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71.
����IGS����������ֵ�����ıȽϷ��� 总被引:13,自引:4,他引:13
?????GPS???????????????????????????????????????????????о???????????????????????????????????????????????????????????廹?????????????????????????????????????????????????????????????????λ????????????????????????????????????о???????????????????????????????????????????????????????λ??? 相似文献
72.
利用Fortran语言编程实现了精密钟差文件的读取及信息筛选;在此基础上,利用滑动式Lagrange插值方法对精密钟差进行了加密,并对结果进行分析与讨论,得出了几点有益的结论。 相似文献
73.
不同插值方法对CORS高程时间序列的影响分析 总被引:2,自引:0,他引:2
在CORS站高程时间序列的研究中,当连续缺失较多数据时,插值显得尤为重要。为了较好地解决这个问题,本文尝试采用正交多项式拟合的方法,分别利用正交多项式拟合、拉格朗日和三次样条等插值方法对高程时间序列进行插值,并对不同方法的插值结果进行了分析比较,验证了正交多项式拟合的可行性及有效性。结果表明:在高程时间序列插值中,三次样条插值结果较差;连续缺失3个点及以下时,正交多项式拟合、拉格朗日插值结果均较好,插值效果相当;随着缺失点数量的增加,正交多项式拟合结果要优于另2种方法。 相似文献
74.
The Navier–Stokes-α equation is a regularised form of the Euler equation that has been employed in representing the sub-grid scales in large-eddy simulations. Determined efforts have been made to place it on a secure deductive foundation. This requires two steps to be completed. The first is fundamental and consists of establishing from the equations governing the fluid flow, a relationship between two velocities called by Holm (Chaos, 2002a, 12, 518) the “filtered” and “unfiltered” velocities. The second consists of the relation between these two velocities. Until now, the preferred route to the first objective has been variational, by varying the action using Hamilton's principle. Soward and Roberts (J. Fluid Mech., 2008, 604, 297) followed that variational route and established the existence of an important but unwelcome term omitted by Holm in his derivation. It is shown here that the Soward and Roberts result may be derived from Euler's equation by a direct approach with considerably greater efficiency. Holm achieved the second objective by making a “Taylor hypothesis”, which we use here to evaluate the unwelcome term missing from his analysis of the first step. The resulting model equations differ from those of Holm's α model, and the attractive mean Kelvin's circulation theorem that follows from his α equations is no longer valid. For that reason, we call the term omitted by Holm unwelcome. 相似文献
75.
���ں������˲���PPP�ྶ��������о� 总被引:1,自引:0,他引:1
????PPP???????????????????PPP??λ?????????о?????????PPP??ú????????????????????????????λ???????????????????λ??????е??????????????????????????????????????????????У????????????????÷?Χ???????????????????IGS??????????????ú???????????????????PPP?????λ???????????????????????????3???????????????69.2%??72.3%??27.6%?? 相似文献
76.
77.
D. Nesvorný F. Thomas S. Ferraz-Mello A. Morbidelli 《Celestial Mechanics and Dynamical Astronomy》2002,82(4):323-361
We develop a formalism of the non-singular evaluation of the disturbing function and its derivatives with respect to the canonical variables. We apply this formalism to the case of the perturbed motion of a massless body orbiting the central body (Sun) with a period equal to that of the perturbing (planetary) body. This situation is known as the co-orbital motion, or equivalently, as the 1/1 mean motion commensurability. Jupiter's Trojan asteroids, Earth's co-orbital asteroids (e.g., (3753) Cruithne, (3362) Khufu), Mars' co-orbital asteroids (e.g., (5261) Eureka), and some Jupiter-family comets are examples of the co-orbital bodies in our solar system. Other examples are known in the satellite systems of the giant planets. Unlike the classical expansions of the disturbing function, our formalism is valid for any values of eccentricities and inclinations of the perturbed and perturbing body. The perturbation theory is used to compute the main features of the co-orbital dynamics in three approximations of the general three-body model: the planar-circular, planar-elliptic, and spatial-circular models. We develop a new perturbation scheme, which allows us to treat cases where the classical perturbation treatment fails. We show how the families of the tadpole, horseshoe, retrograde satellite and compound orbits vary with the eccentricity and inclination of the small body, and compute them also for the eccentricity of the perturbing body corresponding to a largely eccentric exoplanet's orbit.This revised version was published online in October 2005 with corrections to the Cover Date. 相似文献
78.
王涛 《测绘与空间地理信息》2017,40(9)
借助GPS卫星精密星历,使用Lagrange多项式插值法和Chebyshev多项式拟合法内插出GPS卫星的瞬时位置,确定了插值精度与插值阶数的关系,并对这两种方法的优缺点进行了对比分析。计算结果表明:内插卫星瞬时坐标时所选取的插值阶数不应过高或过低,三维坐标分量在最佳插值精度时选取的插值阶数并不完全相同,Chebyshev多项式拟合法相比Lagrange多项式插值法的插值效果更好。因此,建议在优先选用Chebyshev多项式拟合法内插卫星瞬时坐标的同时,对三维坐标分量分别选取不同的插值阶数,以达到最优的插值精度。 相似文献
79.
陆源污染物对连云港海域环境影响研究 总被引:6,自引:0,他引:6
应用沿深平均二维模型模拟了连云港海域的潮流场,分析了该海域的潮波特性,在此基础上,应用扩散方程对连云港海域的水污染扩散进行了数值模拟,得到了港域水体的半交换期;比较分析了西大堤对该水域水交换的影响;计算了港域水体的Lagrange余流场,并分析了其对污染物运移的影响,得到了港域几个典型位置的Lagrange轨迹;计算了港域的纳潮量,综合分析了港域水体的物理自净能力。 相似文献
80.
We present the derivation of the discrete Euler–Lagrange equations for an inverse spectral element ocean model based on the shallow water equations. We show that the discrete Euler–Lagrange equations can be obtained from the continuous Euler–Lagrange equations by using a correct combination of the weak and the strong forms of derivatives in the Galerkin integrals, and by changing the order with which elemental assembly and mass averaging are applied in the forward and in the adjoint systems. Our derivation can be extended to obtain an adjoint for any Galerkin finite element and spectral element system.We begin the derivations using a linear wave equation in one dimension. We then apply our technique to a two-dimensional shallow water ocean model and test it on a classic double-gyre problem. The spectral element forward and adjoint ocean models can be used in a variety of inverse applications, ranging from traditional data assimilation and parameter estimation, to the less traditional model sensitivity and stability analyses, and ensemble prediction. Here the Euler–Lagrange equations are solved by an indirect representer algorithm. 相似文献