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Impulse-Response and CAD-Model-Based Physical Modeling in FAUST

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HAL Id: hal-01526607

https://hal-mines-paristech.archives-ouvertes.fr/hal-01526607v2

Submitted on 7 Feb 2018

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Impulse-Response and CAD-Model-Based Physical Modeling in FAUST

Pierre-Amaury Grumiaux, Romain Michon, Emilio Jesús Gallego Arias, Pierre Jouvelot

To cite this version:

Pierre-Amaury Grumiaux, Romain Michon, Emilio Jesús Gallego Arias, Pierre Jouvelot. Impulse-Response and CAD-Model-Based Physical Modeling in FAUST. Linux Audio Conférence 2017, May 2017, Saint Etienne, France. 2017. �hal-01526607v2�

(2)

I

MPULSE

-R

ESPONSE AND

CAD-M

ODEL

-B

ASED

P

HYSICAL

M

ODELING

IN

F

AUST

P.-A. G

RUMIAUX

, R. M

ICHON

, E. G

ALLEGO

A

RIAS AND

P. J

OUVELOT

pierreamaury.grumiaux@gmail.com, rmichon@ccrma.stanford.edu, {emilio.gallego_arias,pierre.jouvelot}@mines-paristech.fr

C

ONTEXT

The FAUST programming language [4] has proven to be well suited to

implement physical models of music instruments using waveguides and model synthesis [1][2][3]. We developed two tools allowing to easily generate FAUST modal physical models:

1. ir2dsp.py takes the audio file of an impulse response and con-verts it into a FAUST program implementing the corresponding

modal physical model;

2. mesh2dsp.py outputs the same type of model from a .stl file specifying a 3D object.

F

AUST

M

ODAL

P

HYSICAL

M

ODEL

Linear percussion instruments can be implemented using banks of resonant bandpass filters [2]. Each filter implements one mode of the system and is configured with 3 parameters : the frequency of the mode, its gain and its resonance duration (t60). Its FAUST version,

modeFilter below, uses a biquad filter (tf2) and computes its poles and zeroes for a given frequency and t60.

modeFilter(f,t60) = tf2(b0,b1,b2,a1,a2) with{ b0 = 1; b1 = 0; b2 = -1; w = 2*PI*f/SR; r = pow(0.001,1/float(t60*SR)); a1 = -2*r*cos(w); a2 = rˆ2; }; mode(f,t60,gain) = modeFilter(f,t60)*gain;

Modal physical models are implemented using multiple parallel (par in FAUST) instances of mode calls. The FAUST-generated block

diagram corresponding to such an implementation is presented be-low (we used arbitrary parameters here).

mode(100)(0.9f)(0.9f)

mode(200)(0.8f)(0.9f)

mode(300)(0.6f)(0.5f)

mode(400)(0.5f)(0.6f)

process

Such a model can be excited by a filtered noise impulse.

White Noise Lowpass Highpass Envelope To Model

I R

2

D S P

.

P Y

AND M E S H

2

F A U S T

ir2dsp.py takes an audio file and extracts modal physical model-based information for each mode: frequency and gain, by carrying out peak detection; t60, by measuring bandwidth at -3 dB. A FAUST

file is then generated. With this tool, one can strike any object, record the resulting sound and turn it into a playable digital instrument.

mesh2dsp.py gives the same output, using a .stl file (describing a 3D object) as input, as follows:

• conversion of the input object to a mesh;

• Finite Element Analysis (FEA) using the Elmer package, with the Young modulus, Poisson coefficient and density of the ma-terial as parameters:

• frequency and gain computation from eigenvalues and mass participation for each mode;

• t60 values input (these values cannot be computed by this method unfortunately, so they are user-provided parameters).

E

VALUATION

Spectrograms of (a) the recording of the IR of a can and (b) its ir2dsp.py-generated modal physical model:

(a)

(b)

The original and synthesized sound representations are relatively close (but see Future Directions).

F

UTURE

D

IRECTIONS

We plan to improve ir2dsp.py by using a better t60 measurement algorithm. For now, the calculation is done by measuring the band-width for each peak, while it would be a better approach to extract it from a time-frequency representation of the signal.

Regarding mesh2dsp.py, we would like to try other open-source packages than Elmer to carry out FEA.

R

EFERENCES

[1] R. Michon, J. O. Smith. Faust-STK: a set of linear and nonlinear physical models for the Faust programming language. In Proceedings of the DAFx-11 Conference, 2011

[2] J. O. Smith. Physical Audio Signal Processing for Virtual Musical Instruments and Dig-ital Audio Effects. W3K Publishing, 2010

[3] J.-M. Adrien. The Missing Link: Modal Synthesis. In "Representations of Musical Signals", MIT Press, 1991

[4] Y. Orlarey, D. Fober, S. Letz. Syntactical and Semantical Aspects of Faust. Soft Com-puting, 2004

Project funded by ANR FEEVER. Linux Audio Conf., St-Etienne, May 18-21, 2017.

A

RTIFACTS

Source code available at: https://github.com/rmichon/pmFaust/

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