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Bagherbandi, Mohammad and Sjöberg, Lars E., 2025. A short note on GIA related surface gravity versus height changes in Fennoscandia. Journal of Geodesy, 99(1):2, doi:10.1007/s00190-024-01921-7.
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@ARTICLE{2025JGeod..99....2B, author = {{Bagherbandi}, Mohammad and {Sj{\"o}berg}, Lars E.}, title = "{A short note on GIA related surface gravity versus height changes in Fennoscandia}", journal = {Journal of Geodesy}, keywords = {GRACE, Gravity change, Land uplift, Gravimetry, Fennoscandia, Glacial Isostatic Adjustment, Engineering, Geomatic Engineering}, year = 2025, month = jan, volume = {99}, number = {1}, eid = {2}, pages = {2}, abstract = "{Vertical land motion and the redistribution of masses within and on the surface of the Earth affect the Earth's gravity field. Hence, studying the ratio between temporal changes of the surface gravity <inline-formula id=``IEq1''><mml:math id=``IEq1\_Math''><mml:mfenced close=``)'' open=``(''><mml:mover accent=``true''><mml:mi>g</mml:mi><mml:mo>Ë</mml:mo></mml:mover> </mml:mfenced></mml:math></inline-formula> and height (<inline- formula id=``IEq2''><mml:math id=``IEq2\_Math''><mml:mover accen t=``true''><mml:mi>h</mml:mi><mml:mo>Ë</mml:mo></mml:mover></mml :math></inline-formula>) is important in geoscience, e.g., for reduction of gravity observations, assessing satellite gravimetry missions, and tuning vertical land motion models. Sj{\"o}berg and Bagherbandi (2020) estimated a combined ratio of <inline-formula id=``IEq3''><mml:math id=``IEq3\_Math''><mml:mrow><mml:mover accent=``true''><mml:mi>g </mml:mi><mml:mo>Ë</mml:mo></mml:mover><mml:mo stretchy=``false''>/</mml:mo><mml:mover accent=``true''><mml:mi> h</mml:mi><mml:mo>Ë</mml:mo></mml:mover></mml:mrow></mml:math></ inline-formula> in Fennoscandia based on relative gravity observations along the 63 degree gravity line running from V{\r{a}}gstranda in Norway to Joensuu in Finland, 688 absolute gravity observations observed at 59 stations over Fennoscandia, monthly gravity data derived from the GRACE satellite mission between January 2003 and August 2016, as well as a land uplift model. The weighted least-squares solution of all these data was <inline-formula id=``IEq4''><mml:math id=``IEq4\_Math''><mml:mrow><mml:mover accent=``true''><mml:mi>g </mml:mi><mml:mo>Ë</mml:mo></mml:mover><mml:mo stretchy=``false''>/</mml:mo><mml:mover accent=``true''><mml:mi> h</mml:mi><mml:mo>Ë</mml:mo></mml:mover></mml:mrow></mml:math></ inline-formula> = â 0.166 {\ensuremath{\pm}} 0.011 {\ensuremath{\mu}}Gal/mm, which corresponds to an upper mantle density of about 3402 {\ensuremath{\pm}} 95 kg/m$^{3}$. The present note includes additional GRACE data to June 2017 and GRACE Follow-on data from June 2018 to November 2023. The resulting weighted least-squares solution for all data is <inline-formula id=``IEq5''><mml:math id=``IEq5\_Math''><mml:mrow><mml:mover accent=``true''><mml:mi>g </mml:mi><mml:mo>Ë</mml:mo></mml:mover><mml:mo stretchy=``false''>/</mml:mo><mml:mover accent=``true''><mml:mi> h</mml:mi><mml:mo>Ë</mml:mo></mml:mover></mml:mrow></mml:math></ inline-formula> = â 0.160 {\ensuremath{\pm}} 0.011 {\ensuremath{\mu}}Gal/mm, yielding an upper mantle density of about 3546 {\ensuremath{\pm}} 71 kg/m$^{3}$. The outcomes show the importance of satellite gravimetry data in Glacial Isostatic Adjustment (GIA) modeling and other parameters such as land uplift rate. Utilizing a longer time span of GRACE and GRACE Follow-on data allows us to capture fine variations and trends in the gravity-to-height ratio with better precision. This will be useful for constraining and adjusting GIA models and refining gravity observations.}", doi = {10.1007/s00190-024-01921-7}, adsurl = {https://ui.adsabs.harvard.edu/abs/2025JGeod..99....2B}, adsnote = {Provided by the SAO/NASA Astrophysics Data System} }
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