RMSB
RMSB - frequency band rms
Usage:
RMSB X SR DEF P1 P2 P3 REF TYP TABLE COL WIN DBREF
Inputs:
X | amplitude spectrum vector (linear!!!) |
SR | sampling rate in Hz |
DEF | type of band/frequency definition {Direct , Equal , Geometric }
|
P1,P2,P3 | band definitions parameters (depends on DEF - see table below) |
REF | Absolute , Band |Relative }
|
TYP | type of rms output values {Power , LInear , LOgarithmic }
|
TABLE | name of parameter table |
COL | 1st column for rms values in output table |
WIN | either a number (length of signal window) or a vector (length = length of signal window) |
DBREF | reference value for logarithmic output |
Outputs:
Y | band rms values |
Function:
This function computes the energy in different frequency bands of the spectrum X. The input X must be a magnitude spectrum (linear magnitudes) with an equally spaced frequency scale and a frequency range from 0 to SR/2 (e.g. an fft spectrum). The energy bands are defined by the inputs DEF and P1-P3 in the following manner:
Table 20: Frequency band definitions selected by input DEF
value of DEF | P1 | P2 | P3 | description |
0 or DIRECT
|
fmin1 ...fminn | fmax1 ...fmaxn | - | The energy in the frequency bands [fmin1,fmax1] .. [fminn,fmaxn] is computed. Overlapping bands are possible. |
1 or EQUAL
|
fmin | fmax | n | The frequency range [fmin,fmax] is split into n bands with equal bandwidth b=(fmax-fmin)/n. The boundaries of the n frequency bands are set to [fmin+i.b, fmin+(i+1).b] (with: i=0,..,n-1) |
2 or GEOMETRIC
|
fmin | fmax | n | The frequency range [fmin,fmax] is split into n bands with constant bandwidth ratio q=(fmax/fmin)1/n. The boundaries of the n frequency bands are set to [fmin.qi, fmin.q(i+1)] (with: i=0,..,n-1) |
To compute the energy in a frequency band the squared magnitudes inside the band are added. The input REF can be used to compute relative or absolute energy values.
Table 21: Compute relative or absolute rms values
value of REF | energy computation |
0 , 1 , FULL orABSOLUTE
|
The energy ei is the sum of all aj2 with frequency fj is inside the band i. |
2 , 3 , BAND orRELATIVE
|
The energy ei is computed as described above and than multiplied with k=2/SR.bi. This mode can be used to compute the energy density in a band. |
Before the computed energy values are stored in the output Y, they are converted according to the value of input TYP.
Table 22: Type of output values
value of TYP | value stored in Y (and in the table columns) |
0 or POWER
|
energy values ei as computed |
1 or LINEAR
|
ei1/2 |
2 or LOGARITHMIC
|
10.log10(ei) |
If a table (defined by TABLE and COL) is specified, the values are also stored in the columns COL to COL+n-1 of the table. In each evaluation cycle the columns of one entry are filled (starting at entry 0).