E-3 The Newton form of a geodesic in Maupertuis gauge (sphere, ellipsoid-of-revolution) 553
11.7 h 9 h
6 h
3 h
0 h
Fig. E.3. Maupertuis gauged geodesic on S
2
R , conformal coordinates generated by the universal transverse
Mercator projection, solution of the boundary value problem, departing point Frankfurt, arrival point Taipeh,
time given for constant speed movement with respect to the arrival point.
11.7 h 9 h 6 h 3 h 0 h
Fig. E.4. Maupertuis gauged geodesic on S
2
R , conformal coordinates generated by the universal Lambert
projection, solution of the boundary value problem, departing point Frankfurt, arrival point Taipeh, time
given for constant speed movement with respect to the arrival point.
11.7 h 9 h
6 h
3 h
0 h
Fig. E.3. Maupertuis gauged geodesic on S
2
R , conformal coordinates generated by the universal transverse
Mercator projection, solution of the boundary value problem, departing point Frankfurt, arrival point Taipeh,
time given for constant speed movement with respect to the arrival point.
11.7 h 9 h 6 h 3 h 0 h
Fig. E.4. Maupertuis gauged geodesic on S
2
R , conformal coordinates generated by the universal Lambert
projection, solution of the boundary value problem, departing point Frankfurt, arrival point Taipeh, time
given for constant speed movement with respect to the arrival point.