This C code performs an interpolation of band gains and...

August 26, 2025 at 08:36 AM

static void interp_band_gain(float *g, const float *bandE) { int i,j; memset(g, 0, FREQ_SIZE); for (i=1;i<NB_BANDS;i++) { int band_size; band_size = eband20ms[i+1]-eband20ms[i]; for (j=0;j<band_size;j++) { float frac = (float)j/band_size; g[eband20ms[i] + j] = (1-frac)*bandE[i-1] + frac*bandE[i]; } } for (j=0;j<eband20ms[1];j++) g[j] = bandE[0]; for (j=eband20ms[NB_BANDS];j<eband20ms[NB_BANDS+1];j++) g[j] = bandE[NB_BANDS-1]; }

This C code performs an interpolation of band gains and applies it to the array g based on the input energy in bands (bandE). Here's a step-by-step explanation:

  1. Parameter Description:

    • g: A floating-point array where the interpolated gain values will be stored.
    • bandE: A constant floating-point input array containing the energy levels for bands.
    • eband20ms: Likely an external (global) constant integer array defining the start indices of each band.
    • NB_BANDS: Likely an external (global) integer defining the total number of bands.
    • FREQ_SIZE: Likely an external (global) constant defining the size of the g array.
  2. Initialization:

    memset(g, 0, FREQ_SIZE);
    

    The g array is initialized to zeros for all FREQ_SIZE elements.

  3. Main Interpolation Loop:

    for (i = 1; i < NB_BANDS; i++) {
        ...
    }
    
    • For each band, starting at the second band (i = 1), the code calculates how to blend energy values between the i-1-th band and the i-th band.
    • The size of the current band, band_size, is determined by subtracting the starting index of the current band (eband20ms[i]) from the next band index (eband20ms[i+1]).
    • For each position within that band, the code computes a linear interpolation between the energy values bandE[i-1] and bandE[i].
      • frac is a fractional value (from 0 to 1) based on the position within the band.
      • The interpolated energy at each position is calculated as: [ g[\text{position}] = (1 - \text{frac}) \cdot \text{bandE[i-1]} + \text{frac} \cdot \text{bandE[i]} ]
  4. Edge Cases (Handling First and Last Bands):

    • For frequencies before the first band (eband20ms[1]), the gain values in g are set to the first energy value in bandE:
      for (j = 0; j < eband20ms[1]; j++) g[j] = bandE[0];
      
    • For frequencies after the last band's end (eband20ms[NB_BANDS]), the gain values in g are set to the last energy value in bandE:
      for (j = eband20ms[NB_BANDS]; j < eband20ms[NB_BANDS+1]; j++) g[j] = bandE[NB_BANDS-1];
      
  5. Purpose: The function smoothly interpolates gain values across frequency bands defined by eband20ms based on the input bandE. This ensures a gradual transition of gains between bands, avoiding abrupt changes. Additionally, it handles edge cases by setting the gain in untouched regions to the nearest energy boundaries (bandE[0] or bandE[NB_BANDS-1]).

  6. Usage: This kind of code is common in applications like audio or speech processing, where frequency bands are divided and energy values (e.g., spectral energies) need to be smoothed across bands for further processing or synthesis.

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