唐古拉山冬克玛底冰川反照率变化特征研究

根据夏季消融期成像的Landsat TM影像和2000-2009年间的MOD10A1数据资料, 分析了唐古拉山区冬克玛底冰川反照率的时空变化特征. 结果表明: 受空间尺度效应和现有反演方法的影响, 由遥感反演的反照率资料在数值上存在一定的误差, 但基本上能够反映冰川反照率的时空变化特征. 从空间分布上来看, 该冰川反照率随海拔升高呈增大趋势, 其中在平衡线附近的变化最为显著; 受地形因素的影响, 在同一海拔带内部也存在着较大的差异. 从年内变化上来看, 该冰川反照率日际变化波动较大, 且具有明显的季节变化特征. 从年际变化上来看, 自2000年以来该冰川年均反照率的变化波动较大, 总体呈微弱下降的趋势, 这主要与年降雪和冰面污化程度有关; 不考虑降雪对冰面反照率的影响, 2000-2009年间该冰川在消融期的反照率呈逐年减小的趋势, 变化速率约为-0.0083·a^-1, 其原因在于夏季气温的升高和冰面污化程度的加大.     

天山乌鲁木齐河源1号冰川消融期反照率特征

消融期冰川反照率特征研究对于深入理解冰川消融过程及其对气候变化的响应机理具有重要意义。利用Landsat卫星影像反演反照率数据,MODIS逐日反照率产品数据以及野外观测反照率数据,分析了天山乌鲁木齐河源1号冰川2016年消融期（5—8月）反照率时空变化特征。研究表明：消融早期,冰川反照率空间变化不明显;消融中后期,总体上呈现随海拔的升高而增大的趋势,在平衡线附近增速最快。消融期冰川反照率整体呈下降趋势,而且在6—7月份变化最为剧烈。平衡线附近反照率时间变化尤其显著,积累区次之,消融区最弱。冰川反照率的时空变化主要由冰面特征决定。气温和固态降水是其驱动因素。冰川反照率随气温的升高而降低,但固态降水会打破其随气温的变化趋势,引起反照率的增加。污化物显著降低冰面反照率,尤其在可见光波段（380~760 nm）。此外,即使冰面特征相对均一,反照率还呈现随太阳入射角的增大而增大的趋势,主要由冰川局部地形（坡度与坡向）差异所致。     

祁连山区雪冰反照率变化及其对冰川物质平衡的影响

雪冰反照率能够改变冰川表面能量收支平衡,是影响冰川消融的重要因素之一。利用祁连山地区冰川面积矢量数据、MODIS逐日积雪反照率、气温和降水以及冰川物质平衡等数据,探讨了祁连山典型冰川区雪冰反照率特征及其对冰川物质平衡的影响。结果表明：祁连山地区冰川多年平均反照率为0.532,冰川区面积大小与其多年平均反照率之间呈显著正相关（R²=0.16,P<0.05,N=91）,即冰川面积缩减1 km²,对应的平均反照率下降0.0025。祁连山老虎沟12号冰川反照率在夏季有明显的海拔效应,且强于其他时段,达到0.047?（100m）^-1。典型冰川年均物质平衡量与冰川表面夏季（6—8月）平均反照率之间存在显著的正相关关系,老虎沟12号冰川和七一冰川决定系数R²分别达到了0.48（P<0.05）和0.66（P <0.05）。冰川表面夏季平均反照率这一指标能够较好地衡量青藏高原北部祁连山地区冰川物质平衡的变化。     

Study on the spatial and temporal variations of the surface albedo on Muz Taw Glacier,Sawir Mountains北大核心CSCD

冰川反照率时空变化特征研究对于评估冰川能量物质平衡及认识冰川消融过程至关重要。本文基于高空间分辨率的Landsat OLI影像和高时间分辨率的MOD10A1产品,并结合冰面反照率实测数据,开展了2011—2021年北疆萨吾尔山木斯岛冰川表面反照率的时空变化特征及其对冰川物质平衡影响的研究。结果表明:Landsat反演反照率和MOD10A1反照率与同期内冰面实测反照率的相关性分别为0.95和0.62,均显示木斯岛冰川表面反照率存在显著的时空变化特征;在空间尺度上,冰面反照率沿主流线整体随海拔升高呈增加趋势。但由于局部地形差异,反照率在海拔3 600 m以下区域随海拔升高出现下降趋势;在同一海拔处,反照率沿冰川两侧边缘向中部递增。2011—2021年,冰川年均反照率微弱增加,消融期内(5—8月)平均反照率与全年平均反照率的变化速率分别为0.0024 a-1和0.0017 a-1;逐月反照率具有显著的季节变化特征,6—8月冰面反照率较低(0.330),12月—次年2月冰面反照率较高(0.586);消融期内冰川消融区反照率下降幅度大于积累区。研究进一步表明,夏季(6—8月)平均反照率与冰川物质平衡存在显著的正相关(R=0.84,P<0.01),气温、固态降水、云量、太阳入射角、吸光性杂质等是影响冰川反照率变化的重要因素。该研究将对冰川消融过程和机理、能量物质平衡模拟等工作提供重要的基础支撑。     

青藏高原唐古拉山多年冻土区夏、秋季节总辐射和地表反照率特征分析

根据青藏高原唐古拉山多年冻土区2005年6月24日~10月16日的总辐射、分光辐射和分光反照率观测资料,利用总辐射和大气层顶太阳辐射的比值——日有效透射率T_eff,用聚类分析法将资料划分为晴天、多云和阴天三类天气,分析了该地区夏、秋季节总辐射、分光辐射比例和分光反照率的日变化和季节变化规律.结果表明,夏季总辐射与大气层顶的差值和日际变化幅度最大,秋季以后这种差值和日际变化幅度减小.天空状况对分光辐射比例和地表反照率均有影响,表现为近红外辐射比例晴天比阴天大,可见光比例晴天比阴天小,各波段反照率晴天均比阴天大.反照率在夏季最低,秋季较高,反照率的日变化有依存分光辐射比例的关系,这大致可以解释地表反照率依存太阳高度角而变化的现象.无积雪地面反照率近红外波段大于可见光波段,地表有积雪时,反照率明显不同,其可见光波段反照率大于近红外波段反照率.功率谱分析表明,日有效透射率T_eff存在着2~3 d的周期,它是该地区天气系统活动影响太阳辐射收入的一个反映,指示出唐古拉山地区天气系统亦有2~3 d的周期性.     

基于相机摄影测量的冰面反照率反演方法研究

雪冰反照率是冰川与积雪能量平衡计算的关键参数,也是观测的难点. 为测量冰面反照率,试验采用相机摄影测量技术,在祁连山十一冰川开展了自动拍摄、并利用共线方程进行冰川正射制图,在此基础上于2012年7月28日-8月18日在冰川表面开展了不同海拔梯度的反照率观测. 通过统计分析晴天与阴天观测反照率与对应点相机拍摄获取的RGB归一化指数之间的关系,对十一冰川进行冰面反照率参数化方法研究. 结果表明：晴天冰面反照率与RGB归一化指数存在明显的指数关系,拟合R²达到0.79;而阴天的统计关系较差,线性拟合R²仅为0.52. 据此尝试利用晴天的拟合公式对整个冰面进行反照率参数化,计算表明：在晴天冰川表面地形阴影区的反照率存在低估现象,而无阴影区的反照率估算结果可信度较高. 利用2013年的反照率观测数据进行了参数化方案的验证,结果表明：观测值与模拟值平均误差仅为0.037,表明利用RGB影像对反照率参数化具有一定的可用性和可靠性.     

我国冬季季节性积雪反照率的观测与模拟——以东北地区为例

应用了一种新的模式spectral albedo model for dirty snow,简称SAMDS,研究了不同参数对于积雪反照率的影响,结果表明：在天顶角固定为60°的条件下,新雪的粒径从50 μm增大到800 μm,使其宽波段反照率从0.92减小到0.78;相对于非球形的雪粒,球形雪粒的积雪反照率更低;吸光性颗粒物对光谱反照率的影响主要在可见光和紫外波段。此外,雪粒径的增大能使吸光性颗粒物的光吸收效应增强。结合东北地区的实测数据,我们发现SAMDS模拟的积雪宽波段反照率与实测结果较为一致。同时,SAMDS模式模拟结果表明,在东北地区,积雪中0.1~1 μg·g^-1的黑碳浓度导致积雪宽波段反照率减少2%~8%,造成的瞬时辐射强迫为9~35 W·m^-2。     

基于MODIS数据的青藏高原冰川反照率时空分布及变化研究

冰川反照率对冰川融化具有重要影响,以2000-2013年MODIS的MOD10A1逐日积雪反照率数据资料为基础,分析了青藏高原冰川反照率的时空分布及变化。结果表明：冰川年平均反照率变化范围是0.42（枪勇冰川）~0.75（PT5冰川）,其中夏季平均反照率变化范围是0.45（来古冰川）~0.69（东绒布冰川和古里雅冰川）。冰川反照率空间分布并没有明显的规律性,而冰川反照率的变化速率空间分布规律明显——南部较大往北减小,北部反照率出现增大现象。研究区内大部分冰川反照率呈波动降低的趋势,年平均反照率和夏季平均反照率变化速率最大值都出现在枪勇冰川,分别是-0.015 a^-1和-0.019 a^-1。木吉和木孜塔格冰川年平均和夏季平均冰川反照率都增大,木吉冰川是由于2012年的高反照率引起的,而木孜塔格冰川主要与该地区气温降低、降水增多有关。     

中国西部不同类型冰川区积雪及其融水径流中稳定同位素比率的时空变化及其气候效应

为了调查和比较我国海洋型、大陆型和极大陆型冰川覆盖区大气降水、冰川、积雪和融水径流系统内稳定同位素比率的时空分布特征和冰雪相变时的现代同位素分馏过程,在2000—2003年间,按照季节和海拔高度分别对玉龙雪山、慕士塔格峰,念青唐古拉山的桑丹康桑峰以及天山乌鲁木齐河源的1号冰川积雪和冰雪融水径流进行了系统的采样研究.结果表明:在以玉龙雪山为代表的海洋型冰川区,新雪内的1δ8O呈现出显著的时间与空间变化,在冬季表现为“高度效应”,即δ18O值随海拔高度升高和气温降低而降低,反映出冬季风降水的特征;而经过融化的夏季积雪受到“降水量效应”、雪中含水量、蒸发等因素的影响,稳定同位素产生分馏变化“高度效应”空间变化比较复杂,反映出夏季风降水的特征,念青唐古拉山夏季积雪也有相似的特征.在极大陆型冰川分布的慕士塔格山地区和亚大陆型冰川分布的天山乌鲁木齐河源地区,夏季新雪中1δ8O则表现为“高度效应”或者“温度效应”.无论在海洋型冰川或者大陆型冰川分布区,经过融化或正在消融的残余积雪内都有明显的同位素分馏变化,1δ8O值比新雪高.受蒸发作用的影响,冰雪融水在流动过程中,1δ8O随海拔高度的降低、流程和流动时间的增加而增加.由于气候条件的差异,海洋型冰川区冰雪融水相变过程中的同位素分馏和化学作用都比大陆型冰川区强.     

祁连山近期七一冰川融水径流特征分析

利用2006年8月1日-9月30日的实测水文数据,对"七一"冰川融水径流产汇流特征进行了分析,并揭示出该冰川日消融特征.通过对冰川融水量的估算以及径流模数的计算,并与过去的观测结果进行对比,表明近些年来"七一"冰川消融强度和消融量都在增大,而且2006年消融量为近几年观测的最大值.虽然不同年份消融量不一样,但"七一"冰川总的趋势是一直处于萎缩状态,随着全球变暖,"七一"冰川的萎缩可能将继续下去.通过对设立在沿冰川下游方向两个不同的水文断面进行对比分析,结果表明"七一"冰川融水径流在向下游运动过程中有部分水入渗为河谷潜流,观测期内两个相距不到2 km的水文断面间渗漏损耗占近1/3左右.     

Unity of the national and the international in the socio-cultural development of the peoples of the USSR

International unity is becoming ever stronger in this country owing to an increasing similarity in the development of the cultural environment. This comprises the provision of all the country's republics with a sufficient number of schools, theatres, and other institutions and cultural information media in accordance with the needs of the population. An important part is played by the rise in ‘the general educational level, as well as the level of professional qualifications and skills. Among all the Soviet nations and nationalities, this rise being more rapid among formerly backward peoples. Prominent among the factors of internationalization is the progressive development of the nationalities’ cultural resources, while professional culture is being increasingly brought within the reach of the masses.The implementation of the nationalities policy promotes the all-round development of all Soviet nations and nationalities, their drawing together, the upsurge of the individual capabilities of every Soviet citizen.     

Global repeating events in the history of the Earth and the motion of the Sun in the Galaxy

Chronological analyses of correlations between certain global repeating events (mass extinctions of marine organisms, meteorite impacts, and flashes in the frequency of geomagnetic reversals) during the Phanerozoic Eon and the motion of the solar system in the Galaxy are presented for five rotationally symmetrical models for the regular Galactic gravitational field. Thirteen of sixteen mass-extinction events can be described by a repetition interval of 183±3 million years. This is in agreement with the anomalistic period (interval between two subsequent passages of the Sun through the apocenter of its Galactic orbit) in the model of Allen and Martos. The positions of the minima and maxima in Gaussian functions approximating the frequency distribution for geomagnetic reversals also agree with the times of passage of the Sun through the apocenter and pericenter, respectively, of its Galactic orbit in this model. The maximum in the distribution of the deviations of the dates of mass extinctions from the nearest dates of impacts of large, crater-forming bodies is close to zero, providing evidence that many such events are correlated. As a rule, extinctions follow impact events. The impacts of large bodies have occurred most often when the solar system passes through the Galactic plane, while mass extinctions occur more often at some distance from the Galactic plane (about 40 pc). As a rule, intervals of increases in the frequency of geomagnetic reversals coincide with dates of impacts of large bodies. At the same time, these intervals do not show a clear correlation with the dates of mass extinctions. The intensity of mass extinctions, like the energy released by impacts, is consistently higher in periods when the Sun is moving from the apocenter toward the pericenter of its orbit, than when it is moving from the pericenter toward the apocenter. Thus, there is evidence for a variety of relationships between repeating global events in the Phanerozoic and the motion of the Sun in the Galaxy. Long-period variations in the frequency of geomagnetic reversals are correlated with the orbital motion of the Sun, and increases in the frequency of geomagnetic reversals are correlated with impacts. Mass extinctions are correlated with the impacts of large bodies, whose motions may have been perturbed by clouds of interstellar material concentrated toward the Galactic plane and by the shock front associated with the Perseus spiral arm, through which the solar system passes. The velocity of the Sun relative to the spiral pattern is estimated.     

Deviation of the major axis of the inertia ellipsoid of the Moon from the direction toward the Earth

It is known from observations that the center of mass of the Moon does not coincide with the geometric center of its figure, and the line connecting these two centers is not aligned with the direction toward the center of the Earth, instead deviating toward the Southeast. This stationary deviation of the axis of the inertia ellipsoid of the Moon to the South of the direction toward the Earth is analyzed. A system of five linear differential equations describing the physical libration of the Moon in latitude is considered, and these equations are derived using a new vector method taking into account perturbations from the Earth and partly from the Sun. The characteristic equation of this system is obtained, and all five oscillation frequencies are found. Special attention is paid to the fifth (zero) frequency, for which the solution of the latitude libration equations are stationary and represents a previously unknown additional motion of the rotational axis of theMoon in a cone with a small opening angle. In contrast to the astronomical precession of the Earth, the rotation of the angular-velocity vector is in the positive direction (counter-clockwise), with the period T ₃ = 27.32 days. On this basis, this phenomenon has been named “quasi-precession.” This quasi-precession leads to a stationary inclination of the major axis of the inertia ellipsoid of theMoon to the South (for an observer on Earth), making it possible to explain one component of the observed deviation of the center of mass of the Moon from the direction toward the Earth. The opening angle of the quasiprecession cone is approximately 0.834″.     

从榴辉岩与围岩的关系论苏鲁榴辉岩的形成与折返

位于华北和扬子两板块碰撞带中的苏鲁榴辉岩形成的温压条件不但是超高压，而且是高温。榴辉岩的PTt轨迹表明其为陆-陆磁撞俯冲带的产物。榴辉岩的区域性围岩花岗质片麻岩为新元古代同碰撞期花岗岩，榴辉岩及其他直接围岩皆呈包体存在于其中，并见新元古代花岗岩呈脉状侵入榴辉岩包体中。区域性围岩新元古代花岗岩的锆石中发现有柯石英、绿辉石等包裹体，表明新元古代花岗岩的组成物质也经受过超高压变质作用，且榴辉岩与围岩新元古代花岗岩的锆石U-Pb体系同位素年龄基本相同。但新元古代花岗岩所记录的变质作用和变形作用期次（或阶段）却少于榴辉岩。椐上述可得如下推断：超高压榴辉岩与新元古代花岗岩岩浆是同时在碰撞带底部（俯冲板块前部）形成的；榴辉岩的第一折返阶段是由新元古代花岗岩岩浆携带上升的，其第二折返阶段是和新元古代花岗岩一起由逆冲及区域性隆起而上升，遭受剥蚀。     

某高速公路下伏煤矿采空区稳定性分析

在论述某高速公路下伏砦脖煤矿采空区地质、采矿和工程地质特征的基础上, 进行了稳定性数值模拟分析, 定性与定量地分析与评价了该煤矿采空区的地表变形特征及稳定性。研究结果表明: 该煤矿采空区的变形尚未完成, 对拟建的高速公路将产生很大的危害, 必须采取相应的工程治理措施。      

摩擦桩基桩土间极限摩阻力取值问题探讨

通过对广珠东线高速公路横沥大桥的试桩及土体的工程地质条件分析,总结出影响摩擦桩基桩土间极限摩阻力取值的一般问题以及解决问题的方法和措施。     

The Importance of the Precipitation and the Susceptibility of the Slopes for the Triggering of Landslides Along the Roads

In order to characterise the influence of the heavyrains on the observed landslides during the 1996–1997hydrological cycle, rainfall records for the last 100years are analysed from 104 stations in easternAndalusia. Regarding the amounts of rain recordedbetween October 1996 and March 1997 in the 104stations studied, 31 presented new all-time records;15 presented values that were 80–100% of thepre-1995 record; 49 stations, 80–50%; and 9stations, < 50%. A map has been devised of thesusceptibility of the materials through which thesouth-eastern Andalusian road network crosses,together with an inventory of the damage caused byinstability phenomena on banks and cuttings of theroad network during the winter of 1996–1997. Therelationships between the rainfall during the studyperiod, the damage caused to the road network and thesusceptibility of the materials affected are analysed.The results indicate that there is a clearcorrespondence between the rainfall recorded and thesusceptibility of the materials with the inventorieddamage. It is concluded that the widespread seriousdamage caused in early 1997 to the roads andsurrounding areas in the Alpujarra region and thecoast of the Province of Granada was mainly caused bythe extraordinarily heavy rains. However, considerablyless damage was observed where the susceptibility ofthe terrain is low, thus highlighting the extremeusefulness of terrain-susceptibility maps for riskprevention and territorial planning.     

Paleomagnetic implications on the evolution of the tethys belt from the atlantic ocean to the pamirs since the triassic

We first re-examined the apparent polar wander curves for stable Eurasia and Africa since the Triassic. These curves were then combined together with curves of North and South America according to the kinematics of the Atlantic ocean and a synthetic polar wander curve was given. Then, most of the paleomagnetic results from the Tethys mobile belt, from the Atlantic to the Pamirs, were analysed.Several groups of plates, microplates and blocks can be seen. First, relatively stable regions like Maghreb and Sicily, which have not moved much. Then we have a group formed by Iberia, Sardinia, Italy and, to a lesser extent, Corsica and the Western and Central Alps. For these blocks, movements are anticlockwise rotations chiefly driven by the anticlockwise rotation of Africa, but they are sometimes stronger.To the east, a major change takes place. The north of the Aegean Sea and the Ionian zone are clockwise rotated and these rotations are recent: Oligocene-Miocene for the first part, Pliocene to the present for the second part.A major problem arises in Turkey, Caucasus and Iran. Paleomagnetic results indicate a position far to the south of Eurasia, and, at the same time, geological evidence is in favour of a position close to Eurasia. We discuss these discrepancies.