Astron. Astrophys. 357, 1073-1085 (2000)
6. Nonlinear damping of the phase-mixed AWs in corona
As in the Discussion, we take the length-scale of the field-aligned
inhomogeneity in a coronal hole km,
the transverse inhomogeneity length-scale ranging as 1 km
km, and wave amplitudes ranging
from 0.01 to 0.03 for .
For wave frequencies
s-1 (see Discussion), the nonuniformity restrictions for
the decay into counterstreaming waves may be satisfied. Then, using
the damping rate (57) in (32), we find that the pump wave amplitude
decays with height as
![[EQUATION]](img315.gif)
where the distance of nonlinear damping
![[EQUATION]](img316.gif)
To compare this height with the field-aligned wavelength we rewrite
as
![[EQUATION]](img318.gif)
where the coefficient before
strongly depends on the perpendicular nonuniformity length-scale
.
Let us apply the above results to phase-mixed Alfvén waves
in a coronal hole. Taking m,
, and
m, we obtain a low damping height
in the coronal holes, varying in the range from
with
km, up to
with
km. Note that the ion gyroradius is
nevertheless very small compared to
at these heights.
The corresponding transverse wavelengths,
km with
km and
km with
km, are much longer than the
dissipative length-scale, m. This
is exactly the point we made in the Introduction that the effect of
FLR in Alfvén waves comes into play at length scales which are
much longer than .
© European Southern Observatory (ESO) 2000
Online publication: June 5, 2000
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