ellint.c
来自「math library from gnu」· C语言 代码 · 共 628 行 · 第 1/2 页
C
628 行
double sin_phi = sin(phi); double sin2_phi = sin_phi*sin_phi; double x = 1.0 - sin2_phi; double y = 1.0 - k*k*sin2_phi; gsl_sf_result rf; int status = gsl_sf_ellint_RF_e(x, y, 1.0, mode, &rf); result->val = sin_phi * rf.val; result->err = GSL_DBL_EPSILON * fabs(result->val) + fabs(sin_phi*rf.err); if (nc == 0) { return status; } else { gsl_sf_result rk; /* add extra terms from periodicity */ const int rkstatus = gsl_sf_ellint_Kcomp_e(k, mode, &rk); result->val += 2*nc*rk.val; result->err += 2*fabs(nc)*rk.err; return GSL_ERROR_SELECT_2(status, rkstatus); } }}/* [Carlson, Numer. Math. 33 (1979) 1, (4.2)] */intgsl_sf_ellint_E_e(double phi, double k, gsl_mode_t mode, gsl_sf_result * result){ /* Angular reduction to -pi/2 < phi < pi/2 (we should really use an exact reduction but this will have to do for now) BJG */ double nc = floor(phi/M_PI + 0.5); double phi_red = phi - nc * M_PI; phi = phi_red; { const double sin_phi = sin(phi); const double sin2_phi = sin_phi * sin_phi; const double x = 1.0 - sin2_phi; const double y = 1.0 - k*k*sin2_phi; if(x < GSL_DBL_EPSILON) { gsl_sf_result re; const int status = gsl_sf_ellint_Ecomp_e(k, mode, &re); /* could use A&S 17.4.14 to improve the value below */ result->val = 2*nc*re.val + GSL_SIGN(sin_phi) * re.val; result->err = 2*fabs(nc)*re.err + re.err; return status; } else { gsl_sf_result rf, rd; const double sin3_phi = sin2_phi * sin_phi; const int rfstatus = gsl_sf_ellint_RF_e(x, y, 1.0, mode, &rf); const int rdstatus = gsl_sf_ellint_RD_e(x, y, 1.0, mode, &rd); result->val = sin_phi * rf.val - k*k/3.0 * sin3_phi * rd.val; result->err = GSL_DBL_EPSILON * fabs(sin_phi * rf.val); result->err += fabs(sin_phi*rf.err); result->err += k*k/3.0 * GSL_DBL_EPSILON * fabs(sin3_phi * rd.val); result->err += k*k/3.0 * fabs(sin3_phi*rd.err); if (nc == 0) { return GSL_ERROR_SELECT_2(rfstatus, rdstatus); } else { gsl_sf_result re; /* add extra terms from periodicity */ const int restatus = gsl_sf_ellint_Ecomp_e(k, mode, &re); result->val += 2*nc*re.val; result->err += 2*fabs(nc)*re.err; return GSL_ERROR_SELECT_3(rfstatus, rdstatus, restatus); } } }}/* [Carlson, Numer. Math. 33 (1979) 1, (4.3)] */intgsl_sf_ellint_P_e(double phi, double k, double n, gsl_mode_t mode, gsl_sf_result * result){ /* Angular reduction to -pi/2 < phi < pi/2 (we should really use an exact reduction but this will have to do for now) BJG */ double nc = floor(phi/M_PI + 0.5); double phi_red = phi - nc * M_PI; phi = phi_red; /* FIXME: need to handle the case of small x, as for E,F */ { const double sin_phi = sin(phi); const double sin2_phi = sin_phi * sin_phi; const double sin3_phi = sin2_phi * sin_phi; const double x = 1.0 - sin2_phi; const double y = 1.0 - k*k*sin2_phi; gsl_sf_result rf; gsl_sf_result rj; const int rfstatus = gsl_sf_ellint_RF_e(x, y, 1.0, mode, &rf); const int rjstatus = gsl_sf_ellint_RJ_e(x, y, 1.0, 1.0 + n*sin2_phi, mode, &rj); result->val = sin_phi * rf.val - n/3.0*sin3_phi * rj.val; result->err = GSL_DBL_EPSILON * fabs(sin_phi * rf.val); result->err += fabs(sin_phi * rf.err); result->err += n/3.0 * GSL_DBL_EPSILON * fabs(sin3_phi*rj.val); result->err += n/3.0 * fabs(sin3_phi*rj.err); if (nc == 0) { return GSL_ERROR_SELECT_2(rfstatus, rjstatus); } else { gsl_sf_result rp; /* add extra terms from periodicity */ const int rpstatus = gsl_sf_ellint_Pcomp_e(k, n, mode, &rp); result->val += 2*nc*rp.val; result->err += 2*fabs(nc)*rp.err; return GSL_ERROR_SELECT_3(rfstatus, rjstatus, rpstatus); } }}/* [Carlson, Numer. Math. 33 (1979) 1, (4.4)] */intgsl_sf_ellint_D_e(double phi, double k, double n, gsl_mode_t mode, gsl_sf_result * result){ /* Angular reduction to -pi/2 < phi < pi/2 (we should really use an exact reduction but this will have to do for now) BJG */ double nc = floor(phi/M_PI + 0.5); double phi_red = phi - nc * M_PI; phi = phi_red; /* FIXME: need to handle the case of small x, as for E,F */ { const double sin_phi = sin(phi); const double sin2_phi = sin_phi * sin_phi; const double sin3_phi = sin2_phi * sin_phi; const double x = 1.0 - sin2_phi; const double y = 1.0 - k*k*sin2_phi; gsl_sf_result rd; const int status = gsl_sf_ellint_RD_e(x, y, 1.0, mode, &rd); result->val = sin3_phi/3.0 * rd.val; result->err = GSL_DBL_EPSILON * fabs(result->val) + fabs(sin3_phi/3.0 * rd.err); if (nc == 0) { return status; } else { gsl_sf_result rd; /* add extra terms from periodicity */ const int rdstatus = gsl_sf_ellint_Dcomp_e(k, mode, &rd); result->val += 2*nc*rd.val; result->err += 2*fabs(nc)*rd.err; return GSL_ERROR_SELECT_2(status, rdstatus); } }}intgsl_sf_ellint_Dcomp_e(double k, gsl_mode_t mode, gsl_sf_result * result){ if(k*k >= 1.0) { DOMAIN_ERROR(result); } else { const double y = 1.0 - k*k; /* FIXME: still need to handle k~=~1 */ gsl_sf_result rd; const int status = gsl_sf_ellint_RD_e(0.0, y, 1.0, mode, &rd); result->val = (1.0/3.0) * rd.val; result->err = GSL_DBL_EPSILON * fabs(result->val) + fabs(1.0/3.0 * rd.err); return status; }}/* [Carlson, Numer. Math. 33 (1979) 1, (4.5)] */intgsl_sf_ellint_Kcomp_e(double k, gsl_mode_t mode, gsl_sf_result * result){ if(k*k >= 1.0) { DOMAIN_ERROR(result); } else if(k*k >= 1.0 - GSL_SQRT_DBL_EPSILON) { /* [Abramowitz+Stegun, 17.3.34] */ const double y = 1.0 - k*k; const double a[] = { 1.38629436112, 0.09666344259, 0.03590092383 }; const double b[] = { 0.5, 0.12498593597, 0.06880248576 }; const double ta = a[0] + y*(a[1] + y*a[2]); const double tb = -log(y) * (b[0] + y*(b[1] + y*b[2])); result->val = ta + tb; result->err = 2.0 * GSL_DBL_EPSILON * (fabs(result->val) + fabs(k/y)); return GSL_SUCCESS; } else { /* This was previously computed as, return gsl_sf_ellint_RF_e(0.0, 1.0 - k*k, 1.0, mode, result); but this underestimated the total error for small k, since the argument y=1-k^2 is not exact (there is an absolute error of GSL_DBL_EPSILON near y=0 due to cancellation in the subtraction). Taking the singular behavior of -log(y) above gives an error of 0.5*epsilon/y near y=0. (BJG) */ double y = 1.0 - k*k; int status = gsl_sf_ellint_RF_e(0.0, y, 1.0, mode, result); result->err += 0.5 * GSL_DBL_EPSILON / y; return status ; }}/* [Carlson, Numer. Math. 33 (1979) 1, (4.6)] */intgsl_sf_ellint_Ecomp_e(double k, gsl_mode_t mode, gsl_sf_result * result){ if(k*k >= 1.0) { DOMAIN_ERROR(result); } else if(k*k >= 1.0 - GSL_SQRT_DBL_EPSILON) { /* [Abramowitz+Stegun, 17.3.36] */ const double y = 1.0 - k*k; const double a[] = { 0.44325141463, 0.06260601220, 0.04757383546 }; const double b[] = { 0.24998368310, 0.09200180037, 0.04069697526 }; const double ta = 1.0 + y*(a[0] + y*(a[1] + a[2]*y)); const double tb = -y*log(y) * (b[0] + y*(b[1] + b[2]*y)); result->val = ta + tb; result->err = 2.0 * GSL_DBL_EPSILON * result->val; return GSL_SUCCESS; } else { gsl_sf_result rf; gsl_sf_result rd; const double y = 1.0 - k*k; const int rfstatus = gsl_sf_ellint_RF_e(0.0, y, 1.0, mode, &rf); const int rdstatus = gsl_sf_ellint_RD_e(0.0, y, 1.0, mode, &rd); result->val = rf.val - k*k/3.0 * rd.val; result->err = rf.err + k*k/3.0 * rd.err; return GSL_ERROR_SELECT_2(rfstatus, rdstatus); }}/* [Carlson, Numer. Math. 33 (1979) 1, (4.3) phi=pi/2] */intgsl_sf_ellint_Pcomp_e(double k, double n, gsl_mode_t mode, gsl_sf_result * result){ if(k*k >= 1.0) { DOMAIN_ERROR(result); } /* FIXME: need to handle k ~=~ 1 cancellations */ else { gsl_sf_result rf; gsl_sf_result rj; const double y = 1.0 - k*k; const int rfstatus = gsl_sf_ellint_RF_e(0.0, y, 1.0, mode, &rf); const int rjstatus = gsl_sf_ellint_RJ_e(0.0, y, 1.0, 1.0 + n, mode, &rj); result->val = rf.val - (n/3.0) * rj.val; result->err = rf.err + fabs(n/3.0) * rj.err; return GSL_ERROR_SELECT_2(rfstatus, rjstatus); }}/*-*-*-*-*-*-*-*-*-* Functions w/ Natural Prototypes *-*-*-*-*-*-*-*-*-*-*/#include "eval.h"double gsl_sf_ellint_Kcomp(double k, gsl_mode_t mode){ EVAL_RESULT(gsl_sf_ellint_Kcomp_e(k, mode, &result));}double gsl_sf_ellint_Ecomp(double k, gsl_mode_t mode){ EVAL_RESULT(gsl_sf_ellint_Ecomp_e(k, mode, &result));}double gsl_sf_ellint_Pcomp(double k, double n, gsl_mode_t mode){ EVAL_RESULT(gsl_sf_ellint_Pcomp_e(k, n, mode, &result));}double gsl_sf_ellint_Dcomp(double k, gsl_mode_t mode){ EVAL_RESULT(gsl_sf_ellint_Dcomp_e(k, mode, &result));}double gsl_sf_ellint_F(double phi, double k, gsl_mode_t mode){ EVAL_RESULT(gsl_sf_ellint_F_e(phi, k, mode, &result));}double gsl_sf_ellint_E(double phi, double k, gsl_mode_t mode){ EVAL_RESULT(gsl_sf_ellint_E_e(phi, k, mode, &result));}double gsl_sf_ellint_P(double phi, double k, double n, gsl_mode_t mode){ EVAL_RESULT(gsl_sf_ellint_P_e(phi, k, n, mode, &result));}double gsl_sf_ellint_D(double phi, double k, double n, gsl_mode_t mode){ EVAL_RESULT(gsl_sf_ellint_D_e(phi, k, n, mode, &result));}double gsl_sf_ellint_RC(double x, double y, gsl_mode_t mode){ EVAL_RESULT(gsl_sf_ellint_RC_e(x, y, mode, &result));}double gsl_sf_ellint_RD(double x, double y, double z, gsl_mode_t mode){ EVAL_RESULT(gsl_sf_ellint_RD_e(x, y, z, mode, &result));}double gsl_sf_ellint_RF(double x, double y, double z, gsl_mode_t mode){ EVAL_RESULT(gsl_sf_ellint_RF_e(x, y, z, mode, &result));}double gsl_sf_ellint_RJ(double x, double y, double z, double p, gsl_mode_t mode){ EVAL_RESULT(gsl_sf_ellint_RJ_e(x, y, z, p, mode, &result));}
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