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The Continuous-Time Impulse
An impulse in continuous time must have ``zero width''
and unit area under it. One definition is
![$\displaystyle \delta(t) \isdef \lim_{\Delta \to 0} \left\{\begin{array}{ll} \fr...
...eq t\leq \Delta \\ [5pt] 0, & \hbox{otherwise}. \\ \end{array} \right. \protect$](http://www.dsprelated.com/josimages/mdft/img1689.png) |
(B.3) |
An impulse can be similarly defined as the limit of
any
integrable pulse shape
which maintains unit area and approaches zero width at time 0. As a
result, the impulse under every definition has the so-called
sifting property under integration,
 |
(B.4) |
provided

is continuous at

. This is often taken as the
defining property of an impulse, allowing it to be defined in terms
of non-vanishing function limits such as
(Note, incidentally, that

is in

but not

.)
An impulse is not a function in the usual sense, so it is called
instead a distribution or generalized function
[10,36]. (It is still commonly called a ``delta function'',
however, despite the misnomer.)
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Existence of the Fourier TransformNext:
Fourier Series (FS) and Relation to DFT
written by Julius Orion Smith III
Julius Smith's background is in electrical engineering (BS Rice 1975, PhD Stanford 1983). He is presently Professor of Music and Associate Professor (by courtesy) of Electrical Engineering at
Stanford's Center for Computer Research in Music and Acoustics (CCRMA), teaching courses and pursuing research related to signal processing applied to music and audio systems. See
http://ccrma.stanford.edu/~jos/ for details.