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1.
对2004年苏门答腊-安达曼岛地震的测地学机制讨论   总被引:1,自引:0,他引:1  
杨志根 《天文学进展》2007,25(3):270-278
采用GPS测地学观测资料,基于NUVEL-1A板块运动模型,分别估计和讨论了INDI板块与Burma微板块之间、AUST板块与Burma/SE EURA板块之间的聚敛率,以及INDI与AUST板块间的相对速率。结果显示,沿苏门答腊-尼科巴群岛和沿安达曼群岛两个阶段的地壳破裂分别与AUST板块和Burma板块间、INDI板块和Burma板块间的聚敛率密切相关,从板块运动学角度提供了解释整个苏门答腊-安达曼群岛地壳破裂带上板块间耦合由南向北递减观测结论的佐证;在NUVEL-1A板块运动模型的背景下,2004年苏门答腊-安达曼岛主震应当为AUST板块相对于Burma/SE EURA板块以近60 mm/a,方向NE 30°~35°的运动所致,而非INDI板块或印-澳(INDI-AUST)板块运动所致;根据2004年苏门答腊-安达曼岛地壳破裂特征并结合其余震的分布,进一步肯定了AUST板块西北边界带的地质位置分布。  相似文献   

2.
云南天文台抚仙湖老鹰地太阳观测基地处于小江断裂带两侧分支的控制之下,但该基地址点的地质构造未见断裂错动.址点之东5000m,北1000m,南1500m,P1-P2β-C等地层未见缺失,组成由P2β玄武岩为核,P1、c等地层为翼的向斜构造.因此,该地块是断裂带中相对稳定的地质小块体,址点的地层为P1虎斑状灰岩、白云岩夹白云质灰岩是溶蚀岩层.应注意和防范抚仙湖水体的浪蚀对石灰岩本体的溶蚀等潜在的地质缺陷.虽说抚仙湖老鹰地太阳观测基地所处地块是地震活动带中相对稳定的地质块体,但它不能脱离小江断裂带西侧分支的控制,因此,在基建规划和实施中应作抗Ⅷ度地震的技术防范.  相似文献   

3.
观测角     
12月3日水星西大距今年水星共有3次酉大距(4月16日、8月14日和12月3日),以12月3日这次大距对观测最为有利。这是因为水星的赤纬高于太阳的赤纬,水星在日出时地平高度较高,利于观测。对于北京(地理纬度40°N)纬度的地区来说,日出时(北京时间7时04分),水星的地平高度近于20°,方位角为东偏南约40°。而水星升出地平的时刻为北京时间5时37分。晨光始的时刻为6时34分。日出前可见水星的时间较久。地理纬度越高,可见条件越好,地理纬度越低,日出前可见水星时间越短。12月14日双子座流星雨极盛12月7日~18日双子座流星雨出现,14日…  相似文献   

4.
目前决定射电活动星系核Doppler因子δ的方法,主要是用均匀球状源模型的同步自康普顿机制(SSC)关联射电和X射线(或光学)波段各一点的流量来定出δ.观测表明,此方法有较大的不足.本文发展了一种新方法,一方面将SSC机制推广到非均匀情况,另一方面是用谱拟合代替点计算.我们首次用这种方法对3C273的Doppler因子进行了推算.计算结果表明,3C273的多普勒因子δ~313.在假设喷流中非均匀成分和喷流整体的运动速度相同时,得到相对论性束流运动方向与视向的夹角θ~15°.根据δ定出源的内禀亮温度约为50×1010K,缓解了“康普顿灾变”的困难.由于非均匀模型比均匀模型更接近射电活动星系核中心致密子源的真实物理图象,有关参数由3C273的同时性和准同时性多波段观测定出,观测结果对SSC机制提供了较好的支持,故理论和观测相符,由此确定的多普勒因子是更可信的.  相似文献   

5.
利用视向速度资料和依巴谷星表的自行资料,研究了经典造父变星的银河系运动学问题.采用Ogorodnikov-Milne三维运动学模型,获得银河系旋转速度V0=240.5±10.2km/s(取太阳至银心距离为8.5kpc)同时发现,在太阳附近沿银河系旋转方向存在一种收缩运动,其值((V(/(()/R=-2.60±1.07kms-1kpc-1.本文分析了产生这种收缩运动的原因.另外,得出太阳运动速度S=18.7±0.86km/s向点=54.4°±2.9°=+26.6°±2.6°  相似文献   

6.
以地球平极长期漂移的观测值为约束 ,基于地球上 8个冰盖的参数 ,调整并得到南极冰盖的地面质心位置可能不在南极点 ,而是位于余纬 16 8°~ 170°、东经 78°~ 82°附近。表明南极冰盖参数的改变对平极长期漂移方向的影响是灵敏的 ,对冰期后地壳反弹引起的地球自转主惯性张量有约 1.4 %的相对影响。采用全球冰盖参数和修正的南极冰盖参数估计得到平极长期漂移的方向为西经78° .3,比作者等人 2 0 0 1年得到的理论平极长期漂移方向为西经 74° .8的结果可能更接近于实测。估计表明 ,地球上其它 2 9个小冰盖的冰融事件引起的冰期后地壳反弹对地球平极的长期漂移和地球自转速率长期变化的综合影响在目前的天文观测精度下仍可以忽略。  相似文献   

7.
报告了在埃及赛路姆观测到的2006年3月29日日全食白光偏振测量的基本结果.我们使用的是一架便携式反射望远镜,焦距为640mm(F/D=8).在物镜前方安置可旋转线偏振片,每次旋转角度45°,终端为尼康数码相机.观测过程中,改变曝光时间并旋转偏振片,总共获取20张数码照片.文中讨论并呈现了介于 1.3 R⊙<r <3.0 R⊙范围内的白光偏振方向和偏振度的大小分布.  相似文献   

8.
土星的季节     
地球的自转轴与其绕日轨道面垂直方向的偏离,即黄赤交角(以下称“倾角”)为23°.5。地球白转与公转运动的结合产生了地球上的昼夜交替、四季变化和五带(热带、南北温带和南北寒带)的区分。虽然土星的赤道面与其绕日轨道面的交角与地球的相近,为26°.7,但各个季节的天数要比地球上相应的季节长得多,这是因为土星的公转周期为地球的29.5倍。  相似文献   

9.
介绍了差分VLBI技术确定空间飞行器位置的原理。在上海、乌鲁木齐和昆明站开展了对地球同步卫星的首次国内差分VLBI观测 ,实验中选择 3颗角距小于 15°的ICRF射电源作为参考源 ,克服了卫星观测的特殊性带来的困难 ,成功地获得了卫星信号的干涉条纹。基于条纹拟合的结果和系统差分析 ,估计双差单向测距的总误差约为 4 1cm ,双差单向测速的总误差约为 0 .14 8mm/s,相当于在地球同步轨道上 8m的位置误差和 2 .8mm/s的速度误差  相似文献   

10.
基于冰期后地壳反弹理论,采用地球上4个最大冰帽的参数,计算了最近21000年以来冰帽的融化对地球惯性张量的影响,得到理论和长期极移方向为西经74°2。现代空间测地技术的观测结果表明,关美板块不存在明显的北向运动,所以国际上9个纬度观测序列的平纬近80年的长期变化存在着随经度的系统性分布尚不能得到很好解释.,变化研究给出3-4mas/a的长期极移结果有等进一步证实。  相似文献   

11.
We calculate the H and CaII K profiles under different velocity models with chromospheric condensations and investigate the effect of the velocity in different layers on the profiles from a semi-empirical standpoint. The results show that the short-time, H blue asymmetry in the early stage of the flare can be caused by condensations in the transition zone, that the subsequent red asymmetry is the result of the downward motion of matter in the upper chromosphere, while the later CaII K asymmetries can be explained by downward velocities of 10–20 km/s in the middle and lower chromosphere.  相似文献   

12.
We study central collisions between millimeter-sized dust projectiles and centimeter-sized dust targets in impact experiments. Target and projectile are dust aggregates consisting of micrometer-sized SiO2 particles. Collision velocities range up to 25 m/s. The general outcome of a collision strongly depends on the impact velocity. For collisions below 13 m/s rebound and a small degree of fragmentation occur. However, at higher collision velocities up to 25 m/s approximately 50% of the mass of the projectile rigidly sticks to the target after the collision. Thus, net growth of a body is possible in high speed collisions. This supports the idea that planetesimal formation via collisional growth is a viable mechanism at higher impact velocities. Within our set of parameters the experiments even suggest that higher impact velocities might be preferable for growth in collisions between dusty bodies. For the highest impact velocities most of the ejecta is within small dust aggregates about 500 μm in size. In detail the size distribution of ejected dust aggregates is flat for very small particles smaller than 500 μm and follows a power law for larger ejected dust aggregates with a power of −5.6±0.2. There is a sharp upper cut-off at about 1 mm in size with only a few particles being slightly larger. The ejection angle is smaller than 3° with respect to the target surface. These fast ejecta move with 40±10% of the impact velocity.  相似文献   

13.
Paper XIII of this series presented radial velocities for 406 stars in certain of the Clube Selected Areas, a set of areas systematically arranged in Galactic coordinates. We now complete the survey by providing the radial velocities, mostly obtained at the European Southern Observatory (ESO), of 625 stars in the six southernmost Areas. Each star has been measured at least twice; the mean velocities have standard errors typically of 0.2–0.3 km s−1. Additional observations made from Haute-Provence of many of the stars that are observable from there have helped to identify, and in some instances to characterize, the ∼70 spectroscopic binaries discovered in this programme. The final results of the programme, complementing those given in table 3 of Paper XIII, are summarized in Table 12 , which presents the mean velocities and velocity dispersions in the six southern Areas. It is noted that the difference between Paper XIII and this one as regards the provenance of the radial velocities has led to a small difference in zero-points, which is discussed in Section 3 and needs to be taken into account in any analysis of the combined data.  

  Table 12.  Synopsis of radial-velocity results – mean velocities and velocity dispersions by Area.  相似文献   


14.
Upcoming surveys for galaxy clusters using the Sunyaev–Zel'dovich effect are potentially sensitive enough to create a peculiar velocity catalogue. The statistics of these peculiar velocities are sensitive to cosmological parameters. We develop a method to explore parameter space using N -body simulations in order to quantify dark matter halo velocity statistics which will be useful for cluster peculiar velocity observations. We show that mass selection bias from a kinetic Sunyaev–Zel'dovich velocity catalogue forecasts rms peculiar velocities with a much more complicated  Ωm  dependency than suggested by linear perturbation theory. In addition, we show that both two-point functions for velocities disagree with linear theory predictions out to  ∼40  h −1 Mpc  separations. A pedagogical appendix is included developing linear theory notation with respect to the two-point peculiar velocities functions.  相似文献   

15.
Chromospheric line-of-sight velocities are investigated in a small pore and its vicinity on the part of the active region NOAA 11024 with a size of 5″. We used Hα spectra of the active region and undisturbed atmosphere obtained with the French–Italian solar telescope THEMIS (Tenerife, Spain). Significant line-of-sight velocity time variations are found. At the beginning of the observations, the investigated region consisted of two areas of oppositely directed flows. The first area had a bright point in the vicinity of the pore and the second area covered the pore. There were upflows in the former and downflows in the latter. Oppositely directed flows appeared in both areas 2.7 min after the start of observations. In the part of the active region with a length of 2Mm, two oppositely directed flows within the same resolution elements, the so-called dual flows, were observed. The size of the area occupied by the dual flows varied quickly. The area shifted toward the pore. The velocity of upflows and downflows reached 25 km/s. The downflows in the first area lasted only for approximately 1 min. Upflows in the second area gradually covered the pore and lasted for 2 min. The resulting velocity field distribution can be due to a new small-scale magnetic flux emergence.  相似文献   

16.
Assuming that the orientation of a pulsar’s velocity vector is parallel to its spin axis, we have calculated the space velocities of 61 pulsars from their tangential velocities. The mean space velocity of the sample is equal to 267 km s-1. The radial velocities and kinematical ages of 20 pulsars are obtained. The decay time of the magnetic field of pulsars is τD = 2 Myr, smaller than previously found  相似文献   

17.
Previous observations of spatially-resolved vertical velocity variations in ten lines of Fe i spanning the height range 0 h 1000 km are re-analyzed using velocity weighting functions. The amplitudes and scale heights of granular and oscillatory velocities are determined, as well as those of the remaining unresolved velocities. I find that the optimal representation of the amplitude of the outward-decreasing granular velocities is an exponentially decreasing function of height, with a scale height of 150 km and a velocity at zero height of 1.27 km s–1. The optimal representation of the same quantities for oscillatory velocities is an exponential increase with height, with a scale height of 1100 km and a velocity at zero height of 0.35 km s–1. The remaining unresolved velocities decrease with height, with a scale height of 380 km and a velocity at zero height of 2.3 km s–1.  相似文献   

18.
Sunspots block the flow of energy to the solar surface. The blocked energy heats the volume beneath the spot, producing a pressure excess which drives an outflow of mass. Linear numerical models of the mass and energy flow around spots were constructed to estimate the predictions of this physical picture against the observed properties of sunspot bright rings and moat flows. The width of the bright ring and moat are predicted to be proportional to the depth of the spot penumbra, in conflict with the observed proportionally of the moat width to the spot diameter. Postulating that spot depths are proportional to spot diameters would bury the moat flow too deeply to be observed, because the radial velocity at the surface is found to be inversely proportional to the depth of the spot penumbra. The radial velocity at the surface is of order a few hundred meters per second after 1 day, in agreement with the observed excess of moat velocities over supergranule velocities.  相似文献   

19.
A. Khlystova 《Solar physics》2013,284(2):343-361
The dynamics of horizontal plasma flows during the first hours of the emergence of active region magnetic flux in the solar photosphere have been analyzed using SOHO/MDI data. Four active regions emerging near the solar limb have been considered. It has been found that extended regions of Doppler velocities with different signs are formed in the first hours of the magnetic flux emergence in the horizontal velocity field. The flows observed are directly connected with the emerging magnetic flux; they form at the beginning of the emergence of active regions and are present for a few hours. The Doppler velocities of flows observed increase gradually and reach their peak values 4?–?12 hours after the start of the magnetic flux emergence. The peak values of the mean (inside the ±?500 m?s?1 isolines) and maximum Doppler velocities are 800?–?970 m?s?1 and 1410?–?1700 m?s?1, respectively. The Doppler velocities observed substantially exceed the separation velocities of the photospheric magnetic flux outer boundaries. The asymmetry was detected between velocity structures of leading and following polarities. Doppler velocity structures located in a region of leading magnetic polarity are more powerful and exist longer than those in regions of following polarity. The Doppler velocity asymmetry between the velocity structures of opposite sign reaches its peak values soon after the emergence begins and then gradually drops within 7?–?12 hours. The peak values of asymmetry for the mean and maximal Doppler velocities reach 240?–?460 m?s?1 and 710?–?940 m?s?1, respectively. An interpretation of the observable flow of photospheric plasma is given.  相似文献   

20.
Balthasar  H.  Schmidt  W.  Wiehr  E. 《Solar physics》1997,171(2):331-336
Penumbral line-core shifts at different heights are determined from the lines Fei 5434.5 Å, Fei 5435.2 Å, and Nii 5435.8 Å using two adjacent water vapor lines for an absolute wavelength scale. The large granular blue shift of 0.6 km s-1 for the faint Fe 5435 line from deep layers yields for the centre-side penumbra absolute velocities up to 3 km s-1. This value is much larger than velocities deduced from the bisectors of the line wings of Ni 5436 and Fe 5434, thus supporting the concern against an interpretation of the line asymmetries in term of a velocity gradient with depth.  相似文献   

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