胜利油气区东营凹陷现今地温场研究

文中利用热导率分散模型,根据地层中砂质含量数据计算东营凹陷第三系各沉积地层单元的原地热导率,再利用热阻率法根据东营凹陷１７０口测温井中测温资料计算出第三系各地层界面上和特征深度处温度,进而研究东营凹陷现今地下温度。计算结果表明,第三系各地介面上地温分布特征主要受各界面埋藏深度控制,而地下各特征深度上地温分布特征主要受热流平面分布特征控制。     

Estimation of surface heat flux and inversion height with a Doppler acoustic sounder

In this paper, acoustic sounder (sodar) derived vertical velocity variance (σ _w ² ) and inversion height (Z _i) are used to compute the surface heat flux during the convective activity in the morning hours. The surface heat flux computed by these methods is found to be of the same order of magnitude as that obtained from tower measurements. Inversion heights derived from sodar reflectivity profiles averaged for an hour are compared with those obtained from the σ _w ² /Z profile. Variation of σ _w ² in the mixed layer is discussed. The data were collected during the Monsoon Trough Boundary Layer Experiment 1990 at Kharagpur. The analysis is made for four days which represent the pre-monsoon, onset, active and relatively weak phases of the summer monsoon 1990. The interaction of the ABL with the monsoon activity is studied in terms of the variation of inversion height, vertical velocity variance and surface heat flux as monsoon progresses from June to August.     

水源热泵系统中地下水流贯通及其对温度场的影响

利用含水层储能的一般特点,提出流贯通;分析流贯通和热贯通的相互作用、相互影响及对工程实际的意义;并基于地下水水热运移的基本原理,建立地下水流动和热量输运的耦合数值模型。在此基础上对沈阳某场地水源热泵工程的运行进行流场及温度场的数值模拟分析,给出产生流贯通的依据,即利用水力坡度定量的判断流贯通发生与否;当水力坡度变化非常小、可忽略不计时,认为含水层出现流贯通;进而研究抽、灌量对流贯通的影响,发现抽、灌量越大,则出现流贯通时间越短;而大量的抽、灌量更容易发生流贯通,进而会引起热贯通的发生。在实际工程中可降低抽、灌水量,在条件许可的情况下可提高抽、灌井的间距,并可在抽、灌井运行一个周期后调整抽灌井位置,以减少热贯通的发生。     

青藏高原路堤边坡遮阳措施辐射影响分析

作为主动保护冻土的典型措施之一的路堤边坡遮阳板护坡措施,对于减少太阳直接辐射到达地表和降低路堤内部温度起到至关重要的作用,阻隔太阳的辐射,减少进入路堤净辐射量和进入地表的热流,降低路堤土体温度．现场试验结果表明：进入天然路堤边坡表面平均净辐射量为300～350W·m^-2,而遮阳板下路堤边坡表面的平均净辐射量为30～4...     

The thermal structure and thickness of continental roots

We compare heat flow data from the Precambrian shields in North America and in South Africa. We also review data available in other less well-sampled Shield regions. Variations in crustal heat production account for most of the variability of the heat flow. Because of this variability, it is difficult to define a single average crustal model representative of a whole tectonic province. The average heat flow values of different Archean provinces in Canada, South Africa, Australia and India differ by significant amounts. This is also true for Proterozoic provinces. For example, the heat flow is significantly higher in the Proterozoic Namaqua–Natal Belt of South Africa than in the Grenville Province of the Canadian Shield (61 vs. 41 mW m⁻² on average). These observations indicate that it is not possible to define single value of the average heat flow for all provinces of the same crustal age. Large amplitude short wavelength variations of the heat flow suggest that most of the difference between Proterozoic and Archean heat flow is of crustal origin. In eastern Canada, there is no good correlation between the local values of heat flow and heat production. In the Archean, Proterozoic and Paleozoic provinces of eastern Canada, heat flow values through rocks with the same heat production are not significantly different. There is therefore no evidence for variations of the mantle heat flow beneath these different provinces. After removing the local crustal heat production from the surface heat flow, the mantle (Moho) heat flow was estimated to be between 10–15 mW m⁻² in the Archean, Proterozoic and Paleozoic provinces of eastern Canada. Estimates of the mantle heat flow in the Kaapvaal craton of South Africa may be slightly higher (≈17 mW m⁻²). Large-scale variations of bulk crustal heat production are well-documented in Canada and imply significant differences of deep lithospheric thermal structure. In thick lithosphere, surficial heat flow measurements record a time average of heat production in the lithospheric mantle and are not in equilibrium with the instantaneous heat production. The low mantle heat flow and current estimates of heat production in the lithospheric mantle do not support a mechanical (conductive) lithosphere thinner than 200 km and thicker than 330 km. Temperature anomalies with surrounding oceanic mantle extend to the convective boundary layer below the conductive layer, and hence to depths greater than these estimates. Mechanical and thermal stability of the lithosphere require the mantle part of the lithosphere to be chemically buoyant and depleted in radiogenic elements. Both characteristics are achieved simultaneously by partial melting and melt extraction.     

大孔径闪烁仪和涡动相关仪观测显热通量之间的尺度关系

利用北京昌平小汤山2002年、2004年涡动相关仪和大孔径闪烁仪的观测数据,借助解析足迹模型计算的源区,分析均匀、非均匀下垫面上涡动相关仪和大孔径闪烁仪观测显热通量之间的差异和关系.结果表明:地表的均匀与非均匀性质,直接影响涡动相关仪和大孔径闪烁仪观测的显热通量的差异大小.在分析均匀、非均匀地表上2种仪器源区重叠面积及重叠区域内足迹值大小与观测通量值之间的关系后,构建一个非均匀地表上2台涡动相关仪与1台闪烁仪观测通量之间的尺度关系式.     

浅议水源热泵系统中的地下水回灌

通过对水源热泵使用现状的调查,分析水源热泵的应用范围,同时对水源热泵系统中地下水回灌进行剖析,比较不同类型回灌的效果及所产生的影响,指出最优化的回灌思路,并针对其实际应用过程提出严格成井工艺,制定国内相关技术标准,加强对现有的项目的跟监控等几项推广建议。     

岩石热导率校正对大地热流计算值的影响——以渤海湾盆地冀中坳陷为例

岩石热导率是计算大地热流的基础热物性参数,热导率的选取和校正是正确评估热流的基础。当前在冀中坳陷乃至渤海湾盆地的大地热流计算中,多以受季节性气温变化和地下水活动等因素影响较小的古近系和新近系砂泥质岩层作为大地热流的计算层位,岩石热导率也多参考区域内已有定值,而忽略了热导率对水饱和度、温度和压力的依赖性。笔者等从岩石热导率的温压校正和饱水校正角度出发,计算并比较了不同校正方法对热流值的影响。主要认识如下：(1)岩石热导率作为1个受多因素综合影响的热物性参数,其大小与岩性和矿物组分密切相关,同时通常与孔隙率呈负相关,而与密度呈正相关;(2)热导率高温实验结果显示,冀中坳陷砂岩样品热导率总体上随温度的升高而降低,在30～130℃的温度区间热导率降低了6.8%～11.3%,热导率下降率具有随热导率的降低而减小的趋势;由于砂岩和泥岩具有相对较浅的埋深和较低的原位温压条件,温压对热导率的正负效应可以在一定程度上相互抵消,对于热导率小于2 W/(m·K)的样品,温压对其的影响较小。(3)饱水校正后的冀中坳陷JZ03井和JZ04井古近系—新近系砂泥岩热导率的平均偏差分别高达43.0%、47.5%;(4...     

稀疏非正交填充裂隙岩体水流—传热—应力模型与离散元模拟

为研究填充裂隙水流速度对岩体温度和应力的影响,选取甘肃北山地区的花岗岩,制作了稀疏非正交裂隙岩体模 型,采用河砂填充裂隙后进行模型试验;并对模型试验进行离散元数值模拟,分析了模型试验所测岩体温度和热应力与数 值模拟结果的差异和原因。结果显示：填砂裂隙强化了裂隙介质的热导能力,无填充时岩体温度和热应力比填砂时低;模 型试验和离散元模拟均表明,岩体温度和岩体应力随裂隙水流速度增大而减小,但是系统达到稳态所需要的时间变短;模 型试验中斜裂隙水流对温度场起主要作用;由于现有3DEC软件不能考虑水的热物性参数随温度的变化,进而产生自然对 流换热,斜裂隙水流和靠近热源侧的竖裂隙水流对温度场起主要作用。     

剑川—德钦一带的地热异常:对川滇菱块西北边界和地震活动性的意义

为研究川滇菱块西北缘剑川-德钦一带地热场空间分布特征,探索地热异常区与断裂及地震活动性的关系以及活动块体边界问题,运用4种传统地热温标和多矿物平衡法综合估算了川滇菱块滇西北地区(德钦-维西-剑川-丽江-中甸) 91个地热温泉的最有可能的热储温度,通过克里金插值方法获得了滇西北地区的热储温度空间分布。结果表明,地热异常区主要沿德钦-中甸-大具断裂及其以北的多条近南北向金沙江断裂的分支断层展布,澜沧江断裂带、维西-马登断裂、玉龙雪山东麓断裂和中甸-龙蟠-乔后断裂局部分段表现地热异常;地热异常区的地理展布大致反映了德钦-中甸-大具断裂与金沙江断裂带共同构成了川滇菱形块体的西北边界;绝大多数中强地震震中位于地热中-高值区即地热的横向梯度带上,德钦-中甸-稻城一带地热横向梯度变化较大且历史上强震稀少,未来的地震危险性值得关注。