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A rigid termination is the simplest case of a string
termination. It imposes the constraint that the string cannot move
at the termination. If we terminate a length ideal string at
and , we then have the ``boundary conditions''
|
(5.7) |
where ``'' means ``identically equal to,'' i.e., equal for all
. Let
denote the time in samples to propagate
from one end of the string to the other and back, or the total
``string loop'' delay. The loop delay is also equal to twice the
number of spatial samples along the string.
Applying the traveling-wave decomposition from Eq. (4.2), we have
Therefore, solving for the reflected waves gives
A digital simulation diagram for the
rigidly terminated ideal string is shown in Fig. 4.2.
A ``virtual pick-up'' is shown at the arbitrary location .
Figure 4.2:
The rigidly terminated
ideal string, with a displacement output indicated at position
. Rigid terminations reflect traveling displacement, velocity,
or acceleration waves with a sign inversion. Slope or force waves
reflect with no sign inversion.
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