This is the 2D counterpart to the 3D setae-array model — same Kendall peel physics, but here the peel front is not just read off Kendall's formula, it is driven by real crack-tip fracture kinetics. You set an applied peel force F directly; the simulation computes the energy release rate at the delamination front and integrates the front's motion from a fracture-mechanics rate law, frame by frame.
G = F · (1 − cos θ) energy release rate (mN/mm)
Fcrit = Γ / (1 − cos θ) Kendall's critical peel force
v_front = v₀ · max(0, G/Γ − 1) linear debonding-rate law
If F ≤ Fcrit → G ≤ Γ → front does not move at all.
If F > Fcrit → front advances, faster the further F sits above Fcrit.
Kendall's classic equation F/b = Γ/(1 − cos θ) is the special, rate-independent case of this: it is exactly the force at which the energy release rate first equals the work of adhesion — the threshold below which nothing peels no matter how long you wait. Push F only slightly over that threshold and the front creeps; push it hard over and it peels fast. This is the same Griffith-type fracture criterion used to model real peel-test crack propagation, and it reduces to Kendall's rate-independent law in the quasi-static limit.
- θ slider — the instantaneous angle between the backing film and the surface at the peel front.
- Γ slider — work of adhesion per unit width; higher Γ raises both the critical force and (for a given excess force) slows the front.
- F slider — the peel force per unit width you are actually applying. Below the critical force line the front is locked — this is the gecko's "shear lock" state made explicit as a real threshold, not just a color change.
- Pad width — scales total force by the number of engaged seta columns.