Xf. Xie et Mj. Mumma, MONTE-CARLO SIMULATION OF COMETARY ATMOSPHERES - APPLICATION TO COMETP HALLEY AT THE TIME OF THE GIOTTO SPACECRAFT ENCOUNTER .1. ISOTROPICMODEL/, The Astrophysical journal, 464(1), 1996, pp. 442-456
Isotropic and axisymmetric models of a cometary atmosphere, made up of
H2O and its daughter radicals (H, OH, O, and H-2), have been establis
hed using the Monte Carlo particle transport method, Physical paramete
rs of the gases considered were computed for an isotropic cometary com
a with a gas production rate of 5 x 10(29) molecules s(-1) and helioce
ntric distances of 0.89 AU, corresponding to comet P/Halley at the Gio
tto flyby in 1986 March. The simulated velocity profile of water molec
ules is in good agreement with Giotto Neutral Mass Spectrometer (NMS)
measurements over the entire range from the inner coma to the outer co
ma (800-34,000 km), when realistic semiclassical collision cross secti
ons are used. The successful model for the velocity profile in the out
er coma requires the inclusion of rotational cooling of water molecule
s in this transition region from the optically thick to optically thin
. No evidence is found from our simulation for additional heating from
the recondensation of icy grains in the inner coma with radial distan
ces larger than 500 km. Our simulation demonstrates that selective pho
todestruction of slow water molecules in the inner coma contributes si
gnificantly to the increase of outflow velocity of parent species at r
adial distances larger than 20,000 km, at which photochemical heating
ceases to be important. The simulation also shows clearly the evolutio
n of velocity distributions for gas particles from being thermal in th
e inner coma to nonthermal in the outer coma; the critical distance is
found to be 6000 km for water molecules (at a gas production rate of
5 x 10(29) molecules s(-1)). Outside the collision-dominated region (r
> 10(4) km), hydrogen (H) has three peaks in its velocity distributio
n, one at 18 km s(-1), a second at 8 km s(-1), and a thermal component
peaked at about 1-2 km s(-1), consistent with observational results.
We show that a gas production rate of 4.5 x 10(29) molecules s(-1) giv
es the best fit to the Giotto NMS velocity measurements.