不同荷载模式作用下双层软黏土地基压缩特性研究

天津滨海吹填场区典型的“上软下硬”的双层软黏土地基具有复杂的物理性质和工程特性,其在不同荷载作用模式下的变形特性有所不同,在工程实践中往往会产生较大的工后沉降和不均匀沉降,从而导致修建于其上的建筑物出现诸多工程问题。现阶段对于不同荷载作用下吹填场区形成的“上软下硬”双层软黏土地基的变形特性及机理研究甚少,导致理论研究远远落后于工程实践,制约了吹填场区经济建设的快速发展,因此对此类地基的变形特性展开研究显得尤为重要。基于此,本文针对吹填场区“上软下硬”的双层软黏土地基,开展了反复荷载和恒定荷载作用下的一维固结试验和扫描电镜试验(SEM),得到了不同荷载模式作用下的压缩特性及其微观机理,为吹填场区双层软黏土地基变形模型建立及长期工后沉降预测提供理论依据。研究表明:双层软黏土地基的压缩系数和固结系数在反复荷载作用初期明显减小,而后缓慢减小直至趋于稳定; 与反复荷载相比,恒定荷载作用下试样的压缩系数初期值增加,固结系数初期值减小,其变化量均在40% ~50%的范围内; 当荷载等级一定时,反复荷载作用引起双层软黏土地基产生的沉降量相比于恒定荷载作用多30% ~45%; 随着荷载等级的增加,土样内部大孔隙受到挤压而减少,孔隙的圆度和定向性加强,土体结构更密实,均一化程度提高; 相比于恒定荷载模式,反复荷载作用下土样内部孔隙形状更接近于圆形,孔隙定向性更好,土体内部结构强化程度大,但有序性相对较差。     

基于偏正态概率分布的粒度分布次总体分离及其沉积环境指示意义

沉积物颗粒是某种沉积环境和水动力条件下多个沉积过程的最终产物。粒度分布是原始沉积信息的载体,是来自不同沉积过程的多个次总体的叠加,频率曲线可能表现为双峰或者多峰特征。传统的沉积学粒度分析方法并未深入研究次总体;常见的概率分布模型在分离次总体后无法全面计算统计参数。本文以214份鄱阳湖现代沉积物的粒度分布数据为例,利用偏正态概率分布模型共分离提取977个次总体,计算各个次总体的统计参数,并对比分析了不同沉积环境中次总体参数的异同。结果表明：① 次总体均值、方差、偏度、峰度、所占百分比和最大频率等参数规律明显;② 从曲流河河道到河流末端、在河流末端顺流方向上和河道左右两侧远离河道方向上,粒度分布中主要次总体粒度均值逐渐减小,河道间洼地和湖区沉积物粒度分布的各个次总体占比接近;③ 江心洲的河道砂和河漫滩细粒粒度分布分别由3种和5种不同类型次总体组成。该方法可为沉积环境的定量判断和沉积过程的定量研究提供参考。     

PDC钻头切削齿布齿设计的新思路

切削齿布齿设计是PDC钻头设计的关键。为提高PDC钻头的钻进效率,综合考虑PDC钻头切削齿的设计特点和切削先后顺序等因素,并且通过对PDC钻头单切削齿实验结果进行分析,提出了以冠部轮廓法线为基准的切削齿布齿设计方法。     

卧龙湖煤矿岩浆蚀变煤层中汞的分布与赋存特征

系统采集淮北卧龙湖煤矿岩浆蚀变煤层中岩浆岩、煤及顶底板岩石样品,测试分析了样品中汞、灰分、挥发分、水 分以及各形态硫的含量,探讨了岩浆蚀变煤层中汞的分布与赋存特征。结果表明：（1） 岩浆侵入导致煤中灰分升高,挥发 分降低,煤中硫主要以黄铁矿硫和有机硫存在;（2） 岩浆侵入导致煤中汞的富集,卧龙湖煤矿岩浆蚀变煤层中汞的平均含 量高达0.23×10-6,是华北石炭-二叠纪煤、中国煤以及美国煤中汞的平均含量的1.4 倍,1.2 倍和1.3 倍;（3） 煤中汞的含量 随离岩浆侵入体距离增大有逐渐降低的趋势,但在煤岩接触带附近,汞在岩浆侵入体上方和下方的煤中呈现不同的分布特 征;（4） 煤中的汞主要以无机结合态的形式存在,且大部分赋存在煤中的黄铁矿中,同时亦存在与有机硫结合的汞。岩浆 热液对煤层的侵入,导致煤质以及煤中汞的含量和赋存方式发生了显著变化。     

2011日本东北大地震前震余震重力效应分析

针对2011年日本东北大地震(Tohoku-Oki地震)发生前后较短时间内的多次较大前震和余震和主震混在一起,不利于提取出主震同震信号的问题,该文利用弹性位错理论模拟计算了Tohoku-Oki地震一次较大前震和两次较大余震的同震重力变化,讨论了这3次地震单独和综合的重力效应,并与主震重力变化对比分析,认为这3次前震和余震引起的重力变化数值较大,影响范围广,会直接影响到Tohoku-Oki地震主震的同震重力信号提取,所以需要作为重要误差考虑。     

基于MapGIS数字高程模型基岩面高程等值线图的制作

基岩面高程等值线图是建立三维地质模型所需的一项重要数据,也是三维地质调查工作的一项重要任务。制作基岩面高程等值线的主要数据源为钻孔和地形等高线。在制作过程中,首先对钻孔数据进行筛选和标准化处理,筛选出347个钻孔投影成Map GIS的点文件(.WT),为提高精度,使成图更符合实际情况,结合武汉市地形特征,提取地表基岩露头出露部分等高线(.WL)代表露头区基岩面高程。再利用Map GIS DTM分析数字高程模型对钻孔和等高线对应的点文件和线文件(.WT和.WL)剖分插值网格化,生成平面和立体的基岩面等值线图。通过对Map GIS提供的4种剖分插值结果进行对比分析,应用Kring泛克里格网格化模型绘制的基岩面高程等值线图更符合实际情况,同时也更快速、方便。需要注意的是,在使用Kring泛克里格网格化方法时,应对数据进行正态分布检验。     

Determination of allowable subgrade frost heave with the pavement roughness index in numerical analysis

Frost heave is an upward swelling of soil during cryogenic conditions in cold regions. It is caused by the accumulation of ice crystals in subgrade soil, which grow upwards when freezing temperatures penetrate into the subgrade. This study establishes the allowable soil subgrade frost heave based on the roughness standard of asphalt pavement in China, and aims to balance the pavement design and frost heave resistance of subgrades in cold regions. We formulated a mechanical model of pavement supported by the boundary conditions of differential frost heave, based on the elastic layered system theory. The differential soil subgrade frost heave was modeled as a sinusoidal function, and the allowable frost heave and the roughness index were modeled as the displacement boundaries for the top and bottom of the pavement structure. Then the allowable frost heave was back-calculated according to the roughness standard. Numerical results show that the allowable frost heave depends on the pavement structure, material properties, the highway grade, and other factors. In order to ensure that the actual soil subgrade frost heave is lower than the allowable frost heave, pavement structures and materials need to be selected and designed carefully. The numerical method proposed here can be applied to establish the frost heave resistance of subgrade when the pavement structure and materials are determined.     

Resonance of baroclinic waves in the tropical oceans: The Indian Ocean and the far western Pacific

The Indian Ocean has a particularity, its width is close to half the wavelength of a Rossby wave of biannual frequency, this coincidence having been capitalized on by several authors to give the observations a physical basis. The purpose of this article is to show that this is not the case since the resonance of tropical baroclinic waves occurs in all three oceans. This is because the westward-propagating Rossby wave is retroflexed at the western boundary to form off-equatorial Rossby waves dragged by countercurrents before receding and turning back as a Kelvin wave. Thus a quasi-stationary baroclinic wave is formed, whose mean period is tuned to the forcing period. Two independent basin modes resonantly forced are highlighted – 1) a nearly symmetric zonal 1/2-yr period Quasi-Stationary Wave (QSW) that is resonantly forced by the biannual monsoon. It is formed from first baroclinic mode equatorial-trapped Rossby and Kelvin waves and off-equatorial Rossby waves at the western antinode. This QSW controls the Equatorial Counter Current at the node. The Indian Ocean Dipole (IOD) results from a subharmonic mode locking resulting from the coupling of this QSW and the 2nd, 3rd and 4th baroclinic modes - 2) a 1-yr period QSW formed from an off-equatorial baroclinic Rossby wave, which is induced from the southernmost current of the Indonesian Throughflow through the Timor passage, propagating in the southern and northern hemispheres: the drivers are south-easterlies in the southern hemisphere and monsoon wind in the northern hemisphere.