#include "SpiralDisplay.hpp" Amuencha::SpiralDisplay::SpiralDisplay() : min_midi_note{24} , max_midi_note{72} , gain{1.f} { for (int i{0}; i < 12; i++) note_positions[i] = std::polar(.9f, half_pi - i * two_pi / 12); display_spectrum.resize(num_ID); } void Amuencha::SpiralDisplay::set_min_max_notes(int min_midi_note, int max_midi_note) { if (max_midi_note < min_midi_note) std::swap(min_midi_note, max_midi_note); this->min_midi_note = min_midi_note; this->max_midi_note = max_midi_note; display_bins.clear(); // QPainterPath empty; // base_spiral.swap(empty); // for(int id=0; id use all circles for the approx int num_octaves = (max_midi_note - min_midi_note + 11) / 12; float approx_num_pix = 0.5 * half * pi * num_octaves; int num_bins = (int)(approx_num_pix / approx_pix_bin_width); // one more bound than number of bins display_bins.resize(num_bins + 1); bin_sizes.resize(num_bins); spiral_positions.resize(num_bins + 1); spiral_r_a.resize(num_bins + 1); const float rmin = 0.1; const float rmax = 0.9; // The spiral and bounds are the same independently of how // the log space is divided into notes (e.g. 12ET) // Make it so c is on the y axis. Turn clockwise because people are // used to it (e.g. wikipedia note circle) const float theta_min = half_pi - two_pi * (min_midi_note % 12) / 12; // wrap in anti-trigonometric direction const float theta_max = theta_min - two_pi * (max_midi_note - min_midi_note) / 12; frequencies.resize(num_bins); for (int b{0}; b < num_bins; ++b) { float bratio = (float)b / (num_bins - 1.); frequencies[b] = exp2(log2_fmin + (log2_fmax - log2_fmin) * bratio); bratio = (float)(b - 0.5) / (float)(num_bins - 1.); display_bins[b] = exp2(log2_fmin + (log2_fmax - log2_fmin) * bratio); spiral_r_a[b].r = rmin + (rmax - rmin) * bratio; spiral_r_a[b].a = theta_min + (theta_max - theta_min) * bratio; spiral_positions[b] = std::polar(spiral_r_a[b].r, spiral_r_a[b].a); } // repeat one more time to avoid a second for loops float bratio = (float)(num_bins - 0.5) / (float)(num_bins - 1.); display_bins[num_bins] = exp2(log2_fmin + (log2_fmax - log2_fmin) * bratio); spiral_r_a[num_bins].r = rmin + (rmax - rmin) * bratio; spiral_r_a[num_bins].a = theta_min + (theta_max - theta_min) * bratio; spiral_positions[num_bins] = std::polar(spiral_r_a[num_bins].r, spiral_r_a[num_bins].a); for (int b{0}; b < num_bins; ++b) bin_sizes[b] = display_bins[b + 1] - display_bins[b]; for (int id{0}; id < num_ID; ++id) { display_spectrum[id].resize(num_bins); fill(display_spectrum[id].begin(), display_spectrum[id].end(), 0.); } } void Amuencha::SpiralDisplay::power_handler(int ID, const std::vector &reassigned_frequencies, const std::vector &power_spectrum) { fill(display_spectrum[ID].begin(), display_spectrum[ID].end(), 0.); // simple histogram-like sum, assuming power entries are normalized int nidx = reassigned_frequencies.size(); for (int idx{0}; idx < nidx; ++idx) { float rf = reassigned_frequencies[idx]; int ri = idx; // reassigned frequencies are never too far off the original //if (rf>display_bins[idx] && rfdisplay_bins[ri+1]) { ++ri; if (ri==nidx) break; } if (ri==nidx) continue; // ignore this frequency, it is above display max // Normalization: // - for a given frequency, the sine/window size dependency was already // handled in the frequency analyzer // - but the result should not depend on how many frequencies are provided: // increasing the resolution should not increase the power // => we need a kind of density, not just the histogram-like sum of powers // falling into each bin // - consider the energy is coming from all the original bin size & sum // - This way, using finer bins do not increase the total sum display_spectrum[ID][ri] += power_spectrum[idx] * bin_sizes[idx]; } // - Then, spread on the destination bin for getting uniform density // measure independently of the target bin size for (int idx{0}; idx < nidx; ++idx) display_spectrum[ID][idx] /= bin_sizes[idx]; }