Decameter Type III-Like Bursts

We report the first observations of Type III-like bursts at frequencies 10 – 30 MHz. More than 1000 such bursts during 2002 – 2004 have been analyzed. The frequency drift of these bursts is several times that of decameter Type III bursts. A typical duration of the Type III-like bursts is 1 – 2 s. These bursts are mainly observed when the source active region is located within a few days from the central meridian. The drift rate of the Type III-like bursts can take a large value by considering the velocity of Type III electrons and the group velocity of generated electromagnetic waves.     

Effects of surface flux parameterization on the numerically simulated intensity and structure of Typhoon Morakot (2009)

The effects of surface flux parameterizations on tropical cyclone(TC) intensity and structure are investigated using the Advanced Research Weather Research and Forecasting(WRF-ARW) modeling system with high-resolution simulations of Typhoon Morakot(2009).Numerical experiments are designed to simulate Typhoon Morakot(2009) with different formulations of surface exchange coefficients for enthalpy(C_K) and momentum(C_D) transfers,including those from recent observational studies based on in situ aircraft data collected in Atlantic hurricanes.The results show that the simulated intensity and structure are sensitive to C_K and C_D,but the simulated track is not.Consistent with previous studies,the simulated storm intensity is found to be more sensitive to the ratio of C_K/C_D than to C_K or C_D alone.The pressure-wind relationship is also found to be influenced by the exchange coefficients,consistent with recent numerical studies.This paper emphasizes the importance of C_D and C_K on TC structure simulations.The results suggest that C_D and C_K have a large impact on surface wind and flux distributions,boundary layer heights,the warm core,and precipitation.Compared to available observations,the experiment with observed C_D and C_K generally simulated better intensity and structure than the other experiments,especially over the ocean.The reasons for the structural differences among the experiments with different C_D and C_K setups are discussed in the context of TC dynamics and thermodynamics.     

安顺市一次飑线天气过程的诊断分析

该文利用FNL再分析资料(水平分辨率1°×1°)、常规的地面观测资料、中国国家卫星中心提供的TBB资料、贵阳雷达站提供的雷达资料,针对安顺市2020年5月31日出现的飑线天气过程,进行了环流背景、物理量、数值预报检验以及雷达回波、卫星云图特征等分析。结果表明：此次强对流天气过程是由地面辐合线、高空槽、中低层的低涡切变线和低空急流共同影响造成的;不稳定层结、大的垂直风切变、适当的0 ℃层和-20 ℃层高度为当日的飑线过程提供了有利的不稳定层结条件。贵州省上空出现了大范围的高温高湿区,大值区位于贵州省的中部以南地区,并在该区域存在明显的Ω型能量锋区和湿舌,为此次贵州飑线的触发和发展提供了很好的能量条件。此次飑线过程中,普定和安顺城区雷达回波图上均出现了高反射率因子和速度大值区,飑线中的普通单体在安顺城区发展为超级单体。卫星云图上贵州省中部出现了带状云系,强对流天气发生在对流云团边缘TBB的梯度大值区。从GRAPES-3 km逐小时的预报场与实况对比来看,对此次飑线过程的位置和强度预报都很好,说明该产品对短时预报和监测都有很好的指示意义。     

一种适用于极区的横轴墨卡托海图

极区位于高纬度地区,极区航海图投影采用墨卡托投影时,图上极区附近变形较大,在极点处变形达到无穷大;采用极球面投影时,图上恒向线不是直线;心射切面投影不是正形投影,不能直接在图上量取方位和距离;兰伯特正形投影图上,经度是由角度表示,而不是真的经度;采用横轴墨卡托投影时,几乎所有的经线以及纬线在图上为曲线。以上常用的海图投影不利于船舶在极区安全航行,也不利于航海人员进行海图作业。针对此问题,将构建的伪经纬线网与经纬线网进行转换,通过Matlab得到基于伪经纬线网的横轴墨卡托投影图,此图具有类似于墨卡托海图的特点,图上极区变形失真小,图上伪经纬线的特点可方便极区海图作业。     

坡度随水平分辨率变化及其空间格局研究

以黄土丘陵沟壑区的县南沟流域为研究区,基于1∶1万地形图,利用ANUDEM软件生成5m到200m分辨率DEM,并利用Arc/Info中计算坡度的方法提取了各种分辨率的坡度。研究表明,随着DEM分辨率的降低,单个样点坡度值表现出不确定性,但同一坡度级所有栅格点的坡度均值呈现一定的规律性,低坡度段表现为先升高后降低,中坡度段呈现微弱变化,陡坡度段呈现对数降低趋势;沟沿线上坡度值呈比较剧烈的下降趋势、分水线和流水线上坡度缓慢下降。     

测绘卫星的姿态控制技术

通过分析测绘卫星的姿态控制要求, 研究了卫星姿态控制所涉及的主要误差源, 提出了相应的解决措施, 针对测绘卫星的需求进行了姿态控制系统方案设计。     

West Pacific-type convergent boundaries and their role in the formation of the Central Asian Fold Belt

The type of convergent boundaries forming in the area of mantle plumes is considered. These convergent boundaries (West Pacific type) are characteristic of the western margin of the Pacific. West Pacific-type boundaries are a regular succession of structures from ocean to continent: island arcs, marginal basins, rift basins, and associated OIB-type volcanics at the continental edge. The convergence zones are up to a thousand kilometers wide.Studies of the history of the part of the Central Asian Fold Belt forming the folded periphery of the Siberian continent have shown that the continent drifted above the African plume or corresponding low-velocity mantle province for most of the Phanerozoic (up to the Early Mesozoic inclusive). This fact determined the West Pacific type of convergent boundaries for the accretionary structures of the Central Asian Fold Belt. The drift of Siberia from African to Pacific province in the Late Cenozoic determined the structure and development of the convergent boundary in the western Pacific, including extensive intraplate magmatism in continental Asia in the Late Mesozoic and Cenozoic.     

湖北宜昌石板溪金矿区断层空间结构及其控矿规律研究

断层空间结构包括变形结构和几何结构两部分。本文在解析石板溪金矿区主要断层变形结构和几何结构的基础上，探讨了其空间结构模式和控矿规律。     

冈底斯明则-程巴斑岩-夕卡岩型Mo-Cu矿床成矿时代与含矿岩石成因

冈底斯东南缘克鲁-冲木达矿带以发育渐新世斑岩-夕卡岩型Mo-W-Cu成矿作用而有别于冈底斯中新世斑岩-夕卡岩型Cu-Mo-Au矿带,但是对渐新世成矿岩石类型及成因以及渐新世与中新世斑岩成矿作用存在差异的原因尚不清楚,严重制约了该带矿产资源潜力评价.为此,本文选择矿带内程巴斑岩型Mo矿床及明则夕卡岩型Cu矿床开展了成岩与成矿年代学及含矿岩石成因研究.明则矿区与夕卡岩矿化有关的二长岩的结晶年龄为30.4±0.6Ma,表明夕卡岩矿化时代约30Ma,这与程巴斑岩型Mo矿床矿石中辉钼矿Re-Os同位素分析所揭示的约30Ma矿化时代一致.明则二长岩的SiO2含量为55％ ～57％,K2O含量为2.7％ ～5.0％,属于钾玄岩,具有较高的MgO含量(3.5％～6.9％)、Mg#值(57.6～67.2)以及相容元素含量(Cr =34×10-6 ～379×10-6;Ni为48×10-6～116×10-6).而程巴花岗闪长岩的SiO2含量为65％ ～ 67％,K2O含量为3.2％～4.1％,属于高钾钙碱性岩,具有较低的MgO含量(1.7％～2.1％)、Mg#值(49.5～51.1)以及相容元素含量(Cr =20×10-6～39×10-6;Ni为16×10-6 ～25×10-6).二长岩和花岗闪长岩均显示富集轻稀土元素与大离子亲石元素,亏损高场强元素,具有弱的Eu负异常,但二长岩的REE含量明显高于花岗闪长岩,且具有较低的Sr/Y比值(24 ～49),后者Sr/Y比值为54～68.两种岩石均具有类似的Hf同位素组成,二长岩的εHf(t)值为+2.8～+6.8,花岗闪长岩εHf(t)值为+4.2～ +6.1.综合分析表明,二长岩是受大洋板片流体交代的富集岩石圈地幔部分熔融的产物,而花岗闪长岩是增厚的新生下地壳部分熔融的产物,二者在形成过程中可能发生了幔源镁铁质岩浆与壳源长英质岩浆的混合作用,这种壳幔相互作用导致区域斑岩-夕卡岩型Cu-Mo矿化,但由于该区隆升剥蚀强烈,上部的斑岩型Cu矿体基本被剥蚀而没有保存下来,因此现今表现为斑岩型Mo矿床.     

A Mössbauer study of pseudotachylytes: redox conditions during seismogenic faulting

The redox conditions during frictional melting provide information on the physical and chemical conditions during seismic slip in the crust. Here we examine frictional melts from five localities by analyzing host rocks and corresponding pseudotachylytes using Mössbauer spectroscopy. The faults examined are located at South Mountain, Arizona; Fort Foster, Maine (two localities); Long Ridge fault, North Carolina; and the Homestake shear zone, Colorado. The main iron-bearing phases in the pseudotachylytes are phyllosilicates (biotite, muscovite and clays) and iron oxides (magnetite and hematite) and minor pyrite. The ferrous/ferric ratios of the phyllosilicates in the host rocks are the same as those in the pseudotachylytes, except for the hematite-bearing pseudotachylyte from the Long Ridge fault, which is more oxidized. The magnetites in the host rocks and the corresponding pseudotachylytes have different ferric and ferrous iron distributions, which is attributed to different cation chemistry, rather than redox conditions. With the exception of the South Mountain locality, the ferric/ferrous ratios of the micas are interpreted to record the primary redox state of the pseudotachylyte melt as the calculated oxygen fugacities are consistent with magnetite and hematite equilibria. Pyrite-bearing pseudotachylytes plot ~0–1 log₁₀ units above the fayalite-magnetite-quartz (FMQ) buffer. Magnetite-bearing pseudotachylytes plot ~2–4 log₁₀ units above the FMQ buffer, and hematite-bearing pseudotachylytes plot 3.5 log₁₀ units above the hematite-magnetite (HM) buffer. Hematite-bearing pseudotachylytes, together with previous oxygen isotope data, are inferred to represent melting in the presence of externally derived pressurized water. Other localities are inferred to represent melting under rock-buffered, closed system, conditions. If the localities studied are representative of seismogenic faulting, the calculated oxygen fugacities indicate that, in the system C–O–H–S, H₂O and CO₂ should be the dominant fluid species. This is the first detailed study of the redox state of pseudotachylytes.