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Geodesy
Geodesy
from Wikipedia
A modern instrument for geodetic measurements using satellites

Geodesy or geodetics[1] is the science of measuring and representing the geometry, gravity, and spatial orientation of the Earth in temporally varying 3D. It is called planetary geodesy when studying other astronomical bodies, such as planets or circumplanetary systems.[2]

Geodynamical phenomena, including crustal motion, tides, and polar motion, can be studied by designing global and national control networks, applying space geodesy and terrestrial geodetic techniques, and relying on datums and coordinate systems.

Geodetic job titles include geodesist and geodetic surveyor.[3]

History

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Geodesy began in pre-scientific antiquity, so the very word geodesy comes from the Ancient Greek word γεωδαισία or geodaisia (literally, "division of Earth").[4]

Early ideas about the figure of the Earth held the Earth to be flat and the heavens a physical dome spanning over it.[5] Two early arguments for a spherical Earth were that lunar eclipses appear to an observer as circular shadows and that Polaris appears lower and lower in the sky to a traveler headed South.[6]

Definition

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Geodesy refers to the science of measuring and representing geospatial information, while geomatics encompasses practical applications of geodesy on local and regional scales, including surveying.

Geodesy originated as the science of measuring and understanding Earth's geometric shape, orientation in space, and gravitational field; it is now also applied to other astronomical bodies in the Solar System.[2]

To a large extent, Earth's shape is the result of rotation, which causes its equatorial bulge, and the competition of geological processes such as the collision of plates, as well as of volcanism, resisted by Earth's gravitational field. This applies to the solid surface, the liquid surface (dynamic sea surface topography), and Earth's atmosphere. For this reason, the study of Earth's gravitational field is called physical geodesy.

Geoid and reference ellipsoid

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Geoid, an approximation for the shape of the Earth; shown here with vertical exaggeration (10000 vertical scaling factor).
Ellipsoid - a mathematical representation of the Earth. When mapping in geodetic coordinates, a latitude circle forms a truncated cone.
Equatorial (a), polar (b) and mean Earth radii as defined in the 1984 World Geodetic System

The geoid essentially is the figure of Earth abstracted from its topographical features. It is an idealized equilibrium surface of seawater, the mean sea level surface in the absence of currents and air pressure variations, and continued under the continental masses. Unlike a reference ellipsoid, the geoid is irregular and too complicated to serve as the computational surface for solving geometrical problems like point positioning. The geometrical separation between the geoid and a reference ellipsoid is called geoidal undulation, and it varies globally between ±110 m based on the GRS 80 ellipsoid.

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 purely geometrical. The mechanical ellipticity of Earth (dynamical flattening, symbol J2) can be determined to high precision by observation of satellite orbit perturbations. Its relationship with geometrical flattening is indirect and depends on the internal density distribution or, in simplest terms, the degree of central concentration of mass.

The 1980 Geodetic Reference System (GRS 80), adopted at the XVII General Assembly of the International Union of Geodesy and Geophysics (IUGG), posited a 6,378,137 m semi-major axis and a 1:298.257 flattening. GRS 80 essentially constitutes the basis for geodetic positioning by the Global Positioning System (GPS) and is thus also in widespread use outside the geodetic community. Numerous systems used for mapping and charting are becoming obsolete as countries increasingly move to global, geocentric reference systems utilizing the GRS 80 reference ellipsoid.

The geoid is a "realizable" surface, meaning it can be consistently located on Earth by suitable simple measurements from physical objects like a tide gauge. The geoid can, therefore, be considered a physical ("real") surface. The reference ellipsoid, however, has many possible instantiations and is not readily realizable, so it is an abstract surface. The third primary surface of geodetic interest — the topographic surface of Earth — is also realizable.

Coordinate systems in space

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Datum shift between NAD27 and NAD83, in metres

The locations of points in 3D space most conveniently are described by three cartesian or rectangular coordinates, X, Y, and Z. Since the advent of satellite positioning, such coordinate systems are typically geocentric, with the Z-axis aligned to Earth's (conventional or instantaneous) rotation axis.

Before the era of satellite geodesy, the coordinate systems associated with a geodetic datum attempted to be geocentric, but with the origin differing from the geocenter by hundreds of meters due to regional deviations in the direction of the plumbline (vertical). These regional geodetic datums, such as ED 50 (European Datum 1950) or NAD 27 (North American Datum 1927), have ellipsoids associated with them that are regional "best fits" to the geoids within their areas of validity, minimizing the deflections of the vertical over these areas.

It is only because GPS satellites orbit about the geocenter that this point becomes naturally the origin of a coordinate system defined by satellite geodetic means, as the satellite positions in space themselves get computed within such a system.

Geocentric coordinate systems used in geodesy can be divided naturally into two classes:

  1. The inertial reference systems, where the coordinate axes retain their orientation relative to the fixed stars or, equivalently, to the rotation axes of ideal gyroscopes. The X-axis points to the vernal equinox.
  2. The co-rotating reference systems (also ECEF or "Earth Centred, Earth Fixed"), in which the axes are "attached" to the solid body of Earth. The X-axis lies within the Greenwich observatory's meridian plane.

The coordinate transformation between these two systems to good approximation is described by (apparent) sidereal time, which accounts for variations in Earth's axial rotation (length-of-day variations). A more accurate description also accounts for polar motion as a phenomenon closely monitored by geodesists.

Coordinate systems in the plane

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2D grid for elliptical coordinates
A Munich archive with lithography plates of maps of Bavaria

In geodetic applications like surveying and mapping, two general types of coordinate systems in the plane are in use:

  1. Plano-polar, with points in the plane defined by their distance, s, from a specified point along a ray having a direction α from a baseline or axis.
  2. Rectangular, with points defined by distances from two mutually perpendicular axes, x and y. Contrary to the mathematical convention, in geodetic practice, the x-axis points North and the y-axis East.

One can intuitively use rectangular coordinates in the plane for one's current location, in which case the x-axis will point to the local north. More formally, such coordinates can be obtained from 3D coordinates using the artifice of a map projection. It is impossible to map the curved surface of Earth onto a flat map surface without deformation. The compromise most often chosen — called a conformal projection — preserves angles and length ratios so that small circles get mapped as small circles and small squares as squares.

An example of such a projection is UTM (Universal Transverse Mercator). Within the map plane, we have rectangular coordinates x and y. In this case, the north direction used for reference is the map north, not the local north. The difference between the two is called meridian convergence.

It is easy enough to "translate" between polar and rectangular coordinates in the plane: let, as above, direction and distance be α and s respectively; then we have:

The reverse transformation is given by:

Heights

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Height measurement using satellite altimetry

In geodesy, point or terrain heights are "above sea level" as an irregular, physically defined surface. Height systems in use are:

  1. Orthometric heights
  2. Dynamic heights
  3. Geopotential heights
  4. Normal heights

Each system has its advantages and disadvantages. Both orthometric and normal heights are expressed in metres above sea level, whereas geopotential numbers are measures of potential energy (unit: m2 s−2) and not metric. The reference surface is the geoid, an equigeopotential surface approximating the mean sea level as described above. For normal heights, the reference surface is the so-called quasi-geoid, which has a few-metre separation from the geoid due to the density assumption in its continuation under the continental masses.[7]

One can relate these heights through the geoid undulation concept to ellipsoidal heights (also known as geodetic heights), representing the height of a point above the reference ellipsoid. Satellite positioning receivers typically provide ellipsoidal heights unless fitted with special conversion software based on a model of the geoid.

Geodetic datums

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Because coordinates and heights of geodetic points always get obtained within a system that itself was constructed based on real-world observations, geodesists introduced the concept of a "geodetic datum" (plural datums): a physical (real-world) realization of a coordinate system used for describing point locations. This realization follows from choosing (therefore conventional) coordinate values for one or more datum points. In the case of height data, it suffices to choose one datum point — the reference benchmark, typically a tide gauge at the shore. Thus we have vertical datums, such as the NAVD 88 (North American Vertical Datum 1988), NAP (Normaal Amsterdams Peil), the Kronstadt datum, the Trieste datum, and numerous others.

In both mathematics and geodesy, a coordinate system is a "coordinate system" per ISO terminology, whereas the International Earth Rotation and Reference Systems Service (IERS) uses the term "reference system" for the same. When coordinates are realized by choosing datum points and fixing a geodetic datum, ISO speaks of a "coordinate reference system", whereas IERS uses a "reference frame" for the same. The ISO term for a datum transformation again is a "coordinate transformation".[8]

Positioning

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GPS Block IIA satellite orbits over the Earth.
Geodetic control mark
Navigation device, Apollo program

General geopositioning, or simply positioning, is the determination of the location of points on Earth, by myriad techniques. Geodetic positioning employs geodetic methods to determine a set of precise geodetic coordinates of a point on land, at sea, or in space. It may be done within a coordinate system (point positioning or absolute positioning) or relative to another point (relative positioning). One computes the position of a point in space from measurements linking terrestrial or extraterrestrial points of known location ("known points") with terrestrial ones of unknown location ("unknown points"). The computation may involve transformations between or among astronomical and terrestrial coordinate systems. Known points used in point positioning can be GNSS continuously operating reference stations or triangulation points of a higher-order network.

Traditionally, geodesists built a hierarchy of networks to allow point positioning within a country. The highest in this hierarchy were triangulation networks, densified into the networks of traverses (polygons) into which local mapping and surveying measurements, usually collected using a measuring tape, a corner prism, and the red-and-white poles, are tied.

Commonly used nowadays is GPS, except for specialized measurements (e.g., in underground or high-precision engineering). The higher-order networks are measured with static GPS, using differential measurement to determine vectors between terrestrial points. These vectors then get adjusted in a traditional network fashion. A global polyhedron of permanently operating GPS stations under the auspices of the IERS is the basis for defining a single global, geocentric reference frame that serves as the "zero-order" (global) reference to which national measurements are attached.

Real-time kinematic positioning (RTK GPS) is employed frequently in survey mapping. In that measurement technique, unknown points can get quickly tied into nearby terrestrial known points.

One purpose of point positioning is the provision of known points for mapping measurements, also known as (horizontal and vertical) control. There can be thousands of those geodetically determined points in a country, usually documented by national mapping agencies. Surveyors involved in real estate and insurance will use these to tie their local measurements.

Geodetic problems

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In geometrical geodesy, there are two main problems:

  • First geodetic problem (also known as direct or forward geodetic problem): given the coordinates of a point and the directional (azimuth) and distance to a second point, determine the coordinates of that second point.
  • Second geodetic problem (also known as inverse or reverse geodetic problem): given the coordinates of two points, determine the azimuth and length of the (straight, curved, or geodesic) line connecting those points.

The solutions to both problems in plane geometry reduce to simple trigonometry and are valid for small areas on Earth's surface; on a sphere, solutions become significantly more complex as, for example, in the inverse problem, the azimuths differ going between the two end points along the arc of the connecting great circle.

The general solution is called the geodesic for the surface considered, and the differential equations for the geodesic are solvable numerically. On the ellipsoid of revolution, geodesics are expressible in terms of elliptic integrals, which are usually evaluated in terms of a series expansion — see, for example, Vincenty's formulae.

Observational concepts

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Axial tilt (or Obliquity), rotation axis, plane of orbit, celestial equator and ecliptic. Earth is shown as viewed from the Sun; the orbit direction is counter-clockwise (to the left).
Global gravity anomaly animation over oceans from the NASA's GRACE (Gravity Recovery and Climate Experiment)

As defined in geodesy (and also astronomy), some basic observational concepts like angles and coordinates include (most commonly from the viewpoint of a local observer):

  • Plumbline or vertical: (the line along) the direction of local gravity.
  • Zenith: the (direction to the) intersection of the upwards-extending gravity vector at a point and the celestial sphere.
  • Nadir: the (direction to the) antipodal point where the downward-extending gravity vector intersects the (obscured) celestial sphere.
  • Celestial horizon: a plane perpendicular to the gravity vector at a point.
  • Azimuth: the direction angle within the plane of the horizon, typically counted clockwise from the north (in geodesy and astronomy) or the south (in France).
  • Elevation: the angular height of an object above the horizon; alternatively: zenith distance equal to 90 degrees minus elevation.
  • Local topocentric coordinates: azimuth (direction angle within the plane of the horizon), elevation angle (or zenith angle), distance.
  • North celestial pole: the extension of Earth's (precessing and nutating) instantaneous spin axis extended northward to intersect the celestial sphere. (Similarly for the south celestial pole.)
  • Celestial equator: the (instantaneous) intersection of Earth's equatorial plane with the celestial sphere.
  • Meridian plane: any plane perpendicular to the celestial equator and containing the celestial poles.
  • Local meridian: the plane which contains the direction to the zenith and the celestial pole.

Measurements

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Variations in the gravity field of the Moon, from NASA
Gravity measurement devices, pendulum (left) and absolute gravimeter (right)
A relative gravimeter

The reference surface (level) used to determine height differences and height reference systems is known as mean sea level. The traditional spirit level directly produces such (for practical purposes most useful) heights above sea level; the more economical use of GPS instruments for height determination requires precise knowledge of the figure of the geoid, as GPS only gives heights above the GRS80 reference ellipsoid. As geoid determination improves, one may expect that the use of GPS in height determination shall increase, too.

The theodolite is an instrument used to measure horizontal and vertical (relative to the local vertical) angles to target points. In addition, the tachymeter determines, electronically or electro-optically, the distance to a target and is highly automated or even robotic in operations. Widely used for the same purpose is the method of free station position.

Commonly for local detail surveys, tachymeters are employed, although the old-fashioned rectangular technique using an angle prism and steel tape is still an inexpensive alternative. As mentioned, also there are quick and relatively accurate real-time kinematic (RTK) GPS techniques. Data collected are tagged and recorded digitally for entry into Geographic Information System (GIS) databases.

Geodetic GNSS (most commonly GPS) receivers directly produce 3D coordinates in a geocentric coordinate frame. One such frame is WGS84, as well as frames by the International Earth Rotation and Reference Systems Service (IERS). GNSS receivers have almost completely replaced terrestrial instruments for large-scale base network surveys.

To monitor the Earth's rotation irregularities and plate tectonic motions and for planet-wide geodetic surveys, methods of very-long-baseline interferometry (VLBI) measuring distances to quasars, lunar laser ranging (LLR) measuring distances to prisms on the Moon, and satellite laser ranging (SLR) measuring distances to prisms on artificial satellites, are employed.

Gravity is measured using gravimeters, of which there are two kinds. First are absolute gravimeters, based on measuring the acceleration of free fall (e.g., of a reflecting prism in a vacuum tube). They are used to establish vertical geospatial control or in the field. Second, relative gravimeters are spring-based and more common. They are used in gravity surveys over large areas — to establish the figure of the geoid over these areas. The most accurate relative gravimeters are called superconducting gravimeters, which are sensitive to one-thousandth of one-billionth of Earth-surface gravity. Twenty-some superconducting gravimeters are used worldwide in studying Earth's tides, rotation, interior, oceanic and atmospheric loading, as well as in verifying the Newtonian constant of gravitation.

In the future, gravity and altitude might become measurable using the special-relativistic concept of time dilation as gauged by optical clocks.

Units and measures on the ellipsoid

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The definition of latitude (φ) and longitude (λ) on an ellipsoid of revolution (or spheroid). The graticule spacing is 10 degrees. The latitude is defined as the angle between the normal to the ellipsoid and the equatorial plane.

Geographical latitude and longitude are stated in the units degree, minute of arc, and second of arc. They are angles, not metric measures, and describe the direction of the local normal to the reference ellipsoid of revolution. This direction is approximately the same as the direction of the plumbline, i.e., local gravity, which is also the normal to the geoid surface. For this reason, astronomical position determination – measuring the direction of the plumbline by astronomical means – works reasonably well when one also uses an ellipsoidal model of the figure of the Earth.

One geographical mile, defined as one minute of arc on the equator, equals 1,855.32571922 m. One nautical mile is one minute of astronomical latitude. The radius of curvature of the ellipsoid varies with latitude, being the longest at the pole and the shortest at the equator same as with the nautical mile.

A metre was originally defined as the 10-millionth part of the length from the equator to the North Pole along the meridian through Paris (the target was not quite reached in actual implementation, as it is off by 200 ppm in the current definitions). This situation means that one kilometre roughly equals (1/40,000) * 360 * 60 meridional minutes of arc, or 0.54 nautical miles. (This is not exactly so as the two units had been defined on different bases, so the international nautical mile is 1,852 m exactly, which corresponds to rounding the quotient from 1,000/0.54 m to four digits).

Temporal changes

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Global plate tectonic movement using GPS
How very-long-baseline interferometry (VLBI) works

Various techniques are used in geodesy to study temporally changing surfaces, bodies of mass, physical fields, and dynamical systems. Points on Earth's surface change their location due to a variety of mechanisms:

  • Continental plate motion, plate tectonics[9]
  • The episodic motion of tectonic origin, especially close to fault lines
  • Periodic effects due to tides and tidal loading[10]
  • Postglacial land uplift due to isostatic adjustment
  • Mass variations due to hydrological changes, including the atmosphere, cryosphere, land hydrology, and oceans
  • Sub-daily polar motion[11]
  • Length-of-day variability[12]
  • Earth's center-of-mass (geocenter) variations[13]
  • Anthropogenic movements such as reservoir construction or petroleum or water extraction
A NASA project manager talks about his work for the Space Geodesy Project, including an overview of its four fundamental techniques: GPS, VLBI, LLR/SLR, and DORIS.

Geodynamics is the discipline that studies deformations and motions of Earth's crust and its solidity as a whole. Often the study of Earth's irregular rotation is included in the above definition. Geodynamical studies require terrestrial reference frames[14] realized by the stations belonging to the Global Geodetic Observing System (GGOS[15]).

Techniques for studying geodynamic phenomena on global scales include:

Notable geodesists

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See also

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References

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Further reading

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Revisions and contributorsEdit on WikipediaRead on Wikipedia
from Grokipedia
Geodesy is the scientific discipline that measures and represents the Earth's geometric shape, orientation in space, gravity field, and their variations over time, providing a foundational framework for understanding planetary and dynamics. The field originated in , where scholars like estimated the Earth's circumference around 240 BCE using geometric principles and observations of the sun's angle, laying early groundwork for quantifying the planet's size and form. By the , expeditions such as those led by in Lapland and Charles Marie de at the confirmed the Earth's oblate spheroid shape through arc measurements, resolving debates on whether it was perfectly spherical. The marked a shift with the advent of satellite technology, enabling global-scale observations that refined models like the (WGS 84), which defines an with an equatorial radius of approximately 6,378 kilometers and a of 1/298.257. Geodesy encompasses several interconnected branches, including geometric geodesy, which focuses on determining the Earth's surface coordinates and shape using techniques like and ranging; physical geodesy, which studies the gravity field and the —an irregular equipotential surface approximating mean —to account for mass distribution and deflections; and dynamic geodesy, which examines the Earth's rotation, , and temporal changes such as crustal deformations. These branches rely on precise datums, such as the of 1983 (NAD 83), to establish reference frameworks for consistent positioning worldwide. In modern practice, geodesy employs space-based tools like the (GPS), which uses a constellation of satellites to achieve centimeter-level accuracy in positioning, alongside methods such as (VLBI) and for monitoring geophysical phenomena. Applications span navigation and mapping, where it supports the U.S. National Spatial Reference System for boundary delineation and shoreline charting; hazard assessment, including and volcanic monitoring through millimeter-scale detection of ground motion; and climate studies, tracking sea-level rise, ice mass loss, and at rates of several millimeters per year.

Fundamentals

Definition and Scope

Geodesy is the scientific discipline that deals with the measurement and representation of the 's , physics, and temporal variations, including its , field, and , to determine accurate spatial positions on and near the surface. This encompasses monitoring changes in these properties over time and space, extending to other celestial bodies as well. The field integrates observations from ground-based and space-based techniques to model the as a dynamic . The scope of geodesy is divided into several key branches that address distinct aspects of Earth's properties and measurements. Physical geodesy focuses on the field and the , which represents the surface of Earth's . Geometric geodesy deals with the precise determination of Earth's shape, size, and spatial orientation through coordinate systems. Dynamic geodesy examines Earth's , , and tidal effects, capturing temporal variations. , a cross-cutting branch, employs space-based observations to enhance global-scale measurements across these areas. Geodesy maintains strong interdisciplinary connections with fields such as for precise land mapping, for studying tectonic movements, for sea-level monitoring, and for positioning systems. These links enable applications in creating accurate topographic maps, supporting global navigation satellite systems, and tracking environmental changes like ice mass loss and sea-level rise. A core concept in modern geodesy is achieving positioning accuracy to sub-millimeter levels, particularly through Global Navigation Satellite Systems (GNSS) in static configurations, which underpin high-precision geodetic networks worldwide.

Historical Development

The origins of geodesy trace back to ancient civilizations, where early scholars sought to determine the Earth's size and form through geometric measurements. In the 3rd century BCE, , chief librarian at , calculated the by comparing the angle of the sun's rays at noon in Syene (modern ) and , assuming a distance of about 500 miles between the cities; his estimate of roughly 25,000 miles was remarkably close to the modern value of 24,901 miles for the equatorial circumference. Greek astronomers like further advanced the field in the 2nd century BCE by developing the concepts of , using stellar observations to establish a grid system for mapping positions on the Earth's surface. Roman contributions, such as those by in the 2nd century CE, refined these ideas into a geocentric model that influenced for centuries, though it underestimated the at around 18,000 miles. During the 17th and 18th centuries, theoretical and empirical advances solidified the understanding of 's shape as an oblate spheroid. proposed in his 1687 that gravitational forces would flatten the at the poles due to its rotation, hypothesizing an oblateness that sparked international debate. To test this, the organized expeditions in the and : Pierre Louis Moreau de Maupertuis led a team to Lapland in 1736–1737 to measure a northern arc of the meridian, while Charles Marie de La Condamine's group surveyed a southern arc near the equator in from 1735 to 1744; their findings confirmed a degree of latitude was shorter at the equator than at the poles, validating the oblate spheroid model with a flattening of about 1/300. The 19th century marked the institutionalization of geodesy through mathematical refinements and national mapping efforts. revolutionized geodetic computations in the early 1800s by developing the method, which minimized errors in large-scale networks and became a cornerstone for precise . In the United States, the Coast Survey was established in 1807 under Ferdinand Hassler, the nation's first scientific agency dedicated to coastal mapping and geodetic control; it introduced rigorous techniques across , laying the groundwork for continental-scale datums. Alexander Ross Clarke's 1866 ellipsoid, with a semi-major axis of 6,378,206 meters and flattening of 1/295, provided a widely adopted for North American surveys, influencing the of 1927. In the 20th century, technological innovations expanded geodesy's precision and scope. Following , inertial navigation systems (INS), initially developed for military applications like the , were adapted for geodetic surveying in the 1950s and ; devices such as the Litton INS enabled rapid, autonomous position fixes in remote areas, achieving accuracies of tens of meters over short baselines through gyroscopic and accelerometric measurements. The launch of in 1957 by the initiated the satellite era, as its orbital perturbations provided the first global data on Earth's , refining the oblateness estimate to a flattening reciprocal of 298. The U.S. Navy's Transit system, operational from the early , used Doppler shifts from polar-orbiting satellites to determine positions with 20-meter accuracy, supporting the 1960 (WGS 60) datum. The 1970s and 1980s saw the rise of the (GPS), transforming geodesy into a global, real-time discipline. Conceived in the 1970s by the U.S. Department of Defense, GPS built on Transit technology with a constellation of medium-Earth-orbit satellites broadcasting precise timing signals; initial development included launches of prototype Block I satellites starting in 1978, achieving full operational capability by 1995 but enabling geodetic applications from the mid-1980s with sub-meter static positioning via carrier-phase measurements. This shift from ground-based to space-based methods allowed for centimeter-level accuracy in tectonic studies and datum realizations, culminating in the WGS 84 reference frame. Into the late 20th and early 21st centuries, satellite missions advanced field modeling. The Gravity Recovery and Climate Experiment (GRACE), launched in 2002 by and the , used twin satellites in a low- to measure inter-satellite variations caused by anomalies, providing monthly global maps of 's distribution with resolutions down to 300–400 km and sensitivities to changes as small as 1 cm of water equivalent. Its successor, GRACE Follow-On (GRACE-FO), launched in 2018, continued these observations with enhanced laser for inter-satellite ranging, maintaining data continuity through 2025. By 2025, recent milestones include the integration of (AI) in geodetic data processing, where algorithms enhance the quality of observations from GNSS and by automating detection and , as pursued by the International Association of Geodesy (IAG)'s AI4G initiative to improve product accuracy for system monitoring. Advancements in quantum , leveraging cold-atom , have enabled portable sensors achieving 10^{-8} m/s² precision for field measurements, supporting next-generation satellite missions like proposed quantum-enhanced gradiometers for finer resolution of geoid undulations.

Earth's Geometric and Gravitational Models

Geoid

The is defined as the surface of the Earth's field that best approximates mean in the absence of currents, , and atmospheric effects, extending continuously under landmasses as a hypothetical surface of constant . This surface undulates irregularly due to uneven mass distribution within the , such as variations in crustal density and , resulting in deviations from a smooth or . Physically, the geoid arises from the total gravity potential WW, which combines the gravitational potential VV generated by the Earth's mass (external to the surface) and the centrifugal potential Φ\Phi due to Earth's . On the geoid, WW equals a constant value W0W_0, typically corresponding to global mean sea level. The relationship between the geoid and heights is described by Bruns' formula, which expresses the orthometric height HH above the at a point PP as H=W0WPγ,H = \frac{W_0 - W_P}{\gamma}, where WPW_P is the gravity potential at PP and γ\gamma is the normal gravity (approximating actual on the ). This formula underscores the geoid's role as the zero-level reference for orthometric heights, which measure elevation relative to sea level along plumb lines. Geoid determination involves several methods, each leveraging different observations of the field. Gravimetric methods compute geoid undulations using anomalies through Stokes' integral, which integrates the anomalous over the Earth's surface after removing long-wavelength effects from global models and restoring topographic contributions via the remove-compute-restore technique. Astrogeodetic methods derive local geoid heights from astronomic observations of vertical deflections, combining them with data for high-resolution regional models, particularly in areas with sparse coverage like mountainous . -based approaches, such as those from the Gravity Recovery and Climate Experiment (GRACE), its successor GRACE Follow-On (GRACE-FO, ongoing as of 2025), and Gravity Field and Steady-State Ocean Circulation Explorer (GOCE) missions, provide global field data that inform high-degree spherical harmonic models like the Earth Gravitational Model 2008 (EGM2008), achieving resolutions down to about 10 km. Geoid undulations, or the vertical separations from a reference , typically range from -100 to +100 meters globally, reflecting imbalances in the field. These undulations can be decomposed into components due to anomalous mass distributions ( effects) and topographic loading, with the latter often corrected using digital elevation models to isolate the true signal. The serves as the fundamental reference for orthometric heights, enabling the conversion of satellite-derived ellipsoidal heights to physically meaningful elevations above , which is essential for , , and . It also plays a critical role in unifying global geodetic datums by providing a consistent vertical framework that bridges regional height systems and facilitates accurate realization of international reference frames.

Reference Ellipsoid

The reference ellipsoid is a of an that approximates the 's overall shape for geodetic purposes, defined by its semi-major axis aa (the equatorial ) and f=(ab)/af = (a - b)/a, where bb is the semi-minor axis (the polar ). This model simplifies computations by representing the as a smooth, rotationally symmetric surface, with typical parameters including a6378a \approx 6378 km and b6357b \approx 6357 km to reflect the planet's due to . The dynamical form factor, such as the second-degree gravitational harmonic J2J_2, further refines the model by incorporating rotational effects, with J2=1.08263×103J_2 = 1.08263 \times 10^{-3} in the (GRS80). The surface of the reference ellipsoid is mathematically described by the equation x2+y2a2+z2b2=1,\frac{x^2 + y^2}{a^2} + \frac{z^2}{b^2} = 1, where the zz-axis aligns with the axis, providing a geometric foundation for positioning calculations. Historical reference ellipsoids were developed based on arc measurements and gravitational to fit regional or global observations. The Bessel ellipsoid of 1841, with a=6377397.155a = 6377397.155 m and 1/f=299.15281281/f = 299.1528128, was widely used for European and Asian networks due to its fit to continental measurements. The Clarke ellipsoids, proposed by Alexander Ross Clarke, include the 1866 version (a=6378206.4a = 6378206.4 m, 1/f=294.978698211/f = 294.97869821) optimized for North American surveys, and the 1880 version (a=6378249.2a = 6378249.2 m, 1/f=2931/f = 293) for global applications. A modern standard, the WGS84 ellipsoid (adopted in 1984), uses a=6378137a = 6378137 m and f=1/298.257223563f = 1/298.257223563, derived from and gravitational for worldwide consistency. As the foundational geometric surface in geodesy, the reference serves as the basis for projections, which transform its curved coordinates into flat representations, and for coordinate transformations between different systems. It defines ellipsoidal heights measured perpendicular to this surface, which differ from orthometric heights tied to the by the ellipsoidal-geoid separation. Contemporary refinements to reference ellipsoids, such as those in the International Terrestrial Reference Frame (ITRF), build on the GRS80 parameters and integrate (GPS) observations to achieve sub-centimeter accuracy in realizations like ITRF2020, enabling precise global positioning.

Reference Systems and Datums

Coordinate Systems

In geodesy, coordinate systems provide the mathematical framework for specifying positions on or near the Earth's surface in three dimensions. The two primary types are Cartesian and , both defined relative to a reference that approximates the Earth's shape. Cartesian coordinates, often in the Earth-Centered, Earth-Fixed (ECEF) system, use orthogonal axes (, Z) with the origin at the Earth's ; the Z-axis aligns with the Earth's rotation axis (positive toward the ), the X-axis points toward the at the , and the Y-axis completes the right-handed system. , in contrast, consist of φ (angle from the to the point along the ellipsoid normal), longitude λ (angle from the in the equatorial plane), and ellipsoidal height h (distance along the normal from the ellipsoid surface). Transformations between geodetic and Cartesian coordinates are essential for computations in positioning and . The conversion from geodetic (φ, λ, h) to ECEF Cartesian (X, Y, Z) coordinates is given by: X=(N+h)cosϕcosλ,Y=(N+h)cosϕsinλ,Z=(N(1e2)+h)sinϕ,\begin{align*} X &= (N + h) \cos \phi \cos \lambda, \\ Y &= (N + h) \cos \phi \sin \lambda, \\ Z &= \left( N (1 - e^2) + h \right) \sin \phi, \end{align*} where N=a1e2sin2ϕN = \frac{a}{\sqrt{1 - e^2 \sin^2 \phi}}
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