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淄博市张店南部地热异常成因

通过研究井温曲线类型,确定研究区纯传导地温梯度为2.5℃/100m;结合各单井地温梯度,圈定了地热异常区域;揭示了该区地热异常具有下段以对流为主、上段以传导为主的特点.通过热水水化学和同位素数据的综合分析表明,该区地下热水补给来源为大气降水,热水赋存于断裂裂隙系统中,且沿断裂裂隙垂向运动十分强烈.     

山东省地温梯度分布特征研究

在充分搜集山东省区域地质、构造地质、地热地质及地热遥感解译资料等基础上,开展了山东省地温场现状调查、1∶50万地热遥感解译和测温工作,根据收集资料程度,提出计算地温梯度的方法,计算了整个研究区地温梯度;评价了各个地热区地温梯度的分布规律,并从大地构造、基岩起伏、岩浆活动、地层岩性、断裂构造、地下水活动等方面分析了影响地温场分布的因素,讨论了浅部地温场与深部构造的关系,总结了研究区各区地温梯度的分布特征。     

扩展SSH Hubbard模型的晶格振动矩阵

在计及最近邻电子相互作用的扩展ＳＳＨＨｕｂｂａｒｄ模型时，得到了晶格振动矩阵，它对电子的正负自旋态对称和非对称的各类非线性元激发情形均适用。     

亚洲中东部岩石圈下层网络状塑性流动与应变场

在板块边缘驱动力的挤压作用下,岩石圈下层（含下地壳和岩石圈地幔）塑性流动网络的共轭角随着变形的增大而由初始的直角变为钝角,因此,可根据共轭角的增量推测应变的大小,并给出该层的应变场,亚洲中东部所含3个塑性流动网络系统的研究表明,岩石圈下层的应变场控制或影响着上部地壳的构造变形和地形起伏,表现在应变“凸锋~”与地形凸峰之间的相互对应以及“稳定”块体的低应变效应和应变的波动传播,网络共轭角推测应变的方法为认识板内应变场和构造变形提供了新的途径。     

内蒙古固阳县席麻塔一带共轭剪切带的地质特征及形成机制

通过区调填图在内蒙古固阳县北山新太古代石英闪长岩和中元古代英云闪长岩中发现了韧性剪切带.通过野外调查、应变测量及显微构造、电子探针等方法研究表明, 该韧性剪切带为两组呈共轭组合型式产出, 形成机制与西伯利亚板块和华北板块相互挤压作用有关, 为在地球较深层次、在压扁环境下的简单剪切, 形成时代为中元古代末期, 变质相为绿片岩相.      

剪切带倾角尺度律与局部化启动跳跃稳定研究

研究了剪切带倾角是如何依赖于岩样高度以及剪切带的不稳定性。建立了准脆性材料试件剪切带倾角尺度效应模型,得到了剪切带倾角尺度效应的解析解,且与实验结果比较相符。研究结果表明:剪切带倾角随着试件高度的增加而增加,但其增加幅逐渐减缓,最终趋于稳定值。笔者还对剪应变局部化启动、跳跃和稳定进行了理论分析,解释了实验所观测到的剪切带跳跃现象和砂岩岩样应变局部化较煤样滞后的原因。剪应变局部化是否发生跳跃,关键取决于全程应力-应变曲线软化段是否存在拐点。对于没有拐点的情形,宏观剪切带图案不跳跃。局部化是导致准脆性材料试件剪切带倾角尺度效应的原因。     

Experimental investigation of the harmonic generation by waves over a submerged plate

Experiments in a wave flume have been performed to analyse the nonlinear interaction between regular gravity waves and a submerged horizontal plate used as breakwater. A new method, based on the Doppler shift generated by a moving probes, has been used to discriminate the incident fundamental mode and the reflected fundamental mode. The relationships of the reflection and transmission coefficients to the wave number at different submergence depth ratios are presented. The accurate discrimination, by this method, of the phase-locked and free modes allows the quantification of the higher harmonics generated by the breakwater and the analysis of the nonlinear interaction between the waves and the submerged plate. The transfer of energy from the fundamental mode to higher harmonics is very large in the cases of small submergence depth ratios. The vortices produced at the edges take part in the production of higher harmonics by interaction with the free surface but involve, at the same time, a dissipation process that increases the efficiency of the breakwater.     

Splash-saltation trajectories of soil particles under wind-driven rain

It is usually recognized that relatively large amounts of soil particles cannot be transported by raindrop splashes under windless rain. However, the splash-saltation process can cause net transportation in the prevailing wind direction since variations in splash-saltation trajectory due to the wind are expected in wind-driven rain. Therefore, determining the combined effect of rain and wind on the process should enable improvement of the estimation of erosion for any given prediction technique. This paper presents experimental data on the effects of slope aspect, slope gradient, and horizontal wind velocity on the splash-saltation trajectories of soil particles under wind-driven rain. In a wind tunnel facility equipped with a rainfall simulator, the rains driven by horizontal wind velocities of 6, 10, and 14 m s⁻¹ were allowed to impact three agricultural soils packed into 20×55 cm soil pans placed at both windward and leeward slopes of 7%, 15%, and 20%. Splash-saltation trajectories were measured by trapping the splashed particles at distances downwind on a 7-m uniform slope segment in the upslope and downslope directions, respectively, for windward and leeward slopes. Exponential decay curves were fitted for the mass distribution of splash-saltation sediment as a function of travel distance, and the average splash-saltation trajectory was derived from the average value of the fitted functions. The results demonstrated that the average trajectory of a raindrop-induced and wind-driven soil particle was substantially affected by the wind shear velocity, and it had the greatest correlation (r=0.96 for all data) with the shear velocity; however, neither slope aspect nor slope gradient significantly predicted the splash-saltation trajectory. More significantly, a statistical analysis conducted with nonlinear regression model of C₁(u_*²/g) showed that average trajectory of splash saltation was approximately three times greater than that of typical saltating sand grain.