Ye Lu 2011-03-14. Stefan Bilbao, 2009, Numerical Sound Synthesis: Finite Difference Schemes and...

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Modeling the Mechanical Response of Clarinet Reed Ye Lu 2011-03-14

Transcript of Ye Lu 2011-03-14. Stefan Bilbao, 2009, Numerical Sound Synthesis: Finite Difference Schemes and...

Page 1: Ye Lu 2011-03-14.  Stefan Bilbao, 2009, Numerical Sound Synthesis: Finite Difference Schemes and Simulation in Musical Acoustics.

Modeling the Mechanical Response of Clarinet Reed

Ye Lu2011-03-14

Page 2: Ye Lu 2011-03-14.  Stefan Bilbao, 2009, Numerical Sound Synthesis: Finite Difference Schemes and Simulation in Musical Acoustics.

Reed Instruments

Page 3: Ye Lu 2011-03-14.  Stefan Bilbao, 2009, Numerical Sound Synthesis: Finite Difference Schemes and Simulation in Musical Acoustics.

Stefan Bilbao, 2009, Numerical Sound Synthesis: Finite Difference Schemes and Simulation in Musical Acoustics

A Single-reed Woodwind Mouthpiece

Page 4: Ye Lu 2011-03-14.  Stefan Bilbao, 2009, Numerical Sound Synthesis: Finite Difference Schemes and Simulation in Musical Acoustics.

F. Avanzini and M. van Walstijn, “Modeling the mechanical response of the reed-mouthpiece-lip system of a clarinet. 1. A one-dimensional distributed model”, Acta Acust, 90, 537-547 (2004).

Page 5: Ye Lu 2011-03-14.  Stefan Bilbao, 2009, Numerical Sound Synthesis: Finite Difference Schemes and Simulation in Musical Acoustics.

Single degree of freedom with constant parameters can only be assumed for oscillations at small amplitudes

Reed beating is usually incorporated in a non-physical way by imposing a maximum allowed displacement for the reed tip

The dependence of the reed-mouthpiece system on the lip embouchure is not considered in lumped model

Disadvantage of Lumped Model

Page 6: Ye Lu 2011-03-14.  Stefan Bilbao, 2009, Numerical Sound Synthesis: Finite Difference Schemes and Simulation in Musical Acoustics.

A bar with non-uniform cross-sectional area

Clamped to the mouthpiece at one end

Additional constraints provided by the mouthpiece profile and interaction with the lip

Distributed Representation of the Reed

Page 7: Ye Lu 2011-03-14.  Stefan Bilbao, 2009, Numerical Sound Synthesis: Finite Difference Schemes and Simulation in Musical Acoustics.

The Model

Page 8: Ye Lu 2011-03-14.  Stefan Bilbao, 2009, Numerical Sound Synthesis: Finite Difference Schemes and Simulation in Musical Acoustics.

One-dimensional: assume no torsional modes in the reed

No attempt to model the air flow in the reed channel or to simulate the acoustical resonator

Limitation of the Model

Page 9: Ye Lu 2011-03-14.  Stefan Bilbao, 2009, Numerical Sound Synthesis: Finite Difference Schemes and Simulation in Musical Acoustics.

Boundary Conditions

Page 10: Ye Lu 2011-03-14.  Stefan Bilbao, 2009, Numerical Sound Synthesis: Finite Difference Schemes and Simulation in Musical Acoustics.

Interaction with the mouthpiece and the lip

Page 11: Ye Lu 2011-03-14.  Stefan Bilbao, 2009, Numerical Sound Synthesis: Finite Difference Schemes and Simulation in Musical Acoustics.

Interaction with the mouthpiece and the lip

Page 12: Ye Lu 2011-03-14.  Stefan Bilbao, 2009, Numerical Sound Synthesis: Finite Difference Schemes and Simulation in Musical Acoustics.

Measurements

Page 13: Ye Lu 2011-03-14.  Stefan Bilbao, 2009, Numerical Sound Synthesis: Finite Difference Schemes and Simulation in Musical Acoustics.

Finite Difference Method

Numerical Simulation

Page 14: Ye Lu 2011-03-14.  Stefan Bilbao, 2009, Numerical Sound Synthesis: Finite Difference Schemes and Simulation in Musical Acoustics.

Some Schemes

Page 15: Ye Lu 2011-03-14.  Stefan Bilbao, 2009, Numerical Sound Synthesis: Finite Difference Schemes and Simulation in Musical Acoustics.

Some Schemes

Page 16: Ye Lu 2011-03-14.  Stefan Bilbao, 2009, Numerical Sound Synthesis: Finite Difference Schemes and Simulation in Musical Acoustics.

Discretization

Page 17: Ye Lu 2011-03-14.  Stefan Bilbao, 2009, Numerical Sound Synthesis: Finite Difference Schemes and Simulation in Musical Acoustics.

Unconditional stable when Θ > 1/4

Implicit θ-Scheme

Page 18: Ye Lu 2011-03-14.  Stefan Bilbao, 2009, Numerical Sound Synthesis: Finite Difference Schemes and Simulation in Musical Acoustics.

Implicit θ-Scheme

http://www.tandfonline.com/doi/abs/10.1080/10236190802385298#preview

Page 19: Ye Lu 2011-03-14.  Stefan Bilbao, 2009, Numerical Sound Synthesis: Finite Difference Schemes and Simulation in Musical Acoustics.

The reed tip can not exceed a certain value

The tip is not stopped suddenly but rather gradually

Simulation Result

Page 20: Ye Lu 2011-03-14.  Stefan Bilbao, 2009, Numerical Sound Synthesis: Finite Difference Schemes and Simulation in Musical Acoustics.

Convergence of the Scheme

Page 21: Ye Lu 2011-03-14.  Stefan Bilbao, 2009, Numerical Sound Synthesis: Finite Difference Schemes and Simulation in Musical Acoustics.

Thank You!