Mercurial > hg > camir-aes2014
diff 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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--- /dev/null Thu Jan 01 00:00:00 1970 +0000 +++ b/toolboxes/MIRtoolbox1.3.2/MIRToolbox/mirattacktime.m Tue Feb 10 15:05:51 2015 +0000 @@ -0,0 +1,53 @@ +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'; \ No newline at end of file