Mercurial > hg > camir-aes2014
view toolboxes/MIRtoolbox1.3.2/MIRToolbox/mirattacktime.m @ 0:e9a9cd732c1e tip
first hg version after svn
author | wolffd |
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date | Tue, 10 Feb 2015 15:05:51 +0000 |
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function varargout = mirattacktime(orig,varargin) % a = mirattacktime(x) returns the duration (in s.) of each note attack. % Optional arguments: % a = mirattacktime(x,l) specifies whether to consider the duration in s. % (l='Lin') or the logarithm of that duration (l='Log') following the % approach proposed in Krimphoff et al. (1994). % Default value: l='Lin'. % % Krimphoff, J., McAdams, S. & Winsberg, S. (1994), Caractérisation du % timbre des sons complexes. II : Analyses acoustiques et quantification % psychophysique. Journal de Physique, 4(C5), 625-628. scale.type = 'String'; scale.choice = {'Lin','Log'}; scale.default = 'Lin'; option.scale = scale; specif.option = option; varargout = mirfunction(@mirattacktime,orig,varargin,nargout,specif,@init,@main); function [o type] = init(x,option) o = mironsets(x,'Attack'); type = mirtype(x); function at = main(o,option,postoption) if iscell(o) o = o{1}; end po = get(o,'PeakPosUnit'); pa = get(o,'AttackPosUnit'); at = mircompute(@algo,po,pa,option.scale); fp = mircompute(@frampose,pa,po); at = mirscalar(o,'Data',at,'FramePos',fp,'Title','Attack Time'); at = {at,o}; function fp = frampose(pa,po) pa = sort(pa{1}); po = sort(po{1}); fp = [pa';po']; function at = algo(po,pa,sc) po = sort(po{1}); pa = sort(pa{1}); at = po-pa; if strcmpi(sc,'Log') at = log10(at); end at = at';