Turbulent viscosity and Λ-effect from numerical turbulence models

Homogeneous anisotropic turbulence simulations are used to determine off-diagonal components of the Reynolds stress tensor and its parameterization in terms of turbulent viscosity and Λ-effect. The turbulence is forced in an anisotropic fashion by enhancing the strength of the forcing in the vertical direction. The Coriolis force is included with a rotation axis inclined relative to the vertical direction. The system studied here is significantly simpler than that of turbulent stratified convection which has often been used to study Reynolds stresses. Certain puzzling features of the results for convection, such as sign changes or highly concentrated latitude distributions, are not present in the simpler system considered here. (© 2007 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim)     

陨石的矿物-岩石学特征及其分类

根据陨石的矿物岩石学特征、化学组成及结构可划分为球粒陨石及非球粒陨石质陨石两大类。球粒陨石进一步划分为碳质球粒陨石族(CI,CM,CO,CR,CB,CH,CV及CK球粒陨石)、普通球粒陨石族(H,L,LL球粒陨石)、顽辉石球粒陨石族(EH及EL球粒陨石)、R及K球粒陨石群,而非球粒陨石质陨石进一步划分为原始的无球粒陨石族(Acpulcoites,Lodranites,Wi nonaites,IAB硅酸盐包体及IIICD硅酸盐包体)和分异的陨石族。分异的陨石族包括:无球粒陨石(Angrites,Aubrites,Branchinites,橄辉无球粒陨石,HED灶神星陨石,SNCO火星陨石及月球陨石);石铁陨石(中铁陨石及橄榄陨铁);铁陨石(IAB,IC,IIAB,IIC,IID,IIE,IIIAB,IIICD,IIIE,II IF,IVA及IVB铁陨石化学群)。每一陨石族或陨石群,具有类似的成因或形成历史,并来自同一小行星体或行星体,藉此可建立不同陨石族或陨石群之间的成因联系,并可提供早期太阳星云的物理化学条件及其演化的信息。     

横向载荷作用下刚性桩变位规律研究

目前对横向受载刚性桩的研究主要集中在其承载力方面,对变化规律研究很少。为此提出了利用刚性桩上两点位移求桩上任意一点位移、桩回转中心位置及转角的方法。通过对粉质黏土中的刚性桩进行模型试验与数值计算发现,回转中心位置随位移和载荷的增大,先是急剧下降,然后变缓,最后基本趋于稳定,而且桩埋置参数与土力学参数对回转中心位置的变化规律影响很小;而桩的转角随位移增大近似线性变化。比较发现,由试验和数值计算得到的回转中心极限位置与由极限地基反力法得到的结果相差不大     

The angular momentum transport in rotating turbulent convection

The angular momentum transport in rotating turbulent convection is simulated with the NIRVANA code for Taylor numbers up to 10⁶. The box consists of an unstable layer embedded in two stable overshoot layers. We find the expected anisotropies in the rotating anisotropic turbulence field: 〈u^′2_r〉 exceeds 〈u^′2_ϕ〉, and 〈u^′2_ϕ〉 exceeds 〈u^′2_θ〉. The resulting radial angular momentum transport is directed inwards and peaks in the middle of the convective layer. The resulting latitudinal angular momentum transport is equatorwards, peaks at the surface and is highly concentrated to the equatorial region. Apart from a factor of 2–3 the total amplitudes of the cross‐correlations are of the same order of magnitude. In the lower overshoot region (‘tachocline’) the cross‐correlations are negative. It is argued that the concentration of the latitudinal angular momentum transport towards the surface and towards the equator does not too strongly reduce its potential to produce rotation laws with accelerated equators. (© 2005 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)     

硼同位素及其地质应用研究

硼的两个稳定同位素（10B 和11B）相对质量差较大,因此,硼同位 素分馏较显著。由于分析测量技术方面的改进和创新, 硼同位素地球化学近年来有了长足 的发展。业已查明,自然界中δ11B值变化为 －37‰～+58‰。其中,较负的 δ11B值见于非海相蒸发硼酸盐矿物和某些电气石,而较正的δ11B值见 于某些盐湖卤水和蒸发海水。现代大洋水的δ11B值十分恒定 (+39,5‰)。原始 地幔的δ11B值估测为－10‰±2‰。陨石的δ11B值很不均一,变化 可达90‰。而月岩的δ11B值变化较小（－6‰～+4‰）。由于硼同位素存在大的 分馏和不同地质体中截然不同的δ11B值,硼同位素地质应用范围十分广泛。目 前,硼同位素在研究星云形成过程和宇宙事件,壳-幔演化和板块俯冲作用过程,判别沉积 环境,研究矿床成因,示踪古海洋和古气候条件,和判断环境污染源区等方面的研究中成效显著。     

The temporal variation of the spherical and Cartesian multipoles of the gravity field: the generalized MacCullagh representation

 The Cartesian moments of the mass density of a gravitating body and the spherical harmonic coefficients of its gravitational field are related in a peculiar way. In particular, the products of inertia can be expressed by the spherical harmonic coefficients of the gravitational potential as was derived by MacCullagh for a rigid body. Here the MacCullagh formulae are extended to a deformable body which is restricted to radial symmetry in order to apply the Love–Shida hypothesis. The mass conservation law allows a representation of the incremental mass density by the respective excitation function. A representation of an arbitrary Cartesian monome is always possible by sums of solid spherical harmonics multiplied by powers of the radius. Introducing these representations into the definition of the Cartesian moments, an extension of the MacCullagh formulae is obtained. In particular, for excitation functions with a vanishing harmonic coefficient of degree zero, the (diagonal) incremental moments of inertia also can be represented by the excitation coefficients. Four types of excitation functions are considered, namely: (1) tidal excitation; (2) loading potential; (3) centrifugal potential; and (4) transverse surface stress. One application of the results could be model computation of the length-of-day variations and polar motion, which depend on the moments of inertia. Received: 27 July 1999 / Accepted: 24 May 2000     

1966～1976年华北地震的时间特性及相关触发因素

阐述了１９６６～１９７６年华北地震的时间特性及其相关触发因素－－地球自转和引潮力。这是３００年来华北地区发生的最强烈的一组地震,强震发生的时间有一个共同的特性;在年尺度上大多数地震发生在季节性地球自转速度极在值或极小值时间点附近,即极点附近（或称极点时段）,在月惊工上多数地震发生在朔望附近（或称朔望时段）,在日尺度上半数地震发生在极大水平引潮力时刻附近。表明这些地震与地球自转和日月引潮力关系密切。     

从亚洲大陆块体拼贴过程看大陆造山带的形成与演化

本文就亚洲大陆喜马拉雅造山带和大别-苏鲁造山带构造演化模式进行详细评述,并据大地构造学和古地磁学最新研究成果讨论并总结大陆造山带形成与演化模式,即大陆碰撞造山带的演化可能涉及以下5个连续的过程: 碰撞旋转拼合陆内挤压反弹.     

Tectonics of the Laptev Sea – Moma `Rift' Region: Investigation with Seismologic Broadband Data

Based on teleseismic broadband data, mainly recorded from stationsof the Incorporated Research Institute for Seismology (IRIS) and theGräfenberg (GRF) array in Germany, the focal mechanism and thefocal depth of the largest earthquakes in northeastern Siberia in thetime interval 1976–1996 were determined. For 9 events the relativeanelastic attenuation of the shear wave with respect to the compressionalwave along the travel paths could be calculated. Using the slip vectorsfrom the best constrained focal mechanisms and additional slip vectorsfrom Jemsek et al. (1986) and Parfenov et al. (1988), we obtained the North American–Eurasian pole of rotation west of the Cherskii mountainsat 67.1^° N, 132.3^° E.The investigation shows that the extension of the Arctic Mid-Ocean Ridgeinto the continental shelf acts as a continental graben structure.Actually, the crustal extension is concentrated on the eastern LaptevSea area and the seismicity of the western part of the Laptev Sea canbe explained by the assumption of a separate microplate. In the continentsoutheast of the Laptev Sea a series of northwest trending depressions,known as the Moma `Rift', are observed. Although in this region elevatedheat flow, recent volcanism and a low crustal thickness were found (i.e.Duchkov and Sokolova, 1985; Devyatkin, 1985), there is only a poorcorrelation between the seismicity and the rift valleys. So the Momastructures seem to be related to an aborted rift structure.     

RECORD OF BLOCK ROTATION AND MAGNETIC FIELD REVERSALS IN THE TETHYAN HIMALAYA (HIDDEN VALLEY, CENTRAL NEPAL)

RECORD OF BLOCK ROTATION AND MAGNETIC FIELD REVERSALS IN THE TETHYAN HIMALAYA (HIDDEN VALLEY, CENTRAL NEPAL)