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Geodetic Reference System 1980
Geodetic Reference System 1980
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The Geodetic Reference System 1980 (GRS80) consists of a global reference ellipsoid and a normal gravity model.[1][2][3] The GRS80 gravity model has been followed by the newer more accurate Earth Gravitational Models, but the GRS80 reference ellipsoid is still the most accurate in use for coordinate reference systems, e.g. for the international ITRS, the European ETRS89 and (with a 0,1 mm rounding error) for WGS 84 used for the American Global Navigation Satellite System (GPS).

Background

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Geodesy is the scientific discipline that deals with the measurement and representation of the earth, its gravitational field and geodynamic phenomena (polar motion, earth tides, and crustal motion) in three-dimensional, time-varying space.

The geoid is essentially the figure of the Earth abstracted from its topographic features. It is an idealized equilibrium surface of sea water, the mean sea level surface in the absence of currents, air pressure variations etc. and continued under the continental masses. The geoid, unlike the ellipsoid, is irregular and too complicated to serve as the computational surface on which to solve geometrical problems like point positioning. The geometrical separation between it and the reference ellipsoid is called the geoidal undulation, or more usually the geoid-ellipsoid separation, N. It varies globally between ±110 m.

A reference ellipsoid, customarily chosen to be the same size (volume) as the geoid, is described by its semi-major axis (equatorial radius) a and flattening f. The quantity f = (ab)/a, where b is the semi-minor axis (polar radius), is a purely geometrical one. The mechanical ellipticity of the earth (dynamical flattening, symbol J2) is determined to high precision by observation of satellite orbit perturbations. Its relationship with the geometric flattening is indirect. The relationship depends on the internal density distribution.

The 1980 Geodetic Reference System (GRS 80) posited a 6378137 m semi-major axis and a 1298.257222101 flattening. This system was adopted at the XVII General Assembly of the International Union of Geodesy and Geophysics (IUGG) in Canberra, Australia, 1979.

The GRS 80 reference system was originally used by the World Geodetic System 1984 (WGS 84). The reference ellipsoid of WGS 84 now differs slightly due to later refinements.[citation needed]

The numerous other systems which have been used by diverse countries for their maps and charts are gradually dropping out of use as more and more countries move to global, geocentric reference systems using the GRS80 reference ellipsoid.

Definition

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The reference ellipsoid is usually defined by its semi-major axis (equatorial radius) and either its semi-minor axis (polar radius) , aspect ratio or flattening , but GRS80 is an exception: four independent constants are required for a complete definition. GRS80 chooses as these , , and , making the geometrical constant a derived quantity.

Defining geometrical constants
Semi-major axis = Equatorial Radius = ;
Defining physical constants
Geocentric gravitational constant determined from the gravitational constant and the earth mass with atmosphere ;
Dynamical form factor ;
Angular velocity of rotation ;

Derived quantities

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Derived geometrical constants (all rounded)
Flattening = = 0.003 352 810 681 183 637 418;
Reciprocal of flattening = = 298.257 222 100 882 711 243;
Semi-minor axis = Polar Radius = = 6 356 752.314 140 347 m;
Aspect ratio = = 0.996 647 189 318 816 363;
Mean radius as defined by the International Union of Geodesy and Geophysics (IUGG): = 6 371 008.7714 m;
Authalic mean radius = = 6 371 007.1809 m;
Radius of a sphere of the same volume = = 6 371 000.7900 m;
Linear eccentricity = = 521 854.0097 m;
Eccentricity of elliptical section through poles = = 0.081 819 191 0428;
Polar radius of curvature = = 6 399 593.6259 m;
Equatorial radius of curvature for a meridian = = 6 335 439.3271 m;
Meridian quadrant = 10 001 965.7292 m;
Derived physical constants (rounded)
Period of rotation (sidereal day) = = 86 164.100 637 s

The formula giving the eccentricity of the GRS80 spheroid is:[1]

where

and (so ). The equation is solved iteratively to give

which gives

References

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Revisions and contributorsEdit on WikipediaRead on Wikipedia
from Grokipedia
The Geodetic Reference System 1980 (GRS80) is a standardized geocentric reference framework for , comprising a reference and a normal designed to model Earth's shape and with high precision for global mapping, surveying, and applications. Adopted by the International Union of Geodesy and Geophysics (IUGG) at its XVII in in 1979, GRS80 replaced the earlier Geodetic Reference System 1967 (GRS67) to incorporate improved measurements of Earth's , dynamical form factor, and rotation. Its defining parameters include a semi-major axis a of 6,378,137 meters, an inverse 1/f of 298.257222101 (yielding a f of approximately 0.00335281068118 and a semi-minor axis b of 6,356,752.3141 meters), the geocentric GM of 3.986005 × 10¹⁴ m³ s⁻², the dynamical form factor J₂ of 1082.63 × 10⁻⁶, and Earth's ω of 7.292115 × 10⁻⁵ rad s⁻¹. These values establish an centered at Earth's , with the Z-axis aligned to the Conventional International Origin (CIO) and the X-axis to the Bureau International de l'Heure (BIH) zero meridian. GRS80 provides the foundational ellipsoid for several modern geodetic datums, most notably serving as the basis for the World Geodetic System 1984 (WGS84), which was developed by the U.S. Department of Defense and implemented in 1987 for GPS operations, though WGS84 features a slightly refined inverse flattening of 298.257223563 to account for updated satellite data. It is also integral to the North American Datum of 1983 (NAD83), widely used in North American surveying and maintained by the National Geodetic Survey (NGS). The system's normal gravity formula, based on Somigliana's equation, computes theoretical gravity values—such as 9.7803267715 m s⁻² at the equator and 9.8321863685 m s⁻² at the poles—essential for height determinations and geophysical modeling, with provisions for atmospheric corrections. Despite minor evolutions in related systems, GRS80 remains a cornerstone of international geodesy, supporting applications in satellite navigation, crustal dynamics, and global change monitoring due to its alignment with Doppler satellite observations and laser ranging data from the late 1970s.

History and Development

Origins and Adoption

The Geodetic Reference System 1980 (GRS80) emerged in the late 1970s as part of international efforts to standardize geodetic parameters amid advancing satellite technology and global measurement needs. It was developed under the auspices of the International Association of Geodesy (IAG), specifically through Special Study Group 5.39 on fundamental geodetic constants, which focused on reconciling geometric, gravitational, and rotational parameters for a cohesive Earth model. Key contributions came from Helmut Moritz, who led the formulation of the system's ellipsoidal and potential field definitions, and Richard H. Rapp, who provided critical analyses of gravity data and parameter estimation techniques to support the group's recommendations. The primary purpose of GRS80 was to establish a geocentric that could serve as a unified framework for precise geometric and gravimetric positioning worldwide, addressing the limitations of disparate national datums such as various Clarke ellipsoids that had led to inconsistencies in global mapping and navigation. This initiative built on prior IAG work, including the Geodetic Reference System 1967, but incorporated updated observations from to enhance accuracy for geophysical and astronomical applications. By prioritizing a consistent set of defining parameters, GRS80 aimed to facilitate in international scientific collaborations and replace fragmented local systems with a single, authoritative standard. GRS80 was formally adopted at the XVII General Assembly of the International Union of and Geophysics (IUGG) held in , , in December 1979, through Resolution No. 7. This resolution recognized the need for an updated geocentric system and endorsed GRS80's parameters as the official IAG reference, urging its adoption in geodetic practice to promote uniformity. The adoption marked a pivotal step in global , enabling subsequent developments in coordinate reference frames and gravity modeling.

Relation to Earlier Systems

The Geodetic Reference System 1980 (GRS80) represents a significant evolution in geodetic modeling, building upon a lineage of reference ellipsoids that began with regionally focused systems in the 19th and early 20th centuries. Earlier ellipsoids, such as the Clarke 1866 model—characterized by a semi-major axis of 6,378,206 m and flattening of 1/294.978—were designed primarily for North American surveys and exhibited regional biases, fitting local undulations well but deviating substantially from a global, geocentric representation of Earth's shape. Similarly, the International of 1924, based on Hayford's 1909 determinations with a semi-major axis of 6,378,388 m and flattening of 1/297, was optimized for European and broader international networks but suffered from similar limitations, as its center was offset from Earth's , leading to inconsistencies in global applications. These regional systems gave way to more standardized global models in the mid-20th century, culminating in the Geodetic Reference System 1967 (GRS67), which served as the direct predecessor to GRS80. Adopted by the International Association of Geodesy (IAG) in 1967, GRS67 featured a semi-major axis of 6,378,160 m and flattening of 1/298.247, representing an improvement in accuracy based on terrestrial gravity and astronomical observations, although it was geocentric but relied on data that was less precise than subsequent satellite measurements. By the late 1970s, GRS67 was recognized as inadequate for emerging precision requirements, prompting its replacement as outlined in IUGG Resolution No. 7 (1979), which emphasized the need for updated constants to better reflect Earth's size, shape, and gravity field. The development of GRS80 was motivated by the advent of space-based geodetic techniques in the , which necessitated a shift toward truly global, geocentric reference frames to accommodate data from satellite Doppler tracking (e.g., via the Transit system), (SLR), and other observations. These technologies provided unprecedented global coverage and accuracy, revealing discrepancies in older models' alignments with Earth's and rotation axis, thus driving the transition from regionally biased ellipsoids to a unified system suitable for international scientific and navigational purposes. This evolution marked a pivotal advancement in , enabling consistent worldwide coordinate referencing without the distortions inherent in prior systems.

Defining Parameters

Ellipsoidal Parameters

The Geodetic Reference System 1980 (GRS80) establishes the shape of its reference through two fundamental geometric parameters: the semi-major axis and the . These parameters define an oblate spheroid that approximates the Earth's mean surface, serving as the geometric foundation for coordinate transformations and geodetic computations. The semi-major axis, denoted aa, is defined exactly as 6,378,137 meters, corresponding to the equatorial radius of the . This precise value was adopted to align with contemporary measurements of the Earth's equatorial dimensions. The , denoted ff, is defined exactly as 1/298.2572221011/298.257222101, or equivalently f=0.00335281068118f = 0.00335281068118. This ratio quantifies the ellipsoid's compression along the polar axis relative to the , reflecting the 's oblateness. Both parameters were determined through a of global , gravimetric, and data, aimed at minimizing discrepancies between observed and modeled parameters. This adjustment process, conducted by the International Association of Geodesy (IAG), incorporated data from orbits and anomalies to achieve optimal fit for the reference . Within GRS80, the authalic radius serves as an intermediate quantity in gravity field modeling, representing the radius of a sphere with the same surface area as the ellipsoid.

Gravitational and Rotational Parameters

The gravitational and rotational parameters of the Geodetic Reference System 1980 (GRS80) provide the dynamic foundation for modeling the Earth's normal gravity potential, essential for precise geodetic calculations. These parameters were adopted by the International Union of Geodesy and Geophysics (IUGG) at its XVII General Assembly in Canberra in 1979, through Resolution No. 7, to standardize global reference computations. The geocentric gravitational constant, denoted GMGM, is defined as 3.986005×10143.986005 \times 10^{14} m³ s⁻². This value is the product of the Newtonian GG and the total mass of the MM, encompassing the atmosphere, and serves as the central term in the expansion for GRS80. The dynamical form factor J2J_2 is specified as 1.08263×1031.08263 \times 10^{-3}, or equivalently 108263×108108263 \times 10^{-8}. It represents the dominant oblateness effect due to the Earth's , calculated as J2=(CA)/(Ma2)J_2 = (C - A)/(M a^2), where CC and AA are the polar and equatorial moments of , respectively, excluding permanent tidal deformation, and aa is the equatorial radius. The of ω\omega is fixed at exactly 7.292115×1057.292115 \times 10^{-5} rad s⁻¹. This precise value reflects the conventional mean sidereal rate of the , incorporating the centrifugal potential in the total gravity field model. Collectively, these parameters were derived from analyses of orbit perturbations—such as those observed in ranging and Doppler tracking—and anomaly measurements, ensuring a consistent representation of the Earth's dynamic figure when combined with the static ellipsoidal geometry.

Derived Quantities

Geometric Quantities

The geometric quantities of the Geodetic Reference System 1980 (GRS80) ellipsoid are secondary properties computed directly from its defining semi-major axis a=6,378,137a = 6{,}378{,}137 m and f=1/298.257222101f = 1/298.257222101. These include lengths and measures that characterize the shape and size of the reference for geodetic computations, such as positioning and mapping. The semi-minor axis bb, representing the polar radius, is derived as b=a(1f)b = a(1 - f), yielding b=6,356,752.314140b = 6{,}356{,}752.314140 m. This value defines the ellipsoid's compression along the rotation axis, essential for converting between geodetic and Cartesian coordinates. The first eccentricity squared e2e^2 quantifies the ellipsoid's deviation from a and is calculated via e2=2ff2=0.00669438002290e^2 = 2f - f^2 = 0.00669438002290. This parameter appears in formulas for meridian arcs and geodetic latitudes. The linear eccentricity ε\varepsilon, the from the ellipsoid's to the focus, is given by ε=ae2=521,854.0097\varepsilon = a \sqrt{e^2} = 521{,}854.0097
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