In geography, **latitude** is a coordinate that specifies the north–south position of a point on the surface of the Earth or another celestial body. Latitude is given as an angle that ranges from −90° at the south pole to 90° at the north pole, with 0° at the Equator. Lines of constant latitude, or *parallels*, run east–west as circles parallel to the equator. Latitude and longitude are used together as a coordinate pair to specify a location on the surface of the Earth.

- Background
- Determination
- Latitude on the sphere
- The graticule on the sphere
- Named latitudes on the Earth
- Latitude on the ellipsoid
- Ellipsoids
- The geometry of the ellipsoid
- Geodetic and geocentric latitudes
- Meridian distance
- Meridian distance on the sphere
- Meridian distance on the ellipsoid
- Auxiliary latitudes
- Geocentric latitude
- Parametric latitude (or reduced latitude)
- Rectifying latitude
- Authalic latitude
- Conformal latitude
- Isometric latitude
- Inverse formulae and series
- Numerical comparison of auxiliary latitudes
- Latitude and coordinate systems
- Geodetic coordinates
- Spherical polar coordinates
- Ellipsoidal-harmonic coordinates
- Coordinate conversions
- Astronomical latitude
- See also
- References
- Footnotes
- Citations
- External links

On its own, the term "latitude" normally refers to the *geodetic latitude* as defined below. Briefly, the geodetic latitude of a point is the angle formed between the vector perpendicular (or * normal *) to the ellipsoidal surface from the point, and the plane of the equator.

Two levels of abstraction are employed in the definitions of latitude and longitude. In the first step the physical surface is modeled by the geoid, a surface which approximates the mean sea level over the oceans and its continuation under the land masses. The second step is to approximate the geoid by a mathematically simpler reference surface. The simplest choice for the reference surface is a sphere, but the geoid is more accurately modeled by an ellipsoid of revolution. The definitions of latitude and longitude on such reference surfaces are detailed in the following sections. Lines of constant latitude and longitude together constitute a graticule on the reference surface. The latitude of a point on the *actual* surface is that of the corresponding point on the reference surface, the correspondence being along the normal to the reference surface, which passes through the point on the physical surface. Latitude and longitude together with some specification of height constitute a geographic coordinate system as defined in the specification of the ISO 19111 standard.^{ [1] }

Since there are many different reference ellipsoids, the precise latitude of a feature on the surface is not unique: this is stressed in the ISO standard which states that "without the full specification of the coordinate reference system, coordinates (that is latitude and longitude) are ambiguous at best and meaningless at worst". This is of great importance in accurate applications, such as a Global Positioning System (GPS), but in common usage, where high accuracy is not required, the reference ellipsoid is not usually stated.

In English texts, the latitude angle, defined below, is usually denoted by the Greek lower-case letter phi (ϕ or φ). It is measured in degrees, minutes and seconds or decimal degrees, north or south of the equator. For navigational purposes positions are given in degrees and decimal minutes. For instance, The Needles lighthouse is at 50°39.734′ N 001°35.500′ W.^{ [2] }

This article relates to coordinate systems for the Earth: it may be adapted to cover the Moon, planets and other celestial objects (planetographic latitude).

For a brief history, see History of latitude.

In celestial navigation, latitude is determined with the meridian altitude method. More precise measurement of latitude requires an understanding of the gravitational field of the Earth, either to set up theodolites or to determine GPS satellite orbits. The study of the figure of the Earth together with its gravitational field is the science of geodesy.

The graticule is formed by the lines of constant latitude and constant longitude, which are constructed with reference to the rotation axis of the Earth. The primary reference points are the poles where the axis of rotation of the Earth intersects the reference surface. Planes which contain the rotation axis intersect the surface at the meridians; and the angle between any one meridian plane and that through Greenwich (the Prime Meridian) defines the longitude: meridians are lines of constant longitude. The plane through the centre of the Earth and perpendicular to the rotation axis intersects the surface at a great circle called the Equator. Planes parallel to the equatorial plane intersect the surface in circles of constant latitude; these are the parallels. The Equator has a latitude of 0°, the North Pole has a latitude of 90° North (written 90° N or +90°), and the South Pole has a latitude of 90° South (written 90° S or −90°). The latitude of an arbitrary point is the angle between the equatorial plane and the normal to the surface at that point: the normal to the surface of the sphere is along the radial vector.

The latitude, as defined in this way for the sphere, is often termed the spherical latitude, to avoid ambiguity with the geodetic latitude and the auxiliary latitudes defined in subsequent sections of this article.

Besides the equator, four other parallels are of significance:

Arctic Circle 66° 34′ (66.57°) N Tropic of Cancer 23° 26′ (23.43°) N Tropic of Capricorn 23° 26′ (23.43°) S Antarctic Circle 66° 34′ (66.57°) S

The plane of the Earth's orbit about the Sun is called the ecliptic, and the plane perpendicular to the rotation axis of the Earth is the equatorial plane. The angle between the ecliptic and the equatorial plane is called variously the axial tilt, the obliquity, or the inclination of the ecliptic, and it is conventionally denoted by i. The latitude of the tropical circles is equal to i and the latitude of the polar circles is its complement (90° - *i*). The axis of rotation varies slowly over time and the values given here are those for the current epoch. The time variation is discussed more fully in the article on axial tilt.^{ [lower-alpha 1] }

The figure shows the geometry of a cross-section of the plane perpendicular to the ecliptic and through the centres of the Earth and the Sun at the December solstice when the Sun is overhead at some point of the Tropic of Capricorn. The south polar latitudes below the Antarctic Circle are in daylight, whilst the north polar latitudes above the Arctic Circle are in night. The situation is reversed at the June solstice, when the Sun is overhead at the Tropic of Cancer. Only at latitudes in between the two tropics is it possible for the Sun to be directly overhead (at the zenith).

On map projections there is no universal rule as to how meridians and parallels should appear. The examples below show the named parallels (as red lines) on the commonly used Mercator projection and the Transverse Mercator projection. On the former the parallels are horizontal and the meridians are vertical, whereas on the latter there is no exact relationship of parallels and meridians with horizontal and vertical: both are complicated curves.

Normal Mercator | Transverse Mercator | |||
---|---|---|---|---|

\ |

In 1687 Isaac Newton published the * Philosophiæ Naturalis Principia Mathematica *, in which he proved that a rotating self-gravitating fluid body in equilibrium takes the form of an oblate ellipsoid.^{ [3] } (This article uses the term *ellipsoid* in preference to the older term *spheroid*.) Newton's result was confirmed by geodetic measurements in the 18th century. (See Meridian arc.) An oblate ellipsoid is the three-dimensional surface generated by the rotation of an ellipse about its shorter axis (minor axis). "Oblate ellipsoid of revolution" is abbreviated to 'ellipsoid' in the remainder of this article. (Ellipsoids which do not have an axis of symmetry are termed triaxial.)

Many different reference ellipsoids have been used in the history of geodesy. In pre-satellite days they were devised to give a good fit to the geoid over the limited area of a survey but, with the advent of GPS, it has become natural to use reference ellipsoids (such as WGS84) with centre at the centre of mass of the Earth and minor axis aligned to the rotation axis of the Earth. These geocentric ellipsoids are usually within 100 m (330 ft) of the geoid. Since latitude is defined with respect to an ellipsoid, the position of a given point is different on each ellipsoid: one cannot exactly specify the latitude and longitude of a geographical feature without specifying the ellipsoid used. Many maps maintained by national agencies are based on older ellipsoids, so one must know how the latitude and longitude values are transformed from one ellipsoid to another. GPS handsets include software to carry out datum transformations which link WGS84 to the local reference ellipsoid with its associated grid.

The shape of an ellipsoid of revolution is determined by the shape of the ellipse which is rotated about its minor (shorter) axis. Two parameters are required. One is invariably the equatorial radius, which is the semi-major axis, a. The other parameter is usually (1) the polar radius or semi-minor axis, b; or (2) the (first) flattening, f; or (3) the eccentricity, e. These parameters are not independent: they are related by

Many other parameters (see ellipse, ellipsoid) appear in the study of geodesy, geophysics and map projections but they can all be expressed in terms of one or two members of the set a, b, f and e. Both f and e are small and often appear in series expansions in calculations; they are of the order 1/298 and 0.0818 respectively. Values for a number of ellipsoids are given in Figure of the Earth. Reference ellipsoids are usually defined by the semi-major axis and the *inverse* flattening, 1/*f*. For example, the defining values for the WGS84 ellipsoid, used by all GPS devices, are^{ [4] }

- a (equatorial radius): 6378137.0 m exactly
- 1/
*f*(inverse flattening): 298.257223563 exactly

from which are derived

- b (polar radius): 6356752.31425 m
*e*^{2}(eccentricity squared): 0.00669437999014

The difference between the semi-major and semi-minor axes is about 21 km (13 miles) and as fraction of the semi-major axis it equals the flattening; on a computer monitor the ellipsoid could be sized as 300 by 299 pixels. This would barely be distinguishable from a 300-by-300-pixel sphere, so illustrations usually exaggerate the flattening.

The graticule on the ellipsoid is constructed in exactly the same way as on the sphere. The normal at a point on the surface of an ellipsoid does not pass through the centre, except for points on the equator or at the poles, but the definition of latitude remains unchanged as the angle between the normal and the equatorial plane. The terminology for latitude must be made more precise by distinguishing:

*Geodetic latitude*: the angle between the normal and the equatorial plane. The standard notation in English publications is ϕ. This is the definition assumed when the word latitude is used without qualification. The definition must be accompanied with a specification of the ellipsoid.*Geocentric latitude*(also known as*spherical latitude*, after the 3D polar angle): the angle between the radius (from centre to the point on the surface) and the equatorial plane. (Figure below). There is no standard notation: examples from various texts include θ, ψ, q, ϕ′,*ϕ*_{c},*ϕ*_{g}. This article uses θ.

**Geographic latitude** must be used with care, as some authors use it as a synonym for geodetic latitude whilst others use it as an alternative to the astronomical latitude. "Latitude" (unqualified) should normally refer to the geodetic latitude.

The importance of specifying the reference datum may be illustrated by a simple example. On the reference ellipsoid for WGS84, the centre of the Eiffel Tower has a geodetic latitude of 48° 51′ 29″ N, or 48.8583° N and longitude of 2° 17′ 40″ E or 2.2944°E. The same coordinates on the datum ED50 define a point on the ground which is 140 metres (460 feet) distant from the tower.^{[ citation needed ]} A web search may produce several different values for the latitude of the tower; the reference ellipsoid is rarely specified.

The length of a degree of latitude depends on the figure of the Earth assumed.

On the sphere the normal passes through the centre and the latitude (ϕ) is therefore equal to the angle subtended at the centre by the meridian arc from the equator to the point concerned. If the meridian distance is denoted by *m*(*ϕ*) then

where R denotes the mean radius of the Earth. R is equal to 6,371 km or 3,959 miles. No higher accuracy is appropriate for R since higher-precision results necessitate an ellipsoid model. With this value for R the meridian length of 1 degree of latitude on the sphere is 111.2 km (69.1 statute miles) (60.0 nautical miles). The length of 1 minute of latitude is 1.853 km (1.151 statute miles) (1.00 nautical miles), while the length of 1 second of latitude is 30.8 m or 101 feet (see nautical mile).

In Meridian arc and standard texts^{ [5] }^{ [6] }^{ [7] } it is shown that the distance along a meridian from latitude ϕ to the equator is given by (ϕ in radians)

where *M*(*ϕ*) is the meridional radius of curvature.

The * quarter meridian * distance from the equator to the pole is

For WGS84 this distance is 10001.965729 km.

The evaluation of the meridian distance integral is central to many studies in geodesy and map projection. It can be evaluated by expanding the integral by the binomial series and integrating term by term: see Meridian arc for details. The length of the meridian arc between two given latitudes is given by replacing the limits of the integral by the latitudes concerned. The length of a *small* meridian arc is given by^{ [6] }^{ [7] }

Δ^{1}_{lat} | Δ^{1}_{long} | |
---|---|---|

0° | 110.574 km | 111.320 km |

15° | 110.649 km | 107.550 km |

30° | 110.852 km | 96.486 km |

45° | 111.132 km | 78.847 km |

60° | 111.412 km | 55.800 km |

75° | 111.618 km | 28.902 km |

90° | 111.694 km | 0.000 km |

When the latitude difference is 1 degree, corresponding to π/180 radians, the arc distance is about

The distance in metres (correct to 0.01 metre) between latitudes − 0.5 degrees and + 0.5 degrees on the WGS84 spheroid is

The variation of this distance with latitude (on WGS84) is shown in the table along with the length of a degree of longitude (east–west distance):

A calculator for any latitude is provided by the U.S. Government's National Geospatial-Intelligence Agency (NGA).^{ [8] }

The following graph illustrates the variation of both a degree of latitude and a degree of longitude with latitude.

There are six **auxiliary latitudes** that have applications to special problems in geodesy, geophysics and the theory of map projections:

- Geocentric latitude
- Parametric (or reduced) latitude
- Rectifying latitude
- Authalic latitude
- Conformal latitude
- Isometric latitude

The definitions given in this section all relate to locations on the reference ellipsoid but the first two auxiliary latitudes, like the geodetic latitude, can be extended to define a three-dimensional geographic coordinate system as discussed below. The remaining latitudes are not used in this way; they are used *only* as intermediate constructs in map projections of the reference ellipsoid to the plane or in calculations of geodesics on the ellipsoid. Their numerical values are not of interest. For example, no one would need to calculate the authalic latitude of the Eiffel Tower.

The expressions below give the auxiliary latitudes in terms of the geodetic latitude, the semi-major axis, a, and the eccentricity, e. (For inverses see below.) The forms given are, apart from notational variants, those in the standard reference for map projections, namely "Map projections: a working manual" by J. P. Snyder.^{ [9] } Derivations of these expressions may be found in Adams^{ [10] } and online publications by Osborne^{ [6] } and Rapp.^{ [7] }

The **geocentric latitude** is the angle between the equatorial plane and the radius from the centre to a point of interest.

When the point is on the surface of the ellipsoid, the relation between the geocentric latitude (θ) and the geodetic latitude (ϕ) is:

For points not on the surface of the ellipsoid, the relationship involves additionally the ellipsoidal height *h*:

where N is the prime vertical radius of curvature. The geodetic and geocentric latitudes are equal at the equator and at the poles but at other latitudes they differ by a few minutes of arc. Taking the value of the squared eccentricity as 0.0067 (it depends on the choice of ellipsoid) the maximum difference of may be shown to be about 11.5 minutes of arc at a geodetic latitude of approximately 45° 6′.^{ [lower-alpha 2] }

The **parametric latitude** or **reduced latitude**, β, is defined by the radius drawn from the centre of the ellipsoid to that point Q on the surrounding sphere (of radius a) which is the projection parallel to the Earth's axis of a point P on the ellipsoid at latitude ϕ. It was introduced by Legendre^{ [11] } and Bessel^{ [12] } who solved problems for geodesics on the ellipsoid by transforming them to an equivalent problem for spherical geodesics by using this smaller latitude. Bessel's notation, *u*(*ϕ*), is also used in the current literature. The parametric latitude is related to the geodetic latitude by:^{ [6] }^{ [7] }

The alternative name arises from the parameterization of the equation of the ellipse describing a meridian section. In terms of Cartesian coordinates p, the distance from the minor axis, and z, the distance above the equatorial plane, the equation of the ellipse is:

The Cartesian coordinates of the point are parameterized by

Cayley suggested the term *parametric latitude* because of the form of these equations.^{ [13] }

The parametric latitude is not used in the theory of map projections. Its most important application is in the theory of ellipsoid geodesics, (Vincenty, Karney^{ [14] }).

The **rectifying latitude**, μ, is the meridian distance scaled so that its value at the poles is equal to 90 degrees or π/2 radians:

where the meridian distance from the equator to a latitude ϕ is (see Meridian arc)

and the length of the meridian quadrant from the equator to the pole (the polar distance) is

Using the rectifying latitude to define a latitude on a sphere of radius

defines a projection from the ellipsoid to the sphere such that all meridians have true length and uniform scale. The sphere may then be projected to the plane with an equirectangular projection to give a double projection from the ellipsoid to the plane such that all meridians have true length and uniform meridian scale. An example of the use of the rectifying latitude is the equidistant conic projection. (Snyder, Section 16).^{ [9] } The rectifying latitude is also of great importance in the construction of the Transverse Mercator projection.

The **authalic latitude** (after the Greek for "same area"), ξ, gives an equal-area projection to a sphere.

where

and

and the radius of the sphere is taken as

An example of the use of the authalic latitude is the Albers equal-area conic projection.^{ [9] }^{: §14 }

The **conformal latitude**, χ, gives an angle-preserving (conformal) transformation to the sphere. ^{ [15] }

where gd(*x*) is the Gudermannian function. (See also Mercator projection.)

The conformal latitude defines a transformation from the ellipsoid to a sphere of *arbitrary* radius such that the angle of intersection between any two lines on the ellipsoid is the same as the corresponding angle on the sphere (so that the shape of *small* elements is well preserved). A further conformal transformation from the sphere to the plane gives a conformal double projection from the ellipsoid to the plane. This is not the only way of generating such a conformal projection. For example, the 'exact' version of the Transverse Mercator projection on the ellipsoid is not a double projection. (It does, however, involve a generalisation of the conformal latitude to the complex plane).

The **isometric latitude**, ψ, is used in the development of the ellipsoidal versions of the normal Mercator projection and the Transverse Mercator projection. The name "isometric" arises from the fact that at any point on the ellipsoid equal increments of ψ and longitude λ give rise to equal distance displacements along the meridians and parallels respectively. The graticule defined by the lines of constant ψ and constant λ, divides the surface of the ellipsoid into a mesh of squares (of varying size). The isometric latitude is zero at the equator but rapidly diverges from the geodetic latitude, tending to infinity at the poles. The conventional notation is given in Snyder (page 15):^{ [9] }

For the *normal* Mercator projection (on the ellipsoid) this function defines the spacing of the parallels: if the length of the equator on the projection is E (units of length or pixels) then the distance, y, of a parallel of latitude ϕ from the equator is

The isometric latitude ψ is closely related to the conformal latitude χ:

The formulae in the previous sections give the auxiliary latitude in terms of the geodetic latitude. The expressions for the geocentric and parametric latitudes may be inverted directly but this is impossible in the four remaining cases: the rectifying, authalic, conformal, and isometric latitudes. There are two methods of proceeding.

- The first is a numerical inversion of the defining equation for each and every particular value of the auxiliary latitude. The methods available are fixed-point iteration and Newton–Raphson root finding.
- When converting from isometric or conformal to geodetic, two iterations of Newton-Raphson gives double precision accuracy.
^{ [16] }

- When converting from isometric or conformal to geodetic, two iterations of Newton-Raphson gives double precision accuracy.
- The other, more useful, approach is to express the auxiliary latitude as a series in terms of the geodetic latitude and then invert the series by the method of Lagrange reversion. Such series are presented by Adams who uses Taylor series expansions and gives coefficients in terms of the eccentricity.
^{ [10] }Orihuela^{ [17] }gives series for the conversions between all pairs of auxiliary latitudes in terms of the third flattening,*n*= (*a*-*b*)/(*a*+*b*). Karney^{ [18] }establishes that the truncation errors for such series are consistently smaller that the equivalent series in terms of the eccentricity. The series method is not applicable to the isometric latitude and one must find the conformal latitude in an intermediate step.^{ [6] }

The plot to the right shows the difference between the geodetic latitude and the auxiliary latitudes other than the isometric latitude (which diverges to infinity at the poles) for the case of the WGS84 ellipsoid. The differences shown on the plot are in arc minutes. In the Northern hemisphere (positive latitudes), *θ* ≤ *χ* ≤ *μ* ≤ *ξ* ≤ *β* ≤ *ϕ*; in the Southern hemisphere (negative latitudes), the inequalities are reversed, with equality at the equator and the poles. Although the graph appears symmetric about 45°, the minima of the curves actually lie between 45° 2′ and 45° 6′. Some representative data points are given in the table below. The conformal and geocentric latitudes are nearly indistinguishable, a fact that was exploited in the days of hand calculators to expedite the construction of map projections.^{ [9] }^{: 108 }

To first order in the flattening *f*, the auxiliary latitudes can be expressed as *ζ* = *ϕ* − *Cf* sin 2*ϕ* where the constant *C* takes on the values [1⁄2, 2⁄3, 3⁄4, 1, 1] for *ζ* = [*β*, *ξ*, *μ*, *χ*, *θ*].

ϕ | Parametricβ − ϕ | Authalicξ − ϕ | Rectifyingμ − ϕ | Conformalχ − ϕ | Geocentricθ − ϕ |
---|---|---|---|---|---|

0° | 0.00′ | 0.00′ | 0.00′ | 0.00′ | 0.00′ |

15° | −2.88′ | −3.84′ | −4.32′ | −5.76′ | −5.76′ |

30° | −5.00′ | −6.66′ | −7.49′ | −9.98′ | −9.98′ |

45° | −5.77′ | −7.70′ | −8.66′ | −11.54′ | −11.55′ |

60° | −5.00′ | −6.67′ | −7.51′ | −10.01′ | −10.02′ |

75° | −2.89′ | −3.86′ | −4.34′ | −5.78′ | −5.79′ |

90° | 0.00′ | 0.00′ | 0.00′ | 0.00′ | 0.00′ |

The geodetic latitude, or any of the auxiliary latitudes defined on the reference ellipsoid, constitutes with longitude a two-dimensional coordinate system on that ellipsoid. To define the position of an arbitrary point it is necessary to extend such a coordinate system into three dimensions. Three latitudes are used in this way: the geodetic, geocentric and parametric latitudes are used in geodetic coordinates, spherical polar coordinates and ellipsoidal coordinates respectively.

At an arbitrary point P consider the line PN which is normal to the reference ellipsoid. The geodetic coordinates P(*ɸ*,*λ*,*h*) are the latitude and longitude of the point N on the ellipsoid and the distance PN. This height differs from the height above the geoid or a reference height such as that above mean sea level at a specified location. The direction of PN will also differ from the direction of a vertical plumb line. The relation of these different heights requires knowledge of the shape of the geoid and also the gravity field of the Earth.

The geocentric latitude θ is the complement of the *polar angle* or * colatitude *θ′ in conventional spherical polar coordinates in which the coordinates of a point are P(*r*,*θ*′,*λ*) where r is the distance of P from the centre O, θ′ is the angle between the radius vector and the polar axis and λ is longitude. Since the normal at a general point on the ellipsoid does not pass through the centre it is clear that points P' on the normal, which all have the same geodetic latitude, will have differing geocentric latitudes. Spherical polar coordinate systems are used in the analysis of the gravity field.

The parametric latitude can also be extended to a three-dimensional coordinate system. For a point P not on the reference ellipsoid (semi-axes OA and OB) construct an auxiliary ellipsoid which is confocal (same foci F, F′) with the reference ellipsoid: the necessary condition is that the product ae of semi-major axis and eccentricity is the same for both ellipsoids. Let u be the semi-minor axis (OD) of the auxiliary ellipsoid. Further let β be the parametric latitude of P on the auxiliary ellipsoid. The set (*u*,*β*,*λ*) define the **ellipsoidal-harmonic coordinates**^{ [19] } or simply *ellipsoidal coordinates*^{ [5] }^{: §4.2.2 } (although that term is also used to refer to geodetic coordinate). These coordinates are the natural choice in models of the gravity field for a rotating ellipsoidal body. The above applies to a biaxial ellipsoid (a spheroid, as in oblate spheroidal coordinates); for a generalization, see triaxial ellipsoidal coordinates.

The relations between the above coordinate systems, and also Cartesian coordinates are not presented here. The transformation between geodetic and Cartesian coordinates may be found in geographic coordinate conversion. The relation of Cartesian and spherical polars is given in spherical coordinate system. The relation of Cartesian and ellipsoidal coordinates is discussed in Torge.^{ [5] }

**Astronomical latitude** (Φ) is the angle between the equatorial plane and the true vertical direction at a point on the surface. The true vertical, the direction of a plumb line, is also the gravity direction (the resultant of the gravitational acceleration (mass-based) and the centrifugal acceleration) at that latitude.^{ [5] } Astronomic latitude is calculated from angles measured between the zenith and stars whose declination is accurately known.

In general the true vertical at a point on the surface does not exactly coincide with either the normal to the reference ellipsoid or the normal to the geoid. The geoid is an idealized, theoretical shape "at mean sea level". Points on land do not lie precisely on the geoid, and the vertical at a point at a specific time is influenced by tidal forces which the theoretical geoid averages out. The angle between the astronomic and geodetic normals is called * vertical deflection * and is usually a few seconds of arc but it is important in geodesy.^{ [5] }^{ [20] }

Astronomical latitude is not to be confused with declination, the coordinate astronomers use in a similar way to specify the angular position of stars north–south of the celestial equator (see equatorial coordinates), nor with ecliptic latitude, the coordinate that astronomers use to specify the angular position of stars north–south of the ecliptic (see ecliptic coordinates).

- Altitude (mean sea level)
- Bowditch's American Practical Navigator
- Cardinal direction
- Circle of latitude
- Colatitude
- Declination on celestial sphere
- Degree Confluence Project
- Geodesy
- Geodetic datum
- Geographic coordinate system
- Geographical distance
- Geomagnetic latitude
- Geotagging
- Great-circle distance
- History of latitude
- Horse latitudes
- International Latitude Service
- List of countries by latitude
- Longitude
- Natural Area Code
- Navigation
- Orders of magnitude (length)
- World Geodetic System

The **Mercator projection** is a conformal cylindrical map projection presented by Flemish geographer and cartographer Gerardus Mercator in 1569. It became the standard map projection for navigation due to its ability to represent north as "up" and south as "down" everywhere while preserving local directions and shapes. However, as a result, the Mercator projection inflates the size of objects the further they are from the equator. In a Mercator projection, landmasses such as Greenland and Antarctica appear far larger than they actually are relative to landmasses near the equator. Despite these drawbacks, the Mercator projection is well-suited to marine navigation and internet web maps and continues to be widely used today.

An **azimuth** is the angular measurement in a spherical coordinate system which represents the horizontal angle from a cardinal direction, most commonly north.

A **geographic coordinate system** (**GCS**) is a spherical or geodetic coordinate system for measuring and communicating positions directly on Earth as latitude and longitude. It is the simplest, oldest and most widely used of the various spatial reference systems that are in use, and forms the basis for most others. Although latitude and longitude form a coordinate tuple like a cartesian coordinate system, the geographic coordinate system is not cartesian because the measurements are angles and are not on a planar surface.

**Earth radius** is the distance from the center of Earth to a point on or near its surface. Approximating the figure of Earth by an Earth spheroid, the radius ranges from a maximum of nearly 6,378 km (3,963 mi) to a minimum of nearly 6,357 km (3,950 mi).

In navigation, a **rhumb line**, **rhumb**, or **loxodrome** is an arc crossing all meridians of longitude at the same angle, that is, a path with constant bearing as measured relative to true north.

In geodesy, conversion among different geographic coordinate systems is made necessary by the different geographic coordinate systems in use across the world and over time. Coordinate conversion is composed of a number of different types of conversion: format change of geographic coordinates, conversion of coordinate systems, or transformation to different geodetic datums. Geographic coordinate conversion has applications in cartography, surveying, navigation and geographic information systems.

The **transverse Mercator** map projection is an adaptation of the standard Mercator projection. The transverse version is widely used in national and international mapping systems around the world, including the Universal Transverse Mercator. When paired with a suitable geodetic datum, the transverse Mercator delivers high accuracy in zones less than a few degrees in east-west extent.

The **scale** of a map is the ratio of a distance on the map to the corresponding distance on the ground. This simple concept is complicated by the curvature of the Earth's surface, which forces scale to vary across a map. Because of this variation, the concept of scale becomes meaningful in two distinct ways.

The **Universal Transverse Mercator** (**UTM**) is a map projection system for assigning coordinates to locations on the surface of the Earth. Like the traditional method of latitude and longitude, it is a horizontal position representation, which means it ignores altitude and treats the earth surface as a perfect ellipsoid. However, it differs from global latitude/longitude in that it divides earth into 60 zones and projects each to the plane as a basis for its coordinates. Specifying a location means specifying the zone and the *x*, *y* coordinate in that plane. The projection from spheroid to a UTM zone is some parameterization of the transverse Mercator projection. The parameters vary by nation or region or mapping system.

A **Lambert conformal conic projection** (**LCC**) is a conic map projection used for aeronautical charts, portions of the State Plane Coordinate System, and many national and regional mapping systems. It is one of seven projections introduced by Johann Heinrich Lambert in his 1772 publication *Anmerkungen und Zusätze zur Entwerfung der Land- und Himmelscharten*.

**Local tangent plane coordinates** (**LTP**), also known as **local ellipsoidal system**, **local geodetic coordinate system**, or **local vertical, local horizontal coordinates** (**LVLH**), are a spatial reference system based on the tangent plane defined by the local vertical direction and the Earth's axis of rotation. It consists of three coordinates: one represents the position along the northern axis, one along the local eastern axis, and one represents the vertical position. Two right-handed variants exist: **east, north, up** (**ENU**) coordinates and **north, east, down** (**NED**) coordinates. They serve for representing state vectors that are commonly used in aviation and marine cybernetics.

A **great ellipse** is an ellipse passing through two points on a spheroid and having the same center as that of the spheroid. Equivalently, it is an ellipse on the surface of a spheroid and centered on the origin, or the curve formed by intersecting the spheroid by a plane through its center. For points that are separated by less than about a quarter of the circumference of the earth, about , the length of the great ellipse connecting the points is close to the geodesic distance. The great ellipse therefore is sometimes proposed as a suitable route for marine navigation. The great ellipse is special case of an earth section path.

In geodesy and navigation, a **meridian arc** is the curve between two points on the Earth's surface having the same longitude. The term may refer either to a segment of the meridian, or to its length.

An **Earth ellipsoid** or **Earth spheroid** is a mathematical figure approximating the Earth's form, used as a reference frame for computations in geodesy, astronomy, and the geosciences. Various different ellipsoids have been used as approximations.

**Geographical distance** or **geodetic distance** is the distance measured along the surface of the Earth, or the shortest arch length.

**Geodetic coordinates** are a type of curvilinear orthogonal coordinate system used in geodesy based on a *reference ellipsoid*. They include **geodetic latitude** (north/south) ϕ, *longitude* (east/west) λ, and **ellipsoidal height**h. The triad is also known as **Earth ellipsoidal coordinates**.

Transverse Mercator projection has many implementations. Louis Krüger in 1912 developed one of his two implementations that expressed as a power series in the longitude difference from the central meridian. These series were recalculated by Lee in 1946, by Redfearn in 1948, and by Thomas in 1952. They are often referred to as the **Redfearn series**, or the Thomas series. This implementation is of great importance since it is widely used in the U.S. State Plane Coordinate System, in national and also international mapping systems, including the Universal Transverse Mercator coordinate system (UTM). They are also incorporated into the Geotrans coordinate converter made available by the United States National Geospatial-Intelligence Agency. When paired with a suitable geodetic datum, the series deliver high accuracy in zones less than a few degrees in east-west extent.

The **Bowring series of the transverse mercator** published in 1989 by Bernard Russel Bowring gave formulas for the Transverse Mercator that are simpler to program but retain millimeter accuracy.

In geodesy and geophysics, **theoretical gravity** or **normal gravity** is an approximation of the true gravity on Earth's surface by means of a mathematical model representing Earth. The most common model of a smoothed Earth is a rotating Earth ellipsoid of revolution.

The study of **geodesics on an ellipsoid** arose in connection with geodesy specifically with the solution of triangulation networks. The figure of the Earth is well approximated by an *oblate ellipsoid*, a slightly flattened sphere. A *geodesic* is the shortest path between two points on a curved surface, analogous to a straight line on a plane surface. The solution of a triangulation network on an ellipsoid is therefore a set of exercises in spheroidal trigonometry.

- ↑ The value of this angle today is 23°26′10.0″ (or 23.43611°). This figure is provided by Template:Circle of latitude.
- ↑ An elementary calculation involves differentiation to find the maximum difference of the geodetic and geocentric latitudes.

- ↑ "ISO 19111 Geographic information — Referencing by coordinates".
*ISO*. 2021-06-01. Retrieved 2022-01-16. - ↑ The Corporation of Trinity House (10 January 2020). "1/2020 Needles Lighthouse". Notices to Mariners. Retrieved 24 May 2020.
- ↑ Newton, Isaac. "Book III Proposition XIX Problem III".
*Philosophiæ Naturalis Principia Mathematica*. Translated by Motte, Andrew. p. 407. - ↑ National Imagery and Mapping Agency (23 June 2004). "Department of Defense World Geodetic System 1984" (PDF). National Imagery and Mapping Agency. p. 3-1. TR8350.2. Retrieved 25 April 2020.
- 1 2 3 4 5 Torge, W. (2001).
*Geodesy*(3rd ed.). De Gruyter. ISBN 3-11-017072-8. - 1 2 3 4 5 Osborne, Peter (2013). "Chapters 5,6".
*The Mercator Projections*. doi:10.5281/zenodo.35392. for LaTeX code and figures. - 1 2 3 4 Rapp, Richard H. (1991). "Chapter 3".
*Geometric Geodesy, Part I*. Columbus, OH: Dept. of Geodetic Science and Surveying, Ohio State Univ. hdl:1811/24333. - ↑ "Length of degree calculator". National Geospatial-Intelligence Agency. Archived from the original on 2012-12-11. Retrieved 2011-02-08.
- 1 2 3 4 5 Snyder, John P. (1987).
*Map Projections: A Working Manual*. U.S. Geological Survey Professional Paper 1395. Washington, DC: United States Government Printing Office. Archived from the original on 2008-05-16. Retrieved 2017-09-02. - 1 2 Adams, Oscar S. (1921).
*Latitude Developments Connected With Geodesy and Cartography (with tables, including a table for Lambert equal area meridional projection*(PDF). Special Publication No. 67. US Coast and Geodetic Survey. (*Note*: Adams uses the nomenclature isometric latitude for the conformal latitude of this article (and throughout the modern literature).) - ↑ Legendre, A. M. (1806). "Analyse des triangles tracés sur la surface d'un sphéroïde".
*Mém. Inst. Nat. Fr*. 1st semester: 130–161. - ↑ Bessel, F. W. (1825). "Über die Berechnung der geographischen Langen und Breiten aus geodatischen Vermessungen".
*Astron. Nachr*.**4**(86): 241–254. arXiv: 0908.1824 . Bibcode:2010AN....331..852K. doi:10.1002/asna.201011352. S2CID 118760590.**Translation:**Karney, C. F. F.; Deakin, R. E. (2010). "The calculation of longitude and latitude from geodesic measurements".*Astron. Nachr*.**331**(8): 852–861. arXiv: 0908.1824 . Bibcode:1825AN......4..241B. doi:10.1002/asna.18260041601. S2CID 118630614. - ↑ Cayley, A. (1870). "On the geodesic lines on an oblate spheroid".
*Phil. Mag*.**40**(4th ser): 329–340. doi:10.1080/14786447008640411. - ↑ Karney, C. F. F. (2013). "Algorithms for geodesics".
*Journal of Geodesy*.**87**(1): 43–55. arXiv: 1109.4448 . Bibcode:2013JGeod..87...43K. doi:10.1007/s00190-012-0578-z. S2CID 119310141. - ↑ Lagrange, Joseph-Louis (1779). "Sur la Construction des Cartes Géographiques".
*Oevres*(in French). Vol. IV. p. 667. - ↑ Karney, Charles F. F. (August 2011). "Transverse Mercator with an accuracy of a few nanometers".
*Journal of Geodesy*.**85**(8): 475–485. arXiv: 1002.1417 . Bibcode:2011JGeod..85..475K. doi:10.1007/s00190-011-0445-3. S2CID 118619524. - ↑ Orihuela, Sebastián (2013). "Funciones de Latitud".
- ↑ Karney, Charles F. F. (2023). "On auxiliary latitudes".
*Survey Review*. arXiv: 2212.05818 . doi:10.1080/00396265.2023.2217604. - ↑ Holfmann-Wellenfor & Moritz (2006)
*Physical Geodesy*, p.240, eq. (6-6) to (6-10). - ↑ Hofmann-Wellenhof, B.; Moritz, H. (2006).
*Physical Geodesy*(2nd ed.). ISBN 3-211-33544-7.

- GEONets Names Server. Archived 2008-03-09 at the Wayback Machine . access to the National Geospatial-Intelligence Agency's (NGA) database of foreign geographic feature names.
- Resources for determining your latitude and longitude Archived 2008-05-19 at the Wayback Machine
- Convert decimal degrees into degrees, minutes, seconds. Archived 2012-11-07 at the Wayback Machine – info about decimal to sexagesimal conversion.
- Convert decimal degrees into degrees, minutes, seconds
- Distance calculation based on latitude and longitude – JavaScript version
- 16th Century Latitude Survey
- Determination of Latitude by Francis Drake on the Coast of California in 1579

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