Next 
Prev 
Up 
Top

Index 
JOS Index 
JOS Pubs 
JOS Home 
Search
Rigid Terminations
A rigid termination is the simplest case of a string (or tube)
termination. It imposes the constraint that the string (or air) cannot move
at the termination. (We'll look at the more practical case of a yielding
termination in §9.2.1.) If we terminate a length
ideal string at
and
, we then have the ``boundary conditions''

(7.9) 
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 travelingwave decomposition from Eq.
(6.2), we have
Therefore, solving for the reflected waves gives
A digital simulation diagram for the
rigidly terminated ideal string is shown in Fig.6.3.
A ``virtual pickup'' is shown at the arbitrary location
.
Figure 6.3:
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.

Subsections
Next 
Prev 
Up 
Top

Index 
JOS Index 
JOS Pubs 
JOS Home 
Search
[How to cite this work] [Order a printed hardcopy] [Comment on this page via email]