In order to study the nature of the oscillations detected in Hya, it is
necessary to compare the observed frequency spectrum with model predictions,
taking into account the constraints on the three observational stellar
parameters
,
L and Z. We have redetermined the atmospheric
parameters and use
K,
,
,
[M/H] =
(
)
and
.
Details of how these values were obtained
will be reported in a subsequent paper.
Using the evolution code of
Christensen-Dalsgaard (1982), evolutionary tracks were produced, spanning the
error box defined by the uncertainties of
,
L and Z.
The model tracks were computed using the EFF equation of state
(Eggleton et al. 1973), OPAL opacities (Iglesias et al. 1992),
Bahcall & Pinsonneault (1992) nuclear cross sections, and the mixing-length
formalism (MLT) for convection.
The evolutionary track passing through the observed (
,
L)
corresponds to a mass of
for Z = 0.019(Fig. 4). Oscillation frequencies were calculated for the model in
that track closest to the observed location of
Hya in the HR diagram. The
average separation between radial modes in the range 50-100
Hz is
Hz in agreement with the observational value.
The model frequencies fit a linear relation for orders
5 < n < 17 or
Hz given by
with absolute values only 1-2
Hz from the observed frequencies.
The maximum deviation of the model frequencies from the line is
Hz.
Radial modes are expected to dominate the spectrum for giant stars (cf.
Dziembowski et al. 2001, Fig. 2). Further analysis of the spectrum
is beyond the scope of the current discovery paper and will be done
in a forthcoming paper, dealing in detail with the issue of modelling and
considering also the possibility that Hya could be a core
helium burning star with a smaller mass.
Copyright ESO 2002