichiometric magnetite, the influence of the Verwey transition is greatly reduced, and anomalous behaviour is observed at T _k .  相似文献