郯庐断裂带是热异常带吗:来自断裂带南段热流的约束

郯庐断裂带是东亚最重要的断裂之一,在构造地质、岩石矿物、地震分布等领域得到了广泛的关注,然而少有针对郯庐断裂带地热学的研究.本文作者对郯庐断裂带南段7口钻井进行了系统测温,采用光学扫描法测试了6口钻井的142块岩心和13块露头样品的热导率,获得了6个高质量的热流数据.结合已发表的热流和地震剖面资料,我们获得了郯庐断裂带南段的岩石圈结构.研究表明,郯庐断裂带南段现今地温梯度从南到北有增大的趋势,介于21.8~30.3℃·km^-1.大地热流值介于44.0~81.7 mW·m^-2,平均61.4±10.8 mW·m^-2,表现为正常大地热流的特征,并非热异常带.最大热流值出现在庐枞盆地的大陆科学钻探井ZK03处,上地壳浅部极高的生热层很可能是高热流的主要因素.沿郯庐断裂南段地震带浅源地震发震带的底界和350℃等温面耦合较好,指示了深部结构的差异.     

基于地震各向异性分析郯庐断裂带中段深部构造特征

利用郯庐断裂带中段附近10个宽频带台站的远震波形资料,基于上地幔地震各向异性来分析郯庐断裂带中段深部构造特征。本研究得到,郯庐断裂带中段深部平均快波偏振方向为93．8°,即郯庐断裂带中段深部主张应变（张应力）方向,对照GPS资料和地震资料的研究表明,郯庐断裂带中段地壳和深部上地幔的形变存在总体的一致性,即郯庐断裂带中段岩石层的形变具有统一特征,地壳与深部上地幔处于相似的应力应变状态中。     

郯庐断裂带地震活动特征

本文较为详细地研究了郯庐断裂带及附近地区的地震活动，其主要结果为：１、郯庐断裂带地震活动由四个地震活动区段组成，该带活动的主体区段是那城─—渤海─—海城．２、郯庐断裂带地震活动的周期性是形成邦城─—海城区段中强地震活动的主要原因．３、郯庐断裂带中北段（邦城─—海城）Ｍ≥６．０级地震具有较好的迁移规律．４、郯庐断裂带近代小震活动表现出南段随机性，中段呈线性，北段具有密集区带性等特点。５、郯庐断裂带震源深度表现出南、北段浅，中段深，且散度大的特点。６、郯庐断裂带Ｑ值分布表明，沂沭带介质强度的完整性较差。     

渤海及邻区地震地质、地球物理场和地震活动特征

对渤海及周转地区地质构造,地球物理场特征及地震活动特征进行了分析和研究。结果表明：该区域发育有ＮＮＥ、ＮＷ和ＮＷＷ向３组断裂,在渤海海域ＮＮＥ向的郯庐断裂被ＮＷＷ向断裂分割为３段,中段地震活动最强,发生过３次７级以上地震和３次６级以上地震,在空间上,地震活动可以划分为２个带,即郯庐地震带和燕山－渤海地震带。渤海中部地区热流值偏高,莫霍界面和康腊界面隆起,上地幔高层层埋深浅,为３０～５０ｍ。     

下扬子区地温场和大地热流密度分布

根据下扬子区５０余口井温测量资料，从中选取能代表地层温度的井温数据计算地温梯度，在实验室中测量中、新生界的１１０余块砂岩和泥岩热导率及古生界碳酸岩和砂岩１００余块露头样品的热导率．在此基础上，确定了４１口井的大地热流密度值．地温梯度和大地热流密度分布表明，下扬子大部分地区中生代构造热事件伴随的热异常已不明显，而新生代时期岩石层拉张地区─－苏北盆地和郯庐断裂带是高热流密度和高地温梯度区．     

华北地热场研究

本文阐述了地热场在冀中—下辽河拗陷和临清拗陷及东邻地区呈现为高值,汾谓断陷带也较高,在渤中拗陷和郯庐断裂带更高;在燕山—太行山隆起区却呈现为低值,周口拗陷和鲁西隆起区也较低;燕山山前地带介于二者之间;华北大地热流划分8个区域取平均值为1.55HFU。提出华北四个区域的地壳、上地幔热结构,分区计算沉积岩层、花岗岩质层和玄武岩质层底部的温度和热流值;并用四个地区的平均热流值推导出该区的岩石圈厚度和底部温度。分析了地热场与地质及其它地球物理场的关系;重点探讨了地球内热与地震孕育和发生的内在联系。     

郯庐断裂带中段全新世活断层的特征滑动行为与特征地震

郯庐断裂带中段全新世活断层由３个独立的破裂段组成。从各破裂段的运动性质、位移分布看，断层的运动属特征地震型滑动。地震活动以强震活动为主，强震具有周期性原地重复发生的特点，且其强度基本相同；中强地震缺失或很少发生；ｂ值在高震级范围内具低ｂ值的非线性关系。这些特点正是特征地震的典型表现．根据郯庐断裂带中段活断层全新世以来的活动特点看，未来该区仍然以特征地震方式活动．按郯庐带的强震复发间隔和各段的最新一次活动时代推算，未来一段时期内新沂－宿迁段复发大震的可能性较大，安丘段次之，莒县－郯城段复发大震的可能性则很小。     

郯庐断裂带中段(沂沭断裂带)电性结构研究与孕震环境

穿过郯庐断裂带中段（沂沭断裂带,36°N）所做的大地电磁测深（MT）剖面长约150km.使用Robust技术和远参考道大地电磁方法处理观测数据.通过分析视电阻率、阻抗相位、Swift二维偏离度和区域走向,定性确定测区的电性结构.二维反演解释中选择非线性共轭梯度（NLCG）方法,使用TE、TM两种模式资料联合反演,沿剖面的二维电性结构显示：自西向东,鲁西隆起、郯庐断裂带、胶莱坳陷及鲁东隆起4个电性区块分别对应,鲁东和鲁西隆起区为高阻,郯庐断裂带电性结构复杂,高、低阻相间,胶莱坳陷为低阻（高导）区.沿MT剖面附近曾发生3个地震,其震源区处在电性变化剧烈部位,并在震源区附近存在高导体.     

郯庐断裂带中段中上地壳介质非均匀性

利用山东省和江苏省数字地震台网24个台站的269个小震记录, 采用散射S波包络展宽法对郯庐断裂带中段中上地壳小尺度介质非均匀性进行了研究. 结果表明: 郯庐断裂带中段中上地壳介质呈现强烈的横向非均匀性, 该断裂带为不同强度、 不同尺度介质非均匀体分布的边界; 强弱介质非均匀性边界往往与深部构造发育具有较强的相关性; 中强震孕育与强弱非均匀体的分布有关, 地震多发生在强弱非均匀体的过渡带上. 郯庐断裂带中上地壳介质非均匀分布特征可能与苏鲁超高压变质带、 深部构造及岩浆活动有关.      

郯庐断裂带合肥—宿迁段及邻区大地电磁三维成像

本文利用覆盖郯庐断裂带合肥-宿迁段及邻区的大地电磁阵列数据,应用大地电磁三维反演技术和印模重构方法,获得了测区可靠的三维电阻率模型.该电性模型中,郯庐断裂带东西两侧在浅部均有高阻分布,在深部电性结构显著不同,具有西低东高的特征,而郯庐断裂带则是两侧高低阻明显分界带;在南北方向,电性结构也存在较大不均匀性,嘉山地区呈现低...     

The Geothermal Study of the Mid-Segment of the Tancheng-Lujiang Fault Zone and Its Neighboring Region

In this paper,25 new terrestrial heat flow values newly observed along the mid-segment of the Tancheng-Lujiang fault zone are listed.With these geothermal data and 37 other terrestrial heat flow values(previously published),we describe the distribution features of terrestrial heat flows in the area.In this research,the two-dimensional temperature structure from the surface to lithospheric bottom of the Huaibei-Sixian-Jinhu profile is inferred by using the finite-element method and the temperature and heat flow of sedimentary,granitic,and basaltic layers is calculated.     

从卫星红外亮温与大地热流的关系看地震前的热红外异常

一些强地震前地表可产生热异常是人们比较一致的认识,但能否用卫星遥感技术观测到地下热异常则存在很大的分歧.本文试图通过分析热红外亮温与大地热流值的关系,探讨利用卫星遥感技术观测地震热异常的可能性及其存在的一些问题.研究结果表明:（1）在绝大多数情况下,亮温随大地热流值的升高而升高,升高的速率平均为0.057℃/mW·m^-2.如果地震引起的大地热流异常为100 mW·m^-2,则有可能产生卫星红外平均亮温约5.7℃的异常.（2）不同地区亮温随大地热流值变化速率不同,即使地震前出现了卫星热红外亮温异常,但不同地区表现也是不同的.（3）在一些地区一些季节,亮温与大地热流值关系不明显,可能是亮温数据受气象因素干扰所致.这说明地震前的热红外亮温异常是复杂的,甚至有时是难于观测到的.     

两淮煤田大地热流分布及其构造控制

基于127块煤系地层岩石样品的热导率测定结果,并结合59个井田内可靠的系统测温数据,计算得出两淮煤田的大地热流值,并编制大地热流分布图,其结果表明:两淮煤田大地热流值变化范围为29.7~83.9mW·m-2,平均值为58.3mW·m-2,和其他沉积盆地存在一定的差异,且淮南煤田大地热流值(63.7mW·m-2)远大于淮北煤田(55.2mW·m-2).综合分析得出,两淮煤田大地热流与其他盆地的差异以及淮南煤田热流值高于淮北煤田的现象为构造演化和区域地质背景的控制结果;而研究区内热流的分布不均主要是由于受地质构造对地温场的影响所致,推覆构造上下盘现今热流值的差异尤为突出.     

塔里木盆地现今地热特征

地温梯度和大地热流是揭示盆地现今热状态的重要参数,它们对理解盆地的构造-热演化过程及油气资源评价等方面均具有重要意义.利用塔里木盆地约470口井的地层测试温度资料和941块岩石热导率数据,本文计算了塔里木盆地38个新的大地热流数据,进而揭示了该盆地现今地热分布特征.研究表明,塔里木盆地现今地温梯度变化范围为17～32 ℃/km,平均为22.6±3.0 ℃/km;大地热流变化范围为26.2～65.4 mW/m²,平均为43.0±8.5 mW/m².与我国其他大中型沉积盆地相比,它表现为低地温、低大地热流的冷盆的热状态,但仍具有与世界上典型克拉通盆地相似的地热背景.整体而言,盆地隆起区地温梯度和热流相对较高,坳陷区地温梯度和热流则偏低.此外,我们还发现塔里木盆地现有的油气田区一般位于高地温梯度区域,这可能与下部热流体的向上运移和聚集有关.影响塔里木盆地现今地热特征的因素包括盆地深部结构、构造演化、岩石热物理性质、盆地基底构造形态和烃类聚集等.     

查干凹陷大地热流

查干凹陷是银根-额济纳旗盆地最具勘探潜力的凹陷, 但是查干凹陷及整个银根-额济纳旗盆地的大地热流研究仍为空白, 严重制约该盆地的油气资源的评价. 本文通过测试19口井107块岩芯的岩石热导率和岩石热导率原位校正, 利用协和平均公式计算得到查干凹陷各地层的岩石热导率大小; 并利用9口井的温度数据, 结合岩石热导率数据对查干凹陷的地温梯度和大地热流进行了计算. 研究结果表明查干凹陷具有构造稳定区和构造活动区之间的中温型地温场特征, 其平均地温梯度和大地热流分别为33.6℃/km, 74.5 mW/m². 本文的研究成果为查干凹陷及银根-额济纳旗盆地油气资源评价提供地热参数.     

Simulations of the 2004 lava flow at Etna volcano using the magflow cellular automata model

Since the mechanical properties of lava change over time, lava flows represent a challenge for physically based modeling. This change is ruled by a temperature field which needs to be modeled. MAGFLOW Cellular Automata (CA) model was developed for physically based simulations of lava flows in near real-time. We introduced an algorithm based on the Monte Carlo approach to solve the anisotropic problem. As transition rule of CA, a steady-state solution of Navier-Stokes equations was adopted in the case of isothermal laminar pressure-driven Bingham fluid. For the cooling mechanism, we consider only the radiative heat loss from the surface of the flow and the change of the temperature due to mixture of lavas between cells with different temperatures. The model was applied to reproduce a real lava flow that occurred during the 2004–2005 Etna eruption. The simulations were computed using three different empirical relationships between viscosity and temperature.     

Combined Effect of Climatic Variations and Groundwater Movement on Observed Heat Flow

In most practical situations, the upper part of a geological section consists of loose sediments, in which heat transfer cannot be described as a purely conductive process. To investigate such situations a one-dimensional numerical model of terrestrial temperature field formation under the combined influence of vertical groundwater filtration and ground surface temperature changes has been developed. The model allows one to consider the perturbation of heat flow interval values resulting from short- and long-period temperature waves propagating into permeable rocks under conditions of advective heat transfer, caused by vertical groundwater filtration. The results show that temperature profiles and interval heat flow values are sensitive to both the paleoclimatic history and the rate of groundwater filtration. The latter plays the prevailing role in the variations of geothermal field parameters, especially within the uppermost part of the loose sediments in unconfined aquifers. The problem was solved for a permeable layer, underlaid by an impermeable layer. This schematisation of water exchange is the typically accepted for hydrogeological analysis. Even at very low rates of filtration the intensity of this effect is enhanced substantially for long-period variations. In the extreme case (for periods of temperature variations of the order of 100,000 years) at typical rates of filtration within the permeable layer, an almost gradient-free zone can be formed down to depths of a few hundred metres. For the case of upward filtration, on the contrary, the influence of climatic variations on the terrestrial temperature field becomes substantially attenuated.     

Large‐scale erosion and overbank deposition caused by the July 2013 flood of the Abu River,Yamaguchi City,Japan

This paper reports on the erosion, transport, and deposition processes associated with an overbank deposit formed by the flooding of the Abu River on July 28, 2013, in Yamaguchi City, Japan. At the study site, river flows overtopped the levee revetment upstream of a meander bend cutting it off and flowing back into the main channel downstream. In this sequential process, it deposited large amounts of sediments, ranging from mud to cobbles, on the floodplain. The surface of paddy fields adjacent to a railway line, located at the center of the affected floodplain, was severely eroded by the flood flows. Overbank deposits composed of both upstream finer sediments and eroded coarser terrestrial sediments are laid down in the affected area. Large amounts of pebbles and cobbles originating from the eroded terrestrial area formed a gravelly pile on top of the sand and gravel sediments derived from the river. This finding indicates that sands and gravels were deposited prior to the formation of the gravelly pile, probably before and during peak flood flows. An inverse grading structure is evident in the lower to middle part of these comparatively thick deposits, most likely due to differences in transport pattern between entrained terrestrial gravels and upstream finer sediments.     

南海北部陆坡深水区的海底原位热流测量

海底热流数据是开展海洋地球动力学研究和油气资源评价的基础数据.南海北部陆坡深水区蕴含有丰富的油气和水合物资源,而该区热流站位很少.为了解陆坡深水区水合物有利区块的地热特征,利用剑鱼1型海底原位热流探针,在南海西沙海域和神狐海域成功获得了16个站位的热流值.测量结果表明,西沙海槽与白云凹陷都具有较高的热流值,西沙海槽区除1个站位结果不可信外,另2个站位所测海底表层地温梯度分别为105.3 和99.9℃·km^-1,原位热流分别为89±1和87±1 mW·m^-2;白云凹陷中部区域13个站位测得表层地温梯度变化于58.5~100.7 ℃·km^-1,热流值除4个站位低于70 mW·m^-2外,其余都变化于75±2~101±4 mW·m^-2范围,比前人在白云凹陷东部获得的热流高.分析认为,西沙海槽和白云凹陷区域的高地热特征与陆坡深水区的高热背景、晚期断裂发育、底辟、岩浆侵入和热流体活动等有关.