Astron. Astrophys. 354, 296-304 (2000)
Appendix A
System (1) can be Fourier-analyzed in terms of
, with the
sign according to (2, 3), to obtain
a set of algebraic equations:
![[EQUATION]](img196.gif)
The linearized variables can be put in a non dimensional form, as
described in Sect. 2, and Eqs. (A.1), (A.2) and (A.3) can be solved to
obtain , with
and K specifying relations
between density, velocities and pressure in the plane-wave solutions
as:
![[EQUATION]](img199.gif)
Appendix B
The amplitudes for an initial
pressure pulse are:
![[EQUATION]](img200.gif)
![[EQUATION]](img201.gif)
where ,
is the solution of dispersion
relation for acoustic modes and is
the solution for internal gravity modes.
and
are the amplitudes of acoustic
modes while and
are the amplitude of internal
gravity modes.
© European Southern Observatory (ESO) 2000
Online publication: January 31, 2000
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