| /******************************************************************** |
| * * |
| * THIS FILE IS PART OF THE OggVorbis SOFTWARE CODEC SOURCE CODE. * |
| * USE, DISTRIBUTION AND REPRODUCTION OF THIS LIBRARY SOURCE IS * |
| * GOVERNED BY A BSD-STYLE SOURCE LICENSE INCLUDED WITH THIS SOURCE * |
| * IN 'COPYING'. PLEASE READ THESE TERMS BEFORE DISTRIBUTING. * |
| * * |
| * THE OggVorbis SOURCE CODE IS (C) COPYRIGHT 1994-2009 * |
| * by the Xiph.Org Foundation http://www.xiph.org/ * |
| * * |
| ******************************************************************** |
| |
| function: linear scale -> dB, Bark and Mel scales |
| last mod: $Id: scales.h 16227 2009-07-08 06:58:46Z xiphmont $ |
| |
| ********************************************************************/ |
| |
| #ifndef _V_SCALES_H_ |
| #define _V_SCALES_H_ |
| |
| #include <math.h> |
| #include "os.h" |
| |
| #ifdef _MSC_VER |
| /* MS Visual Studio doesn't have C99 inline keyword. */ |
| #define inline __inline |
| #endif |
| |
| /* 20log10(x) */ |
| #define VORBIS_IEEE_FLOAT32 1 |
| #ifdef VORBIS_IEEE_FLOAT32 |
| |
| static inline float unitnorm(float x){ |
| union { |
| ogg_uint32_t i; |
| float f; |
| } ix; |
| ix.f = x; |
| ix.i = (ix.i & 0x80000000U) | (0x3f800000U); |
| return ix.f; |
| } |
| |
| /* Segher was off (too high) by ~ .3 decibel. Center the conversion correctly. */ |
| static inline float todB(const float *x){ |
| union { |
| ogg_uint32_t i; |
| float f; |
| } ix; |
| ix.f = *x; |
| ix.i = ix.i&0x7fffffff; |
| return (float)(ix.i * 7.17711438e-7f -764.6161886f); |
| } |
| |
| #define todB_nn(x) todB(x) |
| |
| #else |
| |
| static float unitnorm(float x){ |
| if(x<0)return(-1.f); |
| return(1.f); |
| } |
| |
| #define todB(x) (*(x)==0?-400.f:log(*(x)**(x))*4.34294480f) |
| #define todB_nn(x) (*(x)==0.f?-400.f:log(*(x))*8.6858896f) |
| |
| #endif |
| |
| #define fromdB(x) (exp((x)*.11512925f)) |
| |
| /* The bark scale equations are approximations, since the original |
| table was somewhat hand rolled. The below are chosen to have the |
| best possible fit to the rolled tables, thus their somewhat odd |
| appearance (these are more accurate and over a longer range than |
| the oft-quoted bark equations found in the texts I have). The |
| approximations are valid from 0 - 30kHz (nyquist) or so. |
| |
| all f in Hz, z in Bark */ |
| |
| #define toBARK(n) (13.1f*atan(.00074f*(n))+2.24f*atan((n)*(n)*1.85e-8f)+1e-4f*(n)) |
| #define fromBARK(z) (102.f*(z)-2.f*pow(z,2.f)+.4f*pow(z,3.f)+pow(1.46f,z)-1.f) |
| #define toMEL(n) (log(1.f+(n)*.001f)*1442.695f) |
| #define fromMEL(m) (1000.f*exp((m)/1442.695f)-1000.f) |
| |
| /* Frequency to octave. We arbitrarily declare 63.5 Hz to be octave |
| 0.0 */ |
| |
| #define toOC(n) (log(n)*1.442695f-5.965784f) |
| #define fromOC(o) (exp(((o)+5.965784f)*.693147f)) |
| |
| #endif |