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design note · Water Fuel Cell · computed

WFC design session v17: reasoning

Lab note, 3 July — ppm/surface sweep at low temp.

Findings confirm the ionic-branch knee sits right at 0.1ppm Na+ near 3°C: bulk water R climbs to ~128kΩ and the Randles series resistance (11.1Ω) is now dominated entirely by the double-layer geometry, not the electrolyte. What's interesting is that surface_factor (0.25 through 0.7) had zero effect on the top-line numbers — C_dl scales with area as expected (1.9µF→5.3µF) but since displacement current is already 99.1% and the tank is capacitively dominated, cell series R and hence current draw don't move. That tells me at this ppm/temp point the double-layer area is not the current-limiting lever anymore — I was hoping reducing surface area would buy back margin below 983.6mA, but it's flat. The real degrees of freedom left are ppm and temperature: dropping from 3°C to 4°C (candidate #5) cost me Q (97.5→94.3) and pushed current down only marginally (983.6→948.6mA) while raising f_r slightly. Breakdown margin stayed enormous (×143-147) across the board, so I'm not breakdown-limited here — I'm current-limited by design intent, sitting deliberately just under 1A.

Adopting #1: identical performance to #2-4 but minimum surface_factor (0.25) means least electrode area/cost for the same result — no reason to pay for more Cdl area when it buys nothing.

Next session: hold surface_factor fixed at 0.25, sweep ppm below 0.1 (toward near-deionized) and temperature down toward 0°C to see if the knee moves further and current drops below the 900mA mark with margin to spare.

Basis

Confidence
0.70
Recorded
Published
30 Aug 2026
Device
Water Fuel Cell
Component
cell
Source Ref
design session v17
Notebook Id
1361

design-loop