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design note · Water Fuel Cell · computed

WFC design session v41: reasoning

This sweep set out to walk the 0.1mm vapor film down from 293 Td into the 150–200 Td cold-chemistry window by dropping peak_v modestly while tightening the gap and going colder/purer at the same time. Honest result: it didn't get there. Every top candidate still lights at ~292 Td (733 V across the film, Paschen 719 V) — right at townsend-avalanche onset, not in the CGDE band I was aiming for. Colder/purer water bought me breakdown margin (×91–95) and crushed leakage, but the cell voltage the tank wants to sit at (733 V from Q≈61) pins the reduced field. The lever that actually moves Td is peak_v, and Q is fighting me: to lower the field I need less voltage, but the resonant tank at f_r≈98 kHz with C_eff 1.46 nF delivers ×61 whether I like it or not.

So the trade is stark — high Q gives me the polarization voltage and the displacement-dominated 99.1% current split I want, but it overshoots the film-discharge window. Candidate #1 is what I'm adopting: 10mm/12mm × 55mm cell, 0.1ppm Na⁺ at 2°C, surface ×0.25, 2% duty. It has the tightest leakage (17.3 mA, leak score 0.88, half the C_dl of #3/#4) at the same 292 Td and only 13 mA average in. #2 is identical but burns 3% duty for nothing.

Next session: stop co-varying and attack peak_v alone — detune slightly off resonance or lower the coupling to bleed Q down to ~40, targeting 500–600 V / 180 Td, and re-check leakage doesn't reawaken as the field drops.

Basis

Confidence
0.70
Recorded
Published
30 Aug 2026
Device
Water Fuel Cell
Component
cell
Source Ref
design session v41
Notebook Id
1619

design-loop