The earth’s gravity field recovery using the third invariant of the gravity gradient tensor from GOCE

Abstract Due to the independence of the gradiometer instrument’s orientation in space, the second invariant $$I_2$$ I 2 of gravity gradients in combination with individual gravity gradients are demonstrated to be valid for gravity field determination. In this contribution, we develop a novel gravity...

Descripción completa

Guardado en:
Detalles Bibliográficos
Autores principales: Lin Cai, Xiaoyun Wan, Houtse Hsu, Jiangjun Ran, Xiangchao Meng, Zhicai Luo, Zebing Zhou
Formato: article
Lenguaje:EN
Publicado: Nature Portfolio 2021
Materias:
R
Q
Acceso en línea:https://doaj.org/article/d7e9233dd8bc448d9ab3f0dae340d794
Etiquetas: Agregar Etiqueta
Sin Etiquetas, Sea el primero en etiquetar este registro!
id oai:doaj.org-article:d7e9233dd8bc448d9ab3f0dae340d794
record_format dspace
spelling oai:doaj.org-article:d7e9233dd8bc448d9ab3f0dae340d7942021-12-02T14:11:29ZThe earth’s gravity field recovery using the third invariant of the gravity gradient tensor from GOCE10.1038/s41598-021-81840-12045-2322https://doaj.org/article/d7e9233dd8bc448d9ab3f0dae340d7942021-02-01T00:00:00Zhttps://doi.org/10.1038/s41598-021-81840-1https://doaj.org/toc/2045-2322Abstract Due to the independence of the gradiometer instrument’s orientation in space, the second invariant $$I_2$$ I 2 of gravity gradients in combination with individual gravity gradients are demonstrated to be valid for gravity field determination. In this contribution, we develop a novel gravity field model named I3GG, which is built mainly based on three novel elements: (1) proposing to utilize the third invariant $$I_3$$ I 3 of the gravity field and steady-state ocean circulation explorer (GOCE) gravity gradient tensor, instead of using the $$I_2$$ I 2 , similar to the previous studies; (2) applying an alternative two-dimensional fast fourier transform (2D FFT) method; (3) showing the advantages of $$I_3$$ I 3 over $$I_2$$ I 2 in the effect of measurement noise from the theoretical and practical computations. For the purpose of implementing the linearization of the third invariant, this study employs the theory of boundary value problems with sphere approximation at an accuracy level of $$O(J_2^2\cdot T_{ij})$$ O ( J 2 2 · T ij ) . In order to efficiently solve the boundary value problems, we proposed an alternative method of 2D FFT, which uses the coherent sampling theory to obtain the relationship between the 2D FFT and the third invariant measurements and uses the pseudo-inverse via QR factorization to transform the 2D Fourier coefficients to spherical harmonic ones. Based on the GOCE gravity gradient data of the nominal mission phase, a novel global gravity field model (I3GG) is derived up to maximum degree/order 240, corresponding to a spatial resolution of 83 km at the equator. Moreover, in order to investigate the differences of gravity field determination between $$I_3$$ I 3 with $$I_2$$ I 2 , we applied the same processing strategy on the second invariant measurements of the GOCE mission and we obtained another gravity field model (I2GG) with a maximum degree of 220, which is 20 degrees lower than that of I3GG. The root-mean-square (RMS) values of geoid differences indicates that the effects of measurement noise of I3GG is about 20% lower than that on I2GG when compared to the gravity field model EGM2008 (Earth Gravitational Model 2008) or EIGEN-5C (EIGEN: European Improved Gravity model of the Earth by New techniques). Then the accuracy of I3GG is evaluated independently by comparison the RMS differences between Global Navigation Satellite System (GNSS)/leveling data and the model-derived geoid heights. Meanwhile, the re-calibrated GOCE data released in 2018 is also dealt with and the corresponding result also shows the similar characteristics.Lin CaiXiaoyun WanHoutse HsuJiangjun RanXiangchao MengZhicai LuoZebing ZhouNature PortfolioarticleMedicineRScienceQENScientific Reports, Vol 11, Iss 1, Pp 1-13 (2021)
institution DOAJ
collection DOAJ
language EN
topic Medicine
R
Science
Q
spellingShingle Medicine
R
Science
Q
Lin Cai
Xiaoyun Wan
Houtse Hsu
Jiangjun Ran
Xiangchao Meng
Zhicai Luo
Zebing Zhou
The earth’s gravity field recovery using the third invariant of the gravity gradient tensor from GOCE
description Abstract Due to the independence of the gradiometer instrument’s orientation in space, the second invariant $$I_2$$ I 2 of gravity gradients in combination with individual gravity gradients are demonstrated to be valid for gravity field determination. In this contribution, we develop a novel gravity field model named I3GG, which is built mainly based on three novel elements: (1) proposing to utilize the third invariant $$I_3$$ I 3 of the gravity field and steady-state ocean circulation explorer (GOCE) gravity gradient tensor, instead of using the $$I_2$$ I 2 , similar to the previous studies; (2) applying an alternative two-dimensional fast fourier transform (2D FFT) method; (3) showing the advantages of $$I_3$$ I 3 over $$I_2$$ I 2 in the effect of measurement noise from the theoretical and practical computations. For the purpose of implementing the linearization of the third invariant, this study employs the theory of boundary value problems with sphere approximation at an accuracy level of $$O(J_2^2\cdot T_{ij})$$ O ( J 2 2 · T ij ) . In order to efficiently solve the boundary value problems, we proposed an alternative method of 2D FFT, which uses the coherent sampling theory to obtain the relationship between the 2D FFT and the third invariant measurements and uses the pseudo-inverse via QR factorization to transform the 2D Fourier coefficients to spherical harmonic ones. Based on the GOCE gravity gradient data of the nominal mission phase, a novel global gravity field model (I3GG) is derived up to maximum degree/order 240, corresponding to a spatial resolution of 83 km at the equator. Moreover, in order to investigate the differences of gravity field determination between $$I_3$$ I 3 with $$I_2$$ I 2 , we applied the same processing strategy on the second invariant measurements of the GOCE mission and we obtained another gravity field model (I2GG) with a maximum degree of 220, which is 20 degrees lower than that of I3GG. The root-mean-square (RMS) values of geoid differences indicates that the effects of measurement noise of I3GG is about 20% lower than that on I2GG when compared to the gravity field model EGM2008 (Earth Gravitational Model 2008) or EIGEN-5C (EIGEN: European Improved Gravity model of the Earth by New techniques). Then the accuracy of I3GG is evaluated independently by comparison the RMS differences between Global Navigation Satellite System (GNSS)/leveling data and the model-derived geoid heights. Meanwhile, the re-calibrated GOCE data released in 2018 is also dealt with and the corresponding result also shows the similar characteristics.
format article
author Lin Cai
Xiaoyun Wan
Houtse Hsu
Jiangjun Ran
Xiangchao Meng
Zhicai Luo
Zebing Zhou
author_facet Lin Cai
Xiaoyun Wan
Houtse Hsu
Jiangjun Ran
Xiangchao Meng
Zhicai Luo
Zebing Zhou
author_sort Lin Cai
title The earth’s gravity field recovery using the third invariant of the gravity gradient tensor from GOCE
title_short The earth’s gravity field recovery using the third invariant of the gravity gradient tensor from GOCE
title_full The earth’s gravity field recovery using the third invariant of the gravity gradient tensor from GOCE
title_fullStr The earth’s gravity field recovery using the third invariant of the gravity gradient tensor from GOCE
title_full_unstemmed The earth’s gravity field recovery using the third invariant of the gravity gradient tensor from GOCE
title_sort earth’s gravity field recovery using the third invariant of the gravity gradient tensor from goce
publisher Nature Portfolio
publishDate 2021
url https://doaj.org/article/d7e9233dd8bc448d9ab3f0dae340d794
work_keys_str_mv AT lincai theearthsgravityfieldrecoveryusingthethirdinvariantofthegravitygradienttensorfromgoce
AT xiaoyunwan theearthsgravityfieldrecoveryusingthethirdinvariantofthegravitygradienttensorfromgoce
AT houtsehsu theearthsgravityfieldrecoveryusingthethirdinvariantofthegravitygradienttensorfromgoce
AT jiangjunran theearthsgravityfieldrecoveryusingthethirdinvariantofthegravitygradienttensorfromgoce
AT xiangchaomeng theearthsgravityfieldrecoveryusingthethirdinvariantofthegravitygradienttensorfromgoce
AT zhicailuo theearthsgravityfieldrecoveryusingthethirdinvariantofthegravitygradienttensorfromgoce
AT zebingzhou theearthsgravityfieldrecoveryusingthethirdinvariantofthegravitygradienttensorfromgoce
AT lincai earthsgravityfieldrecoveryusingthethirdinvariantofthegravitygradienttensorfromgoce
AT xiaoyunwan earthsgravityfieldrecoveryusingthethirdinvariantofthegravitygradienttensorfromgoce
AT houtsehsu earthsgravityfieldrecoveryusingthethirdinvariantofthegravitygradienttensorfromgoce
AT jiangjunran earthsgravityfieldrecoveryusingthethirdinvariantofthegravitygradienttensorfromgoce
AT xiangchaomeng earthsgravityfieldrecoveryusingthethirdinvariantofthegravitygradienttensorfromgoce
AT zhicailuo earthsgravityfieldrecoveryusingthethirdinvariantofthegravitygradienttensorfromgoce
AT zebingzhou earthsgravityfieldrecoveryusingthethirdinvariantofthegravitygradienttensorfromgoce
_version_ 1718391873044742144