Abstract
Two different treatments in ocean dynamics are found between the gravity and pressure gradient force. Vertical component is 5–6 orders of magnitude larger than horizontal components for the pressure gradient force in largescale motion, and for the gravity in any scale motion. The horizontal pressure gradient force is considered as a dominant force in oceanic motion from planetary to small scales. However, the horizontal gravity is omitted in oceanography completely. A nondimensional C number (ratio between the horizontal gravity and the Coriolis force) is used to identify the importance of horizontal gravity in the ocean dynamics. Unexpectedly large C number with the global mean around 24 is obtained using the community datasets of the marine geoid height and ocean surface currents. New largescale ocean dynamic equations with the real gravity are presented such as hydrostatic balance, geostrophic equilibrium, thermal wind, equipotential coordinate system, and vorticity equation.
Introduction
Gravity is greatly simplified in oceanography from a threedimensional vector field [g = (g_{λ}, g_{φ}, g_{z})] with (λ, φ, z) being the (longitude, latitude, height) and (i, j, k) being the corresponding unit vectors with eastward positive for i, northward positive for j, and upward positive (in the Earth radial direction) for k to a vertical vector (−g_{0}k) with the uniform gravity g_{0} = 9.81 m/s^{2}. The feasibility of such a practice has never been challenged because the horizontal components (g_{λ}, g_{φ}) are much smaller (5–6 orders of magnitudes) than the vertical component g_{z} and the deviation of the magnitude of g_{z} to g_{0} is also very small. However, similar situation also occurs with the threedimensional pressure gradient force: the horizontal pressure gradient force is much smaller (5–6 orders of magnitudes) than the vertical pressure gradient force in largescale oceanic motion. The horizontal pressure gradient forces are considered important in oceanic motion for any scales. Thus, the feasibility to neglect the horizontal gravity components (g_{λ}, g_{φ}) against the vertical gravity (g_{z}) needs to be investigated. The correct approach is to compare the horizontal gravity with the horizontal forces such as the Coriolis force or the horizontal pressure gradient force.
Reference coordinate systems
The polar spherical coordinates (more popular) and oblate spherical coordinates (less popular, see Appendix) are the reference coordinate system used in the Earth science. In all the fields of the Earth science such as meteorology, oceanography, and geodesy, the horizontal component of any vector A is on the spherical surface if the polar spherical coordinates are used or on the ellipsoidal surface if the oblate spherical coordinates are used,
no matter the variable is evaluated on the geoid, isobaric, isopycnal, or topographicfollowing surfaces. Ocean numerical models have several representations of the vertical (i.e., the radial) coordinate such as zcoordinate^{1,2}, isopycnal coordinate^{3,4}, topographicfollowing coordinate (i.e., sigmacoordinate)^{5,6}. However, the horizontal component of the vector A is always given by (1).
Three forms of the gravity
Three forms of gravity exist in geodesy and oceanography: the real gravity g(λ, φ, z), the normal gravity [−g(φ)k], and the uniform gravity (−g_{0}k, g_{0} = 9.81 m/s^{2}). The real gravity (g) is a threedimensional vector field, which is decomposed into
where g_{h} is the horizontal gravity component; and (g_{z}k) is the vertical gravity component. The normal gravity vector [−g(φ)k] (vertical vector) is associated with a mathematically modeled Earth (i.e., a rigid and geocentric ellipsoid) called the normal Earth. The normal Earth is a spheroid (i.e., an ellipsoid of revolution), has the same total mass and angular velocity as the Earth, and coincides its minor axis with the mean rotation of the Earth^{7}. Similar to g(λ, φ, z), the normal gravity [−g(φ)k] is the sum of the gravitational and centrifugal accelerations exerted on the water particle by the normal Earth. Its intensity g(φ) is called the normal gravity and determined analytically. For example, the World Geodetic System 1984 uses the Somiglina equation to represent g(φ)^{8}
where (a, b) are the equatorial and polar semiaxes; a is used for the Earth radius, R = a = 6.3781364 × 10^{6} m; b = 6.3567523 × 10^{6} m; e is the spheroid’s eccentricity; g_{e} = 9.780 m/s^{2}, is the gravity at the equator; and g_{p} = 9.832 m/s^{2} is the gravity at the poles. The uniform gravity (−g_{0}k) is commonly used in oceanography.
Real and normal gravity potential
Let (P, Q) be the Newtonian gravitational potential of the (real Earth, normal Earth) and P_{R} \(( = \Omega^{2} r^{2} \cos^{2} \varphi /2)\)) be the potential of the Earth’s rotation. Let V = P + P_{R} be the gravity potential of the real Earth (associated with real gravity g) and E = Q + P_{R} be the gravity potential of the normal Earth [associated with the normal gravity g(φ)k]. The potential of the normal gravity [−g(φ)k] is given by
The gravity disturbance is the difference between the real gravity g(λ, φ, z) and the normal gravity [−g(φ)k] at the same point^{9}. The potential of the gravity disturbance (called the disturbing gravity potential) is given by
Consequently, the centrifugal effect disappears and the disturbing gravity potential (T) can be considered a harmonic function. With the disturbing gravity potential T, the real gravity g (= g_{h} + g_{z}k) is represented by
where \(\nabla_{h}\) is the horizontal vector differential operator. The geoid height relative to the normal Earth (i.e., reference spheroid) is given by Bruns’ formula^{10}
Equations (5), (6), (7) clearly show that the fluctuation of the marine geoid is independent of the Earth rotation and dependent on the disturbing gravity potential (T) evaluated at z = 0 only.
The disturbing static gravity potential (T) outside the Earth masses in the spherical coordinates with the spherical expansion is given by^{11}
where G = 6.674 × 10^{−11}m^{3}kg^{−1} s^{−2}, is the gravitational constant; M = 5.9736 × 10^{24} kg, is the mass of the Earth; r is the radial distance with z = r−R; \(P_{l,m} (\sin \varphi )\) are the Legendre associated functions with (l, m) the degree and order of the harmonic expansion; \((C_{l,m} ,C_{l,m}^{el} ,S_{l,m} )\) are the harmonic geopotential coefficients (Stokes parameters with \(C_{l,m}^{el}\) belonging to the reference ellipsoid.
From Eqs. (4) and (5) the potential of the real gravity is given by
From Eq. (6) the real gravity is represented by
The horizontal gravity component at the reference ellipsoid surface (z = 0) is obtained using (7) and (10)^{12,13}
An approximate 3D gravity field for oceanography
According to Eq. (8) (i.e., the spectral of the disturbing static gravity potential T), the ratio between T(λ, φ, z) to T(λ, φ, 0) through the water column can be roughly estimated by
where H is the water depth. Since R is the radius of the Earth and more than 3 orders of magnitude larger than the water depth H. This leads to the first approximation that the surface disturbing gravity potential T(λ, φ, 0) is used for the whole water column,
Since the deviation of the vertical component of the gravity (g_{z}) to a constant (−g_{0}) is 3–4 orders of magnitude smaller than g_{0}, it leads to the second approximation
With the two approximations, the near real gravity in the water column is given by
Correspondingly, the potential of the real gravity is approximately given by
where Eq. (9) is used.
Unexpectedly large horizontal gravity component
For simplicity, the local coordinates (x, y, z) are used from now on to replace the polar spherical coordinates with x representing longitude (eastward positive) and y representing latitude (northward positive). The local and spherical coordinate systems are connected by
The EIGEN6C4 model^{14,15}, listed on the website http://icgem.gfzpotsdam.de/home, was developed jointly by the GFZ Potsdam and GRGS Toulouse up to degree and order 2190 to produce global static geoid height (N) dataset. Following the instruction, the author ran the EIGEN6C4 model in 1° × 1° resolution for 17 s to get the global N (Fig. 1) with mean value of 30.57 m, minimum value of 106.20 m, and maximum of 85.83 m. Two locations on the marine geoid are identified with N_{A} = − 99.76 m at A (80° W, 3° N) in the Indian Ocean, and N_{B} = 65.38 m at B (26° W, 45° N) in the North Atlantic Ocean, i.e., ΔN_{AB} = 165.14 m. The big circle distance between A and B is about ΔL = 7920 km. Equation (11) shows that the corresponding g_{h} at z = 0 is computed by
With the geoid height data obtained from the EIGEN6C4, N(x, y), the horizontal gravity components g_{x} (Fig. 2a) and g_{y} (Fig. 2b) at z = 0 are computed using Eq. (11). The magnitude of the horizontal gravity vector is calculated by
as shown in Fig. 2c. The histogram of g_{h} (Fig. 2d) indicates a positively skewed distribution with a long tail extending to values larger than 100 mGal (1 mGal = 10^{−5} m s^{−2}). The statistical characteristics of g_{h} are 20.84 mGal as the mean, 15.89 mGal as the standard deviation, 3.11 as the skewness, and 21.63 as the kurtosis. The statistical estimate of the mean intensity of the horizontal gravity g_{h} (20.84 mGal) is coherent with the simple calculation of g_{h}_{AB} between points A and B (20.45 mGal). The two values (20.84 mGal, 20.45 mGal) are unexpectedly large.
C number to identify importance of the horizontal gravity
The importance of the horizontal gravity can be identified by a nondimensional C number^{16} from the analysis of horizontal gravity versus the Coriolis force,
where f = 2Ωsinφ, is the Coriolis parameter; and U is the speed of the horizontal current. With Eq. (11) the C number at z = 0 is given by
where ΔL is the horizontal scale of the motion.
The Ocean Surface Current Analysis Realtime (OSCAR) third degree resolution 5day mean surface current vectors^{17} on 26 February 2020 (Fig. 3a) was downloaded from the website https://podaactools.jpl.nasa.gov/drive/files/allData/oscar/ and the data at the same 1° × 1° grid points as the EIGEN6C4 data were used. The data represent vertically averaged surface currents over the top 30 m of the upper ocean, which consist of a geostrophic component with a thermal wind adjustment using satellite sea surface height, and temperature and a winddriven ageostrophic component using satellite surface winds. The histogram of the OSCAR current speed U(x, y) (Fig. 3b) indicates a positively skewed distribution with a long tail extending to values larger than 0.4 m/s. The statistical characteristics of U are 0.1397 m/s as the mean, 0.1414 m/s as the standard deviation, 3.013 as the skewness, and 21.01 as the kurtosis. The histogram of the corresponding Coriolis force \(fU(x,y)\) (Fig. 3c) also shows a positively skewed distribution with a long tail extending to values larger than 2.5 mGal. The statistical characteristics of \(fU\) are 0.8815 mGal as the mean, 1.029 mGal as the standard deviation, 3.379 as the skewness, and 20.24 as the kurtosis. Comparison between Figs. 2d and 3c leads to the fact that the mean intensity of horizontal gravity component \({\mathbf{g}}_{h} \) (= 20.84 mGal) is nearly 24 times as large as the mean intensity of the Coriolis force identified from the OSCAR surface currents on 26 February 2020. Such unexpectedly large horizontal gravity component is also shown in the world ocean distribution of (1/C_{0}) values (Fig. 4a). The histogram of (1/C_{0}) (Fig. 4b) indicates a positively skewed distribution with a long tail extending to values larger than 0.18. The statistical characteristics of (1/C_{0}) are 0.04238 as the mean, 0.04108 as the standard deviation, 1.447 as the skewness, and 4.481 as the kurtosis. Thus, the global mean of C_{0} is about 23.6, which is coherent with the rough estimate given above using the geoid height data at the two points A and B (near 24).
New equations with the real gravity
Application of the Newton’s second law of motion into the ocean for the largescale motions with the Boussinesq approximation leads to
if the pressure gradient force, gravitation, and friction are the only real forces. Here, \({{\varvec{\Omega}}} = \Omega \left( {{\mathbf{j}}\cos \varphi + {\mathbf{k}}\sin \varphi } \right)\), is the Earth rotation vector with Ω = 2π/(86,400 s) the Earth rotation rate; ρ is the density; ρ_{0} = 1028 kg/m^{3}, is the characteristic density; U = (u, v), is the horizontal velocity vector; \(\nabla\) is the three dimensional vector differential operator; and D/Dt is the total time rate of change; F = (F_{x}, F_{y}), is the frictional force and usually represented using vertical eddy viscosity K,
The continuity equation is given by
where w is the vertical velocity. Substitution of (16) into (22) leads to
Equation (25) can be easily used by any ocean numerical model with just adding the horizontal gravity component represented by \((\rho g_{0} \nabla_{h} N)\).
Hydrostatic balance
Largescale oceanic motion is hydrostatically balanced,
Vertical integration of this equation from the marine geoid (i.e., V = 0) to any equipotential surface V leads to the integral form of the hydrostatic balance
where S is the sea surface height; and the marine geoid surface (N) is the coincidence of the equipotential and isobaric surfaces (i.e., balance of the 3D pressure gradient force and gravity on N).
Equipotential (V) coordinate system
The hydrostatic Eq. (27) clearly shows that a single valued monotonic relationship exists between gravitational potential and the depth in each vertical water column. Thus, we may use (V) as the independent vertical coordinate. The negative sign is due to the vertical component of the gravity is defined positive downward. The total derivative is expanded as
The continuity Eq. (24) becomes
here,
where ω is the “vertical velocity” in the Vcoordinate. Note that V is the static gravitational potential such that ∂V/∂t = 0.
Dynamic equations in the equipotential coordinate system
The horizontal pressure gradients can be computed from (27),
Substitution of (31) into (22) leads to the horizontal momentum equations
Extended geostrophic equilibrium and thermal wind relation
For steady state (no total derivative) without friction, Eqs. (32a) and (32b) become the extended equations for the geostrophic currents
Vertical derivative of (33a) and (33b) leads to the extended thermal wind relation
where the vertical differentiation of lower limit (V) of the integrals of the righthand side of (33a) and (33b)
is used.
Vorticity equation
Subtraction of the differentiation of the longitudinal component of Eq. (25) with respect to y from the differentiation of the latitudinal component of Eq. (25) with respect to x leads to the vorticity equation,
where \(J(\rho ,N) = (\partial \rho /\partial x)(\partial N/\partial y)  (\partial \rho /\partial y)(\partial N/\partial x)\), is the Jacobian; \(\beta = df/dy\) is the latitudinal change of the Coriolis parameter; and \(\zeta = \partial v/\partial x  \partial u/\partial y\) is the vertical vorticity.
Conclusion
The nondimensional C number is used to identify relative importance of the horizontal gravity and the Coriolis force using the geoid height data (N) provided by the EIGEN6C4 gravity model, and the Ocean Surface Current Analysis Realtime (OSCAR) surface current vectors on 26 February 2020. Unexpectedly large value of the C number (global mean around 24) may surprise both oceanographic and geodetic communities. It is very hard for my oceanographic colleagues to accept such strong horizontal gravity (at z = 0), which is an order of magnitude lager that the Coriolis force. Thus, in situ measurement of gravity may be needed for oceanography in addition to the routine hydrographic and current meter measurements.
A geodesist may also be surprised that the horizontal gravity (z = 0) associated with the geoid height (N) varying between 106.20 m to 85.83 m (well accepted by the geodetic community), which was produced by a community gravity model (EIGEN64C), generates the ocean currents with the intensity nearly 24 times as large as the currents identified from the ocean surface current analysis realtime (OSCAR) (oceanographic community product).
How to resolve such incoherency between the two communities on this issue becomes urgent. The new ocean dynamic equations including the horizontal gravity may provide a theoretical framework to resolve the incoherency since the potential of the real gravity (V) obtained from a geodetic gravity model is explicitly in the dynamical equations. Besides, use of the real gravity in the ocean dynamics may ultimately resolve some fundamental problems in oceanography such as reference level, and absolute geostrophic current calculation. A new dynamic system for largescale oceanic motion with the real gravity is presented such as hydrostatic balance, geostrophic equilibrium, thermal wind, equipotential coordinate system, and the vorticity equation. Close collaboration between the oceanographic and geodetic communities helps the use of the real gravity in oceanography and the verification of the gravity model in geodesy with oceanographic data.
Change history
26 April 2022
This article has been retracted. Please see the Retraction Notice for more detail: https://doi.org/10.1038/s41598022108460
References
Sun, F., Kim, V. S., Huang, B. & Wang, D. Water exchange between the subpolar and subtropical North Pacific Ocean in an OGCM. Sci. China D 47, 37–48 (2004).
Chu, P. C., Fan, C. W. & Cai, W. J. P vector method evaluated using modular ocean model (MOM). J. Oceanogr. 54, 185–198 (1998).
Wang, D., Wang, J. & Wu, L. Regime shifts in the North Pacific simulated by a COADSdriven isopycnal model. Adv. Atmosph. Sci. 20, 743–754 (2003).
Chu, P. C. & Li, R. F. South China Sea isopycnal surface circulations. J. Phys. Oceanogr. 30, 2419–2438 (2000).
Chu, P. C. & Fan, C. W. Sixthorder difference scheme for sigma coordinate ocean models. J. Phys. Oceanogr. 27, 2064–2071 (1997).
Chu, P. C., Lu, S. H. & Chen, Y. C. Evaluation of the Princeton Ocean model using the South China Sea Monsoon experiment (SCSMEX) data. J. Atmos. Oceanic Technol. 18, 1521–1539 (2001).
Vaniček, P. & Krakiwsky, E. Geodesy: The Concepts 697 (NorthHolland, Amsterdam, 1986).
National GeospatialIntelligence Agency. Department of Defense World Geodetic System 1984 (WGS84). Its definition and relationships with local geodetic systems. NIMA TR8350.2., 3rd Edition, Equation 4–1 (1984).
Hackney, R. I. & Featherstone, W. E. Geodetic versus geophysical perspectives of the ‘gravity anomaly’. Geophys. J. Int. 154, 35–43 (2003).
Sandwell, D. T. & Smith, W. H. F. Marine gravity anomaly from Geosat and ERS 1 satellite altimetry. J. Geophys. Res. 102(B5), 10039–10054 (1997).
Kostelecký, J., Klokočnìk, J., Bucha, B., Bezdĕk, A. & Fӧrste, C. Evaluation of the gravity model EIGEN6C4 in comparison with EGM2008 by means of various functions of the gravity potential and by BNSS/levelling. Geoinform. FCE CTU. https://doi.org/10.14311/gi.14.1.1 (2015).
Chu, P. C. Two types of absolute dynamic ocean topography. Ocean Sci. 14, 947–957 (2018).
Chu, P. C. A. Complete formula of ocean surface absolute geostrophic current. Nat. Sci. Rep, 10, Article number 1445 (2020).
Ince, E. S. et al. ICGEM: 15 years of successful collection and distribution of global gravitational models, associated services, and future plans. Earth Syst. Sci. Data 11, 647–674 (2019).
Förste, C., Bruinsma, S.L., Abrikosov, O., Lemoine, J.M., Marty, J.C., Flechtner, F., Balmino, G., Barthelmes, F., & Biancale, R. EIGEN6C4. The latest combined global gravity field model including GOCE data up to degree and order 2190 of GFZ Potsdam and GRGS Toulouse, https://doi.org/10.5880/icgem.2015.1 (2014).
Chu, P. C.Occurrence of spurious geostrophic currents on the marine geoid without horizontal gravity component. Nat. Sci. Rep, in press (2020).
ESR. OSCAR third deg. ver. 1. PO.DAAC, CA, USA. Dataset accessed [20201110] athttps://doi.org/10.5067/OSCAR03D01 (2009).
Gill, A. E. AtmosphereOcean Dynamics. International Geophysics Series Vol. 30, 91–94 (Academic Press, New York, 1982).
Acknowledgements
The author thanks the International Centre for Global Erath Models (ICGEM) for the EIGEN6C4 geoid undulation data, and the NASA Jet Propulsion Laboratory for the OSCAR Third Degree Resolution Ocean Surface Currents. He also thanks Mr. Chenwu Fan for computational assistance, and the Naval Postgraduate School Research Office for paying the publication cost.
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P.C.C. designed the project, obtained the datasets, conducted the computation, and wrote the manuscript.
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Appendix: Oblate spheroid coordinates versus polar spherical coordinates
Appendix: Oblate spheroid coordinates versus polar spherical coordinates
This paper uses the polar spherical coordinates rather than the oblate spheroid coordinates for computational simplicity with a small error (0.17%)^{18}. The oblate spheroid coordinates share the same longitude (λ) but different latitude (φ_{ob}) and radial coordinate (representing vertical) (r_{ob}). The relationship between the oblate spheroid coordinates (λ, φ_{ob}, r_{ob}) and the polar spherical coordinates (λ, φ, r) is given by^{18}
where d is the half distance between the two foci of the ellipsoid. For the normal Earth, d = 521.854 km. The vector differential operator in the oblate spheroid coordinates is represented by
where R = 6.3781364 × 10^{6} m, is the semimajor axis of the normal Earth (Earth radius). The coefficients (\(h_{\lambda }^{ob}\), \(h_{\varphi }^{ob}\), \(h_{r}^{ob}\)) are given by
However, the vector differential operator in the polar spherical coordinates is represented by
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Chu, P.C. RETRACTED ARTICLE: Ocean dynamic equations with the real gravity. Sci Rep 11, 3235 (2021). https://doi.org/10.1038/s41598021828821
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DOI: https://doi.org/10.1038/s41598021828821
Further reading

The “horizontal” components of the real gravity are not relevant to ocean dynamics
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