| /third_party/boost/libs/math/example/ |
| D | HSO3SO4.cpp | 107 float theta1; in test_SO3_semipolar() local
116 theta1 = -pi+(idxtheta1*(2*pi))/number_of_intervals; in test_SO3_semipolar()
123 ::std::cout << "theta1 = " << theta1 << " ; "; in test_SO3_semipolar()
127 … ::boost::math::quaternion<float> q = ::boost::math::semipolar(rho, alpha, theta1, theta2); in test_SO3_semipolar()
163 float theta1; in test_SO3_multipolar() local
173 theta1 = -pi+(idxtheta1*(2*pi))/number_of_intervals; in test_SO3_multipolar()
180 ::std::cout << "theta1 = " << theta1 << " ; "; in test_SO3_multipolar()
184 … ::boost::math::quaternion<float> q = ::boost::math::multipolar(rho1, theta1, rho2, theta2); in test_SO3_multipolar()
355 float theta1; in test_SO4_spherical() local
381 theta1 = -pi+(idxtheta1*(2*pi))/number_of_intervals; in test_SO4_spherical()
[all …]
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| /third_party/skia/gm/ |
| D | mandoline.cpp | 189 float theta1 = 2*SK_ScalarPI/nquads * (i + .5f); in onDraw() local
191 mandoline.sliceQuadratic({cosf(theta1)*2, sinf(theta1)*2}, in onDraw()
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| /third_party/flutter/skia/gm/ |
| D | mandoline.cpp | 189 float theta1 = 2*SK_ScalarPI/nquads * (i + .5f); in onDraw() local
191 mandoline.sliceQuadratic({cosf(theta1)*2, sinf(theta1)*2}, in onDraw()
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| /third_party/boost/boost/geometry/formulas/ |
| D | thomas_inverse.hpp | 88 CT const theta1 = math::equals(lat1, pi_half) ? lat1 : in apply() local
95 CT const theta_m = (theta1 + theta2) / c2; in apply()
96 CT const d_theta_m = (theta2 - theta1) / c2; in apply()
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| D | thomas_direct.hpp | 93 CT const theta1 = math::equals(lat1_alt, pi_half) ? lat1_alt : in apply() local
96 CT const sin_theta1 = sin(theta1); in apply()
97 CT const cos_theta1 = cos(theta1); in apply()
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| /third_party/boost/libs/math/test/ |
| D | octonion_test.cpp | 512 float theta1 = 0; in octonion_manual_test() local
519 << "rho1 = " << rho1 << " , theta1 = " << theta1 in octonion_manual_test()
524 << ::boost::math::multipolar(rho1, theta1, rho2, theta2, in octonion_manual_test()
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| D | quaternion_test.cpp | 551 T theta1 = 0; in BOOST_AUTO_TEST_CASE_TEMPLATE() local
553 q1 = ::boost::math::multipolar(rho1, theta1, rho2, theta2); in BOOST_AUTO_TEST_CASE_TEMPLATE()
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| /third_party/boost/boost/math/ |
| D | quaternion.hpp | 1061 T const & theta1, in semipolar() argument
1067 T a = cos(alpha)*cos(theta1); in semipolar()
1068 T b = cos(alpha)*sin(theta1); in semipolar()
1078 T const & theta1, in multipolar() argument
1085 T a = rho1*cos(theta1); in multipolar()
1086 T b = rho1*sin(theta1); in multipolar()
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| D | octonion.hpp | 4058 T const & theta1, in multipolar() argument
4069 T a = rho1*cos(theta1); in multipolar()
4070 T b = rho1*sin(theta1); in multipolar()
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| /third_party/boost/libs/math/doc/octonion/ |
| D | output_more.txt | 37 The value of the octonion represented in multipolar form by rho1 = 1 , theta1 = 0 , rho2 = 2 , thet…
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| D | math-octonion.qbk | 133 … ``[link math_toolkit.oct_create multipolar]``(T const & rho1, T const & theta1, T const & rho2, T…
809 …template<typename T> octonion<T> multipolar(T const & rho1, T const & theta1, T const & rho2, T co…
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| /third_party/boost/libs/math/doc/quaternion/ |
| D | output_more.txt | 50 The value of the quaternion represented in multipolar form by rho1 = 1 , theta1 = 0 , rho2 = 2 , th…
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| D | math-quaternion.qbk | 126 …reation_semipolar semipolar]``(T const & rho, T const & alpha, T const & theta1, T const & theta2);
127 …_quaternions.creation_multipolar multipolar]``(T const & rho1, T const & theta1, T const & rho2, T…
705 …template<typename T> quaternion<T> semipolar(T const & rho, T const & alpha, T const & theta1, T c…
706 …template<typename T> quaternion<T> multipolar(T const & rho1, T const & theta1, T const & rho2, T …
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| /third_party/skia/third_party/externals/freetype/src/base/ |
| D | ftstroke.c | 204 FT_Angle theta1, theta2; in ft_cubic_is_small_enough() local
285 theta1 = ft_pos_abs( FT_Angle_Diff( *angle_in, *angle_mid ) ); in ft_cubic_is_small_enough()
288 return FT_BOOL( theta1 < FT_SMALL_CUBIC_THRESHOLD && in ft_cubic_is_small_enough()
1635 FT_Angle theta1, phi1, theta2, phi2, rotate, alpha0 = 0; in FT_Stroker_CubicTo() local
1641 theta1 = FT_Angle_Diff( angle_in, angle_mid ) / 2; in FT_Stroker_CubicTo()
1645 length1 = FT_DivFix( stroker->radius, FT_Cos( theta1 ) ); in FT_Stroker_CubicTo()
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| /third_party/flutter/skia/third_party/externals/freetype/src/base/ |
| D | ftstroke.c | 205 FT_Angle theta1, theta2; in ft_cubic_is_small_enough() local
286 theta1 = ft_pos_abs( FT_Angle_Diff( *angle_in, *angle_mid ) ); in ft_cubic_is_small_enough()
289 return FT_BOOL( theta1 < FT_SMALL_CUBIC_THRESHOLD && in ft_cubic_is_small_enough()
1667 FT_Angle theta1, phi1, theta2, phi2, rotate, alpha0 = 0; in FT_Stroker_CubicTo() local
1673 theta1 = FT_Angle_Diff( angle_in, angle_mid ) / 2; in FT_Stroker_CubicTo()
1677 length1 = FT_DivFix( stroker->radius, FT_Cos( theta1 ) ); in FT_Stroker_CubicTo()
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| /third_party/freetype/src/base/ |
| D | ftstroke.c | 204 FT_Angle theta1, theta2; in ft_cubic_is_small_enough() local
285 theta1 = ft_pos_abs( FT_Angle_Diff( *angle_in, *angle_mid ) ); in ft_cubic_is_small_enough()
288 return FT_BOOL( theta1 < FT_SMALL_CUBIC_THRESHOLD && in ft_cubic_is_small_enough()
1633 FT_Angle theta1, phi1, theta2, phi2, rotate, alpha0 = 0; in FT_Stroker_CubicTo() local
1639 theta1 = FT_Angle_Diff( angle_in, angle_mid ) / 2; in FT_Stroker_CubicTo()
1643 length1 = FT_DivFix( stroker->radius, FT_Cos( theta1 ) ); in FT_Stroker_CubicTo()
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| /third_party/skia/src/core/ |
| D | SkPathBuilder.cpp | 515 SkScalar theta1 = SkScalarATan2(unitPts[0].fY, unitPts[0].fX); in arcTo() local
517 SkScalar thetaArc = theta2 - theta1; in arcTo()
542 SkScalar startTheta = theta1; in arcTo()
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| D | SkPath.cpp | 1225 SkScalar theta1 = SkScalarATan2(unitPts[0].fY, unitPts[0].fX); in arcTo() local
1227 SkScalar thetaArc = theta2 - theta1; in arcTo()
1252 SkScalar startTheta = theta1; in arcTo()
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| /third_party/openGLES/extensions/NV/ |
| D | NV_path_rendering.txt | 1621 … theta1,dtheta,t) ncp.y = c[4] npep.y = c[4]
1623 theta1,dtheta,t)
1625 …_SMALL_CCW_ARC_TO_NV theta1,dtheta,t) ncp.y = c[4] npep.y = cp.…
1627 theta1,dtheta,t)
1629 … theta1,dtheta,t) ncp.y = c[4] npep.y = c[4]
1631 theta1,dtheta,t)
1633 …_SMALL_CW_ARC_TO_NV theta1,dtheta,t) ncp.y = c[4] npep.y = cp.…
1635 theta1,dtheta,t)
1637 … theta1,dtheta,t) ncp.y = c[4] npep.y = c[4]
1639 theta1,dtheta,t)
[all …]
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| /third_party/skia/third_party/externals/opengl-registry/extensions/NV/ |
| D | NV_path_rendering.txt | 1621 … theta1,dtheta,t) ncp.y = c[4] npep.y = c[4]
1623 theta1,dtheta,t)
1625 …_SMALL_CCW_ARC_TO_NV theta1,dtheta,t) ncp.y = c[4] npep.y = cp.…
1627 theta1,dtheta,t)
1629 … theta1,dtheta,t) ncp.y = c[4] npep.y = c[4]
1631 theta1,dtheta,t)
1633 …_SMALL_CW_ARC_TO_NV theta1,dtheta,t) ncp.y = c[4] npep.y = cp.…
1635 theta1,dtheta,t)
1637 … theta1,dtheta,t) ncp.y = c[4] npep.y = c[4]
1639 theta1,dtheta,t)
[all …]
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| /third_party/flutter/skia/src/core/ |
| D | SkPath.cpp | 1487 SkScalar theta1 = SkScalarATan2(unitPts[0].fY, unitPts[0].fX); in arcTo() local
1489 SkScalar thetaArc = theta2 - theta1; in arcTo()
1514 SkScalar startTheta = theta1; in arcTo()
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