The environment of the young stellar object GL 490 has been studied us
ing submillimeter emission lines of CO and fundamental vibrational ban
d absorption lines of CO. High spatial resolution observations were ma
de in the emission lines of CO J = 3-2, (CO)-C-13 J = 3-2, and CO J =
6-5. A high spectral resolution (lambda/Delta lambda = 43,000) M-band
(4.7 mu m) spectrum of GL 490 was obtained and shows fundamental vibra
tional band lines of CO and (CO)-C-13 from a range of rotational state
s. CO J = 3-2 maps reveal numerous moving clumps with outflow speeds f
rom a few km s(-1) to 40 km s(-1). The CO J = 3-2 emission, combined w
ith (CO)-C-13 J = 3-2 and CO J = 2-1 emission, shows that the outflowi
ng gas has temperatures from 10 K to 30 K. The CO J = 6-5 emission dem
onstrates that the clumps also contain hotter gas, with excitation tem
peratures from 30 K to 100 K. A range of temperatures is consistent wi
th the presence of shocks. The masses of the dumps range from 0.01 to
0.5 M.. The absence of alignment of the clumps argues against their ej
ection from the central object as interstellar ''bullets.'' The range
of speeds of the outflowing gas is consistent with a wind-driven outfl
ow, in which a fast stellar wind sweeps up a shelf of ambient gas. The
clumps would represent shell fragments. The acceleration of preexisti
ng clumps of ambient gas by the ram pressure of a fast wind can also p
roduce the moving clumps. The CO lines in the absorption spectrum show
a strong absorption component blueshifted by 13 km s(-1) with respect
to the ambient cloud. The absence of an enhancement in CO J = 3-2 emi
ssion at the same velocity suggests that the blueshifted absorbing gas
fills only a small fraction of the 15'' beam. The (CO)-C-13 infrared
absorption lines show that the quiescent gas in the line of sight to G
L 490 contains two temperature components, T = 24 K and T = 107 K, wit
h (CO)-C-13 column densities N-24K = 5.6 x 10(16) cm(-2) and N-107K =
6.9 x 10(16) cm(-2). The 24 K gas is the expected cold gas in the mole
cular cloud. The 107 K gas is evidence for the existence of a ''hot co
re'' about GL 490. Hot gas is also shown by the CO J = 6-5 emission. T
he decrease in CO J = 6-5 intensity with distance from GL 490 is used
to obtain a diameter for the hot core of 12,000 AU. The fact that the
CO J = 6-5 intensity peaks at GL 490 suggests that GL 490 itself, rath
er than external ultraviolet radiation, is the source of heating for t
he 107 K gas.