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The unit impulse function

The unit impulse is very useful in the analysis of signals, linear systems , and sampling . Consider the plot of a rectangular pulse in [link] . Note the height of the pulse is 1 / τ and the width of the pulse is τ . So we can write

- x p ( t ) d t = 1

As we let τ get small, then the width of the pulse gets successively narrower and its height gets progressively higher. In the limit as τ approaches zero, we have a pulse which has infinite height, and zero width, yet its area is still one. We define the unit impulse function as

δ ( t ) lim τ 0 x p ( t )
Rectangular pulse, x p ( t ) approaches the unit impulse function, δ ( t ) , as τ approaches zero.

The area under δ ( t ) is one, and so we can write

- δ ( t - τ ) d t = 1

If we multiply the unit impulse by a constant, K , its area is now equal to that constant, i.e.

- K δ ( t - τ ) d t = K

The area of the unit impulse is usually indicated by the number shown next to the arrow as seen in [link] .

K δ ( t - τ ) .

Suppose we multiply the signal x ( t ) with a time-shifted unit impulse, δ ( t - τ ) . The product is a unit impulse, having an area of x ( τ ) . This is illustrated in [link] .

Sifting property of unit impulse, the product of the two signals, x ( t ) and δ ( t - τ ) , is x ( τ ) δ ( t - τ ) . Consequently, the area under x ( τ ) δ ( t - τ ) is x ( τ ) .

In other words,

- x ( t ) δ ( t - τ ) d t = x ( τ )

Equation [link] is called the sifting property of the unit impulse. As we will see, the sifting property of the unit impulse will be very useful.

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Source:  OpenStax, Signals, systems, and society. OpenStax CNX. Oct 07, 2012 Download for free at http://cnx.org/content/col10965/1.15
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