Z Transform of Difference Equations
Since z transforming the convolution representation for digital filters was
so fruitful, let's apply it now to the general difference equation,
Eq.(5.1). To do this requires two properties of the z transform,
linearity (easy to show) and the shift theorem
(derived in §6.3 above). Using these two properties, we
can write down the z transform of any difference equation by inspection, as
we now show. In
§6.8.2, we'll show how to invert by inspection as well.
Repeating the general difference equation for LTI filters, we have
(from Eq.(5.1))
Let's take the z transform of both sides, denoting the transform by
. Because
is a linear operator,
it may be distributed through the terms on the right-hand side as
follows:7.3
where we used the superposition and scaling properties of linearity
given on page
, followed by use of the shift
theorem, in that order. The terms in
may be grouped together
on the left-hand side to get

Factoring out the common terms and
gives
![$\displaystyle Y(z)\left[1 + a_1 z^{-1}+ \cdots + a_N z^{-N}\right]
= X(z)\left[b_0 + b_1 z^{-1}+ \cdots + b_M z^{-M}\right].
$](http://www.dsprelated.com/josimages_new/filters/img669.png)

the z transform of the difference equation yields



Thus, taking the z transform of the general difference equation led to a new formula for the transfer function in terms of the difference equation coefficients. (Now the minus signs for the feedback coefficients in the difference equation Eq.

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Factored Form
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Z Transform of Convolution