  We study the motion of discrete interfaces driven by ferromagnetic
interactions on the two-dimensional triangular lattice by coupling the Almgren,
Taylor and Wang minimizing movements approach and a discrete-to-continuum
analysis, as introduced by Braides, Gelli and Novaga in the pioneering case of
the square lattice. We examine the motion of origin-symmetric convex
"Wulff-like" hexagons, i.e. origin-symmetric convex hexagons with sides having
the same orientations as those of the hexagonal Wulff shape related to the
density of the anisotropic perimeter $\Gamma$-limit of the ferromagnetic
energies as the lattice spacing vanishes. We compare the resulting limit motion
with the corresponding evolution by crystalline curvature with natural
mobility.
