Between p = 0.58 and p = 0.60 almost nothing changes in quantity, yet everything changes in kind. Each cell of this 96×64 grid is opened independently with probability p, adjacent open cells merge into clusters, and right at the threshold p_c ≈ 0.5927 for the two-dimensional square lattice a cluster suddenly appears linking the top edge to the bottom. Exactly at that point the giant cluster is riddled with holes like a fractal and at its most fragile; the larger the grid, the steeper the jump from sealed to leaking.
Between p = 0.58 and p = 0.60 almost nothing changes in quantity, yet everything changes in kind. Each cell of this 96×64 grid is opened independently with probability p, adjacent open cells merge into clusters, and right at the threshold p_c ≈ 0.5927 for the two-dimensional square lattice a cluster suddenly appears linking the top edge to the bottom. Exactly at that point the giant cluster is riddled with holes like a fractal and at its most fragile; the larger the grid, the steeper the jump from sealed to leaking.
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