海洋环境下粉煤灰混凝土的抗冻性与抗氯离子渗透性的耦合

针对海洋环境条件,重点研究了粉煤灰混凝土的抗冻性和氯离子渗透性能的相互关系.试验分别研究了水胶比、粉煤灰等量取代水泥掺量大小、引气剂掺量等因素对抗冻性和抗氯离子渗透性能的影响,并与普通混凝土进行了对比.结果表明,粉煤灰不增加混凝土的抗海水冻融耐久性;粉煤灰增加混凝土的抗氯离子渗透性能,但是掺量超过30%,抗氯离子渗透性能下降;粉煤灰对混凝土抗冻性和抗氯离子渗透性的耦合影响在30%左右存在一个最佳掺量.为评估混凝土的抗冻性和氯离子扩散性的耦合性能,提出了新的评价方法--冻渗比(R值方法),并进行了试验验证.SEM和MIP微观分析与R值方法评价的结果是吻合的.     

综合工程物探在九寨沟核心景区水循环系统研究中应用评价

综合物探技术是一种高新技术,在岩土工程中有广泛的应用前景。文章介绍了瑞雷波勘探和直流电法在九寨沟核心景区水循环系统中的应用,对方法原理进行了简单阐述,并探讨了对综合工程物探技术在九寨沟景区第四系化学沉积钙华层和冰碛地层的划分的分析评价。     

灰色关联度法在地下水脆弱性评价与分区中的应用

提出采用灰色系统理论中的灰色关联度分析方法对地下水脆弱性进行研究,选取地下水位埋深、包气带岩性、含水层砂层厚度等6个因子建立脆弱性评价指标体系,采用离差最大化方法确定评价指标的权重,使得权重的分配有了一定的理论依据。并以MATLAB为平台编制了常用计算程序,将其应用于抚州市地下水脆弱性评价与分区,取得良好结果。     

郑州市区断裂深循环型地热资源计算与评价

地热资源是一利用前景广阔的新型清洁环保能源。对郑州市区断裂深循环型热储模型进行了分析,采用积存热量法（体积法）对断裂深循环型地热资源进行了计算与评价,最后提出建议：建议河南省加大地热资源勘查投入力度,严格执行有关行业标准,进行系统的地热勘查评价工作。     

自转微椭、非均匀地球的潮汐变形

鉴于当前国际上关于自转微椭、非均匀地球（ＳＲＥＨＩ）的固体潮汐响应的结果之间存在明显分歧,特别是Ｌｏｖｅ数ｋ及重力潮汐因子δ对纬度的依赖情况截然不同,本文借助于摄动法与张量正则分量的广义球谐展开建立起来的侧向非均匀、自转微椭、粘弹地球的潮汐模拟理论,计算了ＳＲＥＨＩ地球的潮汐形变及相应的引力位变化．结果表明,描述径向位移的Ｌｏｖｅ数的纬度依赖部分系数ｈ＋与球对称部分ｈ０＋δｈ０之比不大于１．０‰;对Ｏ１波为０．２７‰;对Ｍ2波为０．１９‰;对Ｍ3波为０．４９‰;对Ｍ4波为０．８８‰．描述地球引力位变化的Ｌｏｖｅ数的纬度依赖部分系数ｋ＋与球对称部分ｋ０＋δｋ０之比小于３．０‰;对Ｏ１波为２．６７‰;对Ｍ２波为１．８９‰;对Ｍ３波为２．２４‰;对Ｍ４波为２．７０‰．     

区域水资源可持续利用评价

水资源可持续利用评价是可持续发展战略研究的核心问题之一,选取合适的评价方法是正确评价水资源可持续利用的基本前提。在目前提出的评价方法中,关键性的问题是如何合理确定各个评价指标的权重,层次分析法是解决这一问题常用的有效方法。但是,层次分析法没有给出判断矩阵一致性的调整方法;而且评价结果也只能表明各个指标对水资源可持续利用的影响大小,并不能判断研究区水资源可持续利用程度。本文在层次分析法的基础上,探讨了判断矩阵一致性的修正方法,构造出判断水资源可持续利用程度的综合指数,并对云南省水资源可持续利用程度进行评价。     

竖直受力桩的影响半径rm讨论

提出计算竖直受力桩的位移协调法,具有模型简单、参数易取的优点。用来分析桩侧土影响半径rm,结果表明,随着桩顶荷载P增大,桩长细比L/d增大,都会使rm扩大;土质越好,rm越小。此外,也说明,现行建筑基础规范中有关桩间距规定的合理性。     

Inversion of two-dimensional tidal open boundary conditions of M<Subscript>2</Subscript> constituent in the Bohai and Yellow Seas

Two-dimensional tidal open boundary conditions of the M2 constituent in the Bohai and Yellow Seas(BYS) have been estimated by assimilating T/P altimeter data.During inversion,independent point(IP) strategy was used,in which several IPs on the open boundary is assumed,values at these IPs can be optimized with an adjoint method,and those at other grid points are determined by linearly interpolating the values at IPs.The reasonability and feasibility of the model are tested by ideal twin experiments.In the practical experiment(PE) after assimilation,the cost function may reach 1% or less of its initial value.Mean absolute errors in amplitude and phase can be less than 5 cm and 5°,respectively,and the obtained co-chart can show the character of the M2 constituent in the BYS.The results of the PE indicate that using only two IPs on the open boundary can yield better simulated results.     

The electrical structure of the Slave craton

The Slave craton in northwestern Canada, a relatively small Archean craton (600×400 km), is ideal as a natural laboratory for investigating the formation and evolution of Mesoarchean and Neoarchean sub-continental lithospheric mantle (SCLM). Excellent outcrop and the discovery of economic diamondiferous kimberlite pipes in the centre of the craton during the early 1990s have led to an unparalleled amount of geoscientific information becoming available.

Over the last 5 years deep-probing electromagnetic surveys were conducted on the Slave, using the natural-source magnetotelluric (MT) technique, as part of a variety of programs to study the craton and determine its regional-scale electrical structure. Two of the four types of surveys involved novel MT data acquisition; one through frozen lakes along ice roads during winter, and the second using ocean-bottom MT instrumentation deployed from float planes.

The primary initial objective of the MT surveys was to determine the geometry of the topography of the lithosphere–asthenosphere boundary (LAB) across the Slave craton. However, the MT responses revealed, completely serendipitously, a remarkable anomaly in electrical conductivity in the SCLM of the central Slave craton. This Central Slave Mantle Conductor (CSMC) anomaly is modelled as a localized region of low resistivity (10–15 Ω m) beginning at depths of 80–120 km and striking NE–SW. Where precisely located, it is spatially coincident with the Eocene-aged kimberlite field in the central part of the craton (the so-called “Corridor of Hope”), and also with a geochemically defined ultra-depleted harzburgitic layer interpreted as oceanic or arc-related lithosphere emplaced during early tectonism. The CSMC lies wholly within the NE–SW striking central zone defined by Grütter et al. [Grütter, H.S., Apter, D.B., Kong, J., 1999. Crust–mantle coupling; evidence from mantle-derived xenocrystic garnets. Contributed paper at: The 7th International Kimberlite Conference Proceeding, J.B. Dawson Volume, 1, 307–313] on the basis of garnet geochemistry (G10 vs. G9) populations.

Deep-probing MT data from the lake bottom instruments infer that the conductor has a total depth-integrated conductivity (conductance) of the order of 2000 Siemens, which, given an internal resistivity of 10–15 Ω m, implies a thickness of 20–30 km. Below the CSMC the electrical resistivity of the lithosphere increases by a factor of 3–5 to values of around 50 Ω m. This change occurs at depths consistent with the graphite–diamond transition, which is taken as consistent with a carbon interpretation for the CSMC.

Preliminary three-dimensional MT modelling supports the NE–SW striking geometry for the conductor, and also suggests a NW dip. This geometry is taken as implying that the tectonic processes that emplaced this geophysical–geochemical body are likely related to the subduction of a craton of unknown provenance from the SE (present-day coordinates) during 2630–2620 Ma. It suggests that the lithospheric stacking model of Helmstaedt and Schulze [Helmstaedt, H.H., Schulze, D.J., 1989. Southern African kimberlites and their mantle sample: implications for Archean tectonics and lithosphere evolution. In Ross, J. (Ed.), Kimberlites and Related Rocks, Vol. 1: Their Composition, Occurrence, Origin, and Emplacement. Geological Society of Australia Special Publication, vol. 14, 358–368] is likely correct for the formation of the Slave's current SCLM.