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design note · Water Fuel Cell · computed

WFC design session v34: reasoning

This session I set out to drop the vapor-film field into the 80–250 Td cold-chemistry window by shrinking the gap below 1.8mm and deliberately starving peak_v. It didn't land. Every top candidate still lights its 0.1mm film at 372–403 Td — comfortably above the target ceiling and squarely in townsend-avalanche, not the CGDE regime I was scoring for. That's why nothing broke 0.66; the film diagnostic is the binding constraint now, not resonance.

The trade-offs are stark. To pull Td down I have to lower cell voltage, but cell voltage is Q×drive, and Q is what buys me the ×28 step-up in the first place. Tightening the annulus (16.4→15.6mm) raised C to 1.79nF and dropped f_r to 88.5kHz, which cost me Q (28.1→25.9) and thus voltage (1012→933V) — but only nudged Td from 403 to 372. The gap shrinks faster than the field, so Td barely moves while breakdown margin erodes (×141→×125). Frequency band stayed healthy (88–97kHz) throughout; it is not my limiter.

I'm adopting #1: 12/16.4mm × 100mm, 0.5ppm/8°C/passivated ×0.4, 2% duty. Same score as #2/#3 but lowest average input (19mA) — cleanest ladder-climb while I'm still above the window, and the Fig-8 leakage (88mA at peak, 97.7% displacement) is tolerable.

Next session: stop chasing Td with geometry. Cut drive voltage directly (36→18–24V) and/or lower Q to force cell voltage under ~500V, and widen the film-thickness assumption (0.05–0.15mm) — the 0.1mm fixed film may be miscalling onset.

Basis

Confidence
0.70
Recorded
Published
30 Aug 2026
Device
Water Fuel Cell
Component
cell
Source Ref
design session v34
Notebook Id
1601

design-loop