- In the same way they can be used to simulate traveling waves in free space, delay lines can be used to simulate one-dimensional (1D) wave propagation along strings or in acoustic tubes. Since waves can propagate simultaneously in two opposite directions along such a 1D waveguide, two delay lines are necessary.
- It can be shown that a discrete time and space solution to the 1D lossless wave equation is given by

(3) *n*and spatial indices*m*. - The spatial sampling interval is given by
*X*=*c T*_{s}meters, or the distance traveled by sound in one temporal sampling interval. In this way, each traveling-wave component moves left or right one spatial sample for each time sample. - Physical wave variables are given by the superposition of traveling waves. In a one-dimensional system, we can use two systems of unit delay elements to model left- and right-going traveling waves and sum delay-line values at corresponding ``spatial'' locations to obtain physical outputs, as depicted below.
**Figure 13:**Discrete-time simulation of ideal, lossless wave propagation with observation points at*x*= 0 and*x*= 3*X*= 3*cT*. - Any ideal, lossless, one-dimensional waveguide can be simulated in this way. The model is exact at the sampling instants to within the numerical precision of the processing system.
- In many modeling contexts, the calculation of physical output values can be limited to just one or two discrete spatial locations. Individual unit delay elements are more typically combined and represented by digital delay lines, as shown below.
- The delay lines can be initialized with displacement data corresponding to any bandlimited, arbitrary waveshape.

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