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Global tide - FES99

Ocean tides represent more than 80% of ocean variability. Sea level variations and consecutive currents near the coast are complicated processes; modelling pelagic and coastal tides leads to a better knowledge of this phenomena.

FES (Finite Element Solution) uses hydrodynamics computing to provide tide waves on a global scale dedicated to scientists or defence and industry communities.
Methodology is based on finite elements modelling combined with in-situ and altimetry data assimilation. Accuracy is about a few centimeters in the open ocean and a few decimeters near coastal areas.

Numerical model

Tide equation are solved on finite elements triangular grids. Unknowns (i.e slope tide velocity components) are computed on this grid.
Each grid triangular element is Lagrange P2, which means that slope is computed on the 3 vertexes and on the 3 midpoints (six nodes in total). Each velocity is computed on the 7 Gauss points. Thus we obtain interpolated velocities that we can derive to obtain node's slope. Grids are choosed to be larger on deep ocean areas and narrow on coastal areas (Le Provost et Vincent [1986] cryteria).
Finally this finite elements medel (herre called CEFMO) allow us to obtain slope values and corresponding errors on every nodes.


Tide gauges measurements are mainly located along coasts or on islands, with a period of an hour. Altimetry data's coverage is more homegeneous on the globe, but less efficient on coastal areas, with a period of several days.
Combining this two types of observations leads to a better ocean surface coverage, from coastal areas/ continental shelfs to open ocean. This data are then assimilated in previous numerical model, using representative method.


Tide gauges location. Tide gauges datasets come from WOCE (World Ocean Circulation Experiment), IAPSO (Inter-Agency Procurement Services Office) and BHI (Bureau Hydrographique International).
Altimetry crossover points selected for FES99. Altimetry data come from crossover points analysis of Topex/ Poseidon measurements.

FES99 tide waves

Representative method does not need all data (5318 crossover points in total) for the assimilation. Then a selection is made:

  • no data located out of the grid
  • no data located deeper than 200 meters: crossover analysis in not enough efficient there, wich is compensated by maregraphic data availability
  • a minimal distance (600 kilometers, ie double of distance between two T/P tracks on equator) between crossover points, so that we don't get any oversampled points.
Wave name M2 S2 N2 K2 2N2 K1 O1 Q1
Number of assimilated data 1470 1444 1323 1343 237 1584 1588 1339

FES99 provides eight primary waves (M2, S2, N2, K2, 2N2, K1, O1 and Q1) and nineteen secondary waves (m2, n2, L2, l2,T2, e2, h2, P1, 2Q1, r1, s1, J1, c1, M11, M12, OO1, j1, p1, and q1).
Following plots show the exemple of M2 and K1 waves. M2 semi-diurnal tide is one of the largest components; it is the tide generated by the attraction of an "ideal" Moon, in a perfectly circular orbit around the Earth's equator. K1 diurnal tide reflects variations in the declination of the Sun and Moon.

Amplitude (left) and phase (right) of semi-diurnal tide M2.
Amplitude (left) and phase (right) of diurnal tide K1.
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