When converting a transfer function to state-space form by hand, the step of pulling out the direct path, like we did in going from Eq. (E.13) to Eq. (E.14), can be bypassed [29, p. 87].
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Figure E.2 gives the standard direct-form-II structure for a second-order IIR filter. Unlike Fig.E.1, it includes a direct path from the input to the output. The filter coefficients are all given directly by the transfer function, Eq. (E.13).
This form can be converted directly to state-space form by carefully
observing all paths from the input and state variables to the output.
For example, reaches the output through gain 2 on the right,
but also via gain
on the left and above. Therefore, its
contribution to the output is
, as
obtained in the DF-II realization with direct-path pulled out shown in
Fig.E.1. The state variable
reaches the output with
gain
, again as we obtained before. Finally, it
must also be observed that the gain of the direct path from input to
output is
.