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Slurry‐processed composite solid electrolyte membranes for all‐solid‐state batteries (ASSBs) are governed by particle size and binder molecular weight. Here, we vary Li 6 PS 5 Cl (LPSCl) average particle size ( d p = ~5.6, ~7.5, and ~9.0 µm) and polyisobutylene (PIB) binder molecular weight (M w = ~1050, ~1550, and ~3050 kg mol −1 ) across a factorial design to resolve their effect on ionic conductivity ( σ ion ), ionic tortuosity factor ( τ ), and activation volume ( V * ) under controlled stack pressure ( P s ). Physics‐based electrical equivalent circuit (EEC) models reveal that mechanical consolidation drives a transition from interface‐controlled to constriction‐dominated transport at a formulation‐dependent onset pressure, evidencing geometric and rheological effects as separable yet interacting control parameters. From the EEC parameters, a geometric–rheological decoupling framework has been derived and validated against unseen d p – M w combinations ( R 2 = 0.82 for σ ion and 0.85 for τ and V * ), establishing binder M w as the dominant variable whose penalty cannot be recovered by higher P s . Particle size acts as a secondary modulator: ~7.5 µm particle selection balances contact‐network density against binder kinetics, while at ~9 µm particle‐skeleton dynamics increasingly dominate, defining the framework’s upper quantitative boundary. Dry‐room calendering identifies lower‐ M w , intermediate‐ d p combinations that retain above 75% of original σ ion as a window for scalable processing.
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Suttor et al. (2026) studied this question.
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