造山的高原——青藏高原巨型造山拼贴体和造山类型

青藏高原是一个巨型碰撞造山拼贴体,它的形成与始特提斯、古特提斯和新特提斯洋盆的先后开启、消减、闭合以及古大陆的裂解、诸地体的移动、会聚和拼合有关。造山类型形成于不同时期海(洋)盆俯冲、地体碰撞和陆内会聚的不同阶段。多地体/多岛弧/多弧前海的构架表明,诸多的俯冲型山链可以产生在地体边界的活动陆缘一侧,古特提斯南、北两洋盆的双向俯冲构筑了双向俯冲型山链;碰撞型山链由于地体边界与块体驱动方向的几何学关系形成“正向碰撞型”和“斜向碰撞型”造山类型。“斜向碰撞型山链”与走滑断裂的形成、规模及其运动学直接相关。50~60Ma印度/亚洲碰撞不仅形成青藏高原造山拼贴体的最后成员———喜马拉雅山链,而且在拼贴体的北缘由于陆内俯冲作用使早期形成的山链在整修后又一次崛起。青藏高原的周缘山链铸成屏障与外侧的克拉通相隔。青藏高原巨型碰撞造山拼贴体的形成是亚洲大陆自北往南的增生和造山迁移的生长结果,其所反映的活动长期性、非原地性、俯冲/碰撞/陆内造山类型的多样性、碰撞造山的多期性以及造山的复合叠置性比世界上任何一个复合山链(或造山拼贴体)来得复杂、多彩。     

Tectonic role of ophiolite-bearing terranes in the development of the Southern Apennines orogenic belt

New data on ophiolite-bearing terranes of the Liguride Complex, together with some information on the terranes of the Sicilide Complex, result in a better understanding of the role and tectonic significance of these units in the construction of the Southern Apennines orogenic belt. The Liguride Complex is composed of two main tectonic units overlain by a thick turbiditic sequence of Late Oligocene-Middle Miocene age. The uppermost one (Frido Unit) is a polydeformed and polymetamorphosed sequence, composed of two tectonic subunits of shales and calc-schists, respectively, containing blocks of ophiolite, garnet gneiss, amphibolites and granitoids. This unit is thrust over the un-metamorphosed terranes (Calabro–Lucano Flysch Unit) consisting of a broken formation with blocks of Late Jurassic ophiolite and their sedimentary cover, Cretaceous-Eocene pelagic sediments and Late Oligocene volcaniclastic deposits. The Frido Unit underwent HP/LT metamorphism (P= 8–10 Kb; T= 400–500 °C) resulting in glaucophane and lawsonite assemblages in the ophiolitic rocks and aragonite in the meta-limestones and calc-schists, followed by greenschist fades metamorphism (P= 4 Kb; T= 300–350 °C). From a structural point of view units of the Liguride Complex comprise structures developed at different structural levels, indicating progressive non-coaxial deformation in response to tectonic transport towards the N-NE. The ophiolite-bearing terranes of the Liguride Complex can be considered as a remnant of an accretionary complex in which the Calabro Lucano Flysch Unit represents the toe of the wedge where frontal accretion processes occur and the Frido Unit is a deeper portion. Emplacement of the Frido Unit is explained as being due to formation of a deep duplex structure during the early stage of continental collision processes. The polarity of tectonic transport provides new evidence that the Liguride Complex represents a suture zone between the Apulian and the Calabrian blocks. The age of collision appears to be not older than late Oligocene. The allochtonous terranes of the Liguride and Sicilide Complexes, therefore, represent a complete accretionary wedge which records, first, subduction of the Neotethys ocean beneath the Calabrian (Europe) continental margin and, later, continental collision with the African block.     

喜马拉雅造山带东构造结拉布拉多期和格林威尔期造山作用的记录

位于喜马拉雅东构造结西北部的南迦巴瓦复合体,是构造应力最强、隆升和剥蚀最快、新生代变质和深熔作用最强的地区。为厘定该地区早期的变质岩浆作用,本文对南迦巴瓦复合体北部的花岗片麻岩和混合岩进行了岩石学和年代学研究。花岗片麻岩原岩为富钾的偏铝质花岗岩,具有岩浆弧花岗岩的成分特征。花岗片麻岩中的锆石具有岩浆锆石的环带结构,记录了487.9±1.6Ma的一期构造岩浆事件;混合岩的锆石具有明显的核-边结构,核部和边部的不协和线交点年龄分别为1559±13Ma、1154±12Ma。对比印度大陆东部的西隆高原、东高止造山带,发现三者都经历了拉布拉多期、格林威尔期以及泛非期的造山作用。因此,我们认为喜马拉雅东构造结与这两个地区密切相关,可能是他们向北的延伸,这三者可能组成统一的印度大陆东部造山带,一起经历了哥伦比亚超大陆、Rodinia和冈瓦纳超大陆的聚合与裂解过程。     

粉喷桩工程性状试验研究

对水泥加固土的工程特性进行了系统的研究。 现场开展了粉喷桩单桩及复合地基静载试验, 对粉喷桩复合地基承载力、桩土应力比及单桩荷载传递规律进行了分析和研究。取得了一些有益的结果, 这些结果对粉喷桩工程实践具有指导意义     

南秦岭东江口岩体中丰富金矿矿床特征与成因浅析

陕西省宁陕县丰富金矿产于南秦岭构造带东江口岩体内,为一中型规模金矿床,赋矿围岩为黑云母二长花岗岩。矿床形成于印支-燕山期秦岭造山过程中由碰撞向伸展构造体制转变的后碰撞构造环境,成矿时代限定为200Ma左右的燕山早期,矿床类型为硫化物石英脉型和破碎带蚀变岩型。金的赋存状态有包裹金、裂隙金及晶隙金三种,以裂隙金和晶隙金为主,具有多期成矿特征。围绕主岩浆期后超浅成-浅成侵入的中基性岩脉、岩枝、岩株呈环状展布的缓倾斜断裂是主要的控矿和赋矿构造,成矿作用与主岩浆期后火山-次火山作用或隐蔽爆破作用引发的热液作用有关。     

An example of structural and metamorphic relationships in the Musgrave orogenic belt,central Australia

The western Musgrave Ranges are broadly divided into three groups of metamorphic rocks. A central granulite‐facies core is bounded on the north by rocks of amphibolite grade and on the south by rocks transitional between the granulite and amphibolite facies. Faults trending east‐west separate the three groups of rocks.

The detailed structural relationships between the granulites and the lower grade rocks are described and discussed. The granulites are structurally relatively simple and are characterised by the presence of a strong southwesterly‐plunging, mineral‐streaking lineation. In marked contrast, the transitional rocks are more complexly folded on a macroscopic scale and they also have a well‐developed mineral lineation plunging to the southeast. These two lineation orientations are considered to be directions of maximum elongation. The amphibolite‐facies rocks are also complexly folded and at least two lineations related to different phases of deformation have been recognized.

A suite of foliated and lineated dolerite dykes which occurs throughout the area inherited their fabric during a period of intense deformation and recrystallization, which resulted in the development of numerous mylonite zones.

It is suggested that the granulite‐facies rocks may represent a suite of cover rocks which have been thrust in a northerly direction over a pre‐existing amphibolite‐facies basement.     

昆仑—秦岭造山系的几个问题

昆仑—秦岭带加里东旋回的洋盆不是从元古代继承下来的,而是由寒武纪裂谷发展而来的,它在志留纪即宣告封闭;昆仑石炭纪—二叠纪海底裂谷带或可能的小洋盆,在晚二叠世前已经消失,三叠纪时昆仑—秦岭带只有海,而没有洋。因此,印支造山运动并不是洋盆消失后的陆—陆碰撞造山,而是陆—陆叠复造山(大陆壳消减造山)作用。     

The role of satellite altimetry in gravity field modelling in coastal areas

During recent years altimetry from the two geodetic missions of GEOSAT and ERS-1 has enabled the derivation of high resolution near global gravity field from altimetry [Andersen and Knudsen, 1995, 1996; Sandwell and Smith, 1997].Altimetric gravity fields are unique in the sense that they provide global uniform gravity information with very high resolution, and these global marine gravity fields are registered on a two by two minute grid corresponding to 4 by 4 kilometres at the equator.In this presentation several coastal complications in deriving the marine gravity field from satellite altimetry will be investigated using the KMS98 gravity field. Comparison with other sources of gravity field information like airborne and marine gravity observations will be carried out and two fundamentally different test areas (Azores and Skagerak) will be studied to investigated the different role of these different sources of gravity information.     

初论板内造山带

讨论了关于板内造山带含义的不同认识。指出板内造山带是一种特殊类型的造山带,而不是板缘造山带或板间造山带持续发展的结果。简要介绍分别发育在４ 个大陆的不同时代的板内造山带,总结板内造山带在区域大地构造位置、造山带构造格局、构造变形与变质作用、岩浆活动与沉积作用、造山带构造演化等方面与板缘造山带的差异。板内造山带形成于相对较老且强硬的岩石圈板块内部,造山带内部构造单元不具有平行于造山带走向分布的特征,即不具有线状构造格局,构造变形具有地台基底乃至整个地壳卷入的厚皮构造性质,同造山区域变质作用微弱,同造山岩浆活动、沉积作用和构造变形均无极性演化趋势。岩石圈拆沉作用（ｄｅｌａｍｉｎａｔｉｏｎ） 可较好地解释板内造山带的火山活动特征。尽管板块间相互作用（ 俯冲或碰撞）所产生的水平挤压应力似乎更易于阐明板内造山带的收缩变形特征;但是,板块间相互碰撞或俯冲产生的边界应力可否有效地被远程传递,尚有待进一步研究和解决。将板块间相互作用的水平应力场与岩石圈纵向物质与能量调整（ 重力、热力等） 因素作综合考虑,可能是解决板内造山带造山作用机制的有效途径     

关于造山带花岗岩类填图方法的讨论——以西秦岭天水地区为例

花岗岩类的分类理论决定其填图方法.现行的单元-超单元填图方法是依据花岗岩类的I型、S型分类理论和同源岩浆演化理论而建立的.由于同源岩浆演化理论的不完善性,造山带地壳结构及地质构造特征的复杂性、地质作用过程的多样性,导致了形成花岗岩类源岩组分的复杂性,使得I型、S型分类在造山带具有不确定性,因而单元-超单元填图方法在造山带实践中存在较多问题和矛盾.造山带花岗岩类填图方法应以基本岩石分类方案为依据,以野外可识别、易掌握的客观岩石学、矿物学、组构学为准则, 客观、真实地反映造山带花岗岩类的特色.     

Elevator tectonics and orogenic collapse of a Tibetan-style plateau in the European Variscides: the role of the Bohemian shear zone

Variscan collision of peri-Gondwanan terranes led to a doubly vergent crustal wedge that was thicker than 55 km in the area of the Bohemian Massif. This crustal thickness resulted in a highly elevated Bohemian plateau with a topographic height >3–4 km. The Bohemian plateau was covered with unmetamorphic Paleozoic strata, all of which are today well preserved in the Tepla–Barrandian unit because of crustal-scale vertical slip along the Bohemian shear zone (BSZ). The BSZ forms a subvertical, ca. 500-km long and up to 2-km wide belt of dip–slip mylonites which show several 90° deflections in map view. Tepla-Barrandian-down movements were active under retrograde metamorphic conditions, starting with granulite and ceasing with greenschist facies conditions. As slip along the BSZ was largely vertical and led to a minimum throw of 10 km, this type of crustal-scale deformation is referred to as elevator tectonics. The elevator-style movements caused the juxtaposition of the supracrustal Tepla–Barrandian lid (the “elevator”) against high-grade rocks of the extruding orogenic root. The BSZ has further governed the foci of mantle-derived plutonism. New U–Pb zircon and monazite TIMS dating of six plutons suggest that emplacement of mantle-derived melts along the BSZ lasted for at least 20 m.y., starting with the emplacement of the Klatovy granodiorite at 347 +4/−3 Ma and ceasing with the emplacement of the Drahotin pluton at 328 ± 1 Ma. When taking into account the new ages of synkinematic plutons, the simultaneous vertical slip along the individual segments of the BSZ (North, West, and Central Bohemian shear zone) is bracketed to the period 343–337 Ma. Elevator tectonics was probably controlled by delamination of thickened mantle lithosphere that caused a dramatic thermal turnover and heating-up of the orogenic root. The overheated lower crust was thermally softened by anatexis and diffusion creep resulting in channel flow, vertical extrusion, fast uplift, and exhumation of the orogenic root.     

Single-layer folding in marble and limestone: An experimental study

Folding experiments have been carried out on single-layers of Carrara marble and Solnhofen limestone at a confining pressure of 275 bars, temperature of 400°C, and strain rates of 5.5×10⁻⁷ to 8.2×10⁻⁷. The marble and limestone layers were embedded in a rock-salt matrix and in a matrix of a mixture of 60% fine-grained halite and 40% fine-grained calcite, respectively, and deformed to different percentages of bulk shortening. Aspect ratios of the layers varied between 11.25 and 15. The stress-strain relationship reveals that strain increased with a very small increment in compressive stresses, once folding was initiated.With progressive deformation the bulk strain is compensated by folding along one fold hinge. The resulting folds are concentric and a combination of class 1a, 1b and 3 type. The changes in the arc length, layer thickness, limb dip and wavelength with progressive folding in marble layers, are discussed.The microstructure and texture of the folded marble and limestone layers have been investigated optically and by means of an X-ray texture goniometer. The inner fold arc exhibits a strong preferred orientation, whereas in the outer fold are the preferred orientation is poorly developed. Differences in the fabric in medium-grained marble and fine-grained limestone layers have been attributed to the difference in mechanism of deformation.     

Ductile rebound of an orogenic root: case study and numerical model of gravity tectonics in the Western Gneiss Complex, Caledonides, southern Norway

The main Caledonian deformation in the Western Gneiss Complex (southern Norway) has been interpreted as resulting from the gravity-driven ductile rebound of the orogenic root. Detailed field data from the Sognefjord profile, a 60-km long, continuously exposed shore section through the complex, are compared with the results of a numerical scale model of root rebound dimensioned according to reconstructions of the overall tectonic evolution. The strain pattern in the model can be closely tied to the previously recognized structural regimes, from east to west: R1 – little deformed Precambrian basement (stiff orogenic lid, basal part of upper crust); R2 – heterogeneously sheared basement ('simple shear' domain at upper crust/lower crust boundary); R3 – completely overprinted basement with eclogitic remnants ('pure shear' regime in the lower crust of the rebounded root). Subsequent to root rebound the profile remained practically unaffected by later tectonic events, except for tilting/uplift/erosion, providing a unique example of deep-seated gravity tectonics.     

Large tank experiment on nitrate fate and transport: the role of permeability distribution

A long-term elution experiment to study the saturated transport of pre-accumulated fertilizers by-products, was conducted within a large tank (4 × 8 × 1.4 m) equipped with 26 standard piezometers. Sandy sediments (35 m³), used to fill the tank, were excavated from an unconfined alluvial aquifer near Ferrara (Northern Italy); the field site was connected to a pit lake located in a former agricultural field. To evaluate spatial heterogeneity, the tank’s filling material was characterized via slug tests and grain-size distribution analysis. The investigated sediments were characterized by a large spectrum of textures and a heterogeneous hydraulic conductivity (k) field. Initial tank pore water composition exhibited high concentration of nitrate (NO₃ ⁻) sulfate (SO₄ ²⁻) calcium (Ca²⁺), and magnesium (Mg²⁺), due to fertilizer leaching from the top soil in the field site. The initial spatial distribution of NO₃ ⁻ and SO₄ ²⁻ was heterogeneous and not related to the finer grain-size content (<63 μm). The tank’s material was flushed with purified tap water for 800 days in steady-state conditions; out flowing water was regularly sampled to monitor the migration rate of fertilizer by-products. Complete removal of NO₃ ⁻ and SO₄ ²⁻ took 500 and 600 days, respectively. Results emphasized organic substrate availability and spatial heterogeneities as the most important constraints to denitrification and nitrogen removal, which increase the time required to achieve remediation targets. Finally, the obtained clean-up time was compared with a previous column experiment filled with the same sediments.     

Timing of orogenic events in the Lachlan Orogen

A substantial database of ⁴⁰Ar/³⁹Ar ages, collected recently from micas in western and central Victoria, has been used in several recent papers as support for continuous, diachronous deformation across western and central Victoria lasting through much of the Early Palaeozoic. This paper reviews these ages, together with field evidence collected over the last ten years. It provides an alternative interpretation, that mica growth and overgrowth in western Victoria was not continuous but episodic, occurring at ca 455 Ma, 440 Ma and 425 Ma, with little or no mica growth recorded from between these times. These ages have been obtained from mica in regional cleavage, crenulation cleavage and in quartz veins, and from across the entire width of the Stawell and Bendigo structural zones of western Victoria. A sharp change in mica ages occurs at the Mt William Fault, east of which no mica growth older than about 380 Ma is recorded. Several ages used in support for diachronous deformation are not related to deformation: an ⁴⁰Ar/³⁹Ar age of 417 Ma from Chewton is from the aureole of a Devonian granite, and an age of 410 Ma from the Melbourne Zone is shown to contain a substantial amount of inherited mica. If it is accepted that mica growth can be used to date deformation, then the ⁴⁰Ar/³⁹Ar ages indicate episodic, not continuous, deformation in western Victoria (Stawell and Bendigo Zones). The sharp decrease in the deformation age in the Melbourne Zone, east of the Mt William Fault, agrees well with field evidence that shows continuous sedimentation in the Melbourne Zone in the period (Ordovician to mid‐Early Devonian) during which the Stawell and Bendigo zones were undergoing deformation. Some correlation also exists between the ⁴⁰Ar/³⁹Ar ages from western Victoria and well‐constrained deformational events in the eastern Lachlan Orogen. The pattern of deformation has important corollaries in any model that attempts to understand what drives the deformation. While plate convergence must be the ultimate driving force, the pattern is quite inconsistent with deformation of a crust that was being drawn progressively into subduction zones, as proposed in recently published models. Rather, the observed pattern suggests that deformation happened in several very brief events, probably on semi‐rigid plates.     

An experimental investigation of density-stratified inertial gravity currents

Turbidity currents and pyroclastic density currents may originate as stratified flows or develop stratification during propagation. Analogue, density‐stratified laboratory currents are described, using layers of salt solutions with different concentrations and depths to create the initial vertical stratification. The evolving structure of the flow depends on the distribution of the driving buoyancy between the layers, B* (proportional to the layer volumes and densities), and their density ratio, ρ*. When the lower layer contains more salt than the upper layer, and so has a greater proportion of the driving buoyancy (B* < 0·5), this layer can run ahead leading to streamwise or longitudinal stratification (ρ*→0), or the layers can mix to produce a homogeneous current (ρ*→1). If the upper layer contains more salt and thus buoyancy (B* > 0·5), this layer travels to the nose of the current by mixing into the back of the head along the body/wake density interface to produce a homogeneous flow (ρ*→1) or overtaking, leading to streamwise stratification (ρ*→0). Timescales describing the mixing between the layers and the streamwise separation of the layers are used to understand these flow behaviours and are in accordance with the experimental observations. Distance–time measurements of the flow front show that strongly stratified flows initially travel faster than weakly stratified flows but, during their later stages, they travel more slowly. In natural flows that are stratified in concentration and grain size, internal features, such as stepwise grading, gradual upward fining and reverse grading, could be produced depending on B* and ρ*. Stratification may also be expected to affect interactions with topography and overall fan architecture.     

An approach to folding kinematics from the analysis of folded oblique surfaces

Two-dimensional analysis of folded surfaces oblique to the mechanical layering can shed light on the kinematic mechanisms that operated during the development of folds. A new version of the program ‘FoldModeler’, developed in the Mathematica™ environment, is used to obtain the deformed configuration of an initial pattern of oblique surfaces deformed by any combination of the most common kinematic folding mechanisms: flexural flow, tangential longitudinal strain, with or without area change and heterogeneous simple shear. The layer can also undergo any form of homogeneous strain at any moment of the folding process. The outputs of the program provide complete information about the strain distribution in the folded layer that includes graphs of the angle between the oblique surfaces as a function of the inclination of the layering through the fold. These graphs can be very useful to discriminate between the mechanisms that operate in the development of natural folds, and they have been obtained and discussed for the most common combinations of strain patterns. The program is applied to obtain theoretical folds that give a good fit of some natural examples of folded oblique surfaces.     

On the origin of orogenic volcanism

It is widely believed that the explanation of orogenic volcanism lies in the shear heating and subsequent partial melting of the crustal fraction of subducted lithosphere. Careful examination of simple models of the shear-heating process indicates, however, that this process cannot occur in a system with constant strain-rate boundary conditions, for reasonable values of the strain rate and material parameters. Thermal runaway cannot occur because viscous dissipation process is limited by the effect of temperature on viscosity, although shear-heating instability may develop during non-steady-state shear at stress or strain-rate values above certain critical values. Examination of subduction history models indicates that supercritical shear stresses constant over some tens of kilometers may be found in subduction shear zones. Since instability may develop if such conditions are present over even a 1–10 km range, it is still possible that non-steady-state process could explain the origin of orogenic volcanism.

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Zusammenfassung Schererwärmung bis zum partiellen Aufschmelzen der subduzierten Kruste wird vielfach als Ursache des orogenen Vulkanismus genannt. Eine sorgfältige Betrachtung eines einfachen Schererwämungsmodells führt zu folgenden Resultaten: Schererwärmung unter Vorgabe konstanter Dehnungsrate in der Scherzone führt zu allmählicher Erwärmung, wobei die Temperatur unter der Solidusgrenze bleibt, sofern man vernünftige Werte der Modellparameter wählt. Die Temperaturerhöhung bleibt in diesem Fall beschränkt durch die Rückkopplung von Temperatur und Viskosität. Schererwärmungsinstabilitäten, die zu partiellem Aufschmelzen führen, sind möglich, sofern bei nicht-stationärer Schererwärmung die Scherspannung oder die Dehnungsrate gewisse kritische Werte übersteigen. Es wird gezeigt, daß die Annahme superkritischer und konstanter Scherspannung entlang von 1–10 km langen Wegstücken der subduzierten Kruste mit Beobachtungen und Modellrechnungen verträglich ist. In diesem Fall können Scherinstabilitäten in einer Tiefe von 100 km bis 200 km in der subduzierten Kruste auftreten.

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Résumé On croit couramment que l'explication du volcanisme orogénique se trouve dans l'échauffement causé pai les tensions d'arrachement et dans la fusion partielle consécutive de la fraction crustale de la lithosphere en voie de subduction. Une considération soigneuse d'un modèle simple d'échauffement par tensions conduit aux résultats suivants: un échauffement sous de telles tensions et dans des conditions avantageuses d'un degré d'extension constant dans la zone de cisaillement conduit à un échauffement par broyage où la température reste maintenue en-dessous de la limite du solidus pour autant qu'on choisisse des valeurs raisonables pour les paramètres du modèle. L'élévation de température reste dans ce cas limitée par le couple température-viscosité. Les instabilités par échauffement sous tension qui conduisent à la mise en fusion partielle, sont possibles pour autant que, sous un échauffement non stationnaire, le cisaillement ou le degré d'extension ne dépasse pas certaines valeurs critiques. On montre que l'adoption d'une tension de cisaillement supercritique et constante le long de tronçons de 1–10 km de la croûte en voie de subduction est compatible avec les observations et avec les calculs déduits du modèle. Dans ce cas des instabilités sous l'effet du cisaillement peuvent se produire dans la croûte en voie de subduction à une profondeur de 100 à 200 km.

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激电找矿在拾金坡矿区的试验研究

应用激发极化法 (简称激电 )查明拾金坡矿区优选区内主要脉体的含矿性 ,含金石英脉体的走向和深部的产状 ,为布置钻探工程提供依据     

秦岭—大别造山带(湖北段)重力场特征与造山带构造

利用区域重力资料,通过位场分离、转换技术,揭示了造山带深部构造特征。正的线状重磁异常带及各阶小波细节,清晰地反映了桐柏—大别及东秦岭造山带南缘缝合带的位置,特别是重力异常小波四阶逼近,深部构造特征更加醒目。在鄂西北地区岩石圈所呈现出的"立交桥式"双层结构中,自由空间、均衡重力、剩余重力异常及小波各阶细节明显地反映出相对浅部的造山带近东西向延伸的构造特征;各阶逼近结果则反映了相对深部的地壳-岩石圈地幔南北向伸展的构造特征。应用地球物理资料来研究地球岩石圈结构、构造,除深层地震外,区域重力也是最有效方法手段之一。特别是近年来二维小波变换技术日趋成熟,为应用区域重力资料解决诸如造山带深部构造等疑难问题提供了新的手段和工作思路。