A droplet resting on a rough hydrophobic surface can sit either fully wetting the texture (Wenzel state) or suspended on the tips of the asperities, trapping air underneath (Cassie–Baxter state) — the regime a good anti-soiling nanocoating is engineered for. For a droplet resting only on the pillar tops, the apparent contact angle θ* follows the Cassie–Baxter equation:
cos θ* = f_s (cos θ_Y + 1) − 1
f_s = π·(r/S)² — solid area fraction of the pillar tips (r = pillar radius, S = pitch)
θ_Y = intrinsic (Young) contact angle of the flat coating material, fixed here at 108°
(a typical low-surface-energy fluorosilane/PDMS coating)
Lower solid fraction f_s (sparse, tall, thin pillars) traps more air and pushes θ* toward 180°, the lotus-leaf regime. It also lowers contact-line pinning, which controls the sliding (roll-off) angle α_c via the Furmidge relation for a droplet on an incline:
m g sin α_c = w γ (cos θ_R − cos θ_A)
θ_A ≈ θ* (advancing angle, on the Cassie state)
θ_R ≈ θ* − Δθ, Δθ ≈ Δθ_max·f_s (fewer pillar edges to pin the receding line as f_s drops)
Using representative values for a 1 mm water droplet (γ = 0.072 N/m, ρ = 1000 kg/m³) gives sin α_c ≈ 3.5·(cos θ_R − cos θ_A). When the panel's tilt exceeds α_c the droplet is no longer pinned: it rolls downhill and, because it barely touches the pillar tips, picks up loose dust particles on the way — the mechanism engineers call self-cleaning. Below α_c the droplet stays put and just sits on the dust instead of removing it.
- Pillar height / pitch / radius fraction — the actual nanofabrication knobs (e.g. deep reactive-ion etching or nanoimprint lithography) that set f_s.
- Panel tilt — the real-world mounting angle of the module; compare it against α_c to see whether rain self-cleans this coating.
- Droplet size is shown enlarged relative to the pillars for visibility — real pillars are 10²–10³ nm, real droplets are mm-scale.