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Finite-precision effects are much more of a concern with IIR filters than with FIR filters, since the effects are more difficult to analyze andminimize, coefficient quantization errors can cause the filters to become unstable, and disastrous things like large-scale limit cycles can occur.
Suppose there are several quantization points in an IIR filter structure. By our simplifying assumptions about quantization errorand Parseval's theorem, the quantization noise variance at the output of the filter from the th quantizer is
A general approach to find is to write state equations for the equivalent structure as seen by , and to determine the transfer function according to .
The above figure illustrates the quantization points in a typical implementation of a Direct-Form II IIRsecond-order section. What is the total variance of the output error due to all of thequantizers in the system?
By making the assumption that each represents a noise source that is white, independent of the other sources, and additive, the variance at the output is the sum of the variances atthe output due to each noise source: The variance due to each noise source at the outputcan be determined from ; note that by our assumptions, and is the transfer function from the noise source to the output .
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