We have obtained new shock-wave equation of state (EOS) and release ad
iabat data for rhyolite. These data are combined with those of Swegle
(1989, 1990) to give an experimental Hugoniot which is described by U-
s = 2.53(+/- 0.08) + 3.393(+/- 0.37)u(p) for u(p) < 0.48 km s(-1), U-s
= 3.85(+/- 0.05) + 0.65(+/- 0.03)u(p) for 0.48 less than or equal to
u(p) < 2.29 km s(-1), U-s = 1.52(+/- 0.08) + 1.67(+/- 0.02)u(p) for 2.
29 less than or equal to u(p) < 4.37 km s(-1), and U-s = 3.40(+/- 034)
+ 1.24(+/- 0.06)u(p) for u(p) greater than or equal to 4.37 km s(-1),
with rho(0) = 2.357 +/- 0.052 Mg m(-3). We suggest that the Hugoniot
data give evidence of three distinct phases-both low-and high-pressure
solid phases and, possibly, a dense molten phase. EOS parameters for
these phases are rho(0) = 2.494 +/- 0.002 Mg m(-3), K-S0 = 37 +/- 2 GP
a, K' = 6.27 +/- 0.25, and gamma = 1.0(V/V-0) for the low-pressure sol
id phase; rho(0) = 3.834 +/- 0.080 Mg m(-3), K-S0 = 128 +/- 20 GPa, K'
= 3.7 +/- 1.4, and gamma = 1.5 +/- 0.5 for the solid high-pressure ph
ase; and rho(0) = 3.71 +/- 0.10 Mg m(-3), K-S0 = 127 +/- 25 GPa, K' =
2.1 +/- 1.0, and gamma = 1.5 +/- 1.0 for the dense liquid. Transition
regions of the Hugoniot cover the ranges of 9-34 GPa for the low-press
ure-high-pressure solid transition and 90-120 GPa for the high-pressur
e solid-liquid transition. Release paths from high-pressure states, ca
lculated from the EOS parameters, suggest that the material remains in
the high-pressure solid phase upon release. Release paths frost both
the high-pressure solid and liquid fall above the Hugoniot until the H
ugoniot enters the low-pressure-high-pressure mixed phase region, when
the release paths then cross the Hugoniot and fall below it, ending a
t significantly higher zero-pressure densities than that of the low-pr
essure phase. The low-pressure release paths fall very close to the Hu
goniot. Estimates of residual heat deposition, based on shock-release
path hysteresis, range from 20 to 60 per cent of the shock Hugoniot en
ergy.