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Clarinet Reed Modelling
Ye Lu2011-4-11
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
Lumped Modelling
Euler Method
Compute the Inverse Laplace transform to get impulse response of the analogue filter
Sample the impulse response (quickly enough to avoid aliasing problem)
Compute z-transform of resulting sequence
Impulse Invariant method
Linear multistep methods used for the numerical solution of ordinary differential equations
Adams-Moulton Methods
Linear multistep methods used for the numerical solution of ordinary differential equations
Adams-Moulton Methods
A. M. Schneider, J. T. Kaneshige, and F. D. Groutage. Higher Order s-to-z Mapping Functions and their Application in Digitizing Continuous-Time Filters. Proc. IEEE, 79(11):1661–1674, Nov. 1991.
Frequency Response
Used for a generic linear system and are based on a polynomial interpolation of the system input
Weighted Sample Methods
Weighted Sample Methods
Numerical Methods
Weighted Sample Methods
Weighted Sample Methods
Weighted Sample Methods
Weighted Sample Methods
Typical resonance frequency lie in the high frequency region, non-critical in helping self-sustained oscillations
the reed resonance has a role in adjusting pitch, loudness and tone color, and in helping transitions to high regimes of oscillation (S. C. Thompson. The Effect of the Reed Resonance on Woodwind Tone Production. J. Acoust. Soc. Am., 66(5):1299–1307, Nov. 1979.)
Frequency Domain Analysis
Euler Method provide poor accuracy even with Fs=44100Hz
Results for the AM methods are in good agreement with theoretical predictions
the magnitude of AM2 amplifies the magnitude of the resonance
the methods becomes unstable at Fs = 190000Hz
Frequency Domain Analysis
Results for the WS methods are in excellent agreement with theoretical predictions, even at low sampling rates
Numerical dissipation is introduced, the amplitude responses is smaller
The phase responses are well preserved by both methods
WS methods better approximate the reed frequency response than AM methods
Frequency Domain Analysis
Time Domain Analysis
The quasi-static estimated value underestimates the true pt (D. H. Keefe. )
Time Domain Analysis
For all the digital reeds, pt converges to the dynamic estimate pressure1802
1-step methods exhibit robustness with respect to the sampling rate
Time Domain Analysis
Time Domain Analysis the clarion register can be produced
without opening the register hole, if the reed resonance matches a low harmonic of the playing frequency and the damping is small enough
an extremely low damping causes the reed regime to be produced
Time Domain Analysis
The Model
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
Boundary Conditions
Implicit θ-Scheme
http://www.tandfonline.com/doi/abs/10.1080/10236190802385298#preview
Implicit θ-Scheme
http://www.tandfonline.com/doi/abs/10.1080/10236190802385298#preview
The reed tip can not exceed a certain value
The tip is not stopped suddenly but rather gradually
Simulation Result
The Reed Model
Implicit θ-Scheme
Reed Construction
The cause of the discontinuity in the one-dimensional case is not the omittance of the reed’s torsional motion
Numerical Results
The reed-lay interaction exhibits a stronger non-linearity when
(1) The player’s lip moves towards the free end of the reed
(2) When a thinner reed is used
Numerical Results
The closer the lip is positioned towards the free end of the reed, the stronger the non-linear behavior of S becomes
Numerical Results
F. Avanzini. Computational Issues in Physically-based Sound Models. Ph.D. Thesis, Dept. of Computer Science and Electronics, University of Padova (Italy), 2001.
M. van Walstijn and F. Avanzini. Modelling the mechanical response of the reed-mouthpiece-lip system of a clarinet. Part II. A lumped model approximation. Acta Acustica united with Acustica, 93(3):435-446, May 2007.
F. Avanzini and M. van Walstijn. Modelling the Mechanical Response of the Reedmouthpiece- lip System of a Clarinet. Part I. A One-Dimensional Distributed Model. Acta Acustica united with Acustica, 90(3):537-547 (2004).
A. M. Schneider, J. T. Kaneshige, and F. D. Groutage. Higher Order s-to-z Mapping Functions and their Application in Digitizing Continuous-Time Filters. Proc. IEEE, 79(11):1661–1674, Nov. 1991.
C.Wan and A. M. Schneider. Further Improvements in Digitizing Continuous-Time Filters. IEEE Trans. Signal Process., 45(3):533–542, March 1997.
V. Chatziioannou and M. van Walstijn. Reed vibration modelling for woodwind instruments using a two-dimensional finite difference method approach. In International Symposium on Musical Acoustics, Barcelona, 2007.
References
Thank You!