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in terms of α into the expression for ∆S , we obtain
k y
k 2
||
ω
|
a ( x 1 )
|
2 .
∆S
|
b 0 |
(4.66)
8
The amplitude b 0 and location of the FLR-point x 1 depend, in (4.66), on
frequency ω and wavenumber k y . For a complete solution of the problem
either a numerical or an analytical solution of (4.53) or (4.58) are necessary.
The right bottom panel of Fig. 4.3 shows the results of numerical calculations
of the Pointing vector. The wave energy loss is equal to the divergence of the
Pointing vector.
It is important, that the energy flux is finite also behind the turning point.
The tunneling effect supports the energy input to the resonance surface. A
finite energy per unit area equal to the Pointing vector discontinuous jump
at the resonance surface dissipates in a thin resonance layer. Behind the res-
onance surface the energy flux becomes small and it vanishes at σ
0.
Under non-monotonous c A ( x ) distribution more than one resonance surfaces
can exist and the energy flux behind the first resonance surface is finite.
References
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1974.
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S.
Hydrodynamic
and
Hydromagnetic
Stability ,
Oxford
University Press,Oxford, England, 1961.
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