| 1 | ######################################################################## |
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| 2 | # BigFloat for Tcl |
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| 3 | # Copyright (C) 2003-2005 ARNOLD Stephane |
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| 4 | # |
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| 5 | # BIGFLOAT LICENSE TERMS |
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| 6 | # |
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| 7 | # This software is copyrighted by Stephane ARNOLD, (stephanearnold <at> yahoo.fr). |
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| 8 | # The following terms apply to all files associated |
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| 9 | # with the software unless explicitly disclaimed in individual files. |
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| 10 | # |
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| 11 | # The authors hereby grant permission to use, copy, modify, distribute, |
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| 12 | # and license this software and its documentation for any purpose, provided |
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| 13 | # that existing copyright notices are retained in all copies and that this |
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| 14 | # notice is included verbatim in any distributions. No written agreement, |
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| 15 | # license, or royalty fee is required for any of the authorized uses. |
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| 16 | # Modifications to this software may be copyrighted by their authors |
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| 17 | # and need not follow the licensing terms described here, provided that |
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| 18 | # the new terms are clearly indicated on the first page of each file where |
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| 19 | # they apply. |
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| 20 | # |
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| 21 | # IN NO EVENT SHALL THE AUTHORS OR DISTRIBUTORS BE LIABLE TO ANY PARTY |
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| 22 | # FOR DIRECT, INDIRECT, SPECIAL, INCIDENTAL, OR CONSEQUENTIAL DAMAGES |
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| 23 | # ARISING OUT OF THE USE OF THIS SOFTWARE, ITS DOCUMENTATION, OR ANY |
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| 24 | # DERIVATIVES THEREOF, EVEN IF THE AUTHORS HAVE BEEN ADVISED OF THE |
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| 25 | # POSSIBILITY OF SUCH DAMAGE. |
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| 26 | # |
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| 27 | # THE AUTHORS AND DISTRIBUTORS SPECIFICALLY DISCLAIM ANY WARRANTIES, |
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| 28 | # INCLUDING, BUT NOT LIMITED TO, THE IMPLIED WARRANTIES OF MERCHANTABILITY, |
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| 29 | # FITNESS FOR A PARTICULAR PURPOSE, AND NON-INFRINGEMENT. THIS SOFTWARE |
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| 30 | # IS PROVIDED ON AN "AS IS" BASIS, AND THE AUTHORS AND DISTRIBUTORS HAVE |
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| 31 | # NO OBLIGATION TO PROVIDE MAINTENANCE, SUPPORT, UPDATES, ENHANCEMENTS, OR |
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| 32 | # MODIFICATIONS. |
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| 33 | # |
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| 34 | # GOVERNMENT USE: If you are acquiring this software on behalf of the |
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| 35 | # U.S. government, the Government shall have only "Restricted Rights" |
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| 36 | # in the software and related documentation as defined in the Federal |
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| 37 | # Acquisition Regulations (FARs) in Clause 52.227.19 (c) (2). If you |
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| 38 | # are acquiring the software on behalf of the Department of Defense, the |
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| 39 | # software shall be classified as "Commercial Computer Software" and the |
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| 40 | # Government shall have only "Restricted Rights" as defined in Clause |
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| 41 | # 252.227-7013 (c) (1) of DFARs. Notwithstanding the foregoing, the |
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| 42 | # authors grant the U.S. Government and others acting in its behalf |
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| 43 | # permission to use and distribute the software in accordance with the |
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| 44 | # terms specified in this license. |
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| 45 | # |
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| 46 | ######################################################################## |
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| 47 | |
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| 48 | package require Tcl 8.4 |
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| 49 | package require math::bignum |
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| 50 | |
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| 51 | # this line helps when I want to source this file again and again |
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| 52 | catch {namespace delete ::math::bigfloat} |
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| 53 | |
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| 54 | # private namespace |
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| 55 | # this software works only with Tcl v8.4 and higher |
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| 56 | # it is using the package math::bignum |
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| 57 | namespace eval ::math::bigfloat { |
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| 58 | # cached constants |
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| 59 | # ln(2) with arbitrary precision |
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| 60 | variable Log2 |
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| 61 | # Pi with arb. precision |
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| 62 | variable Pi |
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| 63 | variable _pi0 |
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| 64 | # some constants (bignums) : {0 1 2 3 4 5 10} |
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| 65 | variable zero |
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| 66 | set zero [::math::bignum::fromstr 0] |
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| 67 | variable one |
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| 68 | set one [::math::bignum::fromstr 1] |
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| 69 | variable two |
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| 70 | set two [::math::bignum::fromstr 2] |
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| 71 | variable three |
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| 72 | set three [::math::bignum::fromstr 3] |
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| 73 | variable four |
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| 74 | set four [::math::bignum::fromstr 4] |
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| 75 | variable five |
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| 76 | set five [::math::bignum::fromstr 5] |
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| 77 | variable ten |
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| 78 | set ten [::math::bignum::fromstr 10] |
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| 79 | } |
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| 80 | |
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| 81 | |
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| 82 | |
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| 83 | |
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| 84 | ################################################################################ |
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| 85 | # procedures that handle floating-point numbers |
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| 86 | # these procedures are sorted by name (after eventually removing the underscores) |
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| 87 | # |
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| 88 | # BigFloats are internally represented as a list : |
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| 89 | # {"F" Mantissa Exponent Delta} where "F" is a character which determins |
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| 90 | # the datatype, Mantissa and Delta are two Big integers and Exponent a raw integer. |
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| 91 | # |
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| 92 | # The BigFloat value equals to (Mantissa +/- Delta)*2^Exponent |
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| 93 | # So the internal representation is binary, but trying to get as close as possible to |
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| 94 | # the decimal one. |
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| 95 | # When calling fromstr, the Delta parameter is set to the value of the last decimal digit. |
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| 96 | # Example : 1.50 belongs to [1.49,1.51], but internally Delta is probably not equal to 1, |
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| 97 | # because of the binary representation. |
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| 98 | # |
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| 99 | # So Mantissa and Delta are not limited in size, but in practice Delta is kept under |
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| 100 | # 2^32 by the 'normalize' procedure, to avoid a never-ended growth of memory used. |
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| 101 | # Indeed, when you perform some computations, the Delta parameter (which represent |
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| 102 | # the uncertainty on the value of the Mantissa) may increase. |
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| 103 | # Exponent, as a classic integer, is limited to the interval [-2147483648,2147483647] |
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| 104 | |
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| 105 | # Retrieving the parameters of a BigFloat is often done with that command : |
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| 106 | # foreach {dummy int exp delta} $bigfloat {break} |
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| 107 | # (dummy is not used, it is just used to get the "F" marker). |
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| 108 | # The isInt, isFloat, checkNumber and checkFloat procedures are used |
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| 109 | # to check data types |
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| 110 | # |
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| 111 | # Taylor development are often used to compute the analysis functions (like exp(),log()...) |
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| 112 | # To learn how it is done in practice, take a look at ::math::bigfloat::_asin |
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| 113 | # While doing computation on Mantissas, we do not care about the last digit, |
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| 114 | # because if we compute wisely Deltas, the digits that remain will be exact. |
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| 115 | ################################################################################ |
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| 116 | |
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| 117 | |
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| 118 | ################################################################################ |
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| 119 | # returns the absolute value |
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| 120 | ################################################################################ |
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| 121 | proc ::math::bigfloat::abs {number} { |
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| 122 | checkNumber number |
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| 123 | if {[isInt $number]} { |
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| 124 | # set sign to positive for a BigInt |
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| 125 | return [::math::bignum::abs $number] |
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| 126 | } |
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| 127 | # set sign to positive for a BigFloat into the Mantissa (index 1) |
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| 128 | lset number 1 [::math::bignum::abs [lindex $number 1]] |
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| 129 | return $number |
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| 130 | } |
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| 131 | |
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| 132 | |
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| 133 | ################################################################################ |
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| 134 | # arccosinus of a BigFloat |
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| 135 | ################################################################################ |
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| 136 | proc ::math::bigfloat::acos {x} { |
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| 137 | # handy proc for checking datatype |
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| 138 | checkFloat x |
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| 139 | foreach {dummy entier exp delta} $x {break} |
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| 140 | set precision [expr {($exp<0)?(-$exp):1}] |
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| 141 | # acos(0.0)=Pi/2 |
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| 142 | # 26/07/2005 : changed precision from decimal to binary |
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| 143 | # with the second parameter of pi command |
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| 144 | set piOverTwo [floatRShift [pi $precision 1]] |
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| 145 | if {[iszero $x]} { |
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| 146 | # $x is too close to zero -> acos(0)=PI/2 |
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| 147 | return $piOverTwo |
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| 148 | } |
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| 149 | # acos(-x)= Pi/2 + asin(x) |
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| 150 | if {[::math::bignum::sign $entier]} { |
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| 151 | return [add $piOverTwo [asin [abs $x]]] |
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| 152 | } |
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| 153 | # we always use _asin to compute the result |
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| 154 | # but as it is a Taylor development, the value given to [_asin] |
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| 155 | # has to be a bit smaller than 1 ; by using that trick : acos(x)=asin(sqrt(1-x^2)) |
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| 156 | # we can limit the entry of the Taylor development below 1/sqrt(2) |
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| 157 | if {[compare $x [fromstr 0.7071]]>0} { |
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| 158 | # x > sqrt(2)/2 : trying to make _asin converge quickly |
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| 159 | # creating 0 and 1 with the same precision as the entry |
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| 160 | variable one |
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| 161 | variable zero |
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| 162 | set fzero [list F $zero -$precision $one] |
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| 163 | set fone [list F [::math::bignum::lshift 1 $precision] \ |
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| 164 | -$precision $one] |
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| 165 | # when $x is close to 1 (acos(1.0)=0.0) |
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| 166 | if {[equal $fone $x]} { |
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| 167 | return $fzero |
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| 168 | } |
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| 169 | if {[compare $fone $x]<0} { |
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| 170 | # the behavior assumed because acos(x) is not defined |
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| 171 | # when |x|>1 |
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| 172 | error "acos on a number greater than 1" |
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| 173 | } |
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| 174 | # acos(x) = asin(sqrt(1 - x^2)) |
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| 175 | # since 1 - cos(x)^2 = sin(x)^2 |
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| 176 | # x> sqrt(2)/2 so x^2 > 1/2 so 1-x^2<1/2 |
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| 177 | set x [sqrt [sub $fone [mul $x $x]]] |
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| 178 | # the parameter named x is smaller than sqrt(2)/2 |
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| 179 | return [_asin $x] |
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| 180 | } |
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| 181 | # acos(x) = Pi/2 - asin(x) |
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| 182 | # x<sqrt(2)/2 here too |
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| 183 | return [sub $piOverTwo [_asin $x]] |
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| 184 | } |
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| 185 | |
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| 186 | |
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| 187 | ################################################################################ |
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| 188 | # returns A + B |
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| 189 | ################################################################################ |
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| 190 | proc ::math::bigfloat::add {a b} { |
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| 191 | checkNumber a b |
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| 192 | if {[isInt $a]} { |
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| 193 | if {[isInt $b]} { |
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| 194 | # intAdd adds two BigInts |
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| 195 | return [::math::bignum::add $a $b] |
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| 196 | } |
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| 197 | # adds the BigInt a to the BigFloat b |
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| 198 | return [addInt2Float $b $a] |
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| 199 | } |
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| 200 | if {[isInt $b]} { |
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| 201 | # ... and vice-versa |
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| 202 | return [addInt2Float $a $b] |
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| 203 | } |
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| 204 | # retrieving parameters from A and B |
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| 205 | foreach {dummy integerA expA deltaA} $a {break} |
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| 206 | foreach {dummy integerB expB deltaB} $b {break} |
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| 207 | # when we add two numbers which have different digit numbers (after the dot) |
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| 208 | # for example : 1.0 and 0.00001 |
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| 209 | # We promote the one with the less number of digits (1.0) to the same level as |
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| 210 | # the other : so 1.00000. |
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| 211 | # that is why we shift left the number which has the greater exponent |
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| 212 | # But we do not forget the Delta parameter, which is lshift'ed too. |
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| 213 | if {$expA>$expB} { |
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| 214 | set diff [expr {$expA-$expB}] |
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| 215 | set integerA [::math::bignum::lshift $integerA $diff] |
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| 216 | set deltaA [::math::bignum::lshift $deltaA $diff] |
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| 217 | set integerA [::math::bignum::add $integerA $integerB] |
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| 218 | set deltaA [::math::bignum::add $deltaA $deltaB] |
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| 219 | return [normalize [list F $integerA $expB $deltaA]] |
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| 220 | } elseif {$expA==$expB} { |
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| 221 | # nothing to shift left |
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| 222 | return [normalize [list F [::math::bignum::add $integerA $integerB] \ |
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| 223 | $expA [::math::bignum::add $deltaA $deltaB]]] |
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| 224 | } else { |
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| 225 | set diff [expr {$expB-$expA}] |
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| 226 | set integerB [::math::bignum::lshift $integerB $diff] |
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| 227 | set deltaB [::math::bignum::lshift $deltaB $diff] |
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| 228 | set integerB [::math::bignum::add $integerA $integerB] |
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| 229 | set deltaB [::math::bignum::add $deltaB $deltaA] |
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| 230 | return [normalize [list F $integerB $expA $deltaB]] |
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| 231 | } |
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| 232 | } |
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| 233 | |
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| 234 | ################################################################################ |
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| 235 | # returns the sum A(BigFloat) + B(BigInt) |
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| 236 | # the greatest advantage of this method is that the uncertainty |
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| 237 | # of the result remains unchanged, in respect to the entry's uncertainty (deltaA) |
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| 238 | ################################################################################ |
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| 239 | proc ::math::bigfloat::addInt2Float {a b} { |
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| 240 | # type checking |
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| 241 | checkFloat a |
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| 242 | if {![isInt $b]} { |
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| 243 | error "'$b' is not a BigInt" |
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| 244 | } |
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| 245 | # retrieving data from $a |
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| 246 | foreach {dummy integerA expA deltaA} $a {break} |
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| 247 | # to add an int to a BigFloat,... |
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| 248 | if {$expA>0} { |
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| 249 | # we have to put the integer integerA |
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| 250 | # to the level of zero exponent : 1e8 --> 100000000e0 |
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| 251 | set shift $expA |
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| 252 | set integerA [::math::bignum::lshift $integerA $shift] |
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| 253 | set deltaA [::math::bignum::lshift $deltaA $shift] |
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| 254 | set integerA [::math::bignum::add $integerA $b] |
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| 255 | # we have to normalize, because we have shifted the mantissa |
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| 256 | # and the uncertainty left |
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| 257 | return [normalize [list F $integerA 0 $deltaA]] |
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| 258 | } elseif {$expA==0} { |
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| 259 | # integerA is already at integer level : float=(integerA)e0 |
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| 260 | return [normalize [list F [::math::bignum::add $integerA $b] \ |
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| 261 | 0 $deltaA]] |
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| 262 | } else { |
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| 263 | # here we have something like 234e-2 + 3 |
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| 264 | # we have to shift the integer left by the exponent |$expA| |
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| 265 | set b [::math::bignum::lshift $b [expr {-$expA}]] |
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| 266 | set integerA [::math::bignum::add $integerA $b] |
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| 267 | return [normalize [list F $integerA $expA $deltaA]] |
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| 268 | } |
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| 269 | } |
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| 270 | |
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| 271 | |
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| 272 | ################################################################################ |
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| 273 | # arcsinus of a BigFloat |
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| 274 | ################################################################################ |
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| 275 | proc ::math::bigfloat::asin {x} { |
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| 276 | # type checking |
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| 277 | checkFloat x |
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| 278 | foreach {dummy entier exp delta} $x {break} |
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| 279 | if {$exp>-1} { |
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| 280 | error "not enough precision on input (asin)" |
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| 281 | } |
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| 282 | set precision [expr {-$exp}] |
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| 283 | # when x=0, return 0 at the same precision as the input was |
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| 284 | if {[iszero $x]} { |
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| 285 | variable one |
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| 286 | variable zero |
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| 287 | return [list F $zero -$precision $one] |
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| 288 | } |
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| 289 | # asin(-x)=-asin(x) |
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| 290 | if {[::math::bignum::sign $entier]} { |
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| 291 | return [opp [asin [abs $x]]] |
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| 292 | } |
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| 293 | # 26/07/2005 : changed precision from decimal to binary |
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| 294 | set piOverTwo [floatRShift [pi $precision 1]] |
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| 295 | # now a little trick : asin(x)=Pi/2-asin(sqrt(1-x^2)) |
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| 296 | # so we can limit the entry of the Taylor development |
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| 297 | # to 1/sqrt(2)~0.7071 |
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| 298 | # the comparison is : if x>0.7071 then ... |
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| 299 | if {[compare $x [fromstr 0.7071]]>0} { |
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| 300 | variable one |
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| 301 | set fone [list F [::math::bignum::lshift 1 $precision] \ |
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| 302 | -$precision $one] |
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| 303 | # asin(1)=Pi/2 (with the same precision as the entry has) |
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| 304 | if {[equal $fone $x]} { |
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| 305 | return $piOverTwo |
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| 306 | } |
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| 307 | if {[compare $x $fone]>0} { |
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| 308 | error "asin on a number greater than 1" |
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| 309 | } |
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| 310 | # asin(x)=Pi/2-asin(sqrt(1-x^2)) |
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| 311 | set x [sqrt [sub $fone [mul $x $x]]] |
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| 312 | return [sub $piOverTwo [_asin $x]] |
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| 313 | } |
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| 314 | return [normalize [_asin $x]] |
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| 315 | } |
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| 316 | |
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| 317 | ################################################################################ |
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| 318 | # _asin : arcsinus of numbers between 0 and +1 |
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| 319 | ################################################################################ |
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| 320 | proc ::math::bigfloat::_asin {x} { |
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| 321 | # Taylor development |
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| 322 | # asin(x)=x + 1/2 x^3/3 + 3/2.4 x^5/5 + 3.5/2.4.6 x^7/7 + ... |
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| 323 | # into this iterative form : |
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| 324 | # asin(x)=x * (1 + 1/2 * x^2 * (1/3 + 3/4 *x^2 * (... |
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| 325 | # ...* (1/(2n-1) + (2n-1)/2n * x^2 / (2n+1))...))) |
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| 326 | # we show how is really computed the development : |
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| 327 | # we don't need to set a var with x^n or a product of integers |
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| 328 | # all we need is : x^2, 2n-1, 2n, 2n+1 and a few variables |
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| 329 | foreach {dummy mantissa exp delta} $x {break} |
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| 330 | set precision [expr {-$exp}] |
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| 331 | if {$precision+1<[::math::bignum::bits $mantissa]} { |
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| 332 | error "sinus greater than 1" |
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| 333 | } |
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| 334 | # precision is the number of after-dot digits |
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| 335 | set result $mantissa |
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| 336 | set delta_final $delta |
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| 337 | # resultat is the final result, and delta_final |
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| 338 | # will contain the uncertainty of the result |
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| 339 | # square is the square of the mantissa |
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| 340 | set square [intMulShift $mantissa $mantissa $precision] |
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| 341 | # dt is the uncertainty of Mantissa |
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| 342 | set dt [::math::bignum::add 1 [intMulShift $mantissa $delta [expr {$precision-1}]]] |
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| 343 | # these three are required to compute the fractions implicated into |
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| 344 | # the development (of Taylor, see former) |
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| 345 | variable one |
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| 346 | set num $one |
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| 347 | # two will be used into the loop |
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| 348 | variable two |
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| 349 | variable three |
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| 350 | set i $three |
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| 351 | set denom $two |
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| 352 | # the nth factor equals : $num/$denom* $mantissa/$i |
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| 353 | set delta [::math::bignum::add [::math::bignum::mul $delta $square] \ |
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| 354 | [::math::bignum::mul $dt [::math::bignum::add $delta $mantissa]]] |
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| 355 | set delta [::math::bignum::add 1 [::math::bignum::rshift [::math::bignum::div \ |
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| 356 | [::math::bignum::mul $delta $num] $denom] $precision]] |
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| 357 | # we do not multiply the Mantissa by $num right now because it is 1 ! |
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| 358 | # but we have Mantissa=$x |
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| 359 | # and we want Mantissa*$x^2 * $num / $denom / $i |
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| 360 | set mantissa [intMulShift $mantissa $square $precision] |
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| 361 | set mantissa [::math::bignum::div $mantissa $denom] |
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| 362 | # do not forget the modified Taylor development : |
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| 363 | # asin(x)=x * (1 + 1/2*x^2*(1/3 + 3/4*x^2*(...*(1/(2n-1) + (2n-1)/2n*x^2/(2n+1))...))) |
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| 364 | # all we need is : x^2, 2n-1, 2n, 2n+1 and a few variables |
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| 365 | # $num=2n-1 $denom=2n $square=x^2 and $i=2n+1 |
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| 366 | set mantissa_temp [::math::bignum::div $mantissa $i] |
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| 367 | set delta_temp [::math::bignum::add 1 [::math::bignum::div $delta $i]] |
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| 368 | # when the Mantissa increment is smaller than the Delta increment, |
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| 369 | # we would not get much precision by continuing the development |
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| 370 | while {![::math::bignum::iszero $mantissa_temp]} { |
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| 371 | # Mantissa = Mantissa * $num/$denom * $square |
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| 372 | # Add Mantissa/$i, which is stored in $mantissa_temp, to the result |
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| 373 | set result [::math::bignum::add $result $mantissa_temp] |
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| 374 | set delta_final [::math::bignum::add $delta_final $delta_temp] |
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| 375 | # here we have $two instead of [fromstr 2] (optimization) |
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| 376 | # num=num+2,i=i+2,denom=denom+2 |
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| 377 | # because num=2n-1 denom=2n and i=2n+1 |
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| 378 | set num [::math::bignum::add $num $two] |
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| 379 | set i [::math::bignum::add $i $two] |
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| 380 | set denom [::math::bignum::add $denom $two] |
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| 381 | # computes precisly the future Delta parameter |
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| 382 | set delta [::math::bignum::add [::math::bignum::mul $delta $square] \ |
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| 383 | [::math::bignum::mul $dt [::math::bignum::add $delta $mantissa]]] |
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| 384 | set delta [::math::bignum::add 1 [::math::bignum::rshift [::math::bignum::div \ |
|---|
| 385 | [::math::bignum::mul $delta $num] $denom] $precision]] |
|---|
| 386 | set mantissa [intMulShift $mantissa $square $precision] |
|---|
| 387 | set mantissa [::math::bignum::div [::math::bignum::mul $mantissa $num] $denom] |
|---|
| 388 | set mantissa_temp [::math::bignum::div $mantissa $i] |
|---|
| 389 | set delta_temp [::math::bignum::add 1 [::math::bignum::div $delta $i]] |
|---|
| 390 | } |
|---|
| 391 | return [list F $result $exp $delta_final] |
|---|
| 392 | } |
|---|
| 393 | |
|---|
| 394 | ################################################################################ |
|---|
| 395 | # arctangent : returns atan(x) |
|---|
| 396 | ################################################################################ |
|---|
| 397 | proc ::math::bigfloat::atan {x} { |
|---|
| 398 | checkFloat x |
|---|
| 399 | variable one |
|---|
| 400 | variable two |
|---|
| 401 | variable three |
|---|
| 402 | variable four |
|---|
| 403 | variable zero |
|---|
| 404 | foreach {dummy mantissa exp delta} $x {break} |
|---|
| 405 | if {$exp>=0} { |
|---|
| 406 | error "not enough precision to compute atan" |
|---|
| 407 | } |
|---|
| 408 | set precision [expr {-$exp}] |
|---|
| 409 | # atan(0)=0 |
|---|
| 410 | if {[iszero $x]} { |
|---|
| 411 | return [list F $zero -$precision $one] |
|---|
| 412 | } |
|---|
| 413 | # atan(-x)=-atan(x) |
|---|
| 414 | if {[::math::bignum::sign $mantissa]} { |
|---|
| 415 | return [opp [atan [abs $x]]] |
|---|
| 416 | } |
|---|
| 417 | # now x is strictly positive |
|---|
| 418 | # at this moment, we are trying to limit |x| to a fair acceptable number |
|---|
| 419 | # to ensure that Taylor development will converge quickly |
|---|
| 420 | set float1 [list F [::math::bignum::lshift 1 $precision] -$precision $one] |
|---|
| 421 | if {[compare $float1 $x]<0} { |
|---|
| 422 | # compare x to 2.4142 |
|---|
| 423 | if {[compare $x [fromstr 2.4142]]<0} { |
|---|
| 424 | # atan(x)=Pi/4 + atan((x-1)/(x+1)) |
|---|
| 425 | # as 1<x<2.4142 : (x-1)/(x+1)=1-2/(x+1) belongs to |
|---|
| 426 | # the range : ]0,1-2/3.414[ |
|---|
| 427 | # that equals ]0,0.414[ |
|---|
| 428 | set pi_sur_quatre [div [pi $precision 1] $four] |
|---|
| 429 | return [add $pi_sur_quatre [atan \ |
|---|
| 430 | [div [sub $x $float1] [add $x $float1]]]] |
|---|
| 431 | } |
|---|
| 432 | # atan(x)=Pi/2-atan(1/x) |
|---|
| 433 | # 1/x < 1/2.414 so the argument is lower than 0.414 |
|---|
| 434 | set pi_over_two [div [pi $precision 1] $two] |
|---|
| 435 | return [sub $pi_over_two [atan [div $float1 $x]]] |
|---|
| 436 | } |
|---|
| 437 | if {[compare $x [fromstr 0.4142]]>0} { |
|---|
| 438 | # atan(x)=Pi/4 + atan((x-1)/(x+1)) |
|---|
| 439 | # x>0.420 so (x-1)/(x+1)=1 - 2/(x+1) > 1-2/1.414 |
|---|
| 440 | # > -0.414 |
|---|
| 441 | # x<1 so (x-1)/(x+1)<0 |
|---|
| 442 | set pi_sur_quatre [div [pi $precision 1] $four] |
|---|
| 443 | return [add $pi_sur_quatre [atan \ |
|---|
| 444 | [div [sub $x $float1] [add $x $float1]]]] |
|---|
| 445 | } |
|---|
| 446 | # precision increment : to have less uncertainty |
|---|
| 447 | # we add a little more precision so that the result would be more accurate |
|---|
| 448 | # Taylor development : x - x^3/3 + x^5/5 - ... + (-1)^(n+1)*x^(2n-1)/(2n-1) |
|---|
| 449 | # when we have n steps in Taylor development : the nth term is : |
|---|
| 450 | # x^(2n-1)/(2n-1) |
|---|
| 451 | # and the loss of precision is of 2n (n sums and n divisions) |
|---|
| 452 | # this command is called with x<sqrt(2)-1 |
|---|
| 453 | # if we add an increment to the precision, say n: |
|---|
| 454 | # (sqrt(2)-1)^(2n-1)/(2n-1) has to be lower than 2^(-precision-n-1) |
|---|
| 455 | # (2n-1)*log(sqrt(2)-1)-log(2n-1)<-(precision+n+1)*log(2) |
|---|
| 456 | # 2n(log(sqrt(2)-1)-log(sqrt(2)))<-(precision-1)*log(2)+log(2n-1)+log(sqrt(2)-1) |
|---|
| 457 | # 2n*log(1-1/sqrt(2))<-(precision-1)*log(2)+log(2n-1)+log(2)/2 |
|---|
| 458 | # 2n/sqrt(2)>(precision-3/2)*log(2)-log(2n-1) |
|---|
| 459 | # hence log(2n-1)<2n-1 |
|---|
| 460 | # n*sqrt(2)>(precision-1.5)*log(2)+1-2n |
|---|
| 461 | # n*(sqrt(2)+2)>(precision-1.5)*log(2)+1 |
|---|
| 462 | set n [expr {int((log(2)*($precision-1.5)+1)/(sqrt(2)+2)+1)}] |
|---|
| 463 | incr precision $n |
|---|
| 464 | set mantissa [::math::bignum::lshift $mantissa $n] |
|---|
| 465 | set delta [::math::bignum::lshift $delta $n] |
|---|
| 466 | # end of adding precision increment |
|---|
| 467 | # now computing Taylor development : |
|---|
| 468 | # atan(x)=x - x^3/3 + x^5/5 - x^7/7 ... + (-1)^n*x^(2n+1)/(2n+1) |
|---|
| 469 | # atan(x)=x * (1 - x^2 * (1/3 - x^2 * (1/5 - x^2 * (...*(1/(2n-1) - x^2 / (2n+1))...)))) |
|---|
| 470 | # what do we need to compute this ? |
|---|
| 471 | # x^2 ($square), 2n+1 ($divider), $result, the nth term of the development ($t) |
|---|
| 472 | # and the nth term multiplied by 2n+1 ($temp) |
|---|
| 473 | # then we do this (with care keeping as much precision as possible): |
|---|
| 474 | # while ($t <>0) : |
|---|
| 475 | # $result=$result+$t |
|---|
| 476 | # $temp=$temp * $square |
|---|
| 477 | # $divider = $divider+2 |
|---|
| 478 | # $t=$temp/$divider |
|---|
| 479 | # end-while |
|---|
| 480 | set result $mantissa |
|---|
| 481 | set delta_end $delta |
|---|
| 482 | # we store the square of the integer (mantissa) |
|---|
| 483 | set delta_square [::math::bignum::lshift $delta 1] |
|---|
| 484 | set square [intMulShift $mantissa $mantissa $precision] |
|---|
| 485 | # the (2n+1) divider |
|---|
| 486 | set divider $three |
|---|
| 487 | # computing precisely the uncertainty |
|---|
| 488 | set delta [::math::bignum::add 1 [::math::bignum::rshift [::math::bignum::add \ |
|---|
| 489 | [::math::bignum::mul $delta_square $mantissa] \ |
|---|
| 490 | [::math::bignum::mul $delta $square]] $precision]] |
|---|
| 491 | # temp contains (-1)^n*x^(2n+1) |
|---|
| 492 | set temp [opp [intMulShift $mantissa $square $precision]] |
|---|
| 493 | set t [::math::bignum::div $temp $divider] |
|---|
| 494 | set dt [::math::bignum::add 1 [::math::bignum::div $delta $divider]] |
|---|
| 495 | while {![::math::bignum::iszero $t]} { |
|---|
| 496 | set result [::math::bignum::add $result $t] |
|---|
| 497 | set delta_end [::math::bignum::add $delta_end $dt] |
|---|
| 498 | set divider [::math::bignum::add $divider $two] |
|---|
| 499 | set delta [::math::bignum::add 1 [::math::bignum::rshift [::math::bignum::add \ |
|---|
| 500 | [::math::bignum::mul $delta_square [abs $temp]] [::math::bignum::mul $delta \ |
|---|
| 501 | [::math::bignum::add $delta_square $square]]] $precision]] |
|---|
| 502 | set temp [opp [intMulShift $temp $square $precision]] |
|---|
| 503 | set t [::math::bignum::div $temp $divider] |
|---|
| 504 | set dt [::math::bignum::add [::math::bignum::div $delta $divider] $one] |
|---|
| 505 | } |
|---|
| 506 | # we have to normalize because the uncertainty might be greater than 99 |
|---|
| 507 | # moreover it is the most often case |
|---|
| 508 | return [normalize [list F $result [expr {$exp-$n}] $delta_end]] |
|---|
| 509 | } |
|---|
| 510 | |
|---|
| 511 | |
|---|
| 512 | ################################################################################ |
|---|
| 513 | # compute atan(1/integer) at a given precision |
|---|
| 514 | # this proc is only used to compute Pi |
|---|
| 515 | # it is using the same Taylor development as [atan] |
|---|
| 516 | ################################################################################ |
|---|
| 517 | proc ::math::bigfloat::_atanfract {integer precision} { |
|---|
| 518 | # Taylor development : x - x^3/3 + x^5/5 - ... + (-1)^(n+1)*x^(2n-1)/(2n-1) |
|---|
| 519 | # when we have n steps in Taylor development : the nth term is : |
|---|
| 520 | # 1/denom^(2n+1)/(2n+1) |
|---|
| 521 | # and the loss of precision is of 2n (n sums and n divisions) |
|---|
| 522 | # this command is called with integer>=5 |
|---|
| 523 | # |
|---|
| 524 | # We do not want to compute the Delta parameter, so we just |
|---|
| 525 | # can increment precision (with lshift) in order for the result to be precise. |
|---|
| 526 | # Remember : we compute atan2(1,$integer) with $precision bits |
|---|
| 527 | # $integer has no Delta parameter as it is a BigInt, of course, so |
|---|
| 528 | # theorically we could compute *any* number of digits. |
|---|
| 529 | # |
|---|
| 530 | # if we add an increment to the precision, say n: |
|---|
| 531 | # (1/5)^(2n-1)/(2n-1) has to be lower than (1/2)^(precision+n-1) |
|---|
| 532 | # Calculus : |
|---|
| 533 | # log(left term) < log(right term) |
|---|
| 534 | # log(1/left term) > log(1/right term) |
|---|
| 535 | # (2n-1)*log(5)+log(2n-1)>(precision+n-1)*log(2) |
|---|
| 536 | # n(2log(5)-log(2))>(precision-1)*log(2)-log(2n-1)+log(5) |
|---|
| 537 | # -log(2n-1)>-(2n-1) |
|---|
| 538 | # n(2log(5)-log(2)+2)>(precision-1)*log(2)+1+log(5) |
|---|
| 539 | set n [expr {int((($precision-1)*log(2)+1+log(5))/(2*log(5)-log(2)+2)+1)}] |
|---|
| 540 | incr precision $n |
|---|
| 541 | # first term of the development : 1/integer |
|---|
| 542 | set a [::math::bignum::div [::math::bignum::lshift 1 $precision] $integer] |
|---|
| 543 | # 's' will contain the result |
|---|
| 544 | set s $a |
|---|
| 545 | # Taylor development : x - x^3/3 + x^5/5 - ... + (-1)^(n+1)*x^(2n-1)/(2n-1) |
|---|
| 546 | # equals x (1 - x^2 * (1/3 + x^2 * (... * (1/(2n-3) + (-1)^(n+1) * x^2 / (2n-1))...))) |
|---|
| 547 | # all we need to store is : 2n-1 ($denom), x^(2n+1) and x^2 ($square) and two results : |
|---|
| 548 | # - the nth term => $u |
|---|
| 549 | # - the nth term * (2n-1) => $t |
|---|
| 550 | # + of course, the result $s |
|---|
| 551 | set square [::math::bignum::mul $integer $integer] |
|---|
| 552 | variable two |
|---|
| 553 | variable three |
|---|
| 554 | set denom $three |
|---|
| 555 | # $t is (-1)^n*x^(2n+1) |
|---|
| 556 | set t [opp [::math::bignum::div $a $square]] |
|---|
| 557 | set u [::math::bignum::div $t $denom] |
|---|
| 558 | # we break the loop when the current term of the development is null |
|---|
| 559 | while {![::math::bignum::iszero $u]} { |
|---|
| 560 | set s [::math::bignum::add $s $u] |
|---|
| 561 | # denominator= (2n+1) |
|---|
| 562 | set denom [::math::bignum::add $denom $two] |
|---|
| 563 | # div $t by x^2 |
|---|
| 564 | set t [opp [::math::bignum::div $t $square]] |
|---|
| 565 | set u [::math::bignum::div $t $denom] |
|---|
| 566 | } |
|---|
| 567 | # go back to the initial precision |
|---|
| 568 | return [::math::bignum::rshift $s $n] |
|---|
| 569 | } |
|---|
| 570 | |
|---|
| 571 | |
|---|
| 572 | ################################################################################ |
|---|
| 573 | # returns the integer part of a BigFloat, as a BigInt |
|---|
| 574 | # the result is the same one you would have |
|---|
| 575 | # if you had called [expr {ceil($x)}] |
|---|
| 576 | ################################################################################ |
|---|
| 577 | proc ::math::bigfloat::ceil {number} { |
|---|
| 578 | checkFloat number |
|---|
| 579 | set number [normalize $number] |
|---|
| 580 | if {[iszero $number]} { |
|---|
| 581 | # returns the BigInt 0 |
|---|
| 582 | variable zero |
|---|
| 583 | return $zero |
|---|
| 584 | } |
|---|
| 585 | foreach {dummy integer exp delta} $number {break} |
|---|
| 586 | if {$exp>=0} { |
|---|
| 587 | error "not enough precision to perform rounding (ceil)" |
|---|
| 588 | } |
|---|
| 589 | # saving the sign ... |
|---|
| 590 | set sign [::math::bignum::sign $integer] |
|---|
| 591 | set integer [abs $integer] |
|---|
| 592 | # integer part |
|---|
| 593 | set try [::math::bignum::rshift $integer [expr {-$exp}]] |
|---|
| 594 | if {$sign} { |
|---|
| 595 | return [opp $try] |
|---|
| 596 | } |
|---|
| 597 | # fractional part |
|---|
| 598 | if {![equal [::math::bignum::lshift $try [expr {-$exp}]] $integer]} { |
|---|
| 599 | return [::math::bignum::add 1 $try] |
|---|
| 600 | } |
|---|
| 601 | return $try |
|---|
| 602 | } |
|---|
| 603 | |
|---|
| 604 | |
|---|
| 605 | ################################################################################ |
|---|
| 606 | # checks each variable to be a BigFloat |
|---|
| 607 | # arguments : each argument is the name of a variable to be checked |
|---|
| 608 | ################################################################################ |
|---|
| 609 | proc ::math::bigfloat::checkFloat {args} { |
|---|
| 610 | foreach x $args { |
|---|
| 611 | upvar $x n |
|---|
| 612 | if {![isFloat $n]} { |
|---|
| 613 | error "BigFloat expected : received '$n'" |
|---|
| 614 | } |
|---|
| 615 | } |
|---|
| 616 | } |
|---|
| 617 | |
|---|
| 618 | ################################################################################ |
|---|
| 619 | # checks if each number is either a BigFloat or a BigInt |
|---|
| 620 | # arguments : each argument is the name of a variable to be checked |
|---|
| 621 | ################################################################################ |
|---|
| 622 | proc ::math::bigfloat::checkNumber {args} { |
|---|
| 623 | foreach i $args { |
|---|
| 624 | upvar $i x |
|---|
| 625 | if {![isInt $x] && ![isFloat $x]} { |
|---|
| 626 | error "'$x' is not a number" |
|---|
| 627 | } |
|---|
| 628 | } |
|---|
| 629 | } |
|---|
| 630 | |
|---|
| 631 | |
|---|
| 632 | ################################################################################ |
|---|
| 633 | # returns 0 if A and B are equal, else returns 1 or -1 |
|---|
| 634 | # accordingly to the sign of (A - B) |
|---|
| 635 | ################################################################################ |
|---|
| 636 | proc ::math::bigfloat::compare {a b} { |
|---|
| 637 | if {[isInt $a] && [isInt $b]} { |
|---|
| 638 | return [::math::bignum::cmp $a $b] |
|---|
| 639 | } |
|---|
| 640 | checkFloat a b |
|---|
| 641 | if {[equal $a $b]} {return 0} |
|---|
| 642 | return [expr {([::math::bignum::sign [lindex [sub $a $b] 1]])?-1:1}] |
|---|
| 643 | } |
|---|
| 644 | |
|---|
| 645 | |
|---|
| 646 | |
|---|
| 647 | |
|---|
| 648 | ################################################################################ |
|---|
| 649 | # gets cos(x) |
|---|
| 650 | # throws an error if there is not enough precision on the input |
|---|
| 651 | ################################################################################ |
|---|
| 652 | proc ::math::bigfloat::cos {x} { |
|---|
| 653 | checkFloat x |
|---|
| 654 | foreach {dummy integer exp delta} $x {break} |
|---|
| 655 | if {$exp>-2} { |
|---|
| 656 | error "not enough precision on floating-point number" |
|---|
| 657 | } |
|---|
| 658 | set precision [expr {-$exp}] |
|---|
| 659 | # cos(2kPi+x)=cos(x) |
|---|
| 660 | foreach {n integer} [divPiQuarter $integer $precision] {break} |
|---|
| 661 | # now integer>=0 and <Pi/2 |
|---|
| 662 | set d [expr {[tostr $n]%4}] |
|---|
| 663 | # add trigonometric circle turns number to delta |
|---|
| 664 | set delta [::math::bignum::add [abs $n] $delta] |
|---|
| 665 | set signe 0 |
|---|
| 666 | # cos(Pi-x)=-cos(x) |
|---|
| 667 | # cos(-x)=cos(x) |
|---|
| 668 | # cos(Pi/2-x)=sin(x) |
|---|
| 669 | switch -- $d { |
|---|
| 670 | 1 {set signe 1;set l [_sin2 $integer $precision $delta]} |
|---|
| 671 | 2 {set signe 1;set l [_cos2 $integer $precision $delta]} |
|---|
| 672 | 0 {set l [_cos2 $integer $precision $delta]} |
|---|
| 673 | 3 {set l [_sin2 $integer $precision $delta]} |
|---|
| 674 | default {error "internal error"} |
|---|
| 675 | } |
|---|
| 676 | # precision -> exp (multiplied by -1) |
|---|
| 677 | lset l 1 [expr {-([lindex $l 1])}] |
|---|
| 678 | # set the sign |
|---|
| 679 | set integer [lindex $l 0] |
|---|
| 680 | ::math::bignum::setsign integer $signe |
|---|
| 681 | lset l 0 $integer |
|---|
| 682 | return [normalize [linsert $l 0 F]] |
|---|
| 683 | } |
|---|
| 684 | |
|---|
| 685 | ################################################################################ |
|---|
| 686 | # compute cos(x) where 0<=x<Pi/2 |
|---|
| 687 | # returns : a list formed with : |
|---|
| 688 | # 1. the mantissa |
|---|
| 689 | # 2. the precision (opposite of the exponent) |
|---|
| 690 | # 3. the uncertainty (doubt range) |
|---|
| 691 | ################################################################################ |
|---|
| 692 | proc ::math::bigfloat::_cos2 {x precision delta} { |
|---|
| 693 | # precision bits after the dot |
|---|
| 694 | set pi [_pi $precision] |
|---|
| 695 | set pis4 [::math::bignum::rshift $pi 2] |
|---|
| 696 | set pis2 [::math::bignum::rshift $pi 1] |
|---|
| 697 | if {[::math::bignum::cmp $x $pis4]>=0} { |
|---|
| 698 | # cos(Pi/2-x)=sin(x) |
|---|
| 699 | set x [::math::bignum::sub $pis2 $x] |
|---|
| 700 | set delta [::math::bignum::add 1 $delta] |
|---|
| 701 | return [_sin $x $precision $delta] |
|---|
| 702 | } |
|---|
| 703 | return [_cos $x $precision $delta] |
|---|
| 704 | } |
|---|
| 705 | |
|---|
| 706 | ################################################################################ |
|---|
| 707 | # compute cos(x) where 0<=x<Pi/4 |
|---|
| 708 | # returns : a list formed with : |
|---|
| 709 | # 1. the mantissa |
|---|
| 710 | # 2. the precision (opposite of the exponent) |
|---|
| 711 | # 3. the uncertainty (doubt range) |
|---|
| 712 | ################################################################################ |
|---|
| 713 | proc ::math::bigfloat::_cos {x precision delta} { |
|---|
| 714 | variable zero |
|---|
| 715 | variable one |
|---|
| 716 | variable two |
|---|
| 717 | set float1 [::math::bignum::lshift $one $precision] |
|---|
| 718 | # Taylor development follows : |
|---|
| 719 | # cos(x)=1-x^2/2 + x^4/4! ... + (-1)^(2n)*x^(2n)/2n! |
|---|
| 720 | # cos(x)= 1 - x^2/1.2 * (1 - x^2/3.4 * (... * (1 - x^2/(2n.(2n-1))...)) |
|---|
| 721 | # variables : $s (the Mantissa of the result) |
|---|
| 722 | # $denom1 & $denom2 (2n-1 & 2n) |
|---|
| 723 | # $x as the square of what is named x in 'cos(x)' |
|---|
| 724 | set s $float1 |
|---|
| 725 | # 'd' is the uncertainty on x^2 |
|---|
| 726 | set d [::math::bignum::mul $x [::math::bignum::lshift $delta 1]] |
|---|
| 727 | set d [::math::bignum::add 1 [::math::bignum::rshift $d $precision]] |
|---|
| 728 | # x=x^2 (because in this Taylor development, there are only even powers of x) |
|---|
| 729 | set x [intMulShift $x $x $precision] |
|---|
| 730 | set denom1 $one |
|---|
| 731 | set denom2 $two |
|---|
| 732 | set t [opp [::math::bignum::rshift $x 1]] |
|---|
| 733 | set delta $zero |
|---|
| 734 | set dt $d |
|---|
| 735 | while {![::math::bignum::iszero $t]} { |
|---|
| 736 | set s [::math::bignum::add $s $t] |
|---|
| 737 | set delta [::math::bignum::add $delta $dt] |
|---|
| 738 | set denom1 [::math::bignum::add $denom1 $two] |
|---|
| 739 | set denom2 [::math::bignum::add $denom2 $two] |
|---|
| 740 | set dt [::math::bignum::rshift [::math::bignum::add [::math::bignum::mul $x $dt]\ |
|---|
| 741 | [::math::bignum::mul [::math::bignum::add $t $dt] $d]] $precision] |
|---|
| 742 | set dt [::math::bignum::add 1 $dt] |
|---|
| 743 | set t [intMulShift $x $t $precision] |
|---|
| 744 | set t [opp [::math::bignum::div $t [::math::bignum::mul $denom1 $denom2]]] |
|---|
| 745 | } |
|---|
| 746 | return [list $s $precision $delta] |
|---|
| 747 | } |
|---|
| 748 | |
|---|
| 749 | ################################################################################ |
|---|
| 750 | # cotangent : the trivial algorithm is used |
|---|
| 751 | ################################################################################ |
|---|
| 752 | proc ::math::bigfloat::cotan {x} { |
|---|
| 753 | return [::math::bigfloat::div [::math::bigfloat::cos $x] [::math::bigfloat::sin $x]] |
|---|
| 754 | } |
|---|
| 755 | |
|---|
| 756 | ################################################################################ |
|---|
| 757 | # converts angles from degrees to radians |
|---|
| 758 | # deg/180=rad/Pi |
|---|
| 759 | ################################################################################ |
|---|
| 760 | proc ::math::bigfloat::deg2rad {x} { |
|---|
| 761 | checkFloat x |
|---|
| 762 | set xLen [expr {-[lindex $x 2]}] |
|---|
| 763 | if {$xLen<3} { |
|---|
| 764 | error "number too loose to convert to radians" |
|---|
| 765 | } |
|---|
| 766 | set pi [pi $xLen 1] |
|---|
| 767 | return [div [mul $x $pi] [::math::bignum::fromstr 180]] |
|---|
| 768 | } |
|---|
| 769 | |
|---|
| 770 | |
|---|
| 771 | |
|---|
| 772 | ################################################################################ |
|---|
| 773 | # private proc to get : x modulo Pi/2 |
|---|
| 774 | # and the quotient (x divided by Pi/2) |
|---|
| 775 | # used by cos , sin & others |
|---|
| 776 | ################################################################################ |
|---|
| 777 | proc ::math::bigfloat::divPiQuarter {integer precision} { |
|---|
| 778 | incr precision 2 |
|---|
| 779 | set integer [::math::bignum::lshift $integer 1] |
|---|
| 780 | set dpi [_pi $precision] |
|---|
| 781 | # modulo 2Pi |
|---|
| 782 | foreach {n integer} [::math::bignum::divqr $integer $dpi] {break} |
|---|
| 783 | # end modulo 2Pi |
|---|
| 784 | set pi [::math::bignum::rshift $dpi 1] |
|---|
| 785 | foreach {n integer} [::math::bignum::divqr $integer $pi] {break} |
|---|
| 786 | # now divide by Pi/2 |
|---|
| 787 | # multiply n by 2 |
|---|
| 788 | set n [::math::bignum::lshift $n 1] |
|---|
| 789 | # pis2=pi/2 |
|---|
| 790 | set pis2 [::math::bignum::rshift $pi 1] |
|---|
| 791 | foreach {m integer} [::math::bignum::divqr $integer $pis2] {break} |
|---|
| 792 | return [list [::math::bignum::add $n $m] [::math::bignum::rshift $integer 1]] |
|---|
| 793 | } |
|---|
| 794 | |
|---|
| 795 | |
|---|
| 796 | ################################################################################ |
|---|
| 797 | # divide A by B and returns the result |
|---|
| 798 | # throw error : divide by zero |
|---|
| 799 | ################################################################################ |
|---|
| 800 | proc ::math::bigfloat::div {a b} { |
|---|
| 801 | variable one |
|---|
| 802 | checkNumber a b |
|---|
| 803 | # dispatch to an appropriate procedure |
|---|
| 804 | if {[isInt $a]} { |
|---|
| 805 | if {[isInt $b]} { |
|---|
| 806 | return [::math::bignum::div $a $b] |
|---|
| 807 | } |
|---|
| 808 | error "trying to divide a BigInt by a BigFloat" |
|---|
| 809 | } |
|---|
| 810 | if {[isInt $b]} {return [divFloatByInt $a $b]} |
|---|
| 811 | foreach {dummy integerA expA deltaA} $a {break} |
|---|
| 812 | foreach {dummy integerB expB deltaB} $b {break} |
|---|
| 813 | # computes the limits of the doubt (or uncertainty) interval |
|---|
| 814 | set BMin [::math::bignum::sub $integerB $deltaB] |
|---|
| 815 | set BMax [::math::bignum::add $integerB $deltaB] |
|---|
| 816 | if {[::math::bignum::cmp $BMin $BMax]>0} { |
|---|
| 817 | # swap BMin and BMax |
|---|
| 818 | set temp $BMin |
|---|
| 819 | set BMin $BMax |
|---|
| 820 | set BMax $temp |
|---|
| 821 | } |
|---|
| 822 | # multiply by zero gives zero |
|---|
| 823 | if {[::math::bignum::iszero $integerA]} { |
|---|
| 824 | # why not return any number or the integer 0 ? |
|---|
| 825 | # because there is an exponent that might be different between two BigFloats |
|---|
| 826 | # 0.00 --> exp = -2, 0.000000 -> exp = -6 |
|---|
| 827 | return $a |
|---|
| 828 | } |
|---|
| 829 | # test of the division by zero |
|---|
| 830 | if {[::math::bignum::sign $BMin]+[::math::bignum::sign $BMax]==1 || \ |
|---|
| 831 | [::math::bignum::iszero $BMin] || [::math::bignum::iszero $BMax]} { |
|---|
| 832 | error "divide by zero" |
|---|
| 833 | } |
|---|
| 834 | # shift A because we need accuracy |
|---|
| 835 | set l [math::bignum::bits $integerB] |
|---|
| 836 | set integerA [::math::bignum::lshift $integerA $l] |
|---|
| 837 | set deltaA [::math::bignum::lshift $deltaA $l] |
|---|
| 838 | set exp [expr {$expA-$l-$expB}] |
|---|
| 839 | # relative uncertainties (dX/X) are added |
|---|
| 840 | # to give the relative uncertainty of the result |
|---|
| 841 | # i.e. 3% on A + 2% on B --> 5% on the quotient |
|---|
| 842 | # d(A/B)/(A/B)=dA/A + dB/B |
|---|
| 843 | # Q=A/B |
|---|
| 844 | # dQ=dA/B + dB*A/B*B |
|---|
| 845 | # dQ is "delta" |
|---|
| 846 | set delta [::math::bignum::div [::math::bignum::mul $deltaB \ |
|---|
| 847 | [abs $integerA]] [abs $integerB]] |
|---|
| 848 | set delta [::math::bignum::div [::math::bignum::add\ |
|---|
| 849 | [::math::bignum::add 1 $delta]\ |
|---|
| 850 | $deltaA] [abs $integerB]] |
|---|
| 851 | set quotient [::math::bignum::div $integerA $integerB] |
|---|
| 852 | if {[::math::bignum::sign $integerB]+[::math::bignum::sign $integerA]==1} { |
|---|
| 853 | set quotient [::math::bignum::sub $quotient 1] |
|---|
| 854 | } |
|---|
| 855 | return [normalize [list F $quotient $exp [::math::bignum::add $delta 1]]] |
|---|
| 856 | } |
|---|
| 857 | |
|---|
| 858 | |
|---|
| 859 | |
|---|
| 860 | |
|---|
| 861 | ################################################################################ |
|---|
| 862 | # divide a BigFloat A by a BigInt B |
|---|
| 863 | # throw error : divide by zero |
|---|
| 864 | ################################################################################ |
|---|
| 865 | proc ::math::bigfloat::divFloatByInt {a b} { |
|---|
| 866 | variable one |
|---|
| 867 | # type check |
|---|
| 868 | checkFloat a |
|---|
| 869 | if {![isInt $b]} { |
|---|
| 870 | error "'$b' is not a BigInt" |
|---|
| 871 | } |
|---|
| 872 | foreach {dummy integer exp delta} $a {break} |
|---|
| 873 | # zero divider test |
|---|
| 874 | if {[::math::bignum::iszero $b]} { |
|---|
| 875 | error "divide by zero" |
|---|
| 876 | } |
|---|
| 877 | # shift left for accuracy ; see other comments in [div] procedure |
|---|
| 878 | set l [::math::bignum::bits $b] |
|---|
| 879 | set integer [::math::bignum::lshift $integer $l] |
|---|
| 880 | set delta [::math::bignum::lshift $delta $l] |
|---|
| 881 | incr exp -$l |
|---|
| 882 | set integer [::math::bignum::div $integer $b] |
|---|
| 883 | # the uncertainty is always evaluated to the ceil value |
|---|
| 884 | # and as an absolute value |
|---|
| 885 | set delta [::math::bignum::add 1 [::math::bignum::div $delta [abs $b]]] |
|---|
| 886 | return [normalize [list F $integer $exp $delta]] |
|---|
| 887 | } |
|---|
| 888 | |
|---|
| 889 | |
|---|
| 890 | |
|---|
| 891 | |
|---|
| 892 | |
|---|
| 893 | ################################################################################ |
|---|
| 894 | # returns 1 if A and B are equal, 0 otherwise |
|---|
| 895 | # IN : a, b (BigFloats) |
|---|
| 896 | ################################################################################ |
|---|
| 897 | proc ::math::bigfloat::equal {a b} { |
|---|
| 898 | if {[isInt $a] && [isInt $b]} { |
|---|
| 899 | return [expr {[::math::bignum::cmp $a $b]==0}] |
|---|
| 900 | } |
|---|
| 901 | # now a & b should only be BigFloats |
|---|
| 902 | checkFloat a b |
|---|
| 903 | foreach {dummy aint aexp adelta} $a {break} |
|---|
| 904 | foreach {dummy bint bexp bdelta} $b {break} |
|---|
| 905 | # set all Mantissas and Deltas to the same level (exponent) |
|---|
| 906 | # with lshift |
|---|
| 907 | set diff [expr {$aexp-$bexp}] |
|---|
| 908 | if {$diff<0} { |
|---|
| 909 | set diff [expr {-$diff}] |
|---|
| 910 | set bint [::math::bignum::lshift $bint $diff] |
|---|
| 911 | set bdelta [::math::bignum::lshift $bdelta $diff] |
|---|
| 912 | } elseif {$diff>0} { |
|---|
| 913 | set aint [::math::bignum::lshift $aint $diff] |
|---|
| 914 | set adelta [::math::bignum::lshift $adelta $diff] |
|---|
| 915 | } |
|---|
| 916 | # compute limits of the number's doubt range |
|---|
| 917 | set asupInt [::math::bignum::add $aint $adelta] |
|---|
| 918 | set ainfInt [::math::bignum::sub $aint $adelta] |
|---|
| 919 | set bsupInt [::math::bignum::add $bint $bdelta] |
|---|
| 920 | set binfInt [::math::bignum::sub $bint $bdelta] |
|---|
| 921 | # A & B are equal |
|---|
| 922 | # if their doubt ranges overlap themselves |
|---|
| 923 | if {[::math::bignum::cmp $bint $aint]==0} { |
|---|
| 924 | return 1 |
|---|
| 925 | } |
|---|
| 926 | if {[::math::bignum::cmp $bint $aint]>0} { |
|---|
| 927 | set r [expr {[::math::bignum::cmp $asupInt $binfInt]>=0}] |
|---|
| 928 | } else { |
|---|
| 929 | set r [expr {[::math::bignum::cmp $bsupInt $ainfInt]>=0}] |
|---|
| 930 | } |
|---|
| 931 | return $r |
|---|
| 932 | } |
|---|
| 933 | |
|---|
| 934 | ################################################################################ |
|---|
| 935 | # returns exp(X) where X is a BigFloat |
|---|
| 936 | ################################################################################ |
|---|
| 937 | proc ::math::bigfloat::exp {x} { |
|---|
| 938 | checkFloat x |
|---|
| 939 | foreach {dummy integer exp delta} $x {break} |
|---|
| 940 | if {$exp>=0} { |
|---|
| 941 | # shift till exp<0 with respect to the internal representation |
|---|
| 942 | # of the number |
|---|
| 943 | incr exp |
|---|
| 944 | set integer [::math::bignum::lshift $integer $exp] |
|---|
| 945 | set delta [::math::bignum::lshift $delta $exp] |
|---|
| 946 | set exp -1 |
|---|
| 947 | } |
|---|
| 948 | set precision [expr {-$exp}] |
|---|
| 949 | # add 8 bits of precision for safety |
|---|
| 950 | incr precision 8 |
|---|
| 951 | set integer [::math::bignum::lshift $integer 8] |
|---|
| 952 | set delta [::math::bignum::lshift $delta 8] |
|---|
| 953 | set Log2 [_log2 $precision] |
|---|
| 954 | foreach {new_exp integer} [::math::bignum::divqr $integer $Log2] {break} |
|---|
| 955 | # new_exp = integer part of x/log(2) |
|---|
| 956 | # integer = remainder |
|---|
| 957 | # exp(K.log(2)+r)=2^K.exp(r) |
|---|
| 958 | # so we just have to compute exp(r), r is small so |
|---|
| 959 | # the Taylor development will converge quickly |
|---|
| 960 | set delta [::math::bignum::add $delta $new_exp] |
|---|
| 961 | foreach {integer delta} [_exp $integer $precision $delta] {break} |
|---|
| 962 | set delta [::math::bignum::rshift $delta 8] |
|---|
| 963 | incr precision -8 |
|---|
| 964 | # multiply by 2^K , and take care of the sign |
|---|
| 965 | # example : X=-6.log(2)+0.01 |
|---|
| 966 | # exp(X)=exp(0.01)*2^-6 |
|---|
| 967 | if {![::math::bignum::iszero [::math::bignum::rshift [abs $new_exp] 30]]} { |
|---|
| 968 | error "floating-point overflow due to exp" |
|---|
| 969 | } |
|---|
| 970 | set new_exp [tostr $new_exp] |
|---|
| 971 | set exp [expr {$new_exp-$precision}] |
|---|
| 972 | set delta [::math::bignum::add 1 $delta] |
|---|
| 973 | return [normalize [list F [::math::bignum::rshift $integer 8] $exp $delta]] |
|---|
| 974 | } |
|---|
| 975 | |
|---|
| 976 | |
|---|
| 977 | ################################################################################ |
|---|
| 978 | # private procedure to compute exponentials |
|---|
| 979 | # using Taylor development of exp(x) : |
|---|
| 980 | # exp(x)=1+ x + x^2/2 + x^3/3! +...+x^n/n! |
|---|
| 981 | # input : integer (the mantissa) |
|---|
| 982 | # precision (the number of decimals) |
|---|
| 983 | # delta (the doubt limit, or uncertainty) |
|---|
| 984 | # returns a list : 1. the mantissa of the result |
|---|
| 985 | # 2. the doubt limit, or uncertainty |
|---|
| 986 | ################################################################################ |
|---|
| 987 | proc ::math::bigfloat::_exp {integer precision delta} { |
|---|
| 988 | set oneShifted [::math::bignum::lshift 1 $precision] |
|---|
| 989 | if {[::math::bignum::iszero $integer]} { |
|---|
| 990 | # exp(0)=1 |
|---|
| 991 | return [list $oneShifted $delta] |
|---|
| 992 | } |
|---|
| 993 | set s [::math::bignum::add $oneShifted $integer] |
|---|
| 994 | variable two |
|---|
| 995 | set d [::math::bignum::add 1 [::math::bignum::div $delta $two]] |
|---|
| 996 | set delta [::math::bignum::add $delta $delta] |
|---|
| 997 | # dt = uncertainty on x^2 |
|---|
| 998 | set dt [::math::bignum::add 1 [intMulShift $d $integer $precision]] |
|---|
| 999 | # t= x^2/2 |
|---|
| 1000 | set t [intMulShift $integer $integer $precision] |
|---|
| 1001 | set t [::math::bignum::div $t $two] |
|---|
| 1002 | set denom $two |
|---|
| 1003 | while {![::math::bignum::iszero $t]} { |
|---|
| 1004 | # the sum is called 's' |
|---|
| 1005 | set s [::math::bignum::add $s $t] |
|---|
| 1006 | set delta [::math::bignum::add $delta $dt] |
|---|
| 1007 | # we do not have to keep trace of the factorial, we just iterate divisions |
|---|
| 1008 | set denom [::math::bignum::add 1 $denom] |
|---|
| 1009 | # add delta |
|---|
| 1010 | set d [::math::bignum::add 1 [::math::bignum::div $d $denom]] |
|---|
| 1011 | set dt [::math::bignum::add $dt $d] |
|---|
| 1012 | # get x^n from x^(n-1) |
|---|
| 1013 | set t [intMulShift $integer $t $precision] |
|---|
| 1014 | # here we divide |
|---|
| 1015 | set t [::math::bignum::div $t $denom] |
|---|
| 1016 | } |
|---|
| 1017 | return [list $s $delta] |
|---|
| 1018 | } |
|---|
| 1019 | ################################################################################ |
|---|
| 1020 | # divide a BigFloat by 2 power 'n' |
|---|
| 1021 | ################################################################################ |
|---|
| 1022 | proc ::math::bigfloat::floatRShift {float {n 1}} { |
|---|
| 1023 | return [lset float 2 [expr {[lindex $float 2]-$n}]] |
|---|
| 1024 | } |
|---|
| 1025 | |
|---|
| 1026 | |
|---|
| 1027 | |
|---|
| 1028 | ################################################################################ |
|---|
| 1029 | # procedure floor : identical to [expr floor($x)] in functionality |
|---|
| 1030 | # arguments : number IN (a BigFloat) |
|---|
| 1031 | # returns : the floor value as a BigInt |
|---|
| 1032 | ################################################################################ |
|---|
| 1033 | proc ::math::bigfloat::floor {number} { |
|---|
| 1034 | variable zero |
|---|
| 1035 | checkFloat number |
|---|
| 1036 | set number [normalize $number] |
|---|
| 1037 | if {[::math::bignum::iszero $number]} { |
|---|
| 1038 | # returns the BigInt 0 |
|---|
| 1039 | return $zero |
|---|
| 1040 | } |
|---|
| 1041 | foreach {dummy integer exp delta} $number {break} |
|---|
| 1042 | if {$exp>=0} { |
|---|
| 1043 | error "not enough precision to perform rounding (floor)" |
|---|
| 1044 | } |
|---|
| 1045 | # saving the sign ... |
|---|
| 1046 | set sign [::math::bignum::sign $integer] |
|---|
| 1047 | set integer [abs $integer] |
|---|
| 1048 | # integer part |
|---|
| 1049 | set try [::math::bignum::rshift $integer [expr {-$exp}]] |
|---|
| 1050 | # floor(n.xxxx)=n |
|---|
| 1051 | if {!$sign} { |
|---|
| 1052 | return $try |
|---|
| 1053 | } |
|---|
| 1054 | # floor(-n.xxxx)=-(n+1) when xxxx!=0 |
|---|
| 1055 | if {![equal [::math::bignum::lshift $try [expr {-$exp}]] $integer]} { |
|---|
| 1056 | set try [::math::bignum::add 1 $try] |
|---|
| 1057 | } |
|---|
| 1058 | ::math::bignum::setsign try $sign |
|---|
| 1059 | return $try |
|---|
| 1060 | } |
|---|
| 1061 | |
|---|
| 1062 | |
|---|
| 1063 | ################################################################################ |
|---|
| 1064 | # returns a list formed by an integer and an exponent |
|---|
| 1065 | # x = (A +/- C) * 10 power B |
|---|
| 1066 | # return [list "F" A B C] (where F is the BigFloat tag) |
|---|
| 1067 | # A and C are BigInts, B is a raw integer |
|---|
| 1068 | # return also a BigInt when there is neither a dot, nor a 'e' exponent |
|---|
| 1069 | # |
|---|
| 1070 | # arguments : -base base integer |
|---|
| 1071 | # or integer |
|---|
| 1072 | # or float |
|---|
| 1073 | # or float trailingZeros |
|---|
| 1074 | ################################################################################ |
|---|
| 1075 | proc ::math::bigfloat::fromstr {args} { |
|---|
| 1076 | if {[set string [lindex $args 0]]=="-base"} { |
|---|
| 1077 | if {[llength $args]!=3} { |
|---|
| 1078 | error "should be : fromstr -base base number" |
|---|
| 1079 | } |
|---|
| 1080 | # converts an integer i expressed in base b with : [fromstr b i] |
|---|
| 1081 | return [::math::bignum::fromstr [lindex $args 2] [lindex $args 1]] |
|---|
| 1082 | } |
|---|
| 1083 | # trailingZeros are zeros appended to the Mantissa (it is optional) |
|---|
| 1084 | set trailingZeros 0 |
|---|
| 1085 | if {[llength $args]==2} { |
|---|
| 1086 | set trailingZeros [lindex $args 1] |
|---|
| 1087 | } |
|---|
| 1088 | if {$trailingZeros<0} { |
|---|
| 1089 | error "second argument has to be a positive integer" |
|---|
| 1090 | } |
|---|
| 1091 | # eliminate the sign problem |
|---|
| 1092 | # added on 05/08/2005 |
|---|
| 1093 | # setting '$signe' to the sign of the number |
|---|
| 1094 | set string [string trimleft $string +] |
|---|
| 1095 | if {[string index $string 0]=="-"} { |
|---|
| 1096 | set signe 1 |
|---|
| 1097 | set string2 [string range $string 1 end] |
|---|
| 1098 | } else { |
|---|
| 1099 | set signe 0 |
|---|
| 1100 | set string2 $string |
|---|
| 1101 | } |
|---|
| 1102 | # integer case (not a floating-point number) |
|---|
| 1103 | if {[string is digit $string2]} { |
|---|
| 1104 | if {$trailingZeros!=0} { |
|---|
| 1105 | error "second argument not allowed with an integer" |
|---|
| 1106 | } |
|---|
| 1107 | # we have completed converting an integer to a BigInt |
|---|
| 1108 | # please note that most math::bigfloat procs accept BigInts as arguments |
|---|
| 1109 | return [::math::bignum::fromstr $string] |
|---|
| 1110 | } |
|---|
| 1111 | set string $string2 |
|---|
| 1112 | # floating-point number : check for an exponent |
|---|
| 1113 | # scientific notation |
|---|
| 1114 | set tab [split $string e] |
|---|
| 1115 | if {[llength $tab]>2} { |
|---|
| 1116 | # there are more than one 'e' letter in the number |
|---|
| 1117 | error "syntax error in number : $string" |
|---|
| 1118 | } |
|---|
| 1119 | if {[llength $tab]==2} { |
|---|
| 1120 | set exp [lindex $tab 1] |
|---|
| 1121 | # now exp can look like +099 so you need to handle octal numbers |
|---|
| 1122 | # too bad... |
|---|
| 1123 | # find the sign (if any?) |
|---|
| 1124 | regexp {^[\+\-]?} $exp expsign |
|---|
| 1125 | # trim the number with left-side 0's |
|---|
| 1126 | set found [string length $expsign] |
|---|
| 1127 | set exp $expsign[string trimleft [string range $exp $found end] 0] |
|---|
| 1128 | set number [lindex $tab 0] |
|---|
| 1129 | } else { |
|---|
| 1130 | set exp 0 |
|---|
| 1131 | set number [lindex $tab 0] |
|---|
| 1132 | } |
|---|
| 1133 | # a floating-point number may have a dot |
|---|
| 1134 | set tab [split $number .] |
|---|
| 1135 | if {[llength $tab]>2} {error "syntax error in number : $string"} |
|---|
| 1136 | if {[llength $tab]==2} { |
|---|
| 1137 | set number [join $tab ""] |
|---|
| 1138 | # increment by the number of decimals (after the dot) |
|---|
| 1139 | incr exp -[string length [lindex $tab 1]] |
|---|
| 1140 | } |
|---|
| 1141 | # this is necessary to ensure we can call fromstr (recursively) with |
|---|
| 1142 | # the mantissa ($number) |
|---|
| 1143 | if {![string is digit $number]} { |
|---|
| 1144 | error "$number is not a number" |
|---|
| 1145 | } |
|---|
| 1146 | # take account of trailing zeros |
|---|
| 1147 | incr exp -$trailingZeros |
|---|
| 1148 | # multiply $number by 10^$trailingZeros |
|---|
| 1149 | set number [::math::bignum::mul [::math::bignum::fromstr $number]\ |
|---|
| 1150 | [tenPow $trailingZeros]] |
|---|
| 1151 | ::math::bignum::setsign number $signe |
|---|
| 1152 | # the F tags a BigFloat |
|---|
| 1153 | # a BigInt in internal representation begins by the sign |
|---|
| 1154 | # delta is 1 as a BigInt |
|---|
| 1155 | return [_fromstr $number $exp] |
|---|
| 1156 | } |
|---|
| 1157 | |
|---|
| 1158 | ################################################################################ |
|---|
| 1159 | # private procedure to transform decimal floats into binary ones |
|---|
| 1160 | # IN : |
|---|
| 1161 | # - number : a BigInt representing the Mantissa |
|---|
| 1162 | # - exp : the decimal exponent (a simple integer) |
|---|
| 1163 | # OUT : |
|---|
| 1164 | # $number * 10^$exp, as the internal binary representation of a BigFloat |
|---|
| 1165 | ################################################################################ |
|---|
| 1166 | proc ::math::bigfloat::_fromstr {number exp} { |
|---|
| 1167 | variable one |
|---|
| 1168 | variable five |
|---|
| 1169 | if {$exp==0} { |
|---|
| 1170 | return [list F $number 0 $one] |
|---|
| 1171 | } |
|---|
| 1172 | if {$exp>0} { |
|---|
| 1173 | # mul by 10^exp, and by 2^4, then normalize |
|---|
| 1174 | set number [::math::bignum::lshift $number 4] |
|---|
| 1175 | set exponent [tenPow $exp] |
|---|
| 1176 | set number [::math::bignum::mul $number $exponent] |
|---|
| 1177 | # normalize number*2^-4 +/- 2^4*10^exponent |
|---|
| 1178 | return [normalize [list F $number -4 [::math::bignum::lshift $exponent 4]]] |
|---|
| 1179 | } |
|---|
| 1180 | # now exp is negative or null |
|---|
| 1181 | # the closest power of 2 to the 'exp'th power of ten, but greater than it |
|---|
| 1182 | set binaryExp [expr {int(ceil(-$exp*log(10)/log(2)))+4}] |
|---|
| 1183 | # then compute n * 2^binaryExp / 10^(-exp) |
|---|
| 1184 | # (exp is negative) |
|---|
| 1185 | # equals n * 2^(binaryExp+exp) / 5^(-exp) |
|---|
| 1186 | set diff [expr {$binaryExp+$exp}] |
|---|
| 1187 | if {$diff<0} { |
|---|
| 1188 | error "internal error" |
|---|
| 1189 | } |
|---|
| 1190 | set fivePow [::math::bignum::pow $five [::math::bignum::fromstr [expr {-$exp}]]] |
|---|
| 1191 | set number [::math::bignum::div [::math::bignum::lshift $number \ |
|---|
| 1192 | $diff] $fivePow] |
|---|
| 1193 | set delta [::math::bignum::div [::math::bignum::lshift 1 \ |
|---|
| 1194 | $diff] $fivePow] |
|---|
| 1195 | return [normalize [list F $number [expr {-$binaryExp}] [::math::bignum::add $delta 1]]] |
|---|
| 1196 | } |
|---|
| 1197 | |
|---|
| 1198 | |
|---|
| 1199 | ################################################################################ |
|---|
| 1200 | # fromdouble : |
|---|
| 1201 | # like fromstr, but for a double scalar value |
|---|
| 1202 | # arguments : |
|---|
| 1203 | # double - the number to convert to a BigFloat |
|---|
| 1204 | # exp (optional) - the total number of digits |
|---|
| 1205 | ################################################################################ |
|---|
| 1206 | proc ::math::bigfloat::fromdouble {double {exp {}}} { |
|---|
| 1207 | set mantissa [lindex [split $double e] 0] |
|---|
| 1208 | # line added by SArnold on 05/08/2005 |
|---|
| 1209 | set mantissa [string trimleft [string map {+ "" - ""} $mantissa] 0] |
|---|
| 1210 | set precision [string length [string map {. ""} $mantissa]] |
|---|
| 1211 | if { $exp != {} && [incr exp]>$precision } { |
|---|
| 1212 | return [fromstr $double [expr {$exp-$precision}]] |
|---|
| 1213 | } else { |
|---|
| 1214 | # tests have failed : not enough precision or no exp argument |
|---|
| 1215 | return [fromstr $double] |
|---|
| 1216 | } |
|---|
| 1217 | } |
|---|
| 1218 | |
|---|
| 1219 | |
|---|
| 1220 | ################################################################################ |
|---|
| 1221 | # converts a BigInt into a BigFloat with a given decimal precision |
|---|
| 1222 | ################################################################################ |
|---|
| 1223 | proc ::math::bigfloat::int2float {int {decimals 1}} { |
|---|
| 1224 | # it seems like we need some kind of type handling |
|---|
| 1225 | # very odd in this Tcl world :-( |
|---|
| 1226 | if {![isInt $int]} { |
|---|
| 1227 | error "first argument is not an integer" |
|---|
| 1228 | } |
|---|
| 1229 | if {$decimals<1} { |
|---|
| 1230 | error "non-positive decimals number" |
|---|
| 1231 | } |
|---|
| 1232 | # the lowest number of decimals is 1, because |
|---|
| 1233 | # [tostr [fromstr 10.0]] returns 10. |
|---|
| 1234 | # (we lose 1 digit when converting back to string) |
|---|
| 1235 | set int [::math::bignum::mul $int [tenPow $decimals]] |
|---|
| 1236 | return [_fromstr $int [expr {-$decimals}]] |
|---|
| 1237 | |
|---|
| 1238 | } |
|---|
| 1239 | |
|---|
| 1240 | |
|---|
| 1241 | |
|---|
| 1242 | ################################################################################ |
|---|
| 1243 | # multiplies 'leftop' by 'rightop' and rshift the result by 'shift' |
|---|
| 1244 | ################################################################################ |
|---|
| 1245 | proc ::math::bigfloat::intMulShift {leftop rightop shift} { |
|---|
| 1246 | return [::math::bignum::rshift [::math::bignum::mul $leftop $rightop] $shift] |
|---|
| 1247 | } |
|---|
| 1248 | |
|---|
| 1249 | ################################################################################ |
|---|
| 1250 | # returns 1 if x is a BigFloat, 0 elsewhere |
|---|
| 1251 | ################################################################################ |
|---|
| 1252 | proc ::math::bigfloat::isFloat {x} { |
|---|
| 1253 | # a BigFloat is a list of : "F" mantissa exponent delta |
|---|
| 1254 | if {[llength $x]!=4} { |
|---|
| 1255 | return 0 |
|---|
| 1256 | } |
|---|
| 1257 | # the marker is the letter "F" |
|---|
| 1258 | if {[string equal [lindex $x 0] F]} { |
|---|
| 1259 | return 1 |
|---|
| 1260 | } |
|---|
| 1261 | return 0 |
|---|
| 1262 | } |
|---|
| 1263 | |
|---|
| 1264 | ################################################################################ |
|---|
| 1265 | # checks that n is a BigInt (a number create by math::bignum::fromstr) |
|---|
| 1266 | ################################################################################ |
|---|
| 1267 | proc ::math::bigfloat::isInt {n} { |
|---|
| 1268 | if {[llength $n]<3} { |
|---|
| 1269 | return 0 |
|---|
| 1270 | } |
|---|
| 1271 | if {[string equal [lindex $n 0] bignum]} { |
|---|
| 1272 | return 1 |
|---|
| 1273 | } |
|---|
| 1274 | return 0 |
|---|
| 1275 | } |
|---|
| 1276 | |
|---|
| 1277 | |
|---|
| 1278 | |
|---|
| 1279 | ################################################################################ |
|---|
| 1280 | # returns 1 if x is null, 0 otherwise |
|---|
| 1281 | ################################################################################ |
|---|
| 1282 | proc ::math::bigfloat::iszero {x} { |
|---|
| 1283 | if {[isInt $x]} { |
|---|
| 1284 | return [::math::bignum::iszero $x] |
|---|
| 1285 | } |
|---|
| 1286 | checkFloat x |
|---|
| 1287 | # now we do some interval rounding : if a number's interval englobs 0, |
|---|
| 1288 | # it is considered to be equal to zero |
|---|
| 1289 | foreach {dummy integer exp delta} $x {break} |
|---|
| 1290 | set integer [::math::bignum::abs $integer] |
|---|
| 1291 | if {[::math::bignum::cmp $delta $integer]>=0} {return 1} |
|---|
| 1292 | return 0 |
|---|
| 1293 | } |
|---|
| 1294 | |
|---|
| 1295 | |
|---|
| 1296 | ################################################################################ |
|---|
| 1297 | # compute log(X) |
|---|
| 1298 | ################################################################################ |
|---|
| 1299 | proc ::math::bigfloat::log {x} { |
|---|
| 1300 | checkFloat x |
|---|
| 1301 | foreach {dummy integer exp delta} $x {break} |
|---|
| 1302 | if {[::math::bignum::iszero $integer]||[::math::bignum::sign $integer]} { |
|---|
| 1303 | error "zero logarithm error" |
|---|
| 1304 | } |
|---|
| 1305 | if {[iszero $x]} { |
|---|
| 1306 | error "number is null" |
|---|
| 1307 | } |
|---|
| 1308 | set precision [::math::bignum::bits $integer] |
|---|
| 1309 | # uncertainty of the logarithm |
|---|
| 1310 | set delta [::math::bignum::add 1 [_logOnePlusEpsilon $delta $integer $precision]] |
|---|
| 1311 | # we got : x = 1xxxxxx (binary number with 'precision' bits) * 2^exp |
|---|
| 1312 | # we need : x = 0.1xxxxxx(binary) *2^(exp+precision) |
|---|
| 1313 | incr exp $precision |
|---|
| 1314 | foreach {integer deltaIncr} [_log $integer] {break} |
|---|
| 1315 | set delta [::math::bignum::add $delta $deltaIncr] |
|---|
| 1316 | # log(a * 2^exp)= log(a) + exp*log(2) |
|---|
| 1317 | # result = log(x) + exp*log(2) |
|---|
| 1318 | # as x<1 log(x)<0 but 'integer' (result of '_log') is the absolute value |
|---|
| 1319 | # that is why we substract $integer to log(2)*$exp |
|---|
| 1320 | set integer [::math::bignum::sub [::math::bignum::mul [_log2 $precision] \ |
|---|
| 1321 | [set exp [::math::bignum::fromstr $exp]]] $integer] |
|---|
| 1322 | set delta [::math::bignum::add $delta [abs $exp]] |
|---|
| 1323 | return [normalize [list F $integer -$precision $delta]] |
|---|
| 1324 | } |
|---|
| 1325 | |
|---|
| 1326 | |
|---|
| 1327 | ################################################################################ |
|---|
| 1328 | # compute log(1-epsNum/epsDenom)=log(1-'epsilon') |
|---|
| 1329 | # Taylor development gives -x -x^2/2 -x^3/3 -x^4/4 ... |
|---|
| 1330 | # used by 'log' command because log(x+/-epsilon)=log(x)+log(1+/-(epsilon/x)) |
|---|
| 1331 | # so the uncertainty equals abs(log(1-epsilon/x)) |
|---|
| 1332 | # ================================================ |
|---|
| 1333 | # arguments : |
|---|
| 1334 | # epsNum IN (the numerator of epsilon) |
|---|
| 1335 | # epsDenom IN (the denominator of epsilon) |
|---|
| 1336 | # precision IN (the number of bits after the dot) |
|---|
| 1337 | # |
|---|
| 1338 | # 'epsilon' = epsNum*2^-precision/epsDenom |
|---|
| 1339 | ################################################################################ |
|---|
| 1340 | proc ::math::bigfloat::_logOnePlusEpsilon {epsNum epsDenom precision} { |
|---|
| 1341 | if {[::math::bignum::cmp $epsNum $epsDenom]>=0} { |
|---|
| 1342 | error "number is null" |
|---|
| 1343 | } |
|---|
| 1344 | set s [::math::bignum::lshift $epsNum $precision] |
|---|
| 1345 | set s [::math::bignum::div $s $epsDenom] |
|---|
| 1346 | variable two |
|---|
| 1347 | set divider $two |
|---|
| 1348 | set t [::math::bignum::div [::math::bignum::mul $s $epsNum] $epsDenom] |
|---|
| 1349 | set u [::math::bignum::div $t $divider] |
|---|
| 1350 | # when u (the current term of the development) is zero, we have reached our goal |
|---|
| 1351 | # it has converged |
|---|
| 1352 | while {![::math::bignum::iszero $u]} { |
|---|
| 1353 | set s [::math::bignum::add $s $u] |
|---|
| 1354 | # divider = order of the term = 'n' |
|---|
| 1355 | set divider [::math::bignum::add 1 $divider] |
|---|
| 1356 | # t = (epsilon)^n |
|---|
| 1357 | set t [::math::bignum::div [::math::bignum::mul $t $epsNum] $epsDenom] |
|---|
| 1358 | # u = t/n = (epsilon)^n/n and is the nth term of the Taylor development |
|---|
| 1359 | set u [::math::bignum::div $t $divider] |
|---|
| 1360 | } |
|---|
| 1361 | return $s |
|---|
| 1362 | } |
|---|
| 1363 | |
|---|
| 1364 | |
|---|
| 1365 | ################################################################################ |
|---|
| 1366 | # compute log(0.xxxxxxxx) : log(1-epsilon)=-eps-eps^2/2-eps^3/3...-eps^n/n |
|---|
| 1367 | ################################################################################ |
|---|
| 1368 | proc ::math::bigfloat::_log {integer} { |
|---|
| 1369 | # the uncertainty is nbSteps with nbSteps<=nbBits |
|---|
| 1370 | # take nbSteps=nbBits (the worse case) and log(nbBits+increment)=increment |
|---|
| 1371 | set precision [::math::bignum::bits $integer] |
|---|
| 1372 | set n [expr {int(log($precision+2*log($precision)))}] |
|---|
| 1373 | set integer [::math::bignum::lshift $integer $n] |
|---|
| 1374 | incr precision $n |
|---|
| 1375 | variable three |
|---|
| 1376 | set delta $three |
|---|
| 1377 | # 1-epsilon=integer |
|---|
| 1378 | set integer [::math::bignum::sub [::math::bignum::lshift 1 $precision] $integer] |
|---|
| 1379 | set s $integer |
|---|
| 1380 | # t=x^2 |
|---|
| 1381 | set t [intMulShift $integer $integer $precision] |
|---|
| 1382 | variable two |
|---|
| 1383 | set denom $two |
|---|
| 1384 | # u=x^2/2 (second term) |
|---|
| 1385 | set u [::math::bignum::div $t $denom] |
|---|
| 1386 | while {![::math::bignum::iszero $u]} { |
|---|
| 1387 | # while the current term is not zero, it has not converged |
|---|
| 1388 | set s [::math::bignum::add $s $u] |
|---|
| 1389 | set delta [::math::bignum::add 1 $delta] |
|---|
| 1390 | # t=x^n |
|---|
| 1391 | set t [intMulShift $t $integer $precision] |
|---|
| 1392 | # denom = n (the order of the current development term) |
|---|
| 1393 | set denom [::math::bignum::add 1 $denom] |
|---|
| 1394 | # u = x^n/n (the nth term of Taylor development) |
|---|
| 1395 | set u [::math::bignum::div $t $denom] |
|---|
| 1396 | } |
|---|
| 1397 | # shift right to restore the precision |
|---|
| 1398 | set delta [::math::bignum::add 1 [::math::bignum::rshift $delta $n]] |
|---|
| 1399 | return [list [::math::bignum::rshift $s $n] $delta] |
|---|
| 1400 | } |
|---|
| 1401 | |
|---|
| 1402 | ################################################################################ |
|---|
| 1403 | # computes log(num/denom) with 'precision' bits |
|---|
| 1404 | # used to compute some analysis constants with a given accuracy |
|---|
| 1405 | # you might not call this procedure directly : it assumes 'num/denom'>4/5 |
|---|
| 1406 | # and 'num/denom'<1 |
|---|
| 1407 | ################################################################################ |
|---|
| 1408 | proc ::math::bigfloat::__log {num denom precision} { |
|---|
| 1409 | # Please Note : we here need a precision increment, in order to |
|---|
| 1410 | # keep accuracy at $precision digits. If we just hold $precision digits, |
|---|
| 1411 | # each number being precise at the last digit +/- 1, |
|---|
| 1412 | # we would lose accuracy because small uncertainties add to themselves. |
|---|
| 1413 | # Example : 0.0001 + 0.0010 = 0.0011 +/- 0.0002 |
|---|
| 1414 | # This is quite the same reason that made tcl_precision defaults to 12 : |
|---|
| 1415 | # internally, doubles are computed with 17 digits, but to keep precision |
|---|
| 1416 | # we need to limit our results to 12. |
|---|
| 1417 | # The solution : given a precision target, increment precision with a |
|---|
| 1418 | # computed value so that all digits of he result are exacts. |
|---|
| 1419 | # |
|---|
| 1420 | # p is the precision |
|---|
| 1421 | # pk is the precision increment |
|---|
| 1422 | # 2 power pk is also the maximum number of iterations |
|---|
| 1423 | # for a number close to 1 but lower than 1, |
|---|
| 1424 | # (denom-num)/denum is (in our case) lower than 1/5 |
|---|
| 1425 | # so the maximum nb of iterations is for: |
|---|
| 1426 | # 1/5*(1+1/5*(1/2+1/5*(1/3+1/5*(...)))) |
|---|
| 1427 | # the last term is 1/n*(1/5)^n |
|---|
| 1428 | # for the last term to be lower than 2^(-p-pk) |
|---|
| 1429 | # the number of iterations has to be |
|---|
| 1430 | # 2^(-pk).(1/5)^(2^pk) < 2^(-p-pk) |
|---|
| 1431 | # log(1/5).2^pk < -p |
|---|
| 1432 | # 2^pk > p/log(5) |
|---|
| 1433 | # pk > log(2)*log(p/log(5)) |
|---|
| 1434 | # now set the variable n to the precision increment i.e. pk |
|---|
| 1435 | set n [expr {int(log(2)*log($precision/log(5)))+1}] |
|---|
| 1436 | incr precision $n |
|---|
| 1437 | # log(num/denom)=log(1-(denom-num)/denom) |
|---|
| 1438 | # log(1+x) = x + x^2/2 + x^3/3 + ... + x^n/n |
|---|
| 1439 | # = x(1 + x(1/2 + x(1/3 + x(...+ x(1/(n-1) + x/n)...)))) |
|---|
| 1440 | set num [::math::bignum::fromstr [expr {$denom-$num}]] |
|---|
| 1441 | set denom [::math::bignum::fromstr $denom] |
|---|
| 1442 | # $s holds the result |
|---|
| 1443 | set s [::math::bignum::div [::math::bignum::lshift $num $precision] $denom] |
|---|
| 1444 | # $t holds x^n |
|---|
| 1445 | set t [::math::bignum::div [::math::bignum::mul $s $num] $denom] |
|---|
| 1446 | variable two |
|---|
| 1447 | set d $two |
|---|
| 1448 | # $u holds x^n/n |
|---|
| 1449 | set u [::math::bignum::div $t $d] |
|---|
| 1450 | while {![::math::bignum::iszero $u]} { |
|---|
| 1451 | set s [::math::bignum::add $s $u] |
|---|
| 1452 | # get x^n * x |
|---|
| 1453 | set t [::math::bignum::div [::math::bignum::mul $t $num] $denom] |
|---|
| 1454 | # get n+1 |
|---|
| 1455 | set d [::math::bignum::add 1 $d] |
|---|
| 1456 | # then : $u = x^(n+1)/(n+1) |
|---|
| 1457 | set u [::math::bignum::div $t $d] |
|---|
| 1458 | } |
|---|
| 1459 | # see head of the proc : we return the value with its target precision |
|---|
| 1460 | return [::math::bignum::rshift $s $n] |
|---|
| 1461 | } |
|---|
| 1462 | |
|---|
| 1463 | ################################################################################ |
|---|
| 1464 | # computes log(2) with 'precision' bits and caches it into a namespace variable |
|---|
| 1465 | ################################################################################ |
|---|
| 1466 | proc ::math::bigfloat::__logbis {precision} { |
|---|
| 1467 | set increment [expr {int(log($precision)/log(2)+1)}] |
|---|
| 1468 | incr precision $increment |
|---|
| 1469 | # ln(2)=3*ln(1-4/5)+ln(1-125/128) |
|---|
| 1470 | set a [__log 125 128 $precision] |
|---|
| 1471 | set b [__log 4 5 $precision] |
|---|
| 1472 | variable three |
|---|
| 1473 | set r [::math::bignum::add [::math::bignum::mul $b $three] $a] |
|---|
| 1474 | set ::math::bigfloat::Log2 [::math::bignum::rshift $r $increment] |
|---|
| 1475 | # formerly (when BigFloats were stored in ten radix) we had to compute log(10) |
|---|
| 1476 | # ln(10)=10.ln(1-4/5)+3*ln(1-125/128) |
|---|
| 1477 | } |
|---|
| 1478 | |
|---|
| 1479 | |
|---|
| 1480 | ################################################################################ |
|---|
| 1481 | # retrieves log(2) with 'precision' bits ; the result is cached |
|---|
| 1482 | ################################################################################ |
|---|
| 1483 | proc ::math::bigfloat::_log2 {precision} { |
|---|
| 1484 | variable Log2 |
|---|
| 1485 | if {![info exists Log2]} { |
|---|
| 1486 | __logbis $precision |
|---|
| 1487 | } else { |
|---|
| 1488 | # the constant is cached and computed again when more precision is needed |
|---|
| 1489 | set l [::math::bignum::bits $Log2] |
|---|
| 1490 | if {$precision>$l} { |
|---|
| 1491 | __logbis $precision |
|---|
| 1492 | } |
|---|
| 1493 | } |
|---|
| 1494 | # return log(2) with 'precision' bits even when the cached value has more bits |
|---|
| 1495 | return [_round $Log2 $precision] |
|---|
| 1496 | } |
|---|
| 1497 | |
|---|
| 1498 | |
|---|
| 1499 | ################################################################################ |
|---|
| 1500 | # returns A modulo B (like with fmod() math function) |
|---|
| 1501 | ################################################################################ |
|---|
| 1502 | proc ::math::bigfloat::mod {a b} { |
|---|
| 1503 | checkNumber a b |
|---|
| 1504 | if {[isInt $a] && [isInt $b]} {return [::math::bignum::mod $a $b]} |
|---|
| 1505 | if {[isInt $a]} {error "trying to divide a BigInt by a BigFloat"} |
|---|
| 1506 | set quotient [div $a $b] |
|---|
| 1507 | # examples : fmod(3,2)=1 quotient=1.5 |
|---|
| 1508 | # fmod(1,2)=1 quotient=0.5 |
|---|
| 1509 | # quotient>0 and b>0 : get floor(quotient) |
|---|
| 1510 | # fmod(-3,-2)=-1 quotient=1.5 |
|---|
| 1511 | # fmod(-1,-2)=-1 quotient=0.5 |
|---|
| 1512 | # quotient>0 and b<0 : get floor(quotient) |
|---|
| 1513 | # fmod(-3,2)=-1 quotient=-1.5 |
|---|
| 1514 | # fmod(-1,2)=-1 quotient=-0.5 |
|---|
| 1515 | # quotient<0 and b>0 : get ceil(quotient) |
|---|
| 1516 | # fmod(3,-2)=1 quotient=-1.5 |
|---|
| 1517 | # fmod(1,-2)=1 quotient=-0.5 |
|---|
| 1518 | # quotient<0 and b<0 : get ceil(quotient) |
|---|
| 1519 | if {[sign $quotient]} { |
|---|
| 1520 | set quotient [ceil $quotient] |
|---|
| 1521 | } else { |
|---|
| 1522 | set quotient [floor $quotient] |
|---|
| 1523 | } |
|---|
| 1524 | return [sub $a [mul $quotient $b]] |
|---|
| 1525 | } |
|---|
| 1526 | |
|---|
| 1527 | ################################################################################ |
|---|
| 1528 | # returns A times B |
|---|
| 1529 | ################################################################################ |
|---|
| 1530 | proc ::math::bigfloat::mul {a b} { |
|---|
| 1531 | checkNumber a b |
|---|
| 1532 | # dispatch the command to appropriate commands regarding types (BigInt & BigFloat) |
|---|
| 1533 | if {[isInt $a]} { |
|---|
| 1534 | if {[isInt $b]} { |
|---|
| 1535 | return [::math::bignum::mul $a $b] |
|---|
| 1536 | } |
|---|
| 1537 | return [mulFloatByInt $b $a] |
|---|
| 1538 | } |
|---|
| 1539 | if {[isInt $b]} {return [mulFloatByInt $a $b]} |
|---|
| 1540 | # now we are sure that 'a' and 'b' are BigFloats |
|---|
| 1541 | foreach {dummy integerA expA deltaA} $a {break} |
|---|
| 1542 | foreach {dummy integerB expB deltaB} $b {break} |
|---|
| 1543 | # 2^expA * 2^expB = 2^(expA+expB) |
|---|
| 1544 | set exp [expr {$expA+$expB}] |
|---|
| 1545 | # mantissas are multiplied |
|---|
| 1546 | set integer [::math::bignum::mul $integerA $integerB] |
|---|
| 1547 | # compute precisely the uncertainty |
|---|
| 1548 | set deltaAB [::math::bignum::mul $deltaA $deltaB] |
|---|
| 1549 | set deltaA [::math::bignum::mul [abs $integerB] $deltaA] |
|---|
| 1550 | set deltaB [::math::bignum::mul [abs $integerA] $deltaB] |
|---|
| 1551 | set delta [::math::bignum::add [::math::bignum::add $deltaA $deltaB] \ |
|---|
| 1552 | [::math::bignum::add 1 $deltaAB]] |
|---|
| 1553 | # we have to normalize because 'delta' may be too big |
|---|
| 1554 | return [normalize [list F $integer $exp $delta]] |
|---|
| 1555 | } |
|---|
| 1556 | |
|---|
| 1557 | ################################################################################ |
|---|
| 1558 | # returns A times B, where B is a positive integer |
|---|
| 1559 | ################################################################################ |
|---|
| 1560 | proc ::math::bigfloat::mulFloatByInt {a b} { |
|---|
| 1561 | checkFloat a |
|---|
| 1562 | foreach {dummy integer exp delta} $a {break} |
|---|
| 1563 | if {![isInt $b]} { |
|---|
| 1564 | error "second argument expected to be a BigInt" |
|---|
| 1565 | } |
|---|
| 1566 | # Mantissa and Delta are simply multplied by $b |
|---|
| 1567 | set integer [::math::bignum::mul $integer $b] |
|---|
| 1568 | set delta [::math::bignum::mul $delta $b] |
|---|
| 1569 | # We normalize because Delta could have seriously increased |
|---|
| 1570 | return [normalize [list F $integer $exp $delta]] |
|---|
| 1571 | } |
|---|
| 1572 | |
|---|
| 1573 | ################################################################################ |
|---|
| 1574 | # normalizes a number : Delta (accuracy of the BigFloat) |
|---|
| 1575 | # has to be limited, because the memory use increase |
|---|
| 1576 | # quickly when we do some computations, as the Mantissa and Delta |
|---|
| 1577 | # increase together |
|---|
| 1578 | # The solution : keep the size of Delta under 9 bits |
|---|
| 1579 | ################################################################################ |
|---|
| 1580 | proc ::math::bigfloat::normalize {number} { |
|---|
| 1581 | checkFloat number |
|---|
| 1582 | foreach {dummy integer exp delta} $number {break} |
|---|
| 1583 | set l [::math::bignum::bits $delta] |
|---|
| 1584 | if {$l>8} { |
|---|
| 1585 | # next line : $l holds the supplementary size (in bits) |
|---|
| 1586 | incr l -8 |
|---|
| 1587 | # now we can shift right by $l bits |
|---|
| 1588 | # always round upper the Delta |
|---|
| 1589 | set delta [::math::bignum::add 1 [::math::bignum::rshift $delta $l]] |
|---|
| 1590 | set integer [::math::bignum::rshift $integer $l] |
|---|
| 1591 | incr exp $l |
|---|
| 1592 | } |
|---|
| 1593 | return [list F $integer $exp $delta] |
|---|
| 1594 | } |
|---|
| 1595 | |
|---|
| 1596 | |
|---|
| 1597 | |
|---|
| 1598 | ################################################################################ |
|---|
| 1599 | # returns -A (the opposite) |
|---|
| 1600 | ################################################################################ |
|---|
| 1601 | proc ::math::bigfloat::opp {a} { |
|---|
| 1602 | checkNumber a |
|---|
| 1603 | if {[iszero $a]} { |
|---|
| 1604 | return $a |
|---|
| 1605 | } |
|---|
| 1606 | if {[isInt $a]} { |
|---|
| 1607 | ::math::bignum::setsign a [expr {![::math::bignum::sign $a]}] |
|---|
| 1608 | return $a |
|---|
| 1609 | } |
|---|
| 1610 | # recursive call |
|---|
| 1611 | lset a 1 [opp [lindex $a 1]] |
|---|
| 1612 | return $a |
|---|
| 1613 | } |
|---|
| 1614 | |
|---|
| 1615 | ################################################################################ |
|---|
| 1616 | # gets Pi with precision bits |
|---|
| 1617 | # after the dot (after you call [tostr] on the result) |
|---|
| 1618 | ################################################################################ |
|---|
| 1619 | proc ::math::bigfloat::pi {precision {binary 0}} { |
|---|
| 1620 | if {[llength $precision]>1} { |
|---|
| 1621 | if {[isInt $precision]} { |
|---|
| 1622 | set precision [tostr $precision] |
|---|
| 1623 | } else { |
|---|
| 1624 | error "'$precision' expected to be an integer" |
|---|
| 1625 | } |
|---|
| 1626 | } |
|---|
| 1627 | if {!$binary} { |
|---|
| 1628 | # convert decimal digit length into bit length |
|---|
| 1629 | set precision [expr {int(ceil($precision*log(10)/log(2)))}] |
|---|
| 1630 | } |
|---|
| 1631 | variable one |
|---|
| 1632 | return [list F [_pi $precision] -$precision $one] |
|---|
| 1633 | } |
|---|
| 1634 | |
|---|
| 1635 | |
|---|
| 1636 | proc ::math::bigfloat::_pi {precision} { |
|---|
| 1637 | # the constant Pi begins with 3.xxx |
|---|
| 1638 | # so we need 2 digits to store the digit '3' |
|---|
| 1639 | # and then we will have precision+2 bits in the mantissa |
|---|
| 1640 | variable _pi0 |
|---|
| 1641 | if {![info exists _pi0]} { |
|---|
| 1642 | set _pi0 [__pi $precision] |
|---|
| 1643 | } |
|---|
| 1644 | set lenPiGlobal [::math::bignum::bits $_pi0] |
|---|
| 1645 | if {$lenPiGlobal<$precision} { |
|---|
| 1646 | set _pi0 [__pi $precision] |
|---|
| 1647 | } |
|---|
| 1648 | return [::math::bignum::rshift $_pi0 [expr {[::math::bignum::bits $_pi0]-2-$precision}]] |
|---|
| 1649 | } |
|---|
| 1650 | |
|---|
| 1651 | ################################################################################ |
|---|
| 1652 | # computes an integer representing Pi in binary radix, with precision bits |
|---|
| 1653 | ################################################################################ |
|---|
| 1654 | proc ::math::bigfloat::__pi {precision} { |
|---|
| 1655 | set safetyLimit 8 |
|---|
| 1656 | # for safety and for the better precision, we do so ... |
|---|
| 1657 | incr precision $safetyLimit |
|---|
| 1658 | # formula found in the Math litterature |
|---|
| 1659 | # Pi/4 = 6.atan(1/18) + 8.atan(1/57) - 5.atan(1/239) |
|---|
| 1660 | set a [::math::bignum::mul [_atanfract [::math::bignum::fromstr 18] $precision] \ |
|---|
| 1661 | [::math::bignum::fromstr 48]] |
|---|
| 1662 | set a [::math::bignum::add $a [::math::bignum::mul \ |
|---|
| 1663 | [_atanfract [::math::bignum::fromstr 57] $precision] [::math::bignum::fromstr 32]]] |
|---|
| 1664 | set a [::math::bignum::sub $a [::math::bignum::mul \ |
|---|
| 1665 | [_atanfract [::math::bignum::fromstr 239] $precision] [::math::bignum::fromstr 20]]] |
|---|
| 1666 | return [::math::bignum::rshift $a $safetyLimit] |
|---|
| 1667 | } |
|---|
| 1668 | |
|---|
| 1669 | ################################################################################ |
|---|
| 1670 | # shift right an integer until it haves $precision bits |
|---|
| 1671 | # round at the same time |
|---|
| 1672 | ################################################################################ |
|---|
| 1673 | proc ::math::bigfloat::_round {integer precision} { |
|---|
| 1674 | set shift [expr {[::math::bignum::bits $integer]-$precision}] |
|---|
| 1675 | # $result holds the shifted integer |
|---|
| 1676 | set result [::math::bignum::rshift $integer $shift] |
|---|
| 1677 | # $shift-1 is the bit just rights the last bit of the result |
|---|
| 1678 | # Example : integer=1000010 shift=2 |
|---|
| 1679 | # => result=10000 and the tested bit is '1' |
|---|
| 1680 | if {[::math::bignum::testbit $integer [expr {$shift-1}]]} { |
|---|
| 1681 | # we round to the upper limit |
|---|
| 1682 | return [::math::bignum::add 1 $result] |
|---|
| 1683 | } |
|---|
| 1684 | return $result |
|---|
| 1685 | } |
|---|
| 1686 | |
|---|
| 1687 | ################################################################################ |
|---|
| 1688 | # returns A power B, where B is a positive integer |
|---|
| 1689 | ################################################################################ |
|---|
| 1690 | proc ::math::bigfloat::pow {a b} { |
|---|
| 1691 | checkNumber a |
|---|
| 1692 | if {![isInt $b]} { |
|---|
| 1693 | error "pow : exponent is not a positive integer" |
|---|
| 1694 | } |
|---|
| 1695 | # case where it is obvious that we should use the appropriate command |
|---|
| 1696 | # from math::bignum (added 5th March 2005) |
|---|
| 1697 | if {[isInt $a]} { |
|---|
| 1698 | return [::math::bignum::pow $a $b] |
|---|
| 1699 | } |
|---|
| 1700 | # algorithm : exponent=$b = Sum(i=0..n) b(i)2^i |
|---|
| 1701 | # $a^$b = $a^( b(0) + 2b(1) + 4b(2) + ... + 2^n*b(n) ) |
|---|
| 1702 | # we have $a^(x+y)=$a^x * $a^y |
|---|
| 1703 | # then $a^$b = Product(i=0...n) $a^(2^i*b(i)) |
|---|
| 1704 | # b(i) is boolean so $a^(2^i*b(i))= 1 when b(i)=0 and = $a^(2^i) when b(i)=1 |
|---|
| 1705 | # then $a^$b = Product(i=0...n and b(i)=1) $a^(2^i) and 1 when $b=0 |
|---|
| 1706 | variable one |
|---|
| 1707 | if {[::math::bignum::iszero $b]} {return $one} |
|---|
| 1708 | # $res holds the result |
|---|
| 1709 | set res $one |
|---|
| 1710 | while {1} { |
|---|
| 1711 | # at the beginning i=0 |
|---|
| 1712 | # $remainder is b(i) |
|---|
| 1713 | set remainder [::math::bignum::testbit $b 0] |
|---|
| 1714 | # $b 'rshift'ed by 1 bit : i=i+1 |
|---|
| 1715 | # so next time we will test bit b(i+1) |
|---|
| 1716 | set b [::math::bignum::rshift $b 1] |
|---|
| 1717 | # if b(i)=1 |
|---|
| 1718 | if {$remainder} { |
|---|
| 1719 | # mul the result by $a^(2^i) |
|---|
| 1720 | # if i=0 we multiply by $a^(2^0)=$a^1=$a |
|---|
| 1721 | set res [mul $res $a] |
|---|
| 1722 | } |
|---|
| 1723 | # no more bits at '1' in $b : $res is the result |
|---|
| 1724 | if {[::math::bignum::iszero $b]} { |
|---|
| 1725 | if {[isInt $res]} { |
|---|
| 1726 | # we cannot (and should not) normalize an integer |
|---|
| 1727 | return $res |
|---|
| 1728 | } |
|---|
| 1729 | return [normalize $res] |
|---|
| 1730 | } |
|---|
| 1731 | # i=i+1 : $a^(2^(i+1)) = square of $a^(2^i) |
|---|
| 1732 | set a [mul $a $a] |
|---|
| 1733 | } |
|---|
| 1734 | } |
|---|
| 1735 | |
|---|
| 1736 | ################################################################################ |
|---|
| 1737 | # converts angles for radians to degrees |
|---|
| 1738 | ################################################################################ |
|---|
| 1739 | proc ::math::bigfloat::rad2deg {x} { |
|---|
| 1740 | checkFloat x |
|---|
| 1741 | set xLen [expr {-[lindex $x 2]}] |
|---|
| 1742 | if {$xLen<3} { |
|---|
| 1743 | error "number too loose to convert to degrees" |
|---|
| 1744 | } |
|---|
| 1745 | set pi [pi $xLen 1] |
|---|
| 1746 | # $rad/Pi=$deg/180 |
|---|
| 1747 | # so result in deg = $radians*180/Pi |
|---|
| 1748 | return [div [mul $x [::math::bignum::fromstr 180]] $pi] |
|---|
| 1749 | } |
|---|
| 1750 | |
|---|
| 1751 | ################################################################################ |
|---|
| 1752 | # retourne la partie entière (ou 0) du nombre "number" |
|---|
| 1753 | ################################################################################ |
|---|
| 1754 | proc ::math::bigfloat::round {number} { |
|---|
| 1755 | checkFloat number |
|---|
| 1756 | #set number [normalize $number] |
|---|
| 1757 | # fetching integers (or BigInts) from the internal representation |
|---|
| 1758 | foreach {dummy integer exp delta} $number {break} |
|---|
| 1759 | if {[::math::bignum::iszero $integer]} { |
|---|
| 1760 | # returns the BigInt 0 |
|---|
| 1761 | variable zero |
|---|
| 1762 | return $zero |
|---|
| 1763 | } |
|---|
| 1764 | if {$exp>=0} { |
|---|
| 1765 | error "not enough precision to round (in round)" |
|---|
| 1766 | } |
|---|
| 1767 | set exp [expr {-$exp}] |
|---|
| 1768 | # saving the sign, ... |
|---|
| 1769 | set sign [::math::bignum::sign $integer] |
|---|
| 1770 | set integer [abs $integer] |
|---|
| 1771 | # integer part of the number |
|---|
| 1772 | set try [::math::bignum::rshift $integer $exp] |
|---|
| 1773 | # first bit after the dot |
|---|
| 1774 | set way [::math::bignum::testbit $integer [expr {$exp-1}]] |
|---|
| 1775 | # delta is shifted so it gives the integer part of 2*delta |
|---|
| 1776 | set delta [::math::bignum::rshift $delta [expr {$exp-1}]] |
|---|
| 1777 | # when delta is too big to compute rounded value ( |
|---|
| 1778 | if {![::math::bignum::iszero $delta]} { |
|---|
| 1779 | error "not enough precision to round (in round)" |
|---|
| 1780 | } |
|---|
| 1781 | if {$way} { |
|---|
| 1782 | set try [::math::bignum::add 1 $try] |
|---|
| 1783 | } |
|---|
| 1784 | # ... restore the sign now |
|---|
| 1785 | ::math::bignum::setsign try $sign |
|---|
| 1786 | return $try |
|---|
| 1787 | } |
|---|
| 1788 | |
|---|
| 1789 | ################################################################################ |
|---|
| 1790 | # round and divide by 10^n |
|---|
| 1791 | ################################################################################ |
|---|
| 1792 | proc ::math::bigfloat::roundshift {integer n} { |
|---|
| 1793 | # $exp= 10^$n |
|---|
| 1794 | set exp [tenPow $n] |
|---|
| 1795 | foreach {result remainder} [::math::bignum::divqr $integer $exp] {} |
|---|
| 1796 | # $remainder belongs to the interval [0, $exp-1] |
|---|
| 1797 | # $remainder >= $exp/2 is the rounding condition |
|---|
| 1798 | # that is better expressed in this form : |
|---|
| 1799 | # $remainder*2 >= $exp , as we are treating integers, not rationals |
|---|
| 1800 | # left shift $remainder by 1 equals to multiplying by 2 and is much faster |
|---|
| 1801 | if {[::math::bignum::cmp $exp [::math::bignum::lshift $remainder 1]]<=0} { |
|---|
| 1802 | return [::math::bignum::add 1 $result] |
|---|
| 1803 | } |
|---|
| 1804 | return $result |
|---|
| 1805 | } |
|---|
| 1806 | |
|---|
| 1807 | ################################################################################ |
|---|
| 1808 | # gets the sign of either a bignum, or a BitFloat |
|---|
| 1809 | # we keep the bignum convention : 0 for positive, 1 for negative |
|---|
| 1810 | ################################################################################ |
|---|
| 1811 | proc ::math::bigfloat::sign {n} { |
|---|
| 1812 | if {[isInt $n]} { |
|---|
| 1813 | return [::math::bignum::sign $n] |
|---|
| 1814 | } |
|---|
| 1815 | # sign of 0=0 |
|---|
| 1816 | if {[iszero $n]} {return 0} |
|---|
| 1817 | # the sign of the Mantissa, which is a BigInt |
|---|
| 1818 | return [::math::bignum::sign [lindex $n 1]] |
|---|
| 1819 | } |
|---|
| 1820 | |
|---|
| 1821 | |
|---|
| 1822 | ################################################################################ |
|---|
| 1823 | # gets sin(x) |
|---|
| 1824 | ################################################################################ |
|---|
| 1825 | proc ::math::bigfloat::sin {x} { |
|---|
| 1826 | checkFloat x |
|---|
| 1827 | foreach {dummy integer exp delta} $x {break} |
|---|
| 1828 | if {$exp>-2} { |
|---|
| 1829 | error "sin : not enough precision" |
|---|
| 1830 | } |
|---|
| 1831 | set precision [expr {-$exp}] |
|---|
| 1832 | # sin(2kPi+x)=sin(x) |
|---|
| 1833 | # $integer is now the modulo of the division of the mantissa by Pi/4 |
|---|
| 1834 | # and $n is the quotient |
|---|
| 1835 | foreach {n integer} [divPiQuarter $integer $precision] {break} |
|---|
| 1836 | set delta [::math::bignum::add $delta $n] |
|---|
| 1837 | variable four |
|---|
| 1838 | set d [::math::bignum::mod $n $four] |
|---|
| 1839 | # now integer>=0 |
|---|
| 1840 | # x = $n*Pi/4 + $integer and $n belongs to [0,3] |
|---|
| 1841 | # sin(2Pi-x)=-sin(x) |
|---|
| 1842 | # sin(Pi-x)=sin(x) |
|---|
| 1843 | # sin(Pi/2+x)=cos(x) |
|---|
| 1844 | set sign 0 |
|---|
| 1845 | switch -- [tostr $d] { |
|---|
| 1846 | 0 {set l [_sin2 $integer $precision $delta]} |
|---|
| 1847 | 1 {set l [_cos2 $integer $precision $delta]} |
|---|
| 1848 | 2 {set sign 1;set l [_sin2 $integer $precision $delta]} |
|---|
| 1849 | 3 {set sign 1;set l [_cos2 $integer $precision $delta]} |
|---|
| 1850 | default {error "internal error"} |
|---|
| 1851 | } |
|---|
| 1852 | # $l is a list : {Mantissa Precision Delta} |
|---|
| 1853 | # precision --> the opposite of the exponent |
|---|
| 1854 | # 1.000 = 1000*10^-3 so exponent=-3 and precision=3 digits |
|---|
| 1855 | lset l 1 [expr {-([lindex $l 1])}] |
|---|
| 1856 | set integer [lindex $l 0] |
|---|
| 1857 | # the sign depends on the switch statement below |
|---|
| 1858 | ::math::bignum::setsign integer $sign |
|---|
| 1859 | lset l 0 $integer |
|---|
| 1860 | # we insert the Bigfloat tag (F) and normalize the final result |
|---|
| 1861 | return [normalize [linsert $l 0 F]] |
|---|
| 1862 | } |
|---|
| 1863 | |
|---|
| 1864 | proc ::math::bigfloat::_sin2 {x precision delta} { |
|---|
| 1865 | set pi [_pi $precision] |
|---|
| 1866 | # shift right by 1 = divide by 2 |
|---|
| 1867 | # shift right by 2 = divide by 4 |
|---|
| 1868 | set pis2 [::math::bignum::rshift $pi 1] |
|---|
| 1869 | set pis4 [::math::bignum::rshift $pi 2] |
|---|
| 1870 | if {[::math::bignum::cmp $x $pis4]>=0} { |
|---|
| 1871 | # sin(Pi/2-x)=cos(x) |
|---|
| 1872 | set delta [::math::bignum::add 1 $delta] |
|---|
| 1873 | set x [::math::bignum::sub $pis2 $x] |
|---|
| 1874 | return [_cos $x $precision $delta] |
|---|
| 1875 | } |
|---|
| 1876 | return [_sin $x $precision $delta] |
|---|
| 1877 | } |
|---|
| 1878 | |
|---|
| 1879 | ################################################################################ |
|---|
| 1880 | # sin(x) with 'x' lower than Pi/4 and positive |
|---|
| 1881 | # 'x' is the Mantissa - 'delta' is Delta |
|---|
| 1882 | # 'precision' is the opposite of the exponent |
|---|
| 1883 | ################################################################################ |
|---|
| 1884 | proc ::math::bigfloat::_sin {x precision delta} { |
|---|
| 1885 | # $s holds the result |
|---|
| 1886 | set s $x |
|---|
| 1887 | # sin(x) = x - x^3/3! + x^5/5! - ... + (-1)^n*x^(2n+1)/(2n+1)! |
|---|
| 1888 | # = x * (1 - x^2/(2*3) * (1 - x^2/(4*5) * (...* (1 - x^2/(2n*(2n+1)) )...))) |
|---|
| 1889 | # The second expression allows us to compute the less we can |
|---|
| 1890 | |
|---|
| 1891 | # $double holds the uncertainty (Delta) of x^2 : 2*(Mantissa*Delta) + Delta^2 |
|---|
| 1892 | # (Mantissa+Delta)^2=Mantissa^2 + 2*Mantissa*Delta + Delta^2 |
|---|
| 1893 | set double [::math::bignum::rshift [::math::bignum::mul $x $delta] [expr {$precision-1}]] |
|---|
| 1894 | set double [::math::bignum::add [::math::bignum::add 1 $double] [::math::bignum::rshift \ |
|---|
| 1895 | [::math::bignum::mul $delta $delta] $precision]] |
|---|
| 1896 | # $x holds the Mantissa of x^2 |
|---|
| 1897 | set x [intMulShift $x $x $precision] |
|---|
| 1898 | set dt [::math::bignum::rshift [::math::bignum::add [::math::bignum::mul $x $delta] \ |
|---|
| 1899 | [::math::bignum::mul [::math::bignum::add $s $delta] $double]] $precision] |
|---|
| 1900 | set dt [::math::bignum::add 1 $dt] |
|---|
| 1901 | # $t holds $s * -(x^2) / (2n*(2n+1)) |
|---|
| 1902 | # mul by x^2 |
|---|
| 1903 | set t [intMulShift $s $x $precision] |
|---|
| 1904 | variable two |
|---|
| 1905 | set denom2 $two |
|---|
| 1906 | variable three |
|---|
| 1907 | set denom3 $three |
|---|
| 1908 | # mul by -1 (opp) and divide by 2*3 |
|---|
| 1909 | set t [opp [::math::bignum::div $t [::math::bignum::mul $denom2 $denom3]]] |
|---|
| 1910 | while {![::math::bignum::iszero $t]} { |
|---|
| 1911 | set s [::math::bignum::add $s $t] |
|---|
| 1912 | set delta [::math::bignum::add $delta $dt] |
|---|
| 1913 | # incr n => 2n --> 2n+2 and 2n+1 --> 2n+3 |
|---|
| 1914 | set denom2 [::math::bignum::add $denom2 $two] |
|---|
| 1915 | set denom3 [::math::bignum::add $denom3 $two] |
|---|
| 1916 | # $dt is the Delta corresponding to $t |
|---|
| 1917 | # $double "" "" "" "" $x (x^2) |
|---|
| 1918 | # ($t+$dt) * ($x+$double) = $t*$x + ($dt*$x + $t*$double) + $dt*$double |
|---|
| 1919 | # Mantissa^ ^--------Delta-------------------^ |
|---|
| 1920 | set dt [::math::bignum::rshift [::math::bignum::add [::math::bignum::mul $x $dt] \ |
|---|
| 1921 | [::math::bignum::mul [::math::bignum::add $t $dt] $double]] $precision] |
|---|
| 1922 | set t [intMulShift $t $x $precision] |
|---|
| 1923 | # removed 2005/08/31 by sarnold75 |
|---|
| 1924 | #set dt [::math::bignum::add $dt $double] |
|---|
| 1925 | set denom [::math::bignum::mul $denom2 $denom3] |
|---|
| 1926 | # now computing : div by -2n(2n+1) |
|---|
| 1927 | set dt [::math::bignum::add 1 [::math::bignum::div $dt $denom]] |
|---|
| 1928 | set t [opp [::math::bignum::div $t $denom]] |
|---|
| 1929 | } |
|---|
| 1930 | return [list $s $precision $delta] |
|---|
| 1931 | } |
|---|
| 1932 | |
|---|
| 1933 | |
|---|
| 1934 | ################################################################################ |
|---|
| 1935 | # procedure for extracting the square root of a BigFloat |
|---|
| 1936 | ################################################################################ |
|---|
| 1937 | proc ::math::bigfloat::sqrt {x} { |
|---|
| 1938 | variable one |
|---|
| 1939 | checkFloat x |
|---|
| 1940 | foreach {dummy integer exp delta} $x {break} |
|---|
| 1941 | # if x=0, return 0 |
|---|
| 1942 | if {[iszero $x]} { |
|---|
| 1943 | variable zero |
|---|
| 1944 | # return zero, taking care of its precision ($exp) |
|---|
| 1945 | return [list F $zero $exp $one] |
|---|
| 1946 | } |
|---|
| 1947 | # we cannot get sqrt(x) if x<0 |
|---|
| 1948 | if {[lindex $integer 0]<0} { |
|---|
| 1949 | error "negative sqrt input" |
|---|
| 1950 | } |
|---|
| 1951 | # (1+epsilon)^p = 1 + epsilon*(p-1) + epsilon^2*(p-1)*(p-2)/2! + ... |
|---|
| 1952 | # + epsilon^n*(p-1)*...*(p-n)/n! |
|---|
| 1953 | # sqrt(1 + epsilon) = (1 + epsilon)^(1/2) |
|---|
| 1954 | # = 1 - epsilon/2 - epsilon^2*3/(4*2!) - ... |
|---|
| 1955 | # - epsilon^n*(3*5*..*(2n-1))/(2^n*n!) |
|---|
| 1956 | # sqrt(1 - epsilon) = 1 + Sum(i=1..infinity) epsilon^i*(3*5*...*(2i-1))/(i!*2^i) |
|---|
| 1957 | # sqrt(n +/- delta)=sqrt(n) * sqrt(1 +/- delta/n) |
|---|
| 1958 | # so the uncertainty on sqrt(n +/- delta) equals sqrt(n) * (sqrt(1 - delta/n) - 1) |
|---|
| 1959 | # sqrt(1+eps) < sqrt(1-eps) because their logarithm compare as : |
|---|
| 1960 | # -ln(2)(1+eps) < -ln(2)(1-eps) |
|---|
| 1961 | # finally : |
|---|
| 1962 | # Delta = sqrt(n) * Sum(i=1..infinity) (delta/n)^i*(3*5*...*(2i-1))/(i!*2^i) |
|---|
| 1963 | # here we compute the second term of the product by _sqrtOnePlusEpsilon |
|---|
| 1964 | set delta [_sqrtOnePlusEpsilon $delta $integer] |
|---|
| 1965 | set intLen [::math::bignum::bits $integer] |
|---|
| 1966 | # removed 2005/08/31 by sarnold75, readded 2005/08/31 |
|---|
| 1967 | set precision $intLen |
|---|
| 1968 | # intLen + exp = number of bits before the dot |
|---|
| 1969 | #set precision [expr {-$exp}] |
|---|
| 1970 | # square root extraction |
|---|
| 1971 | set integer [::math::bignum::lshift $integer $intLen] |
|---|
| 1972 | incr exp -$intLen |
|---|
| 1973 | incr intLen $intLen |
|---|
| 1974 | # there is an exponent 2^$exp : when $exp is odd, we would need to compute sqrt(2) |
|---|
| 1975 | # so we decrement $exp, in order to get it even, and we do not need sqrt(2) anymore ! |
|---|
| 1976 | if {$exp&1} { |
|---|
| 1977 | incr exp -1 |
|---|
| 1978 | set integer [::math::bignum::lshift $integer 1] |
|---|
| 1979 | incr intLen |
|---|
| 1980 | incr precision |
|---|
| 1981 | } |
|---|
| 1982 | # using a low-level (in math::bignum) root extraction procedure |
|---|
| 1983 | set integer [::math::bignum::sqrt $integer] |
|---|
| 1984 | # delta has to be multiplied by the square root |
|---|
| 1985 | set delta [::math::bignum::rshift [::math::bignum::mul $delta $integer] $precision] |
|---|
| 1986 | # round to the ceiling the uncertainty (worst precision, the fastest to compute) |
|---|
| 1987 | set delta [::math::bignum::add 1 $delta] |
|---|
| 1988 | # we are sure that $exp is even, see above |
|---|
| 1989 | return [normalize [list F $integer [expr {$exp/2}] $delta]] |
|---|
| 1990 | } |
|---|
| 1991 | |
|---|
| 1992 | |
|---|
| 1993 | |
|---|
| 1994 | ################################################################################ |
|---|
| 1995 | # compute abs(sqrt(1-delta/integer)-1) |
|---|
| 1996 | # the returned value is a relative uncertainty |
|---|
| 1997 | ################################################################################ |
|---|
| 1998 | proc ::math::bigfloat::_sqrtOnePlusEpsilon {delta integer} { |
|---|
| 1999 | # sqrt(1-x) - 1 = x/2 + x^2*3/(2^2*2!) + x^3*3*5/(2^3*3!) + ... |
|---|
| 2000 | # = x/2 * (1 + x*3/(2*2) * ( 1 + x*5/(2*3) * |
|---|
| 2001 | # (...* (1 + x*(2n-1)/(2n) ) )...))) |
|---|
| 2002 | variable one |
|---|
| 2003 | set l [::math::bignum::bits $integer] |
|---|
| 2004 | # to compute delta/integer we have to shift left to keep the same precision level |
|---|
| 2005 | # we have a better accuracy computing (delta << lg(integer))/integer |
|---|
| 2006 | # than computing (delta/integer) << lg(integer) |
|---|
| 2007 | set x [::math::bignum::div [::math::bignum::lshift $delta $l] $integer] |
|---|
| 2008 | variable four |
|---|
| 2009 | variable two |
|---|
| 2010 | # denom holds 2n |
|---|
| 2011 | set denom $four |
|---|
| 2012 | # x/2 |
|---|
| 2013 | set result [::math::bignum::div $x $two] |
|---|
| 2014 | # x^2*3/(2!*2^2) |
|---|
| 2015 | variable three |
|---|
| 2016 | # numerator holds 2n-1 |
|---|
| 2017 | set numerator $three |
|---|
| 2018 | set temp [::math::bignum::mul $result $delta] |
|---|
| 2019 | set temp [::math::bignum::div [::math::bignum::mul $temp $numerator] $integer] |
|---|
| 2020 | set temp [::math::bignum::add 1 [::math::bignum::div $temp $denom]] |
|---|
| 2021 | while {![::math::bignum::iszero $temp]} { |
|---|
| 2022 | set result [::math::bignum::add $result $temp] |
|---|
| 2023 | set numerator [::math::bignum::add $numerator $two] |
|---|
| 2024 | set denom [::math::bignum::add $two $denom] |
|---|
| 2025 | # n = n+1 ==> num=num+2 denom=denom+2 |
|---|
| 2026 | # num=2n+1 denom=2n+2 |
|---|
| 2027 | set temp [::math::bignum::mul [::math::bignum::mul $temp $delta] $numerator] |
|---|
| 2028 | set temp [::math::bignum::div [::math::bignum::div $temp $denom] $integer] |
|---|
| 2029 | } |
|---|
| 2030 | return $result |
|---|
| 2031 | } |
|---|
| 2032 | |
|---|
| 2033 | ################################################################################ |
|---|
| 2034 | # substracts B to A |
|---|
| 2035 | ################################################################################ |
|---|
| 2036 | proc ::math::bigfloat::sub {a b} { |
|---|
| 2037 | checkNumber a b |
|---|
| 2038 | if {[isInt $a] && [isInt $b]} { |
|---|
| 2039 | # the math::bignum::sub proc is designed to work with BigInts |
|---|
| 2040 | return [::math::bignum::sub $a $b] |
|---|
| 2041 | } |
|---|
| 2042 | return [add $a [opp $b]] |
|---|
| 2043 | } |
|---|
| 2044 | |
|---|
| 2045 | ################################################################################ |
|---|
| 2046 | # tangent (trivial algorithm) |
|---|
| 2047 | ################################################################################ |
|---|
| 2048 | proc ::math::bigfloat::tan {x} { |
|---|
| 2049 | return [::math::bigfloat::div [::math::bigfloat::sin $x] [::math::bigfloat::cos $x]] |
|---|
| 2050 | } |
|---|
| 2051 | |
|---|
| 2052 | ################################################################################ |
|---|
| 2053 | # returns a power of ten |
|---|
| 2054 | ################################################################################ |
|---|
| 2055 | proc ::math::bigfloat::tenPow {n} { |
|---|
| 2056 | variable ten |
|---|
| 2057 | return [::math::bignum::pow $ten [::math::bignum::fromstr $n]] |
|---|
| 2058 | } |
|---|
| 2059 | |
|---|
| 2060 | |
|---|
| 2061 | ################################################################################ |
|---|
| 2062 | # converts a BigInt to a double (basic floating-point type) |
|---|
| 2063 | # with respect to the global variable 'tcl_precision' |
|---|
| 2064 | ################################################################################ |
|---|
| 2065 | proc ::math::bigfloat::todouble {x} { |
|---|
| 2066 | global tcl_precision |
|---|
| 2067 | checkFloat x |
|---|
| 2068 | # get the string repr of x without the '+' sign |
|---|
| 2069 | set result [string trimleft [tostr $x] +] |
|---|
| 2070 | set minus "" |
|---|
| 2071 | if {[string index $result 0]=="-"} { |
|---|
| 2072 | set minus - |
|---|
| 2073 | set result [string range $result 1 end] |
|---|
| 2074 | } |
|---|
| 2075 | set l [split $result e] |
|---|
| 2076 | set exp 0 |
|---|
| 2077 | if {[llength $l]==2} { |
|---|
| 2078 | # exp : x=Mantissa*10^Exp |
|---|
| 2079 | set exp [lindex $l 1] |
|---|
| 2080 | } |
|---|
| 2081 | # Mantissa = integerPart.fractionalPart |
|---|
| 2082 | set l [split [lindex $l 0] .] |
|---|
| 2083 | set integerPart [lindex $l 0] |
|---|
| 2084 | set integerLen [string length $integerPart] |
|---|
| 2085 | set fractionalPart [lindex $l 1] |
|---|
| 2086 | # The number of digits in Mantissa, excluding the dot and the leading zeros, of course |
|---|
| 2087 | set len [string length [set integer $integerPart$fractionalPart]] |
|---|
| 2088 | # Now Mantissa is stored in $integer |
|---|
| 2089 | if {$len>$tcl_precision} { |
|---|
| 2090 | set lenDiff [expr {$len-$tcl_precision}] |
|---|
| 2091 | # true when the number begins with a zero |
|---|
| 2092 | set zeroHead 0 |
|---|
| 2093 | if {[string index $integer 0]==0} { |
|---|
| 2094 | incr lenDiff -1 |
|---|
| 2095 | set zeroHead 1 |
|---|
| 2096 | } |
|---|
| 2097 | set integer [tostr [roundshift [::math::bignum::fromstr $integer] $lenDiff]] |
|---|
| 2098 | if {$zeroHead} { |
|---|
| 2099 | set integer 0$integer |
|---|
| 2100 | } |
|---|
| 2101 | set len [string length $integer] |
|---|
| 2102 | if {$len<$integerLen} { |
|---|
| 2103 | set exp [expr {$integerLen-$len}] |
|---|
| 2104 | # restore the true length |
|---|
| 2105 | set integerLen $len |
|---|
| 2106 | } |
|---|
| 2107 | } |
|---|
| 2108 | # number = 'sign'*'integer'*10^'exp' |
|---|
| 2109 | if {$exp==0} { |
|---|
| 2110 | # no scientific notation |
|---|
| 2111 | set exp "" |
|---|
| 2112 | } else { |
|---|
| 2113 | # scientific notation |
|---|
| 2114 | set exp e$exp |
|---|
| 2115 | } |
|---|
| 2116 | # place the dot just before the index $integerLen in the Mantissa |
|---|
| 2117 | set result [string range $integer 0 [expr {$integerLen-1}]] |
|---|
| 2118 | append result .[string range $integer $integerLen end] |
|---|
| 2119 | # join the Mantissa with the sign before and the exponent after |
|---|
| 2120 | return $minus$result$exp |
|---|
| 2121 | } |
|---|
| 2122 | |
|---|
| 2123 | ################################################################################ |
|---|
| 2124 | # converts a number stored as a list to a string in which all digits are true |
|---|
| 2125 | ################################################################################ |
|---|
| 2126 | proc ::math::bigfloat::tostr {number} { |
|---|
| 2127 | variable five |
|---|
| 2128 | if {[isInt $number]} { |
|---|
| 2129 | return [::math::bignum::tostr $number] |
|---|
| 2130 | } |
|---|
| 2131 | checkFloat number |
|---|
| 2132 | foreach {dummy integer exp delta} $number {break} |
|---|
| 2133 | if {[iszero $number]} { |
|---|
| 2134 | # we do not matter how much precision $number has : |
|---|
| 2135 | # it can be 0.0000000 or 0.0, the result is still the same : the "0" string |
|---|
| 2136 | # not anymore : 0.000 is not 0.0 ! |
|---|
| 2137 | # return 0 |
|---|
| 2138 | } |
|---|
| 2139 | if {$exp>0} { |
|---|
| 2140 | # the power of ten the closest but greater than 2^$exp |
|---|
| 2141 | # if it was lower than the power of 2, we would have more precision |
|---|
| 2142 | # than existing in the number |
|---|
| 2143 | set newExp [expr {int(ceil($exp*log(2)/log(10)))}] |
|---|
| 2144 | # 'integer' <- 'integer' * 2^exp / 10^newExp |
|---|
| 2145 | # equals 'integer' * 2^(exp-newExp) / 5^newExp |
|---|
| 2146 | set binExp [expr {$exp-$newExp}] |
|---|
| 2147 | if {$binExp<0} { |
|---|
| 2148 | # it cannot happen |
|---|
| 2149 | error "internal error" |
|---|
| 2150 | } |
|---|
| 2151 | # 5^newExp |
|---|
| 2152 | set fivePower [::math::bignum::pow $five [::math::bignum::fromstr $newExp]] |
|---|
| 2153 | # 'lshift'ing $integer by $binExp bits is like multiplying it by 2^$binExp |
|---|
| 2154 | # but much, much faster |
|---|
| 2155 | set integer [::math::bignum::div [::math::bignum::lshift $integer $binExp] \ |
|---|
| 2156 | $fivePower] |
|---|
| 2157 | # $integer is the Mantissa - Delta should follow the same operations |
|---|
| 2158 | set delta [::math::bignum::div [::math::bignum::lshift $delta $binExp] $fivePower] |
|---|
| 2159 | set exp $newExp |
|---|
| 2160 | } elseif {$exp<0} { |
|---|
| 2161 | # the power of ten the closest but lower than 2^$exp |
|---|
| 2162 | # same remark about the precision |
|---|
| 2163 | set newExp [expr {int(floor(-$exp*log(2)/log(10)))}] |
|---|
| 2164 | # 'integer' <- 'integer' * 10^newExp / 2^(-exp) |
|---|
| 2165 | # equals 'integer' * 5^(newExp) / 2^(-exp-newExp) |
|---|
| 2166 | set fivePower [::math::bignum::pow $five \ |
|---|
| 2167 | [::math::bignum::fromstr $newExp]] |
|---|
| 2168 | set binShift [expr {-$exp-$newExp}] |
|---|
| 2169 | # rshifting is like dividing by 2^$binShift, but faster as we said above about lshift |
|---|
| 2170 | set integer [::math::bignum::rshift [::math::bignum::mul $integer $fivePower] \ |
|---|
| 2171 | $binShift] |
|---|
| 2172 | set delta [::math::bignum::rshift [::math::bignum::mul $delta $fivePower] \ |
|---|
| 2173 | $binShift] |
|---|
| 2174 | set exp -$newExp |
|---|
| 2175 | } |
|---|
| 2176 | # saving the sign, to restore it into the result |
|---|
| 2177 | set sign [::math::bignum::sign $integer] |
|---|
| 2178 | set result [::math::bignum::abs $integer] |
|---|
| 2179 | # rounded 'integer' +/- 'delta' |
|---|
| 2180 | set up [::math::bignum::add $result $delta] |
|---|
| 2181 | set down [::math::bignum::sub $result $delta] |
|---|
| 2182 | if {[sign $up]^[sign $down]} { |
|---|
| 2183 | # $up>0 and $down<0 and vice-versa : then the number is considered equal to zero |
|---|
| 2184 | # delta <= 2**n (n = bits(delta)) |
|---|
| 2185 | # 2**n <= 10**exp , then |
|---|
| 2186 | # exp >= n.log(2)/log(10) |
|---|
| 2187 | # delta <= 10**(n.log(2)/log(10)) |
|---|
| 2188 | incr exp [expr {int(ceil([::math::bignum::bits $delta]*log(2)/log(10)))}] |
|---|
| 2189 | set result 0 |
|---|
| 2190 | set isZero yes |
|---|
| 2191 | } else { |
|---|
| 2192 | # iterate until the convergence of the rounding |
|---|
| 2193 | # we incr $shift until $up and $down are rounded to the same number |
|---|
| 2194 | # at each pass we lose one digit of precision, so necessarly it will success |
|---|
| 2195 | for {set shift 1} { |
|---|
| 2196 | [::math::bignum::cmp [roundshift $up $shift] [roundshift $down $shift]] |
|---|
| 2197 | } { |
|---|
| 2198 | incr shift |
|---|
| 2199 | } {} |
|---|
| 2200 | incr exp $shift |
|---|
| 2201 | set result [::math::bignum::tostr [roundshift $up $shift]] |
|---|
| 2202 | set isZero no |
|---|
| 2203 | } |
|---|
| 2204 | set l [string length $result] |
|---|
| 2205 | # now formatting the number the most nicely for having a clear reading |
|---|
| 2206 | # would'nt we allow a number being constantly displayed |
|---|
| 2207 | # as : 0.2947497845e+012 , would we ? |
|---|
| 2208 | if {$exp>0} { |
|---|
| 2209 | # we display 423*10^6 as : 4.23e+8 |
|---|
| 2210 | # Length of mantissa : $l |
|---|
| 2211 | # Increment exp by $l-1 because the first digit is placed before the dot, |
|---|
| 2212 | # the other ($l-1) digits following the dot. |
|---|
| 2213 | incr exp [incr l -1] |
|---|
| 2214 | set result [string index $result 0].[string range $result 1 end] |
|---|
| 2215 | append result "e+$exp" |
|---|
| 2216 | } elseif {$exp==0} { |
|---|
| 2217 | # it must have a dot to be a floating-point number (syntaxically speaking) |
|---|
| 2218 | append result . |
|---|
| 2219 | } else { |
|---|
| 2220 | set exp [expr {-$exp}] |
|---|
| 2221 | if {$exp < $l} { |
|---|
| 2222 | # we can display the number nicely as xxxx.yyyy* |
|---|
| 2223 | # the problem of the sign is solved finally at the bottom of the proc |
|---|
| 2224 | set n [string range $result 0 end-$exp] |
|---|
| 2225 | incr exp -1 |
|---|
| 2226 | append n .[string range $result end-$exp end] |
|---|
| 2227 | set result $n |
|---|
| 2228 | } elseif {$l==$exp} { |
|---|
| 2229 | # we avoid to use the scientific notation |
|---|
| 2230 | # because it is harder to read |
|---|
| 2231 | set result "0.$result" |
|---|
| 2232 | } else { |
|---|
| 2233 | # ... but here there is no choice, we should not represent a number |
|---|
| 2234 | # with more than one leading zero |
|---|
| 2235 | set result [string index $result 0].[string range $result 1 end]e-[expr {$exp-$l+1}] |
|---|
| 2236 | } |
|---|
| 2237 | } |
|---|
| 2238 | # restore the sign : we only put a minus on numbers that are different from zero |
|---|
| 2239 | if {$sign==1 && !$isZero} {set result "-$result"} |
|---|
| 2240 | return $result |
|---|
| 2241 | } |
|---|
| 2242 | |
|---|
| 2243 | ################################################################################ |
|---|
| 2244 | # PART IV |
|---|
| 2245 | # HYPERBOLIC FUNCTIONS |
|---|
| 2246 | ################################################################################ |
|---|
| 2247 | |
|---|
| 2248 | ################################################################################ |
|---|
| 2249 | # hyperbolic cosinus |
|---|
| 2250 | ################################################################################ |
|---|
| 2251 | proc ::math::bigfloat::cosh {x} { |
|---|
| 2252 | # cosh(x) = (exp(x)+exp(-x))/2 |
|---|
| 2253 | # dividing by 2 is done faster by 'rshift'ing |
|---|
| 2254 | return [floatRShift [add [exp $x] [exp [opp $x]]] 1] |
|---|
| 2255 | } |
|---|
| 2256 | |
|---|
| 2257 | ################################################################################ |
|---|
| 2258 | # hyperbolic sinus |
|---|
| 2259 | ################################################################################ |
|---|
| 2260 | proc ::math::bigfloat::sinh {x} { |
|---|
| 2261 | # sinh(x) = (exp(x)-exp(-x))/2 |
|---|
| 2262 | # dividing by 2 is done faster by 'rshift'ing |
|---|
| 2263 | return [floatRShift [sub [exp $x] [exp [opp $x]]] 1] |
|---|
| 2264 | } |
|---|
| 2265 | |
|---|
| 2266 | ################################################################################ |
|---|
| 2267 | # hyperbolic tangent |
|---|
| 2268 | ################################################################################ |
|---|
| 2269 | proc ::math::bigfloat::tanh {x} { |
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| 2270 | set up [exp $x] |
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| 2271 | set down [exp [opp $x]] |
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| 2272 | # tanh(x)=sinh(x)/cosh(x)= (exp(x)-exp(-x))/2/ [(exp(x)+exp(-x))/2] |
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| 2273 | # =(exp(x)-exp(-x))/(exp(x)+exp(-x)) |
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| 2274 | # =($up-$down)/($up+$down) |
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| 2275 | return [div [sub $up $down] [add $up $down]] |
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| 2276 | } |
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| 2277 | |
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| 2278 | # exporting public interface |
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| 2279 | namespace eval ::math::bigfloat { |
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| 2280 | foreach function { |
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| 2281 | add mul sub div mod pow |
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| 2282 | iszero compare equal |
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| 2283 | fromstr tostr fromdouble todouble |
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| 2284 | int2float isInt isFloat |
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| 2285 | exp log sqrt round ceil floor |
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| 2286 | sin cos tan cotan asin acos atan |
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| 2287 | cosh sinh tanh abs opp |
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| 2288 | pi deg2rad rad2deg |
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| 2289 | } { |
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| 2290 | namespace export $function |
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| 2291 | } |
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| 2292 | } |
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| 2293 | |
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| 2294 | # (AM) No "namespace import" - this should be left to the user! |
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| 2295 | #namespace import ::math::bigfloat::* |
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| 2296 | |
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| 2297 | package provide math::bigfloat 1.2.1 |
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