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1.
以黄土高原西北缘的靖远和古浪剖面(包含黄土层L1上部和占土壤层SO)作为研究对象,选取代表性样品进行磁化率、频率磁化率、热磁曲线、等温剩磁获得曲线和磁滞回线等测定.结果表明,靖远和古浪L1黄土和SO古土壤具有相似的岩石磁学特征.磁性矿物含量相对较低,载磁矿物均以磁铁矿为主,同时含有磁赤铁矿和赤铁矿,且SO占土壤中的磁赤...  相似文献   

2.
为了研究中亚黄土中的碳酸盐、有机质和可溶性盐等不同组分对磁化率的影响,本文对伊犁黄土样品分别进行盐酸、醋酸、蒸馏水和双氧水等处理,并与黄土高原黄土样品进行了对比.结果表明,盐酸不但可以溶蚀样品中的碳酸盐而且还可以与磁性矿物中的铁离子反应,分解超顺磁性颗粒(SP)中细颗粒组分,造成磁化率降低.与原样相比,中亚和黄土高原醋酸样品质量磁化率(x(f))和频率磁化率(x(fd))分别增加20.3%、53.4%o和4.8%、13.0%,说明中亚黄土碳酸盐对磁化率影响远大于黄土高原,醋酸对Sp没有影响或者影响很小.双氧水和蒸馏水样品x(f)变化幅度小于4%,说明黄土中有机质和易溶组分对磁化率的影响均非常小.此外,通过对中亚和黄土高原盐酸和醋酸样品的温度磁化率(TDS)曲线对比分析,表明黄土高原黄土退热过程磁性矿物的转化可能主要是SP组分中的细颗粒成分,伊犁黄土中纤铁矿和磁赤铁矿或针铁矿含量较黄土高原低.  相似文献   

3.
呼伦湖盆地扎赉诺尔晚第四纪湖泊沉积物为砂,泥质碎屑沉,地东露天矿剖面沉积物样品进行了低,高频磁化率测量,粒度分析,磁性矿物成分鉴定和Al2O3 ,Fe2O3含量分析,分析表明,磁铁矿是沉积物磁化率的主要贡献者,全铁含量控制了磁化率值的变化,磁化率与沉积物粒度呈负相关,进一步讨论认为,磁性矿物主要为粉砂-粘土级碎屑,集中分布在细粒沉积物中,因此造成其率较高,砂质沉积物中频率磁化率较高,其原因可能是其中的磁性颗粒比粉砂一粘土级沉积物中的磁性颗粒更细一些。  相似文献   

4.
佳县红粘土堆积的磁学性质及其古气候意义   总被引:7,自引:1,他引:7  
对佳县剖面红粘土作了较为详细的岩石磁学研究. 实验结果显示, 该地区红粘土堆积与黄土高原黄土-古土壤及其他红粘土堆积既具有相似的磁学性质, 又有明显的自身特点, 磁性矿物以磁铁矿、磁赤铁矿、赤铁矿为主, 褐铁矿/针铁矿含量较小. 同时, 红粘土与剖面上部午城黄土中的古土壤和黄土相似, 较强发育的古土壤层与弱发育的古土壤层相比, 显示低矫顽力特征和较高的超细颗粒含量, 说明在相对湿润气候条件下成壤作用的增强对超细颗粒的形成和磁性矿物的转化具有重要贡献, 体现出晚第三纪红粘土发育的古气候环境与黄土-古土壤相似, 具有波动变化的特点. 与黄土高原东部和南部风尘堆积的磁滞回线特征相比, 佳县红粘土样品达到饱和需要相对较高的磁场强度, 进一步证明了硬磁性矿物的存在和相应较弱的生物化学作用特征, 说明黄土高原北部与东部和南部的气候环境存在一定的差异性, 干旱化的程度相对较高.  相似文献   

5.
大荔人遗址黄土-古土壤剖面岩石磁学性质研究   总被引:1,自引:0,他引:1       下载免费PDF全文
自从大荔人化石被发现以来,其遗址剖面便成为研究热点.先前的研究主要集中在地层的对比划分与头盖骨年龄的推断方面,然而对于载磁矿物的鉴定及其古气候含义方面的研究却相对较少.鉴于此,本文运用热磁分析、饱和等温剩磁和剩磁矫顽力谱分析、磁滞回线分析、频率磁化率分析、热退磁分析等方法,对大荔人遗址剖面进行了系统的岩石磁学性质研究,鉴定出其主要载磁矿物为磁铁矿,赤铁矿,磁赤铁矿,磁畴状态主要是似单畴.磁铁矿,赤铁矿是样品中特征剩磁的携带者;主要起源于成土作用的超顺磁颗粒和新生成的亚铁磁性矿物,是古土壤样品磁化率增强的主要贡献者;古土壤中软磁性矿物的含量高于黄土.样品中磁赤铁矿的含量并不高.黄土-古土壤样品的频率磁化率曲线,古里雅冰芯氧同位素、细微粒浓度曲线,岐山五里铺剖面有机质含量曲线在古气候记录方面具有一致性,都展示出至少从MIS5以来,气候从冰期到间冰期的变化是渐变的,反之则表现了突变特征.上述岩石磁学研究丰富了大荔剖面的磁学领域研究内容,为相关课题的深入研究提供了依据.  相似文献   

6.
CBD方法对天然样品磁性矿物影响   总被引:2,自引:1,他引:1       下载免费PDF全文
本研究选择川西高原、天山和西伯利亚Kurtak剖面的黄土古土壤样品及亚热带非风成样品进行CBD处理,系统测量并对比处理前后的磁学参数,包括低频磁化率、频率磁化率、非磁滞剩磁、饱和等温剩磁、剩磁矫顽力和热磁曲线(J-T曲线),分析处理前后磁性矿物种类、含量和磁畴的变化.结果表明,CBD方法对于磁性矿物的溶解并无明显的选择性,在温度与反应时间一定的条件下,磁性矿物的溶出量主要受控于其粒径分布.CBD方法可以非常有效地去除具有更大比表面积的细粒(< 1 μm)磁性矿物,同时溶解粗粒(>1 μm)磁性矿物外缘,使其粒径变细.CBD处理后磁化率变化存在多种可能,对于成土作用较强的古土壤,CBD方法可以较为准确地提取成土成因的磁性信息;而干旱和过度湿润条件下的风积黄土,不宜使用CBD方法区分原生与次生磁性矿物.  相似文献   

7.
伊犁黄土的磁学性质及其与黄土高原对比   总被引:6,自引:0,他引:6       下载免费PDF全文
近20多年来黄土高原的黄土磁学性质与古气候研究取得了重要进展, 极大地推动了东亚古季风演化、亚洲内陆干旱化及过去全球变化的研究, 但对亚洲内陆天山地区的黄土磁学性质知之甚少. 选择天山伊犁盆地黄土剖面进行了系统的磁性测量, 包括磁化率、无磁滞磁化率、高低温磁化率和磁滞参数等, 并与黄土高原进行了对比, 开展了伊犁黄土的X射线衍射矿物学分析, 初步探讨了伊犁黄土磁化率增强的机制. 结果表明, 伊犁黄土磁性矿物的总含量要远远低于黄土高原, 但磁性矿物类型与黄土高原黄土基本类似, 以磁铁矿、磁赤铁矿和赤铁矿为主, 部分样品还有钛铁矿等. 在磁性矿物中磁赤铁矿占的比例总体上要比黄土高原黄土低, 而磁铁矿和赤铁矿占的比例比黄土高原黄土要高. 磁性矿物的粒度要比黄土高原粗, 以准单畴(PSD)和多畴(MD)为主. 成壤作用产生的细粒超顺磁体对磁化率的贡献非常有限, 粒径为PSD和MD的磁铁矿和磁赤铁矿为伊犁黄土磁化率的主要贡献者. 伊犁黄土磁化率增强既有风速论模式(阿拉斯加或西伯利亚黄土成土模式), 又有黄土高原超细颗粒成壤模式, 但以前一种模式为主导. 伊犁黄土磁化率增强除与源区的原生磁性矿物有关以外, 还与当地的地形气候环境和地质背景有关. 伊犁黄土磁化率增强的机制十分复杂, 将磁化率应用古气候的解释时要慎重.  相似文献   

8.
三门峡盆地晚新生代沉积物磁性载体类型   总被引:3,自引:2,他引:3       下载免费PDF全文
对三门峡盆地晚新生代沉积岩样品进行岩石磁学研究,通过三轴饱和等温剩磁和剩磁矫顽力实验、交变退磁和热退磁实验及磁化率测定,发现黄土-古土壤、河湖相灰绿层和冲洪积层3种不同岩性的磁载体存在显著差异.即黄土-古土壤以磁铁矿为主,赤铁矿和磁赤铁矿很少;河湖相灰绿色沉积磁性矿物含量较低,主要为赤铁矿和磁铁矿,但磁铁矿较多,此外还有一些不稳定磁性矿物(如针铁矿、菱铁矿等);冲洪积物以磁铁矿和赤铁矿为主,磁铁矿相对较多.  相似文献   

9.
甘肃第三系红粘土磁学性质初步研究及古气候意义   总被引:19,自引:4,他引:19  
研究表明红粘土与黄土-古土壤具有共同的磁性矿物, 即磁铁矿、磁赤铁矿、赤铁矿(可能还有褐铁矿); 红粘土的磁化率大小与超细顺磁性颗粒的含量正相关; 它与第四纪的黄土-古土壤相似, 在湿润气候条件下由成壤作用形成的超细铁磁性矿物对于红粘土中古土壤层的磁化率增大有重要的贡献, 并得到了Rb/Sr比值的证实. 尽管红粘土中也发现了磁化率与其成土强度不对应的现象,但总体上看红粘土的磁化率仍不失为一个简便的古气候替代性指标. 根据磁化率曲线, 从红粘土发展到黄土沉积,其间的古气候变化幅度大致等同于阶段5(S1)到阶段2 - 4(L1)的变化幅度, 可能表明第四纪期间风场加强、从源区携带比上新世更多(大约两倍)较粗的弱风化风积物(不含超顺磁性颗粒)到黄土高原. 7.5 Ma以来, 中国北方中部风积红粘土的出现记录了从下伏白垩纪红砂岩到晚第三纪的重要气候转变. 红粘土的发展与白垩纪以来全球干旱化和变冷密切相关, 可能由于当时青藏高原的强烈隆升导致了东亚季风开始或加强, 从而有了红粘土的堆积.  相似文献   

10.
天山北麓黄土环境磁学特征及其古气候意义   总被引:1,自引:0,他引:1       下载免费PDF全文
新疆黄土-古土壤序列环境磁学参数的变化机理及其气候意义仍存在争议.本文选择天山北麓的中梁黄土剖面,系统开展了低温和常温下环境磁学参数的测试与研究,测量包括室温的磁化率与饱和磁化强度,以及磁化率与饱和剩余磁化强度的低温变化.结果发现,该剖面黄土和古土壤样品的磁性矿物主要由磁铁矿与磁赤铁矿组成,不含任何粒级成壤形成的超顺磁矿物颗粒,其磁化率信号主要记录了粉尘磁性矿物含量变化,较高的磁化率指示较强的风动力状况或者较近的风尘源区,新疆黄土的这种环境磁学"风尘输入模式"可用来重建干旱区的风动力强弱变化.  相似文献   

11.
Frequency-dependent magnetic susceptibility, which is an important tool for environmental and palaeoclimatologic research, is usually relatively low, mostly less than 15% of the low frequency value and there is a demand for high precision of its measurement. The accuracy required for the susceptibility measurement at individual operating frequencies for precise determination of the parameter characterizing the frequency-dependent susceptibility was investigated theoretically and also experimentally through repeated measurement of artificial specimens and sediments of a loess/palaeosol sequence using the MFK1 Kappabridge. It was found that the variation in the frequency-dependence in the order of 1% is well reproducible and the measurements can be interpreted in terms of magnetic granulometry even in weakly magnetic materials.  相似文献   

12.
Inter-laboratory and absolute calibrations of rock magnetic parameters are fundamental for grounding a rock magnetic database and for semi-quantitative estimates about the magnetic mineral assemblage of a natural sample. Even a dimensionless ratio, such as anhysteretic susceptibility normalized by magnetic susceptibility (Ka/K) may be biased by improper calibration of one or both of the two instruments used to measure Ka and K. In addition, the intensity of the anhysteretic remanent magnetization (ARM) of a given sample depends on the experimental process by which the remanence is imparted. We report an inter-laboratory calibration of these two key parameters, using two sets of artificial reference samples: a paramagnetic rare earth salt, Gd2O3 and a commercial “pozzolanico” cement containing oxidized magnetite with grain size of less than 0.1 μm according to hysteresis properties. Using Gd2O3 the 10 Kappabridges magnetic susceptibility meters (AGICO KLY-2 or KLY-3 models) tested prove to be cross-calibrated to within 1%. On the other hand, Kappabridges provide a low-field susceptibility value that is ca. 6% lower than the tabulated value for Gd2O3, while average high-field susceptibility values measured on a range of instruments are indistinguishable from the tabulated value. Therefore, we suggest that Kappabridge values should be multiplied by 1.06 to achieve absolute calibration. Bartington Instruments magnetic susceptibility meters with MS2B sensors produce values that are 2-13% lower than Kappabridge values, with a strong dependence on sample centering within the sensor. The Ka/K ratio of ca. 11, originally obtained on discrete cement samples with a 2G Enterprises superconducting rock magnetometer and a KLY-2, is consistent with reference parameters for magnetites of grain size <0.1 μm. On the other hand, Ka values from a 2G Enterprises magnetometer and K values from a Bartington Instruments MS2C loop sensor for u-channel and discrete cement samples, will produce average Ka/K values that are unrealistically high if not properly corrected for the nominal volume detected by the sensors for these instruments. Inter-laboratory measurements of K and Ka for standard paleomagnetic plastic cubes filled with cement indicate remarkable differences in the intensity of the newly produced ARMs (with a standard deviation of ca. 21%), that are significantly larger than the differences observed from the calibration of the different magnetometers employed in each laboratory. Differences in the alternating field decay rate are likely the major source of these variations, but cannot account for all the observed variability. With such large variations in experimental conditions, classical interpretation of a “King plot” of Ka versus K would imply significant differences in the determination of grain size of magnetite particles on the same material.  相似文献   

13.
The study on magnetic properties of the red clay indicates that the red clay and loess- paleosol sequence have a common magnetic mineralogy, with magnetite, maghemite, hematite (and possibly goethite) contributing to the magnetic behavior. The red clay magnetic susceptibility is also found to have a positive relation with extrafine superparamagnetic grains. This suggests that, like the Quaternary loess-paleosols, an ultrafine ferrimagnetic component produced during pe-dogenesis in the red clay under humid conditions also plays an important role in susceptibility enhancement in the soil units. This is supported by the correlation between Rb/Sr ratio and magnetic susceptibility. This signifies that, like the above loess-paleosol sequence, the magnetic susceptibility of the red clay can be used as a general proxy paleoclimatic indicator, although whether its susceptibility in the red clay is comparable to pedogenesis intensity and requires further investigation. Magnetic susceptibility variation in the red clay thus also provides an eo-lian/pedogenic record of paleoclimatic evolution. Study of the background susceptibility indicates that, on average, the absolute scale of the paleoclimatic shift from red clay development to Quaternary loess deposition is similar to the climatic shift from stage 5 (S1) to stage 2-4 (L1). This may suggest that during the Quaternary there is an evident strengthening of the absolute wind intensity to bring more (about double) coarser and less weathered (non-SP fraction) eolian magnetic input from the source regions to the Loess Plateau than during the Pliocene. The presence of eolian red clay since 7.5 Ma BP in central-northern China implies an important envi-ronmental change from the underlying Cretaceous red sandstone. The red clay development was closely related to global drying and climate cooling since the Cretaceous and closely associated with the abrupt uplift of the Qinghai-Xizang Plateau at about that time. This uplift of the plateau intensified the East Asia monsoon system and started red clay deposition.  相似文献   

14.
末次冰期时,在雅鲁藏布大峡谷入口处发育了一个古冰川堰塞湖,称为格嘎古堰塞湖.该堰塞湖是认识冰川阻江地貌效应的重要地质证据.古冰川堰塞湖可能会发生多次溃决洪水,通过堰塞湖沉积的分析可以获取堰塞期间的水文事件的信息.本文通过对古堰塞湖沉积39个样品多种磁学参数的详细分析发现,湖相沉积中的砂层低频磁化率(Xlf)为291×10-8m3/kg,泥质沉积的Xlf仅为42×10-8m3/kg;而非磁滞剩磁磁化率(XARM)和饱和等温剩磁(SIRM)的差别则较小.进一步的X-T、Loop和IRM研究以及XARM/Xlf表明,砂层中包含较多的粗颗粒磁铁矿是Xlf较高的主要原因,说明砂层中的磁性矿物没有经过风化破坏,应为近源沉积,并且快速埋藏,指示了溃决事件.本文的结果表明,利用岩石磁学性质以检测古堰塞湖溃决事件是一种可行的新方法.  相似文献   

15.
The study on magnetic properties of the red clay indicates that the red clay and loesspaleosol sequence have a common magnetic mineralogy, with magnetite, maghemite, hematite (and possibly goethite) contributing to the magnetic behavior. The red clay magnetic susceptibility is also found to have a positive relation with extrafine superparamagnetic grains. This suggests that, like the Quaternary loess-paleosols, an ultrafine ferrimagnetic component produced during pedogenesis in the red clay under humid conditions also plays an important role in susceptibility enhancement in the soil units. This is supported by the correlation between Rb/Sr ratio and magnetic susceptibility. This signifies that, like the above loess-paleosol sequence, the magnetic susceptibility of the red clay can be used as a general proxy paleoclimatic indicator, although whether its susceptibility in the red clay is comparable to pedogenesis intensity and requires further investigation. Magnetic susceptibility variation in the red clay thus also provides an eolian/pedogenic record of paleoclimatic evolution. Study of the background susceptibility indicates that, on average, the absolute scale of the paleoclimatic shift from red clay development to Quaternary loess deposition is similar to the climatic shift from stage 5 (S1) to stage 2–4 (L1). This may suggest that during the Quaternary there is an evident strengthening of the absolute wind intensity to bring more (about double) coarser and less weathered (non-SP fraction) eolian magnetic input from the source regions to the Loess Plateau than during the Pliocene. The presence of eolian red clay since 7.5 Ma BP in central-northern China implies an important environmental change from the underlying Cretaceous red sandstone. The red clay development was closely related to global drying and climate cooling since the Cretaceous and closely associated with the abrupt uplift of the Qinghai-Xizang Plateau at about that time. This uplift of the plateau intensified the East Asia monsoon system and started red clay deposition.  相似文献   

16.
The KLY-4S Kappabridge and KLF-4A Magnetic Susceptibility Meter enable automated measurement of susceptibility variation with field in the ranges of 2–450 A/m and 5–300 A/m (in effective values), respectively. Unfortunately, the measurement accuracy decreases with decreasing field and it is not easy to decide whether the susceptibility variation at the lowest fields is natural phenomenon or results from measuring errors. To overcome this problem, the accuracies of both the above instruments were investigated experimentally using artificial specimens (mixture of pure magnetite and plaster of Paris) with variable susceptibilities ranging from 1 × 10−5 to 5 × 10−2. The complete curve of the field variation of susceptibility of each specimen was measured 10 times and the relative error was calculated for each field. In the KLY-4S Kappabridge, in specimens with susceptibilities higher than 100 × 10−6, the relative errors are lower than 3% in all fields and lower than 1% in the fields stronger than 10 A/m. In the KLF-4A Magnetic Susceptibility Meter, in relatively strongly magnetic specimens with susceptibilities 5 × 10−4 to 5 × 10−2, the relative error is less than 1.5% in the entire field range. While the former instrument is convenient for investigating almost all rock types, the latter instrument is convenient for measuring moderately and strongly magnetic specimens. To facilitate work with field variation of susceptibility curves, showing variable accuracies with field, the programme FieldVar was written. One of its options is plotting the measured data with corresponding field-variable error bars. In this way, a tool is offered for interpreting such susceptibility changes that are sound and reasonable from the point of view of measuring accuracy.  相似文献   

17.
Results of magnetic susceptibility mapping around a coal-burning power plant were used to verify the field in situ measurements with data acquired in laboratory on soil samples collected at approximately the same measurement grid sites at different distance from the source. This comparison enables quantifying the field data obtained using the Bartington MS2 meter and to relate them, at least approximately, to mass specific values. Moreover, it is shown that certain diversity in the grid points of field measurements and soil sampling can slightly bias the field measurements. However, this shift is of minor significance and Bartington field readings can be considered as reliable.  相似文献   

18.
The Longxi region contains different kinds of Cenozoic sediments, including eolian deposits, reworked loess, fluvial and lacustrine deposits. The provenance evolution of these sediments is of great significance in exploring the uplift, tectonic deformation and associated with geomorphic evolution of the Northeastern Tibetan Plateau. In this paper, we used the single-grain zircon provenance analysis to constrain the provenances for the Paleogene alluvial conglomerates and for the Neogene fluvial-lacustrine sediments, and compared them with results from the loess deposits since the Miocene. The results show that: (1) the Paleogene alluvial conglomerates contain a large number of detrital zircons ranging from 560 to 1100 Ma that were derived from the Yangzi Block. However, the sediments of early Miocene have much fewer zircons of this age span, which are characterized by an abundance of zircon ages in the ranges of 200–360 Ma. This indicates that the Paleogene alluvial conglomerates mainly come from the middle and/or southern West Qinling, and the early Miocene sediments are primarily from the northern West Qinling; (2) Late Neogene fluvial sediments (11.5 Ma onward) in Tianshui-Qinan region are dominated by zircon ages of 380–450 Ma. This zircon population is similar to that of the exposed intrusive rocks of southern part of the Liupan Mountains, implying that the southern part of Liupan Mountains probably had already uplifted by 11.5 Ma; (3) Late Miocene lacustrine sediments in Tianshui region have a zircon age spectra that is remarkably different from coeval fluvial deposits, but is similar to the zircon age distributions of the Miocene loess in Qinan region, late Miocene-Pliocene Hipparion red clay and Quaternary loess. This indicates that fine particles within these Miocene lacustrine sediments in Tianshui region may be dominated by aeolian materials. This study reveals that provenance changes of Cenozoic sediments in Tianshui-Qinan region and its geomorphic evolution are closely related to the multi-stage uplift of the Northeastern Tibetan Plateau. In particular, the major uplift of the Northern Tibetan Plateau during late Oligocene-early Miocene may have not only provided the source areas and wind dynamic conditions for the deposits of the Miocene loess, but also provided the geomorphic conditions for its accumulation.  相似文献   

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