Our understanding of stars of the PG 1159 spectral type is not yet sat
isfactory, in spite of the recent success of asteroseismology. Kawaler
and coworkers match the observed pulsation frequencies of PG 1159-035
and PG 2131 + 066 quite well with evolutionary models, but they fail
to identify the mechanism exciting their pulsations. Stanghellini, Cox
, & Starrfield show that the classical kappa, gamma mechanism acting i
n the C/O partial ionization zone can excite certain g-modes but requi
res compositions that seem unrealistic. Here we study the impact of th
e new OPAL opacities on the conditions required to drive the modes obs
erved in the PG 1159 spectral class stars. To this end, we present the
nonadiabatic pulsation results of a parametric survey of quasi-evolut
ionary models of PG 1159 pre-white dwarfs. We examine the effect of va
rying the chemical composition of the driving region, the stellar radi
us, and stellar mass on the location of the instability strip and the
maximum unstable period. Changes in the oxygen mass fraction of the dr
iving region and the stellar radius have a strong effect on the predic
ted spectrum of unstable modes. We do not find unstable modes with per
iods longer than 150 s unless the driving region, located near 10(-9)
M, has at least 50% oxygen. The maximum unstable period increases by
factors of 2-3 when we increase the radius of our models by 40%-50%. D
ecreasing the stellar mass also increases the radius, and the maximum
unstable period increases from similar to 300-400 s at 0.65 M(.) to si
milar to 800 s at 0.50 M(.) for models with 50:50 C/O cores. Based on
these results, we suggest that no pulsating PG 1159 star has a driving
region with photospheric abundances; rather they are probably oxygen-
rich. In addition, we believe PG 1159-035 and PG 1707+427, probably ha
ve larger radii than the seismological models of Kawaler & Bradley pre
dict, because our evolutionary models with pure oxygen cores fail to p
redict unstable modes with periods up to the similar to 1000 s we obse
rve. Models with larger radii also have rates of period change closer
to that observed for the 516 s mode of PG 1159-035. In contrast, our p
resent 50:50 C/O evolutionary models are able to duplicate the observe
d maximum unstable periods of the two coolest pulsating PG 1159 stars,
PG 2131+066 and PG 0122+200. This suggests that the last two stars ha
ve radii close to that predicted by our models, and that their driving
regions are less oxygen-rich than in the hotter pulsating PG 1159 sta
rs.