1 | /******************************************************************** |
2 | * * |
3 | * THIS FILE IS PART OF THE OggVorbis SOFTWARE CODEC SOURCE CODE. * |
4 | * USE, DISTRIBUTION AND REPRODUCTION OF THIS LIBRARY SOURCE IS * |
5 | * GOVERNED BY A BSD-STYLE SOURCE LICENSE INCLUDED WITH THIS SOURCE * |
6 | * IN 'COPYING'. PLEASE READ THESE TERMS BEFORE DISTRIBUTING. * |
7 | * * |
8 | * THE OggVorbis SOURCE CODE IS (C) COPYRIGHT 1994-2009 * |
9 | * by the Xiph.Org Foundation https://xiph.org/ * |
10 | * * |
11 | ******************************************************************** |
12 | |
13 | function: linear scale -> dB, Bark and Mel scales |
14 | |
15 | ********************************************************************/ |
16 | |
17 | #ifndef _V_SCALES_H_ |
18 | #define _V_SCALES_H_ |
19 | |
20 | #include <math.h> |
21 | #include "os.h" |
22 | |
23 | #ifdef _MSC_VER |
24 | /* MS Visual Studio doesn't have C99 inline keyword. */ |
25 | #define inline __inline |
26 | #endif |
27 | |
28 | /* 20log10(x) */ |
29 | #define VORBIS_IEEE_FLOAT32 1 |
30 | #ifdef VORBIS_IEEE_FLOAT32 |
31 | |
32 | static inline float unitnorm(float x){ |
33 | union { |
34 | ogg_uint32_t i; |
35 | float f; |
36 | } ix; |
37 | ix.f = x; |
38 | ix.i = (ix.i & 0x80000000U) | (0x3f800000U); |
39 | return ix.f; |
40 | } |
41 | |
42 | /* Segher was off (too high) by ~ .3 decibel. Center the conversion correctly. */ |
43 | static inline float todB(const float *x){ |
44 | union { |
45 | ogg_uint32_t i; |
46 | float f; |
47 | } ix; |
48 | ix.f = *x; |
49 | ix.i = ix.i&0x7fffffff; |
50 | return (float)(ix.i * 7.17711438e-7f -764.6161886f); |
51 | } |
52 | |
53 | #define todB_nn(x) todB(x) |
54 | |
55 | #else |
56 | |
57 | static float unitnorm(float x){ |
58 | if(x<0)return(-1.f); |
59 | return(1.f); |
60 | } |
61 | |
62 | #define todB(x) (*(x)==0?-400.f:log(*(x)**(x))*4.34294480f) |
63 | #define todB_nn(x) (*(x)==0.f?-400.f:log(*(x))*8.6858896f) |
64 | |
65 | #endif |
66 | |
67 | #define fromdB(x) (exp((x)*.11512925f)) |
68 | |
69 | /* The bark scale equations are approximations, since the original |
70 | table was somewhat hand rolled. The below are chosen to have the |
71 | best possible fit to the rolled tables, thus their somewhat odd |
72 | appearance (these are more accurate and over a longer range than |
73 | the oft-quoted bark equations found in the texts I have). The |
74 | approximations are valid from 0 - 30kHz (nyquist) or so. |
75 | |
76 | all f in Hz, z in Bark */ |
77 | |
78 | #define toBARK(n) (13.1f*atan(.00074f*(n))+2.24f*atan((n)*(n)*1.85e-8f)+1e-4f*(n)) |
79 | #define fromBARK(z) (102.f*(z)-2.f*pow(z,2.f)+.4f*pow(z,3.f)+pow(1.46f,z)-1.f) |
80 | #define toMEL(n) (log(1.f+(n)*.001f)*1442.695f) |
81 | #define fromMEL(m) (1000.f*exp((m)/1442.695f)-1000.f) |
82 | |
83 | /* Frequency to octave. We arbitrarily declare 63.5 Hz to be octave |
84 | 0.0 */ |
85 | |
86 | #define toOC(n) (log(n)*1.442695f-5.965784f) |
87 | #define fromOC(o) (exp(((o)+5.965784f)*.693147f)) |
88 | |
89 | #endif |
90 | |