The 3D simulator treats the whole clay aquitard as one lumped block: the instant head drops by ΔH, the entire layer feels the full effective-stress change at once and compacts by Δb = −Ssk·b₀·ΔH. That is exact only when the clay drains instantly — real clay does not.
This 2D version instead solves Terzaghi's actual 1D consolidation diffusion equation across depth z through the clay, independently at each of 41 depth nodes:
∂s/∂t = c_v(z,t)·∂²s/∂z² (s = local head decline / effective stress)
c_v = K_clay / S_sk(z,t) (S_sk switches per node: elastic ↔ inelastic)
The two sand aquifers on either side are far more permeable, so their head follows the pump instantly — that becomes the boundary condition driving diffusion inward from both faces. Because inelastic storage Sskv is many times larger than elastic Sske, the diffusivity cv collapses once a node goes virgin — so the interior of a thick clay bed can lag the boundary by years to decades. Total compaction is the exact integral of the local elastic/inelastic law over the resolved profile, not one number for the whole layer.
- Profile panel (top) — the live head-decline profile across the aquitard's depth (bright line), with faded "isochrones" from earlier moments so you can watch the diffusion front creep inward. Node color marks elastic (green) vs inelastic/virgin (red) at that depth.
- History panel (bottom) — boundary head decline (reacts instantly) vs. actual land subsidence (lags behind it) over simulated time.
- Committed future subsidence — the compaction that will still happen even if you freeze the pumping rate right now, because the aquitard's interior hasn't caught up to the boundary yet. This delayed/residual compaction is a well-documented real phenomenon (San Joaquin Valley, Jakarta) that a lumped 0-D model can't represent at all — verified numerically to converge to the 3D model's own formula in the no-delay limit, and to reproduce Terzaghi's classic analytical consolidation curve for a fixed diffusivity.