压密注浆的能量分析方法   总被引：6，自引：2，他引：4  

邹金锋  李亮  杨小礼  王志斌  何长明 《岩土力学》2006,27(3):475-478

为了能够从能量的角度分析压密注浆的力学机理,并给出注浆压力的理论解,将整个注浆过程视为无限土体中的圆孔扩张问题,根据注浆过程中能耗区土体在注浆压力和静止土压力作用下的应力、应变和体变关系以及注浆扩孔过程中的能量和体变守恒原理,推导出压密注浆极限注浆压力的理论解答。计算和分析表明,理论解的计算结果与工程实际比较吻合,而且球形扩孔的注浆压力比柱形扩孔的注浆压力要小得多,初步证实了理论解的可靠性。  相似文献   

受压煤岩破裂过程电磁辐射与能量转化规律研究   总被引：5，自引：0，他引：5  

肖红飞  何学秋  王恩元 《岩土力学》2006,27(7):1097-1100

首先对煤岩单轴受压变形破裂过程产生的电磁辐射（EME）、声发射（AE）信号变化规律进行了试验研究,然后在试验测定结果的基础上分析研究了煤岩变形破裂电磁辐射与加载变形能量之间的转换关系。研究结果表明,EME值随着加载时间的增加而增强,声发射信号也呈现同样的规律;电磁辐射的幅值、脉冲数在煤岩主破裂前与应力基本成正相关的关系,出现峰值后降低,试验的各个样品均呈现此变化规律;电磁辐射能和机械能的转化曲线与煤岩单轴加载过程的应力-应变关系曲线是相对应的,且呈现三次多项式的关系。从能量转换的角度来研究煤岩变形破裂电磁辐射与应力之间的关系是可行的。  相似文献   

岩体动力失稳终止点、能量释放量解析解与图解   总被引：3，自引：0，他引：3  

潘岳  王志强  吴敏应 《岩土力学》2006,27(11):1915-1921

以精确和近似突变模型方式,按Ⅱ体的步调,给出了岩体系统动力失稳弹性能释放量的解析解和图解;将地震、岩爆前后阶段岩体系统稳定性的定性认识提高到定量描述;严格确定了岩体系统弹性能瞬间释放终止点位置,为计算地震效率、研究释放的地震能量级、地震应力降、震后断层错距和围岩弹性应变恢复量提供了科学依据。系统失稳时具备对外界做功的本领,地震波能便是失稳的岩体系统以破坏性方式对环境做功。给出的弹性能释放量图解中蕴涵了丰富的信息量,为确定岩体动力失稳问题的数学模型是折迭突变模型给出有力佐证。  相似文献   

一维稳态渗流时非饱和土中的基质吸力分布     

李顺群  赵少飞  王学志 《岩土力学》2006,27(Z1):90-94

首先对非饱和土中的土水势和干土吸水过程中土水势的变化进行了定性分析。然后利用水相连续性条件、广义Darcy定律及Gardner关于非饱和土导水系数和基质吸力的经验公式,建立了非饱和土一维稳态渗流情况下基质吸力沿深度变化的关系表达式,并利用差分方法对稳态入渗和稳态蒸发两种情况进行了求解。根据提出的方法,不仅可以方便地得到基质吸力沿深度的分布,而且可以求出水头和导水系数沿深度的变化。  相似文献   

我国西部地区矿产资源概况   总被引：5，自引：0，他引：5  

李文光 《化工矿产地质》2000,22(3):176-182

我国西部青海、新疆、贵州、宁夏、甘肃、陕西、云南、四川、西藏、内蒙古等省区矿产资源丰富 ,尤其是能源矿产、化工矿产分布相对集中。该区内鄂尔多斯能源富集带、陕甘川有色金属矿产富集区、柴达木化工矿产富集区、塔里木油气富集区及阿尔泰有色金属富集区等已成为吸引投资颇有前景的成矿区带。但目前西部矿产资源开发中还存在一些亟待解决的问题 ,有效地解决这些问题 ,将资源优势转化为经济优势 ,同时使资源开发与环境保护协调发展 ,是西部矿产开发的正确道路。  相似文献   

Computing Lippmann Diagrams from Direct Calculation of Mixing Properties of Solid Solutions: Application to the Barite-Celestite System     

M. Prieto  A. Fernández-González  U. Becker  A. Putnis 《Aquatic Geochemistry》2000,6(2):133-146

The Lippmann diagram for the system(Ba, Sr)SO₄-H₂O was computed at 25 °Cby determining the solid-phase activity coefficientsfrom first principles calculations. Directcalculations of the mixing properties of thebarite-celestite series indicate this solid solutionbehaves as non-ideal and non-regular. At 25 °C,the enthalpy of mixing shows a minimum around 50 mole% SrSO₄ due to an ordering tendency. Thefree energy of mixing shows two minima that delimit awide and symmetric miscibility gap (from 2.1 to 97.9 mole% SrSO₄) at this temperature. The excessfree energy of mixing requires a Guggenheim expansionseries of 5 terms to be described, where the termswith odd exponents are null as a consequence of thesymmetric distribution of the mixing properties withcomposition. The Lippmann diagram shows a peritecticpoint that corresponds to the composition of an aqueoussolution which is simultaneously at equilibrium withthe two extremes of the miscibility gap. The largedifference between the solubility products of theendmembers involves a strong preferential partitioningof the less soluble endmember towards the solid phase,which explains the extremely Ba-poor composition ofthe aqueous solution (aqueous activity fraction forBa²⁺ = 0.000446 ) at the peritectic point.  相似文献   

A Study On Atmospheric Boundary-Layer Characteristics At Anand, India Using Lsp Experimental Data Sets     

A. N. V. Satyanarayana  V. N. Lykossov  U. C. Mohanty 《Boundary-Layer Meteorology》2000,96(3):393-419

An attempt is made to study the planetary boundary layer (PBL) characteristics during the winter period at Anand (22.4°N, 72.6°E), a semi-arid region, which is located in the western part of India. A one-dimensional turbulent kinetic energy (TKE) closure model is used for the study. The structure of the PBL,which consists of profiles of zonal and meridional components of wind,potential temperature and specific humidity, is simulated. A one-dimensional soil heat and moisture transport parameterization scheme is incorporated for the accurate representation of the energy exchange processes at the soil-atmosphere interface. The diurnal variation of fluxes of sensible heat, latent heat, shortwave radiation, net radiation and soil flux, soil temperature at different depths, Richardson number and TKE at the height of the constant flux layer is studied. The model predictions are compared with the available observations obtained from a special Land Surface Processes (LSP) experiment.  相似文献   

Probability Density Function Integrals And Small-Scale Mixing In Turbulent Plumes     

R. J. Brown  B. L. Sawford 《Boundary-Layer Meteorology》2000,97(2):219-249

We analyse cross-wind-integrated statistics of theconcentration field of a conserved scalar for pointand line sources in grid turbulence. In particular,using wind-tunnel measurements we calculate thecross-wind integrated probability density function(pdf) for the scalar concentration. We then use thatquantity in the exact evolution equation for the pdfto calculate the cross-wind integrated mean of therate of dissipation of scalar variance, conditional onthe scalar concentration. Much of the variation ofthese statistics with distance downstream is accountedfor by scaling with concentration, length and timescales based on the development of the mean plume.This scaling thus suggests some simple practicalparameterisations of these statistics in terms ofmean-field quantities. One of the motivations for thiswork is to find a simple parameterisation for thescalar dissipation that can be used for modellingchemical reactions in plumes.We also consider the cross-wind integral of the firstfew moments of the concentration field and show thatthe integration greatly simplifies the budgets forthese moments. Thus the first moment is just thedownstream flux of the scalar, which is constant. Thesecond moment budget provides a check on the meandissipation estimated directly from the pdf evolutionequation.  相似文献   

1998年南海、孟加拉湾夏季风期间动能收支特征   总被引：1，自引：0，他引：1       下载免费PDF全文

梁建茵  吴尚森 《应用气象学报》2000,11(4):400-409

该文采用1998年加密观测资料经同化处理后得到的客观分析格点资料, 对南海地区和孟加拉湾地区的动能收支进行了诊断分析和对比, 得出: B区夏季风爆发, 其850 hPa区域平均总动能表现为爆发性增长, C区则表现为一个逐步增长的过程.越赤道气流通过南边界的动能输送对B区夏季风建立贡献很大, 西边界动能输入对C区夏季风建立也起了十分显著的作用.季风盛行期, B区夏季风动能的发展维持主要是动能水平通量散度的贡献, 其中西边界动能的流入贡献最大, 孟加拉湾夏季风的变化主要为印度季风影响所致; C区夏季风动能主要是依靠其区域内动能制造来维持.对于850 hPa层, B区主要通过斜压过程制造动能, 正压过程破坏更多的动能, C区主要是正压过程制造动能.两区对流层高层都为动能主要流出区, 而对流层低层, B区为动能流入区, C区为动能流出区.  相似文献   

基础隔震结构的能量设计方法   总被引：11，自引：2，他引：9  

周云  徐彤  贺明玄 《地震工程与工程振动》2000,20(3):116-122

本文以能量分析方法为基础,解释了基础隔震结构体系的能量设计原理和设计准则。根据作者建立的标准能量设计反应谱曲线,结合我国现行的抗震设计规范,建立了基础隔震结构体系的能量设计方法,通过能量平衡关系对隔层的变形反应进行预测．最后通过算例说明能量设计方法具有一定的可靠性,为该类体系的进一步推广奠定了基础。  相似文献