Monday, November 2, 2009
Convention Center, Exhibit Hall BC, Second Floor
Virginia C. Aparicio1, Jose Luis Costa1 and Daniel Giménez2, (1)INTA, Balcarce, Argentina
(2)Department of Environmental Sciences, Rutgers State Univ., New Brunswick, NJ
ABSTRACT
Solutes dispersion in soil has received considerable attention because
of the concern about ground water pollution by agricultural chemicals. We
studied solute dispersion by applying pulses of bromide (Br) tracer at the
surface of Mar del Plata
fine illitic loam soil during constant, unsaturated
water infiltration at a flow rate of 11 mm h-1. Water was applied, using
a net of micro-sprinklers over the surface of 12 plots of 30 m2. Ceramic
soil–water suction samplers were installed at each plot at three depths: 1, 1.5
and 2m. Rain gauges were placed at the same position where the ceramic cups
were installed to measure the water flow rate. Solute concentrations measured
at the determined depths and times allowed estimation of average pore-water
velocity and dispersion (D). The Br- concentrations were fitted to
the steady-sate convection-dispersion analytical model en the CXTFIT package.
The bromide breakthrough curves (BTCs) were analyzed
with the classical equilibrium convection–dispersion equation CDE and a
non-equilibrium two-region mobile–immobile model. Pore water velocity
determined with CDE for equilibrium at 1, 1.5 and 2m, were 6.5, 8.7, and 7.8
respectively and D were 413, 797, and 647. Pore water velocity determined with
CDE for non-equilibrium at 1, 1.5 and 2m, were 1.6, 2.7, and 4.7 respectively and
D were 413, 797, and 647. The relative fractions of mobile and immobile water (b) for
non-equilibrium at 1, 1.5 and 2m were 0.22, 0.33, and 0.31 respectively. The non-equilibrium
CD model proved to be better than the equilibrium in interpreting asymmetric BTCs. The lower values of b are an evidence of the degree of
preferential flow for this soil.