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>From this point the development follows the lines given in the SAFARI
Users Guide[4] and subsequent updates. Scalar and
vector potentials are introduced so that
In terms of these potentials, and in the absence of sources, the
equations of motion become
These equations are first subjected to Fourier transform in time and
either Fourier transform (for plane strain) or Hankel transform (for
axial symmetry) in the plane perpendicular to the depth coordinate
z. We show details assuming plane strain with motion restricted to
the xz-plane (the axial symmetry case is similar and follows the
outline in the SAFARI Users Guide). In this event the vector
potentials have only a single nontrivial component,
,
so the displacement components take the form
Furthermore, the constitutive equations, in terms of the potentials,
become
The solution of the transformed equations take the form
where
and
are the transformed potentials and
,
,
and
are functions of angular frequency
and wave
number s.
Also
and
where hf, hs, and k are respectively the complex wavenumbers
associated with fast, slow and shear waves in the Biot medium at
angular frequency .
For the shear wave we have
while the wave numbers associated with the fast and slow waves are
given by
where
and the two compression wave numbers are ordered so that
.
In terms of the six degrees of freedom ,
,
and
for a porous sediment layer, the transformed displacement
and stress components are
Boundary conditions to be satisfied at each interface involve
continuity of pore fluid normal displacement and pressure, and
continuity of displacement and traction components for the frame. To
complete table 1 of the SAFARI Users guide we add the following table
entries where the symbol
means the parameter is not involved,
0 means it should be set to zero, and = means continuity is
enforced at the interface.
In the following table the first four columns correspond to the same
entries in the Users Guide table, while the last column corresponds to
the negative of the traction component
in adjacent fluid
layers.
Type |
Field parameter |
|
w - wf |
u |
|
|
wf |
p |
Biot/vacuum |
|
|
0 |
0 |
|
0 |
Biot/fluid |
= |
|
= |
0 |
|
= |
Biot/solid |
= |
= |
= |
= |
0 |
|
Biot/Biot |
= |
= |
= |
= |
= |
= |
Next: About this document ...
Up: Porous Media Model
Previous: The Model
henrik schmidt
1999-08-25