Environmental Engineering Reference
In-Depth Information
Figure 5.22. Numerical simulation of model ( 5.42 ). The parameters are a
=−
1,
5. The three panels correspond to t equal to 0, 1, and 5
time units. The gray-tone scale is in the interval [
D
=
10, k 0 =
1, and s gn =
0
.
01
,
0
.
01].
Thus the steady uniform case is still
0. However, in this case, the analysis of the
short-term behavior of the temporal component of the model yields
φ
=
0
d
φ
d t
3
3
a
φ φ
+
2 s gn
φ
=
f eff (
φ
)
.
(5.43)
Thus
φ 0 is stable when
φ 0 =
d f eff
d
a
<
0
,
(5.44)
φ
indicating that the contribution of the multiplicative-noise term is negligible with
respect to the linear component of f (
). Thus Eq. ( 5.44 ) shows that in these dynamics
[Eq. ( 5.42 )] noise is not able to have an impact on the short-termbehavior of the system
and no short-term instability occurs. We explain this result by interpreting the short-
term behavior as a result of the interplay between the restoring action that is due to
the tendency of f (
φ
φ
) to drive the system toward the homogeneous state
φ = φ
=
0
0
φ
ξ
φ
and the diverging action that is due to multiplicative noise, g (
)
gn .When
is close
φ 0 , such as those studied in the linear-
stability analysis), the power two in the function g (
φ 0 =
to
0 (i.e., for small displacements from
) strongly reduces the effect of
noise, which becomes unable to hinder the action of the leading term a
φ
).
This result is confirmed by the stability analysis of the dynamics of the ensemble
average. In this case the dispersion relation is
φ
of f (
φ
D ( k 0
k 2 ) 2
γ
( k )
=
a
.
(5.45)
Thus the growth factor
is always negative for any wave number and no patterns
emerge. An example of numerical simulations of model ( 5.42 ) is shown in Fig. 5.22 .
Patterns occur only transiently, and the field then rapidly decays to the homogeneous
state
γ
0 .
Notice that short-term instability can also be present with nonlinear forms of g (
φ
),
provided that the multiplicative component overcomes the action of the deterministic
φ
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