Chondrule formation due to the shock heating of dust particles with a wide
variety of shock properties are examined. We numerically simulate the stead
y postshock region in a framework of one-dimensional hydrodynamics, taking
into account many of the physical and chemical processes that determine the
properties of the region, especially nonequilibrium chemical reactions of
gas species. We mainly focus on the maximum temperature of dust particles a
nd their net cooling rate in relation to the chondrule formation.
We derive the condition of chondrule formation for the shock velocity v(s),
and the preshock density no. For n(0) > 10(14.5) cm(-3), the shock velocit
y should be in a range 6 km s(-1) less than or equal to v(s) less than or e
qual to 7 km s(-1), while for n(0) < 10(14.5) cm(-3), v(s) should be 6x(n(0
)/10(14.5) cm(-3))(-1/5) km s(-1) less than or equal to v(s) less than or e
qual to 7 x(n(0)/10(14.5) cm(-3))(-1/5) km s(-1) for an initial dust partic
le radius of 0.1 rum. The condition has a small dependence on particle size
. We find that the Keplerian velocities and equatorial plane densities arou
nd the asteroidal and Jupiter orbital regions of the minimum mass solar neb
ula model are suitable for chondrule formation. We also find that the gas p
ressure in the postshock region is much higher than the one in the standard
nebula environment. Furthermore, we find that the net cooling rates of 0.1
-1-mm-sized dust particles are about 10(2)-10(5) K h(-1), which are not too
far from experimental values, though the melting region is optically thin.
Those slow net cooling rates are maintained by drag heating in the cooling
phase. These results indicate that the shock heating model can be regarded
as a strong candidate for the mechanism of chondrule formation. (C) 2001 A
cademic Press.