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本文根据Cluster卫星上的粒子成像质谱仪（RAPID）探测器在穿越地球等离子体片过程中的观测数据,统计研究了等离子体片中能量离子能量密度的空间分布（氢离子能量范围从40keV到1500keV,氦离子和氧离子从10keV到1500keV）,并且给出了离子能量密度在不同地磁活动时期随GSE Z向分布的剖面.研究表明能量离子的能量密度以及能量密度的梯度与地磁活动指数Kp之间存在近似线性的关系.观测结果表明形成这种分布变化的主要原因是在地磁活动期间在电流片附近离子能量密度的增加,特别是其中的重离子成分增加更为显著.本文通过一个简化的电流片模型的数值计算,定性地研究了形成能量离子空间分布的机理.计算表明重离子在电流片中可以获得更多的能量,电流片加速可能是形成能量密度分布变化的一种可能的机制. 相似文献
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香蒲、灯心草人工湿地的研究─Ⅱ.净化污水的空间 总被引：26，自引：0，他引：26
应用测定流水中溶氧量的方法,测定了长薄鳅的耗氧率,耗氧量及窒息点．试验表明：长薄鳅的耗氧率（Ｙ’）随鱼体重（Ｗ,ｇ）的增加而增大,其关系式分别为：Ｙ’＝１８６．５７６Ｗ（－０．２０４３）,Ｙ＝０．１８６Ｗ（０．７９６２）．温度对长薄鳅的耗氧率有影响,在１３－３０Ｃ范围内,耗氧率随水温升高而逐渐增大．耗氧率的温度敏感区域是１３－２３Ｃ和２８－３０Ｃ,而在２３－２８Ｃ范围内变化幅度较小,标准代谢量变化 相似文献
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作者发现：太阳辐射,地球自转与公转,黄、赤交角的存在,陆地和海洋在地球表面南、北半球的不规则、不对称地理分布,及地球内部因〖ZZ(〗核外液体〖ZZ)〗形成的分层结构,构成了一套天然的能使地球产生自由章动的日、地间动量（能量）相耦合的物理机制.经研究,由该机制产生的极移具有以下主要特征：（1）极移轨迹的运动周期为13个月（0.92周/年）,该周期由二个主要分量组成,一个为12个月（1周/年）,另一个是14.1个月（0.85周/年,即钱德勒周期）.（2）极移运动轨迹是是椭圆,短半轴（b）与长半轴(a)之比为0.86;扁率（a\|b/a）为1：7.1.（3）瞬时极移振幅|m|的变化：对1周/年项,|m|随太阳回归运动而变化,在二至点时最大,在二分点时最小,具有对称性;对0.85周/年项,|m|随太阳回归运动而变化,在夏至点最大,每年12月5日左右最小.（4）瞬时极移存在反向运动（由东向西）.在1周/年项极移运动中,自转极的正、反方向运动振幅的贡献各占50%;在0.85周/年项的极移运动中,反向运动的时间仅有33天,约占正向运动时间的1/10,正向运动振幅的贡献占96%,反向运动振幅的贡献大约占4%.（5）若以国际极点（CIO）为原点,自转极相对CIO的位移运动轨迹必然落在偏向于CIO的西侧.（6）极移振幅将长期保持下去而不会衰减,原因是太阳辐射为自转轴受迫摆动提供了长期、稳定的激发能源. 相似文献
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利用低纬地磁午链上H和D分量的分均值数据，分析了2000年4月6日磁暴期间磁扰变化的纬度效应。主要特点是：（1）急始期间H分量急始跃变 幅随磁纬降低而减小，且急始变幅的下降率磁纬降低而逐渐增大；（2）初相期间H分量第2峰值的变幅和初相持续时间随磁纬降低而减小；（3）主相期间H分量迅速减小，并随纬度降低最大变幅明显增加；（4）恢复相H分量呈两阶段上升趋势，前一阶段迅速上升，后一了阶段上升速度明显减小。最后对这些磁扰变化的纬度效应与空间电流体系的密切关系作了讨论。 相似文献
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本文探讨了OH Meinel夜气辉辐射的光化学模式，给出OH(ν≤9)分子数密度分布的计算通式，重点研究了化学反应HO\-2+O→OH(ν≤6)+O2对ν≤6各振动能级上OH分子数密度分布以及(ν′—ν″)(ν′≤6)振动带气辉辐射的影响.结果表明，该反应对数密度的贡献随振动能级的减小而增大，对(ν′—ν″)振动带辐射的贡献随着较高振动能级ν′的减小而增大，以春分时为例，它可使第1振动能级上的OH分子最大数密度和（1—0）带的最大辐射率增加约33%，第6振动能级上的最大数密度和（6—ν″）带的最大辐射率增加约7%，（1—0）带的辐射强度增加约30%，（6—ν″）带的强度增加约11%.该反应使各振动能级上分子数密度的高度分布剖面以及各振动带体辐射率的高度分布剖面变宽，最大数密度、最大发射率所处的高度下降1 km左右.此外，该反应的影响程度随着原子氧密度的降低而增大，随着温度的升高而增大，并且在夏至时最大，在冬至时最小. 相似文献
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目的:通过CT增强图像测量肠系膜上动脉与腹主动脉间隙面积,并评估其与体重指数（BMI）的相关性。资料与方法:行腹部CT增强检查的538例非肠系膜上动脉综合征患者,根据体重指数及性别各分成4个级别（Ⅰ级:BMI<18.5 kg/m2;Ⅱ级:BMI 18.5~24.9 kg/m2;Ⅲ级:BMI 25~29.9 kg/m2;Ⅳ级:BMI ≥ 30 kg/m2）。结果:男、女组间隙面积与BMI均呈显著正相关（r=00.50、0.55,P<0.01）,间隙面积与BMI分级均呈中等相关（r=00.43、0.45,P<0.01）。随BMI增加,该间隙面积增大。结论:通过肠系膜上动脉与腹主动脉间隙面积和BMI呈显著正相关,可以为诊断SMAS提供参考值标准及筛查依据。 相似文献
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对2001年昆仑山口西Ms81级地震产生的断层带,布设了沿断层和横跨断层的两条人工地震测线.通过对观测资料的定量分析和处理,求得了昆仑山断层带内部的细结构.分析工作包括从S波震相开始的振幅谱计算、速度频散计算、群速度测量,并用面波频散方法反演S波速度结构,用振幅谱比的方法估计断层带的Q值.野外试验结果表明,S波震相与围陷波组的时间差随炮点与台站之间距离增大而增加,在断层带外的测点上观测到与断层带相关的场地效应.最后得出昆仑山断层带宽度为250m、速度结构为断层内低速的分层结构和Q值为15（断层内）和30（围岩）.虽然昆仑山口西地震的震级比美国加州Landers地震的震级（Ms76）大,且地震产生的破裂带长度长得多,但是这两个地震断层带的宽度却相差不大. 相似文献
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在具有代表性的正旋回砂砾岩储层中，８种不同岩性的典型样品，在５种含油（气）水饱和状态下测试了纵、横波速度（Ｖｐ和Ｖｓ）与有效覆盖压力（△Ｐ）变化关系曲线。结果表明：（１）Ｖｐ和Ｖｓ与△Ｐ呈指数递增，Ｖｐ和Ｖｓ随△Ｐ变化在低压范围比高压范围更敏感，而Ｖｐ比Ｖｓ的灵敏度高。（２）同一状态下，同一非均质单层内的岩性变化范围控制了不同的Ｖｐ－△Ｐ，Ｖｓ－△Ｐ曲线族的宽度。岩性由细到粗，Ｖｐ－△Ｐ曲线由低向高变化，含钙、含砾粗砂岩的Ｖｐ－△Ｐ曲线处于曲线族的上界，砾状砂岩的Ｖｐ－△Ｐ曲线低于含砾粗砂岩的Ｖｐ－△Ｐ曲线。Ｖｓ－△Ｐ曲线也有上述规律。（３）同一样品，研究５种不同饱和度状态下的Ｖｐ－△Ｐ和Ｖｓ－△Ｐ曲线，发现无论压力条件如何，波速与饱和度均呈线性关系。（４）在同一的非均质单层内，Ｖｐ－△Ｐ，Ｖｓ－△Ｐ变化曲线随着含油、气、水饱和状态的不同具有明显的分带性。气饱和Ｖｐ－△Ｐ曲线族在形态及幅度变化上明显区别于油、水饱和状态，束缚水、残余油状态的Ｖｐ－△Ｐ曲线族，Ｖｓ－△Ｐ曲线也有上述规律。气饱和状态的Ｖｐ和Ｖｓ随△Ｐ变化的敏感度高于油、水饱和状态，气饱和状态的Ｖｐ随△Ｐ变化的敏感度高于Ｖｓ。 相似文献
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Hydraulic properties of saturated and unsaturated stony soils were studied on a 3.35 m long column, 1.24 m in diameter, filled with alternating sand and boulder layers. The boulders averaged 6.2 × 15 × 20 cm in size and were laid down on their flat side. Tensiometers and a neutron probe access tube were placed in the column for measuring pressure heads and water contents, respectively. Saturated conditions were obtained by ponding the column. The resulting hydraulic conductivity K was 5.1 m/day. This value could also be calculated from the measured K for the sand alone on separate samples, using a simple equation that takes into account the void ratio of the sand alone and that of the boulder-sand mixture. Unsaturated K was determined by applying water at less than ponded infiltration rates. Resulting relations between the unsaturated K and water content or negative pressure head could also be estimated from the relation between unsaturated K and pressure head for the sand alone and the calculated saturated K of the boulder-sand mixture. The method of Millington and Quirk for calculating the relation between unsaturated K and water content also gave reasonable results. The dispersivity of the boulder-sand column was 18 times that of the sand alone. Pore velocity was accurately estimated as the Darcy velocity divided by the volumetric water content. Hydraulic properties of stony vadose zones are difficult to determine. This work shows that they can be estimated from K relations measured in the laboratory on samples of the soil between the rocks. Knowledge of hydraulic properties of vadose zones is important in predicting movement of water and pollutants to the underlying ground water. 相似文献
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伽马射线与地层介质的康普顿（Ｃｏｍｐｔｏｎ）效应是密度测井的理论基础，介质对伽马射线的康普顿吸收系数取决于介质的原子核性质及其体积密度．（超热或热）中子测井主要反映地层介质的减速性质，而后者主要取决于介质的含氢量．介质含氢量是由介质的组分及其体积密度决定的．本文从上述两种测井方法的测量原理出发，从理论上证明了这两种测井方法并非两种互相独立的测量手段．对于含油气盆地常见沉积岩石及矿物，两种测井测量结果具有相关性．这一结论为密度、中子测井方法组合地质应用提供了理论依据，利用密度－中子测井的相关性可有效地识别轻质油气层特别是天然气层．实例表明，无论水层还是油气层，两种测井曲线均具有良好的相关性．利用这种相关性明显改善了识别天然气层和划分油－气界面的精度． 相似文献
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伽马射线与地层介质的康普顿（Ｃｏｍｐｔｏｎ）效应是密度测井的理论基础，介质对伽马射线的康普顿吸收系数取决于介质的原子核性质及其体积密度．（超热或热）中子测井主要反映地层介质的减速性质，而后者主要取决于介质的含氢量．介质含氢量是由介质的组分及其体积密度决定的．本文从上述两种测井方法的测量原理出发，从理论上证明了这两种测井方法并非两种互相独立的测量手段．对于含油气盆地常见沉积岩石及矿物，两种测井测量结果具有相关性．这一结论为密度、中子测井方法组合地质应用提供了理论依据，利用密度－中子测井的相关性可有效地识别轻质油气层特别是天然气层．实例表明，无论水层还是油气层，两种测井曲线均具有良好的相关性．利用这种相关性明显改善了识别天然气层和划分油－气界面的精度． 相似文献
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Laura Carmine Elsa Aristodemou Christopher Pain Ann Muggeridge Cassiano de Oliveira 《Geophysical Prospecting》2008,56(1):115-140
The purpose of this work was to investigate a new and fast inversion methodology for the prediction of subsurface formation properties such as porosity, salinity and oil saturation, using time‐dependent nuclear well logging data. Although the ultimate aim is to apply the technique to real‐field data, an initial investigation as described in this paper, was first required; this has been carried out using simulation results from the time‐dependent radiation transport problem within a borehole. Simulated neutron and γ‐ray fluxes at two sodium iodide (NaI) detectors, one near and one far from a pulsed neutron source emitting at ～14 MeV, were used for the investigation. A total of 67 energy groups from the BUGLE96 cross section library together with 567 property combinations were employed for the original flux response generation, achieved by solving numerically the time‐dependent Boltzmann radiation transport equation in its even parity form. Material property combinations (scenarios) and their correspondent teaching outputs (flux response at detectors) are used to train the Artificial Neural Networks (ANNs) and test data is used to assess the accuracy of the ANNs. The trained networks are then used to produce a surrogate model of the expensive, in terms of computational time and resources, forward model with which a simple inversion method is applied to calculate material properties from the time evolution of flux responses at the two detectors. The inversion technique uses a fast surrogate model comprising 8026 artificial neural networks, which consist of an input layer with three input units (neurons) for porosity, salinity and oil saturation; and two hidden layers and one output neuron representing the scalar photon or neutron flux prediction at the detector. This is the first time this technique has been applied to invert pulsed neutron logging tool information and the results produced are very promising. The next step in the procedure is to apply the methodology to real data. 相似文献
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The exchanges of water, energy and carbon between the land surface and the atmosphere are tightly coupled, so that errors in simulating evapotranspiration lead to errors in simulating both the water and carbon balances. Areas with seasonally frozen soils present a particular challenge due to the snowmelt-dominated hydrology and the impact of soil freezing on the soil hydraulic properties and plant root water uptake. Land surface schemes that have been applied in high latitudes often have reported problems with simulating the snowpack and runoff. Models applied at the Boreal Ecosystem Research and Monitoring Sites in central Saskatchewan have consistently over-predicted evapotranspiration as compared with flux tower estimates. We assessed the performance of two Canadian land surface schemes (CLASS and CLASS-CTEM) for simulating point-scale evapotranspiration at an instrumented jack pine sandy upland site in the southern edge of the boreal forest in Saskatchewan, Canada. Consistent with past reported results, these models over-predicted evapotranspiration, as compared with flux tower observations, but only in the spring period. Looking systematically at soil properties and vegetation characteristics, we found that the dominant control on evapotranspiration within these models was the canopy conductance. However, the problem of excessive spring ET could not be solved satisfactorily by changing the soil or vegetation parameters. The model overestimation of spring ET coincided with the overestimation of spring soil liquid water content. Improved algorithms for the infiltration of snowmelt into frozen soils and plant-water uptake during the snowmelt and soil thaw periods may be key to addressing the biases in spring ET. 相似文献
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本文导出了一种给出相对烈度在lg R~0之间的收敛解(忽略震级)的小震方程式。结合在贝加尔地区岩石抗震特性调查与文字资料和统一理论,使人们可对震源等势面进行评估。确定了在震源区边界处的地震烈度稳定性和弹性波在地壳中的传播,使得推导出从地震主要参数震级向随震中距不同的烈度定量计算的转换成为可能。获得了烈度(能通量的密度)对距离的双线性相关,给出了能通量密度和相对烈度之间的关系。求出了取决于地表建筑地基的物理特性的振动载荷烈度。在地震学角度,这种强震的定量预测方法是一种提供详细地震区划和场地小区划的可能手段之一。 相似文献
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《Advances in water resources》2005,28(11):1254-1266
A detailed model was formulated to describe the non-isothermal transport of water in the unsaturated soil zone. The model consists of the coupled equations of mass conservation for the liquid phase, gas phase and water vapor and the energy conservation equation. The water transport mechanisms considered are convection in the liquid phase, and convection, diffusion and dispersion of vapor in the gas phase. The boundary conditions at the soil–atmosphere interface include dynamical mass flux and energy flux that accounts for radiation transport. Comparison of numerical simulations results with published experimental data demonstrated that the present model is able to describe water and energy transport dynamics, including situations of low and moderate soil moisture contents. Analysis of field studies on soil drying suggests that that dispersion flux of the water vapor near the soil surface, which is seldom considered in soil drying models, can make a significant contribution to the total water flux. 相似文献
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Absract The manganese content of the surface (river, lake) and subsurface waters of Transbaikalia is determined. The geographical
peculiarities of manganese distribution in natural waters are found to be due to different Mn concentrations in drained rocks
and soils, as well as to the geochemical redox conditions of migration. The areas with low, medium, and high concentrations
of Mn in natural waters and the sources of water in which Mn concentrations exceed MAC are revealed.
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Translated from Vodnye Resursy, Vol. 32, No. 5, 2005, pp. 597–600.
Original Russian Text Copyright ? 2005 by Kashin, Ivanov. 相似文献
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E. M. Dmitriev 《Izvestiya Physics of the Solid Earth》2018,54(5):775-781
Radon-222 is inert radioactive gas with a half-life period of 3.8 days, it is a decay product of radium-226. Being escaped from minerals and underground waters into pore space of rocks and soil, it is transported to the surface by diffusion and advection and gone to the atmosphere. When modeling processes of atmosphere radon transport one sets value of radon flux from the surface, depending on contents of radium-226 in rocks and conditions of radon transport in soil, especially on soil porosity and humidity. The impact of radon turbulent transport in the atmospheric boundary layer (ABL) on radon flux density from the surface is estimated in this paper. It is shown that both for stationary state and for typical diurnal variations of the radon volumetric activity (VA) in the ABL, the correction to the radon flux density caused by its turbulent transport in the ABL is negligible (less than 1%) and doesn’t exceed measurement errors. Thus, when calculating radon VA in the ABL it is really possible to set an average value of the radon flux density on the surface as a boundary condition. 相似文献