『Abstract
Saprolite formation rates influence many important geological
and environmental issues ranging from agricultural productivity
to landscape evolution. Here we investigate the chemical and physical
transformations that occur during weathering by studying small-scale
“saprolites” in the form of weathering rinds, which form on rock
in soil or saprolite and grow in thickness without physical disturbance
with time. We compare detailed observations of weathered basalt
clasts from a chronosequence of alluvial terraces in Costa Rica
to diffusion-reaction simulations of rind formation using the
fully coupled reactive transport model CrunchFlow. The four characteristic
features of the weathered basalts which were specifically used
as criteria for model comparisons include (1) the mineralogy of
weathering products, (2) weathering rind thickness, (3) the coincidence
of plagioclase and augite reaction fronts, and (4) the thickness
of the zones of mineral reaction, i.e. reaction fronts. Four model
scenarios were completed with varying levels of complexity and
degrees of success in matching the observations. To fit the model
to all four criteria, however, it was necessary to (1) treat diffusivity
using a threshold in which it increased once porosity exceeded
a critical value of 9%, and (2) treat mineral surface area as
a fitting factor. This latter approach was presumably necessary
because the mineral-water surface area of the connected (accessible)
porosity in the Costa Rica samples is much less than the total
porosity (Navarre-Sitchler et al., 2009). The model-fit surface
area, here termed reacting surface area, was much smaller than
the BET-measured surface area determined for powdered basaltic
material. In the parent basalt, reacting surface area and diffusivity
are low due to low pore connectivity, and early weathering is
therefore transport controlled. However, as pore connectivity
increases as a result of weathering, the reacting surface area
and diffusivity also increase and weathering becomes controlled
by mineral reaction kinetics. The transition point between transport
and kinetic control appears to be related to a critical porosity
(9%) at which pore connectivity is high enough to allow rapid
transport. Based on these simulations, we argue that the rate
of weathering front advance is controlled by the rate at which
porosity is created in the weathering interface, and that this
porosity increases because of mineral dissolution following a
rate that is largely surface-reaction controlled.』
1. Introduction
2. Weathering age
3. Methods
3.1. Electron microprobe analyses
3.2. Mineralogical changes
3.3. Chemistry of reacting fluids
3.4. Modeling approach
3.4.1. Reactive transport modeling
3.4.2. Effective diffusion coefficients
3.4.3. Mineral reaction rates
4. Results
4.1. Weathering rind thickness in Qt3
4.2. Electron microprobe analyses
4.3. Mineralogical changes
4.4. Chemistry of reacting fluids
5. Discussion
5.1. Features of the weathering rinds
5.2. Model development
5.2.1. Initial conditions
5.2.2. Secondary minerals
6. Model results
6.1. Scenario 1 - uncoupled model with no update of porosity
6.2. Scenario 2 - update of porosity using unmodified Archie's
Law
6.3. Scenario 3 - adjustment of accessible mineral surface area
with unmodified Archie's Law
6.4. Scenario 4 - incorporation of a diffusion threshold model
based on critical porosity
7. Model implications
7.1. Reaction front thickness
7.2. Rind advance rate
8. Implications for weathering studies across scales
9. Conclusions
Acknowledgments
Appendix A. Supplementary data
References