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dc30f461 1/* Single-precision floating point e^x.
f7a9f785 2 Copyright (C) 1997-2016 Free Software Foundation, Inc.
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3 This file is part of the GNU C Library.
4 Contributed by Geoffrey Keating <geoffk@ozemail.com.au>
f7eac6eb 5
dc30f461 6 The GNU C Library is free software; you can redistribute it and/or
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7 modify it under the terms of the GNU Lesser General Public
8 License as published by the Free Software Foundation; either
9 version 2.1 of the License, or (at your option) any later version.
f7eac6eb 10
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11 The GNU C Library is distributed in the hope that it will be useful,
12 but WITHOUT ANY WARRANTY; without even the implied warranty of
13 MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the GNU
41bdb6e2 14 Lesser General Public License for more details.
f7eac6eb 15
41bdb6e2 16 You should have received a copy of the GNU Lesser General Public
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17 License along with the GNU C Library; if not, see
18 <http://www.gnu.org/licenses/>. */
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19
20/* How this works:
21
22 The input value, x, is written as
23
24 x = n * ln(2) + t/512 + delta[t] + x;
25
26 where:
27 - n is an integer, 127 >= n >= -150;
28 - t is an integer, 177 >= t >= -177
29 - delta is based on a table entry, delta[t] < 2^-28
30 - x is whatever is left, |x| < 2^-10
31
32 Then e^x is approximated as
33
34 e^x = 2^n ( e^(t/512 + delta[t])
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35 + ( e^(t/512 + delta[t])
36 * ( p(x + delta[t] + n * ln(2)) - delta ) ) )
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37
38 where
39 - p(x) is a polynomial approximating e(x)-1;
40 - e^(t/512 + delta[t]) is obtained from a table.
41
42 The table used is the same one as for the double precision version;
43 since we have the table, we might as well use it.
44
45 It turns out to be faster to do calculations in double precision than
46 to perform an 'accurate table method' expf, because of the range reduction
47 overhead (compare exp2f).
48 */
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49#include <float.h>
50#include <ieee754.h>
51#include <math.h>
52#include <fenv.h>
53#include <inttypes.h>
54#include <math_private.h>
55
56extern const float __exp_deltatable[178];
57extern const double __exp_atable[355] /* __attribute__((mode(DF))) */;
58
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59static const float TWOM100 = 7.88860905e-31;
60static const float TWO127 = 1.7014118346e+38;
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61
62float
63__ieee754_expf (float x)
f7eac6eb 64{
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65 static const float himark = 88.72283935546875;
66 static const float lomark = -103.972084045410;
67 /* Check for usual case. */
68 if (isless (x, himark) && isgreater (x, lomark))
69 {
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70 static const float THREEp42 = 13194139533312.0;
71 static const float THREEp22 = 12582912.0;
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72 /* 1/ln(2). */
73#undef M_1_LN2
74 static const float M_1_LN2 = 1.44269502163f;
75 /* ln(2) */
76#undef M_LN2
77 static const double M_LN2 = .6931471805599452862;
78
79 int tval;
80 double x22, t, result, dx;
81 float n, delta;
82 union ieee754_double ex2_u;
dc30f461 83
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84 {
85 SET_RESTORE_ROUND_NOEXF (FE_TONEAREST);
f7eac6eb 86
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87 /* Calculate n. */
88 n = x * M_1_LN2 + THREEp22;
89 n -= THREEp22;
90 dx = x - n*M_LN2;
dc30f461 91
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92 /* Calculate t/512. */
93 t = dx + THREEp42;
94 t -= THREEp42;
95 dx -= t;
dc30f461 96
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97 /* Compute tval = t. */
98 tval = (int) (t * 512.0);
66000494 99
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100 if (t >= 0)
101 delta = - __exp_deltatable[tval];
102 else
103 delta = __exp_deltatable[-tval];
dc30f461 104
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105 /* Compute ex2 = 2^n e^(t/512+delta[t]). */
106 ex2_u.d = __exp_atable[tval+177];
107 ex2_u.ieee.exponent += (int) n;
dc30f461 108
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109 /* Approximate e^(dx+delta) - 1, using a second-degree polynomial,
110 with maximum error in [-2^-10-2^-28,2^-10+2^-28]
111 less than 5e-11. */
112 x22 = (0.5000000496709180453 * dx + 1.0000001192102037084) * dx + delta;
113 }
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114
115 /* Return result. */
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116 result = x22 * ex2_u.d + ex2_u.d;
117 return (float) result;
118 }
119 /* Exceptional cases: */
120 else if (isless (x, himark))
121 {
d81f90cc 122 if (isinf (x))
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123 /* e^-inf == 0, with no error. */
124 return 0;
125 else
126 /* Underflow */
127 return TWOM100 * TWOM100;
128 }
129 else
130 /* Return x, if x is a NaN or Inf; or overflow, otherwise. */
131 return TWO127*x;
f7eac6eb 132}
bcf01e6d 133strong_alias (__ieee754_expf, __expf_finite)