Inside a lithium-ion cell, the graphite (or silicon) anode sits below the electrolyte's stability window. On first charge — and continuously, at a slow trickle, ever after — electrolyte molecules reduce at the anode surface and precipitate into a nanometre-scale passivation film: the solid-electrolyte interphase (SEI). It is electronically insulating but ionically conducting, so it protects the electrolyte from further reduction — at the cost of permanently consuming cyclable lithium and adding resistance.
Because fresh electrolyte must diffuse through the existing film to react, growth is diffusion-limited and follows a parabolic (√t) rate law:
δ(t) = √(2 · k_p · t) [SEI thickness, diffusion-limited growth]
k_p(T) = k₀ · exp(−E_a / R·T) [Arrhenius rate constant]
Capacity(t) ≈ Q₀ − c · δ(t) [lithium trapped in film ∝ new SEI formed]
R_cell(t) = R₀ · (1 + δ(t)/δ_ref) [added film resistance, Ohm's law]
- Temperature — enters through the Arrhenius term; every ~10°C roughly doubles the growth rate, so a hot cell ages far faster than a cool one.
- Cycling rate (C-rate) — faster charge/discharge raises local current density and self-heating, accelerating side-reaction kinetics beyond the calendar-aging baseline.
- SEI-stabilizing additive — models electrolyte additives (e.g. FEC, VC) that form a denser, less permeable initial film, roughly halving the long-run growth constant k₀.
- Time acceleration — the film needs months to years to visibly thicken in a real cell; this control fast-forwards simulated calendar time.
The small spheres are the cyclable lithium-ion inventory diffusing in the electrolyte; as the shell thickens, ions are progressively trapped into the growing film — visualizing exactly the irreversible-capacity-loss mechanism that dominates long-term battery aging.