More from Thermodynamics
Other simulators in this category — or see all 40.
Kuramoto Oscillators
All-to-all coupled phases θ_i with intrinsic frequencies ω_i: order parameter r = |N⁻¹ Σ e^{iθ_i}| grows as coupling K crosses the synchronization window—classic mean-field rhythm transition.
Vicsek Model (Active Matter)
Self-propelled particles on a torus align headings with neighbors within radius R, add noise η, then drift at v₀; polarization V_a = |⟨e^{iθ}⟩| captures the flocking crossover with density ρ = N/L².
Wolfram Elementary Cellular Automata
1D binary CA with Wolfram code R∈[0,255]: space–time raster, periodic or null boundaries, single-cell or random IC, rule-bit strip, and informal class hints for textbook rules (e.g. 30, 90, 110, 184).
Eden Growth (Lattice)
Square-lattice Eden model: each step occupies a uniformly random empty von-Neumann neighbor of the cluster; compact growth with a rough interface—track perimeter P vs 2√(πN) as a roughness proxy.
Ising 2D: Wolff Cluster Updates
Ferromagnetic toroidal Ising (h = 0): Swendsen–Wang bond freezing with probability 1 − e^(−2βJ), build a same-spin cluster, flip it—fast mixing near T_c compared to single-spin Metropolis.
Hopfield Associative Memory
10×10 binary Hopfield network: Hebbian pattern storage, energy E = −½ Σ w_ij S_i S_j, and random asynchronous updates that flow downhill to fixed-point recall after noisy cues.