Abstract
To deal specifically with the case of a nearly antipodal geodesic of given terminal positions, an equation in azimuth is produced for solution by the Newton-Raphson Method of successive approximation. When the azimuth is in the region of 90° it is found that an approach is best made by a development in series when the aim is precision calculation. Degeneracy is examined theoretically and graphically.
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Abbreviations
- e:
-
eccentricity of the spheroid
- f:
-
flattening of the spheroid
- φ1, φ2 :
-
geographical latitudes of the ends of the lineP 1 ,P 2 respectively
- U 1 ,U 2 :
-
parametric latitudes corresponding to φ1, φ2 respectively
- L :
-
difference in geographical longitude between the ends of the lineP 1 P 2 . Also as longitude for a point at parametric latitude U on a geodesic for terms ofdU/dL, etc...
- a 1,a 2 :
-
azimuths at the ends of the lineP 1 ,P 2 respectively
- a :
-
azimuth of the line at the equator
- λ:
-
spherical difference in longitude corresponding toL
- σ:
-
spherical central angle
- θ:
-
90°−a
- s1 :
-
sinU1
- c1 :
-
cosU1
- s2 :
-
sinU2
- c2 :
-
cosU2
Reference
H. F. RAINSFORD: Long geodesics on the ellipsoid., B. Géodésique, 37, 12–22. 1955.
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Bowring, B.R. Solution for azimuth of the geodesic in near antipodal situations with special reference to the behaviour of lines for which the azimuth is in the region of 90°. Bull. Geodesique 51, 17–32 (1977). https://doi.org/10.1007/BF02521538
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DOI: https://doi.org/10.1007/BF02521538