01 K & Porosity Variabilities
Before chemistry enters, how do two physical properties together steer a plume?
What you’re watching A reactive plume in an aquifer where both hydraulic conductivity and porosity vary; the plume fingers through the field, with porosity modulating how fast solute actually moves within the high- and low-K zones.
The mechanism Conductivity sets the Darcy flux; porosity converts that flux into the actual (seepage) velocity that carries solute (v = q / n). When both vary, the velocity field — and the plume — depends on their combination, though K variability usually dominates and porosity is a secondary modifier.
Why it matters It sets the physical baseline: even with no chemistry, multiple varying properties shape transport — the starting point before reactive heterogeneity is added.
IGW-NET IGW-NET lets you turn randomness on for one property at a time — K here, porosity there — so you can isolate each one’s role in a controlled, one-variable-at-a-time experiment that is impossible in the field.
02 K & Partitioning Coeff Variabilities
What happens when the chemistry varies in step with the geology — and why is the worst case a negative correlation?
What you’re watching The same reactive plume run four ways: with uniform sorption; with the sorption coefficient (Kd) positively correlated with K; negatively correlated with K; and uncorrelated. The negatively-correlated case is dramatically the most stretched, fingered, and tailed.
The mechanism Sorption retards solute by the factor R, which rises with Kd. In real aquifers Kd is often negatively correlated with K — clay-rich lenses are both low-conductivity and high-sorbing. So the slow zones retard solute even more while the fast zones move it freely: the chemical and physical heterogeneity reinforce each other, amplifying the velocity contrast and trapping parcels far more than K variability alone. A positive correlation would partly cancel — fast zones would also retard — keeping the plume compact.
Why it matters This is why pump-and-treat of a chemically active contaminant is even harder than for an inert one: the very zones that hold the most contaminant are the slowest to flush, so the tail persists far longer. Chemical and geological heterogeneity together are worse than either alone.
IGW-NET IGW-NET lets you switch on randomness in Kd and choose how it correlates with K — positive, negative, or none. Flipping that correlation and watching the plume go from compact to violently tailed reveals an interplay almost impossible to see any other way — simulating the unseen coupling of chemistry and geology.
03 K, Porosity, & Partitioning Coeff Variabilities
Put all three together — how complex does real reactive transport get?
What you’re watching The full case: conductivity, porosity, and sorption all varying, with and without the negative K–Kd correlation. The negatively-correlated runs again show the strongest channeling and tailing, with porosity variability a secondary modifier on top.
The mechanism Real aquifers vary in every property at once, and the properties are cross-correlated. The dominant effect remains the negative K–Kd coupling that traps reactive solute in slow, high-sorbing zones; porosity variability fine-tunes the velocities but does not change the qualitative picture.
Why it matters It is the realistic worst case for characterization and cleanup: a plume whose behavior is set by the joint structure of several uncertain, cross-correlated properties — not by any one of them.
IGW-NET You can turn randomness on or off for any property — K, Kd, porosity, recharge, decay — and prescribe how they correlate, then watch the combined effect. And because the same controls work on an idealized sandbox or on a real site through the global base model, you can explore the interplay of physical and chemical heterogeneity in a teaching case and in an actual aquifer with equal ease — understanding fate and transport in porous media in a way that was previously very hard to reach.