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Non-recirculating filter, second form

Sometimes we will need a variant of the filter above, shown in Figure 8.10, called the elementary non-recirculating filter, second form. Instead of multiplying the delay output by $Q$ we multiply the direct signal by its complex conjugate $\overline{Q}$. (If

\begin{displaymath}
A = a+bi = r \cdot (\cos(\alpha) + i \sin(\alpha))
\end{displaymath}

is any complex number, its complex conjugate is defined as:

\begin{displaymath}
\overline{A} = a-bi = r \cdot (\cos(\alpha) - i \sin(\alpha))
\end{displaymath}

Graphically this flips the entire complex plane across the real axis.) The transfer function of the new filter is

\begin{displaymath}
H(Z) = \overline{Q} - {Z^{-1}}
\end{displaymath}

This gives rise to the same frequency response as before since

\begin{displaymath}
\vert\overline{Q} - {Z^{-1}}\vert = \vert Q - \overline{Z^{-1}}\vert = \vert Q- Z\vert
\end{displaymath}

Here we use the fact that $\overline{Z} = {Z^{-1}}$, for any unit complex number $Z$, as can be verified by writing out $Z\overline{Z}$ in either polar or rectangular form.

Although the two forms of the elementary non-recirculating filter have the same frequency response, their phase responses are different; this will occasionally lead us to prefer the second form.

Figure 8.10: The elementary non-recirculating filter, second form.
\begin{figure}\psfig{file=figs/fig08.10.ps}\end{figure}


next up previous contents index
Next: Elementary recirculating filter Up: Elementary filters Previous: Elementary non-recirculating filter   Contents   Index
Miller Puckette 2006-09-05