// Boost.Geometry
-// Copyright (c) 2016-2017 Oracle and/or its affiliates.
+// Copyright (c) 2016-2018 Oracle and/or its affiliates.
+// Contributed and/or modified by Vissarion Fysikopoulos, on behalf of Oracle
// Contributed and/or modified by Adam Wulkiewicz, on behalf of Oracle
// Use, modification and distribution is subject to the Boost Software License,
#include <boost/math/constants/constants.hpp>
+#include <boost/geometry/core/assert.hpp>
#include <boost/geometry/core/radius.hpp>
#include <boost/geometry/util/condition.hpp>
/*!
\brief The solution of the direct problem of geodesics on latlong coordinates,
- Forsyth-Andoyer-Lambert type approximation with second order terms.
+ Forsyth-Andoyer-Lambert type approximation with first/second order terms.
\author See
- Technical Report: PAUL D. THOMAS, MATHEMATICAL MODELS FOR NAVIGATION SYSTEMS, 1965
http://www.dtic.mil/docs/citations/AD0627893
- Technical Report: PAUL D. THOMAS, SPHEROIDAL GEODESICS, REFERENCE SYSTEMS, AND LOCAL GEOMETRY, 1970
http://www.dtic.mil/docs/citations/AD0703541
-
*/
template <
typename CT,
+ bool SecondOrder = true,
bool EnableCoordinates = true,
bool EnableReverseAzimuth = false,
bool EnableReducedLength = false,
CT const lon1 = lo1;
CT const lat1 = la1;
- if ( math::equals(distance, Dist(0)) || distance < Dist(0) )
- {
- result.lon2 = lon1;
- result.lat2 = lat1;
- return result;
- }
-
CT const c0 = 0;
CT const c1 = 1;
CT const c2 = 2;
CT const pi = math::pi<CT>();
CT const pi_half = pi / c2;
+ BOOST_GEOMETRY_ASSERT(-pi <= azimuth12 && azimuth12 <= pi);
+
// keep azimuth small - experiments show low accuracy
// if the azimuth is closer to (+-)180 deg.
CT azi12_alt = azimuth12;
CT lat1_alt = lat1;
bool alter_result = vflip_if_south(lat1, azimuth12, lat1_alt, azi12_alt);
-
+
CT const theta1 = math::equals(lat1_alt, pi_half) ? lat1_alt :
math::equals(lat1_alt, -pi_half) ? lat1_alt :
atan(one_minus_f * tan(lat1_alt));
CT const N = cos_theta1 * cos_a12;
CT const C1 = f * M; // lower-case c1 in the technical report
CT const C2 = f * (c1 - math::sqr(M)) / c4; // lower-case c2 in the technical report
- CT const D = (c1 - C2) * (c1 - C2 - C1 * M);
- CT const P = C2 * (c1 + C1 * M / c2) / D;
-
+ CT D = 0;
+ CT P = 0;
+ if ( BOOST_GEOMETRY_CONDITION(SecondOrder) )
+ {
+ D = (c1 - C2) * (c1 - C2 - C1 * M);
+ P = C2 * (c1 + C1 * M / c2) / D;
+ }
+ else
+ {
+ D = c1 - c2 * C2 - C1 * M;
+ P = C2 / D;
+ }
// special case for equator:
// sin_theta0 = 0 <=> lat1 = 0 ^ |azimuth12| = pi/2
// NOTE: in this case it doesn't matter what's the value of cos_sigma1 because
CT const W = c1 - c2 * P * cos_u;
CT const V = cos_u * cos_d - sin_u * sin_d;
- CT const X = math::sqr(C2) * sin_d * cos_d * (2 * math::sqr(V) - c1);
CT const Y = c2 * P * V * W * sin_d;
- CT const d_sigma = d + X - Y;
+ CT X = 0;
+ CT d_sigma = d - Y;
+ if ( BOOST_GEOMETRY_CONDITION(SecondOrder) )
+ {
+ X = math::sqr(C2) * sin_d * cos_d * (2 * math::sqr(V) - c1);
+ d_sigma += X;
+ }
CT const sin_d_sigma = sin(d_sigma);
CT const cos_d_sigma = cos(d_sigma);
if (BOOST_GEOMETRY_CONDITION(CalcCoordinates))
{
CT const S_sigma = c2 * sigma1 - d_sigma;
- CT const cos_S_sigma = cos(S_sigma);
+ CT cos_S_sigma = 0;
+ CT H = C1 * d_sigma;
+ if ( BOOST_GEOMETRY_CONDITION(SecondOrder) )
+ {
+ cos_S_sigma = cos(S_sigma);
+ H = H * (c1 - C2) - C1 * C2 * sin_d_sigma * cos_S_sigma;
+ }
CT const d_eta = atan2(sin_d_sigma * sin_a12, cos_theta1 * cos_d_sigma - sin_theta1 * sin_d_sigma * cos_a12);
- CT const H = C1 * (c1 - C2) * d_sigma - C1 * C2 * sin_d_sigma * cos_S_sigma;
CT const d_lambda = d_eta - H;
-
+
result.lon2 = lon1 + d_lambda;
if (! math::equals(M, c0))