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Articles - CCRMA - Stanford University

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Tonal Correction Filter<br />

Let hk(n) = impulse response of kth system pole. Then<br />

∞<br />

Ek = |hk(n)| 2 = total energy<br />

n=0<br />

Thus, total energy is proportional to decay time.<br />

To compensate, Jot proposes a tonal correction filter<br />

E(z) for the late reverb (not the direct signal).<br />

First-order case:<br />

where<br />

and<br />

as before.<br />

E(z) = 1−bz−1<br />

1−b<br />

b = 1−α<br />

1+α<br />

α ∆ = t60(π/T)<br />

t60(0)<br />

41

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