/* Math module -- standard C math library functions, pi and e */ /* Here are some comments from Tim Peters, extracted from the discussion attached to http://bugs.python.org/issue1640. They describe the general aims of the math module with respect to special values, IEEE-754 floating-point exceptions, and Python exceptions. These are the "spirit of 754" rules: 1. If the mathematical result is a real number, but of magnitude too large to approximate by a machine float, overflow is signaled and the result is an infinity (with the appropriate sign). 2. If the mathematical result is a real number, but of magnitude too small to approximate by a machine float, underflow is signaled and the result is a zero (with the appropriate sign). 3. At a singularity (a value x such that the limit of f(y) as y approaches x exists and is an infinity), "divide by zero" is signaled and the result is an infinity (with the appropriate sign). This is complicated a little by that the left-side and right-side limits may not be the same; e.g., 1/x approaches +inf or -inf as x approaches 0 from the positive or negative directions. In that specific case, the sign of the zero determines the result of 1/0. 4. At a point where a function has no defined result in the extended reals (i.e., the reals plus an infinity or two), invalid operation is signaled and a NaN is returned. And these are what Python has historically /tried/ to do (but not always successfully, as platform libm behavior varies a lot): For #1, raise OverflowError. For #2, return a zero (with the appropriate sign if that happens by accident ;-)). For #3 and #4, raise ValueError. It may have made sense to raise Python's ZeroDivisionError in #3, but historically that's only been raised for division by zero and mod by zero. */ /* In general, on an IEEE-754 platform the aim is to follow the C99 standard, including Annex 'F', whenever possible. Where the standard recommends raising the 'divide-by-zero' or 'invalid' floating-point exceptions, Python should raise a ValueError. Where the standard recommends raising 'overflow', Python should raise an OverflowError. In all other circumstances a value should be returned. */ #include "Python.h" #include "_math.h" #include "longintrepr.h" /* just for SHIFT */ #ifdef _OSF_SOURCE /* OSF1 5.1 doesn't make this available with XOPEN_SOURCE_EXTENDED defined */ extern double copysign(double, double); #endif /* sin(pi*x), giving accurate results for all finite x (especially x integral or close to an integer). This is here for use in the reflection formula for the gamma function. It conforms to IEEE 754-2008 for finite arguments, but not for infinities or nans. */ static const double pi = 3.141592653589793238462643383279502884197; static const double sqrtpi = 1.772453850905516027298167483341145182798; static double sinpi(double x) { double y, r; int n; /* this function should only ever be called for finite arguments */ assert(Py_IS_FINITE(x)); y = fmod(fabs(x), 2.0); n = (int)round(2.0*y); assert(0 <= n && n <= 4); switch (n) { case 0: r = sin(pi*y); break; case 1: r = cos(pi*(y-0.5)); break; case 2: /* N.B. -sin(pi*(y-1.0)) is *not* equivalent: it would give -0.0 instead of 0.0 when y == 1.0. */ r = sin(pi*(1.0-y)); break; case 3: r = -cos(pi*(y-1.5)); break; case 4: r = sin(pi*(y-2.0)); break; default: assert(0); /* should never get here */ r = -1.23e200; /* silence gcc warning */ } return copysign(1.0, x)*r; } /* Implementation of the real gamma function. In extensive but non-exhaustive random tests, this function proved accurate to within <= 10 ulps across the entire float domain. Note that accuracy may depend on the quality of the system math functions, the pow function in particular. Special cases follow C99 annex F. The parameters and method are tailored to platforms whose double format is the IEEE 754 binary64 format. Method: for x > 0.0 we use the Lanczos approximation with parameters N=13 and g=6.024680040776729583740234375; these parameters are amongst those used by the Boost library. Following Boost (again), we re-express the Lanczos sum as a rational function, and compute it that way. The coefficients below were computed independently using MPFR, and have been double-checked against the coefficients in the Boost source code. For x < 0.0 we use the reflection formula. There's one minor tweak that deserves explanation: Lanczos' formula for Gamma(x) involves computing pow(x+g-0.5, x-0.5) / exp(x+g-0.5). For many x values, x+g-0.5 can be represented exactly. However, in cases where it can't be represented exactly the small error in x+g-0.5 can be magnified significantly by the pow and exp calls, especially for large x. A cheap correction is to multiply by (1 + e*g/(x+g-0.5)), where e is the error involved in the computation of x+g-0.5 (that is, e = computed value of x+g-0.5 - exact value of x+g-0.5). Here's the proof: Correction factor ----------------- Write x+g-0.5 = y-e, where y is exactly representable as an IEEE 754 double, and e is tiny. Then: pow(x+g-0.5,x-0.5)/exp(x+g-0.5) = pow(y-e, x-0.5)/exp(y-e) = pow(y, x-0.5)/exp(y) * C, where the correction_factor C is given by C = pow(1-e/y, x-0.5) * exp(e) Since e is tiny, pow(1-e/y, x-0.5) ~ 1-(x-0.5)*e/y, and exp(x) ~ 1+e, so: C ~ (1-(x-0.5)*e/y) * (1+e) ~ 1 + e*(y-(x-0.5))/y But y-(x-0.5) = g+e, and g+e ~ g. So we get C ~ 1 + e*g/y, and pow(x+g-0.5,x-0.5)/exp(x+g-0.5) ~ pow(y, x-0.5)/exp(y) * (1 + e*g/y), Note that for accuracy, when computing r*C it's better to do r + e*g/y*r; than r * (1 + e*g/y); since the addition in the latter throws away most of the bits of information in e*g/y. */ #define LANCZOS_N 13 static const double lanczos_g = 6.024680040776729583740234375; static const double lanczos_g_minus_half = 5.524680040776729583740234375; static const double lanczos_num_coeffs[LANCZOS_N] = { 23531376880.410759688572007674451636754734846804940, 42919803642.649098768957899047001988850926355848959, 35711959237.355668049440185451547166705960488635843, 17921034426.037209699919755754458931112671403265390, 6039542586.3520280050642916443072979210699388420708, 1439720407.3117216736632230727949123939715485786772, 248874557.86205415651146038641322942321632125127801, 31426415.585400194380614231628318205362874684987640, 2876370.6289353724412254090516208496135991145378768, 186056.26539522349504029498971604569928220784236328, 8071.6720023658162106380029022722506138218516325024, 210.82427775157934587250973392071336271166969580291, 2.5066282746310002701649081771338373386264310793408 }; /* denominator is x*(x+1)*...*(x+LANCZOS_N-2) */ static const double lanczos_den_coeffs[LANCZOS_N] = { 0.0, 39916800.0, 120543840.0, 150917976.0, 105258076.0, 45995730.0, 13339535.0, 2637558.0, 357423.0, 32670.0, 1925.0, 66.0, 1.0}; /* gamma values for small positive integers, 1 though NGAMMA_INTEGRAL */ #define NGAMMA_INTEGRAL 23 static const double gamma_integral[NGAMMA_INTEGRAL] = { 1.0, 1.0, 2.0, 6.0, 24.0, 120.0, 720.0, 5040.0, 40320.0, 362880.0, 3628800.0, 39916800.0, 479001600.0, 6227020800.0, 87178291200.0, 1307674368000.0, 20922789888000.0, 355687428096000.0, 6402373705728000.0, 121645100408832000.0, 2432902008176640000.0, 51090942171709440000.0, 1124000727777607680000.0, }; /* Lanczos' sum L_g(x), for positive x */ static double lanczos_sum(double x) { double num = 0.0, den = 0.0; int i; assert(x > 0.0); /* evaluate the rational function lanczos_sum(x). For large x, the obvious algorithm risks overflow, so we instead rescale the denominator and numerator of the rational function by x**(1-LANCZOS_N) and treat this as a rational function in 1/x. This also reduces the error for larger x values. The choice of cutoff point (5.0 below) is somewhat arbitrary; in tests, smaller cutoff values than this resulted in lower accuracy. */ if (x < 5.0) { for (i = LANCZOS_N; --i >= 0; ) { num = num * x + lanczos_num_coeffs[i]; den = den * x + lanczos_den_coeffs[i]; } } else { for (i = 0; i < LANCZOS_N; i++) { num = num / x + lanczos_num_coeffs[i]; den = den / x + lanczos_den_coeffs[i]; } } return num/den; } static double m_tgamma(double x) { double absx, r, y, z, sqrtpow; /* special cases */ if (!Py_IS_FINITE(x)) { if (Py_IS_NAN(x) || x > 0.0) return x; /* tgamma(nan) = nan, tgamma(inf) = inf */ else { errno = EDOM; return Py_NAN; /* tgamma(-inf) = nan, invalid */ } } if (x == 0.0) { errno = EDOM; return 1.0/x; /* tgamma(+-0.0) = +-inf, divide-by-zero */ } /* integer arguments */ if (x == floor(x)) { if (x < 0.0) { errno = EDOM; /* tgamma(n) = nan, invalid for */ return Py_NAN; /* negative integers n */ } if (x <= NGAMMA_INTEGRAL) return gamma_integral[(int)x - 1]; } absx = fabs(x); /* tiny arguments: tgamma(x) ~ 1/x for x near 0 */ if (absx < 1e-20) { r = 1.0/x; if (Py_IS_INFINITY(r)) errno = ERANGE; return r; } /* large arguments: assuming IEEE 754 doubles, tgamma(x) overflows for x > 200, and underflows to +-0.0 for x < -200, not a negative integer. */ if (absx > 200.0) { if (x < 0.0) { return 0.0/sinpi(x); } else { errno = ERANGE; return Py_HUGE_VAL; } } y = absx + lanczos_g_minus_half; /* compute error in sum */ if (absx > lanczos_g_minus_half) { /* note: the correction can be foiled by an optimizing compiler that (incorrectly) thinks that an expression like a + b - a - b can be optimized to 0.0. This shouldn't happen in a standards-conforming compiler. */ double q = y - absx; z = q - lanczos_g_minus_half; } else { double q = y - lanczos_g_minus_half; z = q - absx; } z = z * lanczos_g / y; if (x < 0.0) { r = -pi / sinpi(absx) / absx * exp(y) / lanczos_sum(absx); r -= z * r; if (absx < 140.0) { r /= pow(y, absx - 0.5); } else { sqrtpow = pow(y, absx / 2.0 - 0.25); r /= sqrtpow; r /= sqrtpow; } } else { r = lanczos_sum(absx) / exp(y); r += z * r; if (absx < 140.0) { r *= pow(y, absx - 0.5); } else { sqrtpow = pow(y, absx / 2.0 - 0.25); r *= sqrtpow; r *= sqrtpow; } } if (Py_IS_INFINITY(r)) errno = ERANGE; return r; } /* lgamma: natural log of the absolute value of the Gamma function. For large arguments, Lanczos' formula works extremely well here. */ static double m_lgamma(double x) { double r, absx; /* special cases */ if (!Py_IS_FINITE(x)) { if (Py_IS_NAN(x)) return x; /* lgamma(nan) = nan */ else return Py_HUGE_VAL; /* lgamma(+-inf) = +inf */ } /* integer arguments */ if (x == floor(x) && x <= 2.0) { if (x <= 0.0) { errno = EDOM; /* lgamma(n) = inf, divide-by-zero for */ return Py_HUGE_VAL; /* integers n <= 0 */ } else { return 0.0; /* lgamma(1) = lgamma(2) = 0.0 */ } } absx = fabs(x); /* tiny arguments: lgamma(x) ~ -log(fabs(x)) for small x */ if (absx < 1e-20) return -log(absx); /* Lanczos' formula */ if (x > 0.0) { /* we could save a fraction of a ulp in accuracy by having a second set of numerator coefficients for lanczos_sum that absorbed the exp(-lanczos_g) term, and throwing out the lanczos_g subtraction below; it's probably not worth it. */ r = log(lanczos_sum(x)) - lanczos_g + (x-0.5)*(log(x+lanczos_g-0.5)-1); } else { r = log(pi) - log(fabs(sinpi(absx))) - log(absx) - (log(lanczos_sum(absx)) - lanczos_g + (absx-0.5)*(log(absx+lanczos_g-0.5)-1)); } if (Py_IS_INFINITY(r)) errno = ERANGE; return r; } /* Implementations of the error function erf(x) and the complementary error function erfc(x). Method: following 'Numerical Recipes' by Flannery, Press et. al. (2nd ed., Cambridge University Press), we use a series approximation for erf for small x, and a continued fraction approximation for erfc(x) for larger x; combined with the relations erf(-x) = -erf(x) and erfc(x) = 1.0 - erf(x), this gives us erf(x) and erfc(x) for all x. The series expansion used is: erf(x) = x*exp(-x*x)/sqrt(pi) * [ 2/1 + 4/3 x**2 + 8/15 x**4 + 16/105 x**6 + ...] The coefficient of x**(2k-2) here is 4**k*factorial(k)/factorial(2*k). This series converges well for smallish x, but slowly for larger x. The continued fraction expansion used is: erfc(x) = x*exp(-x*x)/sqrt(pi) * [1/(0.5 + x**2 -) 0.5/(2.5 + x**2 - ) 3.0/(4.5 + x**2 - ) 7.5/(6.5 + x**2 - ) ...] after the first term, the general term has the form: k*(k-0.5)/(2*k+0.5 + x**2 - ...). This expansion converges fast for larger x, but convergence becomes infinitely slow as x approaches 0.0. The (somewhat naive) continued fraction evaluation algorithm used below also risks overflow for large x; but for large x, erfc(x) == 0.0 to within machine precision. (For example, erfc(30.0) is approximately 2.56e-393). Parameters: use series expansion for abs(x) < ERF_SERIES_CUTOFF and continued fraction expansion for ERF_SERIES_CUTOFF <= abs(x) < ERFC_CONTFRAC_CUTOFF. ERFC_SERIES_TERMS and ERFC_CONTFRAC_TERMS are the numbers of terms to use for the relevant expansions. */ #define ERF_SERIES_CUTOFF 1.5 #define ERF_SERIES_TERMS 25 #define ERFC_CONTFRAC_CUTOFF 30.0 #define ERFC_CONTFRAC_TERMS 50 /* Error function, via power series. Given a finite float x, return an approximation to erf(x). Converges reasonably fast for small x. */ static double m_erf_series(double x) { double x2, acc, fk; int i; x2 = x * x; acc = 0.0; fk = (double)ERF_SERIES_TERMS + 0.5; for (i = 0; i < ERF_SERIES_TERMS; i++) { acc = 2.0 + x2 * acc / fk; fk -= 1.0; } return acc * x * exp(-x2) / sqrtpi; } /* Complementary error function, via continued fraction expansion. Given a positive float x, return an approximation to erfc(x). Converges reasonably fast for x large (say, x > 2.0), and should be safe from overflow if x and nterms are not too large. On an IEEE 754 machine, with x <= 30.0, we're safe up to nterms = 100. For x >= 30.0, erfc(x) is smaller than the smallest representable nonzero float. */ static double m_erfc_contfrac(double x) { double x2, a, da, p, p_last, q, q_last, b; int i; if (x >= ERFC_CONTFRAC_CUTOFF) return 0.0; x2 = x*x; a = 0.0; da = 0.5; p = 1.0; p_last = 0.0; q = da + x2; q_last = 1.0; for (i = 0; i < ERFC_CONTFRAC_TERMS; i++) { double temp; a += da; da += 2.0; b = da + x2; temp = p; p = b*p - a*p_last; p_last = temp; temp = q; q = b*q - a*q_last; q_last = temp; } return p / q * x * exp(-x2) / sqrtpi; } /* Error function erf(x), for general x */ static double m_erf(double x) { double absx, cf; if (Py_IS_NAN(x)) return x; absx = fabs(x); if (absx < ERF_SERIES_CUTOFF) return m_erf_series(x); else { cf = m_erfc_contfrac(absx); return x > 0.0 ? 1.0 - cf : cf - 1.0; } } /* Complementary error function erfc(x), for general x. */ static double m_erfc(double x) { double absx, cf; if (Py_IS_NAN(x)) return x; absx = fabs(x); if (absx < ERF_SERIES_CUTOFF) return 1.0 - m_erf_series(x); else { cf = m_erfc_contfrac(absx); return x > 0.0 ? cf : 2.0 - cf; } } /* wrapper for atan2 that deals directly with special cases before delegating to the platform libm for the remaining cases. This is necessary to get consistent behaviour across platforms. Windows, FreeBSD and alpha Tru64 are amongst platforms that don't always follow C99. */ static double m_atan2(double y, double x) { if (Py_IS_NAN(x) || Py_IS_NAN(y)) return Py_NAN; if (Py_IS_INFINITY(y)) { if (Py_IS_INFINITY(x)) { if (copysign(1., x) == 1.) /* atan2(+-inf, +inf) == +-pi/4 */ return copysign(0.25*Py_MATH_PI, y); else /* atan2(+-inf, -inf) == +-pi*3/4 */ return copysign(0.75*Py_MATH_PI, y); } /* atan2(+-inf, x) == +-pi/2 for finite x */ return copysign(0.5*Py_MATH_PI, y); } if (Py_IS_INFINITY(x) || y == 0.) { if (copysign(1., x) == 1.) /* atan2(+-y, +inf) = atan2(+-0, +x) = +-0. */ return copysign(0., y); else /* atan2(+-y, -inf) = atan2(+-0., -x) = +-pi. */ return copysign(Py_MATH_PI, y); } return atan2(y, x); } /* Various platforms (Solaris, OpenBSD) do nonstandard things for log(0), log(-ve), log(NaN). Here are wrappers for log and log10 that deal with special values directly, passing positive non-special values through to the system log/log10. */ static double m_log(double x) { if (Py_IS_FINITE(x)) { if (x > 0.0) return log(x); errno = EDOM; if (x == 0.0) return -Py_HUGE_VAL; /* log(0) = -inf */ else return Py_NAN; /* log(-ve) = nan */ } else if (Py_IS_NAN(x)) return x; /* log(nan) = nan */ else if (x > 0.0) return x; /* log(inf) = inf */ else { errno = EDOM; return Py_NAN; /* log(-inf) = nan */ } } static double m_log10(double x) { if (Py_IS_FINITE(x)) { if (x > 0.0) return log10(x); errno = EDOM; if (x == 0.0) return -Py_HUGE_VAL; /* log10(0) = -inf */ else return Py_NAN; /* log10(-ve) = nan */ } else if (Py_IS_NAN(x)) return x; /* log10(nan) = nan */ else if (x > 0.0) return x; /* log10(inf) = inf */ else { errno = EDOM; return Py_NAN; /* log10(-inf) = nan */ } } /* Call is_error when errno != 0, and where x is the result libm * returned. is_error will usually set up an exception and return * true (1), but may return false (0) without setting up an exception. */ static int is_error(double x) { int result = 1; /* presumption of guilt */ assert(errno); /* non-zero errno is a precondition for calling */ if (errno == EDOM) PyErr_SetString(PyExc_ValueError, "math domain error"); else if (errno == ERANGE) { /* ANSI C generally requires libm functions to set ERANGE * on overflow, but also generally *allows* them to set * ERANGE on underflow too. There's no consistency about * the latter across platforms. * Alas, C99 never requires that errno be set. * Here we suppress the underflow errors (libm functions * should return a zero on underflow, and +- HUGE_VAL on * overflow, so testing the result for zero suffices to * distinguish the cases). * * On some platforms (Ubuntu/ia64) it seems that errno can be * set to ERANGE for subnormal results that do *not* underflow * to zero. So to be safe, we'll ignore ERANGE whenever the * function result is less than one in absolute value. */ if (fabs(x) < 1.0) result = 0; else PyErr_SetString(PyExc_OverflowError, "math range error"); } else /* Unexpected math error */ PyErr_SetFromErrno(PyExc_ValueError); return result; } /* math_1 is used to wrap a libm function f that takes a double arguments and returns a double. The error reporting follows these rules, which are designed to do the right thing on C89/C99 platforms and IEEE 754/non IEEE 754 platforms. - a NaN result from non-NaN inputs causes ValueError to be raised - an infinite result from finite inputs causes OverflowError to be raised if can_overflow is 1, or raises ValueError if can_overflow is 0. - if the result is finite and errno == EDOM then ValueError is raised - if the result is finite and nonzero and errno == ERANGE then OverflowError is raised The last rule is used to catch overflow on platforms which follow C89 but for which HUGE_VAL is not an infinity. For the majority of one-argument functions these rules are enough to ensure that Python's functions behave as specified in 'Annex F' of the C99 standard, with the 'invalid' and 'divide-by-zero' floating-point exceptions mapping to Python's ValueError and the 'overflow' floating-point exception mapping to OverflowError. math_1 only works for functions that don't have singularities *and* the possibility of overflow; fortunately, that covers everything we care about right now. */ static PyObject * math_1_to_whatever(PyObject *arg, double (*func) (double), PyObject *(*from_double_func) (double), int can_overflow) { double x, r; x = PyFloat_AsDouble(arg); if (x == -1.0 && PyErr_Occurred()) return NULL; errno = 0; PyFPE_START_PROTECT("in math_1", return 0); r = (*func)(x); PyFPE_END_PROTECT(r); if (Py_IS_NAN(r) && !Py_IS_NAN(x)) { PyErr_SetString(PyExc_ValueError, "math domain error"); /* invalid arg */ return NULL; } if (Py_IS_INFINITY(r) && Py_IS_FINITE(x)) { if (can_overflow) PyErr_SetString(PyExc_OverflowError, "math range error"); /* overflow */ else PyErr_SetString(PyExc_ValueError, "math domain error"); /* singularity */ return NULL; } if (Py_IS_FINITE(r) && errno && is_error(r)) /* this branch unnecessary on most platforms */ return NULL; return (*from_double_func)(r); } /* variant of math_1, to be used when the function being wrapped is known to set errno properly (that is, errno = EDOM for invalid or divide-by-zero, errno = ERANGE for overflow). */ static PyObject * math_1a(PyObject *arg, double (*func) (double)) { double x, r; x = PyFloat_AsDouble(arg); if (x == -1.0 && PyErr_Occurred()) return NULL; errno = 0; PyFPE_START_PROTECT("in math_1a", return 0); r = (*func)(x); PyFPE_END_PROTECT(r); if (errno && is_error(r)) return NULL; return PyFloat_FromDouble(r); } /* math_2 is used to wrap a libm function f that takes two double arguments and returns a double. The error reporting follows these rules, which are designed to do the right thing on C89/C99 platforms and IEEE 754/non IEEE 754 platforms. - a NaN result from non-NaN inputs causes ValueError to be raised - an infinite result from finite inputs causes OverflowError to be raised. - if the result is finite and errno == EDOM then ValueError is raised - if the result is finite and nonzero and errno == ERANGE then OverflowError is raised The last rule is used to catch overflow on platforms which follow C89 but for which HUGE_VAL is not an infinity. For most two-argument functions (copysign, fmod, hypot, atan2) these rules are enough to ensure that Python's functions behave as specified in 'Annex F' of the C99 standard, with the 'invalid' and 'divide-by-zero' floating-point exceptions mapping to Python's ValueError and the 'overflow' floating-point exception mapping to OverflowError. */ static PyObject * math_1(PyObject *arg, double (*func) (double), int can_overflow) { return math_1_to_whatever(arg, func, PyFloat_FromDouble, can_overflow); } static PyObject * math_1_to_int(PyObject *arg, double (*func) (double), int can_overflow) { return math_1_to_whatever(arg, func, PyLong_FromDouble, can_overflow); } static PyObject * math_2(PyObject *args, double (*func) (double, double), char *funcname) { PyObject *ox, *oy; double x, y, r; if (! PyArg_UnpackTuple(args, funcname, 2, 2, &ox, &oy)) return NULL; x = PyFloat_AsDouble(ox); y = PyFloat_AsDouble(oy); if ((x == -1.0 || y == -1.0) && PyErr_Occurred()) return NULL; errno = 0; PyFPE_START_PROTECT("in math_2", return 0); r = (*func)(x, y); PyFPE_END_PROTECT(r); if (Py_IS_NAN(r)) { if (!Py_IS_NAN(x) && !Py_IS_NAN(y)) errno = EDOM; else errno = 0; } else if (Py_IS_INFINITY(r)) { if (Py_IS_FINITE(x) && Py_IS_FINITE(y)) errno = ERANGE; else errno = 0; } if (errno && is_error(r)) return NULL; else return PyFloat_FromDouble(r); } #define FUNC1(funcname, func, can_overflow, docstring) \ static PyObject * math_##funcname(PyObject *self, PyObject *args) { \ return math_1(args, func, can_overflow); \ }\ PyDoc_STRVAR(math_##funcname##_doc, docstring); #define FUNC1A(funcname, func, docstring) \ static PyObject * math_##funcname(PyObject *self, PyObject *args) { \ return math_1a(args, func); \ }\ PyDoc_STRVAR(math_##funcname##_doc, docstring); #define FUNC2(funcname, func, docstring) \ static PyObject * math_##funcname(PyObject *self, PyObject *args) { \ return math_2(args, func, #funcname); \ }\ PyDoc_STRVAR(math_##funcname##_doc, docstring); FUNC1(acos, acos, 0, "acos(x)\n\nReturn the arc cosine (measured in radians) of x.") FUNC1(acosh, m_acosh, 0, "acosh(x)\n\nReturn the hyperbolic arc cosine (measured in radians) of x.") FUNC1(asin, asin, 0, "asin(x)\n\nReturn the arc sine (measured in radians) of x.") FUNC1(asinh, m_asinh, 0, "asinh(x)\n\nReturn the hyperbolic arc sine (measured in radians) of x.") FUNC1(atan, atan, 0, "atan(x)\n\nReturn the arc tangent (measured in radians) of x.") FUNC2(atan2, m_atan2, "atan2(y, x)\n\nReturn the arc tangent (measured in radians) of y/x.\n" "Unlike atan(y/x), the signs of both x and y are considered.") FUNC1(atanh, m_atanh, 0, "atanh(x)\n\nReturn the hyperbolic arc tangent (measured in radians) of x.") static PyObject * math_ceil(PyObject *self, PyObject *number) { static PyObject *ceil_str = NULL; PyObject *method; if (ceil_str == NULL) { ceil_str = PyUnicode_InternFromString("__ceil__"); if (ceil_str == NULL) return NULL; } method = _PyType_Lookup(Py_TYPE(number), ceil_str); if (method == NULL) return math_1_to_int(number, ceil, 0); else return PyObject_CallFunction(method, "O", number); } PyDoc_STRVAR(math_ceil_doc, "ceil(x)\n\nReturn the ceiling of x as an int.\n" "This is the smallest integral value >= x."); FUNC2(copysign, copysign, "copysign(x, y)\n\nReturn x with the sign of y.") FUNC1(cos, cos, 0, "cos(x)\n\nReturn the cosine of x (measured in radians).") FUNC1(cosh, cosh, 1, "cosh(x)\n\nReturn the hyperbolic cosine of x.") FUNC1A(erf, m_erf, "erf(x)\n\nError function at x.") FUNC1A(erfc, m_erfc, "erfc(x)\n\nComplementary error function at x.") FUNC1(exp, exp, 1, "exp(x)\n\nReturn e raised to the power of x.") FUNC1(expm1, m_expm1, 1, "expm1(x)\n\nReturn exp(x)-1.\n" "This function avoids the loss of precision involved in the direct " "evaluation of exp(x)-1 for small x.") FUNC1(fabs, fabs, 0, "fabs(x)\n\nReturn the absolute value of the float x.") static PyObject * math_floor(PyObject *self, PyObject *number) { static PyObject *floor_str = NULL; PyObject *method; if (floor_str == NULL) { floor_str = PyUnicode_InternFromString("__floor__"); if (floor_str == NULL) return NULL; } method = _PyType_Lookup(Py_TYPE(number), floor_str); if (method == NULL) return math_1_to_int(number, floor, 0); else return PyObject_CallFunction(method, "O", number); } PyDoc_STRVAR(math_floor_doc, "floor(x)\n\nReturn the floor of x as an int.\n" "This is the largest integral value <= x."); FUNC1A(gamma, m_tgamma, "gamma(x)\n\nGamma function at x.") FUNC1A(lgamma, m_lgamma, "lgamma(x)\n\nNatural logarithm of absolute value of Gamma function at x.") FUNC1(log1p, m_log1p, 1, "log1p(x)\n\nReturn the natural logarithm of 1+x (base e).\n" "The result is computed in a way which is accurate for x near zero.") FUNC1(sin, sin, 0, "sin(x)\n\nReturn the sine of x (measured in radians).") FUNC1(sinh, sinh, 1, "sinh(x)\n\nReturn the hyperbolic sine of x.") FUNC1(sqrt, sqrt, 0, "sqrt(x)\n\nReturn the square root of x.") FUNC1(tan, tan, 0, "tan(x)\n\nReturn the tangent of x (measured in radians).") FUNC1(tanh, tanh, 0, "tanh(x)\n\nReturn the hyperbolic tangent of x.") /* Precision summation function as msum() by Raymond Hettinger in , enhanced with the exact partials sum and roundoff from Mark Dickinson's post at . See those links for more details, proofs and other references. Note 1: IEEE 754R floating point semantics are assumed, but the current implementation does not re-establish special value semantics across iterations (i.e. handling -Inf + Inf). Note 2: No provision is made for intermediate overflow handling; therefore, sum([1e+308, 1e-308, 1e+308]) returns 1e+308 while sum([1e+308, 1e+308, 1e-308]) raises an OverflowError due to the overflow of the first partial sum. Note 3: The intermediate values lo, yr, and hi are declared volatile so aggressive compilers won't algebraically reduce lo to always be exactly 0.0. Also, the volatile declaration forces the values to be stored in memory as regular doubles instead of extended long precision (80-bit) values. This prevents double rounding because any addition or subtraction of two doubles can be resolved exactly into double-sized hi and lo values. As long as the hi value gets forced into a double before yr and lo are computed, the extra bits in downstream extended precision operations (x87 for example) will be exactly zero and therefore can be losslessly stored back into a double, thereby preventing double rounding. Note 4: A similar implementation is in Modules/cmathmodule.c. Be sure to update both when making changes. Note 5: The signature of math.fsum() differs from __builtin__.sum() because the start argument doesn't make sense in the context of accurate summation. Since the partials table is collapsed before returning a result, sum(seq2, start=sum(seq1)) may not equal the accurate result returned by sum(itertools.chain(seq1, seq2)). */ #define NUM_PARTIALS 32 /* initial partials array size, on stack */ /* Extend the partials array p[] by doubling its size. */ static int /* non-zero on error */ _fsum_realloc(double **p_ptr, Py_ssize_t n, double *ps, Py_ssize_t *m_ptr) { void *v = NULL; Py_ssize_t m = *m_ptr; m += m; /* double */ if (n < m && m < (PY_SSIZE_T_MAX / sizeof(double))) { double *p = *p_ptr; if (p == ps) { v = PyMem_Malloc(sizeof(double) * m); if (v != NULL) memcpy(v, ps, sizeof(double) * n); } else v = PyMem_Realloc(p, sizeof(double) * m); } if (v == NULL) { /* size overflow or no memory */ PyErr_SetString(PyExc_MemoryError, "math.fsum partials"); return 1; } *p_ptr = (double*) v; *m_ptr = m; return 0; } /* Full precision summation of a sequence of floats. def msum(iterable): partials = [] # sorted, non-overlapping partial sums for x in iterable: i = 0 for y in partials: if abs(x) < abs(y): x, y = y, x hi = x + y lo = y - (hi - x) if lo: partials[i] = lo i += 1 x = hi partials[i:] = [x] return sum_exact(partials) Rounded x+y stored in hi with the roundoff stored in lo. Together hi+lo are exactly equal to x+y. The inner loop applies hi/lo summation to each partial so that the list of partial sums remains exact. Sum_exact() adds the partial sums exactly and correctly rounds the final result (using the round-half-to-even rule). The items in partials remain non-zero, non-special, non-overlapping and strictly increasing in magnitude, but possibly not all having the same sign. Depends on IEEE 754 arithmetic guarantees and half-even rounding. */ static PyObject* math_fsum(PyObject *self, PyObject *seq) { PyObject *item, *iter, *sum = NULL; Py_ssize_t i, j, n = 0, m = NUM_PARTIALS; double x, y, t, ps[NUM_PARTIALS], *p = ps; double xsave, special_sum = 0.0, inf_sum = 0.0; volatile double hi, yr, lo; iter = PyObject_GetIter(seq); if (iter == NULL) return NULL; PyFPE_START_PROTECT("fsum", Py_DECREF(iter); return NULL) for(;;) { /* for x in iterable */ assert(0 <= n && n <= m); assert((m == NUM_PARTIALS && p == ps) || (m > NUM_PARTIALS && p != NULL)); item = PyIter_Next(iter); if (item == NULL) { if (PyErr_Occurred()) goto _fsum_error; break; } x = PyFloat_AsDouble(item); Py_DECREF(item); if (PyErr_Occurred()) goto _fsum_error; xsave = x; for (i = j = 0; j < n; j++) { /* for y in partials */ y = p[j]; if (fabs(x) < fabs(y)) { t = x; x = y; y = t; } hi = x + y; yr = hi - x; lo = y - yr; if (lo != 0.0) p[i++] = lo; x = hi; } n = i; /* ps[i:] = [x] */ if (x != 0.0) { if (! Py_IS_FINITE(x)) { /* a nonfinite x could arise either as a result of intermediate overflow, or as a result of a nan or inf in the summands */ if (Py_IS_FINITE(xsave)) { PyErr_SetString(PyExc_OverflowError, "intermediate overflow in fsum"); goto _fsum_error; } if (Py_IS_INFINITY(xsave)) inf_sum += xsave; special_sum += xsave; /* reset partials */ n = 0; } else if (n >= m && _fsum_realloc(&p, n, ps, &m)) goto _fsum_error; else p[n++] = x; } } if (special_sum != 0.0) { if (Py_IS_NAN(inf_sum)) PyErr_SetString(PyExc_ValueError, "-inf + inf in fsum"); else sum = PyFloat_FromDouble(special_sum); goto _fsum_error; } hi = 0.0; if (n > 0) { hi = p[--n]; /* sum_exact(ps, hi) from the top, stop when the sum becomes inexact. */ while (n > 0) { x = hi; y = p[--n]; assert(fabs(y) < fabs(x)); hi = x + y; yr = hi - x; lo = y - yr; if (lo != 0.0) break; } /* Make half-even rounding work across multiple partials. Needed so that sum([1e-16, 1, 1e16]) will round-up the last digit to two instead of down to zero (the 1e-16 makes the 1 slightly closer to two). With a potential 1 ULP rounding error fixed-up, math.fsum() can guarantee commutativity. */ if (n > 0 && ((lo < 0.0 && p[n-1] < 0.0) || (lo > 0.0 && p[n-1] > 0.0))) { y = lo * 2.0; x = hi + y; yr = x - hi; if (y == yr) hi = x; } } sum = PyFloat_FromDouble(hi); _fsum_error: PyFPE_END_PROTECT(hi) Py_DECREF(iter); if (p != ps) PyMem_Free(p); return sum; } #undef NUM_PARTIALS PyDoc_STRVAR(math_fsum_doc, "fsum(iterable)\n\n\ Return an accurate floating point sum of values in the iterable.\n\ Assumes IEEE-754 floating point arithmetic."); static PyObject * math_factorial(PyObject *self, PyObject *arg) { long i, x; PyObject *result, *iobj, *newresult; if (PyFloat_Check(arg)) { PyObject *lx; double dx = PyFloat_AS_DOUBLE((PyFloatObject *)arg); if (!(Py_IS_FINITE(dx) && dx == floor(dx))) { PyErr_SetString(PyExc_ValueError, "factorial() only accepts integral values"); return NULL; } lx = PyLong_FromDouble(dx); if (lx == NULL) return NULL; x = PyLong_AsLong(lx); Py_DECREF(lx); } else x = PyLong_AsLong(arg); if (x == -1 && PyErr_Occurred()) return NULL; if (x < 0) { PyErr_SetString(PyExc_ValueError, "factorial() not defined for negative values"); return NULL; } result = (PyObject *)PyLong_FromLong(1); if (result == NULL) return NULL; for (i=1 ; i<=x ; i++) { iobj = (PyObject *)PyLong_FromLong(i); if (iobj == NULL) goto error; newresult = PyNumber_Multiply(result, iobj); Py_DECREF(iobj); if (newresult == NULL) goto error; Py_DECREF(result); result = newresult; } return result; error: Py_DECREF(result); return NULL; } PyDoc_STRVAR(math_factorial_doc, "factorial(x) -> Integral\n" "\n" "Find x!. Raise a ValueError if x is negative or non-integral."); static PyObject * math_trunc(PyObject *self, PyObject *number) { static PyObject *trunc_str = NULL; PyObject *trunc; if (Py_TYPE(number)->tp_dict == NULL) { if (PyType_Ready(Py_TYPE(number)) < 0) return NULL; } if (trunc_str == NULL) { trunc_str = PyUnicode_InternFromString("__trunc__"); if (trunc_str == NULL) return NULL; } trunc = _PyType_Lookup(Py_TYPE(number), trunc_str); if (trunc == NULL) { PyErr_Format(PyExc_TypeError, "type %.100s doesn't define __trunc__ method", Py_TYPE(number)->tp_name); return NULL; } return PyObject_CallFunctionObjArgs(trunc, number, NULL); } PyDoc_STRVAR(math_trunc_doc, "trunc(x:Real) -> Integral\n" "\n" "Truncates x to the nearest Integral toward 0. Uses the __trunc__ magic method."); static PyObject * math_frexp(PyObject *self, PyObject *arg) { int i; double x = PyFloat_AsDouble(arg); if (x == -1.0 && PyErr_Occurred()) return NULL; /* deal with special cases directly, to sidestep platform differences */ if (Py_IS_NAN(x) || Py_IS_INFINITY(x) || !x) { i = 0; } else { PyFPE_START_PROTECT("in math_frexp", return 0); x = frexp(x, &i); PyFPE_END_PROTECT(x); } return Py_BuildValue("(di)", x, i); } PyDoc_STRVAR(math_frexp_doc, "frexp(x)\n" "\n" "Return the mantissa and exponent of x, as pair (m, e).\n" "m is a float and e is an int, such that x = m * 2.**e.\n" "If x is 0, m and e are both 0. Else 0.5 <= abs(m) < 1.0."); static PyObject * math_ldexp(PyObject *self, PyObject *args) { double x, r; PyObject *oexp; long exp; if (! PyArg_ParseTuple(args, "dO:ldexp", &x, &oexp)) return NULL; if (PyLong_Check(oexp)) { /* on overflow, replace exponent with either LONG_MAX or LONG_MIN, depending on the sign. */ exp = PyLong_AsLong(oexp); if (exp == -1 && PyErr_Occurred()) { if (PyErr_ExceptionMatches(PyExc_OverflowError)) { if (Py_SIZE(oexp) < 0) { exp = LONG_MIN; } else { exp = LONG_MAX; } PyErr_Clear(); } else { /* propagate any unexpected exception */ return NULL; } } } else { PyErr_SetString(PyExc_TypeError, "Expected an int or long as second argument " "to ldexp."); return NULL; } if (x == 0. || !Py_IS_FINITE(x)) { /* NaNs, zeros and infinities are returned unchanged */ r = x; errno = 0; } else if (exp > INT_MAX) { /* overflow */ r = copysign(Py_HUGE_VAL, x); errno = ERANGE; } else if (exp < INT_MIN) { /* underflow to +-0 */ r = copysign(0., x); errno = 0; } else { errno = 0; PyFPE_START_PROTECT("in math_ldexp", return 0); r = ldexp(x, (int)exp); PyFPE_END_PROTECT(r); if (Py_IS_INFINITY(r)) errno = ERANGE; } if (errno && is_error(r)) return NULL; return PyFloat_FromDouble(r); } PyDoc_STRVAR(math_ldexp_doc, "ldexp(x, i)\n\n\ Return x * (2**i)."); static PyObject * math_modf(PyObject *self, PyObject *arg) { double y, x = PyFloat_AsDouble(arg); if (x == -1.0 && PyErr_Occurred()) return NULL; /* some platforms don't do the right thing for NaNs and infinities, so we take care of special cases directly. */ if (!Py_IS_FINITE(x)) { if (Py_IS_INFINITY(x)) return Py_BuildValue("(dd)", copysign(0., x), x); else if (Py_IS_NAN(x)) return Py_BuildValue("(dd)", x, x); } errno = 0; PyFPE_START_PROTECT("in math_modf", return 0); x = modf(x, &y); PyFPE_END_PROTECT(x); return Py_BuildValue("(dd)", x, y); } PyDoc_STRVAR(math_modf_doc, "modf(x)\n" "\n" "Return the fractional and integer parts of x. Both results carry the sign\n" "of x and are floats."); /* A decent logarithm is easy to compute even for huge longs, but libm can't do that by itself -- loghelper can. func is log or log10, and name is "log" or "log10". Note that overflow isn't possible: a long can contain no more than INT_MAX * SHIFT bits, so has value certainly less than 2**(2**64 * 2**16) == 2**2**80, and log2 of that is 2**80, which is small enough to fit in an IEEE single. log and log10 are even smaller. */ static PyObject* loghelper(PyObject* arg, double (*func)(double), char *funcname) { /* If it is long, do it ourselves. */ if (PyLong_Check(arg)) { double x; int e; x = _PyLong_AsScaledDouble(arg, &e); if (x <= 0.0) { PyErr_SetString(PyExc_ValueError, "math domain error"); return NULL; } /* Value is ~= x * 2**(e*PyLong_SHIFT), so the log ~= log(x) + log(2) * e * PyLong_SHIFT. CAUTION: e*PyLong_SHIFT may overflow using int arithmetic, so force use of double. */ x = func(x) + (e * (double)PyLong_SHIFT) * func(2.0); return PyFloat_FromDouble(x); } /* Else let libm handle it by itself. */ return math_1(arg, func, 0); } static PyObject * math_log(PyObject *self, PyObject *args) { PyObject *arg; PyObject *base = NULL; PyObject *num, *den; PyObject *ans; if (!PyArg_UnpackTuple(args, "log", 1, 2, &arg, &base)) return NULL; num = loghelper(arg, m_log, "log"); if (num == NULL || base == NULL) return num; den = loghelper(base, m_log, "log"); if (den == NULL) { Py_DECREF(num); return NULL; } ans = PyNumber_TrueDivide(num, den); Py_DECREF(num); Py_DECREF(den); return ans; } PyDoc_STRVAR(math_log_doc, "log(x[, base])\n\n\ Return the logarithm of x to the given base.\n\ If the base not specified, returns the natural logarithm (base e) of x."); static PyObject * math_log10(PyObject *self, PyObject *arg) { return loghelper(arg, m_log10, "log10"); } PyDoc_STRVAR(math_log10_doc, "log10(x)\n\nReturn the base 10 logarithm of x."); static PyObject * math_fmod(PyObject *self, PyObject *args) { PyObject *ox, *oy; double r, x, y; if (! PyArg_UnpackTuple(args, "fmod", 2, 2, &ox, &oy)) return NULL; x = PyFloat_AsDouble(ox); y = PyFloat_AsDouble(oy); if ((x == -1.0 || y == -1.0) && PyErr_Occurred()) return NULL; /* fmod(x, +/-Inf) returns x for finite x. */ if (Py_IS_INFINITY(y) && Py_IS_FINITE(x)) return PyFloat_FromDouble(x); errno = 0; PyFPE_START_PROTECT("in math_fmod", return 0); r = fmod(x, y); PyFPE_END_PROTECT(r); if (Py_IS_NAN(r)) { if (!Py_IS_NAN(x) && !Py_IS_NAN(y)) errno = EDOM; else errno = 0; } if (errno && is_error(r)) return NULL; else return PyFloat_FromDouble(r); } PyDoc_STRVAR(math_fmod_doc, "fmod(x, y)\n\nReturn fmod(x, y), according to platform C." " x % y may differ."); static PyObject * math_hypot(PyObject *self, PyObject *args) { PyObject *ox, *oy; double r, x, y; if (! PyArg_UnpackTuple(args, "hypot", 2, 2, &ox, &oy)) return NULL; x = PyFloat_AsDouble(ox); y = PyFloat_AsDouble(oy); if ((x == -1.0 || y == -1.0) && PyErr_Occurred()) return NULL; /* hypot(x, +/-Inf) returns Inf, even if x is a NaN. */ if (Py_IS_INFINITY(x)) return PyFloat_FromDouble(fabs(x)); if (Py_IS_INFINITY(y)) return PyFloat_FromDouble(fabs(y)); errno = 0; PyFPE_START_PROTECT("in math_hypot", return 0); r = hypot(x, y); PyFPE_END_PROTECT(r); if (Py_IS_NAN(r)) { if (!Py_IS_NAN(x) && !Py_IS_NAN(y)) errno = EDOM; else errno = 0; } else if (Py_IS_INFINITY(r)) { if (Py_IS_FINITE(x) && Py_IS_FINITE(y)) errno = ERANGE; else errno = 0; } if (errno && is_error(r)) return NULL; else return PyFloat_FromDouble(r); } PyDoc_STRVAR(math_hypot_doc, "hypot(x, y)\n\nReturn the Euclidean distance, sqrt(x*x + y*y)."); /* pow can't use math_2, but needs its own wrapper: the problem is that an infinite result can arise either as a result of overflow (in which case OverflowError should be raised) or as a result of e.g. 0.**-5. (for which ValueError needs to be raised.) */ static PyObject * math_pow(PyObject *self, PyObject *args) { PyObject *ox, *oy; double r, x, y; int odd_y; if (! PyArg_UnpackTuple(args, "pow", 2, 2, &ox, &oy)) return NULL; x = PyFloat_AsDouble(ox); y = PyFloat_AsDouble(oy); if ((x == -1.0 || y == -1.0) && PyErr_Occurred()) return NULL; /* deal directly with IEEE specials, to cope with problems on various platforms whose semantics don't exactly match C99 */ r = 0.; /* silence compiler warning */ if (!Py_IS_FINITE(x) || !Py_IS_FINITE(y)) { errno = 0; if (Py_IS_NAN(x)) r = y == 0. ? 1. : x; /* NaN**0 = 1 */ else if (Py_IS_NAN(y)) r = x == 1. ? 1. : y; /* 1**NaN = 1 */ else if (Py_IS_INFINITY(x)) { odd_y = Py_IS_FINITE(y) && fmod(fabs(y), 2.0) == 1.0; if (y > 0.) r = odd_y ? x : fabs(x); else if (y == 0.) r = 1.; else /* y < 0. */ r = odd_y ? copysign(0., x) : 0.; } else if (Py_IS_INFINITY(y)) { if (fabs(x) == 1.0) r = 1.; else if (y > 0. && fabs(x) > 1.0) r = y; else if (y < 0. && fabs(x) < 1.0) { r = -y; /* result is +inf */ if (x == 0.) /* 0**-inf: divide-by-zero */ errno = EDOM; } else r = 0.; } } else { /* let libm handle finite**finite */ errno = 0; PyFPE_START_PROTECT("in math_pow", return 0); r = pow(x, y); PyFPE_END_PROTECT(r); /* a NaN result should arise only from (-ve)**(finite non-integer); in this case we want to raise ValueError. */ if (!Py_IS_FINITE(r)) { if (Py_IS_NAN(r)) { errno = EDOM; } /* an infinite result here arises either from: (A) (+/-0.)**negative (-> divide-by-zero) (B) overflow of x**y with x and y finite */ else if (Py_IS_INFINITY(r)) { if (x == 0.) errno = EDOM; else errno = ERANGE; } } } if (errno && is_error(r)) return NULL; else return PyFloat_FromDouble(r); } PyDoc_STRVAR(math_pow_doc, "pow(x, y)\n\nReturn x**y (x to the power of y)."); static const double degToRad = Py_MATH_PI / 180.0; static const double radToDeg = 180.0 / Py_MATH_PI; static PyObject * math_degrees(PyObject *self, PyObject *arg) { double x = PyFloat_AsDouble(arg); if (x == -1.0 && PyErr_Occurred()) return NULL; return PyFloat_FromDouble(x * radToDeg); } PyDoc_STRVAR(math_degrees_doc, "degrees(x)\n\n\ Convert angle x from radians to degrees."); static PyObject * math_radians(PyObject *self, PyObject *arg) { double x = PyFloat_AsDouble(arg); if (x == -1.0 && PyErr_Occurred()) return NULL; return PyFloat_FromDouble(x * degToRad); } PyDoc_STRVAR(math_radians_doc, "radians(x)\n\n\ Convert angle x from degrees to radians."); static PyObject * math_isnan(PyObject *self, PyObject *arg) { double x = PyFloat_AsDouble(arg); if (x == -1.0 && PyErr_Occurred()) return NULL; return PyBool_FromLong((long)Py_IS_NAN(x)); } PyDoc_STRVAR(math_isnan_doc, "isnan(x) -> bool\n\n\ Check if float x is not a number (NaN)."); static PyObject * math_isinf(PyObject *self, PyObject *arg) { double x = PyFloat_AsDouble(arg); if (x == -1.0 && PyErr_Occurred()) return NULL; return PyBool_FromLong((long)Py_IS_INFINITY(x)); } PyDoc_STRVAR(math_isinf_doc, "isinf(x) -> bool\n\n\ Check if float x is infinite (positive or negative)."); static PyMethodDef math_methods[] = { {"acos", math_acos, METH_O, math_acos_doc}, {"acosh", math_acosh, METH_O, math_acosh_doc}, {"asin", math_asin, METH_O, math_asin_doc}, {"asinh", math_asinh, METH_O, math_asinh_doc}, {"atan", math_atan, METH_O, math_atan_doc}, {"atan2", math_atan2, METH_VARARGS, math_atan2_doc}, {"atanh", math_atanh, METH_O, math_atanh_doc}, {"ceil", math_ceil, METH_O, math_ceil_doc}, {"copysign", math_copysign, METH_VARARGS, math_copysign_doc}, {"cos", math_cos, METH_O, math_cos_doc}, {"cosh", math_cosh, METH_O, math_cosh_doc}, {"degrees", math_degrees, METH_O, math_degrees_doc}, {"erf", math_erf, METH_O, math_erf_doc}, {"erfc", math_erfc, METH_O, math_erfc_doc}, {"exp", math_exp, METH_O, math_exp_doc}, {"expm1", math_expm1, METH_O, math_expm1_doc}, {"fabs", math_fabs, METH_O, math_fabs_doc}, {"factorial", math_factorial, METH_O, math_factorial_doc}, {"floor", math_floor, METH_O, math_floor_doc}, {"fmod", math_fmod, METH_VARARGS, math_fmod_doc}, {"frexp", math_frexp, METH_O, math_frexp_doc}, {"fsum", math_fsum, METH_O, math_fsum_doc}, {"gamma", math_gamma, METH_O, math_gamma_doc}, {"hypot", math_hypot, METH_VARARGS, math_hypot_doc}, {"isinf", math_isinf, METH_O, math_isinf_doc}, {"isnan", math_isnan, METH_O, math_isnan_doc}, {"ldexp", math_ldexp, METH_VARARGS, math_ldexp_doc}, {"lgamma", math_lgamma, METH_O, math_lgamma_doc}, {"log", math_log, METH_VARARGS, math_log_doc}, {"log1p", math_log1p, METH_O, math_log1p_doc}, {"log10", math_log10, METH_O, math_log10_doc}, {"modf", math_modf, METH_O, math_modf_doc}, {"pow", math_pow, METH_VARARGS, math_pow_doc}, {"radians", math_radians, METH_O, math_radians_doc}, {"sin", math_sin, METH_O, math_sin_doc}, {"sinh", math_sinh, METH_O, math_sinh_doc}, {"sqrt", math_sqrt, METH_O, math_sqrt_doc}, {"tan", math_tan, METH_O, math_tan_doc}, {"tanh", math_tanh, METH_O, math_tanh_doc}, {"trunc", math_trunc, METH_O, math_trunc_doc}, {NULL, NULL} /* sentinel */ }; PyDoc_STRVAR(module_doc, "This module is always available. It provides access to the\n" "mathematical functions defined by the C standard."); static struct PyModuleDef mathmodule = { PyModuleDef_HEAD_INIT, "math", module_doc, -1, math_methods, NULL, NULL, NULL, NULL }; PyMODINIT_FUNC PyInit_math(void) { PyObject *m; m = PyModule_Create(&mathmodule); if (m == NULL) goto finally; PyModule_AddObject(m, "pi", PyFloat_FromDouble(Py_MATH_PI)); PyModule_AddObject(m, "e", PyFloat_FromDouble(Py_MATH_E)); finally: return m; }