diff options
Diffstat (limited to 'src/projections/tobmerc.cpp')
| -rw-r--r-- | src/projections/tobmerc.cpp | 19 |
1 files changed, 8 insertions, 11 deletions
diff --git a/src/projections/tobmerc.cpp b/src/projections/tobmerc.cpp index a1616036..f05a9b6b 100644 --- a/src/projections/tobmerc.cpp +++ b/src/projections/tobmerc.cpp @@ -9,27 +9,24 @@ PROJ_HEAD(tobmerc, "Tobler-Mercator") "\n\tCyl, Sph"; -#define EPS10 1.e-10 -static double logtanpfpim1(double x) { /* log(tan(x/2 + M_FORTPI)) */ - if (fabs(x) <= DBL_EPSILON) { - /* tan(M_FORTPI + .5 * x) can be approximated by 1.0 + x */ - return log1p(x); - } - return log(tan(M_FORTPI + .5 * x)); -} - static PJ_XY tobmerc_s_forward (PJ_LP lp, PJ *P) { /* Spheroidal, forward */ PJ_XY xy = {0.0, 0.0}; double cosphi; - if (fabs(fabs(lp.phi) - M_HALFPI) <= EPS10) { + if (fabs(lp.phi) >= M_HALFPI) { + // builtins.gie tests "Test expected failure at the poles:". However + // given that M_HALFPI is strictly less than pi/2 in double precision, + // it's not clear why shouldn't just return a large result for xy.y (and + // it's not even that large, merely 38.025...). Even if the logic was + // such that phi was strictly equal to pi/2, allowing xy.y = inf would be + // a reasonable result. proj_errno_set(P, PJD_ERR_TOLERANCE_CONDITION); return xy; } cosphi = cos(lp.phi); xy.x = P->k0 * lp.lam * cosphi * cosphi; - xy.y = P->k0 * logtanpfpim1(lp.phi); + xy.y = P->k0 * asinh(tan(lp.phi)); return xy; } |
