Faramatic™: Capacitor Network Synthesizer

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

Left: Controls, ΔC Metrics & Package Scaler • Right: Interactive Scrubber & 5-Tab Multi-Charts • Bottom: Dielectric Physics & Pareto Theory

Faramatic™ Synthesizer & Hysteresis Resolver

Normal Synthesis
4
Quick Select:
Pareto States --
Game Fit --%
Fit NRMSE --%
BOM Cost $0.00
Span ΔC --
Min Step ΔCmin --
Max Gap ΔCmax --
Package Range --
Base Capacitors & Required Packages: Seed Mode

Boundary Ranges & Switch Fabric

Log10 Bounds (pF)
100 pF
102
100 nF
105
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): --
Capacitors: 42×24px [Index Only]
✓
Pareto Selection Justification:

Canonical optimal selection: Lowest equivalent series resistance ESR_eq and fewest toggled switches across equivalent capacitance paths.

Y-Scale:
• Dark Line: Synthesized Pareto States • Shaded Area: Precision Envelope [±P] • Stepped Red Line: Minimum Required SMD Footprint
Active Op-Amp Filter / Miller Integrator Parameters:

Dielectric Physics, Volumetric Footprint Scaling & Pareto Degeneracy

Faramatic™ Physical Theory

Dielectric Volumetric Limit Law

$$\text{Vol} \ge \frac{C \cdot V_{\text{rated}}^2}{\varepsilon_0 \varepsilon_r E_{\text{breakdown}}^2}$$

Why Capacitors Must Scale in Size: Unlike thin-film resistors where sheet resistivity $\rho/t$ and laser trimming allow any value from $1\,\Omega$ to $10\,\text{M}\Omega$ in an invariant 0603 footprint, electrostatic energy storage requires physical dielectric volume. High capacitance forces footprint jumps: 0402 ($\le 10\,\text{nF}$) → 0603 ($\le 220\,\text{nF}$) → 0805 ($\le 2.2\,\mu\text{F}$) → 1206 ($\le 10\,\mu\text{F}$) → 1210 / Tantalum ($> 10\,\mu\text{F}$).

Pareto State Count Disparity

$$\frac{\Delta C}{C_{\text{large}}} = \frac{C_{\text{small}}}{C_{\text{large}}} < \varepsilon_{\text{cluster}}$$

Extreme Decade Masking: When synthesized values span $\ge 3$ decades, combining extreme parts ($C_{\text{large}} \parallel C_{\text{small}}$) creates relative shifts smaller than the Pareto clustering tolerance ($\varepsilon < 0.15\%$). The Pareto optimizer collapses these topologically distinct formulas into a single cluster. Faramatic employs an adaptive threshold $\varepsilon_{\text{cluster}} = \min(0.0015, P/5)$ to preserve high-precision states.

Equivalent Series Resistance (ESR)

$$ESR_{\text{series}} = \sum_k ESR_k, \quad \frac{1}{ESR_{\text{parallel}}} = \sum_k \frac{1}{ESR_k}$$

Capacitor parasitics track as equivalent series resistance ($ESR$) and switch $R_{\text{on}}$. Parallel combinations compound capacitance while dividing $ESR$, yielding high $Q$-factor states. In filtering, $ESR$ and interconnect parasitics determine the ultimate high-frequency stopband floor.

Lockstep Rank-1 Singularity

$$\mu([C_0, C_0]) = 0 \implies n = 1, \quad C_{\text{min}} \equiv C_{\text{max}}$$

When $C_{\text{min}} = C_{\text{max}}$, the target interval has zero measure, collapsing degrees of freedom to $n = 1$. The state machine enters lockstep array mode: both boundaries travel together. Dragging $n > 1$ or clicking the decouple badge immediately restores the prior multi-capacitor state from hysteresis memory.