Environmental Engineering Reference
In-Depth Information
0
s m s c ,D 0
s m s c ,D 0
s m s c ,D 0
t
Figure 5.17. Scheme of the possible evolutions of small initial displacement depend-
ing on the noise intensity and the strength of the spatial coupling.
that noise-induced instability is transient, in the sense that the state
0 is recovered in
the long term. This behavior is shown by the thin continuous curve in Fig. 5.17 :Noise
initially induces a growth (i.e., an instability) of
φ
φ
,butfor t →∞
the difference
| φ φ 0 |
tends to zero. This behavior (i) explains why this mechanism is called
short-term instability and (ii) suggests that the steady-state pdf of
φ
is expected to be
unimodal, with the mode at
φ 0 ,evenwhen s m exceeds the threshold s c .
We now consider spatiotemporal dynamics (i.e., D
=
0). Differently from the
subcritical case, when s m >
s c , the spatial coupling introduces qualitative changes with
respect to the zero-dimensional case. In fact, for suitable values of the strength D of the
coupling, the spatial term in Eq. ( 5.31 ) takes advantage of the noise-induced short-term
instability that also exists in the spatiotemporal dynamics (in fact,
φ /∂
t
d
φ /
d t
for t
from decaying to zero. As a
consequence, the spatial coupling locks the system in a new ordered state, with
0) and prevents the displacement
| φ φ 0 |
φ
different from
φ 0 and variable in space. In this case the temporal trajectory of
φ
does
not exhibit a convergence to
, as shown by the thick curve in Fig. 5.17 .
Thus the spatial coupling is responsible for maintaining the dynamics away from the
state
φ
0 for t
→∞
0 . Before investigating the behavior of some prototype models, we describe in
Box 5.5 an analytical tool used to detect the possible presence of short-term instability
in stochastic dynamical systems.
Once the short-term instability has been detected, the ability of spatiotemporal
stochastic dynamics ( B5.5-1 ) to give rise to periodic patterns is typically investigated
by the prognostic tools described in Boxes 5.1, 5.2, and 5.3.
φ
5.4.1 Prototype model
To illustrate howpattern formation can be induced bymultiplicative noise, we consider
the prototype model:
∂φ
3
D ( k 0 +∇
2 ) 2
t =
a
φ φ
+ φξ gn
φ,
(5.34)
 
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