See one field cell become a self-adjusting coherent system.
This solver exposes each local term instead of hiding the result behind color. Every cell carries a field state, phase, coherence, compression response, expansion response, baseline ΔQ, event ΔQ, and UFR contribution. An adaptive engine recalculates the core formula on every virtual attosecond microcycle and feeds the current lattice state back into the next set of effective parameters.
Fundamental-cell lattice
Click a cell to inspect it. Use an injection mode, then drag or click to change the local state.
One equation, resolved into observable local roles
The visual is not a single texture. Each view isolates a term that contributes to the same cell update, allowing the user to see where structure, difference, coupling, and propagation enter the MEFI model.
Fundamental cell state
F, θ, ΔQ are the local state variables. A cell has a field value, a phase, and a structured difference before it joins a larger pattern.
Local difference
∇²F compares one cell with its nearest neighbors. Positive curvature feeds expansion; negative curvature feeds compression.
Compression kr
C = kr·max(−∇²F,0)/(r²(1+r)). This is the inward/organizing response used by the solver.
Expansion kc
E = kc·max(∇²F,0)/r². This is the outward/regulating response used by the solver.
Coherence
Neighbor phase vectors are averaged into a 0–1 local coherence. Higher coherence reduces effective radius and strengthens organized UFR response.
ΔQ
Baseline and injected event differences combine locally. The sign determines direction; magnitude changes impedance and the UFR contribution.
UFR factor
fUFR = coherence·(1+|ΔQ|)·(1+propagation). The factor is computed per cell, then phase-modulated in observer time.
Emergence
Repeated local updates produce waves, nodes, stable bands, and cascades. The emergent view averages cells; it never replaces their underlying values.
Attosecond feedback
Each virtual-attosecond microcycle recomputes the lattice, derives bounded effective coefficients from the result, and returns them to the next core-formula evaluation. The displayed base → effective values expose that feedback directly.
The adaptive rule is visible and bounded
The slider values are base parameters. A dimensionless state driver is recalculated from the previous full-lattice solution, then used to derive the starred effective parameters in the live formula. Bounds prevent the feedback loop from silently producing unstable or undefined coefficients.
State driver
S = clamp(.52⟨|ΔQ|⟩ + 2.4|⟨E−C⟩| + .36(1−⟨coh⟩) + .08|⟨F⟩|, 0, 1)
Directional imbalance
I = tanh(10⟨E−C⟩). Positive values bias expansion feedback; negative values bias compression feedback.
Effective compression
kr* = kr·clamp[1 + A(.34S − .24I + .12(1−coh)), .35, 2.5]
Effective expansion
kc* = kc·clamp[1 + A(.34S + .24I + .08coh), .35, 2.5]
Adaptive integration
Coupling rises with coherence, damping rises with stress, and effective Δt tightens under stress. Each revised set is used for exactly one modeled-attosecond microcycle before the formula is recalculated again.
From difference to the next field state
The highlighted stage follows the currently dominant contribution at the selected cell.
Selected-cell evolution
The chart records the selected cell through time. The ledger shows the current formula terms and whether each is increasing or reducing the next state.
| Term | Live value | Role |
|---|---|---|
| Local curvature ∇²F | 0.0000 | Chooses expansion or compression route |
| Expansion Ekc | 0.0000 | Positive bracket contribution |
| Compression Ckr | 0.0000 | Subtracted bracket contribution |
| ΔQ impedance | 1.0000 | Scales the bracket |
| ΔQ × fUFR | 0.0000 | Coherent difference contribution |
| Neighbor diffusion | 0.0000 | Local propagation exchange |
| Damping | 0.0000 | Stability term |
| Total ΔF/Δt | 0.0000 | Integrated into Fnext |