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| author | Philipp Le <philipp-le-prviat@freenet.de> | 2021-04-28 23:33:35 +0200 |
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| committer | Philipp Le <philipp-le-prviat@freenet.de> | 2021-04-28 23:33:35 +0200 |
| commit | 0fd30ff9113ef34d769ff0728e9be9cb9dad0c4f (patch) | |
| tree | 869830b6d9336e39135aa587ffe6b89c9828879d /chapter02 | |
| parent | 81dcd195ac57fd89ef79d02e467e9fa86024b416 (diff) | |
| download | dcs-lecture-notes-0fd30ff9113ef34d769ff0728e9be9cb9dad0c4f.zip dcs-lecture-notes-0fd30ff9113ef34d769ff0728e9be9cb9dad0c4f.tar.gz dcs-lecture-notes-0fd30ff9113ef34d769ff0728e9be9cb9dad0c4f.tar.bz2 | |
Typo fixes
Diffstat (limited to 'chapter02')
| -rw-r--r-- | chapter02/content_ch02.tex | 2 |
1 files changed, 1 insertions, 1 deletions
diff --git a/chapter02/content_ch02.tex b/chapter02/content_ch02.tex index dbcbf62..9996706 100644 --- a/chapter02/content_ch02.tex +++ b/chapter02/content_ch02.tex @@ -1105,7 +1105,7 @@ This equation resembles \eqref{eq:ch02:def_inv_fourier_transform}. An example for the duality is the convolution in time-domain. Due to the duality, it becomes a multiplication in the frequency domain. \begin{equation} - \mathcal{F}\left\{ \underline{f}(t) * \underline{f}(t) \right\} = \mathcal{F}\left\{\underline{f}(t)\right\} \cdot \mathcal{F}\left\{\underline{g}(t)\right\} + \mathcal{F}\left\{ \underline{f}(t) * \underline{g}(t) \right\} = \mathcal{F}\left\{\underline{f}(t)\right\} \cdot \mathcal{F}\left\{\underline{g}(t)\right\} \label{eq:ch02:op_conv} \end{equation} |