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Loading effect of a self-consistent equilibrium ocean pole tide on the gravimetric parameters of the gravity pole tides at superconducting gravimeter stations

机译:自洽平衡海潮对超导重力仪站重力极重力参数的影响

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The gravimetric parameters of the gravity pole tide are the amplitude factor δ, which is the ratio of gravity variations induced by polar motion for a real Earth to variations computed for a rigid one, and the phase difference κ between the observed and the rigid gravity pole tide. They can be estimated from the records of superconducting gravimeters (SGs). However, they are affected by the loading effect of the ocean pole tide. Recent results from TOPEX/Poseidon (TP) altimeter confirm that the ocean pole tide has a self-consistent equilibrium response. Accordingly, we calculate the gravity loading effects as well as their influence on the gravimetric parameters of gravity pole tide at all the 26 SG stations in the world on the assumption of a self-consistent equilibrium ocean pole tide model. The gravity loading effect is evaluated between 1 January 1997 and 31 December 2006. Numerical results show that the amplitude of the gravity loading effect reaches 10~(-9) ms~(-2), which is larger than the accuracy (10~(-10) ms~(-2)) of a SG. The gravimetric factor δ is 1% larger at all SG stations. Then, the contribution of a self-consistent ocean pole tide to the pole tide gravimetric parameters cannot be ignored as it exceeds the current accuracy of the estimation of the pole tide gravity factors. For the nine stations studied in Ducarme et al. [Ducarme, B., Venedikov, A.P., Arnoso, J., et al., 2006. Global analysis of the GGP superconducting gravimeters network for the estimation of the pole tide gravimetric amplitude factor. J. Geodyn. 41, 334-344.], the mean of the modeled tidal factors δ_m = 1.1813 agrees very well with the result of a global analysis δ_(CH) = 1.1816 ± 0.0047 in that paper. On the other hand, the modeled phase difference κ_m varies from -0.273° to 0.351°. Comparing to the two main periods of the gravity pole tide, annual period and Chandler period, κ_m is too small to be considered. Therefore, The computed time difference κ_L induced by a self-consistent ocean pole tide produces a negligible effect on κ_m. It confirms the results of Ducarme et al., 2006, where no convincing time difference was found in the SG records.
机译:重力极潮的重力参数是振幅因子δ,它是由实际地球的极地运动引起的重力变化与为一个刚性地球计算的变化之比,以及观测到的和刚性重力极之间的相位差κ浪潮。可以从超导重力仪(SGs)的记录中估算它们。但是,它们受到洋潮的载荷效应的影响。 TOPEX / Poseidon(TP)高度计的最新结果证实,海极潮汐具有自洽的平衡响应。因此,我们在假设自洽平衡洋极潮模型的前提下,计算了世界上所有26个SG站的重力载荷效应及其对重力极潮的重量参数的影响。在1997年1月1日至2006年12月31日期间对重力作用进行了评估。数值结果表明,重力作用的幅度达到10〜(-9)ms〜(-2),大于精度(10〜( SG)-10)ms〜(-2))。在所有SG站中,重量系数δ都大1%。然后,自相一致的海洋极潮对极潮重力参数的贡献不容忽视,因为它超过了目前估计的极潮重力因子的精度。对于Ducarme等人研究的9个站。 [Ducarme,B.,Venedikov,A.P.,Arnoso,J.,et al。,2006. GGP超导重力仪网络的全局分析,用于估算极潮重力重量系数。 J. Geodyn。 41,334-344。],模拟潮汐因子δ_m= 1.1813的平均值与该论文中整体分析δ_(CH)= 1.1816±0.0047的结果非常吻合。另一方面,建模的相位差κ_m在-0.273°至0.351°之间变化。与重力极潮的两个主要时期(年度时期和钱德勒时期)相比,κ_m太小,无法考虑。因此,自相一致的海极潮汐引起的计算时间差κ_L对κ_m的影响可忽略不计。它证实了Ducarme等人(2006年)的结果,在SG记录中未发现令人信服的时差。

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