文13西块油藏岩石形变对采收率影响研究

低渗透、异常高压油藏弹性能量充足,储层欠压实,岩石易发生弹塑性变形。根据这些油藏特性,从达西定律的角度推导出了室内一维岩芯中最终采出程度与岩石物性变化的近似关系式,并引入渗透率变化因子分析采收率的影响因素,进而以文13西块油藏岩石为例,通过不同流体介质的渗透率压敏性试验,以及不同加压方式下渗透率变化试验,结合降压弹性开采试验和水驱物理模拟试验,以渗透率变化因子为基础,分析并讨论该类油藏的开采方法。结果表明：该类油藏在保持较慢降压速度、较高孔隙压力水平时,能够获得较高的油藏采收率。     

中国气温变化的两个基本模态的诊断和模拟研究

我国地域辽阔,气候复杂多变,在全球变暖的背景下研究中国近百年来的气温变化具有重要的意义。为此我们重建了中国东部71个站1880—2004年四季气温距平序列。通过EOF分析发现了中国气温变化的2种最基本的模态：东部一致变化和关内关外相反变化。这2种模态不随季节变化,而且在不同时期也是稳定的。通过研究这2种模态与变暖趋势的关系发现,20世纪80年代以来的变暖主要是由于第一模态在该时期持续的正位相增强造成的;而20世纪20~40年代的变暖主要是由于第二模态所呈现的正位相所造成的。此外,我们检验了这2种模态在大气环流模式（CAM）中的表现。结果表明：121年（模式中1880—2000年）的集合模拟在一定程度上可以重现第一模态的变化,而第二模态则仅在冬季表现明显。最后,以冬季为例,利用1880—2004年重建及观测的500 hPa高度场资料,通过合成分析进一步研究了这2种模态的环流机制：第一模态正位相对应纬向环流增强,表现在地面气温分布上为东部一致变暖。而负位相则对应东亚大槽加深,东部地区一致变冷。第二模态正位相对应的环流分布则为从东亚北部到阿留申为负距平,东亚到北太平洋中纬度为正距平;对应地面气温分布为关内变暖关外变冷。负位相时环流分布基本相反。这样的环流机制得到了模式研究的支持。     

Dominant Modes of Interannual Variability in Atmospheric Water Vapor Content over East Asia during Winter and Their Associated Mechanisms

Atmospheric water vapor content(WVC) is a critical factor for East Asian winter precipitation. This study investigates the dominant modes of interannual variability in WVC over East Asia during winter and their underlying mechanisms.Based on the empirical orthogonal function(EOF) method, the leading mode(EOF1, R~2 = 28.9%) of the interannual variability in the East Asian winter WVC exhibits a meridional dipole pattern characterized by opposite WVC anomalies over northeastern China and eastern China; the second mode(EOF2, R~2 = 24.3%) of the interannual variability in the East Asian winter WVC exhibits a monopole pattern characterized by consistent WVC anomalies over eastern China. EOF1 is mainly modulated by two anomalous zonal water vapor transport(WVT) branches over northeastern China and eastern China, which are associated with an anomalous atmospheric wave train over Eurasia affected by sea ice cover in the Kara Sea-Barents Sea(SIC-KSBS) area in the preceding October-November(ON). EOF2 is mainly modulated by an anomalous westerly WVT branch over eastern China, which is associated with a circumglobal atmospheric zonal wave train in the Northern Hemisphere. This circumglobal zonal wave train is modulated by concurrent central and eastern tropical Pacific sea surface temperature anomalies. The SIC-KSBS anomalies in ON and the concurrent SST anomalies over tropical Pacific may partially account for the interannual variability of EOF1 and EOF2 winter WVC, and thus may provide a theoretical basis for improving the prediction of winter climate over East Asia.     

地球自由振荡弹性简正模研究进展与展望

在构建现代地球模型时,地球内部分层结构主要是根据地震波资料确定的;而地球内部密度及弹性参数,特别是地幔以下大尺度结构的密度分布,则主要是根据地球自由振荡的弹性简正模观测资料确定的.本文概述了地球自由振荡简正模本征值的求解理论和方法,介绍了球型和环型模态位移场表达式,讨论了地球自由振荡模态的衰减、分裂与耦合效应;总结了多线态分裂谱线探测和分裂参数估计的方法,综述了利用弹性简正模开展地震矩张量、地球三维非均匀性结构和内核超速旋转约束与反演研究的主要进展和存在的问题.最后作为展望,本文还讨论了地球自由振荡简正模的未来研究趋势.     

中国冬夏季气温和降水异常耦合关系的SVD与MEOF分析对比

以揭示中国冬、夏季气温、降水之间的同期耦合时空特征为例,比较了SVD与MEOF分析所得主要正交模的相关关系及均衡性,论证了SVD方法在揭示两个要素场序列互相关关系上的优越性。结果表明:1) SVD的分解对象仅包含反映两种要素场相关关系的信息,而MEOF还包含了两个要素场各自的自相关信息,前者分解对象更纯粹。2) MEOF和SVD揭示的气温和降水空间耦合模态正负异常分布大致相似,但相较SVD所揭示的耦合模态,MEOF分析的冬、夏季气温、降水主要正交模存在不均衡现象,即一个主要MEOF正交模往往侧重描述两种异常要素场中的一种,这种差异在冬季尤为突出。SVD方法揭示了中国冬、夏季同期气温、降水间局域高温少降水或低温多降水是二者主要异常配置,且相关性夏强冬弱。3)比较SVD、MEOF方法同序正交模的相关系数和均衡度发现,SVD多数正交模的相关系数较MEOF的更大、更稳定,且均通过显著性检验,MEOF的冬季部分正交模相关系数未通过显著性检验; SVD主要正交模的均衡性冬季优于MEOF分析、夏季优于(第一模态)或者接近于(第二、三模态) MEOF分析。故SVD方法是揭示两要素之间耦合关系的更好方法。     

基于环流和海温的稻曲病指数长期预报模型研究

稻曲病属于典型的"气象型"病害,为了提前预报出适宜稻曲病发生的气象等级与提供足够的防治准备时间,根据中长期天气预报原理,充分考虑大气环流和太平洋海温对区域气象条件影响的滞后性,利用近40 a的江苏逐日气象观测资料、大气环流指数和海温资料,采用空间拓扑原理和最优相关普查等统计方法,挑选出了对综合稻曲病指数影响最显著的预报因子,并通过滑动平均和主成分识别等检验方法确保预报因子的稳定性和独立性,最终分别建立了基于大气环流因子和基于海温因子的综合稻曲病指数长期预报模型。经过检验,两种模型的模拟效果均理想,能提前一个月预报出综合稻曲病指数以及对应的发病气象等级。     

Could the energy near the FCN and the FICN be explained by luni-solar or atmospheric forcing?

The observed time-series of precession/nutation show residuals with respect to an empirical model based on the rigid Earth theoretical nutations and a frequency dependent transfer function with resonances to the Earth's normal modes. These residuals display energy mainly in the frequency domain around 430 and 500 days in the inertial frame. In this frequency band, the energy is possibly related to two normalmode frequencies: the free core nutation (FCN) and the free inner core nutation (FICN). In this paper, we examine the possibility of obtaining this energy from the resonance effect induced by a luni-solar (or planetary) forcing, or by an atmospheric forcing at a frequency very close to these Earth free nutations. The amplification factor due to the resonance is computed from an analytical formula expressed in the case of a simplified three-layer ellipsoidal rotating earth (with an elastic inner core, a liquid outer core and an elastic mantle), as well as the empirical formula based on the analysis of VLBI observations. For the tidal forcing, the theoretical results do not show any resonance at the level of precision we have examined but it is still possible to find one frequency near the FCN or FICN frequencies which could be excited. In contrast, for the atmospheric pressure the level of energy needed could be obtained from the diurnal pressure, depending on the noise level of the Earth's global pressure. We also show that the combination of three waves can explain the observed decrease of energy with time. While the tidal potential amplitudes are too small, a pressure noise level of 0.5 Pa would be sufficient to excite these waves.     

Effects of a mushy transition zone at the inner core boundary on the Slichter modes

This article investigates the effects of a mushy inner core boundary on the eigenperiods of the Slichter modes for a simple, but realistic, earth model (rotating, spherical configuration, elastic inner core and mantle, neutrally stratified, inviscid, compressible liquid core). It is found that the influence of the mushy boundary layer is substantial compared with some other effects, such as those from elasticity of the mantle, non-neutral stratification of the liquid outer core and ellipticity of the Earth and centrifugal potential. The results obtained here may set a lower bound on the eigenperiods of the Slichter modes for a realistic earth model. For example, for a PREM model, the lower bound of the central period of the Slichter modes should be about 5.3 hr.