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1.
天山北缘新近系沉积物岩石磁学研究 总被引：4，自引：0，他引：4
岩石磁学研究表明, 天山北缘塔西河剖面新近系可划分为湖相沉积型、河流相沉积型和冲积扇沉积型三种类型, 分别对应于剖面的底部(沙湾组和塔西河组中下部)、中部(塔西河组顶部和独山子组中下部)和上部(独山子组顶部和西域组), 其中湖相沉积岩石磁学性质复杂, 除与沉积物物源密切相关外, 还可能受风化作用、原地磁性矿物自生或成岩作用以及生物活动的影响, 天然剩磁强度为10-3~10-2 A/m, 主要磁性矿物为磁铁矿, 高矫顽力磁性矿物可能为针铁矿. 磁性矿物颗粒由假单畴和单畴(PSD+SD)或单畴和超顺磁混合组成(SD+SP); 河流相沉积天然剩磁强度为10-2~10-1 A/m, 主要磁性矿物为磁铁矿和赤铁矿, 磁性矿物颗粒为假单畴(PSD), 450~580℃可获得稳定的特征剩磁方向, 特征剩磁载磁矿物为磁铁矿; 冲积扇沉积天然剩磁强度介于湖相和河流相沉积之间, 主要磁性矿物也为磁铁矿和赤铁矿, 580~680℃获得稳定特征剩磁方向, 特征剩磁载磁矿物为赤铁矿, 磁性矿物颗粒为假单畴(PSD). 相似文献
2.
对甘肃西山坪遗址剖面样品进行磁化率、频率磁化率、热磁分析、非磁滞剩磁和等温剩磁等一系列岩石磁学实验测试,分析环境磁学参数特征变化,试图探讨西山坪遗址研究意义,为今后深入研究该沉积序列蕴含的古环境记录提供了岩石磁学基础.结果表明：西山坪遗址剖面沉积物中磁性矿物主要以低矫顽力的磁铁矿和磁赤铁矿为主,高矫顽力磁性矿物赤铁矿含量极其有限,越向剖面表层,强磁性矿物含量逐渐增加.磁性矿物颗粒表现出黄土的典型特征,以单畴、准单畴为主,含有一定量的超顺磁颗粒,颗粒度越向剖面表层越细.从物源上看,遗址沉积物主要来自近源的黄土风尘堆积,主要是风成堆积,并混合大量人类活动信息,给今后综合研究岩石磁学与人类活动特征的关系有一定借鉴意义. 相似文献
3.
中中新世黄土高原风尘堆积序列磁化率显著增高，在区域内已成为地层对比标志，然而其磁性增强机制依然不清楚.本文对秦安地区QA-I剖面约14～17.1 Ma期间的黄土-古土壤样品进行了系统的环境磁学、岩石磁学(热磁性质、磁滞性质、非磁滞剩磁与饱和等温剩磁比值χARM/SIRM等)和色度指标分析.结果表明，QA-I剖面黄土-古土壤序列样品中磁性矿物为准单畴(PSD)磁铁矿、超顺磁/单畴(SP/SD)磁赤铁矿和赤铁矿，古土壤中细粒磁赤铁矿含量高于上下相邻黄土层.CBD(Citrate-Bicarbonate-Dithionite)处理方法显示，中中新世风尘序列中碎屑成因的PSD磁铁矿含量变化不大，约14.5～16.0 Ma期间成壤成因SP/SD磁赤铁矿含量的增多，是导致该时期风尘堆积序列磁化率增强的主要原因；这与该时期较低的土壤发育程度并不一致，表明CBD处理方法虽然可有效获取成壤成因SP/SD磁赤铁矿信息，却无法区分其为当地还是源区成壤成因.低温磁学研究表明，QA-I剖面约14.5～16.0 Ma期间SP/SD磁赤铁矿可能为碎屑磁铁矿颗粒的风化外壳，其含量高低变化与风尘样... 相似文献
4.
黄铁矿热转化矿物相变过程的岩石磁学研究 总被引：2，自引：0，他引：2
对天然黄铁矿样品在氩气和空气环境中受热发生的矿物相变过程进行了系统的岩石磁学研究,结果表明：氩气环境（还原环境）下,黄铁矿受热分解转化的产物是磁黄铁矿,其粒度为单畴,矫顽力和剩磁矫顽力分别约为20和30mT,它在还原环境中是稳定的．而空气环境（氧化环境）中黄铁矿受热分解、转化后的最终产物为单畴赤铁矿,FORC图显示其矫顽力高达1400mT,相应的热转化序列为：黄铁矿→磁黄铁矿→磁铁矿→赤铁矿．上述结果对于理解还原环境沉积物的磁性、岩石次生化学剩磁和陨石磁学性质都具有重要参考意义． 相似文献
5.
本文对发育在澳大利亚悉尼附近的Long Reef Beach中新世古土壤剖面进行了系统的岩石磁学研究,测量了磁化率、饱和磁化强度、饱和等温剩磁、非磁滞剩磁等常温磁学参数和磁滞回线,并对所有样品进行了热磁分析.实验结果表明:全新世软土层主要磁性矿物为MD颗粒磁铁矿,磁性矿物含量与黄土高原黄土层相当.中新世老成土层随地层深度增加主要磁性矿物由磁铁矿转变为磁赤铁矿,随着磁铁矿向磁赤铁矿的转化,开始出现赤铁矿;磁性矿物粒径分布较广,以PSD颗粒为主,其次为SD颗粒,同时含有少量MD颗粒;磁性矿物含量高于黄土高原强发育古土壤层.中新世红土矿层主要磁性矿物为赤铁矿,同时含有少量磁赤铁矿和针铁矿,属于铁的富集层,赤铁矿以SD颗粒为主,含少量PSD和MD颗粒.Long Reef Beach中新世古土壤形成时期,对应着一种全球性高温多雨气候,地表化学风化作用十分强烈.丰富的降水,导致中新世老成土层发生淋溶作用,磁铁矿在向下淋溶迁移过程中逐渐氧化为磁赤铁矿和赤铁矿,铁氧化物最终在红土矿层淀积,磁赤铁矿经高温压实作用再结晶转化为赤铁矿.磁性矿物转化过程可概括为磁铁矿—磁赤铁矿化的磁铁矿—磁赤铁矿—赤铁矿,其中部分磁赤铁矿具有热稳定性,在空气(氩气)环境中加热到700℃未发生转化. 相似文献
6.
以热磁分析为主,对中国北方泥河湾盆地更新世河湖相地层中灰绿色粉砂和灰黄色粉砂/细砂两种典型沉积物进行了详细的岩石磁学研究,有效确定了这两类沉积物中磁性矿物的种类、粒度特征以及加热过程中磁性矿物的变化过程和产物,并对其包含的古环境意义进行了初步探讨.灰绿色粉砂样品主要含有磁铁矿和赤铁矿两种磁性矿物,磁性相对较弱,颗粒相对较细;灰黄色粉砂/细砂主要含有磁铁矿和磁赤铁矿,磁性相对较强,颗粒相对较粗.在氩气环境中经700℃加热处理后,这两种沉积物中的绿泥石都分解,并生成超细粒（处于超顺磁和单畴颗粒区间）的磁铁矿,导致磁化率大幅升高.因此泥河湾盆地沉积物的热磁特征可以用来检测样品中绿泥石的相对含量,进而反映该地区化学风化作用强度的变化.此外,灰绿色粉砂样品中绿泥石含量比灰黄色粉砂/细砂样品的含量高,在氩气中加热后,磁化率升高幅度也较高,可能反映了化学风化相对较弱的沉积环境. 相似文献
7.
8.
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
9.
石炭-二叠纪时期被认为是全球构造运动机制由古到新的转换期.在这一时期内,塔里木板块内部经历了大规模的岩浆活动,构成了我国境内又一个大火成岩省.综合研究塔里木大火成岩省早二叠世玄武岩中磁性矿物组合类型、特征和粒径,可为进一步明确其快速形成过程提供必要的岩石磁学依据.本文对采自柯坪地区库普库兹满和开派兹雷克组样品进行了系统的岩石磁实验,包括饱和等温剩磁获得曲线、三轴等温剩磁系统热退磁实验、k-T曲线、磁滞回线和一阶反转曲线等.实验结果表明,库普库兹满组和开派兹雷克组样品中以钛磁铁矿和磁铁矿等低矫顽力磁性矿物为主,磁性矿物磁畴类型为SD、PSD与MD颗粒混合.本文结果还显示开派兹雷克组与库普库兹满组样品适宜开展进一步的古强度研究. 相似文献
10.
本文选择内蒙古呼伦湖表层沉积物为研究对象,通过测量沉积物样品的室温下χ-T曲线、等温剩磁获得曲线和反向场退磁曲线、一阶反转曲线(FORC图)以及低温(20～300 K)下剩磁随温度变化曲线、Verwey转变温度,结合电子显微镜分析,获得了样品中磁性矿物组成信息.揭示出呼伦湖表层沉积物中磁性矿物含量较低,以假畴磁铁矿为主,含有部分单畴和多畴颗粒.这些结果对于理解呼伦湖沉积物的磁性信号、古环境和古气候重建等具有研究价值. 相似文献
11.
Rock magnetic criteria for the detection of biogenic magnetite 总被引：15，自引：0，他引：15
Bruce M. Moskowitz Richard B. Frankel Dennis A. Bazylinski 《Earth and Planetary Science Letters》1993,120(3-4):283-300
We report results on the magnetic properties of magnetites produced by magnetotactic and dissimilatory iron-reducing bacteria. Magnetotactic bacterial (MTB) strains MS1, MV1 and MV2 and dissimilatory iron-reducing bacterium strain GS-15, grown in pure cultures, were used in this study. Our results suggest that a combination of room temperature coercivity analysis and low temperature remanence measurements provides a characteristic magnetic signature for intact chains of single domain (SD) particles of magnetite from MTBs. The most useful magnetic property measurements include: (1) acquisition and demagnetization of isothermal remanent magnetization (IRM) using static, pulse and alternating fields; (2) acquisition of anhysteretic remanent magnetization (ARM); and (3) thermal dependence of low temperature (20 K) saturation IRM after cooling in zero field (ZFC) or in a 2.5 T field (FC) from 300 K. However, potentially the most diagnostic magnetic parameter for magnetosome chain identification in bulk sediment samples is related to the difference between low temperature zero-field and field cooled SIRMs on warming through the Verwey transition (T ≈ 100 K). Intact chains of unoxidized magnetite magnetosomes have ratios of δFC/δZFC greater than 2, where the parameter δ is a measure of the amount of remanence lost by warming through the Verwey transition. Disruption of the chain structure or conversion of the magnetosomes to maghemite reduces the δFC/δZFC ratio to around 1, similar to values observed for some inorganic magnetite, maghemite, greigite and GS-15 particles. Numerical simulations of δFC/δZFC ratios for simple binary mixtures of magnetosome chains and inorganic magnetic fractions suggest that the δFC/δZFC parameter can be a sensitive indicator of biogenic magnetite in the form of intact chains of magnetite magnetosomes and can be a useful magnetic technique for identifying them in whole-sediment samples. The strength of our approach lies in the comparative ease and rapidity with which magnetic measurements can be made, compared to techniques such as electron microscopy. 相似文献
12.
We have investigated the low-temperature behavior of a suite of ‘grown’ synthetic and natural magnetites that span single-domain (SD) and multidomain (MD) behavior. Synthetic samples had been grown in the laboratory either in an aqueous medium or in glass. Natural samples included SD magnetites occurring in plagioclase and truly MD magnetites in the form of large octahedra. In all experiments a sample was first given a saturation remanence at room temperature; next, moment was measured continuously during cooling and warming between 230 K and 60 K. Similar to results reported earlier by other workers, magnetic memory is large in SD samples, whereas truly MD samples are almost completely demagnetized by cycling between room temperature and 60 K. Pseudo-single-domain samples exhibit behavior that is intermediate with respect to that of the SD and truly MD states. When data from this study are combined with data obtained by Hartstra [10] from sized, natural magnetites, it is found that the percentage of total remanence that survives cycling between room temperature and 60 K decreases linearly with the logarithm of grain size and, thus, with increasing number of domains. This relation suggests that memory can provide a reasonable estimate of grain size in those magnetite-bearing rocks for which these samples provide good analogues. Remarkably, some of the large natural octahedra provide a magnified view of MD response to low temperatures and thus reveal two surprising and intriguing types of behavior. First, below approximately 180 K these octahedra demagnetize through a series of large Barkhausen jumps. Second, near 117 K these same octahedra exhibit a ‘wild zone’, where magnetic moment executes large, random excursions. We interpret these two phenomena as direct evidence for the unpinning and irreversible displacement of domain walls in response to the drop in coercivity and, possibly, the broadening of domain walls as temperatures drop toward the isotropic point. One implication of this behavior is that cooling to progressively lower temperatures could provide an effective method for stepwise removal of paleomagnetic components carried by MD grains, even without passage through the isotropic point of magnetite. 相似文献
13.
A Precambrian metadolerite dyke has two distinct types of remanence carriers; those with medium/high coercivities (unblocking fields of 20–120 mT) and those with low coercivities (unblocking fields of <15 mT). Optical examination reveals numerous submicron probably opaque inclusions in the plagioclase feldspar and also large opaque grains consisting of coarse oxidation-exsolution intergrowths of magnetite and ilmenite. All opaque phases have been examined using transmission electron microscopy together with microanalysis and electron diffraction. The submicron inclusions in the plagioclase are titanomagnetites(0 < x ≤ 0.14) with a size range between about 0.01 and 0.5 μm and axial ratios between 1 (equidimensional) and about 0.3. Many of these inclusions fall in the single-domain field but some are probably pseudo-single-domain. The large opaque grains contain almost pure magnetite and ilmenite and show no fine-scale exsolution; the magnetite regions of the intergrowths are of multidomain size and reveal multidomain structure under Lorentz electron microscopy. There are also some primary ilmenites containing very fine exsolved haematite, and there are very fine plates of ilmenite and very elongate needles of magnetite within the augite. Experiments on artificial samples containing very carefully prepared separates of plagioclase and large opaque grains show that the pure plagioclase acquires a remanence with unblocking fields of 20–140 mT and blocking temperatures of 390–590°C and the large opaque grains acquire a remanence with unblocking fields of less than 15 mT but a wide range of blocking temperatures up to about 570°C. It is concluded that the medium/high coercivity component of remanence in the rock is carried largely or possibly entirely by the submicron magnetites within the plagioclase and that the low coercivity component is carried largely or entirely by the multidomain magnetites in the large opaques. The contribution of the magnetite needles in the augite is uncertain as the rock does not contain any detectable component of remanence with the extremely high coercivities expected from their very elongate shape. 相似文献
14.
Palaeomagnetism of the loess/palaeosol sequence in Viatovo (NE Bulgaria) in the Danube basin 总被引：1，自引：0，他引：1
Diana Jordanova Jozef Hus Jordan Evlogiev Raoul Geeraerts 《Physics of the Earth and Planetary Interiors》2008,167(1-2):71-83
The results of a palaeomagnetic investigation of a 27 m thick loess/palaeosol sequence in Viatovo (NE Bulgaria) are presented in this paper. The sequence consists of topsoil S0, seven loess horizons (L1–L7) and six interbedded palaeosols (S1–S6) overlying a red clay (terra rossa) complex. Magnetic viscosity experiments, IRM acquisition, AMS analysis and NRM stepwise alternating and thermal demagnetisation experiments of pilot samples were implemented for precise determination of the characteristic remanence and construction of a reliable magnetostratigraphical scheme. Analysis of IRM acquisition curves using the expectation – maximization algorithm of Heslop et al. [Heslop, D., Dekkers, M., Kruiver, P., van Oorschot, H., 2002. Analysis of isothermal remanent magnetization acquisition curves using the expectation – maximization algorithm. Geophys. J. Int., 148, 58–64] suggests that the best fitting is obtained by three coercivity components. Component 1 corresponds to SD maghemite/magnetite, while component 2 is probably related to the presence of oxidised detrital magnetites. The third component shows varying coercivities depending on the degree of pedogenic alteration of the samples and probably reflects the presence of detrital magnetite grains oxidised at different degree.
The relevance of the Viatovo section as a key representative sequence for the loess cover in the Danube basin is confirmed by the presence of geomagnetic polarity changes in the lower part of the sequence. The youngest one recorded in the seventh loess unit L7 can be identified as corresponding to the Matuyama/Brunhes palaeomagnetic polarity transition. Two normal magnetozones were found in the red clay complex, probably corresponding to the Jaramillo and Olduvai subchronozones of the Matuyama chron. 相似文献
15.
Christopher R. Scotese Rob Van der Voo Chad McCabe 《Physics of the Earth and Planetary Interiors》1982,30(4):385-395
Paleomagnetic directions for the Upper Silurian and Lower Devonian carbonates of the Helderberg escarpment (New York State) differ from expected Late Silurian and Early Devonian directions for cratonic North America. The mean direction (D = 165°, I = −10°; paleopole at 50°N 129°E) is similar to Late Carboniferous and Early Permian results. Negative fold tests, and a lack of reversals, suggest that the magnetization is secondary. However, low coercivities, low blocking temperatures, the thermomagnetic curves (TC near 570°C) and the acquisition of isothermal remanent magnetizations all suggest that the remanence is carried by magnetite. If a detrital origin of these magnetites is assumed, the secondary nature of the remanence would argue for thermal resetting as a result of deep burial of the rocks. However, no evidence for such thermal resetting is seen in the alteration of conodonts. More likely perhaps is a chemical or thermochemical origin of the remanence; this would require the magnetites to be authigenic. 相似文献
16.
泰国Ｋｈｏｒａｔ盆地西部的晚二叠世石灰岩的古地磁研究表明磁铁矿为稳定剩磁的主要载体多组分磁分量分离技术揭示了高温磁组分（或高矫顽力）具有呈对分布的正、反极性．但是，应用逐渐展平岩层法可以发现各采样点的平均特征磁化方向在岩层展平至３０％时．磁化方向最为集中．这一发现表明二叠纪石灰岩中所揭示出的磁化方向很可能形成于褶皱（期）过程中．野外观察表明，二叠纪石灰岩在印支期发生强烈褶皱并被晚三叠世湖相石灰岩角度不整合覆盖．所以二叠纪石灰岩的重磁化很可能发生在中、晚三叠世的印支期．这些石灰岩样品切片后经显微镜、扫描电镜和电子探针分析，次生磁铁矿多数与方解石微晶和铁质碳酸钙粒共生，且多分布在方解石脉附近．重磁化很可能是由于印支期造山运动时，铁质碳酸钙受碳水化合物流体的蚀变作用所引起的。 相似文献
17.
通过下佛罗统磁性地层学研究,获得了一些能记录岩石形成时的地磁场的样品,根据常规的古地磁方法,等温剩磁和热退磁实验,说明这些岩石的主要载磁矿物为磁铁矿.磁滞回线参数的测量表明多数载磁矿物磁铁矿为假单磁畴,少量样品则可能为假单磁畴与多磁畴的混合物.通过与北美古生代重磁化岩石的磁滞回线参数比值对比,说明重磁化与非重磁化岩五磁滞回线参数比值的分布趋势有明显差别,这一差别可能用于判定岩石的重磁化和非重磁化性质. 相似文献
18.
通过下佛罗统磁性地层学研究,获得了一些能记录岩石形成时的地磁场的样品,根据常规的古地磁方法,等温剩磁和热退磁实验,说明这些岩石的主要载磁矿物为磁铁矿.磁滞回线参数的测量表明多数载磁矿物磁铁矿为假单磁畴,少量样品则可能为假单磁畴与多磁畴的混合物.通过与北美古生代重磁化岩石的磁滞回线参数比值对比,说明重磁化与非重磁化岩五磁滞回线参数比值的分布趋势有明显差别,这一差别可能用于判定岩石的重磁化和非重磁化性质. 相似文献
19.
This paper reports the alternating field demagnetization characteristics of glass–ceramic magnetite assemblages carrying weak-field thermoremanent magnetization (TRM), weak-field anhysteretic remanent magnetization (ARM), and saturation remanence (Jrs). Average grain sizes vary from less than 0.1 μm to approximately 100 μm, and hysteresis parameters indicate that these assemblages encompass single-domain (SD) through truly multidomain (MD) behavior. In all assemblages, weak-field TRM and weak-field ARM are more stable to alternating field demagnetization than is (Jrs). This response is especially remarkable in the 100 μm assemblage, which otherwise displays truly MD behavior. Although the SD samples pass the Lowrie–Fuller test for SD behavior, calculations presented here show that populations of noninteracting, uniaxial SD grains should behave in just the opposite sense to that reported originally by Lowrie and Fuller. This discrepancy could indicate that SD, glass–ceramic magnetite populations are more affected by magnetic interactions than would be expected for magnetite crystals that nucleated individually from a silicate matrix. This interpretation is supported by the SD assemblages failing the ‘Cisowski' test: that is, the curves for acquisition and AF demagnetization of (Jrs) intersect well below the 50% mark. However, a second and intriguing explanation of the SD-like results obtained from all samples is that alternating field demagnetization characteristics reflect a strong dependence of local energy minimum domain state, and its associated stability, on the state of magnetization. 相似文献