Next |
Prev |
Up |
Top
|
Index |
JOS Index |
JOS Pubs |
JOS Home |
Search
The above form of the dynamic scattering junction is analogous to the
Kelly-Lochbaum (KL) scattering junction (§C.8.4).
The one-multiply form of the KL junction is well known
(§C.8.5) [299]. The same basic derivation works for our
problem as well to yield a one-filter form for the string-mass
scattering junction.
We cannot simply substitute our reflectances and transmittances for
the reflection and transmission coefficients in the KL result because
our problem is a series connection of two identical string
sections loaded by a junction mass, while the KL junction is derived
for the parallel connection of two acoustic tube sections with
no load at the junction; these differences lead to different signs
as well as introducing the Laplace variable
.
For force waves, we get the following:
The one-filter form follows from the observation that
appears in both computations, and therefore need only be implemented once:
This structure is diagrammed in Fig.9.20.
Again, the above results follow immediately from the more general
formulation of §C.12.
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]