Summary: We present a proof of a conjecture made in the field of crystal growth. Namely, for an initial state consisting of any number of growing crystals moving outwards with normal velocity given to be \(\gamma(\vec n)\), for \(\vec n\) the unit outwards normal, then the asymptotic growth shape is a Wulff crystal, appropriately scaled in time. This shape minimizes the surface energy, which is the surface integral of \(\gamma(\vec n)\), for a given volume. The proof works in any number of dimensions. Additionally, we develop a new approach for obtaining the Wulff shape by minimizing the surface energy divided by the enclosed volume to the \({1\over d}\) power in \(R^d\). We show that if we evolve a convex surface (not enclosing a Wulff shape) under the motion described above, that the quantity to be minimized strictly decreases to its minimum as time increases. We have thus discovered a link between this surface evolution and this (generally nonconvex) energy minimization. A generalized Huyghen’s principle is obtained. Finally, given the asymptotic shape, we also obtain the associated (unique) convex \(\gamma(\vec n)\). The key technical tools are the level set method and the theory and characterization of viscosity solutions to Hamilton-Jacobi equations.