The Global S1Tide
Open Access
- 1 August 2004
- journal article
- Published by American Meteorological Society in Journal of Physical Oceanography
- Vol. 34 (8) , 1922-1935
- https://doi.org/10.1175/1520-0485(2004)034<1922:tgst>2.0.co;2
Abstract
The small S1 ocean tide is caused primarily by diurnal atmospheric pressure loading. Its excitation is therefore unlike any other diurnal tide; in particular, pressure loading is maximum near the equator where the diurnal gravitational potential is zero. The global character of the S1 tide is here determined by numerical modeling and by analysis of Ocean Topography Experiment (TOPEX)/Poseidon satellite altimeter data. The two approaches yield reasonably consistent results. Amplitudes exceeding 1 cm in several regions are further confirmed by comparison with coastal tide gauges. Notwithstanding their excitation differences, S1 and other diurnal tides are found to share several common features, such as relatively large amplitudes in the Arabian Sea, the Labrador Sea, the Sea of Okhotsk, and the Gulf of Alaska. The most noticeable difference is the lack of an S1 Antarctic Kelvin wave. These similarities and differences can be explained in terms of the coherences between near-diurnal oceanic normal m... Abstract The small S1 ocean tide is caused primarily by diurnal atmospheric pressure loading. Its excitation is therefore unlike any other diurnal tide; in particular, pressure loading is maximum near the equator where the diurnal gravitational potential is zero. The global character of the S1 tide is here determined by numerical modeling and by analysis of Ocean Topography Experiment (TOPEX)/Poseidon satellite altimeter data. The two approaches yield reasonably consistent results. Amplitudes exceeding 1 cm in several regions are further confirmed by comparison with coastal tide gauges. Notwithstanding their excitation differences, S1 and other diurnal tides are found to share several common features, such as relatively large amplitudes in the Arabian Sea, the Labrador Sea, the Sea of Okhotsk, and the Gulf of Alaska. The most noticeable difference is the lack of an S1 Antarctic Kelvin wave. These similarities and differences can be explained in terms of the coherences between near-diurnal oceanic normal m...Keywords
This publication has 38 references indexed in Scilit:
- Diurnal and semidiurnal variations in global surface wind and divergence fieldsJournal of Geophysical Research: Atmospheres, 1999
- Diurnal and Semidiurnal Tides in Global Surface Pressure FieldsJournal of the Atmospheric Sciences, 1999
- Diurnal and Semidiurnal Variations of the Surface Wind Field over the Tropical Pacific OceanJournal of Climate, 1998
- Oceanic tidal angular momentum and Earth's rotation variationsProgress in Oceanography, 1997
- Diurnal/semidiurnal polar motion excited by oceanic tidal angular momentumJournal of Geophysical Research, 1996
- Energetics of global ocean tides from Geosat altimetryJournal of Geophysical Research: Oceans, 1991
- Solution of the tidal equations for the M 2 and S 2 tides in the world oceans from a knowledge of the tidal potential alonePhilosophical Transactions of the Royal Society of London. Series A, Mathematical and Physical Sciences, 1978
- Meteorology of the upper atmosphereReviews of Geophysics, 1975
- Corrected Tables of Tidal HarmonicsGeophysical Journal International, 1973
- New Computations of the Tide-generating PotentialGeophysical Journal of the Royal Astronomical Society, 1971