## Ideal Acoustic Tube

As discussed in §C.7.3, the most commonly used digital
waveguide variables (``wave variables'') for *acoustic tube*
simulation are traveling *pressure* and *volume-velocity*
samples. These variables are exactly analogous to the traveling force
and transverse-velocity waves used for vibrating string models.

The Ohm's law relations for acoustic-tube wave variables may be written as follows (cf. Eq.(6.6)):

Here is the right-going traveling

*longitudinal pressure wave*component, is the left-going pressure wave, and are the left- and right-going

*volume velocity waves*. For acoustic tubes, the wave impedance is given by

(Acoustic-Tube Wave Impedance) | (7.8) |

where denotes the density (mass per unit volume) of air, is sound speed in air, and is the cross-sectional area of the tube.

In this formulation, the acoustic tube is assumed to contain only
*traveling plane waves* to the left and right. This is a
reasonable assumption for wavelengths much larger than the
tube diameter (
). In this case, a change in the
tube cross-sectional area along the tube axis will cause lossless
*scattering* of incident plane waves. That is, the plane wave
splits into a transmitted and reflected component such that wave
energy is conserved (see Appendix C for a detailed derivation).

Figure 6.2 shows a piecewise cylindrical tube model of the
vocal tract and a corresponding digital simulation [245,297].
In the figure, denotes the *reflection coefficient*
associated with the first tube junction (where the cross-sectional
area changes), and is the corresponding *transmission
coefficient* for traveling *pressure* plane waves. The
corresponding reflection and transmission coefficients for
*volume velocity* are and , respectively. Again,
see Appendix C for a complete derivation.

At higher frequencies, those for which
, changes
in the tube cross-sectional area give rise to *mode
conversion* (which we will neglect in this chapter).
Mode conversion means that an incident plane wave (the simplest mode of
propagation in the tube) generally
scatters into waves traveling in many directions, not just the two
directions along the tube axis. Furthermore, even along the tube axis,
there are higher orders of mode propagation associated with ``node lines''
in the transverse plane (such as Bessel functions of integer order
[541]). When mode conversion occurs, it is necessary to keep
track of many components in a more general *modal expansion* of
the acoustic field [336,13,50]. We may say that
when a plane wave encounters a change in the cross-sectional tube
area, it is ``converted'' into a sum of propagation modes. The coefficients
(amplitude and phase) of the new modes are typically found by matching
boundary conditions. (Pressure and volume-velocity must be continuous
throughout the tube.)

As mentioned above, in acoustic tubes we work with *volume
velocity*, because it is volume velocity that is conserved when a
wave propagates from one tube section to another. For plane waves in
open air, on the other hand, we use *particle velocity*, and in
this case, the wave impedance of open air is
instead.
That is, the appropriate wave impedance in open air (not inside an
acoustic tube) is pressure divided by particle-velocity for any traveling
plane wave. If denotes a sample of the volume-velocity
plane-wave traveling to the right in an acoustic tube of
cross-sectional area , and if denotes the corresponding
particle velocity, then we have

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Rigid Terminations

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Ideal Vibrating String