Self-Avoiding Walk & Flory Exponent

Polymers in good solvent swell: end-to-end distance R ~ Nν with ν ≈ 0.588 in 3D (ν = 3/4 in 2D)

Parameters

80
20
Current N
End-to-end R
⟨R²⟩^½ (this N)
Fitted ν (log-log slope)
Theory ν₂D = 3/40.750
Self-Avoiding Walk (SAW) & Flory Theory

A random walk on a 2D lattice that cannot revisit any site. Flory (1949) minimized free energy F = R²/Nb² + N²/R^d to get:

ν = 3/(d+2)
• d=2: ν = 3/4 = 0.75 (exact, Nienhuis 1982)
• d=3: ν ≈ 0.588 (exact RG)
• d=4: ν = 1/2 (upper critical dim)

This is polymer science's most important scaling law. In good solvent, excluded volume interactions cause swelling. The walk displayed uses a pivot algorithm (MCMC) for efficient sampling.

The log-log plot shows R vs N — the slope gives ν. Collect data at multiple N to see the power law emerge.