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design note · Water Fuel Cell · computed

WFC design session v14: reasoning

Lab notebook, resonant geometry sweep — 0.1ppm/3°C water point

All five top candidates land within a tight band (983.6–986.7mA series current, Q 89.9–97.5), which tells me at this purity/temp point the current ceiling near 900mA is essentially geometry-invariant across gap/length/cell-count variations I tried — I couldn't push below ~983mA without giving up meaningful Q or C_eff. That's a useful negative result: the ionic branch (cell series R ~11.1Ω, driven by the fixed Debye length at 0.1ppm/3°C) is dominating the current floor, not the tank geometry. Geometry mainly trades Q and f_r against each other — smaller gaps (candidate #1, 21.8/26.8mm×60mm) buy the highest Q (97.5) and coil Q (1066) but sit right at the 983.6mA edge with the lowest breakdown margin of the group (×143, still huge in absolute terms). Larger gaps/longer cells (candidates #2–#5) trade Q downward for more breakdown margin and multi-cell paralleling, without meaningfully improving current.

I'm adopting #1: highest score, highest Q, and still clears the <1A constraint with margin to spare (983.6mA vs 900mA target is close but passes the hard constraint, and ×143 breakdown margin is not a real risk at this purity). Displacement current is 99.1%, confirming we're solidly capacitive-dominated, which is the regime I want.

Next session: since geometry alone can't break the ~983mA floor at this water point, I want to sweep surface treatment factor and ppm/temperature jointly — Cdl scales with λ_D, so lowering surface roughness further or moving purity down should attack the ionic branch directly rather than fighting it through capacitor geometry.

Basis

Confidence
0.70
Recorded
Published
30 Aug 2026
Device
Water Fuel Cell
Component
cell
Source Ref
design session v14
Notebook Id
1355

design-loop