Ohmatic™: Resistor Network Synthesizer

L. Van Warren, PhD • Version-I © 2026 • All Rights Reserved

Left: Controls, ΔR Metrics & Lockstep Singularity Machine • Right: Interactive Scrubber & 5-Tab Multi-Charts • Bottom: KaTeX Theory

Ohmatic™ Synthesizer & Hysteresis Resolver

Normal Synthesis
4
Quick Select:
Pareto States --
Game Fit --%
Fit NRMSE --%
BOM Cost $0.00
Span ΔR --
Min Step ΔRmin --
Max Gap ΔRmax --
Span Ratio SR --
Base Resistors (1..n): Seed Mode

Boundary Ranges & Switch Fabric

Log10 Bounds
10 kΩ
104
1.0 MΩ
106
Switches:--
R_on:-- Ω
C_off:-- pF

State Sequence Scrubber & Switching Engine

State 1 / 1
0% (Parallel)
Switch Toggles:ΔS = 0
Glitch Energy:-- nJ
T_settle:-- μs
Active Circuit Schematic (Crisp Single-Pixel Canvas): --
Resistors: 42×24px [Index Only]
✓
Pareto Selection Justification:

Canonical optimal selection: Lowest parasitic capacitance C_eq and fewest toggled switches across equivalent resistance paths.

Y-Scale:
• Dark Line: Synthesized Pareto States • Shaded Area: Precision Envelope [±P] • Dashed Line: Ideal Progression Objective
Inverting Op-Amp Feedback Filter Parameters:

Mathematical Models, Circuit Principles & Range Singularity Hysteresis Theorem

Ohmatic™ Synthesis Theory

Singularity Hysteresis & Lockstep

$$\Delta R_{\text{span}} = R_{\text{max}} - R_{\text{min}}, \quad \mu([R_0, R_0]) = 0$$

Lockstep Coupling Theorem: When $n = 1$, the resistor array can only synthesize a single degenerate point. Consequently, $R_{\text{min}}$ and $R_{\text{max}}$ must travel together in lockstep. Reciprocally, when $R_{\text{min}} = R_{\text{max}}$, network degrees of freedom collapse to $n = 1$. The state machine preserves $n_{\text{prior}} \ge 2$ in hysteresis memory, restoring prior state upon range decoupling.

$$0 < \Delta R_{\text{min}} \le R_{k+1} - R_k \le \Delta R_{\text{max}} < R_{\text{max}}$$

Cograph SP-Trees & Pareto Filter

$$R_{\text{series}} = \sum_k R_k, \quad \frac{1}{R_{\text{parallel}}} = \sum_k \frac{1}{R_k}$$

Cographs (complement-reducible graphs) contain no induced $P_4$ paths and decompose into canonical Series-Parallel trees. When redundant topologies yield equivalent resistances ($\vert{}\Delta R / R\vert{} < 0.15\%$), the Ohmatic™ Pareto engine selects:

$$\arg\min \Big[ C_{\text{eq}}(\mathcal{T}) \Big] \to \arg\min \Big[ \Delta S(\mathcal{T}) \Big] \to \arg\max \Big[ I_{\text{max}}(\mathcal{T}) \Big]$$

Parasitic Capacitance & Cutoff

$$\frac{1}{C_{\text{series}}} = \sum_k \frac{1}{C_k}, \quad C_{\text{parallel}} = \sum_k C_k$$

Parasitic capacitance follows the inverse harmonic algebraic dual of resistance. For identical base packaging ($C_p / R_k \approx \text{const}$), the network preserves an inherent time-constant invariance:

$$f_c = \frac{1}{2\pi R_{\text{eq}} C_{\text{eq}}}, \quad \tau = R_{\text{eq}} \cdot C_{\text{eq}} \approx \text{constant}$$

Switch Hamming & Op-Amp Filter

$$\Delta S = \sum_{j=1}^{n} |s_j^{(k)} - s_j^{(k-1)}|, \quad E_{\text{glitch}} \propto \Delta S \cdot (1 + \eta_{\text{seq}})$$

Staggering switch actuation ($\eta_{\text{seq}} > 0$) causes ripple chatter, increasing transient glitch energy. For inverting op-amp feedback loops:

$$A_v(f) = -\frac{Z_f(f)}{R_{\text{in}}} = -\frac{R_{\text{eq}}}{R_{\text{in}} \sqrt{1 + (2\pi f R_{\text{eq}} C_{\text{eq}})^2}}$$