1 | /******************************************************************** |
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2 | * * |
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3 | * THIS FILE IS PART OF THE OggVorbis SOFTWARE CODEC SOURCE CODE. * |
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4 | * USE, DISTRIBUTION AND REPRODUCTION OF THIS LIBRARY SOURCE IS * |
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5 | * GOVERNED BY A BSD-STYLE SOURCE LICENSE INCLUDED WITH THIS SOURCE * |
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6 | * IN 'COPYING'. PLEASE READ THESE TERMS BEFORE DISTRIBUTING. * |
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7 | * * |
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8 | * THE OggVorbis SOURCE CODE IS (C) COPYRIGHT 1994-2007 * |
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9 | * by the Xiph.Org Foundation http://www.xiph.org/ * |
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10 | * * |
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11 | ******************************************************************** |
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12 | |
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13 | function: linear scale -> dB, Bark and Mel scales |
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14 | last mod: $Id: scales.h 13293 2007-07-24 00:09:47Z xiphmont $ |
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15 | |
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16 | ********************************************************************/ |
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17 | |
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18 | #ifndef _V_SCALES_H_ |
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19 | #define _V_SCALES_H_ |
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20 | |
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21 | #include <math.h> |
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22 | #include "os.h" |
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23 | |
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24 | /* 20log10(x) */ |
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25 | #define VORBIS_IEEE_FLOAT32 1 |
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26 | #ifdef VORBIS_IEEE_FLOAT32 |
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27 | |
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28 | static float unitnorm(float x){ |
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29 | union { |
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30 | ogg_uint32_t i; |
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31 | float f; |
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32 | } ix; |
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33 | ix.f = x; |
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34 | ix.i = (ix.i & 0x80000000U) | (0x3f800000U); |
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35 | return ix.f; |
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36 | } |
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37 | |
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38 | /* Segher was off (too high) by ~ .3 decibel. Center the conversion correctly. */ |
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39 | static float todB(const float *x){ |
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40 | union { |
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41 | ogg_uint32_t i; |
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42 | float f; |
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43 | } ix; |
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44 | ix.f = *x; |
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45 | ix.i = ix.i&0x7fffffff; |
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46 | return (float)(ix.i * 7.17711438e-7f -764.6161886f); |
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47 | } |
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48 | |
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49 | #define todB_nn(x) todB(x) |
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50 | |
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51 | #else |
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52 | |
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53 | static float unitnorm(float x){ |
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54 | if(x<0)return(-1.f); |
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55 | return(1.f); |
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56 | } |
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57 | |
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58 | #define todB(x) (*(x)==0?-400.f:log(*(x)**(x))*4.34294480f) |
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59 | #define todB_nn(x) (*(x)==0.f?-400.f:log(*(x))*8.6858896f) |
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60 | |
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61 | #endif |
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62 | |
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63 | #define fromdB(x) (exp((x)*.11512925f)) |
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64 | |
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65 | /* The bark scale equations are approximations, since the original |
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66 | table was somewhat hand rolled. The below are chosen to have the |
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67 | best possible fit to the rolled tables, thus their somewhat odd |
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68 | appearance (these are more accurate and over a longer range than |
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69 | the oft-quoted bark equations found in the texts I have). The |
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70 | approximations are valid from 0 - 30kHz (nyquist) or so. |
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71 | |
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72 | all f in Hz, z in Bark */ |
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73 | |
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74 | #define toBARK(n) (13.1f*atan(.00074f*(n))+2.24f*atan((n)*(n)*1.85e-8f)+1e-4f*(n)) |
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75 | #define fromBARK(z) (102.f*(z)-2.f*pow(z,2.f)+.4f*pow(z,3.f)+pow(1.46f,z)-1.f) |
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76 | #define toMEL(n) (log(1.f+(n)*.001f)*1442.695f) |
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77 | #define fromMEL(m) (1000.f*exp((m)/1442.695f)-1000.f) |
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78 | |
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79 | /* Frequency to octave. We arbitrarily declare 63.5 Hz to be octave |
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80 | 0.0 */ |
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81 | |
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82 | #define toOC(n) (log(n)*1.442695f-5.965784f) |
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83 | #define fromOC(o) (exp(((o)+5.965784f)*.693147f)) |
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84 | |
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85 | #endif |
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86 | |
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