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Horizontal coordinate system

The horizontal coordinate system, also known as the alt-azimuth or horizon system, is a celestial coordinate framework used in astronomy to specify the position of objects in the sky relative to an observer's local horizon and zenith.^[1]^[2] It employs two primary angular measurements: altitude (or elevation), which is the angle above the horizon ranging from 0° at the horizon to 90° at the zenith (and negative values below the horizon), and azimuth, which is the horizontal angle measured clockwise from true north, spanning 0° to 360°.^[1]^[3] This system is observer-dependent, relying on the specific location (latitude and longitude) and time of observation, as Earth's rotation causes coordinates to change continuously throughout the day.^[2]^[3] In operation, the horizontal system conceptualizes the sky as a celestial sphere centered on the observer, with the horizon serving as the fundamental plane dividing the visible upper hemisphere from the lower one.^[1] The zenith represents the point directly overhead, perpendicular to the horizon, while the nadir is directly below; vertical circles pass through the zenith and a celestial object, aiding in altitude measurement, and the meridian is the great circle connecting north and south horizon points through the zenith.^[4]^[5] Unlike fixed equatorial systems based on Earth's rotational axis, the horizontal system is local and time-variable, making it intuitive for naked-eye observations or alt-azimuth telescope mounts but requiring conversions for tracking stars over extended periods.^[1]^[6] This coordinate system finds practical applications in amateur and professional astronomy, particularly for radio telescopes and modern observatories like NASA's Deep Space Network, where its simplicity supports symmetric mechanical designs and precise pointing.^[1] However, it becomes undefined at the celestial poles, where azimuth lacks meaning, and is influenced by local horizon obstructions such as terrain or buildings, often mapped in horizon masks for accurate observations.^[2]^[4] Overall, the horizontal system provides an accessible, ground-based perspective essential for initial sky navigation and real-time positioning.^[3]^[6]

Fundamentals

Definition and Principles

The horizontal coordinate system, also known as the alt-azimuth system, is a spherical coordinate framework in astronomy centered on the observer, using the local horizon as the fundamental reference plane and the zenith—the point directly overhead—as the system's pole. This setup allows for the specification of celestial object positions by measuring angles relative to the observer's immediate surroundings on Earth, projecting the sky onto a celestial sphere with the observer at its center.^[3]^[7] In contrast to sky-fixed systems like the equatorial coordinates, which are aligned with the Earth's rotational axis and remain invariant over short timescales, the horizontal system is inherently local and geocentric, with coordinates that vary continuously due to Earth's rotation and the observer's geographic position. Positions in this system are defined relative to the observer's meridian—the great circle passing through the zenith and north celestial pole—and the horizon plane, requiring precise knowledge of the observer's latitude and local sidereal time to compute or interpret them accurately.^[8]^[3]^[7] The system's two primary coordinates are altitude, representing the angular elevation above the horizon, and azimuth, denoting the horizontal angular distance from a reference direction such as true north. Developed from practical naked-eye observations, this framework provides an intuitive, observer-centric approach to locating objects in the sky, ideal for terrestrial-based viewing without reliance on complex instruments.^[3]^[8] It often serves as an intermediate step for transforming positions to equatorial coordinates.^[7]

Historical Development

The horizontal coordinate system, also known as the altazimuth system, has roots in ancient astronomical practices where observers relied on the local horizon as a fundamental reference for sighting celestial bodies. In Babylonian astronomy from the 8th century BCE, early forms of horizon-based measurements emerged through the tracking of rising and setting times of stars, particularly Ziqpu stars used to mark culminations relative to the horizon for calendrical and predictive purposes. This approach influenced Greek astronomers, who formalized horizon observations in the 2nd century CE, as seen in Claudius Ptolemy's Almagest, where he described measurements of altitudes from the horizon and azimuthal directions for constructing star catalogs and planetary models within a geocentric framework. These ancient methods prioritized practical sightings over precise coordinate grids, laying the groundwork for later systematic use. During the medieval period, Islamic astronomers advanced the horizontal system through innovations in instrumentation, notably the astrolabe, which integrated altazimuth features for navigation and timekeeping by the 10th century. Scholars like al-Battani (c. 858–929 CE) refined Ptolemaic techniques, incorporating rotatable dials on astrolabes to measure altitudes and azimuths relative to the horizon, enabling accurate determinations of the qibla (direction to Mecca) and prayer times across diverse latitudes.^[9] This development, building on translated Greek texts, emphasized the system's utility in observational astronomy and surveying, with astrolabes becoming widespread tools in the Islamic world by the 11th century.^[10] In the 16th and 17th centuries, European astronomers like Tycho Brahe (1546–1601) further refined the system for high-precision observations, employing large altazimuth instruments such as quadrants to record altitudes and azimuths of stars and planets, which informed his detailed star catalog and contributed to the transition toward integrating horizontal data with equatorial coordinates. Brahe's meticulous measurements at Uraniborg observatory demonstrated the system's effectiveness for naked-eye astronomy before the telescope era. By the 18th century, the formal mathematical description of the horizontal system solidified, particularly through Tobias Mayer's (1723–1762) work on lunar distance methods, where he developed tables and algorithms to compute lunar altitudes and azimuths for longitude determination at sea, enhancing navigational accuracy. The 19th and early 20th centuries saw the horizontal system's adoption in telescope design, with altazimuth mounts gaining prominence for their simplicity in tracking objects across the sky. Instruments like the altazimuth telescopes produced by Troughton & Simms in the mid- to late 19th century, such as those used in the 1874 Transit of Venus expeditions, featured setups suitable for meridian observations, reflecting a shift toward mechanical supports that facilitated routine use in observatories despite the rise of equatorial mounts.^[11] This evolution underscored the system's enduring role in practical astronomy, bridging ancient observational traditions with modern instrumentation.

Components

Altitude

In the horizontal coordinate system, altitude is defined as the angular distance measured along the vertical circle from the astronomical horizon to the position of a celestial object, ranging from 0° at the horizon to 90° at the zenith directly overhead. This coordinate quantifies the vertical elevation of the object relative to the observer's local horizontal plane.^[12] Measurement conventions specify that altitude values are positive for objects above the horizon and can extend to negative values for those below it, particularly in contexts involving atmospheric corrections where apparent positions may dip beneath the horizon.^[13] Geometrically, altitude represents the object's height on the observer's celestial dome, projecting its position onto the imaginary sphere centered at the observer, independent of horizontal direction.^[14] Historically, altitude has been measured using instruments like the sextant, which determines the angle between the horizon and a celestial body for navigation purposes.^[15] In modern astronomy, theodolites provide precise vertical angle measurements, often integrated into alt-azimuth telescopes for accurate positioning.^[16] An altitude of 0° corresponds to the astronomical horizon, which is the apparent boundary between Earth and sky as seen by the observer and differs from the true geometric horizon due to the bending of light rays by atmospheric refraction.^[17] Altitude pairs with azimuth to specify a complete location in the observer's sky.^[1]

Azimuth

In the horizontal coordinate system, azimuth represents the angular direction of a celestial object measured along the horizon from a reference point, typically true north, in a clockwise manner to the point where the object's vertical circle intersects the horizon, with values ranging from 0° to 360°. This measurement standard in astronomy uses true north as the starting point, where 0° indicates due north, 90° due east, 180° due south, and 270° due west, facilitating precise localization in the observer's horizontal plane. In certain navigational contexts, particularly in the southern hemisphere or specific maritime traditions, azimuth may instead be measured clockwise from true south to align with local conventions.^[18] Geometrically, the azimuth defines the orientation of the vertical circle—a great circle on the celestial sphere that passes through the zenith, the nadir, and the celestial object, intersecting the horizon perpendicularly at the azimuth point.^[14] This circle serves as the plane of reference for both azimuth and altitude measurements. An azimuth of 0° specifically aligns with the horizon point where the north celestial meridian meets the observer's local horizon.^[6] Distinctions exist between true azimuth, referenced to the geographic North Pole, and magnetic azimuth, referenced to the magnetic north pole; the latter requires corrections for magnetic declination to convert to true values using compass adjustments.^[19] Complementing the altitude coordinate, azimuth provides the full directional specification needed for locating objects in the horizontal system.^[2]

Mathematical Description

Coordinate Definitions

The horizontal coordinate system relies on spherical trigonometry to define the positions of celestial objects relative to an observer's local horizon and meridian. Central to this is the astronomical triangle formed by three key points on the celestial sphere: the zenith (the point directly overhead), the north celestial pole (the projection of Earth's rotational axis), and the celestial object in question. This triangle enables the calculation of altitude and azimuth through the application of spherical laws of sines and cosines, relating the object's equatorial coordinates to the observer's local frame.^[20]^[21] The primary variables in these definitions include the observer's geographic latitude \phi, the object's declination \delta (its angular distance from the celestial equator), and the local hour angle H (the angular difference between the object's right ascension and the local sidereal time, measured westward from the local meridian). The local sidereal time is implicit in H, as H = \theta - \alpha, where \theta is the local sidereal time and \alpha is the right ascension, typically converted to degrees by multiplying hours by 15. Altitude h represents the angular height above the horizon, ranging from 0° at the horizon to 90° at the zenith, while azimuth A is the horizontal angle from the north point, measured eastward from 0° to 360°.^[20]^[21] The altitude h is given by the formula:

h = \arcsin\left( \sin\delta \sin\phi + \cos\delta \cos\phi \cos H \right)

This equation arises from the spherical law of cosines applied to the zenith distance (90° - h) in the astronomical triangle. Specifically, the law states that for sides a, b, c and opposite angle C, \cos c = \cos a \cos b + \sin a \sin b \cos C; substituting the co-altitude ($90^\circ - h) as side b, co-latitude ($90^\circ - \phi) as side c, co-declination ($90^\circ - \delta) as side a, and hour angle H as angle A at the pole yields \sin h = \sin\phi \sin\delta + \cos\phi \cos\delta \cos H after trigonometric simplification.^[22]^[20] The azimuth A is determined using:

\cos A = \frac{\sin\delta - \sin\phi \sin h}{\cos\phi \cos h}

The quadrant of A is resolved by computing \sin A = -\cos\delta \sin H / \cos h alongside \cos A and using the atan2 function or equivalent to ensure A ranges correctly from 0° to 360° (with north at 0°). This follows from the spherical law of cosines for the angle at the zenith or, equivalently, the law of sines applied to the triangle: \sin A / \sin(90^\circ - \delta) = \sin H / \sin(90^\circ - h), leading to the expressions after rearrangement and substitution of the altitude equation.^[20]^[21]

Transformations to Other Systems

The horizontal coordinate system, defined relative to the observer's local horizon, requires transformations to interface with other celestial coordinate systems, such as the equatorial system based on the celestial equator and poles. These conversions account for the observer's geographic latitude \phi and the local sidereal time (LST), which determines the orientation of the celestial sphere at the observation site. LST, expressed in hours or degrees, is crucial as it allows computation of the local hour angle H = \mathrm{LST} - \alpha, where \alpha is the right ascension of the object. Latitude \phi enters the equations via the observer's position on Earth, influencing the projection from the equatorial plane to the local horizon.^[23]^[24] The forward transformation converts equatorial coordinates (right ascension \alpha, declination \delta) to horizontal coordinates (altitude h, azimuth A), typically measured from north (with A = 0^\circ at north, increasing eastward to $360^\circ). First, compute the hour angle H in degrees as H = 15^\circ \times (\mathrm{LST} - \alpha), where LST and \alpha are in hours. The altitude is then given by

\sin h = \sin \delta \sin \phi + \cos \delta \cos \phi \cos H,

and the azimuth by one of two forms, often the cosine variant for quadrant resolution:

\cos A = \frac{\sin \delta - \sin \phi \sin h}{\cos \phi \cos h}, \quad \sin A = -\frac{\cos \delta \sin H}{\cos h}.

These derive from spherical trigonometry in the astronomical triangle formed by the celestial pole, zenith, and object.^[23]^[25]^[24] The inverse transformation, from horizontal ( h, A ) to equatorial ( \alpha, \delta ), begins with the declination:

\sin \delta = \sin \phi \sin h + \cos \phi \cos h \cos A.

The hour angle follows as

\cos H = \frac{\sin h - \sin \delta \sin \phi}{\cos \delta \cos \phi}, \quad \sin H = -\frac{\cos h \sin A}{\cos \delta},

with the right ascension recovered via \alpha = \mathrm{LST} - H (adjusting for the 24-hour cycle). LST and \phi remain essential inputs, ensuring the transformation aligns the local frame with the fixed stellar reference. These equations also stem from the same spherical triangle, solvable iteratively if needed for numerical stability.^[23]^[25]^[24] For a numerical example, consider an observer at latitude \phi = 40^\circ N with LST = 10 h (150°), observing a star at \alpha = 5 h (75°), \delta = 30^\circ. The hour angle is H = 150^\circ - 75^\circ = 75^\circ. Then, \sin h = \sin 30^\circ \sin 40^\circ + \cos 30^\circ \cos 40^\circ \cos 75^\circ \approx 0.5 \times 0.6428 + 0.8660 \times 0.7660 \times 0.2588 \approx 0.3214 + 0.1715 = 0.4929, so h \approx 29.5^\circ. For azimuth, \cos A \approx (\sin 30^\circ - \sin 40^\circ \sin 29.5^\circ) / (\cos 40^\circ \cos 29.5^\circ) \approx (0.5 - 0.6428 \times 0.4929) / (0.7660 \times 0.8704) \approx 0.1834 / 0.6665 \approx 0.275, and \sin A \approx - \cos 30^\circ \sin 75^\circ / \cos 29.5^\circ \approx -0.8660 \times 0.9659 / 0.8704 \approx -0.961. Using atan2(\sin A, \cos A) gives approximately -74°, adjusted to 286° (western side of the meridian, confirmed by \sin A < 0). This illustrates the dependence on LST and \phi for practical computation.^[23] Transformations to the ecliptic coordinate system, which uses the Sun's apparent path as reference, are simpler in cases like solar system objects but generally proceed via the equatorial system as an intermediate step, incorporating the obliquity of the ecliptic (about 23.44°) in rotation matrices. Equatorial remains the primary intermediary for horizontal conversions due to its alignment with stellar catalogs.^[24]

Practical Applications

Observational Astronomy

In observational astronomy, the horizontal coordinate system provides a practical framework for locating and tracking celestial objects relative to the observer's local horizon, enabling precise pointing of telescopes and other instruments without requiring complex celestial computations during observation. This system is particularly valued for its intuitive alignment with the observer's immediate surroundings, allowing astronomers to specify targets using altitude (elevation above the horizon) and azimuth (compass direction along the horizon), which facilitates real-time adjustments based on the object's position in the sky. Alt-azimuth telescope mounts, often abbreviated as alt-az mounts, are designed to rotate around two perpendicular axes: one for altitude (vertical motion) and one for azimuth (horizontal motion), mirroring the horizontal coordinate system directly. These mounts employ simpler mechanical principles compared to equatorial mounts, which align with Earth's rotational axis and require polar alignment; alt-az designs avoid the need for precise clock drives to compensate for sidereal motion, making them more accessible and cost-effective for amateur and educational use. Their advantages include easier setup and lower manufacturing complexity, as the axes are parallel to gravity and the local horizon, reducing the demands on drive mechanisms and enabling smoother tracking for short-duration observations. For instance, many Dobsonians—popular among hobbyists—utilize alt-az mounts for their straightforward push-to operation, allowing observers to manually follow objects across the sky. Modern alt-azimuth telescopes incorporate setting circles on both axes, which are graduated scales calibrated in degrees of altitude and azimuth, allowing observers to manually set the instrument to predetermined coordinates for locating faint or specific targets. These analog dials have evolved into digital encoders, small sensors attached to the mount's axes that provide precise feedback on current position, often integrated with computer control systems for automated pointing. Digital encoders, typically using optical or magnetic technology, achieve resolutions down to arcseconds, enabling go-to telescopes to slew accurately to alt-az coordinates derived from star catalogs, thus streamlining the process of finding deep-sky objects like galaxies or nebulae. Planetarium software applications further enhance the utility of horizontal coordinates by computing and displaying real-time alt-az positions for celestial objects, aiding in observation planning and execution. Programs like Stellarium simulate the night sky from the observer's location, overlaying alt-az grids and predicting object risings, settings, and transits to optimize viewing sessions; for example, it can alert users when a target reaches a favorable altitude above the horizon to minimize atmospheric distortion. These tools interface directly with telescope mounts via protocols like LX200, allowing remote control where the software sends alt-az commands to position the instrument automatically. Observing techniques in amateur and professional astronomy often rely on horizontal coordinates for practical fieldwork, such as using alt-az readouts to star-hop—progressively navigating from bright reference stars to fainter targets—or to schedule sessions around an object's meridian transit when it achieves maximum altitude. Planners calculate rising and setting times in alt-az terms to account for local horizon obstructions like trees or buildings, ensuring efficient use of dark-sky time; a common method involves plotting alt-az paths on charts to identify optimal viewing windows, particularly for transient events like meteor showers. In radio astronomy, the horizontal coordinate system is essential for pointing steerable dish antennas using alt-azimuth mounts, allowing them to track sources across the sky. Early observatories, such as the one at Jodrell Bank established in 1945, used alt-az coordinates for meridian transit observations to scan the sky systematically, capturing radio emissions from the Sun and other sources during their passage through the zenith. This approach persists in some facilities, while modern ones like the Allen Telescope Array employ steerable alt-az pointing to optimize signal collection from various sources, including geostationary or low-elevation objects.^[26] Celestial navigation relies on the horizontal coordinate system to determine an observer's position on Earth by measuring the altitude and azimuth of celestial bodies such as stars, planets, or the Sun. The altitude, which is the angular height above the horizon, provides information about the observer's latitude, while the azimuth, the horizontal direction from true north, helps establish longitude through lines of position. This method uses sight reduction to convert these measurements into geographic coordinates, traditionally via tables or modern calculators, allowing navigators to fix their position without reliance on electronic systems.^[27] The core procedure involves timing the altitude measurement of a known celestial body using tools like the sextant, which captures the angle between the body and the horizon. The observed altitude is corrected for atmospheric refraction, instrument errors, and the observer's eye height to obtain the true altitude. Sight reduction tables, such as those in Publication No. 229, or computational aids then use this data along with the body's declination and Greenwich Hour Angle from nautical ephemerides to calculate the expected altitude and azimuth at an assumed position near the dead-reckoning location. The difference between observed and calculated altitudes yields an intercept, plotted perpendicular to the azimuth line to form a line of position; multiple such lines from different bodies intersect to yield latitude and longitude.^[27]^[28] Historically, the sextant was essential for these altitude shots, with azimuth often determined separately using a pelorus or computed during reduction to plot the line of position. During World War II, aviators in aircraft like the B-17 Flying Fortress and B-25 Mitchell employed compact sextants, such as the A-10 model, to perform celestial fixes over oceans, averaging multiple sightings to counter turbulence and achieve positional accuracy within miles. These practices were critical for long-range bombing missions and submarine patrols, where dead reckoning alone was insufficient.^[29] In modern aviation and maritime operations, celestial navigation serves as a GPS-independent backup, particularly in scenarios involving electronic warfare or satellite denial. The U.S. Navy reinstated training in 2016 after a hiatus, emphasizing its role in ensuring positional awareness amid GPS vulnerabilities like spoofing. Maritime vessels, including commercial ships, maintain sextants and almanacs for emergency use, with automated systems emerging to streamline reductions while preserving the horizontal coordinate framework.^[30] The azimuth measurement is particularly vital in great-circle sailing, as it provides the bearing to the celestial body's geographic position, enabling navigators to plot the shortest path over Earth's curved surface for efficient routing. This integration of horizontal coordinates with equatorial data from ephemerides ensures precise course adjustments.^[31]

Limitations and Considerations

Dependence on Observer

The horizontal coordinate system, also known as the alt-azimuth system, is inherently tied to the observer's geographic position, with altitude and azimuth values varying significantly based on latitude and longitude. Latitude determines the elevation of the celestial poles above the horizon; for instance, the north celestial pole's altitude equals the observer's latitude, making it visible only from the Northern Hemisphere and reaching 90° at the North Pole.^[32] Circumpolar stars, which never set, are those whose declination exceeds 90° minus the observer's latitude—for example, a star at +60° declination is circumpolar (remains above the horizon) for observers north of 30° N but rises and sets daily from the equator.^[24]^[33] Longitude affects azimuth through the local meridian, which is the projection of the geographic meridian onto the celestial sphere, shifting the reference for north-south alignments as the observer moves east or west.^[7] Temporal variations further emphasize the system's observer-centric nature, as Earth's daily rotation causes altitude and azimuth to change continuously for any fixed celestial object, even if the observer remains stationary—objects rise, culminate, and set over approximately 24 hours.^[2] This daily motion is quantified by the hour angle, which depends on local sidereal time rather than solar time; sidereal time tracks the stars' positions relative to the vernal equinox, advancing about 4 minutes faster per solar day due to Earth's orbital motion, thus requiring sidereal clocks for precise alt-azimuth predictions.^[34] Annually, Earth's orbit around the Sun alters the apparent positions, compounding these changes and making coordinates valid only for a specific date.^[7] For example, a star's altitude at midnight culmination is higher for observers at latitudes closer to its declination, such as Polaris appearing nearly overhead at 90° N but only 40° high at 40° N latitude.^[24]^[32] Orientation factors, particularly the definition of true north, are essential for azimuth measurements, which start at 0° for true north and increase eastward to 360°. True north is determined astronomically via Polaris in the Northern Hemisphere or a gyrocompass for precision, distinguishing it from magnetic north to avoid navigational errors. The distinction between sidereal and solar time underscores this, as solar time aligns with the Sun's position for civil purposes, while sidereal time governs stellar coordinates, directly influencing azimuth calculations through the local hour angle.^[34] Unlike the equatorial system, no fixed catalog of horizontal coordinates exists because they are transient and observer-specific, necessitating real-time computations from equatorial data using the observer's latitude, longitude, and sidereal time for each observation.^[35]^[2] This variability requires software or ephemerides to convert stable right ascension and declination into instantaneous alt-azimuth values.^[7]

Atmospheric and Instrumental Effects

In the horizontal coordinate system, atmospheric refraction significantly impacts observations by bending light rays from celestial objects as they pass through Earth's atmosphere, causing them to appear higher in altitude than their true positions. This effect is most pronounced near the horizon, where the ray path is longest and encounters the greatest density gradient, resulting in an apparent elevation increase of up to approximately 0.57° for standard conditions. The refraction angle depends on the object's apparent altitude h, atmospheric temperature, and pressure; correction tables, such as those in the Astronomical Almanac, adjust for these variables by subtracting the refraction from the observed altitude to obtain the true value. A simplified empirical formula for the refraction R (in degrees) under standard conditions is R ≈ 1° / tan(h + 7.31° / (h + 4.4°)), where h is the observed altitude in degrees, though more precise models integrate ray-tracing through layered atmospheric profiles for high-accuracy applications like geodesy.^[36] Instrumental errors in devices measuring horizontal coordinates, such as alt-azimuth telescopes and marine sextants, introduce systematic offsets that must be calibrated to ensure accuracy. In telescopes, collimation errors occur when the optical axis deviates from the mechanical axis of the mount, leading to pointing inaccuracies that vary with altitude and azimuth; these are typically quantified through star observations across the sky and corrected via encoder adjustments or software models, achieving residual errors below 1 arcsecond in modern systems. For sextants used in celestial navigation, common errors include index error (misalignment of the index arm), side error (non-perpendicular mirrors), and perpendicularity error (tilted horizon mirror), which can shift measured altitudes by several arcminutes if uncorrected; calibration involves aligning against the horizon or known stars and applying offsets during sight reduction. Parallax in sextant measurements, arising from the observer's eye position relative to the instrument's optical center, is minimized by using the recommended eye relief but requires a small correction of up to 10 arcseconds.^[37]^[38] Defining the true horizon in horizontal coordinates poses challenges due to the observer's elevation and local atmospheric conditions, necessitating specific corrections for reliable measurements. At sea, the dip correction accounts for the geometric depression of the visible horizon below the celestial horizon caused by the observer's height of eye (HE), approximately given by dip ≈ -0.97 × √(HE) arcminutes where HE is in feet, reducing the observed altitude by this amount to reference the true horizontal plane. This correction increases with height—for example, from a 10-meter eye height, it amounts to about 5.6 arcminutes—and is tabulated in navigation almanacs for standard conditions. Terrestrial refraction further complicates horizon definition by bending rays over Earth's curved surface, reducing the apparent dip by typically 10-20% of the geometric value; this is empirically modeled, with standard tables providing the net correction to subtract for the true horizontal plane in precise surveys. Observer location can influence baseline errors in these corrections through varying terrain or elevation, but such effects are generally minor compared to standard atmospheric models. Parallactic effects, or topocentric parallax, are negligible for distant stars but become relevant for nearby solar system objects in horizontal coordinate observations, particularly in navigation. For the Sun, the horizontal parallax is about 8.8 arcseconds, causing a slight apparent shift in altitude and azimuth depending on the observer's position, while for the Moon it reaches up to 57 arcminutes near the horizon, requiring subtraction from observed altitudes to compute geocentric positions. These corrections are standard in sight reduction tables and are most critical during lunar observations for longitude determination, where uncorrected parallax can introduce errors exceeding 10 nautical miles in position fixes. Modern GPS integration aids in applying these parallactic adjustments by providing precise topocentric coordinates.^[39]

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[32]
Circumpolar Constellations: Visible All The Year Round - Star Walk
For example, a star with a declination of +60° will always stay above the horizon for observers located north of latitude 30° N (90 – 60 = 30). You can check ...
[33]
Time, coordinate systems, observability tools - NMSU Astronomy
Sidereal is relevant for position of stars: stars come back to the same position every sidereal day. As we'll see below, a given star crosses the meridian when ...
[34]
[PDF] Finding Celestial Object - Orange County Astronomers
Alt-azimuth coordinates are not constant. They vary depending on the hour and the latitude of the observer. Astronomical charts do not show alt-azimuth.
[35]
Astronomical refraction and airmass - NASA ADS
For a realistic atmosphere an approximate formula is given for X and, finally, the standard mean refraction in the Pulkovo tables are approximated. 2. A ...
[36]
[PDF] Telescope Pointing - Caltech Astronomy
The collimation error CH describes how accurately the telescope optics are aligned within the tube, whether the tube is at right-angles to the declination axis ...
[37]
[PDF] COMDTPUB P16721 NVIC 02-18 August 6, 2018 NAVIGATION ...
Aug 6, 2018 · 1. The candidate removes the adjustable sextant errors in the following order: a. Perpendicularity; b. Side error; and.
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Celestial Navigation Data for Assumed Position and Time
The output table gives both almanac data and altitude corrections for each celestial body that is above the horizon at the place and time that you specify.