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1.
基于通信卫星的导航系统可以利用比地球静止轨道(Geostationary Earth Orbit,GEO)高约200 km的倾斜高圆轨道(inclined Highly Circular Orbit,iHCO)通信卫星组成导航星座.结合两种轨道高度的倾斜高圆轨道通信卫星,仿真分析了利用倾斜高圆轨道卫星组成的中国区域定位系统(Chinese Area Positioning System,CAPS)的导航性能,并讨论了利用倾斜高圆轨道卫星组成的中国区域定位系统实现中国区域覆盖的最佳星座布局.  相似文献   

2.
中国区域定位系统(Chinese Area Positioning System,CAPS)把寿命末期的地球静止轨道(Geostationary Earth Orbit,GEO)通信卫星推到比GEO轨道高约200 km的倾斜高圆轨道(inclined Highly Circular Orbit,iHCO),卫星相对地球向西漂移。利用该类卫星组建CAPS导航星座,可以实现全球范围内的导航通信覆盖。重点开展基于iHCO通信卫星的CAPS星座优化研究,结果表明:利用GEO通信卫星和iHCO通信卫星组成的星座可以实现较好的空间星座布局,可以满足一般导航用户的需要。  相似文献   

3.
中国区域定位系统(Chinese Area Positioning System,CAPS)拟采用比地球静止轨道(Geostationary Earth Orbit,GEO)高150 km至300 km的倾斜高圆轨道(inclined Highly Circular Orbit,iHCO)通信卫星组建全球导航通信星座。基于全球范围内的卫星测控网分布情况,分析了测控站对倾斜高圆轨道卫星的可见性,提出测控站布局的优化方案,并研究了站星链路的方位角、俯仰角和距离特性。  相似文献   

4.
卫星通信是地球上无线电设备之间利用人造卫星作为中继站进行的通信。地球静止轨道(Geostationary Earth Orbit,GEO)通信卫星由于其相对地球静止的特性,被广泛应用于通信、气象、导航等领域。通信地球站是卫星通信的重要环节,准确调整接收天线的方位角、俯仰角和极化角是地面接收站有效进行通信的关键条件之一。结合线极化角的定义,研究了一种适用于地球静止轨道卫星通信的线极化角矢量计算方法,可用于指导卫星通信地球站接收天线的极化角调整。  相似文献   

5.
环火卫星运动的坐标系附加摄动及相应坐标系的选择   总被引:1,自引:0,他引:1  
与处理地球卫星相关问题类似,在研究和处理环火卫星(尤其是低轨卫星)的轨道问题时,宜采用火心历元平赤道坐标系,即火心天球坐标系,其xy坐标面和x轴方向就是相应的平赤道面和平春分点方向.与地球的岁差章动现象类似,在该坐标系中,火星赤道面在空间的摆动同样会引起坐标系附加摄动.采用类似对地球岁差章动的处理方法,在一定精度前提下,基于IAU2000火星定向模型,处理了火星赤道面摆动中的岁差效应,并在此基础上,研究岁差对环火卫星轨道的影响,给出了相应的火星非球形引力位的变化及其导致的卫星轨道的坐标系附加摄动解,其表达形式简单,引用方便.与高精度数值解的比对表明,该分析解能够满足通常的精度要求.因此,在处理环火卫星(即使是低轨卫星)轨道及其相关问题时,可以采用统一坐标系:火心天球坐标系.而不必像当初处理地球卫星那样,为了避免计算坐标系附加摄动而引进一种混合型赤道坐标系,即采用瞬时真赤道面和历元平春分点方向作为其xy坐标面和x轴方向.在统一坐标系的选择下,实际工作中就不会存在坐标系转换的麻烦.  相似文献   

6.
选用非滑动式拉格朗日(Lagrange)插值法和滑动式Lagrange插值法对北斗卫星导航系统(Beidou Satellite Navigation Syetem, BDS)精密星历进行插值,通过大量实验对北斗卫星导航系统卫星的插值精度与两种方法及插值阶次的关系进行研究。实验结果表明:(1)分别采用非滑动式和滑动式Lagrange插值时,中地球轨道卫星(Medium Earth Orbit, MEO)和倾斜地球同步轨道卫星(Inclined Geosynchronous Satellite Orbit, IGSO)的插值误差随阶次增加近似呈"U"形和"L"形分布,地球同步静止轨道卫星(Geostationary Earth Orbit, GEO)的插值误差随阶次的增加逐渐增大,并趋向于近似平稳;(2)当插值阶次较低时,两种方法的插值误差均呈现一定的规律性,但地球同步静止轨道卫星插值误差的规律性弱于中地球轨道卫星和倾斜地球同步轨道卫星;(3)各卫星采用两种方法的最优插值阶次相差均在1以内,且最佳插值阶次下,滑动式Lagrange插值精度较非滑动式可提高11.96%~44.01%,地球同步静止轨道卫星插值精度优于中地球轨道卫星和倾斜地球同步轨道卫星。  相似文献   

7.
月球物理天平动对环月轨道器运动的影响   总被引:3,自引:0,他引:3  
张巍  刘林 《天文学报》2005,46(2):196-206
月球物理天平动是月球赤道在空间真实的摆动,会导致月球引力场在空间坐标系中的变化,从而引起环月轨道器(以下称为月球卫星)的轨道变化,这与地球的岁差章动现象对地球卫星轨道的影响类似.采用类似对地球岁差章动的处理方法,讨论月球物理天平动对月球卫星轨道的影响,给出相应的引力位的变化及卫星轨道的摄动解,清楚地表明了月球卫星轨道的变化规律,并和数值解进行了比对,从定性和定量方面作一讨论.  相似文献   

8.
在我们的太阳系中有很多的卫星。其中最为著名的当属环绕地球的月亮。月亮不仅造成了地球海洋的潮汐。还为我们带来了日食和月食的壮丽景象。月亮上没有大气或海洋。生命在那里无法存在。但是我们太阳系内的其他卫星上的情形又是如何呢?而那些新发现的系外行星是否也可能拥有自己的卫星呢?  相似文献   

9.
章动与极移 地球的自转实质上是地球作为一个天体绕质心作“定点转动”,地球又与它的卫星月球一起绕太阳公转,绕地月的共同质心作旋转运动。因为地一月系统的质心在地球本体内,故使地球自转轴的方向既在空间变化,又在地球的本体内变化;空间变化表现为“章动”和“岁差”;本体变化表现为地极的迁移(如周年极移、钱德勒摆动等)。举例来说,  相似文献   

10.
针对地基卫星测控系统(Tracking Telemetry and Command, TT&C)系统对地球静止轨道(Geostation-\lk ary Earth Orbit, GEO)卫星在空间和时间覆盖上的局限性, 提出小倾角低地球轨道(Low Earth Orbit, LEO)多星组网天基平台对GEO卫星进行跟踪定轨的方法. 根据空间环境和光学可视条件对仿真数据进行筛选以模拟真实的观测场景, 利用光学测角数据, 使用数值方法对GEO卫星的轨道进行确定. 结果与参考轨道进行重叠对比, 在平台轨道精度5 m、测量精度5rq\rq、 定轨弧长12 h的情况下, 两颗LEO卫星对GEO卫星进行跟踪定轨的精度可达到千米量级, 4颗LEO卫星对GEO目标进行跟踪定轨的精度可达到百米量级. 随着LEO组网卫星数量的增加, 定轨精度得到了较大的提高.  相似文献   

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In the numerical integrations of the outer planets, when the inner planets are not considered, the initial conditions are determined by least square adjustment with a complete ephemeris. In the present work, we compute the resulting uncertainty on the initial conditions by the analysis of the very simple problem which consists in fitting by least squares a straight line to a sine curve. Explicit formulae for the computation of the error due to the fitting process are given. In particular, fitting over an integer number of periods is very close to the worst case. The determination of the initial conditions in the LONGSTOP project (Milani,et al., 1987) is analysed as an example. It is shown that the uncertainty on the main frequencies of the secular system due to the determination of the initial conditions is of the order of 0.01 arcsec/year.  相似文献   

13.
The tidal force effects of a spherical galaxy passing head-on through a disk galaxy have been studied at various regions of the disk galaxy and for various orientations of the disk galaxy with respect to the direction of relative motion of the two galaxies. The density distribution of the disk galaxy is taken to be, (r)=ce–4r/R , where c is the central density andR is the radius of the disk. The density distribution of the spherical galaxy is taken to be that of a oolytrope of indexn=4. It is found that as a result of the collision, through the central parts and the outer parts of the disk galaxy remain intact, the region in between these two regions disrupts. Thus a ring galaxy with a nucleus embedded in the ring-i.e., a ring galaxy of the RN-type, is formed.  相似文献   

14.
The star WR 7a, also known as SPH 2, has a spectrum that resembles that of V Sagittae stars although no O  vi emission has been reported. The Temporal Variance Spectrum – TVS – analysis of our data shows weak but strongly variable emission of O  vi lines which is below the noise level in the intensity spectrum.
Contrary to what is seen in V Sagittae stars, optical photometric monitoring shows very little, if any, flickering. We found evidence of periodic variability. The most likely photometric period is   P phot= 0.227(±14) d  , while radial velocities suggest a period of   P spec= 0.204(±13) d  . One-day aliases of these periods can not be ruled out. We call attention to similarities with HD 45166 and DI Cru (= WR 46), where multiple periods are present. They may be associated to the binary motion or to non-radial oscillations.
In contrast to a previous conclusion by Pereira et al., we show that WR 7a contains hydrogen. The spectrum of the primary star seems to be detectable as the N  v 4604 Å  absorption line is visible. If so, it means that the wind is optically thin in the continuum and that it is likely to be a helium main sequence star.
Given the similarity to HD 45166, we suggests that WR 7a may be a qWR – quasi Wolf–Rayet – star. Its classification is WN4h/CE in the Smith, Shara & Moffat three-dimensional classification system.  相似文献   

15.
We present a quasar model with a rotating disk and a massive nucleus. We use this model in order to characterize the motion in the model (regular or chaotic) and to connect the extent of the chaotic regions to the physical parameters of the model. Numerical experiments suggest that, there are connections between the extent of the chaotic areas and the parameters of the system. Furthermore, it is shown that the form of numerically found relationships can be expressed analytically. Comparison to previous work is also made. (© 2005 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)  相似文献   

16.
The objective of this paper is to develop a simple model of an encounter between a comet and a planet, with a subsequent capture or an escape, and to study the potential consequences. The hypothetical scenario is as follows: a comet with a conic orbit meets close to one of its vertices (located near the ecliptic plane), a jovian planet, and transforms its orbit. There are two hypotheses which are made for the shock: this vertex becomes one of the final vertices and the orbital plane of the comet is unchanged during the encounter as it was the case for Brooks 2 in 1886. In this model, it was able to find an equation which was then used to obtain the pre‐ and post‐encounter orbits elements and the kind of orbit (ellipse, hyperbola, parabola) with respect to the initial inclination. The numerical experiments with the observed comets often provide pre‐encounter orbits with an aphelion point located near another jovian planet farther from the Sun, and so on with sometimes several planets, or with an aphelion point located beyond the Pluto orbit. This revised version was published online in July 2006 with corrections to the Cover Date.  相似文献   

17.
We formulate the problem of an infinitesimal particle moving in the space under the influence of the gravitational force induced by a homogeneous annulus disk fixed on a plane. We compute using different coordinates and in terms of an elliptic integral the potential associated to this problem. Also we study the symmetries of the associated potential. After that, we look at the dynamics in some particular cases, namely: in the line perpendicular to the plane that contains the annulus disk and passes through the center of the ring and on the plane that contains the massive annulus.   相似文献   

18.
A spread in parallel beam velocity is found to have little effect on the previous results from the model by Dungey and Strangeway (1976). However, examination of the eigenfunctions for the same model indicates that perpendicular temperature may be the key to beam stability.  相似文献   

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