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| author | André Nusser <andre.nusser@googlemail.com> | 2020-02-10 17:50:09 +0100 |
|---|---|---|
| committer | André Nusser <andre.nusser@googlemail.com> | 2020-02-10 17:50:09 +0100 |
| commit | c11b67d70774c81800263f9bcda2a559407f2dcf (patch) | |
| tree | 780a99f4f7b453869e6e6e31c1ee552493bb35b5 /sampling_alg_lac2020 | |
| parent | f85ddfcaf9cd2ab534f8395945a104d8d89391a0 (diff) | |
Minor fix in formula layout.
Diffstat (limited to 'sampling_alg_lac2020')
| -rw-r--r-- | sampling_alg_lac2020/LAC-20.tex | 2 |
1 files changed, 1 insertions, 1 deletions
diff --git a/sampling_alg_lac2020/LAC-20.tex b/sampling_alg_lac2020/LAC-20.tex index b143713..da7230a 100644 --- a/sampling_alg_lac2020/LAC-20.tex +++ b/sampling_alg_lac2020/LAC-20.tex @@ -419,7 +419,7 @@ Since this is not something that can be easily measured, each sample power is instead calculated as the power of the signal in an initial attack period of the audio of the main channel: \[ -power(s, n) = \sum\limits_{i=0}^n s[i]^2, +\mathit{power}(s, n) = \sum\limits_{i=0}^n s[i]^2, \] where $n$ is defined on a per instrument basis and will vary from instrument to instrument and $s[i]$ is the $i$th audio sample of the main |