Gnomonic projection
The Gnomonic projection is an azimuthal map projection that represents points on a sphere's surface by projecting them radially from the sphere's center onto a tangent plane, causing all great circles—the shortest paths between points on the sphere—to appear as straight lines on the map.[1][2][3]
Originating over 2,000 years ago among ancient Greek astronomers, the projection was employed by figures such as Thales of Miletus (c. 636–546 BCE) for star maps and later formalized by Hipparchus in the 2nd century BCE and Claudius Ptolemy around 150 CE.[3] It derives its name from the Greek gnōmōn (sundial indicator), reflecting early associations with sundial construction, and was mathematically refined in the 16th century by Johann Werner and Gerardus Mercator for both celestial and terrestrial applications.[3][4] By the Renaissance, it appeared in works like Johannes Kepler's 1606 star map and was adapted for world maps by cartographers such as Jean Cossin (1570) and Jodocus Hondius (1606–1609), though its use for geographic mapping remained limited until the 19th century due to challenges in constructing it without globes.[3][4]
As a perspective projection, it is neither conformal (preserving angles) nor equal-area, with distortion increasing rapidly away from the central point of tangency, making it unsuitable for mapping more than a hemisphere or areas beyond about 90 degrees from the center.[1][2][5] In its polar aspect, meridians radiate as straight lines from the pole, while parallels form concentric circles; in equatorial or oblique aspects, meridians are straight, and parallels curve except for the straight equator.[2][5] Modern formulations, including ellipsoidal versions developed by Martin Hotine in 1946–1947 and series expansions by John P. Snyder in 1979, support its use in digital mapping systems.[3]
The projection's defining advantage lies in navigation and planning, where great-circle routes appear as straight lines, facilitating the plotting of shortest paths for ships, aircraft, and even seismic studies; it has been applied to regions like Antarctica, the Pacific Ocean in USGS mapping projects.[2][3][5] It also serves in astronomy for star charts and in polyhedral globe approximations, though its severe areal and shape distortions limit broader cartographic applications.[1][3]
Fundamentals
Definition
The gnomonic projection is a type of map projection that mathematically transforms the curved, three-dimensional surface of the Earth—or any sphere—onto a flat, two-dimensional plane, enabling the representation of spherical geography in a usable format.[3]
As an azimuthal projection, it originates from a central point at the sphere's center, projecting surface points onto a plane tangent to the sphere at the chosen central location, such as a pole.[5] This perspective setup ensures that all great circles—the shortest paths between any two points on the sphere—appear as straight lines on the map, making it particularly suited for visualizing direct routes across the globe.[6]
The term "gnomonic" stems from the ancient Greek word gnōmōn, meaning the upright pointer or style of a sundial that casts shadows to indicate time, reflecting the projection's central radiating geometry akin to rays from a sundial's gnomon.[7]
Visually, gnomonic maps are centered on a specific point, such as a geographic pole, and maximally display a hemisphere without interruption. Meridians radiate outward as straight lines from the center, while parallels form concentric circular arcs expanding away from it; in the equatorial aspect, the equator manifests as a straight line perpendicular to the central meridian, with other parallels as curving arcs.[6]
Geometric Construction
The gnomonic projection is geometrically constructed by positioning a plane tangent to the Earth's spherical surface at a selected projection center, which serves as the origin of the map. This tangent plane is perpendicular to the radius of the sphere at the center point, ensuring initial contact without intersection elsewhere. Rays are then extended from the geometric center of the sphere (the projection point) through each point on the sphere's surface, continuing until they intersect the tangent plane, thereby mapping the spherical points onto the flat surface. This central perspective mimics viewing the globe from its core looking outward.[1]
The process begins with choosing the projection center, often the North Pole for polar-oriented maps, where the tangent plane touches at that pole and the plane's normal aligns with the Earth's axis. For construction, the sphere is represented with the center at point O, and the tangent plane is placed at the desired point S on the surface; rays from O through surface points P intersect the plane at corresponding map points P'. Key elements include the projection center O as the fixed origin inside the sphere, the tangent plane as the receiving surface, and the straight-line rays that preserve geodesic paths, such that great circles on the sphere appear as straight lines on the map. The setup inherently limits the projection to less than one full hemisphere, as points on the opposite side would require rays extending to infinity or beyond the plane, preventing representation of the entire globe without discontinuity.[8]
Variants of the gnomonic projection differ based on the location of the tangent point, determining the map's orientation and coverage. In the pole-centered (polar) variant, the tangent plane contacts the sphere at a pole, resulting in a circular map where meridians radiate outward as straight lines from the center and parallels form concentric circles, ideal for high-latitude regions. Conversely, the equatorial-centered variant places the tangent plane at a point on the equator, producing a map with parallel meridians perpendicular to the equatorial straight line and curved parallels, suitable for equatorial views but with similar hemispheric constraints. Despite these orientations, the gnomonic projection is fundamentally an azimuthal type, centered on a specific point, and can be adapted to any location on the sphere by adjusting the tangent point accordingly.[1]
History
Origins
The gnomonic projection traces its roots to ancient Greek astronomy, where it emerged as a central perspective method for mapping the celestial sphere onto a plane. Approximately 2,000 years ago, Greek scholars developed this technique for constructing star maps, with speculative attribution to Thales of Miletus (c. 636–546 BCE) for early applications in charting stellar positions. Hipparchus (c. 190–120 BCE), often regarded as the father of scientific astronomy, advanced celestial mapping using straight parallels, laying foundational principles for projections that preserved great circle paths as straight lines, though not explicitly named as gnomonic at the time. Claudius Ptolemy (c. 90–168 CE) described an equidistant conic projection in his Geographia (Book 1, Chapter 20), covering latitudes from 63°N to 16°S, with meridians as straight lines converging at the pole; this conic approach influenced subsequent astronomical and cartographic representations, though it differed from the true perspective gnomonic projection.[3]
During the medieval period, Islamic scholars refined spherical geometry and astronomical instruments, contributing to the broader development of projection techniques, though specific applications to the gnomonic projection are not well-documented. These advancements were evident in medieval star charts and practical tools for celestial observation.[3]
In the early modern era, the projection gained recognition in Europe for navigational and celestial purposes. In the 16th century, Johann Werner and Gerardus Mercator mathematically refined the gnomonic projection for both celestial and terrestrial uses. It appeared in Johannes Kepler's 1606 star map and was adapted for world maps by cartographers such as Jean Cossin (1570) and Jodocus Hondius (1606–1609). By this time, it was also incorporated into nautical charts to plot great circle routes as straight lines, facilitating calculations for transoceanic voyages. Mercator's 1569 world map included polar insets using the related azimuthal equidistant projection. This practical integration into seafaring tools, alongside its continued use in sundials and celestial mapping, solidified the projection's importance up to the 18th century, when it became a standard for hemispheric navigation charts emphasizing geometric accuracy over conformal properties.[3][4]
Key Developments
The gnomonic projection received its formal name in the 19th century, derived from the Greek term "gnōmōn" referring to the sundial's straightedge, reflecting the projection's geometric resemblance to sundial hour markings; prior to this, it was known as the "horologium" or sundial projection.[3] This naming aligned with growing interest in precise cartographic methods during the era's advancements in geodesy and surveying, though the projection's core principles dated to antiquity.[3]
In the 20th century, the gnomonic projection gained prominence in aviation and radio transmission mapping due to its unique property of depicting all great circles as straight lines, facilitating the plotting of shortest-path routes such as transoceanic flights.[3] Around 1920, it served as the foundation for the two-point azimuthal projection, an extension that rendered great-circle arcs between specific points as straight lines, further enhancing its utility in long-distance navigation.[3] By mid-century, applications expanded to satellite tracking and extraterrestrial mapping, where accurate azimuths and geodesic representations proved essential for space mission planning and orbital path visualization.[3]
As of November 2025, digital implementations have integrated the gnomonic projection into geographic information systems (GIS) software, enabling efficient computational rendering for modern mapping needs. In ArcGIS, support was introduced in version 8.1.1 (2001) and persists in current releases, allowing users to generate azimuthal maps with customizable central points for applications like polar region analysis.[9] Similarly, QGIS leverages the PROJ library, which has long provided forward and inverse transformations for the gnomonic projection on both spherical and ellipsoidal models, supporting custom projections via proj-strings for high-precision geospatial workflows.[8] These tools have streamlined post-2000 enhancements in computational cartography, reducing manual distortion handling through automated re-projection algorithms.[3]
Projection Equations
The gnomonic projection is formulated using spherical coordinates, where a point on the sphere is defined by its geodetic latitude \phi and longitude \lambda, both typically in radians for computational purposes. The projection center is specified by central latitude \phi_1 and central longitude \lambda_0. For the standard north polar case, where the center is at the North Pole (\phi_1 = 90^\circ), the colatitude \theta = 90^\circ - \phi represents the angular distance from the pole. The projection assumes a spherical Earth of radius R, often normalized to R = 1 for simplicity in derivations.[3]
The forward projection equations map these spherical coordinates to Cartesian coordinates (x, y) on the tangent plane. In the north polar aspect, the equations are:
x = R \cot \phi \sin(\lambda - \lambda_0)
y = -R \cot \phi \cos(\lambda - \lambda_0)
These yield the position relative to the origin at the projection center, with meridians as straight lines radiating outward and parallels as concentric arcs. The radial distance from the center is \rho = R \cot \phi = R \tan \theta, increasing to infinity at the horizon (\phi = 0^\circ, \theta = 90^\circ). A unique singularity occurs at the antipodal point (\theta = 180^\circ), where distances become undefined and infinite, limiting the projection to less than a full hemisphere.[3]
These equations derive from a vector projection onto the tangent plane. Consider a unit sphere (R = [1](/page/1)) with the projection center at the North Pole, so the tangent plane is z = [1](/page/1). A point P on the sphere has Cartesian coordinates (\cos \phi \cos \lambda, \cos \phi \sin \lambda, \sin \phi). The ray from the sphere's center through P intersects the plane at t \cdot P, where t \sin \phi = [1](/page/1), so t = 1 / \sin \phi. The projected coordinates are then x = \cos \phi \cos \lambda / \sin \phi = \cot \phi \cos \lambda and y = \cot \phi \sin \lambda, with the sign convention for y adjusted for northward orientation. This perspective projection preserves great circles as straight lines via central projection geometry.[3]
The formulation assumes a tangent projection (plane touching the sphere at the center), though secant variants adjust the plane to intersect the sphere for reduced distortion over larger areas; the tangent case is standard for derivations. Computations use a unit sphere for simplicity, scaling by R afterward. Points are only projectable if visible from the center, i.e., angular distance c < 90^\circ, where \cos c = \sin \phi > 0.[3]
For an arbitrary projection center, the forward equations in oblique aspect are:
\cos c = \sin \phi_1 \sin \phi + \cos \phi_1 \cos \phi \cos(\lambda - \lambda_0)
k' = \frac{1}{\cos c}
x = R k' \cos \phi \sin(\lambda - \lambda_0)
y = R k' [\cos \phi_1 \sin \phi - \sin \phi_1 \cos \phi \cos(\lambda - \lambda_0)]
Here, c is the angular distance from the center, and k' is the local scale factor. To align an arbitrary pole, a rotation matrix transforms the coordinate system: first rotate longitudes by -\lambda_0 around the z-axis, then tilt the latitude pole from $90^\circ to \phi_1 using rotations around the x- and y-axes, apply the polar projection, and inverse-rotate the results. This matrix approach, composed of standard Euler rotations, ensures the center aligns with the projection pole.[3]
Inverse Projection
The inverse projection for the gnomonic map transforms planar coordinates (x, y) back to spherical coordinates (\phi, \lambda), where \phi is the latitude and \lambda is the longitude relative to the central meridian. For the polar aspect, with the projection center at the north pole and sphere radius R, the colatitude \theta (angular distance from the pole) is given by \theta = \arctan\left(\sqrt{x^2 + y^2} / R\right), the latitude by \phi = 90^\circ - \theta, and the relative longitude by \Delta\lambda = \atantwo(x, -y), then \lambda = \lambda_0 + \Delta\lambda to account for the correct quadrant.[3] These equations assume a spherical Earth and apply within the visible hemisphere.
The derivation stems from the geometry of the central projection ray: a point on the sphere at angular distance \theta from the center projects to a radial distance \rho = \sqrt{x^2 + y^2} = R \tan \theta on the tangent plane, yielding \theta = \arctan(\rho / R) via inversion of the tangent function; the longitude follows from the azimuthal angle in the plane, adjusted via the two-argument arctangent for directional accuracy.[3] This trigonometric relation ties planar distances directly to great-circle angular measures along the central ray, with \rho scaling proportionally to \tan \theta.
A key challenge in the inverse projection is its limitation to one hemisphere (\theta < 90^\circ), as the tangent plane captures only rays from the sphere's center that intersect positively; beyond this, \rho \to \infty as \theta \to 90^\circ, rendering the mapping undefined for the opposite hemisphere without multiple charts or plane extensions.[3] Edge cases near \theta = 90^\circ introduce numerical instability due to the asymptotic behavior of \tan \theta, often requiring careful handling in computations to avoid overflow or precision loss.
In computational implementations, the inverse can be formulated via vector normalization to ensure the result lies on the unit sphere: for a unit sphere (R = 1), construct the direction vector \mathbf{v} = (-y, x, 1), normalize to \hat{\mathbf{v}} = \mathbf{v} / \|\mathbf{v}\|, then extract \phi = \arcsin(\hat{v}_z) and \lambda = \lambda_0 + \atantwo(\hat{v}_y, \hat{v}_x). This approach leverages the perspective geometry directly and mitigates some scaling issues. Pseudocode for the polar case (in degrees, assuming R = 1) is as follows:
function inverse_gnomonic(x, y):
rho = sqrt(x*x + y*y)
if rho == 0:
return 90.0, 0.0 # phi, lambda at [pole](/page/Pole)
d = sqrt(rho*rho + 1.0)
phi = asin(1.0 / d) * 180 / pi # [latitude](/page/Latitude)
lambda_rel = atan2(x, -y) * 180 / pi # relative [longitude](/page/Longitude)
return phi, lambda_rel
function inverse_gnomonic(x, y):
rho = sqrt(x*x + y*y)
if rho == 0:
return 90.0, 0.0 # phi, lambda at [pole](/page/Pole)
d = sqrt(rho*rho + 1.0)
phi = asin(1.0 / d) * 180 / pi # [latitude](/page/Latitude)
lambda_rel = atan2(x, -y) * 180 / pi # relative [longitude](/page/Longitude)
return phi, lambda_rel
[1]
For high-precision applications in geographic information systems (GIS), particularly the ellipsoidal gnomonic projection where closed-form inverses are more complex, modern iterative solvers such as the Newton-Raphson method are employed to refine solutions to the nonlinear geodesic equations underlying the transformation.[10] This involves solving for arc length s_{12} along the geodesic via iterations on the reduced length and azimuth, typically converging in 2-4 steps for distances up to 10,000 km, enabling accurate reverse mapping even near projection limits.[10]
Properties
Preservation Characteristics
The gnomonic projection uniquely preserves the straight-line representation of great circles, mapping all great circles on the sphere as straight lines on the plane, which corresponds to the shortest paths or geodesics between points.[2][11][1] This property arises from its perspective construction with the projection point at the Earth's center, making it particularly valuable for identifying geodesic routes without computation.[2] In contrast, rhumb lines, which maintain constant bearing, appear as curved paths on the projection.[12]
The projection is not conformal, meaning it does not preserve local angles except at the central point of projection, where angles between meridians are true in the polar aspect.[2][1] Scale is true only at this central point and increases radially outward, leading to progressive distortion in distances and directions away from the center.[2][12] As an azimuthal projection, it maintains correct directions from the center to any point, providing azimuthal equidistance in bearing but not in actual distance measurement.[11]
Neither areas nor shapes are preserved, with significant inflation of areas and elongation of shapes occurring near the projection's edges, where distortion becomes extreme beyond about 90 degrees from the center.[2][12] This lack of equal-area or conformal preservation limits its utility to small regions or polar caps, typically within a 60-degree radius for moderate accuracy.[2]
Distortion Patterns
The gnomonic projection exhibits significant distortions that increase radially from the central point, making it unsuitable for mapping areas beyond a limited radius. The principal scale factors differ by direction: the meridional scale factor h, along radii from the center, is h = \sec^2 \theta, while the parallel scale factor k, perpendicular to the radii, is k = \sec \theta, where \theta is the angular distance from the center in radians. Both factors equal 1 at the center (\theta = 0) but grow without bound as \theta approaches $90^\circ, rendering the antipodal hemisphere unmappable on a finite plane.[3]
Application of Tissot's indicatrix reveals that infinitesimal circles on the sphere project to ellipses elongated in the meridional direction, with the ratio of major to minor axes equal to \sec \theta. This radial elongation intensifies toward the projection's horizon, where the ellipses become infinitely stretched, highlighting severe linear distortion in shapes extending outward. Angular distortion, measured as the maximum deviation \omega from right angles, reaches up to 31.1° across the projectable hemisphere.[3][13]
Area distortion in the gnomonic projection is given by the product of the principal scales, m = h \cdot k = \sec^3 \theta, which expands cubically with distance from the center and becomes infinite at \theta = 90^\circ. This results in gross overestimation of areas near the boundary, with a maximum distortion ratio of 5.19 relative to the center. Shape distortion manifests as differential stretching of parallels relative to meridians, preserving no conformality except at the origin, though the projection's perspective nature causes all distortions to converge at infinity along the 90° horizon.[3][13]
In digital mapping contexts, modern metrics such as the angular distortion index—derived from Tissot's parameters—quantify these effects for applications beyond Earth, including lunar and Martian terrains. For instance, on ellipsoidal approximations of these bodies, the gnomonic projection yields comparable maximum angular distortions of around 31.1°, though area ratios vary slightly due to differing oblateness (e.g., lower for the Moon's near-sphericity versus Earth's). These indices aid in selecting hybrid projections for planetary rendering, where gnomonic's radial patterns limit its use to small-scale, center-focused views.[13]
Applications
Navigation and Route Planning
The gnomonic projection is essential in nautical navigation for plotting great circle routes—the shortest distances between two points on the Earth's surface—as straight lines on specialized charts. This enables mariners to efficiently plan long-distance voyages, such as transatlantic crossings from Europe to North America, by drawing the optimal path directly on the gnomonic chart and then transferring selected waypoints to a Mercator chart for practical use during the journey, as Mercator charts preserve constant compass bearings for steering.[14]
In aviation, the projection supports flight planning by allowing great circle paths to appear as straight lines, which is particularly advantageous for polar routes connecting major cities in North America and Asia. These routes leverage the Earth's curvature to shorten distances, reducing fuel consumption relative to rhumb line alternatives; for instance, a New York to Hong Kong flight can save approximately 16,000 liters of fuel through polar path optimization.[15][16]
Modern digital tools incorporate gnomonic principles for seamless great circle computation in navigation systems. Electronic Chart Display and Information Systems (ECDIS), mandated by the International Maritime Organization for commercial shipping, support gnomonic-based route planning alongside primary Mercator views, allowing real-time calculation and overlay of shortest paths on electronic nautical charts. Similarly, aviation apps like SkyVector utilize embedded great circle algorithms derived from gnomonic geometry to generate efficient flight plans interactively.[17][18]
As advancements in aircraft range and computational aids emphasized shortest-path optimization in both maritime and aerial operations, gnomonic projections saw increased use for long-haul efficiency.[19]
The projection has also been applied to regional mapping, such as for Antarctica and the Pacific Ocean in USGS projects, and in seismic studies for plotting great-circle paths.[3]
In recent years, gnomonic projections have found application in simulations for satellite path planning, particularly for low-Earth orbit missions, where the straight-line representation of great circles aids in modeling and optimizing trajectories amid perturbations like atmospheric drag.[20]
Astronomy and Celestial Mapping
The gnomonic projection has been employed in astronomy since the 19th century for creating all-sky maps and star atlases, where its key advantage is rendering great circles—such as the ecliptic or equatorial paths—as straight lines, facilitating the plotting of celestial motions and alignments.[21] This property proved particularly valuable for early star charts used in planetariums and telescope observations, allowing astronomers to visualize and predict the apparent paths of stars and planets without curvature distortion in local sky regions.[22] By the early 20th century, gnomonic star atlases became standard tools for amateur and professional observers, enabling precise manual reductions of telescope pointings by aligning observed great-circle arcs directly on the map.[21]
In planetary mapping, NASA has utilized gnomonic projections to reprocess lander imagery for extraterrestrial surface analysis, notably with the 1976 Viking missions on Mars, where stereo images were transformed via gnomonic methods to generate perspective views and path-planning mosaics for rover navigation.[23] Similarly, for lunar exploration, polar gnomonic projections have been applied to model illumination and terrain for rover trajectories, as seen in analyses supporting missions like the Lunar Reconnaissance Orbiter, where great-circle routes on the Moon's surface are depicted linearly to assess lighting conditions and safe paths.[24] These applications extend to broader space operations, including satellite trajectory planning, where orbital great circles are mapped as straight lines to simplify collision avoidance and mission design in near-Earth and deep-space environments.[25] The projection's utility in deep space is evident in tracking comet paths, which approximate great-circle projections from Earth's viewpoint, allowing linear representation of hyperbolic trajectories for predictive modeling.[25]
Modern astronomical software continues to leverage the gnomonic projection for image processing and visualization, with tools like Stellarium incorporating it as a core sky projection mode to simulate telescope fields of view and generate printable charts where celestial great circles remain straight.[26] SAOImage DS9, a widely used FITS viewer, supports gnomonic (TAN) projections through World Coordinate System (WCS) standards, enabling astronomers to analyze and reproject deep-sky images for accurate astrometry in surveys.[27] Post-2010 advancements include its integration in exoplanet mapping pipelines, where gnomonic reprojections handle distorted sky coordinates from transit observations, and in data visualization for missions like the Nancy Grace Roman Space Telescope, facilitating the tessellation and alignment of multi-instrument celestial mosaics for high-resolution atmospheric studies as of 2025.[28]
Comparisons
With Other Azimuthal Projections
The gnomonic projection shares the azimuthal family characteristic with stereographic and orthographic projections, preserving true directions from the central point of tangency, which makes all three suitable for polar or hemispheric mapping where radial accuracy is essential.[11] However, the gnomonic projection is unique in rendering all great circles as straight lines, facilitating the visualization of shortest paths on Earth's surface, whereas the stereographic and orthographic projections only depict great circles as straight lines when they radiate from the center.[5] This distinction arises from their geometric constructions: the gnomonic projects from the Earth's center onto a tangent plane, the stereographic from a point on the sphere's surface opposite the plane, and the orthographic from an infinite distance using parallel rays.[29]
In comparison to the stereographic projection, the gnomonic does not preserve angles or local shapes, leading to non-conformal mapping where angles are distorted away from the center, while the stereographic is conformal, maintaining angles and thus better preserving the shapes of small features.[11] The gnomonic's scale distortion escalates infinitely toward the projection's edge, rendering it unusable for areas beyond about 60° from the center, in contrast to the stereographic's more gradual scale and area distortions that allow coverage of larger regions, such as entire continents or polar areas.[5] Consequently, the gnomonic excels in applications requiring straight-line geodesics, like route planning, whereas the stereographic is preferred for polar maps and geophysical analyses where angle preservation aids in detailed feature representation.[29]
Relative to the orthographic projection, the gnomonic provides a fuller hemispheric view but with an infinite edge due to its central projection point, while the orthographic simulates an external viewpoint, limiting it to a half-sphere appearance with a finite but curved edge and no straight great circles except from the center.[11] Both exhibit increasing area and shape distortions from the center, but the orthographic's distortions create a more visually realistic globe-like effect suitable for illustrative purposes, such as celestial or planetary views, whereas the gnomonic's extreme distortions prioritize navigational utility over aesthetics.[5] Use cases diverge accordingly: the orthographic is ideal for thematic world maps or space-oriented depictions, contrasting the gnomonic's focus on practical geodesic plotting.[29]
To illustrate distortion differences within the azimuthal family, the following table summarizes representative scale distortion indices (as percentages of true scale) for meridian distances from the center, based on standard analyses for polar aspects; values increase radially and highlight the gnomonic's rapid escalation.
| Distance from Center | Gnomonic Scale Distortion (%) | Stereographic Scale Distortion (%) | Orthographic Scale Distortion (%) |
|---|
| 15° | 7.2 | ~1.7 | ~3.4 |
| 45° | 100 | ~17 | ~29 |
| 60° | 300 | ~33 | ~50 |
| 90° (edge) | Infinite | ~100 | 100 (total collapse) |
With Conic and Cylindrical Projections
The gnomonic projection, as an azimuthal type, differs fundamentally from cylindrical projections like the Mercator in its geometric construction and distortion profile. While the gnomonic projects from the Earth's center onto a tangent plane, resulting in infinite radial distortion that limits it to a hemisphere or less, the Mercator wraps a cylinder tangent at the equator, producing parallel meridians and increasingly spaced parallels toward the poles with infinite latitudinal distortion at high latitudes.[5][30] The Mercator is conformal, preserving local shapes and angles for accurate directional plotting, but it curves great circles into rhumb lines, whereas the gnomonic renders all great circles as straight lines, prioritizing geodesic paths over conformality.[31][5]
In contrast to conic projections such as the Albers equal-area conic, the gnomonic is limited to a single tangent point, often at a pole, making it unsuitable for broad latitudinal spans beyond about 60 degrees from the center due to rapidly increasing distortions.[30] The Albers, however, employs a secant cone intersecting the globe along two standard parallels (typically in mid-latitudes, e.g., 29.5°N and 45.5°N for the contiguous United States), minimizing areal distortion between them while preserving areas accurately across larger east-west extents.[5][31] Unlike the gnomonic's azimuthal equidistance from the center, conic projections lack this directional focus, with meridians converging and parallels forming arcs, which better suits regional mapping but introduces shape distortions outside the standard parallels.[30]
These differences highlight the gnomonic's strengths in polar or short-range geodesic applications, such as high-latitude route planning, compared to cylindrical projections' suitability for global or equatorial coverage and conic types' efficacy for mid-latitude continental areas.[5] Cylindrical and conic projections do not inherently preserve azimuthal properties, making them less ideal for point-specific directionality, though the gnomonic excels locally at the expense of global usability.[31] In practice, the gnomonic is frequently paired with the Mercator for navigation, using the former to plot straight-line great circle routes and the latter for conformal charting during travel.[5]