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design note · Water Fuel Cell · computed

WFC design session v33: reasoning

Lab note — CGDE-window sweep, Randles floor. This run was supposed to walk the vapor-film field down into the 80–250 Td cold-chemistry window by shrinking the gap (sub-3mm) and driving harder at low duty. It didn't get there. My best candidates light the 0.1mm film at 314–358 Td — still Townsend-avalanche, still above the 3–6 eV band I'm scoring for. The 0.643 plateau is the model telling me it can't reach the window without either a smaller gap or a lower cell voltage, and lowering voltage collapses the resonant rise I need. Honest read: the "reward" is coming from margin and displacement fraction (97.7%), not from actually sitting in the window.

The trade-off is clean. Q≈25 buys me ×25 voltage magnification (899V from 36V) but at 1.03A circulating — that's the real wire/switch rating, not the 21mA average. Tightening the annulus (#4/#5, 17.6mm tube) raises C to 2.47nF, drops f_r to 85.6kHz and Q to 21.9, which pulls Td down to 314 — the right direction — but costs breakdown margin (×148 vs ×180). The duty triplet (#1/#2/#3) is identical physics, just more average current for the same shot; I take the leanest.

Adopting #1: 14mm/19mm × 120mm, 0.5ppm/8°C/×0.4 passivation, 2% duty. Lowest average current, highest margin, and displacement-dominated so Faradaic leakage (109mA peak) stays inhibited while voltage climbs.

Next session: push gap below 1.8mm and drop peak_v deliberately to chase 250 Td head-on; sweep film thickness (0.05–0.15mm) since Paschen is thickness-sensitive. The window, not resonance, is the constraint now.

Basis

Confidence
0.70
Recorded
Published
30 Aug 2026
Device
Water Fuel Cell
Component
cell
Source Ref
design session v33
Notebook Id
1597

design-loop