Mercurial > hg > svcore
view data/model/test/TestFFTModel.h @ 1143:d649818fc249
Update JAMS output to JAMS v0.2.0. We now (for the first time?!) write actual JAMS schema-compliant output when possible, though it isn't possible for many types of plugin. The output for all tested combinations of transforms is valid JSON even where it isn't schema-compliant.
author | Chris Cannam |
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date | Wed, 04 Nov 2015 10:07:29 +0000 |
parents | 1517d4c60e88 |
children | 457a1a619c5f |
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/* -*- c-basic-offset: 4 indent-tabs-mode: nil -*- vi:set ts=8 sts=4 sw=4: */ /* Sonic Visualiser An audio file viewer and annotation editor. Centre for Digital Music, Queen Mary, University of London. This program is free software; you can redistribute it and/or modify it under the terms of the GNU General Public License as published by the Free Software Foundation; either version 2 of the License, or (at your option) any later version. See the file COPYING included with this distribution for more information. */ #ifndef TEST_FFT_MODEL_H #define TEST_FFT_MODEL_H #include "../FFTModel.h" #include "MockWaveModel.h" #include "Compares.h" #include <QObject> #include <QtTest> #include <QDir> #include <iostream> #include <complex> using namespace std; class TestFFTModel : public QObject { Q_OBJECT private: void test(DenseTimeValueModel *model, WindowType window, int windowSize, int windowIncrement, int fftSize, int columnNo, vector<vector<complex<float>>> expectedValues, int expectedWidth) { for (int ch = 0; in_range_for(expectedValues, ch); ++ch) { for (int polar = 0; polar <= 1; ++polar) { FFTModel fftm(model, ch, window, windowSize, windowIncrement, fftSize, bool(polar)); QCOMPARE(fftm.getWidth(), expectedWidth); int hs1 = fftSize/2 + 1; QCOMPARE(fftm.getHeight(), hs1); vector<float> reals(hs1 + 1, 0.f); vector<float> imags(hs1 + 1, 0.f); reals[hs1] = 999.f; // overrun guards imags[hs1] = 999.f; fftm.getValuesAt(columnNo, &reals[0], &imags[0]); for (int i = 0; i < hs1; ++i) { float eRe = expectedValues[ch][i].real(); float eIm = expectedValues[ch][i].imag(); if (reals[i] != eRe || imags[i] != eIm) { cerr << "NOTE: output is not as expected for column " << i << " in channel " << ch << " (polar store = " << polar << ")" << endl; cerr << "expected : "; for (int j = 0; j < hs1; ++j) { cerr << expectedValues[ch][j] << " "; } cerr << "\nactual : "; for (int j = 0; j < hs1; ++j) { cerr << complex<float>(reals[j], imags[j]) << " "; } cerr << endl; } COMPARE_FUZZIER_F(reals[i], eRe); COMPARE_FUZZIER_F(imags[i], eIm); } QCOMPARE(reals[hs1], 999.f); QCOMPARE(imags[hs1], 999.f); } } } private slots: // NB. FFTModel columns are centred on the sample frame, and in // particular this means column 0 is centred at sample 0 (i.e. it // contains only half the window-size worth of real samples, the // others are 0-valued from before the origin). Generally in // these tests we are padding our signal with half a window of // zeros, in order that the result for column 0 is all zeros // (rather than something with a step in it that is harder to // reason about the FFT of) and the results for subsequent columns // are those of our expected signal. void dc_simple_rect() { MockWaveModel mwm({ DC }, 16, 4); test(&mwm, RectangularWindow, 8, 8, 8, 0, { { {}, {}, {}, {}, {} } }, 4); test(&mwm, RectangularWindow, 8, 8, 8, 1, { { { 4.f, 0.f }, {}, {}, {}, {} } }, 4); test(&mwm, RectangularWindow, 8, 8, 8, 2, { { { 4.f, 0.f }, {}, {}, {}, {} } }, 4); test(&mwm, RectangularWindow, 8, 8, 8, 3, { { { }, {}, {}, {}, {} } }, 4); } void dc_simple_hann() { // The Hann window function is a simple sinusoid with period // equal to twice the window size, and it halves the DC energy MockWaveModel mwm({ DC }, 16, 4); test(&mwm, HanningWindow, 8, 8, 8, 0, { { {}, {}, {}, {}, {} } }, 4); test(&mwm, HanningWindow, 8, 8, 8, 1, { { { 4.f, 0.f }, { 2.f, 0.f }, {}, {}, {} } }, 4); test(&mwm, HanningWindow, 8, 8, 8, 2, { { { 4.f, 0.f }, { 2.f, 0.f }, {}, {}, {} } }, 4); test(&mwm, HanningWindow, 8, 8, 8, 3, { { { }, {}, {}, {}, {} } }, 4); } }; #endif