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Gravitational energy changes of planet earth under mass perturbations

Chao, Benjamin F., Gao, Chunchun, and Li, Zhen, 2026. Gravitational energy changes of planet earth under mass perturbations. Journal of Geodesy, 100(6):46, doi:10.1007/s00190-026-02065-6.

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@ARTICLE{2026JGeod.100...46C,
       author = {{Chao}, Benjamin F. and {Gao}, Chunchun and {Li}, Zhen},
        title = "{Gravitational energy changes of planet earth under mass perturbations}",
      journal = {Journal of Geodesy},
     keywords = {Gravitational energy, Multipole expansion, Eulerian density anomaly, Lagrangian deformation, GRACE},
         year = 2026,
        month = jun,
       volume = {100},
       number = {6},
          eid = {46},
        pages = {46},
     abstract = "{The gravitational energy E$_{g}$ plays a deciding role in the
        thermodynamic evolution of planet Earth in the destination of
        seeking the lowest energy configuration. This paper examines
        E$_{g}$ and its changes {\ensuremath{\Delta}}E$_{g}$ due to
        geophysical mass perturbations. We derive the multipolar
        partitioning of E$_{g}$ based on the gravitational multipole
        expansion formalism, thereby study {\ensuremath{\Delta}}E$_{g}$,
        a quantity quadratic in dependence on density, due to
        perturbations of two distinct forms: (i) Eulerian density
        anomaly, and (ii) Lagrangian deformation. Perturbation (i)
        carries a negative {\ensuremath{\Delta}}E$_{g}$ relative to the
        laterally mean configuration from which the density anomaly is
        referenced. We calculate the surficial upper bound of this
        {\ensuremath{\Delta}}E$_{g}$ with GRACE-observed time-variable
        Stokes coefficients for the Earth, where we find a present-day
        \raisebox{-0.5ex}\textasciitilde 3 GW secular increase in
        Earth's (non-quadrupolar) E$_{g}$ superposed on seasonal and
        interannual undulations. Any monopolar
        {\ensuremath{\Delta}}E$_{g}$, however, is oblivious to external
        gravitational observations given the non-uniqueness of the
        gravitational inversion. Perturbation (ii) carries a positive
        {\ensuremath{\Delta}}E$_{g}$ relative to the unperturbed
        configuration of equilibrium, hence is by itself unfavored
        energy-wise. Case in point is the spin-induced ``oblating''
        process resulting in the planet's polar oblateness, which can
        happen spontaneously upon the accompanying, over-compensating
        decrease in the spin kinetic energy under the conservation of
        angular momentum.}",
          doi = {10.1007/s00190-026-02065-6},
       adsurl = {https://ui.adsabs.harvard.edu/abs/2026JGeod.100...46C},
      adsnote = {Provided by the SAO/NASA Astrophysics Data System}
}

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