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- // Boost.Geometry
- // Copyright (c) 2016-2019 Oracle and/or its affiliates.
- // Contributed and/or modified by Adam Wulkiewicz, on behalf of Oracle
- // Use, modification and distribution is subject to the Boost Software License,
- // Version 1.0. (See accompanying file LICENSE_1_0.txt or copy at
- // http://www.boost.org/LICENSE_1_0.txt)
- #ifndef BOOST_GEOMETRY_FORMULAS_INVERSE_DIFFERENTIAL_QUANTITIES_HPP
- #define BOOST_GEOMETRY_FORMULAS_INVERSE_DIFFERENTIAL_QUANTITIES_HPP
- #include <boost/geometry/core/assert.hpp>
- #include <boost/geometry/util/condition.hpp>
- #include <boost/geometry/util/math.hpp>
- namespace boost { namespace geometry { namespace formula
- {
- /*!
- \brief The solution of a part of the inverse problem - differential quantities.
- \author See
- - Charles F.F Karney, Algorithms for geodesics, 2011
- https://arxiv.org/pdf/1109.4448.pdf
- */
- template <
- typename CT,
- bool EnableReducedLength,
- bool EnableGeodesicScale,
- unsigned int Order = 2,
- bool ApproxF = true
- >
- class differential_quantities
- {
- public:
- static inline void apply(CT const& lon1, CT const& lat1,
- CT const& lon2, CT const& lat2,
- CT const& azimuth, CT const& reverse_azimuth,
- CT const& b, CT const& f,
- CT & reduced_length, CT & geodesic_scale)
- {
- CT const dlon = lon2 - lon1;
- CT const sin_lat1 = sin(lat1);
- CT const cos_lat1 = cos(lat1);
- CT const sin_lat2 = sin(lat2);
- CT const cos_lat2 = cos(lat2);
- apply(dlon, sin_lat1, cos_lat1, sin_lat2, cos_lat2,
- azimuth, reverse_azimuth,
- b, f,
- reduced_length, geodesic_scale);
- }
- static inline void apply(CT const& dlon,
- CT const& sin_lat1, CT const& cos_lat1,
- CT const& sin_lat2, CT const& cos_lat2,
- CT const& azimuth, CT const& reverse_azimuth,
- CT const& b, CT const& f,
- CT & reduced_length, CT & geodesic_scale)
- {
- CT const c0 = 0;
- CT const c1 = 1;
- CT const one_minus_f = c1 - f;
- CT sin_bet1 = one_minus_f * sin_lat1;
- CT sin_bet2 = one_minus_f * sin_lat2;
-
- // equator
- if (math::equals(sin_bet1, c0) && math::equals(sin_bet2, c0))
- {
- CT const sig_12 = dlon / one_minus_f;
- if (BOOST_GEOMETRY_CONDITION(EnableReducedLength))
- {
- BOOST_GEOMETRY_ASSERT((-math::pi<CT>() <= azimuth && azimuth <= math::pi<CT>()));
- int azi_sign = math::sign(azimuth) >= 0 ? 1 : -1; // for antipodal
- CT m12 = azi_sign * sin(sig_12) * b;
- reduced_length = m12;
- }
-
- if (BOOST_GEOMETRY_CONDITION(EnableGeodesicScale))
- {
- CT M12 = cos(sig_12);
- geodesic_scale = M12;
- }
- }
- else
- {
- CT const c2 = 2;
- CT const e2 = f * (c2 - f);
- CT const ep2 = e2 / math::sqr(one_minus_f);
- CT const sin_alp1 = sin(azimuth);
- CT const cos_alp1 = cos(azimuth);
- //CT const sin_alp2 = sin(reverse_azimuth);
- CT const cos_alp2 = cos(reverse_azimuth);
- CT cos_bet1 = cos_lat1;
- CT cos_bet2 = cos_lat2;
- normalize(sin_bet1, cos_bet1);
- normalize(sin_bet2, cos_bet2);
- CT sin_sig1 = sin_bet1;
- CT cos_sig1 = cos_alp1 * cos_bet1;
- CT sin_sig2 = sin_bet2;
- CT cos_sig2 = cos_alp2 * cos_bet2;
- normalize(sin_sig1, cos_sig1);
- normalize(sin_sig2, cos_sig2);
- CT const sin_alp0 = sin_alp1 * cos_bet1;
- CT const cos_alp0_sqr = c1 - math::sqr(sin_alp0);
- CT const J12 = BOOST_GEOMETRY_CONDITION(ApproxF) ?
- J12_f(sin_sig1, cos_sig1, sin_sig2, cos_sig2, cos_alp0_sqr, f) :
- J12_ep_sqr(sin_sig1, cos_sig1, sin_sig2, cos_sig2, cos_alp0_sqr, ep2) ;
- CT const dn1 = math::sqrt(c1 + ep2 * math::sqr(sin_bet1));
- CT const dn2 = math::sqrt(c1 + ep2 * math::sqr(sin_bet2));
- if (BOOST_GEOMETRY_CONDITION(EnableReducedLength))
- {
- CT const m12_b = dn2 * (cos_sig1 * sin_sig2)
- - dn1 * (sin_sig1 * cos_sig2)
- - cos_sig1 * cos_sig2 * J12;
- CT const m12 = m12_b * b;
- reduced_length = m12;
- }
- if (BOOST_GEOMETRY_CONDITION(EnableGeodesicScale))
- {
- CT const cos_sig12 = cos_sig1 * cos_sig2 + sin_sig1 * sin_sig2;
- CT const t = ep2 * (cos_bet1 - cos_bet2) * (cos_bet1 + cos_bet2) / (dn1 + dn2);
- CT const M12 = cos_sig12 + (t * sin_sig2 - cos_sig2 * J12) * sin_sig1 / dn1;
- geodesic_scale = M12;
- }
- }
- }
- private:
- /*! Approximation of J12, expanded into taylor series in f
- Maxima script:
- ep2: f * (2-f) / ((1-f)^2);
- k2: ca02 * ep2;
- assume(f < 1);
- assume(sig > 0);
- I1(sig):= integrate(sqrt(1 + k2 * sin(s)^2), s, 0, sig);
- I2(sig):= integrate(1/sqrt(1 + k2 * sin(s)^2), s, 0, sig);
- J(sig):= I1(sig) - I2(sig);
- S: taylor(J(sig), f, 0, 3);
- S1: factor( 2*integrate(sin(s)^2,s,0,sig)*ca02*f );
- S2: factor( ((integrate(-6*ca02^2*sin(s)^4+6*ca02*sin(s)^2,s,0,sig)+integrate(-2*ca02^2*sin(s)^4+6*ca02*sin(s)^2,s,0,sig))*f^2)/4 );
- S3: factor( ((integrate(30*ca02^3*sin(s)^6-54*ca02^2*sin(s)^4+24*ca02*sin(s)^2,s,0,sig)+integrate(6*ca02^3*sin(s)^6-18*ca02^2*sin(s)^4+24*ca02*sin(s)^2,s,0,sig))*f^3)/12 );
- */
- static inline CT J12_f(CT const& sin_sig1, CT const& cos_sig1,
- CT const& sin_sig2, CT const& cos_sig2,
- CT const& cos_alp0_sqr, CT const& f)
- {
- if (Order == 0)
- {
- return 0;
- }
- CT const c2 = 2;
- CT const sig_12 = atan2(cos_sig1 * sin_sig2 - sin_sig1 * cos_sig2,
- cos_sig1 * cos_sig2 + sin_sig1 * sin_sig2);
- CT const sin_2sig1 = c2 * cos_sig1 * sin_sig1; // sin(2sig1)
- CT const sin_2sig2 = c2 * cos_sig2 * sin_sig2; // sin(2sig2)
- CT const sin_2sig_12 = sin_2sig2 - sin_2sig1;
- CT const L1 = sig_12 - sin_2sig_12 / c2;
- if (Order == 1)
- {
- return cos_alp0_sqr * f * L1;
- }
-
- CT const sin_4sig1 = c2 * sin_2sig1 * (math::sqr(cos_sig1) - math::sqr(sin_sig1)); // sin(4sig1)
- CT const sin_4sig2 = c2 * sin_2sig2 * (math::sqr(cos_sig2) - math::sqr(sin_sig2)); // sin(4sig2)
- CT const sin_4sig_12 = sin_4sig2 - sin_4sig1;
-
- CT const c8 = 8;
- CT const c12 = 12;
- CT const c16 = 16;
- CT const c24 = 24;
- CT const L2 = -( cos_alp0_sqr * sin_4sig_12
- + (-c8 * cos_alp0_sqr + c12) * sin_2sig_12
- + (c12 * cos_alp0_sqr - c24) * sig_12)
- / c16;
- if (Order == 2)
- {
- return cos_alp0_sqr * f * (L1 + f * L2);
- }
- CT const c4 = 4;
- CT const c9 = 9;
- CT const c48 = 48;
- CT const c60 = 60;
- CT const c64 = 64;
- CT const c96 = 96;
- CT const c128 = 128;
- CT const c144 = 144;
- CT const cos_alp0_quad = math::sqr(cos_alp0_sqr);
- CT const sin3_2sig1 = math::sqr(sin_2sig1) * sin_2sig1;
- CT const sin3_2sig2 = math::sqr(sin_2sig2) * sin_2sig2;
- CT const sin3_2sig_12 = sin3_2sig2 - sin3_2sig1;
- CT const A = (c9 * cos_alp0_quad - c12 * cos_alp0_sqr) * sin_4sig_12;
- CT const B = c4 * cos_alp0_quad * sin3_2sig_12;
- CT const C = (-c48 * cos_alp0_quad + c96 * cos_alp0_sqr - c64) * sin_2sig_12;
- CT const D = (c60 * cos_alp0_quad - c144 * cos_alp0_sqr + c128) * sig_12;
- CT const L3 = (A + B + C + D) / c64;
- // Order 3 and higher
- return cos_alp0_sqr * f * (L1 + f * (L2 + f * L3));
- }
- /*! Approximation of J12, expanded into taylor series in e'^2
- Maxima script:
- k2: ca02 * ep2;
- assume(sig > 0);
- I1(sig):= integrate(sqrt(1 + k2 * sin(s)^2), s, 0, sig);
- I2(sig):= integrate(1/sqrt(1 + k2 * sin(s)^2), s, 0, sig);
- J(sig):= I1(sig) - I2(sig);
- S: taylor(J(sig), ep2, 0, 3);
- S1: factor( integrate(sin(s)^2,s,0,sig)*ca02*ep2 );
- S2: factor( (integrate(sin(s)^4,s,0,sig)*ca02^2*ep2^2)/2 );
- S3: factor( (3*integrate(sin(s)^6,s,0,sig)*ca02^3*ep2^3)/8 );
- */
- static inline CT J12_ep_sqr(CT const& sin_sig1, CT const& cos_sig1,
- CT const& sin_sig2, CT const& cos_sig2,
- CT const& cos_alp0_sqr, CT const& ep_sqr)
- {
- if (Order == 0)
- {
- return 0;
- }
- CT const c2 = 2;
- CT const c4 = 4;
- CT const c2a0ep2 = cos_alp0_sqr * ep_sqr;
- CT const sig_12 = atan2(cos_sig1 * sin_sig2 - sin_sig1 * cos_sig2,
- cos_sig1 * cos_sig2 + sin_sig1 * sin_sig2); // sig2 - sig1
- CT const sin_2sig1 = c2 * cos_sig1 * sin_sig1; // sin(2sig1)
- CT const sin_2sig2 = c2 * cos_sig2 * sin_sig2; // sin(2sig2)
- CT const sin_2sig_12 = sin_2sig2 - sin_2sig1;
- CT const L1 = (c2 * sig_12 - sin_2sig_12) / c4;
- if (Order == 1)
- {
- return c2a0ep2 * L1;
- }
- CT const c8 = 8;
- CT const c64 = 64;
-
- CT const sin_4sig1 = c2 * sin_2sig1 * (math::sqr(cos_sig1) - math::sqr(sin_sig1)); // sin(4sig1)
- CT const sin_4sig2 = c2 * sin_2sig2 * (math::sqr(cos_sig2) - math::sqr(sin_sig2)); // sin(4sig2)
- CT const sin_4sig_12 = sin_4sig2 - sin_4sig1;
-
- CT const L2 = (sin_4sig_12 - c8 * sin_2sig_12 + 12 * sig_12) / c64;
- if (Order == 2)
- {
- return c2a0ep2 * (L1 + c2a0ep2 * L2);
- }
- CT const sin3_2sig1 = math::sqr(sin_2sig1) * sin_2sig1;
- CT const sin3_2sig2 = math::sqr(sin_2sig2) * sin_2sig2;
- CT const sin3_2sig_12 = sin3_2sig2 - sin3_2sig1;
- CT const c9 = 9;
- CT const c48 = 48;
- CT const c60 = 60;
- CT const c512 = 512;
- CT const L3 = (c9 * sin_4sig_12 + c4 * sin3_2sig_12 - c48 * sin_2sig_12 + c60 * sig_12) / c512;
- // Order 3 and higher
- return c2a0ep2 * (L1 + c2a0ep2 * (L2 + c2a0ep2 * L3));
- }
- static inline void normalize(CT & x, CT & y)
- {
- CT const len = math::sqrt(math::sqr(x) + math::sqr(y));
- x /= len;
- y /= len;
- }
- };
- }}} // namespace boost::geometry::formula
- #endif // BOOST_GEOMETRY_FORMULAS_INVERSE_DIFFERENTIAL_QUANTITIES_HPP
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