The success of air sparging as a remedial technology for treatment of conta
minated aquifers is well documented. However, there is no consensus, to dat
e, on the mechanisms that control the flow of injected air through the satu
rated ground. Currently, only qualitative results from laboratory experimen
ts are available to predict the zone of influence of a sparging well. Given
that the patterns of air flow through the soil will ultimately determine t
he efficiency of an air sparging treatment, it is important to quantify how
sparged air travels through a saturated porous medium. The main objective
of this research is to develop a model that describes air transport through
saturated porous media. This paper presents results from an ongoing study
that employs centrifuge modeling to reproduce in situ air sparging conditio
ns. Centrifuge testing is an experimental technique that allows reduced-sca
le duplication, in the laboratory, of the stresses and pressure distributio
ns encountered in the field. In situ conditions are critical in the develop
ment of actual air flow patterns. Experiments are being conducted in a tran
sparent porous medium consisting of crushed borosilicate glass submerged in
fluids of matching indices of refraction. Air is observed as it flows thro
ugh the porous medium at varying gravitational accelerations. Recorded imag
es of experiments allow the determination of flow patterns, breakthrough ve
locities, and plume shapes as a function of g-level and injection pressure.
Results show that air flow patterns vary from fingering, at low g-levels,
to pulsing at higher accelerations. Grain and pore size distribution of the
porous medium do not exclusively control air flow characteristics, Injecto
r geometry has a definite effect on breakthrough velocities and air plume s
hapes. Experiments have been conducted to compare the velocity of air Row t
hrough the saturated porous medium to that of air in pure liquids. Results
show that the velocity of air through the medium is lower than that in the
pure fluid, as expected. At high g-levels however, plume breakthrough veloc
ities are proportional to the velocity of the air in the pure fluid. (C) 20
00 Elsevier Science B.V. All rights reserved.