As mentioned above, digital waveguide models are built out of digital delaylines and filters (and nonlinear elements), and they can be understood as propagating and filtering sampled travelingwave solutions to the wave equation (PDE), such as for air, strings, rods, and the like [#!MADW!#,#!SmithPMUDW!#]. It is noteworthy that strings, woodwinds, and brasses comprise three of the four principal sections of a classical orchestra (all but percussion). The digital waveguide modeling approach has also been extended to propagation in 2D, 3D, and beyond [#!VanDuyneAndSmithMesh!#,#!FinnishMesh!#,#!vanDuy96!#,#!sav01!#]. They are not finitedifference models, but paradoxically they are equivalent under certain conditions (Appendix E). A summary of historical aspects appears in §A.9.
As mentioned at Eq.(1.1), the ideal wave equation comes directly from Newton's laws of motion ( ). For example, in the case of vibrating strings, the wave equation is derived from first principles (in Chapter 6, and more completely in Appendix C) to be
where
Defining , we obtain the usual form of the PDE known as the ideal 1D wave equation.
As has been known since d'Alembert [#!dAlembert!#], the 1D wave equation is obeyed by arbitrary traveling waves at speed :
To show this, just plug or (or any linear combination of them) into the wave equation Eq.(1.15). Thus, is the travelingwave propagation speed expressed in terms of the string tension and mass density .
In digital waveguide modeling, the travelingwaves are sampled:
where denotes the time sampling interval in seconds, denotes the spatial sampling interval in meters, and and are defined for notational convenience.
An ideal string (or air column) can thus be simulated using a bidirectional delay line, as shown in Fig.1.13 for the case of an sample section of ideal string or air column. The `` '' label denotes its wave impedance (§6.1.5) which is needed when connecting digital waveguides to each other and to other kinds of computational physical models (such as finite difference schemes). While propagation speed on an ideal string is , we will derive (§C.7.3) that the wave impedance is .

Figure 1.14 (from Chapter 6, §6.3), illustrates a simple digital waveguide model for rigidly terminated vibrating strings (more specifically, one polarizationplane of transverse vibration). The travelingwave components are taken to be displacement samples, but the diagram for velocitywave and accelerationwave simulation are identical (inverting reflection at each rigid termination). The output signal is formed by summing travelingwave components at the desired ``virtual pickup'' location (position in this example). To drive the string at a particular point, one simply takes the transpose [#!JOSFP!#] of the output sum, i.e., the input excitation is summed equally into the left and rightgoing delaylines at the same position (details will be discussed near Fig.6.14).
In Chapter 9 (example applications), we will discuss digital waveguide models for singlereed instruments such as the clarinet (Fig.1.15), and bowedstring instruments (Fig.1.16) such as the violin.