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Let us start from (4.18) and
introduce
with
given by (4.14):
where
|
(113) |
is ``triad-interaction'' frequency and
is triad
interaction time. One can consider (B1 - B2) as an
integral equation for the damping of wave
and for the frequency
.
First we consider these equations in the limit of weak interaction
where, , and the main contribution to the first term in
(B1) comes from the region where
|
(114) |
These are conservation laws for 3-wave confluence processes . The main contribution for the second term in (B1) comes
from the region
|
(115) |
These are conservation laws for decays processes . For weak
interaction one may replace in (4.2) and (4.3)
on
. Than it follows from
(4.2) and (4.3) that
with
directed along . This fact makes it natural to introduce in integrals (B1)
new variables: scale positive variable and two-dimensional
vector such that
|
(116) |
In the first term of (B1)
|
(117) |
In the second term
|
(118) |
For the denominators in integrals (B1) strongly
depend on . Indeed:
This allows to neglect dependence of interaction
and correlation in numerator of
(B1) for estimation. The result is
where
|
(122) |
is a factor in (2.20) so that for parallel or almost parallel
wavevectors
. After
changing of variables this integral becomes to be more transparent:
One may estimate
from the fact that
our expressions were obtained by expanding in , therefore
should be at least .
Now let us consider the imaginary and real part of
separately. It is convenient to begin with
:
Here we changed the upper limit of integration:
because the main contribution to the integral comes from the area
. After trivial integration with respect of
one has:
This expression for
corresponds to that given by
the kinetic equation [1] for waves. For further progress it is
necessary to do some assumption about . Let us assume that
vanishes with growing of faster than
. For such
spectra the main contribution to the integral comes from small . In this case contributions from first and second integrals in
(B14) coincides and may be represented in the form:
|
|
|
(126) |
In this case contributions from first and second integrals in
(B14) coincides and may be represented in the form:
|
|
|
(127) |
Next: Estimation of the two-loop
Up: Statistical Description of Acoustic
Previous: Rules for writing and
Dr Yuri V Lvov
2007-01-17