Next |
Prev |
Up |
Top
|
JOS Index |
JOS Pubs |
JOS Home |
Search
The DW state-space model is given in terms of the FDTD state-space
model by Eq. (32). The similarity transformation matrix
is
bidiagonal, so that
and
are both approximately
diagonal when the output is string displacement for all
. However,
since
given in Eq. (12) is upper triangular, the input matrix
can replace sparse input matrices
with only
half-sparse
, unless successive columns of
are equally
weighted, as discussed in §4. We can say that local
K-variable excitations may correspond to non-local W-variable
excitations. From Eq. (36) and Eq. (37), we see that
displacement inputs are always local in both systems.
Therefore, local FDTD and non-local DW excitations can only occur when
a variable dual to displacement is being excited, such as velocity.
If the external integrator Eq. (38) is used, all inputs are
ultimately displacement inputs, and the distinction disappears.
Next |
Prev |
Up |
Top
|
JOS Index |
JOS Pubs |
JOS Home |
Search
Download wgfdtd.pdf