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Details
Inventors: Van Duyne, Scott A.;
Assignee: Stanford University (Stanford, CA)
Primary Examiner: Mai; Tan V.
Assistant Examiner:
Attorney, Agent or Firm: Lumen Intellectual Property Services

A coupled mode digital filter which simulates any number of arbitrarily tuned modes coupled together so as to share the same loss element at a junction loaded by an arbitrary impedance function is formed from the combination of one first order allpass filter ?28! and one unit delay ?30! per mode and one shared coupling filter?36!. This coupled mode digital filter may be excited by a stored or generated excitation signal, or a filtered excitation signal, to produce inharmonic percussive sounds and musically interesting two-stage and beating decay envelopes resulting from natural coupling of modes of near frequencies

DETAILED DESCRIPTION A block diagram of a preferred embodiment of the invention is shown in FIG.
5.
It includes a collection of m first order allpass (FOAP) filters 28(1), 28(2), .
.
.
, 28(m) and a collection of m corresponding unit delay elements 30(1), 30(2), .
.
.
, 30(m).
As shown in FIG.
5, the FOAP and unit delay pairs are arranged with corresponding adders 31(1), 31(2), .
.
.
, 31(m) to form a collection of m negative feedback loops 32(1), 32(2), .
.
.
, 32(m) corresponding to the m modes being simulated.
As described in detail below, each of these loops forms a lossless oscillator having a characteristic resonant frequency, and is effectively a novel implementation of a second order filter.
In the preferred embodiment, the mode oscillator loops 32(1), 32(2), .
.
.
, 32(m) are initially excited by a common excitation input signal entering the circuit at an adder 33.
Signals from loops 32(1), 32(2), .
.
.
, 32(m) are then coupled in an adder 34 which sends a coupled mode signal out of the circuit.
The coupled mode signal is also sent to a coupling filter 36 which controls the decay envelope for the synthesized sound.
The attenuated signal then passes through adder 33 and is fed back into the bank of m mode oscillator loops.
FOAP filters 28 have transfer functions of the form: ##EQU2## These m filters may be computed with a set of m corresponding difference equations, for example: ##EQU3## where n is the time sample index, y.
sub.
1 (n), y.
sub.
2 (n), .
.
.
, y.
sub.
m (n) are the respective output signals of filters 28(1), 28(2), .
.
.
, 28(m), and x.
sub.
1 (n), x.
sub.
2 (n), .
.
.
, x.
sub.
m (n) are the respective input signals of the filters.
The FOAP coefficients, a.
sub.
1, a.
sub.
2, .
.
.
, a.
sub.
m, determine the tuning of the m modal frequencies of the coupled mode digital filter.
In the non-decaying case, where the coupling filter will have a gain of 0 for all frequencies, the correct tuning of the resonant modes may be determined as follows.
Consider a single negative feedback loop containing a FOAP filter with transfer function ##EQU4## and a delay element with transfer function D(z)=z



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