Cosmic Cartography
An advanced exploration into the principles and applications of coordinate systems for celestial bodies, from rigid surfaces to gaseous giants.
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Overview
Generalizing Earth's Systems
A planetary coordinate system extends the familiar geographic, geodetic, and geocentric coordinate systems of Earth to other celestial bodies. These systems are essential for precisely locating features on planets, moons, asteroids, and even comets, enabling detailed mapping and scientific analysis.
Nomenclature and Scope
Depending on the specific reference frame, these systems are often termed planetographic, planetodetic, or planetocentric. While the principles are universal, specific applications include selenographic coordinates for the Moon, areographic coordinates for Mars, and so forth. Such systems are crucial for any solid celestial body within our Solar System.
Pioneering Cartography
The foundational work for coordinate systems across nearly all solid bodies in the Solar System was largely established by Merton E. Davies of the Rand Corporation. His contributions provided the framework for mapping Mercury, Venus, Mars, Jupiter's four Galilean moons, and Neptune's largest moon, Triton, among others.
Defining Planetary Datums
Analogous to Earth's geodetic datums, a planetary datum specifies physical reference points or surfaces with fixed coordinates for other celestial bodies. This might involve designating a particular crater as the reference for the prime meridian or defining a best-fitting equigeopotential surface as the zero-level for altitude measurements, such as the Mars datum.
Longitude
Establishing the Prime Meridian
For most celestial bodies with rigid, observable surfaces, the longitude system is defined by referencing a distinct surface feature, such as an impact crater. The north pole is conventionally identified as the pole of rotation situated on the north side of the Solar System's invariable plane, typically near the ecliptic. The precise location of this prime meridian and the north pole's celestial position can shift over time due to the precession of the body's rotational axis.
Rotation and Directionality
The direction of rotation dictates how longitude is measured. If the body exhibits direct (prograde) rotation, where the position angle of the prime meridian increases with time, west longitudes are used (measured positively to the west). Conversely, for retrograde rotation, east longitudes are employed (measured positively to the east). This means that for a distant observer in the plane of the equator, a point passing later has a higher planetographic longitude.
Planetocentric vs. Planetographic
While planetographic longitude varies with rotation direction, planetocentric longitude is consistently measured positively to the east. East is defined as the counterclockwise direction when viewed from above the north pole (the pole closer to Earth's north pole). Longitudes are traditionally denoted with "E" or "W" to indicate polarity, where, for example, -91°, 91°W, +269°, and 269°E all represent the same location.
Specific Planetary Meridians
Modern Martian maps (since approximately 2002) utilize planetocentric coordinates, with the prime meridian established at the Airy-0 crater, a decision guided by historical astronomical observations by Merton E. Davies. For Mercury, a thermocentric coordinate system is used, where the prime meridian passes through the hottest point on its equator, defined as exactly twenty degrees of longitude east of the Hun Kal crater. Tidally-locked bodies, like many moons, have a natural reference longitude passing through the point nearest to their parent body (0° for the primary-facing hemisphere), though libration can cause this point to appear to move.
Latitude
Defining Vertical Position
Similar to longitude, planetographic latitude and planetocentric latitude are defined to specify vertical positions on a celestial body. The zero latitude plane, or the equator, is established as orthogonal to the mean axis of rotation, which passes through the body's poles. This fundamental definition ensures consistency in measuring angular distance from the equator towards the poles.
Reference Surfaces for Latitude
For many planets, such as Earth and Mars, the reference surfaces used for defining latitude are ellipsoids of revolution. These ellipsoids are typically oblate spheroids, meaning their equatorial radius is larger than their polar radius, reflecting the flattening caused by rotation. This geometric model provides a standardized surface against which latitude measurements are made, accounting for the body's overall shape.
Altitude
Expressing Vertical Extent
Vertical position on a celestial body can be expressed relative to a specific vertical datum. This involves using physical quantities analogous to Earth's topographical geocentric distance (compared to a nominal Earth radius or the varying geocentric radius of a reference ellipsoid surface) or altitude/elevation (measured above or below a geoid). These measurements are crucial for understanding the topography and gravitational fields of other worlds.
Planetary Geoids: Areoid and Selenoid
The concept of a geoid, which represents an equipotential surface of a planet's gravity field, is extended to other bodies. For Mars, this is known as the areoid, and for the Moon, the selenoid. These geoids have been meticulously measured using data from satellite missions, such as Mariner 9 and Viking for Mars, and the GRAIL twin satellites for the Moon. Significant departures from an ideal fluid ellipsoid, like Mars' Tharsis volcanic plateau and its antipodes, reveal important geological features and internal structures.
Planetary Shapes
Reference Ellipsoids for Mapping
Reference ellipsoids are fundamental for defining geodetic coordinates and creating accurate maps of planetary bodies, including planets, their satellites, asteroids, and comet nuclei. Well-observed bodies like the Moon and Mars now possess highly precise reference ellipsoids, which serve as the geometric basis for their cartographic representations.
Rocky Bodies: Axis and Mean Surface
For rigid-surface, nearly-spherical bodies, which encompass all rocky planets and many moons, ellipsoids are defined by their axis of rotation and the mean surface height, excluding any atmospheric effects. While Mars exhibits a slight "egg shape" with a polar radius difference of approximately 6 km, its average polar radius is used for defining its ellipsoid. The Earth's Moon, in contrast, is effectively spherical, displaying almost no equatorial bulge.
Gaseous Giants: Defining the Surface
For gaseous planets like Jupiter, which lack a solid surface, an "effective surface" for an ellipsoid is chosen. This is typically defined as the equal-pressure boundary of one bar. Since these planets do not possess permanent, observable surface features, the selection of their prime meridians is determined by mathematical rules and conventions rather than physical landmarks.
Bulges
Quantifying Flattening
Flattening describes the degree to which a spheroid deviates from a perfect sphere. For the Earth, modeled by the WGS84 ellipsoid, the equatorial radius is 6,378,137.0 meters, and the inverse flattening is 298.257223563. This yields a polar radius of 6,356,752.3142 meters, resulting in a difference of 21.385 km between the major and minor semi-axes. This difference, only about 0.335% of the major axis, is often greatly exaggerated in illustrations to visually emphasize the concept of oblateness.
The Origin of Flattening
The phenomenon of flattening in rotating celestial bodies was mathematically proven by Isaac Newton in his 1687 work, Principia. He demonstrated that a rotating, self-gravitating fluid body in equilibrium naturally assumes the shape of an oblate ellipsoid of revolution, or a spheroid. The extent of this flattening is a function of the body's density and the intricate balance between its gravitational force and the centrifugal force generated by its rotation.
Equatorial Bulge of Major Bodies
Any sufficiently massive, rotating celestial body that has drawn itself into a spherical or near-spherical shape will develop an equatorial bulge proportional to its rotation rate. Saturn, with an equatorial bulge of 11,808 km, holds the distinction of having the largest equatorial bulge in our Solar System. This table provides a comparative overview of the equatorial bulge for major celestial bodies:
Equatorial Ridges: A Unique Feature
Distinct from equatorial bulges, equatorial ridges are prominent topographical features found on at least four of Saturn's moons: the large moon Iapetus and the smaller moons Atlas, Pan, and Daphnis. These ridges closely trace the moons' equators. Discovered by the Cassini probe, the ridge on Iapetus is nearly 20 km wide, 13 km high, and 1300 km long. The ridge on Atlas is proportionally even more striking given the moon's diminutive size, contributing to its distinctive disk-like appearance. While similar structures are seen on Pan and Daphnis, their origins and the reasons for their apparent uniqueness to the Saturnian system remain subjects of ongoing scientific inquiry.
Irregular Shapes
Modeling Non-Spherical Bodies
Many small moons, asteroids, and comet nuclei possess highly irregular shapes that deviate significantly from a perfect sphere or even an oblate spheroid. For some of these, such as Jupiter's moon Io, a scalene (triaxial) ellipsoid offers a more accurate geometric approximation than a simple oblate spheroid. This more complex model accounts for three distinct axes, better capturing the non-uniformity of these celestial bodies.
Challenges in Cartography
For celestial bodies with extremely irregular or even non-convex shapes, like the asteroid 433 Eros, the traditional concept of a reference ellipsoid may lose its practical utility. In such cases, even using a spherical reference surface can be problematic, as latitude and longitude may not uniquely identify a single surface location. The complexities introduced by triaxial ellipsoids, particularly in map projections, often lead cartographers to employ simpler spherical reference surfaces in mapping programs to maintain elegant and popular projection properties, despite the geometric compromises.
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References
References
- Davies, M. E., "Surface Coordinates and Cartography of Mercury," Journal of Geophysical Research, Vol. 80, No. 17, June 10, 1975.
- Davies, M. E., S. E. Dwornik, D. E. Gault, and R. G. Strom, NASA Atlas of Mercury, NASA Scientific and Technical Information Office, 1978.
- Davies, M. E., and R. A. Berg, "Preliminary Control Net of Mars,"Journal of Geophysical Research, Vol. 76, No. 2, pps. 373-393, January 10, 1971.
- Merton E. Davies, Thomas A. Hauge, et al.: Control Networks for the Galilean Satellites: November 1979 R-2532-JPL/NASA
- Davies, M. E., P. G. Rogers, and T. R. Colvin, "A Control Network of Triton," Journal of Geophysical Research, Vol. 96, E l, pp. 15, 675-15, 681, 1991.
- Where is zero degrees longitude on Mars? â Copyright 2000 â 2010 European Space Agency. All rights reserved.
- Davies, M. E., and R. A. Berg, "Preliminary Control Net of Mars,"Journal of Geophysical Research, Vol. 76, No. 2, pps. 373-393, January 10, 1971.
- Davies, M. E., "Surface Coordinates and Cartography of Mercury," Journal of Geophysical Research, Vol. 80, No. 17, June 10, 1975.
- First map of extraterrestrial planet â Center of Astrophysics.
- The WGS84 parameters are listed in the National Geospatial-Intelligence Agency publication TR8350.2 page 3-1.
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