Interactive visual01 · advancedBoltzmann Energy Distributionhigh energy is possible, just exponentially rareAt temperature T a state of energy E is weighted by e^(−E/kT). Metropolis sampling reproduces the distribution with a simple accept/reject rule.Copy promptOpen →
Interactive visual02 · commonHeat Diffusioneach cell drifts toward the average of its neighboursHeat flows down temperature gradients at a rate set by the Laplacian. The explicit grid update is four lines of code, and is stable only if αΔt/Δx² ≤ ¼.Copy promptOpen →
Interactive visual03 · coreIdeal Gas Kineticspressure is just particles bouncing off wallsTemperature is average kinetic energy and pressure is momentum delivered to the walls. Bounce point particles in a box and PV = NkT falls out.Copy promptOpen →