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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